Full text
April 27th, 28th, 29th 2 022
Barcelona, Spain
S Y M P O S I U M O N S P A C E E D U C A T I O N A L A C T I V I T I E S
4th Edition
P R O C E E D I N G S O F
Inspiring through space
First edition : julio de 2022
© The Authors , 2022
© Iniciativa Digital Politècnica, 2022
Oficina de Publicacions Acadèmiques Digitals de la UPC
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ISBN: 978-84-19184-40-5
Any form of reproduction, distribution, public communication or transformation of these
works, beyond activities that are directly authorised by law, require the permission of the
owners
The Editors :
Miquel Sureda Anfres
Daniel Garcia-Almiñana
Gisela Detrell
Alberto Garc i a-Rigo
Ramón M. García Alarcia
Guillem Megías Homar
David González Díez
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Preface
The 4th Symposium on Space Educati onal Activit ies (4 th SSEA) was hosted at t he Universi tat
Politècni ca de Catalunya (UPC) · Barcel onaTech in Barcelon a, Spain, from 27th – 29th April 2022. It
was co - organized by the European Space Agency (ESA) and the UPC. The event represented the 4 th
editio n of a successful Space Edu cation symposi um that bega n at the Uni versity o f Padova, It aly, in
2015, followed by the 2 nd Symposium hosted by the Budapest University of Technology and Economi cs,
Hungary, i n 2018, a nd the 3 rd Symposium host ed by the Universit y of Lei cester, UK , i n 2019.
This long - awaited edition exceeded al l expectations and gathered more t han 500 attendees i n
Barcelona. The 4 th SSEA Organiz ing Committee develope d a comp elli ng outreach campaign that
reached to more than 2000 departments and universities. It ra ised support from more than 10 private
companies, and it had wide support f rom the local, regional and country - level institution s. During the
three days of the event in UPC’s venue Edifici V èrtex, the attendees engaged in fruitful research
discussions, established connections among the European sect or and learned from the lat est projects
in space educatio n and student - led projects.
The transformati on of the space secto r, as a result of new tech nology, busine ss and policy trend s,
creates new chal lenges for the education system, which must adapt to new secto r needs . NewSpace,
artificial intell igence, machine learning, additive manufactur ing … A ll these advance s create new needs
for a more interdisciplinary education. This i s the real meani ng of an event like the Symposium on Space
Educational Activi ties .
Here we pre sent the symposium procee dings that summarize all the presentations held during t he event.
We al so i ntrod uce a summ ary of t he sy mposi um or ganiz ati on, e vents and awar ds.
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4 th SSEA22 group pict ure
Keynote Speaker Jordi Puig Suari at the Venue
Gala Di nner a t the Fabra Observat ory
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Organizi ng Inst ituti ons
The 4 th Symposium on Space Educat ional Acti vities ( SSEA) was organised by the European Space
Agency (ESA), through the ESA Academy programme of the ESA Educati on Office ; a nd the Universita t
Politècni ca de Catal unya · Bar celonaTech ( UPC). It was organised in partn ership with the IEEC, ICCUB
and i2cat research centres, as wel l as with the institutional sponsorship of the Generalitat de Catalunya.
The ESA Academy, part of the ESA Educatio n
Office , is ESA's over archi ng programme for
Universi ty student s from ESA member stat es,
Canada, Latvi a, Lithuani a, and Sloveni a . The
ESA Academy provide s students wi th access to
both Hands - on Projects and a Training and
Learning Programme, as well as supporting,
through organisation and funding, the
Symposium on Spa ce Educatio nal Activ ities.
The Universitat Politècnica de Catalunya ·
BarcelonaTech (UPC) is a public inst ituti on of
research and higher education in the fields of
engineering, architecture, sciences and
technology, and one of the leading technical
universities in Europe. UPC’s schools devoted to
research and education on the aerospace field
are: ESEIAAT , EETAC , and ETSETB .
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Organizing C ommittee
The 4 th SSEA was a realit y thanks to the wo rk of a diver se team of committ ed and hard - work ing
members. Fo llowi ng the mott o of “a Sympos iu m made fo r student s – by students”, t he Organisi ng Team
was balanced mi x of professors and students and incl uded member s from different backgrounds and
institution s .
The core Organisi ng Committee was com posed by:
• Dr. Miquel Sureda Anfres ( UPC · Barc elonaTech ) – General Chair
• Mr. Ramón M. García Alarcia (ISAE – SUPAERO ) – Vice -ch air
• Mr. Guille m Megías Homar ( Stanford University ) – Vice -c hair
• Dr. David González Díez ( UPC · BarcelonaTech ) – Vice -c hair
• Dr. Daniel Garcia Almiñana ( UPC · BarcelonaTech ) – Vice -c hair
• Dr. Gisela Detrell ( University of Stuttgart ) – Co -c hair of technical a nd educational activities
• Ms. Magda Escorsa ( UPC · BarcelonaTech ) – Co -c hair of technical a nd educational activities
• Dr. Anna Ferré -M ateu ( Instituto de Astrofísica de Canarias ) – Co -c hair of technical and
educational activities
• Dr. Alberto Garc i a -R igo ( Institut d’Estudis Espacials de Catalunya ) – Co -c hair of technical and
educational activities
• Mr. Alexander Kinnaird ( ESA Academy ) – Co -c hair of technical a nd educational activities
• Ms . Laia L ópez ( International Space University ) – Co -c hair of technical a nd educational
activities
• Ms. Anna Ruiz Ayala ( INECO ) – Co -c hair of tec hnical and educational activities
• Dr. Núria Salán ( UPC · BarcelonaTech ) – Chair of Gender equality, Diversity and Sustainability
Board
• Dr. Adriano Camps ( UPC · BarcelonaTech ) – Chair of Scientific and Technical Activities Board
• Ms. Carme Fenoll ( UPC · BarcelonaTech ) – Chair of Logistics Board
For better preparati on and organ isation o f the eve nt, the Organising Commit tee creat ed and
supervised several autonomous boards tackl ing diff erent aspects such as communications ; logistics ;
scientific and techni cal activities; sponsors ; sustainability , equity and diversi ty; etc.
The Communicatio ns Board , in charge of social med ia, newsletter s , and the even t’s commun ications
and image in gener al , was composed of:
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• Ms. Laia López Llobet, Chair
• Ms. Àurea Cors
• Ms. Blan ca Pavón
• Ms. Lídia Fuentes
• Ms. Mar ina Can te
• Mr. José Ángel Gómez
• Ms. Gemma Domènech
• Mr. Arna u Amorós
The Logisti cs Board , in charge of the event logistics and suppliers , timetable , and social events, was
composed of:
• Ms. Anna Ruiz Ayala, Chair
• Mr. Ju an Fran cisco Lopera Zafra
• Mr. Dan iel S ors
• Ms. Lau ra Gonz ález
• Mr. Ser gio T abasco
• Ms. Núr ia Esc ursel l
• Ms. Ari adna A nguita
The Scienti fic and Technical Board , in charge of the Call for Abstracts, paper select ion, an d
preparation of Proceedi ngs, was composed of:
• Prof. Adr iano Camps ( UPC · Barcel onaTech ), Chair
• Dr. Daniel Garcia Almiñana ( UPC · Bar celonaTech ) , Executive Cha ir
• Dr. Gisel a Detrel l ( Uni versity of Stut tgart )
• Dr. Sil via Rodri guez - Donaire ( UPC · Ba rcelonaTech )
• Dr. Joan Montaña Puig ( UPC · BarcelonaTe ch )
• Dr. Manel Soria ( UPC · BarcelonaTe ch )
• Dr. Pil ar Gil Pons ( UPC · Barcelon aTech )
• Dr. Jordi Gutiér rez Cabell o ( UPC · Barcelon aTech )
• Mr. Pi ero Ga leone (E SA Re tiree, form er Head of ESA Academy )
• Dr. Nigel P. Banni ster ( Universi ty of L eicester )
• Dr. Laszl o Bacsardi ( Budapest Universi ty of Te chnology and Economics )
• Dr. Lorenz o Olivi eri ( Center of Studies a nd Activi ties f or Space “ G. Colombo” )
• Dr. Alber to Garci a - Rigo ( Institut d’Estudis Espacials d e Catalunya )
• Dr. Anna Fe rré - Mateu ( Instituto de Astrofísica d e Canarias )
• Ms. Lai a Lópe z ( International Space Unive rsity )
• Dr. Georg Herdrich ( Univer sity of Stuttgar t )
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• Ms. Mar iona Ba denas Ag ustí ( Mass achus etts Institute of Technology )
• Dr. Maria de Soria ( Jet Propulsion Laboratory )
• Ms. Beat riz Jilet e ( GMV )
• Ms. Arme lle Frenea - Schmi dt ( Swedis h Space Corpor ation )
• Mr. Bor ja Lá zaro To rall es ( Ma nufact uring Technol ogy Ce nter )
• Mr. Jo nathan Becedas ( Elecno r Deimos )
• Mr. Jo rdi Es cofet Miró ( INS Terrassa )
• Mr. Domi ngo Es cutia Muñoz ( ESERO Spain )
• Dr. Ed Ches ter ( Goonhil ly Ear th Sta tion Ltd )
• Dr. Nicol as Nolhi er ( Uni versity Paul Sabat ier of Toulouse )
• Ms. Cl ara Cr uz Nigg ebrugge ( ESA Aca demy )
• Mr. Jo sep Vi rgili Llop ( Space X )
• Mr. Al exander Kinnai rd ( ESA Academy )
• Ms. Ari an e Dedeban ( ESA Ac ademy )
The Sustaina bility, Equity and Div ersity Board , in charge of ensuring the meeting of the event’s social
goals and assigning schol arships, was compo sed of:
• Dr. Núri a Salán, Cha ir
• Dr. Anna Fe rré - Mateu
The Sponsor s Boar d , in charge of secur ing fundi ng through sponsors, taking care of their needs, and
maintai ning exter nal relations, was composed of:
• Mr. Gui llem Megias Homar, Chair
• Dr. David González
• Ms. Magd a Escor sa
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Awards
1 - Best Oral Pr esentation
Title: Dev elopment of a Low - Cost Ground Segment Capable o f Receivi ng Data f rom Nanosate llites : a
Partnershi p between Br azil and Portugal
Authors: J úlio Sant os, Jeremy Silva, J oí£o Braga, André Tei xeira, Mar cos Kakit ani and Hen rique
Alves
2 - Highly Commended Oral Presentat ion 1
Title: The effect of previou s spacefli ght on ot olith - mediate d ocul ar cou nter - roll in cosmon auts after
long dur ation spa ceflight
Authors: Ca tho Schoenmaeker s, Flori s Wuyts and Steven Ji llings
3 - Highly Commended Oral Present ation 2
Title: ASCen SIon Innovat ive Trai ning Networ k: mid - term overview and les sons learned
Authors: Al essia Gl oder, Mart in Tajmar and Chris tian Bach
4 - Best Poster
Title: Ana lysis of Impulsiv e and Low - Thrust Transfer Orbits for ESA's LIS A Mis sion under Third - Body
Perturbati ons
Authors: J uan Palomares , Oriol Lizandre and Blanca Tejedor
5 - Highly Commended Poster
Title: An Augmented Real ity App teaches vol cano monito ring fr om Space in Schools wi th Sentin el - 1
data
Authors: Cl audia Li nd ner, Christi an Nadolsky, Carsten Juergens, Karl - Heinz Ott o and Andrea s Rienow
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Table of Cont ents
PAPERS
Antoni Per ez - Poch et. al .:
Challenge - Based Learning and the Ba rcelona Zer oG Challeng e:
A Space Educat ion Case St udy .............................................................................................................. 3
Alba Badia Rifà et . al.:
Final test ing, pre - launch activities , launch and pos t - launch a nalysis o f a soun ding rock et mad e by
students in Spain ................................................................................................................................... 9
Davide Bel licoso:
A student perspective into ESA Academy Space Systems Engi neering Training Course ................... 15
Elke D'Huys et. al .:
Come fly wi th us: services provide d by the Space Weather EducationCe ntre ..................................... 18
Guill em Oliv ella, Marcel Mari n:
Design and implemen tation o f space e ducation al activities to mot ivate you ng stud ents in C atalonia . 23
Iván Serma noukian Mo lina et. al.:
Missio n anal ysis of nan osatel lite const ellat ions with Op enSatKi t ......................................................... 28
Josep Sit jar Suñer e t. al.:
Design and methodology for a Remot e Sensing course ...................................................................... 34
David Herna ndo - Diaz:
CANSAT Competiti on 2020: Best techn ical dev elopment by OrbiSat team ........................................ 38
Knight Tri stan et. al.:
TOLOSAT project: Gravimet ry and Communic ation ............................................................................ 43
Adrià Rovi ra - Garcia et. al.:
gLAB hands - on education on satell ite navigation ................................................................................ 48
Teresa Peña:
Analysis o f planet ary spacecra ft images with SPICE .......................................................................... 54
Melina Koukou et. al.:
SDR Helix An tenna Deplo yment Experi ment (SHADE) o n board BEXUS .......................................... 60
Hugues Sana, Clio Gie len:
The advanced Mast er of Spa ce Studies at KU Leuven and Ghent Uni versity:
Trends and t endencies i n the prog ram demographics ......................................................................... 66
Jordi Grau Rifà, ESEIAAT UPCSP Spain:
Design and optimizat ion of a rocket structu re foll owing the requiremen ts for the European Rocketry
Challenge (EUROC) to be fabrica ted using additi ve manufact uring .................................................... 72
Pablo Salga do Sánchez:
The “Effect of Marangon i convecti on on heat transfer in Phase Cha nge Material s” experiment , from a
student project to the International Space Station ............................................................................... 78
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Mark Wyl ie, Leonardo Bari laro:
An investi gation i nto cold weld adhes ion fo r spacecraft repair after a space debris impact u sing space
education based sub - orbital sounding rocket plat form ........................................................................ 84
Georgie Crewdso n et. al. :
Supporting an ISS expe riment as PhD students : a case study of the
PARTICLE VIBRATION pr oject ........................................................................................................... 90
Dr. Paul ILIFFE:
The Sat - Comms Game: t eaching a complex sub ject fo r inter discipl inary au diences . ......................... 96
C. J alba et. al. :
DEAR project : Lunar Dust Surfac e inter actions, Risk and Removal i nvestigat ions ........................... 101
Rosa Olive lla et. al.:
Monitor ing n atural phenome na fro m the classr oom wit h Edus at. Pr oposal for a teac hing g uide ( and
support materi al) ................................................................................................................................ 107
Radu - Andrei Ci oaca et. al.:
Testing campai gn for ECRIDA: the UV res in 3D prin ter flyi ng on REXUS ......................................... 113
Will iam C roft s et . al .:
Developing a 3U CubeSat Engineeri ng Model - FlatSat & Chassis Desi gn ....................................... 118
Sara Dall edonne et. al.:
Space Educati on in Eur ope: Statu s and Prospe cts) .......................................................................... 124
Joseph Mangan et. al.:
Experiences in Firmwar e Development for a CubeSat Inst rument Payl oad ...................................... 130
Federico Di Giacomo, Maura Sandri :
Educational activi ties wit h Arduino to lear n about a stronomy ............................................................ 136
Angel Porr as - Hermoso et. al .:
Design and calibra tion proc ess of s olar sen sors for small s atelli te missi ons ................................ ..... 141
Stefan Lobas et. al .:
Cosmic Call Tech – A hands - on space radio workshop for st udents in secondary educati on ............ 147
Jack Reilly et. al. :
EIRFLAT - 1: A FlatSat pl atform for the deve lopment and testing of the 2 U CubeSat EIRSAT -1 ........... 152
Jennifer Hoffmann et. al. :
Development of a Concur rent Engi neering T ut orial as part of t he “ESA_Lab@” initiative ...................... 158
Anita Alf ano et. al.:
Spazio all o Spazio ............................................................................................................................. 164
Marcel Stefk o et. al.:
SAR - An Augmented - Realit y App for Explorat ion of Principl es of Sy nthetic Aperture Ra dar ............. 170
Úrsula Mar tínez et . al.:
ATTITUDE CONTROL RESEARCH WITH EDUCATI ONAL NANOSATELLITES ............................ 174
Ernest Tort osa et. al.:
Progress of the Devel opment of a Two - Sta ge Supersonic Rocket within a
Student’s Associati on ......................................................................................................................... 180
Marcel Liegi bel et . al .:
Meteor observ ation with the SOURCE CubeSat – Develop ing a si mulation to test on - board meteor
detection algori thms ........................................................................................................................... 186
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Daniel Sch loms et. al.:
A Flexibl e CubeSat Edu cation Pl atform Combi ning Soft ware Develo pment and Har dware
Engineerin g ........................................................................................................................................ 192
Javier Cubas et. al.:
An example of Space Engi neering Edu cation i n Spain: a master i n space bas ed on Proj ect - Based
Learning (PBL) ................................................................................................................................... 198
Özlem Baş man Bari laro, Dr Ma rio C ardona
Potential applica tion of a measurement tool f or quali ty assuranc e of E - Learning conten t to a new
MSc in Aerospa ce Engi neeri ng ................................ .......................................................................... 204
Elena Álvar ez Castro et. al.:
Moon Rove r Chal lenge. An edu catio nal sp ace ro botics reso urce t o teac h prog ramming and pr omote
space careers at secondary educati on levels .................................................................................... 210
Johanna Mehringer et. al.:
Suborbital Autorot ation Landi ng Demonstr ator on REXUS 29 .......................................................... 216
Juan Bermejo - Ballesteros et. al.:
Mubody, an ast rodynami cs op en - source Python libr ary focused on librati on points .......................... 222
Adrián Mart ínez et. al .:
Further evi dence of t he long - term thermosph eric density varia tion using 1U C ubeSats ................... 228
Michael Halv orson et. al.:
A Model - Based Syst ems Engineeri ng Approach to Space Mi ssion Educa tion of a Geographi cally
Disperse Student Work force .............................................................................................................. 234
Jonas Jelonek et. al.:
BEXUS30 – ELFI: Measuri ng Schumann r esonances in the atmosp here ......................................... 24 0
Marcela Salaz ar et. al .:
Hypergravi ty induc es changes in physi ology, gene expres sion and e pigenetic s in ze brafish ........... 246
C.C. Lin et. al. :
Challenge of teachi ng complex, end - to - end space system design and development process: Eart h
Observat ion Sa telli te Sys tem Desi gn tr ainin g cour se ........................................................................ 252
Clémence Duboi s et. al .:
Blended - Learning Educati onal Concept for Eart h Observation at Univer sity Leve l ........................... 258
Kevin Waizene gger et. al .:
Development and Testi ng of the 3U+ Cube Sat PCDU for SOURCE ................................................ 264
V. Eschelmül ler et. al .:
Development of a CubeSat CLIMBing t o the Van - Allen belt .............................................................. 270
Maximil ian v on Arni m et. al.:
Improved S ensor Fusion for Flying Lapto p Based on a Multiplicative E KF ........................................ 276
Anton Atanaso v, Viktor Danchev:
Space Communicat ion System for Educati on .................................................................................... 282
Joost Vanreusel et. al. :
ESA Academy’s Or bit Your Thesis! Pr ogramme ............................................................................... 288
Maeve Doy le et. al .:
Update on t he status of the Educational Iris h Research Satelli te (EIRSAT - 1) .................................. 294
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Chantal Capp elletti et. al.:
Establishi ng Thriv ing Univer sity - Level Space Educati on ................................ ................................... 300
Natacha Cal lens et. al .:
The Student Aerospace Chal lenge: a Eu ropean multi discipli nary contest and tert iary educa tional
programme ......................................................................................................................................... 306
A. Camps:
UPC NanoSat - Lab - Past, Present and Future Act iviti es ................................................................... 312
Alejandro García et . al.:
Deployable Fresn el Zone Plate a ntenna for CubeSat s ............................................................. 318
Lana Laskey :
Space Games: Evalu ating Game - Based Vi rtual Reality in Higher Education .................................... 324
Dr. Sara Langston :
Space Educati on: Chall enges and St rategies in Teachi ng Space Pol icy to Techni cal Univers ity
Students ............................................................................................................................................. 330
Arias Hel ena et. al.:
Hypatia I : a mult i - generational and multi - disciplinar y crew of female analog astr onauts dedicated to
space research, scientific outreach, and promotion of female rol e models in space careers ............ 336
Alexis Leo n Delgado et . al.:
A multi - project student space associati on .......................................................................................... 342
Ota Mic halek et. al.:
Findings f rom the ESA Edu cation Fly a Rocket Campai gn – Sensor Experiments Te am .................. 3 48
Tony Erdmann, Mar a Krachten:
Lessons - learned from Te aching Satellite O perations in a No vel Hands - on Student Project Utilizing
In - Orbit Sp acecraf t Duri ng th e COVID - 19 Pandemic ......................................................................... 354
Alexander Ki nnaird et. al .:
A selecti on of l essons lear ned from ph ase C/D of CubeSat pro jects of the Fly Your Satellit e!
Programme ........................................................................................................................................ 360
Markus Grass et . al.:
The Space Stat ion Design Wo rksho p goe s di git al - opport unities and chall enges during pandemic -
times ................................................................................................................................................... 366
Frenea - Schmidt Ar melle et. al.:
From education al programmes t o professi onal proj ects: fi nding fl ight opportunities ......................... 372
Alexander Ki nnaird et. al.:
ESA Academy Acti vities during COVID - 19 ........................................................................................ 378
Claudia Guer ra et. al.:
Fly a Rocket ! ESA's hands - on programme for undergraduate st udents ............................................ 384
Laszlo Bacsardi, Laszlo Csurgai - Horvath:
Establishmen t of th e Spa ce Engineering Program in Hungary .......................................................... 390
Sahba El - Shawa et. al.:
JSRI Space Design Competitions: Education and Outreach for Emerging Space Countries ............ 395
Rovin Perez , Slavey a Abadzhieva :
Design Chal lenges, a nd Outcomes o f Building a Satelli te t he Size o f a Soda Can ........................... 401
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Apoorva Joshi et. al.:
AMORE - Mission concep t over view for a progr essive ly i ndepende nt and self - sustainable
lunar hábitat ....................................................................................................................................... 407
Lara Fernandez
Dep loyment m echanism for an L - Band Helix an tenna on - board the 3Cat -4 1U CubeSat ................. 413
Lorenzo Frezza et. al. :
Lessons learned during t he development of LEDSAT from the students of the S5Lab ..................... 418
Fe derico Toson et. al.:
O- ZONE: affordable strat ospheric air dynamic sampling device ....................................................... 424
Katarzyna Mal inowska, Michał Szwaj ewski :
The role of the key educational paths f or ESA new member states as a risk re duction i ndex for
the newcom ers. .................................................................................................................................. 430
Maur a Zara, Si fat Kaur Alag :
What T hey Want a nd Wha t Th ey Ne ed: T he Ne w Rol e of the Juri st in As sis ting the Young Spac e
Companies ................................................................................................ ......................................... 436
A. Perez - Portero et. al.:
RITA: A 1U multi - sensor Earth observation payload for t he AlainSa t-1 ............................................. 442
Charles Mwang i, Malki a Kelelu e :
Implementa tion of Space C l ubs in Kenya ................................................................ .......................... 446
Joseph Thompson et. al.:
Thermal Charact erization Testing of a Robust and Reliabl e Thermal Kni fe HDRM (Hold Down and
Release Mec hanism) for CubeSat Deploy ables ................................................................................. 452
Gisela Detrel l et. al.:
From Soyuz - docking manoeuvres to mi croalgae cultivat ion:
hands - on training for Master's students ............................................................................................. 458
Alessandro Bortotto et. al.:
ERMES: Design a nd preliminary simulat ions for an autono mous dock ing manoeu vre ..................... 464
Maria Alexand ra Nit a et. al.:
A story ab out how th e novel ROSPIN Academy progr amme is bri nging space education to the
Romanian yout h in th e pandemic c ontext ......................................................................................... .470
Francesco De Ceci o et. al.:
TEASPOON: a once i n a lif etime opport unity to Sedna ..................................................................... 476
Federico Basan a et. al.:
Development of a mult i - payload 2U CubeSat: t he Alba Project ........................................................ 482
Paolo Marzi oli et. al.:
From BEXUS to HEMERA: T he appl ication of l essons learned on the devel opment and
manufact uring of st ratos pheric payl oads at S5Lab ............................................................................ 488
Alondra Sol á Molina et. al.:
Asociación Aeroespacial Cosmos: edu cational impact and returns of a three - year - old student
aerospace association ....................................................................................................................... 494
Francesco Bian chi et. al. :
Collaborat ive Space Design pr oject: A student’ s experi ence ............................................................ 500
Chien Lin Soh et. al.:
Domi Inter Astra ( DIA) Moon Bas e: an i nterdisc iplinar y approach for c ooperation t o build
a near - future Moonb ase and how to use it as an educational too l .................................................... 506
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Laia Casamiquela et. al .:
Finestres a l cel .................................................................................................................................. .512
Léa Rouverand et. al.:
Experiment collabora tion prog ram during a Marti an analogue mission to introduce youn g students
to human sp ace exploratio n ............................................................................................................... 518
Arnau Torre nt et. al. :
Student perspective and l essons learned from par ticipating i n the European Rover Chall enge
2021 ................................................................................................................................................... 524
M. Badi a et. al .:
Montsec Ground Stati on .................................................................................................................... 529
Anastasios - Faid on Retselis et. al.:
Adaptation of the AcubeSAT nanosatel lite project into re mote working during the COVID - 19 era ........... 533
Fernando Amador Pla et. al.:
A multi - perspective comparison of ESA Academy’s Traini ng and Learni ng Programme experiences
before and throughout COVID - 19 pandemic through the eyes of 6 students ............................................. 539
Luis Cormier et. al .:
FlatSat Worksh ops Teaching F undamental Electronics Skil ls for CubeSat Buil ding ................................ . 545
Augustin Gal lois et. al.:
Lotus: Testing Origami - Inspired Structures in Micro gravity ............................................................... 551
Luis García Mozos et. al .:
Artery in Microgravity (AIM): Assembly, Integration, and Testing fo r a Student Payload for the ISS ......... 5 5 7
Oriel Marshal l et. al .:
Demonstrati ng Cosmologi cal and Doppler Reds hift i n the Cl assroom ........................................................ 563
Ana Gebejes et . al.:
Six - year evolution of a space - inspired collab orative p roblem - so lving study program in Finl and ............... 569
Albert Mor ea et. al.:
3 Cat - 4 Mission, 1 - Unit CubeSat for Earth Observ ation:
Evaluation on the q ualific ation and producti on during Phase D .................................................................. 575
Andy Chia et. al.:
Development of a Pro of - of - Conc ept Space Propulsio n System fo r Nanosatel lite appl ications using
Additive Manufacturi ng .................................................................................................................................. 581
Mario Andre Z uegner :
Ice Moon R esearch – A phenomenon cal led plume ..................................................................................... 587
Hendrik Kuh m et. al.:
Design and Development of the Re - Entry Sensor System for the CubeSat Mi ssion SOURCE ................ 593
Roger Macías et. al.:
3D printed telescopes: an interesting tool for teachi ng Astronomy, Sci ence and Te chnology .................. 599
Ferran Salaza r et. al.:
Simulatin g Atmospheric Turbulence : Code Devel opment and Ed ucational Applicat ions .......................... 605
Edwar , Shi ndi Marl ina Oktavi ani et. al. :
Development of Commercia l - Off - The - Shelf Imaging Payloa d for Cl oud Coverage Monitori ng ................. 611
Júlio Santos et. al. :
How to Manage a Rocket ry studen t projec t in f ull quar antine ..................................................................... 617
4 th Symposium on Space Educ ationa l Acti viti es
Barcelon a, Apr il 2 022
XXV
Wan Fa ris Aiza t Wan Aasi m et. al.:
The Structur al Analysi s of Alai nSat - 1: An Earth Observation 3U CubeSat ................................................ 623
Joseph E. G. Middleton et. al .:
Developing low - cost, reusable solar observation pla tforms to advan ce sustainable
heliophysics research ................................................................................................ ............... 629
Zaria Serfo ntein et. al .:
LEOniDAS Drag Sail Experiment on the 2021 ESA Fly Your Thesis!
Parabolic Flight Campaign ....................................................................................................................... 635
Andreas Wolni evik et. al.:
Lessons Learned when Developing a Hi gh Performance Attitude Cont rolled Platform to Achiev e
Microgr avit y for Low - Cost Ex periments ..................................................................................................... 6 41
Mark Ang elo C. Puri o et. al.:
On - boar d Image Classificati on Payload for a 3U CubeSat using Machine Learning for On - Orbit Cloud
Detection ........................................................................................................................................................ 6 47
Slaveya Abadzh ieva et. al.:
Universi ty of Not tingham St udent Space Activit ies to Enrich t he Traditional Cu rriculum ........................... 653
Stefanie Steinbach e t. al.:
Earth obser vation ed ucation f or Zero Hun ger:
A Massive Open Online Cou rse towards achievin g SDG #2 usi ng EO ............................................. 659
Esmée Menting et. al. :
Lessons learnt during the REXUS program on how to manage a st udent Project .................................... 665
Mateusz Zalas iewicz et. al.:
Flight Hard ware and Soft ware Operati ons Performance Review for BAMMsat - on - BEXUS – a BioCubeSat
Prototype Flown on BEXUS30 ....................................................................................................................... 671
Muhammad Sh adab Kha n et. al.:
Development and Fligh t Results of Tal Tech Univer sity Cu beSat Missi on ................................................... 677
Júlio Santos et. al .:
Development of a Low - Cost Ground Segment Capable of Receiv ing Data from Nano satellites: a
Partnershi p between Br azil and Portugal ..................................................................................................... 683
Thibault Gat eau et. al.:
Nanospace and Open - source Tools for CubeSat Preliminary Design:
Review and Pedagogical Use - case .............................................................................................................. 689
Riccardo Restivo Al essi et . al.:
D esigning Greenhouse Subsystems for a Lunar Mi ssion: Th e LOOPS - M Project .................................. 695
Robert Jef frey et. al .:
Teaching comput ational t hinking t o space sci ence student s ....................................................................... 701
Catho Schoenmaek ers et. al.:
The effect of spacef light on the otolith - mediated ocu lar c ounter - roll ........................................................... 707
Alejandro Sans Monguil ó et. al .:
Assessment of a machine - vision - assisted t est bed for spacecraf t ma gnetic clean lines s análisi s ............. 713
André Teixei ra et. al.:
Competitio n, Researc h and Ext ension: The three app roaches to the Popularization of Small Sat ellite s
in the Alt o Parao peba re gion in B razil. ......................................................................................................... 719
4 th Sympo si um o n Space Edu cational A ctiv ities
Barcelona, April 20 22
Page 2 of 6
Acro nyms/ A bbreviations
CNES Cent re Nat ional d ’Études Spatia les
EASA Eur ope a n Aviat ion Safety Agenc y
ESA Europ ean S pace Age ncy
HEI Higher Educ ation Ins titute
IAF Interna tio na l Ast ro nautic al Feder ation
ISU Interna tiona l S pace U niver s ity
SSP Summer Space Pro gram
SEMA Spa nish Soc iety of Aer ospa c e Medic ine
SGAC Space G ener at ion Advisor y Counc il
ST EAM Scienc e, Tec hno logy, Engin eerin g,
Arts and Mathemat ics
UPC Univ er sit a t P olitèc n ica d e Catal unya
VFR Vis ua l F lig ht R eg ula tio n s
1. Introduc tion
Parabol ic f lights h ave be en conduc ted f or a long
tim e as a wa y of perf orm ing shor t - tim e dur atio n
experim ents and t ec hnic al dem ons tratio ns [1 ,
2]. Airc raf t parabo lic f light s provide up t o 25
seconds of reduced gr avi t y . T h e y are used f or
conduct ing shor t invest igat ions in Ph ysica l and
Life Sci ences , both f or s enior res earc hers a n d
for intern ationa l stu den t ex perim entat ion a nd
m otivation, and pub lic outre ac h.
W e repor t on educat ional ex per im ents
conduct ed in the Barcel o na parab olic flight
platfor m (Sabad ell Airport , Barc elon a, Spa in)
with s ingle - e ngi ne aer obat i c airc raf t suc h as the
CAP1 0B ( Figur e 1), ac hieving u p to 8.5
seconds of m icr ogravity in its cock pit.
T he flight prof ile res ults co m ing from a s teady
flight prof ile an introd uc tor y pull - up m aneuv er is
perf orm ed at inc reas ed ac c elerat ion ( rou ghl y 3 -
3.5g for these airc raf t), pilo t r educes thrust and,
with thr ott le or i dle e ngi nes the airpla ne f ollo ws
the par abol ic tr ajec tor y of a f ree - f lying bo dy. As
a conseq ue nce, af ter a shor t p hase of
transiti on, m ic rograv ity is obta ine d for 5 - 8
seconds .
After the reco ver y mane uver a t incr eas ed
acceler ation ( 2.5 - 3g) , th e airplan e f lies agai n
horizont all y to the gro un d lev el for s om e
m inutes bef ore in troduc ing the next p arabo la.
Durin g one f light m ission t ypi ca ll y 10 - 15
parab olas are per form ed. Lar ger airc raf t
provide be twee n 2 0- 25 s econds of m icrogravit y
thank s to a m ore powerf ul eng ine.
T he European Space Ag enc y ( ESA ) h as used
since 1 98 4 six t ypes of airc raf t to c onduc t its
parab olic f light cam paigns [3]: the KC - 135, the
Carav elle f rom C NES, the Russ ian Il yush in Il -
76 MDK, th e Ces sna Cit ation II, t he A irbus A -
300/A - 31 0 ' zero - g' f rom Nov es pace , a ll of them
with 2 or 4 engin es. An im portant num ber of
physic al an d lif e s ciences ex perim ent s ha ve
been co nducte d sho wing the suc ces s of this
k ind of ac ces s to m icr ogravit y.
Our appr oac h is diff erent f rom the s ucc essf ull y
previous l y r epor ted par ab olic flights as we
propose the us e of a sm all single - engine
aerob atic pl ane. T his k ind of airc raf t (Figur e 1)
is cer tifie d t o co nduct th is m anoe uvr e a nd c ould
also be us ed f or pr of ess ional experim ents,
testin g tech no log y and educ atio na l an d
outreach c am paig ns as wel l. H ypogr avit y is
exper ie nced with in the c ock pit for about 8
seconds with a flight prof ile sig nificant l y
diff erent f rom that of larger airc raf t [4] .
Figure 1 . Mudry CAP10B aerobatic aircraft u sed
for educat ional p arabo lic fli ght campaign s.
(Credit : Bar celona - Sab a dell A viation Club)
Parabol ic f lights ha ve been us ed ver y
succ essf ully b y the space agenc ies to cond uct
student c am paigns with the aim to m otivate the
youth to tak e part i n a ero naut ical and spac e
resear ch. T his projec t is inspir ed b y the ES A
Aca dem y hands - on e ducat iona l pr ojec ts and , in
particu lar, b y the very succe ssf ul ESA F l y Yo ur
T hesis Pr ogram [5 ].
2. Object i ves
T he objec tives of par ab olic f lights wit h a n
aerob atic si ngle - en gin e air c raf t are as f ollo ws
[4, 6 ]:
2.1. Sc ientific & Res ear ch
- T o stud y differ ent proc es ses in whic h abr upt
changes of gra vit y work load are app lied. In
particu lar h y p er ( 3 – 3. 5g) to h ypograv it y
(0.05g), and h ypo to h y p er grav ity per iods.
4
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4 th Sympo si um o n Space Edu cational A ctiv ities
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- T o analyse trans ien t phenom ena that m a y
occur af ter shor t periods of h y p er an d
hy pogr avity .
- T o allow exp erim ents for testing t he e quipm ent
in a real para bo lic f light, with t he op portun it y to
m anuall y int eract w ith the equ ipm ent and
provide a proof - of - c oncept bef or e acces sin g
other m ic rogravi ty r esearc h platf orm s.
- If the ex perim ent can be r un in less than 8
seconds of expos ure to hypo grav it y, and t he
residua l acc elerat ion of 0.05 g is accept abl e,
then qua nti tativ e and q ua litati ve m easur em ents
can b e m ade, t hus prov idi ng m eani ngful dat a.
T he parabo lic fl ight can prov ide u p to 20
para b olas in a s ingle f light , and weather
perm itting t he pr ocedur e c an be r epeat ed i n a
single d a y.
- In regards to h um an ph ysiolog y or ph y s ical
experim ents in which a nd the h ypo and
hypergr avit y en viro nm ent pla ys a role, t he
fac ilit y enables dif fer ent experim e nts to be
tested ins ide th e coc k pit, o ne b y on e on board
(Figure 2) . More i nform ation can be f ound at our
laborator y website ( C Sm icrogLab.u pc.edu )
Figure 2 . Human re producti on studies
conduct ed in t his platfor m [7 ]. (Credit: Institut
Dexeu s, UPC & Ba rcelona - Sabadel l Av . Club)
2.2. T ec hnologic al
- Asses sm ent of technolo gica l equipm ent
behav iour in a hyper and h ypogr avit y
environm ent with abrupt c hanges in a tin y
environm ent.
- Safet y ass essm ent of exper im ents and
techno logic al dem ons tratio ns w ithin a par abol ic
flight aircr aft cock pit.
- T raining of wann abe or f uture astr onauts f or
for eseen pri vat e or p ublic s pace m iss ions.
2.3. Educ ati o n & Outreac h
- Allow ing st udents to conduc t han ds - on
experim ents in a re al weight less ness
experie nce.
- Increas ing the ir int eres t for stud ying Sc ienc e,
T echnolog y, Eng ineeri ng , Arts and
Mathem atics (ST E A M) s yll abus, in par ticu lar in
the aer ospac e fie ld.
- Provid ing s tu dents fr om diff erent ba c k grounds
and natio na lities with the oppor tun it y of work ing
as a te am with a c omm on goal, while i nteract in g
with sp ace pr ofes sion als.
- Raisin g pub lic i nterest in s pac e resear ch.
- Creat ing th e oppor tun it y for stud ents to wr ite
and pr esen t t heir s pace r es earch in rele vant
journals and c ongress es, and also to f urth er
appl y to the s pace ag encies e duc ation al
program s building up the ir cur riculum .
3. Chall enge- B ased L earnin g
Challe nge - Based Lear ining (CBL) is a ST EAM
Educat ion m et hodolog y that has been r ecent l y
introduc ed as a c o llabor a tive an d hands - on
appro ach to enc our age s tuden ts to put t he ir
k nowledge in pr act ice b y address ing r eal - lif e
problem s. In 2008, the c o ncept C BL was f irs t
nam ed b y the techn ol og y ent erpris e A pp le® as
a m ethodo log y to m e et the XX Ist C ent ur y
dem ands [8 ] . Higher Educ ation Ins titutio ns
(HEIs) have s een in the re c ent years ho w their
role had to ad apt i tself to th e arisin g chang es in
our societ y and in pa rtic u lar, ST EA M
Univers ities [9]. O ur c olle ges ar e becom ing
fac ilitators f or the st uden ts’ train ing, incl uding in
their s yllabus c om petenc ies (s uch as team work,
creativ it y or inn ovati on sk ills) to be ac quir ed,
which ar e requ ired in n o wada ys’ sci entif ic
endeav ours . Spac e Edu cation is a fie ld
particu larl y suited t o ap pl y CBL, w ith han ds - on
res ear ch pr ojec ts req uiri ng s tud ents t o work
with te am m ates , ment ors and exper ts. T he y ar e
expect ed to tak e ac tions an d c omm unicate their
eff orts in a m ulticultural, i nter nation al s cenar io
in order to pr oduc e an optim al response a
specif ic goa l.
W e her ein prese nt a succ ess f ul CBL Cas e
Stud y which invo lves des igning, im plem enting,
and ac tual ly f l ying a m icr ogravit y exper im ent in
parab olic f light .
4. T he Barcel on a Z eroG C ha llenge
T he Barcelon a ZeroG C hallen ge is an
internat ion al c om petitio n ad dres sed t o
Uni ve r sit y stude nts worldwide (F igur e 3) . It
requires the st udents to b uil d a te am with a
m entor, pr opose, d esig n, build and fl y th eir
experim ent in m icr ogravit y and fina ll y anal y ze
the resu lts an d c omm unicate their find ings.
5
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Figure 3 . Barcel ona ZeroG Challenge
announceme nt. (Cre dit : S GAC )
T he experim ent has to m eet t he r equ irem ents
of a par tic ular platf orm of micrograv it y rese arch
availab le in Barc elona f or educ a tion al and
resear ch pur pos es [10 ] .
More t han f if ty stud ents h ave a lread y f lo wn t heir
experim ents on bo ard an aero bat ic C AP10 B
aircr aft in Barcel ona in p revious e ducat iona l
cam paigns; havi ng pub lis hed t heir r esul ts in
relevant s y m posi um s and sc ientif ic j ournals [4] .
T hese cam paigns, insp ired b y the wel l - k nown
ESA Stude nt’s P arabo l ic Fligh t cam paigns ,
have at trac ted m edia attent ion and h ave
prom oted pub lic a warenes s on ST EAM st udies
as wel l. Four pr ev ious e diti ons of the B arcelon a
ZeroG Challe ng e have t ak en plac e sinc e 201 0 ,
with a si gnif icant num ber of the Inter nat iona l
S pace U n iv ers it y (I SU ) st u dents b ei ng in volved
[11 , 12 , 13 , 14, 15 ]. T hree work shops had b een
held in th e Summ er Space Progr am and in th e
Master S pace Progr am of ISU. A new ed it ion of
this contes t is und er way [10 ], with the winner s
ex pect ed to f l y their ex per im ent in 2022. T his
editio n is organi zed by U niv er sit at P olit èc nic a
de C a talun ya (U PC), t he Barcel ona - Sabade ll
Aviation C lub and SG AC, t he Space Gen erat io n
Advisor y Counc il well - k nown stud ents
assoc iation. Mu lti disci plin ar , d iver se an d
m inor it y team s of students were enc o urag ed to
appl y. An i ndep en dent panel of experts fr om the
European S pace Agenc y (E SA) Aca dem y
conduct ed the fin al se lec tion of the winner
team . In the c urrent ed iti on, the s electe d
students ’ t eam r eceives a 2500 eur os gr ant to
devel op its exper im ent, as we ll as the
opport unit y to fly it in parab olic flig ht. A n
unprece dent num ber of 15 pr oposa ls ha ve been
receiv ed. St ude nts f rom 2 3 dif f erent countr ies
subm itted th eir prop os als ( 60% lif e sc iences
experim ents; 40% ph ysic al s cie nces) . Am ong
the partic ipa nts 6 3.3% c ame f rom Europe,
14.3% fr om Am erica and 1 3.4% f rom As ia. T he
winner team c onsists of four fem ale student s
fr om the U nivers ity of Antioq uia: Lu isa
Fernand a Me ndoza (s pok es person) , Paul ina
Quint ero, Or ian a Mejía and Mar ía d el P ilar
Monsa lve. T he team is called ‘Vera G rav itas’,
which in La tin m eans ‘true gravit y ’ , a nd it a ls o
ref ers as well to Dr. Ver a Ru bin, a f am ous
astronom er who m ade im portant c ont ributi ons
to sc ience [16] . T he y ar e par t of the Co lom bia n
Assoc iation of W o m en in Aerospace , which
aim s to ar i se wom en' s inte rest in th is s cience.
T he team also has a m ent or, Prof es sor Lil iana
Marcela Bust am ante G oe z, from the
Departm ent of Mecha nica l Engin eering at th e
Univers it y of Antioqu ia (F igure 4 ). T heir
propose d ex per im ent is en titled "De posit io n of
tin d r ople ts on elec tro nic com ponents i n the
absence of grav ity."
Figure 4 . ‘ Vera G ravitas ’ Team, w inners of the
Barcelona Z eroG Chall enge 2021.
T he experim ent seeks to stud y how sol deri ng
electron ic c om ponents is aff ected b y
m icrogravi ty, a res earc h t opic th at m a y have
m an y app lic ations in the near f uture. Cur rent l y,
this te am is work ing with t he advic e of
resear cher s f rom UPC and experie nced pi lots
fr om the Bar celon a - Sabad ell Aerocl ub in order
to devel op their exper im ent, ada pt it to the
cock pit of the p lane a nd f l y it th is year 20 22 at
Sabade ll A irport. T he t eam is also en gaged i n
an outr each proj ect to d iff use the ir find in gs [1 7 ].
Further m ore, s tudents f r om our o wn Un iver sit y,
have also the opp ortun it y of des igning and
testi ng t he ir exp er im ents durin g t heir s tu dies
with a s ingu lar han ds - on tr aini ng and a n
i ntroduc tion to s pac e res e arch [4, 11]. Mas ter
and Doc tora l T hesis are good f ram eworks to
include s tud ents’ a dvanc es and contr ibute to
their gr adu ation wit h a si ngular ex p er ie nce.
5. Discus si on
W e first reported a su c ces sful ser ies of
parab olas perf orm ed wi th a lig ht sin gle - engine
aerob atic plane with a l ife s cienc es ex per im ent
on boar d. Between 5 to 8.5 s econds of
m icrogravi ty wer e achiev ed with a lim ited
operat ional cos t. T he opt im ization of the m anual
piloting has m ade possib le to pro vide a qua lit y
of g b et ween 0.05g an d 0. 005g with a g j itter
reductio n depend ing on t he st ren gth of win d
6
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4 th Sympo si um o n Space Edu cational A ctiv ities
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gusts . Ver y lim ited tim e is ne ede d to pr epare
and pe rf orm the exp erim ent so this appr oach is
specif icall y su ited for t hos e k ind of r apid
protot yping techn olog y tes ts, or sim ple
experim ents that do not need hug e or
sophist icated e quipm ents. T hese par abo lic
flights ar e not des igned to com pete with those
f r om space agenc ies requ iring larg er airc raf t,
instea d, the y r ather ext end t he ra nge of
possibi lities a vail able to the r ese arc hers and
students inter es ted in m icrogravit y rese arch.
Am ong the lim itations of sm all aerob atic a irc raf t
are: lim ited cock pit s ize, red uc ed hypo grav it y
tim e, no electr icit y p lugs availab le, onl y one
experim enter at a s ingle f light, higher g j itter
sensiti vit y and a m or e aggr ess ive f light prof ile.
Howe ver, f r om the po int of vie w of pr ovid ing a
hands - o n exper ienc e to stu dents it h as pr oven
very s ucc essf ul at a reas o nabl e cos t.
Educat iona l acti vities ha ve been f rom the
beginn ing an ess ent ial par t of our m otivation,
and ha ve pro vide d m eani ngful r esul ts and a
num ber of f light oppor tu nit ies f or st udents ’
experim ents, as well as tutori als af ter d at a
colle ct ion .
Only t wo m ild episodes of motio n sic k ness have
been r eport ed in m ore than 10 years of
educti onal ac tiv ities. The vis ual f light
conf igurat ion of th is p latf orm allows th e
partici pant an y inconven ien ce durin g the f light ,
and foll owing t he pre - es t abli shed prot oc ol, he or
she woul d be safel y held on ground i n less than
15 m inutes with s peci ali zed m edical car e
availab le on site. Mand ator y safet y brief ings are
conduct ed pr e and post - f ligh t.
Students ’ as soc iations s u ch as the Spac e
Generat ion Adv isor y Co uncil ( SG AC), are
curr entl y invol ved in this e ndea vour. Som e of
the pr ior p artici pant s h ave dec lared the ir
excitem ent for hav ing t he o pportu nit y of ac tua ll y
m aking s pace r ese arch in m ic rogravit y,
provid ing outr each t o th e pub lic, and l ater
pub lish ing th e res ults in s elected c onfer ences
and ind exed j our nals.
T hree ke y factor s to s ucc ess have bee n
ide ntif ie d f r om our years of experienc e: 1 - A
s trong inv olvem ent of stude nts ' ass ociati ons, 2 -
Interna tiona l cooper atio n and 3 - Q ua lit y o f
students ' m entor ing.
Space stu den ts as soc iatio ns are one of the
m ost valuab le as sets in th e astr onautic al f ield t o
prom ote m otivation, m entori ng and a
m eaningf ul career for their m em bers . The y
spread th e word of the opport uni ties t hat
eventu all y arise, and pr ovide an im po r tant
contac ts net work which ar e ess ential to bu ild up
a divers e team such as that req uested in th is
singu lar cha lleng e. Int ern ationa l coop erat ion
involves m aking us e of t he prof ess ional
societi es s uch as IAF to r eac h the nec ess ar y
stak eholders f or star ting and m antaining an
educat ional en dea vour.
Last bu t no t leas t, in t he cas es that a high l y
involve d m entor was engag ed with thei r
students pr ojec t, ther e was a un ique bo os t to
the qual it y of their res ea rch pr oduct. S om e
m entors even att end ed all briefings , supervise d
the experim ent in a particul ar fiel d in which the y
were rec ogn ized ex perts a nd resear chers , an d
contribu ted subs tant iall y t o the suc ces s of t heir
students .
6. Conclu sions
W e have reporte d on th e educat io nal an d
outreach ac tiv ities of an inn ova tive m ic rograv it y
platfor m based on s ingl e - engine aer obatic
planes in Barce lon a ( Spai n) which is o ngo ing,
m aking a s ignif icant im pact a nd insp iring
students ar ound th e world t o get an int eres t on
space m edicine and r ese arc h. T heref ore, we
plan to c onti nue these activ ities an d ex pan d
them in t he near f utur e. Am ong the les sons
learned, t he s tuden ts ’ in volvem ent a nd
internat ion al co operat ion h ave been th e m os t
im portant f act ors that ha ve le d t his p latfor m
succ essf ul. Goo d m entor ing is a k e y factor f or
th e succ ess of stude nts i nvol ved in com plex
Challe nge - Based Lear ning act ivities .
Ackno w ledgements
Man y peopl e have contr ibut ed over t he y e ars to
these B arcelo na para bo lic flights w ith sing le -
engine aero bat ic aircr af t. In par ticu lar, we w ish
to thank our colleag ues f rom the Barcelo na -
Sabade ll A viati on Clu b and thos e flig ht
surgeons f rom the Spanish Soc i e t y of
Aerospac e M edic ine ( S EMA ) w ho have
volunt eere d contr ibut ing to the s af ety of
operat ions . W e are lik ewise gratef u l to al l th e
students and f light part ic ipants a nd the ir
m entors for their s upport a nd contr ibut ion, a nd
also to SG AC and E SA Academ y for their
curr ent inv olvem ent and supp ort. Pr evi ous
partici pat ion of som e of the a uthor s in ES A
hands - o n educ at ional acti vities ha ve bee n a
great sour ce of inspir ation.
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4 th Sympo si um o n Space Edu cational A ctiv ities
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Page 6 of 6
Referen ces
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Friedric h, J. C ler vo y , T. G harib, F. G ai, O .
Minster a nd P. Sundb la d, “T he Fir st J oint
European P artia l - G P ar abolic F lig ht
Cam paign at Moon a nd Mars G ravi t y
Leve ls f or Sc ienc e and Explor ati on”
, Micrograv ity Sc ienc e and Tec hnology ,
24 (6), 3 83 - 3 95 (20 12).
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Clervo y, T . Ghar ib, F. G ai and C. Mor a,
“Europe an par abolic f ligh t cam paigns
with Airbus zero - g: Look in g back at the
A300 a nd look ing f orwar d to th e A310.”
Advances in Space Resear ch , 56 ( 2015 )
1003 - 1013.
[3] V. Pletser, “ Short dur ation m ic rogravit y
experim ents in ph y s ica l an d lif e sc iences
during par abo lic f lights : th e f irs t 30 ESA
cam paigns”, Acta Astr onau tic a , 55 (1 0),
829 - 854 ( 2004) .
[4] A.Pe re z - Poch, D.V . Gon z ález and D .
López, “H ypogra vit y re searc h an d
educat ional para bo l ic fl ight act ivit ies in
Barcel ona: a n e w hub of innov ation in
Europe” , Mic r ogr av ity Scienc e an d
Technol ogy . ( 2016) do i: 10. 1007 /s122 17 -
016 - 9516 - 7 .
[5] N. Calle ns, L. Ha and P. Gal eone .
“ Benefits of ESA G ra vit y -R elated H ands -
on P rogr am m es f or U nivers ity St udents ’
Careers .” Microgr avity Scienc e a n d
Technol ogy , 28, 5 19 - 527 (201 6) doi:
10.1007/s 1 2217 - 01 6 - 950 5 - x
[6 ] M. Brigos, A. Pere z - Poc h, F . Alpist e, J .
T orner, “ Parabolic flights with s ingl e -
engine a eroba tic airc raf t: f light prof ile an d
a com puter s im ulator f or its optimi zation”,
Microgr avi ty Scienc e and T ec hno logy , 26
(4) 229 - 2 39, (2 014).
[7] M. Boada , A. Pere z - Poch , M. Ball ester ,
S. Garc ía - Mo nclús, D .V. Gon zález , S.
Garc ía , P.N. Barri , A. Ve iga ,
“ Microgr avit y eff ects on f ro zen hum an
sperm samples . ”, Journa l of Assis ted
Reprod uctio n and Ge netic s , 37, 2249 -
2257 ( 2020) .
[8] M. Nic hols , and K. C ator , “ Chall enge -
Based Lear ning ” W hite paper . A pp le, Inc .
(2008).
[9] UNESCO . Re th ink ing E du cation . ISB N
978 - 92 -3 - 100088 - 1 (20 15) .
[1 0] The Bar celo na Zer oG C hall enge 2 021,
http:// windo w2th eun ivers e.or g ( las t
acces sed 3 - 202 2 ).
[11 ] M. Azem à, “ Stud y of the fus ed deposi tion
m odeling beh avior u nder m icr ogravit y
condit ions ”, Master Thes is , Univers it at
Politècn ica de C ata lun ya (2 014).
[12 ] H. Allawa y, A. Melynsh yn, A. Kindrat, J.
Muller, A. Pere z - Poc h, D.V. Go nz ález, R.
T hirsk and G. Clém ent, “Per cept ion of
am biguous im ages on weightle ssness” .
Proceed ings of t he ELG RA Symp osiu m ,
Antwer p (20 11).
[13 ] G. Clém ent, H. Alla wa y, M. Dem el, A.
Golem is , A. Ki ndr at, A. M elin y sh yn, T .
Merali an d R. T hirsk , “Long dur atio n
spacef light incre ases dept h am biguity of
reversib le per spec tive figur es ”, P los On e
10(7): e01 323 17 (2 015), doi:
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[14 ] J.R. O sbor ne, M.A. Alo nsopére z, D .
Ferr er, N. G os wam i, D.V. Gon zález, M.
Moser, V. Gr ot e, G. G arc ía - Cuadr ad o
and A. Pe re z - Poch, “Eff ec t of Menta l
Arithm etic on he art rate res ponses duri ng
Parabol ic F lights: t he Barc elona Zero - G
Challe nge”. Microgr av ity Science an d
Technol ogy , 26 (1), 11 - 16 ( 2014).
[1 5 ] A. Schuster , V. Bocc ia, A . Perez - Poch
and , D. V. G onzá lez, “E st im ation of
relativ e dista nce bet wee n two obj ects i n
m icrogravi ty c onditi ons d ur ing par abo lic
flig ht” , Proceed ings of the Elgr a
Sympos ium . Corf ú, Gr eece (2015) . E lgr a
News 31, p.1 65 (2 015).
[1 6 ] Vera Gra vitas T eam ( in Spanish)
https:// www . youtube. com /watch? v= yoP0
9O3gs58 (last ac ces sed: 3 - 2022).
[17 ] Vera C ooper Ru bin. Sm iths onian
Nationa l Air and Spac e Muse um .
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learn/t opic s/ wom en - in - aviat ion/ru bin.c fm
(la st accessed : 3- 2 022).
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th Symposium on Space Educational Activities
Barcelona, April 2022
Final testing, pre-launch activities, launch and post-launch analysis
of a sounding rocket made by students in Spain
Alba Badia Rifà , Daniel Cantos Gálvez , Adam El Ghaib Bougrine
2
, Javier Hidalgo Marí
2
,
1 2
Marc Martí Arasa
2
, Arnau Pena Sapena
2
________________________________________________________________________
Abstract
This paper summarizes the final launch preparation tests, the operations before, during, and
after the launch, and the results of the launch of a supersonic sounding rocket developed by
university students in Spain with the collaboration of INT A (National Institute of Aerospace
T echnology). The students are part of the Cosmic Research association, based at the
Polytechnic University of Catalonia ESEIAA T , and the rocket is called Bondar . INT A is a
Public Research Organization under the Spanish Ministry of Defense dedicated to scientific
research and development of systems and prototypes in the fields of aeronautics, space,
hydrodynamics, security , and defense. The staff of the El Arenosillo Experimentation Center
(CEDEA) collaborated in the Bondar mission with their knowledge and launch capabilities.
The launch of the rocket took place on the 30
th of November of 2021. T wo students from
BiSky , a rocketry team from the University of the Basque Country , also participated in this
project, specifically in the development of the on-board and ground-based avionics
subsystems. The paper presents information on the mission systems, the operations before,
during, and after the countdown to the launch, the documentation required by INT A-CEDEA
for the launch, and the results of said launch. In short, the systems developed by Cosmic
Research for the launch are: the rocket, the launch pad, the rocket transport box, the flight
simulator , and the ground-based rocket tracking station. The documentation required by INT A
includes: a detailed description of the systems, a ground risk assessment, a flight risk
assessment, structural analysis, aerodynamic analysis, and a list of countdown operations.
Launch post-analysis activities evaluate the performance of systems and operations during
the most critical phase of the mission. The Bondar Mission, due to its technical and
operational complexity , was the most ambitious project ever developed by students in Spain
in the field of rocketry . After a successful launch, Bondar became the highest-flying Spanish
student-made rocket, with its apogee around 8 km AGL (Above Ground Level).
Keywords
INT A, launch operations, sounding rocket, Spain, students.
______________________________________________________________________
2 Cosmic Research, Spain
1 Cosmic Research, Spain, [email protected]
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th Symposium on Space Educational Activities
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Acronyms/Abbreviations
CEDEA Centro de Experimentación De El
Arenosillo
CR Cosmic Research
ESEIAA T Escola Superior d’Enginyeria
Industrial, Aeronàutica i Audiovisual
de T errassa
INT A Instituto Nacional de Técnica
Aeroespacial
1. Introduction
CR (Cosmic Research) is a student
association founded in 2016 with the mission
of launching suborbital rockets for the benefit
of society . Since its foundation, the CR’s team
has launched 37 rockets and more than 100
CanSats. With the launch of Resnik in 2017,
the association set the Spanish altitude record
at student level, achieving an apogee of 2 km.
Following its trail, the Bondar mission was
started in 2020, whose goal was to develop all
the technologies necessary to launch a
stratospheric rocket. This paper aims to give
an overview of the steps followed up to the end
of the launch campaign.
2. Mission Systems
2.1. Rocket
Bondar is a 2.6 m long, passively stabilized,
supersonic, aluminum rocket. It is fitted with
custom avionics for apogee detection and
separation, and data downlink. It is a sounding
rocket with payload capabilities up to 0.5 kg.
Figure 1. Bondar rocket
2.2. Launchpad
Horizontally-stabilized structure with variable
elevation angle. It is formed by a six meters tall
tower and rail to provide mechanical guidance
for the rocket during lift of f.
Figure 2. Launchpad
2.3. Rocket transport box
A 2895 x 580 x 690 mm wooden box filled with
custom antistatic and antivibration foams fitting
the rocket shape that prevents it from sliding to
ensure safe transportation during operations.
Figure 3. Rocket transport box
2.4. Flight Simulator
CR’ s own simulator is a 6-Degrees of Freedom
stochastic simulator based on MA TLAB, which
uses semi-empirical aerodynamic models to
predict the rocket trajectory .
2.5. Ground-based rocket tracking
station
T wo antennas were installed on CEDEA ’s
optronic systems to process the in-flight
telemetry data by a custom made ground
tracking station and send this information to
the control center .
3. Operations
In this section, the operations before, during,
and after the countdown will be presented.
These operations start with the review after
transport of all the systems of the mission and
end once the team arrives at the headquarters
after the launch.
3.1. Pre-launch operations
This group is the most extensive. It comprises
activities before arriving at CEDEA and also
operations in the spaceport.
First of all, there is a review of all the mission
systems. When all the systems are checked,
the launch campaign officially starts. This is
followed by the sorting and packing of all the
components. Then the team proceeds to the
transportation. Once in the spaceport, there is
the assembly of all the systems, with the
exception of the motor , the electronics bay and
the recovery bay of the rocket, which are
reserved for the launch operations.
During this phase, 3 tests were conducted. The
verification of the data reception regarding the
avionics and the ground stations, the data
injection verification and a launch operations
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th Symposium on Space Educational Activities
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simulation. When all the tests were passed, the
last step was the flight trajectory simulations.
3.2. Launch operations
The launch operations start with the motor
assembly and end when the motor is ignited.
The most critical operations are reserved for
this period. In short, these activities are, in
chronological order: the assembly of the motor ,
the final assembly of the recovery bay and
electronic bay with the rocket structure, the
introduction of the motor inside the rocket, the
transportation and placement of the rocket in
the launchpad, the final avionics tests and
simulations, the introduction of the ignitor , the
final security checks regarding the drop area
security footprint of the spaceport, and the
ignition of the motor .
Since this group includes the most critical
operations, it was necessary to detail also the
holding operations, the GO/NO-GO criteria and
the emergency procedures.
The holding operations comprise all the
procedures that solve a possible problem
during the countdown. Their importance
derives from the necessity of knowing in each
moment how to solve a problem, given the
tension of the countdown period. Also, it is
extremely important to know how much time it
can take to solve a problem in order to decide
whether the launch operations should be
postponed until the next launch window or not.
The GO/NO-GO criteria includes all the
conditions that must be met in order to
authorize the start of the launch operations.
Some examples are: to not surpass the wind
limits defined by the simulations, to have
favorable weather conditions, to have all the
systems ready and all the flight permissions.
The emergency procedures include the
instructions to follow if one or more of the
potential risks of the launch operations occur .
All the team members must be familiarized
with these protocols and must have a copy
with them.
3.3. Post-launch operations
These operations start once the motor is
ignited and finish when the team arrives at the
headquarters. They are divided into two
groups: the post-launch operations at the
spaceport and the post-launch operations
outside of it.
The post-launch operations at the spaceport
start with the lift of f of the rocket. It leaves the
launchpad at an approximate velocity of 40
m/s. The powered flight lasts 6 seconds, in
which the motor burns all its propellant. Then,
the motor runs out of propellant and it
continues its ascent for approximately 30
seconds. Once the rocket reaches the apogee,
the avionics command the separation of the
recovery bay from the avionics bay and the
drogue parachute is released. At the same
time, the motor bay and the recovery bay are
discarded into the sea. The upper stage
descends at an approximate velocity of 17 m/s
for 8 minutes and then it is recovered from the
sea.
Figure 4. Post-launch operations
Once the avionics bay is recovered, the
electronics team proceeds to recover all the
electronic components and the SD card. They
return to the spaceport and the team starts
sorting and packing all the systems. Finally , the
team proceeds to the transportation of all the
material to the headquarters.
4. Documentation
The safety requirements set by the launch site
demanded the production of various
documents to ensure system integrity and
operational safety before, during and after the
launch.
4.1. System description
T o better understand the Bondar rocket and
serve as reference, a detailed description of all
the components of each system was provided,
including dimensions, materials, and other
complementary information.
4.2. Ground Risk Assessment
For security reasons all risks that might
interfere with the mission were identified,
assessed, and classified. The risks were
evaluated taking into account severity and
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frequency , following a method proposed by
INT A [1][2], to ascertain their criticality . These
values were used to determine if mitigation
strategies were necessary to reduce their
criticality to an acceptable level.
The estimations were based on CR’ s previous
work and other reliable documents. T o ensure
quality the document was reviewed by both
INT A and ASPY , a risk prevention company .
4.3. Flight Risk Assessment
Following the same line of work as the ground
risk assessment, this document compiles all
the risks associated with the flight of the
rocket.
It includes, but is not limited to: motor
explosion, premature separation of recovery
devices, structural failure (specially the fins
and their supports), pitch-roll coupling, high roll
rates, and aeroelastic phenomena.
CR’ s simulator was used to study some of
these risks and propose adequate mitigation
measures, but literature was also consulted for
certain cases.
4.4. Structural Analysis
For both the rocket and the launchpad a FMEA
(Failure Mode and Ef fect Analysis) study was
carried out, identifying the most critical failure
modes and how to prevent them. For those
failure modes related to mechanical overload,
a FEA (Finite Element Analysis) was
performed. The position and magnitude of the
loads experienced in-flight for specific
structural parts were determined with simulator
data, and CAD models for those parts were
designed. With these models, the NX Nastran
Design solver was used, alongside Siemens
NX software, to obtain the strain and stress
profiles for all parts. These results were
compared with the maximum yield values of
the material, thus providing a theoretical Safety
Factor , ensuring that the systems could
withstand their expected loads. Other studied
failure modes, making use of the Hyperworks
suite, included: vibrational modes, local and
global buckling, and fin and ogive overheating.
4.5. Aerodynamic Analysis
The aerodynamic analysis of the rocket
comprised many aspects. First, it offered a
detailed description of the flight simulator ,
followed by the input parameters. The stability
of the rocket was verified under nominal flight
conditions, and the expectable values of
certain parameters were studied throughout
the flight, to serve as inputs for the structural
analysis. Risks associated with aerodynamic
phenomena were also studied. Finally , the
trajectory of the rocket under variable weather
conditions was studied for both nominal and
adverse conditions (motor explosion, loss of
fins, premature separation), to ensure the
spaceport footprint was respected.
5. Results and discussion
The data used to perform the analysis of the
flight comes from three dif ferent sources:
a. CR’s simulator: used during launch
operations to predict the rocket
trajectory and ensure safety .
b. On-board avionics: developed by BiSky
T eam, transmitted data every 0.3 s to
the ground stations.
c. INT A ’s tracking devices: of fer trajectory
data at a 50 Hz rate, starting at 1.16 s
into the flight due to a tracking error
during lift-of f.
5.1. Acceleration
Figure 5. Acceleration during ascent flight
Figure 5 shows the absolute value of the
acceleration during ascent flight. The
acceleration phase lasts approximately 6 s,
and the rest is deceleration.
The readings obtained from the avionics and
INT A are almost identical, except from the
noise present in the latter due to the higher
sampling rate. The divergence at the end is not
significant and is attributed to the distance
between the rocket and the tracking device.
The simulator predicted a higher acceleration
rate during the powered flight, which might not
have been achieved due to subpar motor
performance and higher drag forces.
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The latter can be also observed in the
deceleration phase. A higher peak after motor
burnout indicates a higher supersonic drag,
which quickly decelerates the rocket to the
subsonic region (around 12 s after lift-of f). The
simulator predicted a longer supersonic phase,
lasting until around 15 s.
Acceleration rates in the subsonic region are
almost identical, which leads to the conclusion
that drag discrepancies must be associated
with supersonic drag (associated mostly to
shock waves). The numerous bolts and rivets
in the fuselage, as well as the voluminous fin
supports are believed to be the origin of this
increased drag. Ef forts in the simulator have to
be made to adequately characterize the rocket
drag (updating current models based on [3]),
and constructive improvements are needed for
future rockets.
5.2. V elocity
Figure 6. V elocity during ascent flight. Raw data
Figure 6 presents the velocity readings from
the two ground stations. Station 1 did not
receive consistent data at any point, while
station 3 is not accurate during the majority of
the flight, since it of fers a velocity profile
characteristic of a two-staged rocket. The root
of the problem has not been identified, and can
be associated either with data reading,
transmission or reception. Since acceleration
readings are correct, the velocity will be
obtained through integration (using an explicit
scheme), taking into account the Euler angles
(which define the orientation of the rocket).
After manipulating the avionics data, the
results in figure 7 show a better correlation with
reality . The slight dif ference can arise from the
acceleration discrepancies, inaccuracy of the
Euler angles measured, or due to the
numerical integration scheme.
Figure 7. V elocity during ascent flight.
Manipulated data
The ef fects of increased supersonic drag can
be seen also in this figure, since the change in
slope becomes significant after around 300
m/s (in the transonic region). This strengthens
the hypothesis presented from the acceleration
data.
The deceleration rates after going below Mach
1 are similar and the model for predicting
subsonic drag (also extracted from [3]) is
assumed to be accurate.
5.3. T rajectory
Figure 8. Rocket trajectory
Figure 8 shows the trajectory of the rocket
according to the three sources.
Once again, the level of accuracy of the
avionics, as received by ground station 3, is
high. However , Global Positioning System
(GPS) data is not completely accurate during
the higher speed segment of the flight. This
causes the divergence towards the west during
the ascent. If the time is taken into account, it
could also be observed that the GPS
information is lagging behind during this part,
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were called "space weather operators", and
the logo for the SWIC originates from there
(Figure 1).
Figure 1. SWIC Logo
The Koninklijk Nederlands Meteorologisch
Instituut (KNMI) joined in the development of
the course shortly after . Now also the duty
of ficers of the PECASUS [7] service follow the
S W I C . PE C A S U S p r o v i d e s a d v i s o r i e s o n
en h a n c e d s p a c e we at h e r ac t iv i t y fo r c i v i l
aviation. The STCE supports this service in the
fo rm of th e S WI C, whic h i s o pe n t o a ll
PECASUS partners. The first SWIC took place
in May 2017, with the fourteenth edition in
March 2022. No courses took place in 2020
due to the outbreak of the COVID pandemic. In
total, already more than 100 trainees took part
in this course.
The course is intended as an entry course on
spac e we ath er . It pr ovi des a n el eme nta ry
overview of the relevant aspects of space
weather without invoking complicated
background physics. The course is intended
for meteorologists and space staf f that will be
providing space weather information to military
and civilian end users.
Aside from individual participation, it is also
possible for an institute to request a SWIC to
be organized for their employees. Depending
on the ir aca demic level, th e ins titute can
choose to refresh certain physical and
mathematical basics to allow the trainees an
ea sie r u nd er st an di ng of th e S WIC 's main
portion. This is called the pre-SWIC and is
g i v e n b y t h e r e q u e s t i n g i n s t i t u t e i t s e l f .
S i m i l a r l y , th i s in s t i t u t e ma y al s o el e c t to
educate the trainees on the space weather
ef fects on the specific equipment they handle
(e.g. the military). This so-called post-SWIC
takes place after the main SWIC and is again
the responsibility of the requesting institute.
For obvious reasons, the pre- and post-SWIC
are not a systematic part of the main SWIC.
The introductory course can be extended with
topical modules or tailored to the specific
needs, background level and interests of the
participants. An end user from the aviation or
telecommunication sector , for example, has
other needs than a space weather forecaster
in a solar research centre.
The programme focuses on gaining knowledge
by fact-learning and training skills through
easily accessible methods like repetition and
games. The on-site editions include a visit to
the beating heart of our service centre and a
‘Meet & Greet’ with scientists and forecasters.
SWIC has the tools to evaluate the participants
and can provide an examination certificate.
T h e S W I C i s t a u g h t b y q u a l i f i e d a n d
experienced staf f with extensive expertise in
relevant domains such as scientific research,
so la r phy si c s, spa c e w ea t he r , f or e ca st i ng ,
engineering, communication and outreach, and
teaching.
Due to the COVID pandemic, the courses
planned in 2020 were canceled as participants
were unable to travel to the STCE. From 2021
onwa rds , we restar ted with a fully o nli ne
version of the course. The encounters with
S T C E s ci e n t i s t s w e r e r e p l a c e d b y g u e s t
lectures and the exercises were reinvented
using existing, easily-accessible online tools.
The added benefit of having a fully online
version of the course is that it allows us to
reach an audience that cannot easily travel to
Belgium. W e organized for example a tailored
course for members of the United States Air
Force for whom travelling to Belgium for a 3-
day course is to o time-co nsuming. Online
participation is also advantageous for
environmental and climate reasons and to
avoid extra financial costs. We plan to continue
organizing the SWIC alternating between
online and on-site editions.
3.1. Course Contents
The content focuses on space weather and the
ef fects on man-made infrastructure and its
functionality .
W e discuss solar eruptions of very high-energy
matter and electromagnetic radiation, which
in j ec t m a ss i ve amo u nt s of e ne r gy in t h e
Earth's magnetosphere and ionosphere
leading to pronounced impact on navigation,
communication and energy transport.
The basic concepts and drivers of space
weather are described first, with an added
overview of the different sensors used to
monitor the activity . From the Sun, we move to
the magnetosphere, thermosphere and
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i o n o s p h e r e a n d d i s c u s s h o w t h e y a r e
impacted. The impacts on aviation specifically ,
in particular in the framework of PECASUS, is
described in much detail on the last day of the
course.
B y t h e e n d o f t h e c o u r s e , t h e t r a i n e e s
understand the basics of space weather and
know about the potential impact on technology .
The students are also able to understand and
i n t e r p r e t t h e s p a c e w e a t h e r i n f o r m a t i o n
p r o v i d e d b y t h e s p a c e w e a t h e r f o r e c a s t
centers.
3.2. Didactic Methods
The SWIC caters to a very diverse public,
which are not always trained extensively in
ma t h e m a ti c s an d p h y s i c s . W h i l e w e on l y
expect a medium secondary school knowledge
of mathem atics and physics, most of the
p a r t i c i p a n t s h a v e w o r k i n g e x p e r i e n c e i n
weather forecasting or engineering, and have
an interest in natural and technical sciences.
From time to time we have participants that are
working as civil servants in risk assessment.
Their knowledge of physics is usually limited,
and then we adapt the course accordingly by
e x p a n d i n g m o r e o n t h e b a s i c p r i n c i p l e s .
Everyone is required to have a good working
knowledge of English since that is the teaching
language.
In th e co u r s e we fo c u s o n th e ph y s i c a l
principles of space weather without working
out the details mathematically . There are little
to no equations shown in the course notes. All
principles and concepts are explained verbally
and with graphics and movies, making use of
co mp ar is on s t o k no wn conc ep ts whe re ve r
possible. We intentionally keep the number of
participants low (up to 8 trainees per SWIC in
the more recent editions) such that we can
monitor their understanding and progress
closely .
The on-sit e course comprises three d ays,
while the online course is spread out over four
days. There is a huge amount of material for
the students to absorb. W e found that when
teaching online it is harder for the students to
concentrate for an extended period of time,
also because we cannot do site visits in this
case, which tend to make the day somewhat
lighter . Therefore, we spread the online course
over more days. For the on-site course the
trainees have to travel to the STCE and so it is
best to comprise it into fewer days to reduce
the total time spent on the course.
Starting 2022, the concluding online evaluation
of the course was moved to the week after , so
that there is more teaching time left and the
trainees have more time to study the course
material before being tested. Throughout this
week the teaching staff is available to answer
any remaining questions.
In the course of a lecture day , we alternate
between didactical methods and tools. The
basic principles of space weather are mostly
explained through direct teaching, aided by
presentations. The three experienced teachers
that are responsible for the bulk of the course
c o l l a b o r a t e c l o s e l y t o h a r m o n i s e t h e i r
presentations. They also make sure to involve
the audience through questioning and
interactive slides, and encourage questions
from the trainees. The program alternates
these teaching periods with exercises, games
and recapitulation moments. The main
c o n c e p t s a n d p r i n c i p l e s a r e r e p e a t e d
constantly such that the students can absorb
the theory simply by attending the course. The
trainees also have their own job to attend to
and will have little free moments to spend on
studying outside of the course time. We
anticipate this by including the repetition in the
course program.
T h e e x e r c i s e s i n c l u d e h a n d s - o n m a t e r i a l
where the students work with real-life space
weather data and learn to interpret them. The
g a m e s s u ch as pi c t i o n a r y , t a b o o , ri n g i n g
su n s p o t s [ 8 ] an d b i n g o a r e me an t as a
moment to relax and bond, but also serve as
an opportunity for questions, recapitulation and
repet ition . Duri ng the se exe rcise s we c an
c o r r e c t a n y m i s i n t e r p r e t a t i o n s a s w e l l .
Additionally , each course day starts with a
recapitulation of the previous day and a Q&A
session.
For the online version of the exercises, we use
G o o g l e J a m b o a r d s [ 9 ] , w h i c h a r e f r e e
interactive whiteboards on which the students
can work together . The courses are taught
using the Zoom teleconference software [10]
and we use many of the interactive features
there such as the annotation option to make
explanatory drawings, the breakout rooms to
allow students to work on the exercises in
small groups and the poll feature for quick
tests. The final evaluation of the trainees takes
place online through the STCE website.
The slides of the presentations are provided to
the students and serve as course notes. They
are accompanied by explanatory text, of which
the content is much broader than what was
discussed during the course itself and which
includes useful links. The slides serve as a
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4 th Symposium on Space Educational Activities
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reference for the trainees when executing their
future job interpreting space weather forecasts.
4. Discussion, feedback and reflections
Throughout the SWIC, much attention is spent
on feedback from the students. At the end of
each day and at the end of the course, we ask
the trainees for their reflections, comments and
suggestions. For the students that prefer to
share their opinion in private, we invite them to
do so once more when we deliver them the
course certificate. The teaching staf f can easily
be contacted by the trainees and actively
encourage the students to reach out with
questions and feedback.
Throughout the years, this open attitude has
allowed us to improve the course, for example
in refining the order in which the dif ferent
subjects are tackled and adding extra course
time at the start to introduce basic concepts
that are needed throughout the course.
Also, when transitioning to the online version,
t h e fe e d ba c k o f th e s t u d e n ts wa s m u c h
needed, for example on which online tools
were easy to use and accessible to them. Note
that some work in restricted environments
where the installation of new software is not
allowed.
After each edition, the teaching staff holds a
meeting to critically evaluate the SWIC and to
plan the next one. In these meetings exercises
and course material are fine-tuned. One of the
decisions that came out of them is to decrease
the number of participants in the more recent
editions, allowing for a closer monitoring of the
students as well as more interaction between
them.
5. Conclusions and Outlook
The SWIC has been a major success for the
STCE, allowing us to reach a new public of
meteorologists and aviation staf f. The STCE
a l r e a d y h a d a s t r o n g p o s i t i o n i n p u b l i c
outreach and communication towards the solar
scientific community , yet it is very hard to cross
the borders to other disciplines. Space weather
is by definition an interdisciplinary science with
a broad range of impacts. Through the SWIC,
we can raise the awareness of other research
institutes, companies and nations to space
weather threats. The continued interest in the
course shows there is a real need for this
t r a i n i n g . T o o u r k n o w l e d g e , t h e r e i s n o
equivalent to it in Europe, even worldwide.
In the future we plan to diverge to tailored
courses. In 2021 we organized a custom SWIC
for the United States Air Force, focusing in a
limited time span on the topics that were of
most use to them. We plan to continue on this
route by providing, in addition to the regular
SWIC that is now on point, one-day topical
SWICs focussing on ionosphere, aviation or
high-frequency communication. A one-day ,
specialized course may also attract interested
trainees that are unable to free up multiple
days in their busy work schedule.
Acknowledgements
T h i s w o r k w a s s u p p o r t e d b y t h e S o l a r -
T errestrial Centre of Excellence. We thank our
partners of the Royal Netherlands Air Force
(RNLAF) and the KNMI, for their help in setting
up and continuously improving this course. The
S W I C h a s b e n e f i t e d g r e a t l y f r o m t h e
contributions of its guest speakers and the
guides of the site visits, but also from the
generous feedback of all participants up to
now .
References
[1] SWEC: https://www .stce.be/SWEC ,
last visited: 15th March 2022.
[2] P . V anlommel et al.,, Exploitation,
dissemination, education and outreach in the
frame of the COST action ES0803 "developing
s p a c e w e a t h e r p r o d u c t s a n d s e r v i c e s i n
Europe", Journal of Space Weather and Space
Climate, V ol 4 (8pp), 2014.
[3] PROBA2: https://proba2.sidc.be/
index.php , last visited: 15th March 2022.
[4] S T C E N e w s l e t t e r : https://
www .stce.be/newsletter/ , last visited: 15th
March 2022.
[5] S T C E S h o p : https://www .stce.be/
shop/ , last visited: 15th March 2022.
[6] JSWSC: https://www .swsc-
journal.org/ , last visited: 15th March 2022.
[7] K. Kauristie et al., Space W eather
Services for Civil Aviation—Challenges and
Solutions, Remote Sensing, 13 (18pp), 2021.
[8] Ringing Sunspots: https://stce.be/
esww2019/ringingsunspots.php , last visited:
15th March 2022.
[9] Google Jamboard: https://
support.google.com/jamboard/answer/
7424836?hl=en , last visited: 15th March
2022.
[10] Zoom: https://zoom.us/ , last visited:
15th March 2022.
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Page 1 of 5
D e s i g n a n d i m p l e m e n t a t i o n o f s p a c e e d u c a t i o n a l a c t i v i t i e s t o m o t i v a t e
y o u n g s t u d e n t s i n C a t a l o n i a
Guillem Olivel la 1 , Marcel Marin 2
__________________________________________________________________________
Abstract
STEM education is a new interdisciplina ry concept t hat fuses the l earni ng ob jectives of
sciences, technology, engineerin g and mathematics. A f ter concl uding t hat many
under graduate students are not interested in STE M disciplines and taking into account t he
admiration for space, a series of educational acti vities have been develope d to increase t heir
engagement in this field. The propose d project-based workshops are diverse: desi gning and
launchi ng High Altitude Balloo ns; buildi ng water rockets; protecting an egg from the impac t
with the ground afte r being dropped from a drone; designing and buildi ng paper glide r s ; 3 D
printing cus tomzied quad copters, etc.
One of the most impress ive activities consisted o f desi gning, manufac turing and launching a
low-cost high-altitude balloo n to take photog raphs of the s t ratosphe re. To do so, a kit was
developed and vali dated: t his con tains a GPS t racker, a camera , an EPS b ox, a parachu te and
a hel ium bal loon. The sel ection of the componen ts was done trying to mini mize the operational
cost and maximizing the reliabili t y of the desi gn; the final High Altitude ba lloon weights 350g
and has reached altitudes around 27.000 - 30 . 000 m. The educational act ivity is a 3 to 4 days
workshop in which t he students go through t he process of buildi ng their own HAB, launching
it and eventual ly recove ring i t to obtain t he photographs.
The activiti es ha ve been implemented in multipl e schools and high school s in Cataloni a, and
all of them have shown excellent results. After eval uating t he reasons why the workshops were
well -received, it was conclud ed that s tudents were more implicated than in st andard lecture s
because they went from a passive to an active mindse t. Moreover , the workshops were
de signed to make them become curious and incr ease thei r eagerness to learn, while f orcing
them to think and to tak e important decisions that ultimately in fluence the f inal result, rather
than observing and admi ring somebody else’ s work.
Keywords
STEM , Space , Worksho p, HAB
__________________________________________________________________________
1 GoSTEM, Spa in, gostems pace@gma il.com
2 GoSTEM, Spa in
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Acronyms/Abbr eviations
HAB High Altitude B alloon
STEM Sciences, Tech nology, Eng ineering ,
and Math ematics
UA V Unmanned A erial Veh icle
1. Introduction
STEM education is a new interd isciplinary
concept that fuses the learning objec tives of
sciences, techno logy, engineering an d
mathematics. It is a new way of learnin g, usu ally
related to the project- based meth odology,
which sti mulates interest and c reativity among
students. ST EM careers ar e gro wing more a nd
more as a demand of high- techno logical fut ure
societies ( IoT, Smart Cit ies, 5G …) [1] . Th e
problem lies in the f act that STEM studi es are
usually not the priority among undergr aduate
students and t his cou ld r esult in a decr ease in
the l ife quality o f future societies [2] . Moreover,
there is an important gend er gap when dea ling
with STEM d isciplines: The maj ority of
bachelor’s degrees are obtained by w omen;
however, STEM subjects are no t attr active t o
them [3 ] [4] . I ncreasin g th is i nterest in early
phases of ed ucation such as high sc hool can
reduce the gend er and soci al class gap [5 ].
On the other hand, in many c ountries, it is v ery
common to divide the disciplines int o
mathematics, technology, eng ineering an d
sciences when k illing the c reativity among
students and mak ing the learner lose generality
whilst being close-minde d [6] . This can b e
improved by apply ing a projec t-based
methodology - to increase c reativity and interest
- with a STEM framework. As can be seen, n ew
ways of teac hing ne ed to be put on t he table in
this new era : the l earning procedures need t o
adapt to the new world.
Most of th e progra ms an d activities that use
space to motivate young stude nts to increase
their interest in STEM disciplines use an
admiration-b ased m ethodol ogy: They cons ist of
showing examp les of bi g achievem ents of
difficult cha llenges (outreach strategies of
Rosetta mission a nd Ap ollo program) [7] .
Usually, in this kin d of outreach strate g ies , the
student does not have the opport unity to create
anything. This is a logic al appro ach si nce
access to sp ace is, in the ma j or ity o f c ases,
expensive and technologica lly difficu lt. By doing
so, most of the potential of s pace and its
attractiveness to motivate h igh- school students
to start STEM car eers is lost because t hey
adopt a passive attitude rather than an active
one.
In order to so lve this short coming, a non -prof it
or ganization call ed G oSTEM was creat ed. This
is a project born in the I nternatio nal Space
University t o motivate students from all over the
world to pursue ST EM care ers. The go al of the
organization i s to find an educational project for
each interested schoo l, associat ion, or group of
students co nsidering their needs and the ir
desire to enter th e worl d of space and ST EM.
2. Workshops and activities
Currently, sev eral work shops and proj ect -b ased
activities are bei ng prop osed by GoSTEM .
These are:
1. “High-Altitude B alloon: photographs
from the stratosp here”.
2. “Saturn V: Fragi le launch” .
3. “Opportunity: Landin g in a n unknown
planet”.
4. “Wright Brothers’ ch allenge ”.
5. “ 3D -printing y our own dro ne ”.
All work shops are co mposed of the stag es
depicted in F igure 1.
Figure 1 . Workshops and activities architecture
Follows a s mal l des cription of the ac tivities and
workshops. Not e t hat all t he workshops h ave
been designed to be done w ith several stud ents
working s imultaneous ly. I n some cas es, the
motivation and capabilities among them vary
and th is m a y c ause difficu lties when tr ying to
maintain a uniform flow when doing an activity .
T o solve this pr ob lem, all the workshops
described hereunder have different layers of
complexity and guidance . This allows th e
students to ad apt to dif ferent rhy thms an d to fee l
comfortable wit hin the educ ational activ ity.
2.1. High- Altitude Balloo n: photograp hs from
the stratosphere.
This is, without any doubt, the most impressive
activity do ne by GoSTEM. The educationa l
workshop consists of a 3- 4 days project, whose
ultimate goal is to take a ph otograph of the
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Earth, from the stratospher e as the one shown
in Figure 2.
Figure 2 . Photograph of the Earth at 36.000m
altitude (Taken by GoSTEM).
To do so, the students receive a kit designed by
GoSTEM con taining the following it ems: A
sports camera , tw o indep endent GP S Tracker s ,
all requ ired com ponents to do the platform f or
the H igh-Altitu de B alloon, the p arachute , and
the weather ba lloon with h elium [8].
Figure 3 . GoSTEM High Altitude Balloon kit
2.1.1. Camera
To s elect the most appropriate camera for th e
HAB, fi ve different properties were considered:
weight, cost, image quality, temperatur e
resistance, and battery duration. The final
selection was a n Apeman A8 0, which h as an
image resolution of 20 MP, a maximu m v isual
angle of 170º, a minimu m self-timer shooting
mode of 2s, and a ba tt ery that has proved a
duration of 120m in @ -1 8ºC [9].
For th is com ponent, t he students have to do a
trade-off between the batt ery duration in low
temperatures, imag e quality , and the rate at
which the photogra phs are taken.
2.1.2. GPS Trac ker
For the trac king s ystem, 2 redu ndant devices
are includ ed i n each kit. B oth trackers are GPS-
based but differ on the way of tr ansmitting the ir
position to the ground sta tion: A SPOT Trace is
used to transmit the positi on of the HAB via
satellite (Irid ium- based) [ 10]. A n Invox ia GPS
does the same f unction but t ransmits i ts position
via the SigFox network [11] .
2.1.3. Platform
The Platform is co mposed of thre e d ifferent
components: an EPS Box (internal dimensions
160 mm x 95 mm x 35 mm), cross - linked
polyethylene f or the interior of the box , an d
methyl methacrylate to cover the hole for the
camera.
The s tudents are in charg e of cutti ng, g lu ing ,
and prepar ing the platform to accommod ate al l
other compo nents.
2.1.4. Parachu te
The parachute is built from s cratch using ny lo n
fabric. Th is is one of t h e most interest ing
designs th at the students h ave to d evelop. Fro m
a ba sic equation that represents the static
equilibrium be tween wei ght an d drag, th e
students h ave to derive the parachute diam eter
from a give n H AB mass and drag coefficient.
Moreover, they have to do a tr ade-off to s elect
the termina l velocity o f th e HAB . If the term inal
velocity is t oo high, the c ompone nts inside it
su ch as the camera or GPS can brak e down. On
the other hand, if the termin al velocity is too low,
the H AB c an travel too much hor izontally during
its descent and t his i ncreas es the probab ilities
of landing in remo te areas.
2.1.5. Weather Balloon and He lium .
After m any i terations, it w as concluded th at i s
was high ly rec ommended to use an ov er-
dimensioned weath er ba lloon. This allows the
HAB to asc ent very quickly (which is favora ble
given th e low battery durations in low
stratospheric tem peratures ).
Moreover, onl ine calcu lato rs s uch as the one
presented by H ab hub [ 12], are used to predic t
the flight o f the HA B . Since these on line tool s
require inputs in t he form of pa rame ters that
describe the HAB, stu dents are usu ally
motivated to do test s a nd calculat ions to
estimate properties such as the ascent and
descent velocity .
2.2. Wright Brot hers’ challeng e
This is on e of t he most c omplex activ ities
proposed by GoSTEM. The challenge proposed
to t he students consists o f des igning an d
building a carboard airplane following all the
design guidel ines of a real airplan e.
The concep ts explained t o t he s tudents include
static and dynam ic stability of an airpl ane, Lift,
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Drag, Ce nter of G ravity, etc . This is presented
in a simpli fied way t hat allows the studen ts to
understand the basic concepts withou t
overwhelming t hem.
After go ing throu gh s tructur al and d imensiona l
tests, the a irplanes are thrown using a
dedicated launc h pad.
The structural tests consist of supporting t he
airplanes by the ir w ingtips and hanging a m ass
from the airplane center o f grav ity.
Figure 4 . Wright’s Brothe r’s challenge
2.3. Satur n V: Fra gile launch & Opportunity:
Landing in an unkn own pl anet
These two activit ies a re very similar and share
t he same arc hitectur e: a c hallenge is presented
to the stude nts co nsisting of des igning, building,
and testing a capsul e capa ble of protecting an
egg agai nst its fall to th e groun d. For the f irst
activity (Opportu nity: Landing in an unknown
planet), th e capsule is la unched with a w ater
rocket and, with the s econd one ( Saturn V:
Fragile launch), t he c apsule is la unched with a
quadcopter UA V or by o ther analog means.
As a ll engi neering cha llenges, a set of
re quirements constrai nts the design o f the
students:
• Maximum mass
• Maximum quantity of toke ns used to
buy materi als to c onstruct t he capsule.
(Each student starts the activity with the
same amo unt of t okens and t he non -
complianc e of r equirem ents supposes
the removal of t hem)
• Design envelo pe
This makes th e stud ents t o wor k with a cle ar
objective and t he activ ity fo rces them to retrofit
the design in ord er to meet the req uire ments.
Figure 5 . Opportunity : caps ule launch from UAV.
2.4. 3D - printing your o wn drone
The m ajority of ed ucational ac tivities c onsisting
of building drones are limited to bui lding a pre -
designed UAV. GoSTE M has proposed, for this
activity, t he followin g: the students rec eive all
electronics required to build a standard
quadcopter , a s et of 4 motors, and a fl ight
controller. The chal lenge consists o f designin g
and 3D-prin ting t he fra me (platform) of th e
quadcopter. The final dron e contains a camera
to transmit r eal-t ime i mages and a w ifi-base d
comms sys te m.
Th e activity also de als wit h concepts suc h as
stability vs maneuverab ility by pro posing
different challenges to the s tude nts and making
them adapt t he d esign for each sit uat io n. A n
example of t his is how the students have to
adapt a drone prepared for a n obstac le c ourse
to a dro ne c apable of c ar rying a m ass. The
driver of the first design is m aneuver ability ,
he nce, it has to be designed with short legs and
low mass . The second on e , on the other ha nd,
has to have lon g legs to max imize stability .
The educationa l activity is c om pleme nted with
simulators to prac tice how t o fly a qu adcopter.
3. Results and Discussions
In total, 698 st u dents have part icipate d in
different activit ies, distrib uted as f ollows:
Table 1 . Results [1]
Project
Students
M
F
“High- Al titude Balloon”
13
17
“Opportunity: landing in an …”
2 01
2 47
“Wright Brothers’ challenge”
49
32
“Saturn V: Fragile launch”
68
55
“3D-printing your own drone”
10
6
TOTAL
341
357
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In s ummary, all the activities we re a success : a ll
the st udents ha d a great t ime deve loping their
creations . As a rem inder, the main objective
was to mo tivate young s tudents to engage i n
STEM disc iplines by usi n g the a ttractivene ss of
space. Their m otivation during the act ivities was
obvious since the vas t m aj ority of them were
extremely engage d during all the works hop s .
This c ould dir ectly im ply a gr owth in the number
of s tudents en gaged i n STEM care ers. After
survey ing all the part icipants , they dec lared tha t
they increas ed their c omprehe nsion of the
STEM conce pts tre ated during t he ac tivity .
Furthermore, they emp ha siz ed that the
proposed wor kshops allow ed them to have a
first-hand experienc e with the theoret ical
concepts that the teachers explained to them i n
class.
In terms o f gen der equ ality, 51% of the
participants we re female students an d no
difference was apprec ia ted between the
motivation an d perform ance between femal e
and male stu dents.
4. Conclusions
The educa tiona l proj ect has proved to be a n
excellent platform t o fu lfill the objec t ive of
popularizing STEM disc iplines.
The next st eps woul d be to re ach more and
more schools and ass ociations to con tinu e
motivating yo ung stud ents to enga ge in STE M
disciplines.
As an example of t his, two me as ures have
already been implement ed:
1. The creation of a website to pres ent the
project an d spread it among all the
schools in Cat alonia:
www.go stemspace.com
2. The c reatio n of a summer c amp that
en compass es all Go STEM workshops:
www.spacecamp s.cat
Acknowledgem ents
The t eam wo uld like t o akn owledg e t he
International S pace Un iversity and, in particular,
Joan de Dalm au. We wou ld also like to t hank all
the peop le that have co ntributed to the gr owth
of GoST EM such as: Profes sor Gonglin Sun,
Jordi Mazón a nd Marc B oada.
References
[1] StratoStar We bsite:
www.stratostar.co m/intro - to -project-
based , last vis ited: 15 th February 2022
[2] F. Aarrestad, et al. , S pace and STE M:
one giant leap for educatio n,
In ternationa l Space Univer s ity, 2012.
[3 ] D. Beede, Wom en in STE M: A ge nder
gap to innov ati on , Washing ton, DC:
Economics and Statistics A dministration ,
2011.
[ 4] C. V. McDonal d, STEM Education: A
Review of the C ontribution of the
Disciplines of Science, Tec hnology,
Engineering a nd Mathem atics , Science
education interna tional , 27, 530- 56 9,
2016.
[5] P. Boedeker, S. Nite, R. M. Capraro, M.
M. Capraro , Women in ST EM: The
impact of STEM PBL imple mentation o n
performance, attrition, and course
choice of women , IE EE Fro ntiers in
Education Confere nce (FIE ) , El Paso,
2015.
[6] R. Stichweh, D ifferentiati on of scientif ic
disciplines: causes a nd con sequences ,
Encyclopedia of Life Support Sys tems ,
2003.
[7 ] ESA Outreach Reso urces :
www.sci.esa. int/web/r osetta/- /53593-
outreach-reso urces , last vis ited: 15 th
February 2022 .
[ 8] GoSTEM Web page:
www.gostemspace .com , las t visited: 15 th
February 2022 .
[9] Apeman We bpage:
www.es.apem ans.com , last visited: 1 5 th
February 2022 .
[10] SPOT Webpage: ww w.findmes pot.com ,
last visited: 1 5 th February 2 022.
[11] Invoxia Webpa ge: www. inv oxia.com ,
last visited: 1 5 th February 2 022.
[12] HabHub Websi te:
www.predict.h abhub.org , la st visited:
15 th Februart 2022.
27
DOI: 10.5821/conference-9788419184405.005
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Page 1 of 6
Missi on analysis of na nosat ellite constell ations with OpenSatKit
Iván Sermanoukian Molina 1 , Lluís Montill a Rodríguez 2 , David González Diez 2 , Miquel Sureda
Anfrès 2 , Jorge Mata Díaz 2 , Juan José Alins Delga do 2
__________________________________________________________________________
Abstract
CubeSat r eliability is stil l considered an obstacle due t o the sizeable f ail rates generally
attributed t o the dead - on - ar rival cases and early subsystem malfunct ions. Thus, as CubeSa t s'
primar y pu r pose moves from technolog i cal demonstrations and university projects to missions
where a significant risk of failure is not ac ceptabl e, an inexpensive method to emulate l ow
E arth orbit constellations is being researc hed.
The result s presented have been developed in the framework of the PLATH ON r e se ar c h
project, which intends to develop a h a rdware - in - the - loop emulation platf orm f or nanosatellite
constellations with optical inter - satellite communication and ground - to - sa tellit e link s.
Consequently, a crucial aspect of this project is to have a sufficiently precise orbital propagator
with real - time manoeuvring control and graphical r epresentation.
NASA's O penSatKit , a multi -f a c et ed open - source platform with an inbuilt propagator known as
42, has been chosen t o analyse the programme's feasibility in order to create a constellatio n
test ing bench. A s an initial development of a s oftware - in - the - loop appl ication, t he pre -
processing of files has been automated; enhanced A tti tude D et ermination and C ontrol S y st em
manoeuvres have been added and configured through bidi rectional socket interfaces , and th e
results format has been modif ied to be easi ly post - processed with MATLAB and Simulin k.
Keywords
Constellations , Inte r - Process Communication, Na nosatellites, Orbit P r opagation
__________________________________________________________________________
1 Corres pon ding a uth or: Un iv ers itat Pol itècn ica d e Cat aluny a, Sp ai n , ivan.ser m anouk ian@u pc.edu
2 Univ ers it at Politèc nic a de Cata lunya, Spain
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DOI: 10.5821/conference-9788419184405.006
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Page 2 of 6
Acro nyms/Abbrev iations
ACS Atti tud e Co ntrol System
cFS core Fli ght Sy stem
GNSS Globa l Naviga tion Sate llite Sys tem
GS Ground Statio n
GUI Graphic al Us er In terfac e
HiTL Har dware in the Lo op
IoT Interne t of T hi ngs
IPC Inter - Proc ess Co mmunic ati on
LEO Low Earth Or bit
NASA Nati ona l Aeron aut ics and Spac e
Admin istrati on
NS3 Network Sim ulat or 3
PLATHON Integra ted H ardware i n the loop
simulati on Platform o f Optic al
commu nicat ions in Nan os atel lites
SiTL Softw are in the L oop
SSH Sec ure Shel l Pro tocol
TLE T wo - Line Elemen t
ECEF Ear th - centr ed, Ear th - f ixe d
ECI Earth - centr ed inert ia l
1. Introduc tion
Since th e be ginni ng of the spac e age, sate llit e
desig n phi losop hy wa s dominat ed by
conser vativ e des igns b uilt with highly r elia ble
compon ents to e ndur e ext reme e nviron men tal
condit ions . Durin g the las t t wo deca des, th e
dawn of th e Cu be Sats has c hanged t his
philosop hy , enab ling a whol e world of ne w
possibi lities.
The de ploy ment of m o nument al Cu be Sat
const ellat ions in l ow E arth orbit (L EO ) is s et to
revolut ionis e the s p ace s ector by en ablin g
faster and mor e ec onom ical i nnovat ion c yc les.
However , Cu beSat r elia bility is s till consid ere d
an obs tacle due t o t he siz eabl e fa il rates amon g
univers ities an d c ompani es, genera lly attr ibut ed
to the d ead - on - arr iva l cas es and s ubsy stem
malfunc tions [1]. In rec ent y ears , increas ed
f light experi ence is c h anging this tren d, and
future t estin g sy stems are s et to cons idera b ly
reduce th e pro bab ility of an y malf unc tion .
Mission Ana lys is is th e de sign a nd ana lys is o f
satel lite orb its s uch th at the o bj ectives o f a
space mis sio n are achiev ed in the bes t p oss ible
way. Am ong t he main t ask s and outp uts , this
resear ch has focus ed on gr ound s tat ion
cover age, com mun icat ion a ngl es and d istances
between s atellites , as w ell as ecl ipses and
distance fr om the Su n, w hich are c rucia l to
power s ubs ys tem manoe uv re st rateg ies.
The res ults pres e nted i n t his paper h ave be en
devel oped in the fra mew or k of the Int egr ated
Hardwar e - in - the - loo p (HiTL) emul ation Pla tfor m
of Opt ical C ommun icat ion s in Na nosat ellit es
( PLATHO N , from t he Spanis h ac rony m) .
This r esear ch proj ect int ends to deve lop a
Hardwar e - in - the - loop em u lation p latfor m for
nanosa telli te cons tell ations with opt ical inter -
satel lite com mun icati on an d grou nd - to - s at el lit e
links .
Section 2 s ummar is es the state o f th e art and
program me select io n , sec tion 3 en um erates
new pro gram me con trib utions duri ng all
simulati on sta ges , s ectio n 4 shows the res ults
of the new fe atures , and s ection 5 co nc ludes
with th e c urre nt st ate of th e pr ojec t and pot ential
improve me nts .
2. State of the art
In ord er to pro pag ate or bi ts, t here are open -
sourc e and pr ivate prog rammes that can
perform t he s imu latio ns wi th a w ide r ange o f
detail depen din g on th e pr oj ect requ ireme nts .
Among the ava ilab le op en - sour ce op tio ns, t he
Nationa l Aer onaut ics and Spac e
Admin istrati on ' s ( NA SA) O pen Sat Kit has been
chosen b ec ause it offer s H iTL c apab iliti es and
can be easi ly cus tom ised to int eract w ith the
projec t ' s models . Th us, as the progr amme is
open - source, it is helpfu l for res earch an d
devel opment purp oses , and in troduc es
students and profes si ona ls to the s pace s ector .
2.1. O penSat Kit
OpenS atKit is a multi - f aceted p latfor m that
combi nes t hree indep end ent pr o gram mes [ 2] :
Ball Aer ospac e Cor por ation ' s CO SMO S
comma nd and c on trol pl at form for emb edd ed
system s; NASA ' s core Flight Syst em (cFS), a
platfor m and proj ect - i nd ependen t, re us able
softwar e fr amew ork ; and NA SA ' s 42, a
compreh ens ive, gener al - pu rpos e sim ulati on o f
attitude an d traj ectory dy nam ics and cont ro l
which can be ap plied to n umero us s pacecr aft
compose d of mu ltipl e rigi d or flex ible b od ies [3].
Figure 1 . OpenSa tKit platform connectivity [4 ]
This s tudy aims to analy s e the f eas ibil ity of
NASA ' s 42 orb ita l propag at or in the PLATH ON
projec t and its conn ectiv ity with Op enSat Kit
modules .
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4 th Symposium on Space Educational Activities
Barcelona, April 2022
geometric a nd radiometric correction
techniques and image enhanceme nts.
Finally, the image processing unit s h ows how
to apply the different techniqu es to analyse the
images visually and statistically.
The last unit, applications of remote sensing
images , shows the applications of remote
sensing in different areas: forest, agriculture,
oceans and water, ice , cartography, geology
and land use . It is also the unit where students
learn how to extract information from satellite
data, applying indexes, classifications and
algorithms to obtain Land Surface
Temperature (LST) from thermal bands.
In order to evalu ate t he co mpetences acquired
by the students, they h ave to work on two
different practical activities. Both of them t ry to
emulate a real study ca se, and are designed to
perform the following tasks:
- Search and download images from a public
catalog.
- Apply an image correction p rocess over the
images.
- Create RGB band combinations.
- Calculate indexes, such as NDVI, NDWI,
NBR.
- Apply cloud masks.
- Create image mosaics.
- Obtain LST from thermal bands.
- Execute a supervised classification process .
2.2 The software
The objective of a subject like this is to learn
how to deal with remote sensing images and
apply the correct methodologies in order to
extract use fu l i n formation from them, but not
how to use a specific software, library or
toolbox.
Nonetheless, it is obvious that students will
perform the activities with a specific tool, and
they need to be instructe d on that.
Our f irst approac h is to let the students to
choose their pr eferred tools, alth ough we offer
some recommen dations and materials
(lectures, tut orials, manuals a n d self-st udy
activities) related to specific software.
In that s ense, ou r priority is t o recommend the
use of open-source tools. So, students are
encouraged t o use tools like QGIS with the
SCP plugi n, GRASS Gis and SNAP. With
these tec hnologies, they can complete all t he
mandatory activities, and we consider that are
very u seful for acquiring the mandatory
competences of the subject.
For those students who choose other options,
like ArcGis Pr o , E NVI, Erdas, etc., we don’t
offer support materials, but if necessary we
can give advice through the forums.
2.3 The data
Nowadays there are lots of missions providing
remote sensing images.
It is in fact one of the main competences of the
second unit of the course ( platforms,
satellites and sensors) to be familiar with
some of these missions and know their main
characteristics in order to choose the best one
for a specific project.
As it would be completely impossible to design
activities to work with data from a ll the
available missions, we can select only some of
them.
Due to its impact on the industry, historical
series a nd o pen access, Landsat data are
widely used during the course. Students can
easily obtain the images from Lan d sat
catalogues using applications like Earth
Explorer [1] or t hrough the SCP plugin. Also,
Landsat data form a ts can be directly used by
our recommended so ftware solutions and are
offered in different processing lev e ls.
Data f rom the Copernicus programme a re
also used during the course, especially the
images o ffered b y the Sentinel missions. In
the same way as with Landsa t images,
Sentinel d ata can be obtained for free throu gh
applications like Sen tinel Open Access Hub [2]
or also the SCP plugin.
In t he cas e of Sentinel datasets, we mainly
work with the images provided b y t he optical
sensor on board S entinel 2. But we’ve also
prepared a non-mand atory activity where
students can p ractice with the ra d ar images
provided by Sentinel 1.
2.4 EO4GEO
Our experience dev elop ing projects in the
geospatial sector is f undamental for desig ning
a programme for a sub ject like this. We can
Page 3 of 4
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4 th Symposium on Space Educational Activities
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easily identify the skills that student must
acquire in order to successfully join a team
involved in the use and processing of remote
sensing images.
However, beyond the experience, there are
some tools that ca n be very u seful in order to
help in the design of such a pr o gramme.
EO4GEO[3] is a co-funded project of t he
Erasmus+ Programme of the European Union
which aims to bridge the skills gap betwe en the
supply and demand of education and training
in the space/geospatial sect o rs.
In the framework of EO4GEO, a set of tools
based on the GIS&T body of knowledge [4]
have been developed.
For exampl e, the ‘ Bok Visualization and
Search ’ [5] tool allows users t o navigate and
visualize the EO4GEO BoK in a graphical a nd
textual way. Starting from higher level
concepts representing areas of knowledge in
the field, one can browse down to more
detailed concepts. So, this tool is specially
indicated to identify the knowledge areas and
concepts that the subject sho uld integrate.
Figure 2. BoK Visualization and Search
tool.
The ‘BoK Visualization and Search’ t o ol is
public, and no registration is required .
The ‘ Curriculum De s ign Tool ’ [6] (CDT)
allows u sers to create, edit and find
educational offers in the field of Earth
Observation and Geograp hic Information. The
tool could be useful to define the remote
sensing subject p rogramme re-using
descriptions of related BoK concepts and link
specific EO/GI BoK concepts and skills.
3. Conclusions
Remote sensing is a very valuable source of
information fo r GIS projects. So, from our point
of view, a master’s degree in GIS must include
a course about remote sensing.
A s u bject li ke this should guar an tee t h at
students have learnt the basic principles of
remote sensin g, and have also acquire d
competences in order to search and download
remote sensing images, perform
enhancements and corrections over them, and
also extract information b y applyin g some
processes like RGB band co mbinations, index
calculations, band maths or classifications.
Open-source tools like QGIS and the S CP
plugin, GRASS or SNAP are g ood candidates
to use during the course.
Despite t he wide va riety of providers, the open
catalogues form Landsat and Sentinel are very
useful for acquiring the skill s of the course.
Finally, the GIS&T BoK and tools developed in
the framew o rk of projects like EO4GEO can
help in the design of the cours e topics.
References
[1] E arth Explorer Website:
https://earthexplor er.usgs.gov/ , last
visited: 25 th February 2022.
[2] O pen Access Hub Website:
https://scihub.copernicus. eu/ , last
visited: 25 th February 2022.
[3] E O4GEO: http://www.eo4geo.eu/about-
eo4geo/ , last visited: 7 th March 2022.
[4] G IS&T Body of Knowledge:
http://www.gi-n2k.eu/wp-conte n t/uploads
/2014/01/UCGIS_GISandT _BoK_DigReI
ssue2012.pdf
[5] B oK Visualization and Search:
http://www.eo4geo.eu/to ols/bok-
visualization-and-search/ , last visited: 7 th
March 2022.
[6] Curr iculum Design Tool:
http://www.eo4geo.eu/to ols/curriculum-
design-tool/ , last visited: 7 th March
2022.
Page 4 of 4
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Page 1 of 5
C ANSA T C o mp etiti o n 20 20: B es t te ch ni cal dev elo pmen t b y O r bi S at t eam
Dav id H er nand o - Diaz 1
_ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ _____ ___ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ _
Ab str act
Or biSa t is a high sc ho ol educ at ion al proj ec t t hat w as par t o f t he CA NS AT S P AI N 2 02 0 s tu de nt
com pet iti on or gani z ed by ES ER O. T his pr ojec t has r anke d fi r st in t h e Cat alo nia C h ampio nshi p
an d sec on d at t he Na ti onal Ch ampi ons hi p, wi nnin g th e pri ze f or t he bes t tec hni c al
dev elop m ent. Or bi Sat has s ucc es sf ull y ful fil le d t he objec ti ve of c rea ting a mi ni sat ell it e wit h the
si ze o f a s od a c an th at w as l ater lau nch e d by a r oc ket of the C O SMIC R ese arc h U PC S tu dent s
Ass oci ati on t o anal yze p hysi c al as pe cts of th e ai r suc h as pr es sure , t e m p erat ure, h u m idi ty , or
t h e am ou nt of U V so l a r radi atio n of a t err itor y.
Tha nks to t he Ca nS at pres ent ed by thi s te am, d uri ng t h e la unc h w e wer e abl e t o kn ow t he
pr ese nce o f up t o 15 ch emic al ele ment s i n t he ai r. El em en ts ra ngi ng fr o m hy dr o gen an d
oxy gen c an i ndi ca te w ater in th e at mos p her e or oth er gr een ho use gas es s uch as C O2 or
m et ha ne .
The l aunc h ed r ock et r eac hed a n ap pr oxi mat e hei ght of 5 32. 7 ± 1. 5 me ter s, w it h t he se nsors
we w ere able to det ermi ne th e apo ge e of t he r ocket an d t he s ubs eq uent r el eas e o f th e
mini s atell it e an d de ploy m ent of the par ach ute . W e w er e als o a bl e t o i nter rel at e t he al ti tu de
dat a wi th p ar ame ters s uc h as hu midi ty, UV r adi a ti on, pr es en ce of hydr og en , am on g oth er s.
The C anS at pr ese nt ed by th e Or bi Sa t te a m h ad a uni qu e d esig n n ever s ee n befor e in o th er
CanS at c om pet iti ons , s ol vi ng probl e ms suc h as hi gh w eig ht a nd ov erh e ati ng. T his desi gn
ma de by Aut oC AD w as an op en co nc ept w her e the ai r ca n r efr iger at e t he CPU an d also th e
3D pr int ed c onc ept s ave d 1 25 gr a m s ov er a thir d of the maxi mu m all owe d. In addi tio n, al l t he
dat a c oll ect ed w as broa dca st i n r eal - ti me and r ecei ved by a gr ound s t ati on ev er y 0 .2 5 sec on ds.
Bef ore t he l au nch, a si mul ati on w as c om plet ed es tima tin g a 6 1 se co nds fl i ght , fin al ly , th e re al
fl ight was 5 9 s ec onds . Th e v ast m ajor it y o f t he pr ojec t wa s done d uri ng t he COV ID - 1 9
pa ndemi c , th e c ons eq uenc e w as new meth o dolo gies t o c ar ry on th e pr oj ect w it h a mi ni mum
ti m e for t he w or ksh op an d t est p ha se t ha t w ere sup pli ed wit h s i mula ti ons h avin g a bet ter
per f orm anc e tha n exp ect ed.
Keyw ords
CanS at , E duc atio nal Pr oje ct , ESER O
_ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ _____ ___ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ __ _
1 Univers it at Polit èc nica de Cat alunya ( UPC), S pain, david.her nando. diaz@ es t udiant at. upc . edu
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1. Intr od uc tio n
CanSat is an initiat ive of t he E uropean S pace
Agency [1] that challenges s t udent s from all
over E urope t o build and launc h a mini s a t ellit e
the s ize of a " soda c an" to a height of no m ore
than one k ilomet er . T he challenge f or
part icipant s is t o fit all t he m aj or subsy stems
found in a s at ellit e: elect ric power, sensors , and
the c omm unicat ions sy st em. Ev erything m ust fit
into t he v olume and s hape of a s oda can.
Subsequent ly , t he CanSat will be launched, in
our cas e by a roc ket , t o a height of no more than
one kilomet er . Alt hough on ot her occas ions, it is
dropped f rom a plat f orm , a drone, or a balloon.
Onc e t he CanSat parac hut e [ 2 ][ 3] deploys, t he
miss ion begins, and t he s at ellit e st art s to
perf orm sc ient if ic experiment s as it descends
and lands saf ely . After t he f light , t he t eam s mus t
pro cess the dat a and draw conclus ions about
the f light .
The ex perim ent s that t he CanS at will perf orm
while descending ar e divided int o t wo par t s
fir st ly , t he Prim ary Miss ion, m andat ory f or all
team s and c onsis t ing of t he c onst ant emis sion
fr om t he s at ellit e and recept ion f r om a gr ound
st at ion [4][5 ] of t emper a tur e and at mos pheric
press ure dat a at leas t once per s econd.
The S econdar y Mission is fr ee and is the one
that dif f er ent iates CanSat fr om the o ther t eams.
However, t he im plement at ion of bot h in a
diff er ent way led t he O rbiS at t eam t o win t he
tec hnical ac hievem ent f or the com plexit y and
original it y of t he design, implem ent at ion, and
integr at ion.
In t he c ase of the Or biSat team, the Pr imar y
Miss ion ment ioned abov e communicat ed wit h
the gr ound st at ion f our tim es per se cond,
allowin g us t hat if one of t he temper at ures and
atm ospher ic pr ess ure dat a did not arrive or
arr ived damaged, it could be discarded wit hout
aff ec t ing t he ov erall r esult s. We als o decided t o
ext end it a lit t le more by obtaining t he humidit y
data and s ending t he s at ellit e's GPS posit ion
thr ough t he ant enna, which helpe d t o loc at e it
once it had f allen.
The O r biSat team' s secondary mis sion was t o
recr eat e a kind of pr obe sat ellit e t hat would be
launched on a pl anet ar y m iss ion. A s it
descended t hr ough t he at mos phere, it would
collect dat a on gas es t hat m ight be in t he
atm ospher e of t he hy pot het ical planet . It als o
collect ed inf or mat ion on UV r adiat ion, and all
were st or ed on t wo SD c ards that ser ved as a
backup if one was damaged dur ing t he impac t.
2. Prototy p e
2 . 1. Vers io n 1
The CanS at st r ucture pr esent ed here s hows an
open concept t hat has been ent irely designed in
Aut oCAD, allowing us t o save m any r esour ces
since we wer e able t o perf or m t es ts and
simulat ions of prac t ical s pace for the placement
of t he various ex perim ent s without the need for
fur t her pr int ing.
2.1.1. M ater ial s
The m at erial us ed f or the str ucture was
Polylac t ic A cid, com monly known by its
abbreviat ion ( PLA ). T he pr opert ies of PLA [6]
are int eres t ing; t he one we highlight is it s
melt ing t emper at ure as it is relat iv ely low,
be tween 130 - 180 ºC mak ing it an ideal
mat erial f or 3D print ing. I n addition t o the
proper ties t hat this plast ic has tha t perfec t ly
adapt t o our needs, it is a plas t ic obtained f rom
fer ment ed v eget able st ar ch. In other wor ds, it is
a plast ic t hat does not c ome from petr oleum.
2.1.2. P ro tot yp e parts
This prot ot y pe CanS at (Figure 1) , was divided
into t hr ee part s. The lower par t was where the
batt er y and two S D car ds would be housed. The
middle par t, a c irc ular piec e 3 millim eter s thick ,
serv ed as t he lid of t he lower part and t he bas e
of t he upper part . Finally, t he upper par t was t he
st ruc t ure that would house all t he s ensors , the
Arduino UNO boar d, and t he G P S antenna.
The lower part (Figur e 2) has t hr ee pr ot ect ed
areas; t he f ir st two on the s t arboar d and port
side of the CanS at are symmet ric al and one
mor e in t he aft ar ea. I n addit ion t o pr ot ect ing
batt er ies and S D mem ory cards , t his is t he
place where t his part connect s to the r est of t he
CanSat 's part s .
The upper part has three columns loc at ed at
120º and whose t hick ness is 10. 6 m illimet ers .
Thes e colum ns allow having an inter ior s pace
where all t he sens ors were loc at ed. Mor eover,
we would find a nother cir cular cov er at t ached t o
the c olumns in t he upper part . T his c over has
two holes , t he f irs t and centr al one where t he
eyebolt t hat would j oin t he parac hut e wit h t he
CanSat would be locat ed. T he s econd hole was
used t o pass t he cables from t he lower part to
the upper part .
The piec es of this f ir st CanSat pr o t ot ype wer e
j oined wit h polym er glue.
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Figur e 1 . CanS at Pr o t otype V er si o n 1.
Figur e 2 . L ower part sect i on CanSat P r ot ot y p e
Version 1 .
2.1.3. 3D P r int i ng
The 3D print ing was carr ied out , leaving a
square m esh ins ide t he st r uct ur e, whic h allowed
saving weight , c ount ing both the mesh and the
outer layer , which was solid. A s a res ult , we only
used 30% of t he material c ompar ed t o mak ing
the whole f igur e solid.
2 . 2. Ver s io n 2
We did not hav e t he opport unit y to pr int t his
second pr ot ot ype, alt hough it would hav e
allowed us t o cor rec t err ors t hat we had
detec t ed af t er submitting t he first prot ot y pe t o
some tests.
2.2.1. M ater ial s
The m a ter ials us ed were the s ame as t he first
prot ot ype : P LA plastic and polym eric glue.
2.2.2. Pr otot yp e part s
This sec ond prot ot ype (F igure 3 ) had two
pieces, t he f ir st lower par t f ormed by t he lower
part ment ioned abov e and t he cir cular piece
that ac t ed as a lid. The s econd part was very
similar t o t he upper par t ment ioned bef ore.
The lower part ( Figur e 4 ) in t his prot otype was
going to be t he s um of t he lower par t of the f irst
prot ot ype and t he int er mediat e part , and it also
includes t hr ee holes wher e t he upper part would
fit . It also c ont ains f our holes t hat have the sole
purpose of being places t o pass cables f rom the
lower part t o the upper par t o f t he o ther way
around. Unlike t he pr evious prot ot ype, the rear
area is c over ed, allowin g acc ess t o t he inter ior
area only t hr ough t he f r ont part prot ecting mor e
component s .
The upper area would be very similar to the one
ment ioned in t he f irs t pro tot y pe. The m ain
changes would be s ome bar s in t he lower area
of t he three c olumns that would be inser t ed in
the ot her piece of t his prot ot ype. I n addit ion, we
implem ented c hanges t o r educe the widt h of t he
columns and round of f their inner edges. It
would also include f our holes in the upper part
to allow dif f er ent accesses, t hus reduc ing the
number of c ables needed.
Figur e 3 . CanS at Pr o t otype V er si o n 2.
40
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Figur e 4 . Low er part s ection CanSat P r ot ot y p e
Version 2 .
2.2.3. 3D P r int i ng
The 3D pr int ing would have been carried o ut
following t he m et hod prev iously m ent ioned in
the f ir st protot ype, alt hough slight c hanges
would have. T he lower and u pper part s would
have a dif f erent m esh at this prot otype . T h e
lower par t would hav e been print ed wit h a mesh
of 90%, while t he upper part would have a m e s h
of 45%.
As a r esult, in addit ion t o incr easing t he weight ,
we would not hav e h ad t o ins ert ballast , t hus
occupy ing spac e, which would hav e allowed us
to lower the c ent er of gravit y, thus improving
st abilit y dur ing t he des cent . I n addit ion, t he
CanSat would be posit ioned in t he opt imal way
to open t he par achut e in a s horter time.
3. R esul t s an d disc uss io n
The P rim ary Miss ion t hat the OrbiS at team
planned worked per f ect ly , fulf illing all t he
requir ement s r equest ed by ESE R O Spain. T he
maxim um height t hat the r ock e t r eached was
532.7 ± 1. 5 meters , which was lat er c heck ed
corr ect ly by the organiz at ion.
In t he height gr aph ( Figure 5 ) , it is poss ible t o
observ e t wo peaks after the max imum point of
the gr aph. T he r ock e t itself creat ed t he f ir st one
when the war head deploy m ent. T he rocket
made a sm all char ge explode t o deploy t he
warhead, and sinc e t he sat ellit e was s t ill ins ide
the r ock et, it c ould det ect t hat press ure spike.
The par achut e' s opening caused t he s econd
one since it t ook 2 sec onds to open fr om being
fully f ol ded.
Figur e 5 . H ei g ht gr a p h O r bi S a t launch July 20 20.
On the ot her hand, the S econdar y Mission was
not s o brilliant s ince we had the f ailure of t he
CO2 s ensor , and even hav ing chec ked its
corr ect oper at ion t he day bef ore, it gav e
complet ely err oneous and meaningless dat a.
Ther ef ore, af t er analyzing t he s ensor data, we
had no choice but t o dismiss i t and not tak e its
infor mat ion as relev ant .
The r est of the s ensor s of t he S econdar y
Miss ion work ed perf ec t ly and wit hout problem s.
As we had predict ed, the str ucture ended up
yielding at t he weakes t point . O n c e t h e
compet it ion was over and analyzing t he debr is,
we could see t hat becaus e we had t o load
ballast t he day bef or e t he launch and that t his
ballast exc eeded t he a llowed dim ensions , we
had to br eak a j oint. Unf or tunat ely, when we
reass embled t hat j oint, we did not c lean well t he
surf ac e of t he old adhes ive, and we added new
adhesive on t op of it , creating t iny air chamber s
as we f eared t hat r esult ed in t he break age of t he
lower par t of the CanSat .
As we thought that a slight possibilit y of break
could occ ur at t he lower part of the CanSat , we
att ac hed t he bat t ery t o the main body of t he
CanSat . If the situat ion of that breakage
occur red, t he operation of t he s at ellit e would not
be compr omis ed, and it could c ontinue
operat ing wit hout problem s. So t hat
cont ingency plan work ed perf ec t ly.
CanSat regulat ions requir e a m inimum weight
of 300 gr ams , but thanks t o t he 3D pr int ing used
and the des ign, our c asing had s uch a low mass
that we init ially lack ed 12 5 gram s. T his problem
would have been solv ed wit h t he s econd
vers ion. However , in a c ase closer to t he r ealit y
of launc hing a sat ellit e int o or bit, ev ery gram
saved is money .
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4. Conc l usi ons
Af t er the v arious argum ents expos ed
previous ly, we c onclude t hat t he fir st design we
made was out s t anding sinc e it demonst r ated its
capabilit ies in t he c ompet it ion t o achiev e t he
second pos it ion. Mor eover , it was a fir st t est
prot ot ype of s ever al t hat wer e expec t ed t o be
manuf act ur ed but t he pandemic f or ced t o
modif y t he plans wit h little t im e t o act.
The s econd pr ot oty pe would have s olved t he
biggest problem we had dur ing the c ompet it ion,
the br eakage of part of our CanSat. However , it
would have also helped t o im prov e t he
aest het ics and pos sibly would have allowed us
to be in t he firs t posit ion.
The open c oncept des ign avo ided many
problem s and gave us many options in the days
befor e t he f inal. F or exam ple, after having som e
sever e f ailures in t he cont rol boar ds, it allowed
us t o int roduc e an Ar duino Uno board in t he
CanSat , som et hing t hat other t eam s did not
underst a nd how t o f it. Consequent ly, it has
advant ages when t r ansf er ring it t o ot her t y pes
of s econdar y missions other t han our s. Also,
this design has allowed us to hav e more
accur at e dat a, espec ially in t emper at ure, s ince
no heat pr oduced by t he CPU and gas s ens or s
alter t he meas ures .
Ackno wl edg emen t s
I would lik e to thank the S ant o A ngel sc hool f or
their suppor t and spons ors hip t hrougho ut t he
proj ec t . I would also like to thank the City
Council of G avà f or sponsor ing the nat ional
launch cam paign in G ranada a nd the whole
ESE RO S pain t eam f or organiz ing t he CanSat
Spain 2020 com pet it ion wit h all t he diff ic ult ies it
entailed due t o t he pandem ic.
Referen ces
[1] E SERO. ES 2020 GE TTIN G STAR TE D
WIT H CANS AT : htt ps: //es ero. es / wp -
cont ent / uploads/ 2019/ 10/ T 08_G et t ing_S
tar t ed_wit h_CanSat . pdf , last vis it ed: 5 th
Febr uary 202 0.
[2 ] FRUITY C HUTE S PROF ESSIONAL
AEROSP ACE RECO VERY
SOL UT IONS :
htt ps :// fruit y chut es.com / help_f or_par ach
utes / parac hut e -
help/how_t o_m ake_a_p arachut e. ht m ,
last vis it ed: 5 th July 202 0.
[3 ] ESE RO.E S 2020 DESIG N Y O UR
PARA CHUT E : h ttps ://es ero .es/w p -
cont ent / uploads/ 2019/ 10/ T 10_Par achut e
_Design. pdf , las t visit ed: 5 th Ju ly 202 0.
[4] ESE RO.E S 2020 C OMMUN IC ATIN G
WIT H RADIO : http s ://e se ro .e s/wp -
cont ent / uploads/ 2019/ 10/ T 11_Radio_Co
mm unicat ion. pdf , las t visit ed: 15 th June
202 0.
[5] ESE RO.E S 2020 MEET ARDUI NO :
htt ps :// es ero. es/wp -
cont ent / uploads/ 2019/ 10/ T 04. 1_Meet _A
rduino_C. pdf , last vis it ed: 20 th Januar y
202 0.
[6] J. Lunt, Lar ge - sc ale produc t ion,
proper ties and com mer cial applic at ions
of poly lact ic acid polymers , Poly mer
Degradat ion and St abilit y , 59, 1, 145 -
152 , 1998 .
42
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Page 1 of 5
T O L O S A T p r o j e c t : G r a v i m e t r y a n d C o m m u n i c a t i o n
Knigh t Trista n 1 , Rou sse Axel 2 , Allietta Clémen ce 3 , Bérat Benja min 4
___ _____ _____ _____ _____ __ _____ ___ ______ ____ ___ _____ _____ ____ ___ __ ____ _____
Abs tract
The use of Constellatio ns fo r weather scienc e, security and disaster mo nitor ing is a major ch alleng e for
space application services. Satellite to sate lli te com munication using existing constellatio ns has not
been exte n sively explored yet. It ca n improve t h e communication ti mes fo r sm all -satellite missions which
have limited access to gro und sta tions. T hu s, a m ission to demonstrate th e fea sibility of th is link is
requir ed.
Another elemen t of interest in space application is Ear th Ob servation, espe ci ally in t he co nte x t of Clima te
Change. Gr avimetry allows an understanding of mass transport in the Earth System t hr ough the r em ote
sensing of the time variation of the Earth gravity field. Cub eSats ar e low - cost small- scale and hen ce
lower risk solutions to Earth Obser vation m is sion s. University CubeSats ha ve shown th eir success in
demon st ration and scientific m issions, and ha ve a great potential in pr ovidin g students with pra ctice and
application o n real space syste m s.
In th is conte xt, th e stu dent association s ASTR E and SUPAERO Cub eSat Club h ave joined in a Cube Sat
progr am called TOLOSA T , with the hope of demonstrating such technologies. Gathering 70 stu dents
from T oulouse, the team was split into subsystems in acco r dance with th e concurrent engineer ing
principles. The work performed follow ed rec omme ndations fr om exp erts from the Frenc h National
Centre f or Space Studies (CNES) and the ind ustry.
The TOLOSAT payl oads have to te st an d dem onstr ate new mea ns o f measurin g gravity and add ressing
commu nication issu es. Firstl y, for the gravimetry mission, ou r approach relies solely o n GNSS to
compute the g r avity field, a voiding e xpensive gravim eters. For the communication mission: the Ir idium
constellation will be used as a n int er mediate b etween t he CubeSat a nd t he g r ound sta tion. O ff-th e-shelf
compon ents such as patch antennas a re p lanned to pr ove their efficiency in orbit. T his would imp rove
the coverage a nd the c om munication window.
The pr eliminary design was c om pleted. TOLOSA T was de si gn ed as a 3-unit nanosatellite, on a 97.4°
inclined, 500km high orbit. Ma rg ins wer e a lso en sured to allow a third pa yload to be de fined in the future,
that will be use d for fi n ance and partnerships.
Detailed designs are still required, b ut the ed uc ational pur p oses hav e bee n fulfilled, in t er ms of discover y
of the d evelopment of spac e m issio ns as well as in th e tea m work cultu re. T he te am is now mo ving on
to a n ew phase, dedicated to a more detailed co nception with an on -going focu s on th e intr o duction to
students to technical - but not only - fields of k no wledge applied to space systems.
Keywords
Gravime try, I ridium, Students
___ _____ _____ _____ _____ __ _____ ___ ______ ____ ___ _____ _____ ____ ___ __ ____ ___
1 Knight Tr istan: Univesité Paul Sabatier, Fra nce, [email protected] m
2 Rousse Axel : ISAE-SUPA E RO , F rance
3 Allietta Clémence: ENAC, France
4 Bérat Benjam in: ENSE EIHT, France
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1. Introduct ion
This pape r goes in de tail over the TOLOSAT
student pr oject and its current state as of Marc h
2022.
Section 2 details all ma in aspects o f the syste m
ranging f rom technical to fi nancial progress. It i s
importa nt to not e that the p r oject is se parate d
into subsystem teams which each f o cus on o ne
aspect o r system of the project. In subsectio n
2.1 the two payload t eams f o r Gravimetry an d
Iridium e x p lain th eir me thodological approac h
and expected r esults. T he systems and mission
analysis te am’s role are cove red in subsec ti on
2.2 , and subsection 2.3 separ ates the sp ace
segmen t in the wor k carried out by ea ch of th e
six te chnical teams. Finally, the financ e a nd
partn ership aspect of the m ission is addre ss ed
by subsectio n 2.4 .
2. Result s, progress and discussion
TOLOSAT students achieved the preliminar y
design. Our satellite was designed as a 3 unit
nanosate llite, on a 97.4° inclined, 50 0k m high
orbit. Margins we r e also e nsured to allow a
possible thir d payload to be defined in the
future .
2.1. TOLOSAT pa yloads
The TOLOSAT payload s have to test a nd
demon st rate new m ea ns of measuring g r avity
and ad dressing communic a tion issues.
2.1.1. Gravim etry payload
Our gravimetry mission relies solely on GNSS
to com pute th e gravity field and dr aw a ge oid
(Figu re 1.) (while satellites typically de du ce the
gravity field fr om their orbit using com plex an d
expensive o n -b oard g ravimeters c oupled with
GNSS data [3]).
Figure 1. Earth's ge oid as seen by European
satell ite GOCE (credit ESA) [1]
This does not requ ire h eavy e quipment and was
selected for t h e mission. T his method was fir stly
describe d in detail b y Ales Bezdek and al. [1 ].
Their work highlights th at m apping the g r avity
field could be done without heavy a nd costly
equipm ent, that is why we have based o u r
studies on their r esearch.
Here is a brief sum mary of the a cceleratio n -
based method:
The calcula tions are based on the fa ct that the
geoïd is a n eq ui p otential. Thus , on e has to solv e
a Laplace equation, E q . 1:
𝛥 𝑉 = 𝜕 2 𝑉
𝜕𝑥 2 + 𝜕 2 𝑉
𝜕𝑦 2 + 𝜕 2 𝑉
𝜕𝑧 2 ( 1)
It could be demonstrated th at the solution of thi s
equation is of the following form, whic h
introdu ce Legendre p olynom and Stokes
coefficients, in Eq. 2 :
𝑉 (𝜃, 𝜆 , 𝑟 ) = 𝐺𝑀
𝑟 ∑ ( 𝑅
𝑟 ) 𝑛 ∑ [ 𝐶 𝑛𝑚 𝑐𝑜𝑠 ( 𝑚𝜆 ) +
𝑛
𝑚= 0
∞
𝑛 =0
𝑆 𝑛𝑚 𝑠𝑖𝑛 ( 𝑚𝜆 ) ] . 𝑃
𝑛𝑚 ( 𝑐𝑜𝑠𝜃 ) ( 2 )
This eq uation can be simplify in Eq. 3 :
𝑉 (𝜃, 𝜆 , 𝑟 ) = ∑ [ 𝐶 𝑛𝑚 𝑉 (𝑐) (𝜃 , 𝜆, 𝑟 ) +
𝑛 ,𝑚
𝑆 𝑛𝑚 𝑉 (𝑠) (𝜃, 𝜆 , 𝑟 )] (3)
This solution is a development in spherical
harm onics. Thanks to the four main GNSS
constellations (GPS, GLONASS, GALIL EO an d
BEIDOU) the latitude, longitude and altitude of
the satellite in the Ear t h Center Ea rth Fixe
(ECEF) fr ame ar e known. After convert ing th e
position in the East North Up (ENU) frame , th e
position became 𝜌 (𝑟, 𝜃, 𝜆 ) , where the
param eters are respectively the altitude,
latitude a nd longitud e of the satellite.
Then , its a ccel e ration c an be computed by a
numer ical d erivation thanks to a Golay filter.
The acceler ation is decomposed in a s um of
contribu tions, in Eq. 4:
𝑑 2 𝜌
𝑑𝑡 2 = 𝑎 𝑔𝑟𝑎𝑣 + 𝑎 𝐿𝑆 + 𝑎 𝑡𝑖𝑑𝑒 + 𝑎 𝑁𝐺 + 𝑎 𝑅𝐸𝐿 =
𝑎 𝑔𝑟𝑎𝑣 + 𝑎 𝑜𝑡 ℎ 𝑒𝑟 (4)
With:
● 𝑎 𝐿𝑆 and 𝑎 𝑡𝑖 𝑑𝑒 the acceleration due to
lunisolar p erturbations a nd tides
● 𝑎 𝑁𝐺 and 𝑎 𝑅𝐸𝐿 the acce le ration due to
relativity an d non g r avitational forces
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By applying t h e th i rd Newt on’s law, thi s
accelera tion ca n be linke d to the g radient of t he
potentia l which is g iven by applying the na bla
opera tor to Eq. 3 . Eq. 5 :
𝑎 𝑔𝑟𝑎𝑣 ( 𝜌 ) = 𝛻𝑉 (𝜌 ) = ∑ [𝐶 𝑛𝑚 𝛻 𝑉 ( 𝑐 ) ( 𝜌) +
𝑛 ,𝑚
𝑆 𝑛𝑚 𝛻 𝑉 (𝑐) ( 𝜌)] (5)
Then , the only things which rema i n u nknow n
are th e S to kes coeff icie n ts 𝐶 𝑛𝑚 and 𝑆 𝑛𝑚 . The se
coefficients can be determine d by a pp lying t he
least squa re met hods to this last equation.
Then , all th e terms of the spherical harmonic
developm ent in Eq. 2 are known and one has
access to th e local gr a vity potential.
2.1.2. Iridium payload
Nowadays com m unications with sa te llites are
enabled by ground stations and limited by th e
rare p asses of a sa tellite over a n accessibl e
groun d station.
The TOLOSAT m ission pr oposes a different
type of p rotocol: exploit an e xisti ng
telecomm unication constellation (namel y
Iridium Next) in order to make a relay betwee n
the g round and the sat e llite. T his add ition al
passage ma y enable com munication with the
groun d much m ore frequently: there are inde ed
up to 66 Iridium satellites an d multiple Ir idium
groun d stations.
Several aspects make the Ir idium mission
tricky.
First, the Iridium satellites’ bea ms take th e for m
of visibility cones th at are de signed so that th e
Earth’s surfa ce is entir ely covered (Figure 2.)
Figure 2. Cover a ge of Iridium Next Constellation
on ground [ 2]
As the a ltitude rises, th e cove rage ensured by
the cones decreases, which fixes an important
constra int for our 50 0 km high satellite:
● The s atellite must be in the visibility
cones.
Second, th e existen ce of th e Doppler effe ct
furthe r reduces the total time visibility of o ur
nanosate llite. The Iridium antennas are inde ed
sensitive to the Dopple r f requency shift. T he
modem algo rithms hence imposed an add itio nal
requir ement:
● The frequency shift caused by the
Doppler eff e ct should be lim it e d to +/-
37.5 kHz.
According to certain s ou rces (includin g
specialists from aerospace industry), the time
derivative of the Dop pler ef fect (the Doppler
rate) would also affect the commu nication. Thi s
has to be pr oven and backed by precise valu es.
These two con straints set a limit a ltitude o f
650km and a m i n imum elev ation angle o f 2 4°
for o ur satellite. Fo r a 6 hours covera ge
simulation, we obtained the followin g
estimation s of Tabl e 1:
Tab le 1. Table w ith visibility res u l ts for a 6 hours
cover age simulation [ 1]
Mean time
session
Nb o f
session s
To ta l t i me
visibility
Onl y
visibility
104s
31
214 m in
Wi t h
Doppler
ran ge
51,6s
39
134 m in
Wi t h
Doppler
ran ge
and delta
Doppler
63,5s
8
8 m in
When it comes to hardware ch oices, th e Iridiu m
subsystem selected a L- band antenn a
(1621 MHz) which has been subject to a lin k
budget, and an Iridium mo dem which is in te ste d
and o perated tha nks to a PCB ( Printer Ci rcuit
Board) and driver software the su bsystem
develope d.
2.2. Systems & mission an alysis
The System engin e ering subsystem is in ch arg e
of crea ting and managing the co mple x
architecture of the TOLOSAT project, seen as a
whole system including the nanosatellite, th e
groun d segme nt and the launcher.
This wor k requires the collection of data amon g
all subsystem s. The data is then formatted an d
well-structured th rough the Valispace br owser,
making sur e there are no wrong assumption s
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4 th Symposium on Space Educational Activ ities
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Page 5 of 6
Figure 6 . Vertical (top) and Horizontal (botto m)
errors obt ained with (blue) an d without ( red)
Klobuchar model .
Figure 6 depic ts the ef fec t of cor rectl y modell in g
the io nosph eric del ay on th e user c o ordinat es .
For th is p urpos e, the proc e ss is exec uted t wice.
In the fir st run ( w hos e res ults are depic ted in
blue c olour) , we appl y t he full S PS m odell ing,
with al l ter ms of Eq.1 inc luded . In the s econd
run (dep icted in red c olo ur) , we intent ion all y
disconn ect the ionos pher ic m odel, mainta inin g
all oth er proc ess ing opt ions f rom the SPS
unchan ged.
W e can obs er ve tha t t he vertic al c om ponent of
the error is degr aded b y a f actor three when t he
ionos pher ic de la y is not c or rec ted. As it ca n be
seen, th e ver tica l pos ition error is link ed to the
ionos pher ic de la y mode lling pre vious l y depic ted
in F ig ure 5 . T he bott om plot depic ts the
horizont al com ponent of the error , b y plott ing
the Nort h vs t he East err or. In th is cas e, we do
not appr eci ate a d egrad ati on of the err or.
T he reason f or s uch as ym m etr y in the ver tica l
and hor izo ntal is an exam ple of quest ion pos e d
to the s tude nts us ing g LAB i n the l aborat or y
sess ions. T he a na lysis of the res u lts ra ises
interest in g ques tions and discus sions that l ink
the obs erve d results w ith the t he oretica l
aspect s seen in t he lec ture s.
5. Conclus ions
gLAB is a usef ul tool to lear n about G N SS d ata
proces sing or to expa nd a n y prior k no wledge.
Using actua l dat a s ets c olle cted b y t he public l y
availab le IG S net work , we give a n exam ple of a
straight f or ward proc edu re ta ilore d to
understa nd an d ques tion th e eff ec ts of dif fer ent
error com ponent s in bot h SIS dom ain and the
T he gLA B tool su ite can be
downloa ded toget her with diff erent B ook s and
T utorials on GN SS Dat a P roces sing f rom our
w ebsit e gage. upc. edu.
Acknowledge ments
T he present wor k was suppor ted in par t b y the
by proj ect R T I2018 - 094 2 95 -B- I0 0 f rom the
Agenc ia Españ ol a de In vesti gaci ón of the
Spanish Mi nistr y of Sci enc e, Inn ovati on and
Univers ities MCI N/AEI 1 0.1 3039 /50110 001 103,
whi ch is co - founded b y th e FEDE R progr am .
T he aut hor s ac k nowledge t he us e of data a nd
products pro vided b y the Inter natio na l GNS S
Servic e.
Referen ces
[1] Park inson B, S pilk er J, Enge, P. “G loba l
Position ing S y s tem , Vols
I and II , T heor y
and Ap plic ations ” Am er ican Insti tute of
Aeronaut ic s: Res ton, V A, U SA, 19 96.
[2]
Hofm ann -
W ellenhof B, Lic htenegg er H ,
W asle E (2008) G NSS
–
GlobalNa v igatio n Sate llit e S ystem s .
Springer , Vienn a, Austr ia
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“Spri n
ger Ha ndbook of Global Nav igati on
Satellite S ystem s ” Spring er Cham , Berlin
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Sanz J, J u an JM, Hern ánd ez -
Paj ares M ,
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[10] Interna tiona l T elecom m unic ation Unio n
(2021) “ IT U - R: Ma nagin g th e rad io
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Ibáñe z - Segura, D. Ro v ira -
Garc ia A,
Alonso, MT , S anz J, Jua n JM, Gonzá lez
-
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Martí nez M. “EG NOS
1046 Maritim e Service As ses sm ent”.
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[13]
San z J, Ro vir a - Gar cia A, Her nán dez
-
Pajares M, J u an J M, Ventur a -
T raveset J ,
López -
Ech azarr eta C, "T he ESA /UPC
GNSS -
Lab T ool (gL AB): An adva nce d
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l and prof es sio nal pac k age f or
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Space Appl ications , Ju l. 2 012
[14] United Sta tes D epartm ent of Def ense
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Standar d Pos iti oning Ser vic e
Perf orm ance Sta ndard .
[15] Beutler G , Ro thach er M , Schaer S,
Springer T , Kouba J , N eilan R. T he
Interna tiona l G PS Ser vic e (I
GS) : An
interdis cip linar y ser vice i n suppor t of
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325 – 331
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Analysis of planetary sp acecraft images with SPICE
Teresa Peña
1
, Manel Soria
2
, Paula Betriu 2 , Enrique Garc ía- Melend o 2
__________________________________________________________________________
Abstract
S pacecraft images are an invaluable source of information in Planetary S cience. However,
they must be proce ssed and the ini tial stage is to navigate them , i.e., de termine the longitude
and lati tu de coordinates of each pixel on the image plane. The mai n goal of the present work
is to develop an open - source tool to do so. It will be independent of proprietary software and
implement ed in a widely used languag e (Java, Python ). It will be able to analyse planetary
images taken by different spacecra ft, such as New Hori zons, Cassini or Voyager , with mini mal
user intervention . Here we present the first steps of the process ill ustrating the techniques to
navigate an image of an ell ipsoidal body , obtained from mi ssion kernels using NASA Jet
Propulsion Laboratory SPICE library , considering that the att itude and position of the
spacecraft are available ; correct the camera attitude information; determine the image
resolution for each pixel; and combine different images of a body to generate mosaics with
high resolution.
Keywords
Planetary Scienc e, Planetary Image Processing , SPICE , Open Sof t ware
__________________________________________________________________________
1
Universit at Poli tècnica d e Cataluny a , ESEIAAT, teres a.pen a@estud ianta t . upc.edu (Student)
2
Universit at Politècnica de Catalunya, ESEI AAT, Aerospace Engineering / Physics De partment, Spain .
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Nomenclature
CCD Couple - Charged Device
FOV Field of Vi ew
SPICE Spacecraft Plane t Instrument C -
matrix Event s [4] .
1. Introductio n
Spacecraft images are an inval uable source of
informat ion in Pla netary Science . To mention
just one exa mple, in atmosphe ric science they
can be used to measure wind velocities and
track the ev olution of storm s [1 ,2 ] . The first step
to process the planetary images is usually to
navigate them [3] i.e., determine the longit ude
and latit ude coordinates of each pixel on t he
image plane. In order to do so, accurate
informat ion about the position of the spacecraft
and the attitude of the optical inst rument are
crucial . These data are usually pr esented in t he
form of kernel files generated by the mission
and processed with the SPICE library [4] .
However, attit ude ker nels (C - kernels ) ar e
sometimes not available at all (Voyager) or not
entirely accurate ( Cassini [5]).
Many resear chers have put thei r effort s on
finding the way to proces s the images with very
precise data sets. In [6] a photogrammetri c
control network to generate accurate mosaics of
Jupiter’s moon Europa is developed . In [3] , the
authors present a software package called PLIA
(The Planetary Laboratory for Image Analysis)
to navigate and process images from di fferent
missio ns . The present work is aimed to
eventually develop an open - source tool for
planetary i mage analysis that does not rely on
proprietary software (such as IDL or MATLAB),
minimi zes the need of human inte rventi on in the
navigation process , provides an estimation of
the navigation error for each image and can be
used to process images of different missi ons.
Here , as a first step towar ds the af orementioned
goals, we present algori thms to (a) Navigat e an
image of an elli psoidal body , assuming that the
exact attitude and position of the vehi cle are
available; (b) Correct the camera attitude
informat ion; (c) Obtain th e image resolution for
each pixel; and (d) Combine different images of
the same body in a mosaic to obtain a fu ll
projection, choosing t he best resolution
available for each region .
2. Image projection from known
spacecraft position and instrumen t
attitude
As suming that the attit ude of the camera and
the position of the spacecraft are perfectly
known , the nav igation of the images could be
performed with the algo rithm outlined in this
section. An exam ple of an i mage where lit tle
correction is needed is presente d in Figure 2.
2.1. Project ion of a point i n the i mage plane
Consider a poi nt on the body surf ace (Figure 1),
expressed in its fixed frame,
𝑃
(
𝑋 ! , 𝑌 ! , 𝑍 !
) , T he
rotation matrix from the body frame to the
instrume nt frame, at the instan t of the image,
can be obtained from the kernel data with the
SPICE function cspice_pxform . Afterwards, the
rotated vector is translated to th e location of the
instrume nt by determining the rel ative position
of the frame with SPICE function
cpsice_spkpos .
Once the position of
𝑃
(
𝑋 ! , 𝑌 ! , 𝑍 !
) is expressed
in the fra me of the instrum ent as
𝑃
(
𝑋 " , 𝑌 " , 𝑍 "
) , it
is projected on the image plane and converted
in to pixels, using the intrinsic matrix of the
camera [7] :
𝐾 =
⎣
⎢
⎢
⎡
± #
$ 0 c %
0 ± #
$ c &
0 0 1
⎦
⎥
⎥
⎤
(1)
where
F
is the focal length of the camera,
ρ
the
size of the pixels and
c %
and
c &
the coord inates
of the optical centre of the FOV (point C in
Figure 1) . The homogene ous coordinat es of
𝑃
6 (
𝑢′, 𝑣′, 𝑤′
) can be expressed as:
;
u '
v '
w '
?
= K ·
;
X (
Y (
Z (
? (2)
and finally converted to Cartesi an with:
Figure 1 . Proje ction o f a sur face p oint i n the
image p lane
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𝑢 = ) !
* !
𝑣 = + !
* !
(3)
i n order to obtain t he coordinat es of
𝑃
6 , the
projection of
P
.
2.2. Image navigation
The navigat ion of t he image i s carried out
scanning each pi xel of the CDD to determine if
there is a surface point of the pl anet projected
on it and visible from the spacecraft. To do so,
the intersection points between the ellipsoi d and
a l ine of si ght , which emanates from the centre
of the i nstrument
𝑂
(Figure 1), goes through the
pixel
𝑃
6 considered and continues to infinit e, has
to be obtained .
The equation to determine the inter section
between the line of sight and the ell ipsoid can
be expressed as:
(
𝑆 + 𝜆 𝐿 − 𝐶
)
, 𝐴
(
𝑆 + 𝜆 𝐿 − 𝐶
)
= 1
( 4)
where
𝑆
is the position of the spacecraft , the
scalar
𝜆
(the unknown) is the distance between
the center of the ins trument frame
𝑂
and the
body,
𝐶
is the center of the body ,
𝐴
is a
parametri z ation matrix descri bed below and
𝐿
is
a unitary vector defining the line of sight of each
pixel . A ll the magnitudes are expressed in the
reference frame J2000 (equivalent to the
International Celestial Reference Frame [8] ).
𝐿
is the ve ctor of the line of sight expressed in t he
frame of the camera. Regarding the matrix A,
defined in the pri ncipal axes of the ellipsoid and
composed of the equatorial
𝑟 -
and pol ar
𝑟 .
radii
of the body , it is:
𝐴 =
⎣
⎢
⎢
⎢
⎡
/
0 "
# 0 0
0 /
0 "
# 0
0 0 /
0 $
#
⎦
⎥
⎥
⎥
⎤
(5)
Eq. 4 is expressed as a second - degree
equation , whos e discriminant
∆
is solved . W hen
its value is null or positive, the line of sigh t
intersects t he ellipsoid in one or two points,
respectively . T he smaller value of
𝜆
is the one
referring to the point in the near - fac e of the
body . Then , the surface points of the ellipsoid
are calculated and converted from J2000 to the
body - fixed frame by means of a rotation and a
tra nsla tion as described in sub - section 2.1.
A part from imposing that the intersection point
must be on the edge or inside the body, it is also
necessary that it is illuminated to be seen fr om
the spacecraft and shown in the image.
Function cspice_illumin from the SPICE library
is used w ith this purpose.
Once the previous require ments are verified,
the longitud e and latitude associated to the
surface poi nt proj ected in each pixel are
computed . These values can be obtained with
two SPICE function s , cspice_reclat or
cspice_recpgr , de pending on the system that
wants to be use d to express the lon/la t v al ues,
the planetoce ntric or the planeto graphic one.
2.3. Image projection
In order to obtain the projected image, the
intensity asso ciated with each lon/lat is needed.
Figure 2. Theoreti cal limb of Pluto in New
Horizon’ s image 2 991474 81 [9] . The diff erence
bet ween t he li mbs p osition pr edicted with the
missi on k erne ls and t he i mage can be seen more
clearly in the z oo med area .
Figure 3. I mage p roj ecti on of Plut o fr om New
Horizon’ s image 299147481 [9 ] generated from
Figure 2.
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To com pute i t , we use an interpolation algorithm
based on t he triangulation of the intensity data
obtained from the or iginal image .
In order to consider that the intensity of a pixel
obtained from the interpolati on i s val id, the
surface point associated to it has t o be (a) inside
the FOV of the camera and (b) in the near face
of the planet or moon. The first condition is
verified by co mputing the location of the pixel in
the image plane and, for the second, the angle
between the position vector of the surface point
and the one that has its origin in this point and
its end in the space craft is com puted . If this
angle is smaller than 90º, the point is located in
the near - side of the body and the int erpolated
intensity o f the pixel is main tained.
If one of the previous two conditions is not
fulfilled, the in terpolat ed intensity is changed
into a spe cific value , such as 0 , so in the image
the pixel under consideration is displaye d in
black .
To inc rease t he qu ality of the projection , image
processing techniques ar e used and, more
specifically, sharpening and contrast
adjustment. Th e final result can be seen in
Figure 3.
3. Attitude cor rection fr om known
planetary l imb position
If the attitude of the camera is not perfectly
known , the image navigation provide s wrong
results that lead to unreal ima ge projecti ons or
mosaics . In fact, even the proje ction of Figure 3 ,
where th e kernel is quite ac curate, does not
coincide perfectl y with t hat provided in [ 10 ],
since the longitude is s lightly different.
The in accuracies in the data are manifested as
a displacement of the posit ion of the body wit h
respect to the one that can be seen in the image.
In o rder to correct this mismatch , th e p rocedure
that is proposed here consists of determining
the rotation around the axes of the instrume nt
( with the att itude provided by SPICE) necessary
to make coin cide the position s of the body.
3.1. Limb points on t he image
The ai m of th is work is to provide procedures
that can be used with the majority of images in
which all or a part of the limb of the body is
displayed. However, when t rying to generate
the limb of the planet or moon directly from the
original image, there are f actors that make it
very complicated to do it with completely
automatic methods that do not require the
intervent ion of the user , such as t he presence
of rings in the images of Saturn or the dark
zones of Pluto in the images taken by New
Horizons .
Because of th is, here we propose a method
characteri z ed by the generation of a limb
defined by as many points as desired, whi ch
follow t he limb that can be seen in the image
and are computed in the same way . Thus, is the
user who chooses the zones in which the limb
points should be located and the algorithm
computes the exact pixel . To do so, it first
determines the averag e intensity of th e pixels of
the ba ckground and those of the planet. Then,
the mean of these two values is calcu lated to
know the intensity that the pixel where the limb
point will be located should have .
3.2. Theoretic al limb po sition
As t he points of t he l imb from the i mage a re
expressed in pixels, the limb generated with the
SPICE data (i.e., the theoretical limb) also has
to be exp ressed in th is units in ord er to be
compared.
The theoret ical li mb is defined i n the body - fixed
frame by the main parameters of a conic (i.e.,
center and major and minor semi - axes) ,
obtained from SPICE function cspice_edlimb.
F rom them and the para metric expression of a n
ellipse in 3 - D, an arbitrar y number of points that
are part of the conic can be generated and
afterwards converted into pi xels to be shown in
the i mage. To do so, a rotation and t ranslation
of their position vector from the body - fixed
frame to that of the instrument is performed as
described in previous s ections.
3.3. Correct ion proce dure
To co rrect the mismatch between the limbs of
the body, the frame of the instrument is rotated
causing a variation in t he position of the
theoretical limb. To do this, the rotation mat rix
that ma kes co incide almost perfectly both limbs
ha s to be foun d.
This matri x is de fined by the angles of Euler
(
α, β, γ
) and i s applied to the coordi nates of
each poi nt of the conic expressed in t he f rame
of the instrument:
;
X " !
Y ( !
Z ( !
?
= 𝑅 1
(
γ
)
𝑅 2
(
β
)
𝑅 3
(
α
) ;
X (
Y (
Z (
? (6)
To find the combination of angles t hat
generates the best fi tting, an iterative
minimi zation proc edure is used . The parameter
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to minimize is
𝐷
, the sum of the di stance s
𝑑 4
between each limb point
𝑝 4
and its projec tion on
the theoretical limb conic
𝑡 4
.
𝐷 = 𝑚𝑖𝑛
[ ∑ ] ^ |
𝑝 4 − 𝑡 4
| ^`a (7)
The minimiz ation starts with arbitrary angles,
such as a tenth of the angular field of view of the
camera, and after a few iterat ions t he error is
notably reduced, provided that the number of
limb points is sufficient. Once the right E uler
angles have been obtained, they are used to
generate the correspondi ng rotation matri x.
3.4. Applicat ion of the correcti on to the image
navigation
When the ro tati on matr ix that corre cts th e
attitude of the spacecraft has been computed, i t
has to be applied to the image navigation
procedure and, more specifically, to the pointing
vector (
𝐿
in Eq. 4) used to defined the position
of each pixel of the CCD.
In the cas e presented in Fi gure 5, the Euler
angles are (0.0024
°
, - 0.0032
°
, 0.03 52
°
) and the
total distance or error between limbs is 0.814
pixels.
4. Generati on of i mage mosai cs
An i mage mosaic can be def ined as the union
of multiple image projections, in such a way that
the range of longitude and latitude displayed is
wider th an the on e t hat coul d be shown in each
individua l image projection. For ea ch pixel, t he
image w ith best resolution is selecte d.
The resolution in pixels/meter is com puted as
the square root of the surface that covers each
pixel , which is define d by the m ean verti cal and
horizontal distances between t he pixel whose
resolution wants to be determined and the
adjacent pixels i n each direction. As the pixels
are associated to a longit ude and latitude ,
Vincenty’s formula [11] is used t o compute t he
geodesic distance between t wo pixels on the
surface of an elli psoidal body.
As wit h t he i ntensity of the pixels in the image
projection , the resolution is also interpolate d to
obtain the correct value associated to the lon/ lat
of the pixels. The inter polation algorit hm is
based , as well, on the triangulation of the
resolution data obtained from the or iginal
imag e.
Once the inten sity o f the pixels and its resolu tion
for each image have been filtered, the data of
the image mosaic can be generated by
selecting, f rom the multiple images, the pixels
with a hi gher resolution.
5. Results & Discussion
To ill ustrate the procedure described in this
article, the image mosa ic of Figure 6 is
presented . Here each image has been
represented w ith a different color for clarity.
6. Conclusions
The results provided c onfirm that the fi rst steps
of the work that will end i n the development of
an open - source tool for planetary i mage
analysis have been completed.
Figure 5 . Co mparison of the theoretical and
corrected limbs and terminators of Saturn in
Cassini ’s i mage 14614 06214 [9].
Figure 4 . Iteration of the minim i z ation in
Cassini ’s i mage N151616 9656 of Encel adus [ 9].
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We are now able to navigat e images obta inin g
accurate longit udes and lat itudes, by means of
a correction procedure based on an estimation
of the camera kernel er ror.
However, there are still a few aspe cts that
should be addressed in the near fut ure : (a) the
Newtoni an light time correction and stellar
aberration correct ion; (b) the analysis of images
in which the kernel files are not available, such
as t hose of Voyager 1 and 2; ( c ) the treatment
of images without limb; ( d ) the esti mation of the
error in the image projecti on due t o inaccuracies
in the attitude of the instrume nt or the selection
of limb points ; and ( e ) the estimation and
correction of the spacecraft position when
multip le star s and a body are visible in the
image.
The final algorithm will be implemented in a
widely avail able and portable language such as
Java or Python.
References
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complex storm system i n Saturn's north
polar atmosphere in 2018 , Natur e
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March 2 022.
[9] OPUS3 Websi te: https://opus.pds -
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lanet,targ et,time1,observa tiondura tion&
widgets=i nstrument, observati ontype,tar g
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[1 1] C. Thomas an d W. Featherstone ,
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Figure 6 . Color ed i mage mosai c o f Rhe a from
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and N149999716 9 [9 ].
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S D R H e l i x A n t e n n a D e p l o y m e n t E x p e r i m e n t ( S H A D E ) o n b o a r d B E X U S
Meli na Koukou 1 , Vasi lis Vel liki s 1 , Ioannis Va rvaringos 1 , Konstantino s Koutro poulos 1 , I oannis
Myrsinias 1 , Despina Ekat erini Argiropoulos 1 , Andr onikos Dourmisis 1 , Ores tis Rafail
Nerantzis 2 , Ioannis Ioann ou 1 , Elli Loukaridou Kizi li 1 , Spyros Megal ou 1
__________________________________________________________________________
Abstract
In t he field of space travel, space communica t ions has always presented a slew o f obstacl es
and hurdles that must be overcome in order to complete a success ful missi on. Space limits
inside a satellite or spaceship, vast dista nces betw een satelli tes and ground stations , and a
phenomenon known as "Faraday R otat ion " in the ionosphere are only a few of the most typical
issues. Sa tellite an tennas must b e s mall, compac t, efficien t, and circularly p olarized as a result
of the aforementioned issues. The heli x an tenna is an excell ent ans wer for all of the
requirements . In this work we de velop a deplo yment and poi nting mecha nism of a helix
antenna opera ted wi t h software defined radio algorithms. The f eatur es of hel ix antennas a re
exceptional, and they are especial ly suitable for sa tellite communicati on. Three coaxial
cylinders, two stepper motors, one pulley, and o ne thread make up a deployment-pointing
mechanism. The mecha nism deploys the antenna along its longi t udinal axis and turns it
horizontally toward s the ground station. During the flight, the antenna is deployed and
retracted. Unde r differe nt position ing situations, the GPS, an altimete r, and a compass
calculate the gon dola's position in order to ro tate the anten na towards the Ground S t ation and
close the com m unication link. The antenna's ro t ation mechanism is tr iggere d by the integra t ed
attitude determination and control sys tem algo rithms in order to correct the pointing and
orientation towards the Ground Station. The antenna uses software defined radio algorithms
to achieve weigh t an d volume reductions while maintaining high efficiency and
reconfigurabili t y. The ex periment includes a high-definition camera that provides real- time
information on the anten na's orienta tion and condition. SHADE 's flight on the BEXUS 28/29
balloo n resulted in ef f ective deployment and tran smission, a s well as t he abili ty to r eceive and
decode trans mitt ed pack ets. The rotati ng mecha nism met the pointing requirements, and all
of the sensor's data was correctly saved to our syste m. Throughou t the trip, there were no
signs of the r mal risk.
Keywords
Antenna D eployment, Helix A ntenna, REXU S/BEXUS , Sof tware Defined Rad io, Stratosp heric
Balloo n
__________________________________________________________________________
1 Corresponding a uthor: Aris totle univers ity of Thessal oniki, Gre ece, mkoukou8 @gmail.com
2 University of M acedoni a, Greece
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Acronyms/Abbr eviations:
ADCS Attitude Deter mination & Control
System
AUTH Aristot le Univers ity of T hess aloniki
BER Bit Error Rate
DMCS Deployment Mechanism Control
System
FEM Finite Element M ethod
GH z Giga-Hertz
GMSK Gaussian Minimum Shift K eying
GNSS Global Navigatio n Satellite System
GS Ground Station
HCS Heating Control System
HPBW Half Power B eam Width
LNA Low Noise Ampl ifier
OBCS Observation Con trol Syste m
PA Power Ampl ifier
RX Receiver
SDR Software Defi ned Radio
SHADE SDR Helix Ante nna De ployment
Experiment
SSC Swedish Space Corp oratio n
TT&C Tele metry Track ing and Comma nd
TX Transmitter
TX CS Transmission Control System
1. Introduction
In space te lecommu nication s ystems, closing
long distance links and F araday rot ation are
major c hallenges face d by engineers.
Stratospheric balloons an d oth er high-altitu de
platforms r egularly us e monop oles to
communicate with the gro und s tation, as t heir
omnidirectiona l pro perties nullify any need for
beam steering. Neverthele ss, monopoles have
low gain a nd linear polariz ation that c ould be
easily affected by Faraday rotation; th erefore,
they require high powe r consumption to
establish a link. Helix ant ennas could offer a
solution to t hese issues, wit h their g ood
gain/cost trad e-off and c irc ular polarizat ion tha t
they provide. Even though they are wi dely used
in aerospace communica tion systems , the
geometry of this anten na type, resembling a
relatively long and w ide spring, often v iolates
the volu me restrict ions set i n spac e
applications.
In ad dition, following a present tende ncy in
research and ind ustry to r eplace conve ntional
communication circuits w ith softw a re cores ,
Software Def ined Ra dio (S DR) techn ologies are
gradually es tablished in the s pace s ector. SDR
offers accurate signa l pr ocess ing applications
without unneces sary phys ical c omponents in
small sized mod ules.
SDR H elix Antenna Dep loyment Exper iment
(SHADE) is an SDR operated helix an t enna
with a s pring-b ased deployment mechan ism
and a Ground- Stat ion-Trac king automation
system. A hel ix anten na, pr otected by a t eflon
cover, is opera ted by an SDR module that
transmits d ata to the g round s tation. To
compensate for t he narrow beam width, an
automation sys tem h as been develo ped in
order t o ens ure t hat th e antenna will always
point at the ground station a nd maintain
Telemetry Tracking and Command (TT &C)
applications. Moreover, a deployme nt
mechanism has been i mplemente d whic h
exploits t he antenna's s pring c harac teristics
ensuring a reduce d size for the s ystem.
The exper iment's potentia l was recogn ized by
REXUS/BEXU S progr amme [1] , [2] and SHAD E
was desi gned, imple mented and had a
success ful flight on bo ard a s tratospheric
balloon.
The s tructure of the pr esen t paper is firstly the
Introduction, s econdly the Mechanical D esign
followed by the Ther mal Des ign; after that is the
section of the Electronics and Softw are and
the n th e last technical secti on, the
Telecommunicat ions section. The final s ections
include the Testing an d Verification an d
Conclusion, on which the les sons lea rned are
described, acknowledg me nts and refere nces
are also cited.
2. Mechanical Design
The Mech anical Design aimed to satisfy the
following r equirements. 1) The antenn a’s
deployment 2) the antenn a’s controlled r otation
3) the overall fixat ion of t he experim ent o n the
gondola 4) BEXUS space a nd w eight limitat ions
5) the safety of the experiment’s assembly
during the “cut- the -r ope” phase. T o ac complish
these r equ irements, the mechan ical des ign
consisted of 1) the Anten na’s C asing, wh ich
contained the helix antenna, 2) the External
Box, which co ntain ed the rotat ional mech anism
and t he m otors for de plo yment and r otation
respectively 3) the Electro nics Box and 4) th e
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hum anities and social sciences, exact sciences
and t echno lo gy, or biom e dical scie nces. Th e
initial trainings of t he influx s tud e nts are very
diver se but s ha re a common thread: that the
stude nts demonstrate a str ong interest in the
space s ector an d t hat the y are a ble t o pro ject
their fut ure self in a topic re l evan t t o space.
In some m ore detail, t he MSS is a 6 0 E CTS
pro gr am, ta ke n up as a 1-yea r full -time o r a 2-
year pa rt-time program (Fig u re 1) . Th e
man dat ory c ommon core of 29 ECTS acquaint
the students with the diff erent aspe cts that
toge the r fo rm t he f oundation of sp ace -related
activities. Mandatory c ourses cover l aw &
policy, spa ce missions and sate ll ite technolog y,
sciences aspec ts and earth observations
Depen ding on th eir backg r ound a n d int ere sts,
the students the n deepen their existing
knowled ge th rough more domain -specific
optio nal cou rses, for a total of 16 ECTS. The se
cour ses cover the d oma ins of (i) Space Law,
Policy, Business and M ana g eme n t, (ii ) Space
Sciences – which is very bro a d and covers
topics ranging from sp ace wea th er to r adiation
physics , to life s ci ence – (iii) Spac e Te c hno logy
and Applicati ons . Stu dents can furt hermor e
choo se cou rses fr om other master p rog ram s at
KU Le uven a nd Gh ent Unive rsity, as l ong as
they ar e appropriate for th eir mast er thesis or
their fut ure profe ssi ona l p roject.
Th e master thesis is the final part of the
inter disciplina ry program, in which the acq uired
knowled ge an d int erdisciplinary skill s are
app lied t o a compl ex and concrete p roj ect. T he
mast er thesis is a fo ur mon t hs p r oject mostly
per for med i n t he s econ d s em ester du ring which
the st udent is embedded in a research team at
KU Leuven or G hent U niver si ty, or at an
exter nal institute, o rganisation or private
par tne r, under th e supervision of an ac ademic
pro mot or.
Th anks to the interuniversity e ffor t of the
pro gr am, stud ents get e mbedded in the
acad emic r esea rch expertise of two
inter nati onally-ranked Belgia n universities.
Fu rthermore, the pro g r am benefits f rom high-
pro fil e lect ure rs, in cluding F r ank De W inne, one
of two Belgian astronauts, or Prof. Sarah
Baatou t, he ad of th e Radiobiolo gy Unit of the
Belgian N uclear Research Ce ntre; as w ell as
sever al int ernational experts speaking in the
year ly lecture s eries of th e KU Leuven Ce ntre
for Global Governance Studies.
Fina ll y, ex tracurricular initia tives ar e ta ken to
brin g the stu den ts i n contact with actors in the
differ en t fields of sp ace stu dies. Each year
stude nt exc ursions are organised, including
visits to the E uropean A stronaut Center in
Cologn e, Ger many and the E uropean Space
Resear ch and Researc h and Tec hno logy
Centr e (ES TEC) of E SA in Noordwijk (NL) and
the Belgian Nucle a r Re sear c h Cente r ( S CK -
Cen) . Whene ve r re leva nt, students are given
the opportunity to tak e pa rt in a va riety of
natio nal a nd inte rna tio nal events. R ecen t
Figure 1 . MSS program structure. (*) Students can also include courses fr om other master programs at KU
Leuven or Ghent University. (* *) Depending of the profile of the student: students with an initial master in
Science or Technology have to follow (a) while students with a Humanities background will foll ow (b).
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exam ples encompass t he ES A Y oung Laywe rs’
Symposiu m, t he Luxembourg NewSpace
Europ e Conf ere nc e or th e Belgia n Switch to
Space event, allowin g students to e x pand the
local expertise , int eract wit h indus try lea der s,
policyma kers a nd rese arch experts, g row their
netwo rk and explore new career opportun ities.
3. Pr og r amm atic analysis
T he MSS program is nearing the e nd of its 1 3 th
acad emic ye ar and has gr aduated o ve r 100
stude nts si nce it was first offered in 2009- 2010.
Th is pr ovides us a n inte resting sam ple of
alum ni sp ecifically tr ained to e nter th e spa ce
sector . In this secti on, we investig ate the
dem og raphics of the progr am, including
atte ndance, gen d er balance a n d th e dist ribution
of stu dents among the main study profiles. In a
secon d step, we use s ocial me dia a nd p e rsonal
conta cts to t race th e c urr e nt pr ofessio n al
occup ation s of the pr o gram’s a lumn i t o identify
the secto r (spa c e- vs. non-spa c e-relate d ) an d
subse ctor s (academ ia, (inte r)governmen t al
age ncies, in du stry ) in which th ey are w or ki ng.
Fina ll y, we use the results o f interviews from
alum ni to sh ed some additional perspective s
offe red by young professional on the space
edu cation.
3.1. MSS demog r aphics
Stud e nts’ influ x : Figure 2 displays the nu mber
of stud ents that h ave ent er ed t he program for
each ac adem ic year. W ith an influ x rate of less
than 10 stud ents per yea r in the first few years,
the influx rate h as m ore than d o ubled in t he last
coup le of y ear s with cur rently no less than 29
stude nts registered fo r the a c ad emic y ear 2 021-
2022 (22 new stud e nts and 7 st udents
spre adin g th e 60 -ECTS program ov er two
year s) . A s the re ader wil l notice, Poisson e rror
bar s t hat ar e app ropr i ate for c ounting statistics
have been overla id in Figu re 2. Of course, one
exactly knows t he n umber of registered
stude nts each year , so one may wond e r “ Why
err or bar s ? ”. A s data scientists woul d explain,
conside rin g th e num b er ( N i) of regist ere d
stude nts eac h year ( i) as the r ealization of a
ran do m va riable ( X N ) allows us t o inv estigate
wheth er the observed ye a r- to -ye ar variations
can be explai ned b y sta tistical fluctuations du e
to random s am pling of a consta nt pa rent
pop ulation or w hether sig nificant time -
dep end i ng trends can be identified.
Fo r ex am ple, the 2012 and 2018 pea ks in
Figu re 2 ar e by n o mean significan t, nor is th e
201 0 valley. Yet, the incre ase obse rved of the
last cou ple of y ear s c anno t b e exp l ained by
statistical fluctua tio ns around a co nstant
aver ag e ( null hy pothesis r ejected at 99. 9%-
confid ence) . This su ggests t ha t an ext ern al
facto r came int o play ed to modify the la n dscap e
in which st udents cho ose t heir orientation.
While the nu mber of students i n t ertiar y
edu cation in Belgium grows over th e year s, this
cann ot be invo k ed to explain a short- term
incre ase by a f act or of more t han 2.5. As an
alter nativ e ex planation, one may n ote tha t the
incre ase coincides with t he first aca de mic year
afte r t he sta rt of th e COVID crisis. On e may
ther ef ore w ond e r whether (some) graduating
stude nts felt tha t the jo b-market w ould be
difficult and have t here f or e chosen to pu rsue a
comp lem entar y (post-m aster) e ducation to
incre ase thei r attra ctivity on the markets while
weath erin g the crisis. Interac tions with the
stude nts r eve aled h owever a diffe rent m essage
in which they put forward th eir long -lasting
inter est fo r spa ce, the pe rceived attr activity of
the sector an d the larger me dia att ention to
space- r elated news. Ti me will c erta inly he l p to
differ en tiate between the la t ter t w o hypo t he sis.
Figure 2. Number of students registered in the
program per academic year. Poisson errorbars
have been included.
Figure 3. Distribution of students among the
three specialization profiles of the MSS.
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Gen der balance : A si milar an alysis can be
don e with res pect t o the gender of t he st udents’
pop ulation . Fr om 20 09 to 2017, t he fraction of
fem ale students w as on average o f 14% while ,
since 2018, it s average n ow r eaches 32%. The
post- 20 17 fraction of female stude nts ca nnot be
explain ed b y statistical fluctuation a round the
pre -2 017 rat e and should there f ore be
conside re d as si gnificant ( null hy pothesis
reje cted a t t he 95% -confidence) . Th e beginning
of the tre nd prec ede s th e star t of t he COVID
crisis, and we m ig ht hop e that t his will be a long-
lasting tre n d to imp rove the influx of wo men in a
sector that h as l ong s tanding g ender im ba lance
(as other STEM-related sectors do) .
Specia liza tion profiles: Fi gure 3 displ ays the
distrib ution s of students across the th ree MSS
specializa tion pr ofiles. A vera ges a re 28 %, 25%
and 4 7% for the Law & H umanities, S cience and
Te chno l ogy profiles, respectively. Our analysis
reve als no s tatistically significa nt trends alb eit
smaller sa mple sizes may limit our sensitivity.
Int er nationalization: A last tr end of inte r est is
the larger intern ationa li zati on of th e pr og ram,
with an influ x from abroad that h as do ubled,
fro m an av erage of 11% f rom 2009 to 2017 to
an average of 2 2% in the last 5 ye a rs, des pite a
dro p t o pre-pandemic level in 2020.
3.2. P rofe ssional occupation
One of th e aims of th e M S S is to h elp pre p aring
the students t o star t a career in th e spa ce
sector . A possible me tric of success is thus to
investiga te th e first professio n al occ upation of
the MSS alumn i imm ediately afte r g raduating .
Figu re 4 reveals th at a c onsist ent fracti on of f
abo ut 70% to 75% of the MSS stud ents find a
job in th e spac e sector af ter graduation , but for
202 0 (po ssible impact of t he p andemic?). The
rete ntio n rate howe v er decr e ases over the
year s and d rops be low 5 0% at th e 10 -year
hor iz on. Discussio n with a subset of t he alum ni
that have le ft th e sp ace secto r indicate s th at this
is rath er the r esult of n ew opp ortunities an d
pro fessio nal dev elopments, o r pe rsonal
circum sanc es, rather than a lack of option s
within th e sp ace sector itself.
Among alumni working in the spac e sect or, one
may won der which s ub-sec tors the y are
working in. Figure 5 re veals a goo d mix of
alum ni working in ac ademi a (e.g., researchers
and PhD students at universities and research
cente rs) , governmental agencies ( e.g., ES A,
natio nal a g encies) o r the ind ustry. While the
err or bar s ar e large given the limite d sample
size, the cle ar ris e of t he p rivate sec tor s ha re
(mo stly f ro m wit hin Belgium ) in t he last fou r or
five year s seem to sug gest a m o re dynamic
Belgian job market and a growin g nu mber of
priva te opportunities in the space se c tor.
3.3. Testimo ni als
Th e qu ality of th e MSS prog ra m is r egu la rly
mon itor ed through s urveys and interviews of
our al umni and of representative of the
workfo rce. Below, we report on a sm all subset
of quotes t hat illustrate th e perception of
stude nts and workforce alike.
(Alu m ni) “ W hen I fo un d o ut t his
Advance d Master existed , I im media t ely
app lied. We had all sorts of su bjects. Ca n you
imag ine what it must have been like for an
eng ineer to h ave Space La w or Life Science s in
Space? The diver sity w as exactly what I loved
abo ut the Ma s ter .”
(Alumn i) “ Anot her aspect of the 1 -yea r
expe rien c e t hat changed my li f e was the
netwo rking. Because we w ere so f ew in the
class, w e became a tig ht g roup . To gether , we
Figure 4: Fraction of MSS students with a space-
related professional occupation immediately after
graduating from the MSS
Figure 5 : Distribution, as a function of their
graduation year, of the professional sub -sectors
(see legend) in w hich MSS alumni w orking in the
space sector are w orking. Errorbars have been
neglected for clarity but are of 15 to 20% .
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org anise d m any trips to dif ferent kin ds of
even ts. ”
(Alu m ni) “ T h e dive rse co mpany vi sits allowed
me t o really get to k n ow the indus try. Than ks to
this m aster, I fo und out what I wanted t o do in
life. I b ecame […] . As you can probably im agine ,
I would never have known this job even existed
without this aw esome program .”
(Workf orce) “ The re are o nly limited real
multid isciplinar y sp aces studi es pr o gra m s
availab le, gl obally, a nd th e qu ality of t his
pro gr am is, ar guab ly , a mong s t the highest if not
the h igh est in academ ic quality pur sang .”
(Workf orce) “ T he program is r eally tailored to
wher e your interests lie w hile at t he same time
giving a ll students the same basis t o bu ild on. ”
4. Oth er space- education activities at KU
Le uven
KU Leuven hosts ES ERO Belgium [5] , the
Belgian antenna of th e E uropean S pace
Educatio n Res ource s Office whic h we d o no t
deve lop her further for the sake of place. W e
rath er focus on a less kn own Cube S pec project
[6 - 8] . CubeSpec is a K U Leu ve n-led in -orb it
dem onst ration mission that have been selected
by the E SA GSTP technology pro gram with a
pre li minary launc h date i n 2023. The goal of th e
mission is to en able low-c ost astronomical
spectr osco py from a 6 -unit CubeSat usi ng an
innova tive o ptical desig n and pointing
mech anis m. W hile the mission aims ar e
scientific and tech nolog ical in nature,
CubeSpe c offers si gnificant ed ucational
opp ortunities with s everal master th esis
pro jects or ganized so fa r around var ious
aspe cts of the m is sio n de v elop ment.
5. Con cl usions
In this paper, we have reported o n th e adv anced
Mast er o f Space S tudies (MSS), an
inter disciplina ry post -master tertiary education
pro gr am or gan ize d jointly by K U Leuven a nd
Ghen t Univer sity. T he ins pection of th e st uden ts
dem og raphics and the pr ofessional occu pation
of the MSS’ alumni since its cre ation has
allowed us to identify a nu mber of inte resting
tre nd that we summ a rize below:
Studen t de mograph ics
• Incr ease in regist ere d students in the last 2
year s
• Incr ease in ge nder diversity an d fra ctio n
inter nati onal students since 2018
Professio nal marke ts
• About 75% of MSS alumn i start a
pro fessio nal ca reer in th e space secto r ,
abo ut 2/3 of which rema i n in the sector 10
year s aft er graduation
• Th e pr iv ate sector se ems to be hirin g a
larg er fr action of o ur alumni in the last 4
year s, c or rel ating well with its i ncrease role
in the spac e sector.
Th ese trends ne ed to be consolidated ov er the
next few years by further mo nitoring of the
stude nts’ po pulation and th eir pr ofessional
tra cks, but also by a comp a ris on with similar
statistics fr om oth e r b ranches of S TEM
edu cation.
App en dix: Admission requirements [3,4]
As an advan c ed master’s p rogram, app li cants
are r equired to have successfully completed an
initial maste r’s program before star ti ng the
MSS. T he initial t raining can be very diver se
(e.g ., L aw, Business, E conomics, Physics,
Astrono my, M anagement, E ngine e ring, Design,
Psychology, Biochemistry , Medicine, …). A ll
app licants mu s t fur ther pr esent a CV and a two-
pag e motiva ti on l etter desc ribing the
impo rtance of t he p rogram for thei r pr ofessio n al
expe ctations, especially in view of their p revious
mast er edu c ation . A TOEFL E nglish p roficie ncy
test is a lso r equired.
Refe rences
[1] KNA L website :
http s://www.kna lf estival.be
[2] J. Borr ell, High Representative and Vice -
Preside nt, European Commission ,
“Op ening address o f the 2020 Eu ropean
Space Co nference”
[3 ] MSS Website :
http s://fys.kuleuven.be/ster/education/m
aster -sp ace-studies/master- of -s pace-
studie s
[4] MSS program and sch edu le:
http s://onder wijsa anbod.kuleu ve n.be / op l
eiding en/e/SC_51016979.htm#bl=a ll
[5] ES ERO Belgium: htt ps://e se robelgium.be
[6] Gert et al., Proceedings of th e SP IE ,
Volume 1 06 98, id. 106985R. (2018).
[7] Vanden bussc he et al., 43 rd COSP AR
Scientific Assembly. Abstract E1.20-
0015 - 21, id. 150 9. (20 21)
[8] Bowman et al., Astro no my &
Astroph ysics, Vol. 65 8, A96 (2022)
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D e s i g n a n d o p t i m i z a t i o n o f a r o c k e t s t r u c t u r e f o l l o w i n g t h e r e q u i r e m e n t s
f o r t h e E u r o p e a n R o c k e t r y C h a l l e n g e ( E U R O C ) t o b e f a b r i c a t e d u s i n g
a d d i t i v e m a n u f a c t u r i n g
Jordi Grau Rifà , ESEIA AT UPC SP Spain
____________ _________ ________ ___________ ____ ____________ _________ ________ _
Abstract
Amateur rocket str uctures are usua lly ma de of compos ite materia ls , wood or aluminium , the ir in ternal
geometries and interf aces are usual ly r estricted by th e available manu facturing t echniques. However,
with the app earance of the ad ditive ma nufacturing se ctor new possib ilities arise for the des ign of the
structures and its complex ity.
In this paper a PA-12 and glass fibr e composite s truct ure for the Phobos rocket is designed wh ich the
UPC Space Program a ims t o use to participate in the Europe an Roc ketry chal leng e . The Phobos roc ket
structure i s designed and optimized t o be fabricate d u sing additive ma nufacturin g by Hewlett- Packard .
The s tructure is desi gned using a lattice appro ach to obtai n a PA - 12 skeleton whic h is then reinforced
with a skin of g lass fibre composit e.
Moreover, to ob tain the desired structure an optimization methodology is s et usi ng a desig n loop in
which the critical sec tion o f the rocket is p arametrical ly optimized to reach the equivalent traditional
structure pe r formance. The structure is optimized in the s ize of the lattice ge ometry and in the t hickness
of the sk in as parameters. To d o so, the c ritical lo ad duri ng the flight of t he ro cket is i dentified a nd
translated to the Nas tran environment to run a parametric optimization of the structural model. The
optimized geometry is the n extended to th e r est of the rocket to obtain the overall optimized structure .
In addition, severa l analyses are c onducted to valida te the structure be havi our for the di fferent load
cases. Finally, both the optim ized critical case and the overall optimized struct ure are compared to
traditional design s tructures to obtain conclusive results abou t the us e a nd limitations of the available
additive technolo gy an d its mater ials.
Keywords
Rocketry, Stu dents, Design , Optimizat ion , Structure
____________ _________ ________ ___________ ____ ____________ _________ ________ _
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Nomenclature
T Glass fiber thickness
N Number of tr iangles per perimeter
BF Buck ling factor ( number of tim es
over the critical buc kling load)
Acronyms/Abbr eviations
EuRoC European Roc ketry Cha llenge
ESEIAAT UPC Esc o la Superi or d’Enginyer ies
Industrial, Aeroespaci al i
Audiovisual de Terras sa
UPCSP UPC Space Program
HP Hewlett-Pac kard
1. Introduction
This paper is based on th e final m aster’s thesis
which has the objective to desig n a n optim ized
rocket struc ture which aligns with the
requirements of the Ares mission insid e th e
UPCSP [1] (U PC Space Pr ogram) frame. Th e
Ares missio n a ims to partic ipate i n the EuRoC
[ 2] (European Rock etry Cha llenge) competit ion,
which t akes place in Portuga l using a new
rocket called Ph obos. T he Ph obos rock et
design mi ght us e addit ive ma nufacturing
technologies to im prove several aspects of the
rocket str ucture. The final master’s t hesis a ims
to optimize the r ocket s tructure minim izing
weight and comp aring it to a traditional des ign
giving jus tification f or the use of additive
manufacture tec hniques i n the final rock et.
2. State- of - the -art
ESEIAAT [ 3] (U PC Escola S uperior
d’Enginyeries Industrial, Aeroesp acial i
Audiovisual de Terr assa) has alway s been
involved i n amateur roc ketry with d ifferent
student associations. UPCS P has been
developing several amateur rockets since 2016.
Traditionally, these rockets are made of glass
fibre , aluminium, carb on fibre and wood, with
either self-made engines o r commercial ones.
However, with new tec hno logies such as
additive ma nufacturin g tho se designs may be
able to be improv ed.
M oreover, a lattice structure is sought to be
used in the soluti on explaine d in this paper,
several solutions can be f ound in the industry
such as the A TG Europe [4], wh ich provides
composite str ucture sol utions for r ockets or
satellites or the United L aunch Alliance [5]
which uses a latt ice str ucture milled from
aluminium she ets for its fa irings.
3. Methodolog y
3.1. Work s tructure
The workflow f or the thesis is the fol lowing:
- First a c ritical cas e w ith a c ritical sec tion
of the rocket wi ll be set.
- A traditional critical sect ion w ill be
analysed and used as target for the
optimized critical sec tion.
- The o ptimiza tion process will be
conducted to reach the performance of
the traditional design critica l section.
- Both designs will be exte nded to the
whole rocket.
- Several analys es will be conducte d and
both rocket desi gns will be compare d.
3.2. Critica l load cas e
The critical load cas e use d for the dimensi oning
of the desig n is th e buckling failure m echanism .
A thin-w alled elongat ed c ylindrical rocket
structure could col lapse under t he loads
provided by the simu lation de partment of the
Ares miss ion inside t he UPCSP. Acc ording to
th eir simu lations, t he maximum loads occur
during the i g nition stage of th e launch which
correspond t o an axial load of 3000 N. T his
value w ill be the d imensioni ng l oads of th e
design.
It is worth to mention tha t due to the small
engine and s hort burn time of the r ock et (aroun d
two seconds) no th ermal lo ads are consi dered
in this study. Th e therma l isolation of the eng ine
paired wit h th e thick al u minium wall of its m ount
are e nough to not let heat reach the struct ure
considering the sh ort burni ng time.
3.3. Critica l section of th e rocket
To size t he structure an d optimize correctly the
most c ritical section of th e rocket structure is
selected to be the pay load bay, wh ich
corresponds to a cylinder o f 14 c m in d iameter
and 90 cm o f longitude . Is the most critical
section due to:
- Being the longest empty s ection of t he
rocket.
- Being the s ectio n need ing more empty
space inside for th e payloa d.
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3.4. Design an d Ana lysis metho dology
Two design methodologies will be followed. The
traditional design w ith ty pical materials alrea dy
used by th e U PCSP and t he opt imized design
which incorporates additive manufacturing and
its correspondin g materials.
3.4.1. Tr aditional design
The tradit ional design has the char acteristic of
having a thick skin on th e wal ls of th e rock et.
This sk in ty pically withstan ds all loads on t he
rocket structure, and it is often overs ized for
manufacturing purposes. T he typi cal v alues
from past UPC SP rockets a re:
- Three layers or tw o of glass fibre with a
1:1 ratio in mass to e poxy re sin. A pplied
by hand lay -u p.
- Interior parts made of w ood or 3D
printed PLA po lymer.
- Interfaces b etween skin and inter ior
geometries gl ued or joined by bolts.
3.4.2. Optim ized design
The optimized des ign wi ll be built of one skin of
glass fibre and an i nternal s truc ture based on a
lattice distribution made of triangles . The
internal structure w ill be ad ditive manufac tured.
The optim ization procedure for the structure will
be the following:
- Model w ith N triang les.
- Parametric optimization of the
thickness of the glass fibre skin, the
width, and the height of th e beams of
the triangles.
- Linear buck ling analys is on the
optimized structure.
- Comparis on with th e traditi onal design.
- Iteration loop t o ma tch t he p erformanc e
of the tradition al design.
- Final N triang le o ptimiz ed critical
section mod el.
The triangles in w hich the str ucture is f ormed
are the followi ng:
Figure 2. Base triangle of the structure , in purple
the wi dth of the beam and in black its height.
Several examp les of s imilar f unction ing
structures can be fou nd in the references such
as the Latt ice structure of a s atellite desi gned
by ATG Europe [4].
Once the crit ical optim ized s ection design is
obtained the lattice s tructur e will be extende d to
the whole rocket to obtain the opt imized rocket
design. Add itionally, a thin s kin wa ll jo ined to t he
lattice s tructure o n its exterior will be designed
to facilitate the hand- layup of the composite
material.
3.4.3. Analys is methodol ogy
The an alysis is conducte d using Beta Cae
Systems A nsa [ 5] as a pre- processor, MSC
Nastran [ 6] as a solver and Beta C ae S ystems
Meta [7] as a post -process or.
Two s ets of analysis will be conducted for t he
designs:
- Analys is for the c ritica l s ection and
optimization of the critical section .
- Analys is for the gen eral traditional
rocket design and the optimized rocket
design.
The differe nt analysis un der which both roc ket
designs will be su bmitted a re:
- Strength an alysis: I n whic h the sta t ic -
strength failure mechanism is
simulated.
- Modal an alysis: I n w hich the dy namic
failure mecha nism is simul ate d.
- Linear buck ling: To s imulate part of t he
buckling failure m echanism .
- Non-L inear buckl ing: To s imulate t he
non -linear part of th e b uckling failure
mechanism.
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For the optimized design to be cons idered
usable all t he analyses res ults must be on par
with t he trad itional ones, w hich will be used as
a target for the perform anc e of the o ptimized
structure.
Moreover, a loc al d eformation will be introduce d
into both critical section m odels to unders tand
the structural behaviour in front of possib le
irregularities in the hand l ay -up or
manufacturing proc ess , th is defor mation will be
induced into th e m odel d isplacing the mes h
elements.
3.5. Mater ials
Th ere are t wo types of m aterials used in this
design.
3.5.1. Comp osite materia ls
The c omposite materials used in th is ana lysis
are a glass fibre and ep oxy composite. F or its
modelling the r ule of m ixtur es [8] is applied.
𝐸 𝑐 = 𝑓 𝐸 𝑓 + (1 − 𝑓 )𝐸 𝑚 (1)
Where:
𝑓 = 𝑉 𝑓
𝑉 𝑓 +𝑉 𝑚 (2)
In E q. 2. 𝑉
𝑓 an d 𝑉
𝑚 are the volume fraction of
fibre and matrix respectively. In Eq. 1. The
Young Modulus is calcu lated using the Youn g
modulus of both material s and the volume
fraction 𝑓 of Eq . 2. In a similar way the density ,
compressib le and tensile strength and poisso n
number are also ca lculate d.
The g lass fi bre us ed by UP CSP is a E-g lass V-
twill of 1 65 grams per square meter [9] and t he
Epoxy resin for hand- layup laminates [1 0 ]. Th e
volume fraction used for the de sign is of 67% of
fibre and 33% of matrix.
3.5.2. Other materials
For the trad itional d esign the other mat eria ls to
be modelled are:
- Alumini um 3 003 with i ts mechan ical
properties [1 1 ].
- PA12 wit h its mec hanical properties
provided by HP (Hewlett -Pack ard) [1 2 ].
- PLA, use d for com mon 3D print ing [1 3 ].
4. Results and Discussion
The res ults w ill comprise of the most relevant
results and comparisons betwee n th e following
analysis:
- Tradition al two-layere d critical section
and d ifferent N tria ngle optimized
critical s ections to o btai n the best
optimized critical sec tion.
- General compar ison between the
traditional and optimized final cr itical
sections.
- 4 mm de ep local d eforma tion a t half
length o f the c ritica l s ection between
both cases.
- Tradit ional design rocket and op timized
design rock et lin ear buc kling , non-
linear buckling, modal ana lysis, static
analysis, and masses com parison.
The opt imization process was set with a targ et
critical linea l buck ling load of 30 K N, which
corresponds to the critical load of the traditional
de sign for tw o glass fibr e layers (Factor of
security of 10 over t he desi gn load) .
When comparing the results to the tra ditional
section for a linear buck ling analys is is
obtained:
Figure 3. Comparison between the two-layers
traditional design and the optimization process
of the critical section.
For the critical sec tion in F igure 2 the
optimization process shows a reduction of mass
maintaining t he s ame critical l oad ending up o n
the 24 -triangle confi guration with a total mass o f
0.32 Kg wh ich will be th e u sed configuratio n for
the general optimized rocket .
20000
22000
24000
26000
28000
30000
32000
34000
0 0.2 0.4 0.6 0.8 1
Criti cal load (N)
Weight (k g)
Traditional and Optimized critical sections
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Figure 4. N= 24 triangle con figurations for the
optimized design.
4.1.1. Tr aditional and opt imized critical
section compar ison
For both the traditional t wo-l ayer design an d the
24 triangles o ptimized d esign are comp ared.
Table 1. Comparison between final optimized
critical section and two-layer traditional critical
section
T (mm)
Triangles
(Width x
height , mm)
Mass (Kg)
Max.
Lineal
Load (N )
Traditional
0.50
-
0.17
3.18E+04
Optimized
0.25
3.1x1
0.32
3.03E+04
4.1.2. Global a nd local d eformatio ns
The 4 mm deform ation is induced in th e mode l
at h alf l ength of the cr itical secti on displac ing
mesh elements:
Figure 5. Displaced elements on the mesh with a
depth of 4 mm.
For both cas es a non- linea l buckling analysis is
launched obtai ning:
Table 2. Comparison between Traditional and
Optimized critical sections with a 4 mm deep
deformation under non-linear buckling analysis.
Model
Max. Non-linea l load (N )
Traditional Cr it. Se c t.
13200
Opt. Crit. Se c t.
17400
4.2. General rocket mode l
The tw o-layer traditiona l d esign rocket and a
N=24 Optimized design are compared und er
several analysis.
Figure 6. CAD model of the optimized rocket
design
4.2.1. Linear b uckling analys is
Table 3. Comparison between traditio nal and
optimized rocket designs under linear buckling
analysis.
Traditional
design
Optimized
design
BF (Buc k ling
factor)
6,744
13,076
4.2.2. Non-L inear buckl ing analysis
Table 4. Comparison between traditional and
optimized rocket designs under non -linear
buckling analysis.
Traditional
design
Optimized
design
Max. V on Misses
stress (MPa)
11.9
0. 7
Max. Disp. (mm)
0.2431
0.0121
4.2.3. Modal a nalysis
Table 5. Comparison between traditional and
optimized rocket designs under modal analysis.
Traditional
design
Optimized
design
First mode (Hz)
50 .00
32.63
4.2.4. Static an alysis
Table 6. Comparison between traditional and
optimized rocket designs under static analysis.
Traditional
design
Optimized
design
Max. Von Misses
stress (MPa)
25.7
21 .0
Max. Disp. (mm)
0.3428
0.3276
4.2.5. Mass es
Table 7. Comparison between traditional and
optimized rocket designs masses.
Traditional
design
Optimized
design
Total mass ( K g)
11.13
11.96
5. Conclusions
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There are sev eral sets of co nclusions which c an
be extract ed fr om t he de sign of the r ocket
discussed in th is paper .
The optimize d critical s ecti on did no t reach the
performance of the traditio nal one. Weighting
more and making it unfeas ible t o reach due to
the low Young m odulus of the P A12. T he
optimized design how ev er is b etter at
withstanding loca l deformations, making it less
prone to fai lure under irregularities even though
that both des igns struggl e to withstan d them as
expected.
From both fi nal r ocket designs severa l po ints
must be raised. F irst the opti mized rock et
behaves w ith a much higher BF than the
traditional on e, this could be exp lained d ue to
the increased th ickness of the w al l because of
the beams of PA12.
The non-line ar buck ling an alysis results are not
conclusive enough to extract s ignificant
conclusions. However, bot h d esigns withsta nd
the maximum load.
The modal analysis show s a variation in the
values. These va lues will be used for th e
UPCSP team t o ensure that no excitation
frequency matches the first mode of the des ign.
The s tatic a nalysis is s imilar in bo th des igns,
showing th at both c ould wi thstand t he m axim um
loads. Addition ally, the optimized de s ign h as
lower deformat ions.
Finally, the mas s differenc e is greatly red uced
in the context of the whole rock et, making it
almost similar for both desi gns.
Besides the a nalys is the conclusions c an be
extended t o the Ares mission inside the
UPCSP. It must be co nsidered that several
manufacturing issues arise from the hand -lay up
of th e composite mat erial. The already existin g
strength of the skeleton of the optimized desig n
creates an easier wor k env ironment. It is not
possible to h and- layup one sing l e layer of g lass
fibre properly, thus making al l designs
oversized.
The a dditive manufacturing approach a llows for
complex geometries to a pp ear in t he design.
When updating t he optimized rocket w ith t he
interior interf aces for the pay load, electronics ,
etc. the add itive ma nufactu ring a llows for m uch
convenient solutions. A stan dardized
manufacturing proc edure allow t he rock et to
reach higher q uality s tandar ds than hand made
parts, which increase the reliability a nd safety of
the mission.
References
[1] UPC Space Program. V isited 1 8 Mar.
2022, from https://upcpr ogram.s pace/
[2] European Rock etry Cha llenge. Visited
18 Mar. 2022, from https://euroc.pt/
[3 ] UPC Escola S uperior d’Enginyeries
Industrial, A eroespacia l i Audiovisual d e
Terrassa . Visited 1 8 Mar. 2022, fro m
https://eseiaat.u pc.edu/en
[4] ATG Europe. Visited 1 8 Mar. 2022, from
https://www.at g-euro pe.com/solutions /
[5] Beta CAE systems ANS A. V isited 18
Mar. 20 22, fr om https ://www.beta-
cae.com/ans a.htm
[6] MSC Nastran, Visite d 18 Mar. 2022,
https://www.msc software.c om/fr/product/
msc-nastr an
[ 7] Beta CAE s ystems META. V isited 1 8
Mar. 20 22, fr om https ://www.beta-
cae.com/meta .htm
[8] Science Direct. Visited 1 8 Mar. 202 2,
from
https://www.sc iencedirect.c om/topics/en
gineering/rule - of -m ixture-equat i on
[9] V-Twill 165 Gr S ARGA. Visited 18 Mar.
2022, from
https://www.resin eco.com/e s/fibras - de -
vidrio-o-carbo no/tejid os-s iliones/v-twi ll-
165 - gr -s arga-100cm. html
[10] Resina Epoxi. Visited 18 Mar. 2022, from
https://www.resin eco.com/e s/resina -
epoxi/resina-e poxi-est anda r/
[11] Aluminium 3003. Visited 18 Mar. 2022,
from
https://www.a alco.co.uk/dat asheets/Alu
minium-Alloy- 3003-0- Sheet _59.ashx
[12] HP 3D pri nting ma ter ials. Visited 18 Mar.
202 from
https://www8. hp.com/h201 95/v2/GetPD
F.aspx/4AA7- 7085EE W.pdf
[13] What is PLA? Visite d 1 8 M ar. 2022 from
https://www.tw i-globa l.com/ technical-
knowledge/faqs/w hat- is -pla#Properti es
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A n i n v e s t i g a t i o n i n t o c o l d we l d a d h e s i o n f o r s p a c e c r a f t r e p a i r a f t e r a
s p a c e d e b r i s i m p a c t u s i n g s p a c e e d u c a t i o n b a s e d s u b - o r b i t a l s o u n d i n g
r o c k e t p l a t f o r m .
Mark Wylie 1 , Leonardo B arilaro 2
__________________________________________________________________________
A bstr act
It has b een observed th at sim ilar m etall ic m ateri als, when in con tact and undergo ing relative
displacem ents, c an fuse or weld. In s tandard atm ospheric conditions it is not com m on but in th e spac e
environment the inabilit y of the surf ace interf aces to re -oxide after abras ive contact is hindered, atom ic
diffusion of the m etal occurs, and this can lead t o fusion. Oscillator y motion and Hert zian c ontact stress
between th e two surf aces pla y s a m ajo r role in th e stre ngth of the c old welded joint. It has b een sho wn
that the acti on of a l ow f retting load can a lm ost double the adhesi on forc e under cy c lic loading e ven in
terrestrial a tm ospheric condi tions. In space, c old w el ding was first i dentified in th e 1 9 60 ’s as an adverse
reaction . It has been at tributed to anom alies and failures of deplo yable m ec hanisms. Other research
has allude d t o the potential of this ph enom ena for use in s pacecraft repair in spac e. Examples where
this m ay hold pr om ise is r epair of a spacecra ft hull breach af ter hyperveloc ity im pacts due to
m icro m eteoroids or orbital debris. T his research propos es an investig ation into co ld welding for use in
spacecraf t hull r epa ir. The research intends to qualif y an exp erim ental apparatus to TRL 4 using a sub-
orbital sound ing rock et platform. A j oint research eff ort bet ween the Aer ospace, Me chanica l and
Electronic Departm ent at I.T . Carlow, Ire land , th e D epartm ent of Aviation at Malta College of Arts,
Science, and Tec hnolog y, Malta is under wa y. The proj ect aim s at developing a te st apparatus to appl y
a num ber of custom patch es to sim ulated h yperveloc ity spacecraf t h ull breach e s and investigat e the
adhesion properti es during re- entr y for a range of mec hanical application conditions. A num ber of
cham bers m ay be tes ted and m onitored using pres sure transducers . After Phase 1 ( terrestrial
developm ent and v alidation using a vacuum cham ber ) , there will b e an ap plication to educ ation based
space programm es such as the one offered by the European Space Agenc y (R EXUS). T he core of the
activit y will be the design an d testin g of the experim ental pa yload, sim ulating hull breach es , de ploy m ent
the re pair patc h a nd m onitor ing of its perf orm ance duri ng re -entr y ( Phase 2). T he re covery of the pa yload
will allow further m etallurgical analysis of the cold welded joint (Phase 3). A conc eptual 3-D m odel of
the payload has been developed and is present ed h ere. T he data acquired from the sub- orbital flight
experim ent will tes t the v alidit y of the h y p othesis f or us e of co ld welding for spacec raf t hul l repair b ut wi ll
also detail the deve lopment and im plementation of m ock h y pervelocit y im pacts to rock et skin f or the
purposes of s im ulating hull breac hes in t he space en vironm en t.
Key w ords
Cold w elding adhesion, Hy pervelocity impacts, Space debris, Spacec r aft repair, S ub -orbital
flight
__________________________________________________________________________
1 m ark.wylie@itcarlo w.ie . In stitute of T echnolog y Carlow, Co Carlo w, Ireland .
2 leonardo.bar ilaro@m cast.edu.m t . The Malta College of Arts, Science & T echnolog y, Malta .
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Acronyms/ Abbreviations
CPU Central Process ing U nit
DRAMA De bris Risk Assess ment and Mitigation
Analysis
EM Engineering Model
ESA European Space Agency
EVA Extra V ehicular Activit y
FM Flight Model
HGA High Gain Antenna
HVI Hyperv elocity impact
ISS Internat ional Space St ation
LEO Low Earth O rbit
LGG Light-Gas Gun
LVDT Linear Variable D ifferential Trans former
MASTER Meteoroid And Space de bris
Terrestrial Enviro nment Ref erence
MCAST M alta Co llege of Arts, Scienc e and
Technology
MRS Mini Researc h Modul e
MMOD Microme teoroids a nd Orbital D ebris
NASA National Aeronautics a nd S pace
Administration
ODEM Orbita l Debris Eng ineering Mode ls
RSC Rock et and Space Co rporation
SSEA Symposium on Space Educationa l
Activities
1. Introduction
Orbital artificial habitat sat ellites such as the
International Space St ation (ISS) ha ve
experienced loss of atm osphere due to
perforation of the spacec raft hull. T his can occ ur
from engi n eering failures , manufacturing
defects or Hy perve locit y Im pacts (HVIs) from
space debris and m icr ometeoroids [1] . T he
frequenc y of the s pace de bris impacts c an be
predicted us ing Orbit al Debris Engin eering
Models (ODEM curr ently v 3.1) . T he Metroi d
impac t f lux can be es timated us ing N ASAs
ODPO SSP-3 0425 spec if ication or Europea n
Space Age nc y ’s (ES As) Meteoroid And Space
debris Terr estrial En vironm ent Reference
(MASTER- 8) and DRAMA (Debr is Risk
Assessm ent and Mitigat ion An al y s is) [2 ]. One
estim ation based on earl y m odels predict that in
a 30 - year period m ore than 35,000 secon dar y
debris particle im pacts will occ ur to the ISS and
will be at energ y l evels high enough to perf orate
the solar arra y s [ 1 ].
By the e nd of 2020, t he IS S h as carried out 26
collision avoida nce m ano euvres to es cape
impac t wi th space debris [3]. If a collision is
unavoidable , the ISS is equipped with a bumper
structure k nown as a W hipple/Advanced
Stuffed W hipple plate and this is designed t o
absorb the impact energ y . Ho wever, secondar y
ejecta and collis ion with u nprotected areas can ,
and do, lead to perforatio n of the ISS hu ll. If
there is a hull perf oration, the I SS benef its from
its Lo w Earth Orbit (LEO) and ease of ac cess to
resuppl y an y l ost oxygen . Lo nger m anned
m issions, also suscep tible to hull perf orations,
do not ha ve t his option a nd it is a necess ary
precaution to consider h ow hulls would be
repaired in s pace. There is a paucity of detailed
inform ation in the l iterat ure on how these
leaks/perf orations are repaired and no
standards pu blished but rec ently a descr iption
of a s uccessf ul repair of 2.0 m m diameter hole
in the S oyuz cre w vehicle which was d ock ed to
the Mini Res earch Mo dule ( MRM-1) or Ras svet
m odule was release d [4]. It was stated that th e
perforation was repaired by usi ng a m edical
gauze soak ed in epox y [5]. T he ad hes ive is
k nown as Germ etall-1 and packaged as the
GERMET IC leak repair k it. T his repair k it
includes G erm etall-1 and Anaterm -1u sealant
[6] . T he m ost recent loss in atm osp here was
identified in the Z ve zda S ervice Modu le i n 20 20.
A 2 2 m m l ong crack w as detected i n th e
m odule. It was reporte d that the l eak was
causing a pressure drop o f 1 mm of m ercur y
ever y 8 hours [ 7]. The cr ack was repaired using
an un disclosed sealant. It is obvious that ther e
is a consc ious effort towa rds f inding a viab le
solution. It is proposed to investigate the
intentional cold welding of metals for spacecraf t
hull repair during a sub -orb ital flight and m onitor
the perform ance of s uch repair during re -entr y.
This will also invol ve characteris ing and
replicating perforations from HVIs. T he aim of
this project is to us e an educa tion-base d
sounding rock et platform and student team to
investigate this phenom enon . T he g oal is to
form a pan-E uropean collaboration between
third-level i nstitutes and a ward an MSc in Space
Systems Engin eering. Project Te am Lead,
Materials Eng ineer, Me chanical E ngineer,
Aerospace Engi neer and Electronics /
Comm unications En gineer are some of the
student positions required . 5-10 team m em bers
are require d. W ith th at s aid, th ere are bot h
educational and technical objectives for the
proposed programm e. T his includes the
identification of educat iona l space -b ased
opportunities through pro gram me outreach.
Recruitm ent of a student t eam and appl ication
to an educ ation-bas ed sounding rock et
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programm e. As part of the t echnical o bjectives ,
an En gineering Model (E M) (Ph ase 1) a long
with HVIs perforations w ill be de veloped f or
terrestrial experim entation and validat ion. It is
envisaged that the experim ent s w i ll exam ine
several material candidates, surf ace f inishes
and a range of impact forces and interactions
(fretting and gallin g). The Flight M odel (FM)
(Phase 2) w i ll re -des ign th is experim ental set up
within the c onfines of a sounding rocket m odul e .
It will re quire t he high vac uum conditions , re -
entry press urisation and accelerat ion
forc es/temperatures to validate th e
experim ents. T he m icro-gravity en vironm ent in
this phase ma y also pla y a role i n the e volution
of the joint a dhesion. The experim ent will
in troduce m ock hull per forations and the
experim ent w ill operate autonom ous ly durin g
the f light prof ile. Further m etallurg ical anal ysi s
of the retrieved sam ples wi ll f orm Phase 3 of this
research.
2. HVIs and Co ld Weld A d hesion
2.1. HVI effects
In hypervel ocit y impacts, the projec tile velocit y
exceeds the speed of sound within the t arget
m aterial. T he r esult ing shock wave tha t
propagates across the m aterial is ref lected b y
the surfac es of the target, and reverses its
direction of travel. The superim position of
progressing and reflected waves c an lead to
local stres s levels that exceed the m aterial's
strength, thus caus ing cr acks and/or the
separation of spalls at s ignificant velocities .
W ith decreasing target thick ness, the effects
range f rom cratering, via i nternal cracks , to spal l
detachm ent, and finally to clear ho le
perforations. It has been sho wn that M MOD
impac ts on spacecraf t, accordin g to the debris’
dimensions c an generate [ 8] :
Sm all s urfac e pits d ue to m icrometre -
size im pactors;
Clear ho le penetrati ons f or m illim etre-
size objects ;
Mission-critical dam age f or projectiles
larger than 1 cm
An y impact of a 10 cm catalogue object on a
spacecraf t or orbit al stage will m os t likely im ply
a catastrophic disintegratio n of the target. T his
destructive energy is a c onsequenc e of high
impac t velocities. The eff ects of hypervelocit y
impac ts are a f unct ion of projectile and target
m aterial, im pact velocity, i n cident angle and the
m ass and shape of the proj ectile. At lo w
velocities, plastic def orm ation norm ally prevai ls.
W ith increasing velocities, the impactor will
leave a crater on th e target. Be yond 4 km /s ,
depending on the m aterial s , an im pact will lead
to a c om plete break - up and m elting of the
projectile, and an ejection of c rater m aterial to a
depth of typically two to f ive tim es the diameter
of the projec tile. Usua lly when the impact risk
from m eteoroids and orbita l d ebris is assessed
the m ain concern i s usu ally struc tural dam age.
In this context, the prop osed research targe ts
the pre liminar y assessm ent of a rep air to a
dam aged spacecraf t hull shields. For th is
purpose, a rang e of m ock hull perforati on
configurations will be evalu ated and tested. An
exam ple perforati on ho le cr eated b y a n
Al um inium sphere proj ectile of 2.3 mm diameter
at a speed of 4.8 k m/ s is sh o wn in Figure 1 [ 9 ].
Figure 1 . HVI im pact exa mple o n an Alum ini u m
plate.
2.2. Cold we ld adhes ion
Cold welding is the f usion of tw o m etals at low
tem perature. T heoretic ally, adhesion of two
m etal samples of the same m aterial wi ll occur in
contact prov iding the surf aces were s m ooth
(micros copic scale), free from contam inants
and the cr ystal lattice of th e opposing s urfac es
have the sam e orientation [ 10 ]. There are two
schools of thou ght o n the m echanisms behind
this phenom ena an d the y ar e based on the film
theor y and energ y barr ier t heor y (m is m atch of
cr y sta l lattice and rec rystalli zation theor y ). In
space, th e a bsence of atm o s phere pro vides
necessar y c onditions favourable f or cold weld
adhesion. Furtherm ore, evap oration of
lubricants in high vacuum and i ntim ate contact
of m etal, caus ing disru ption of the ox ide fi lm w i ll
further promote th is f usion. In 1966 N ASA
published a s tate- of - the -art survey in the f ield of
m etal- to -metal a dhes ion or cold weldin g i n
space. T his in vestigation exam ined bot h
positive and n egati ve eff ects of c old welding in
space citing that it ma y be used som eday to
fabricate or re pair structure s in space [ 10 ].
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This was f ollowed i n 1969, when NASA i nitiated
a col d welding program to determ ine the pro per
test environm ent for qualif ying spacecraf t
m echanisms. T his researc h investigated the
eff ects of c y cles, and lubr icated versus non -
lubricated contact. In 1989, it was proffered that
cold welding was sho wn t o be a c redible caus e
of the fai lure of the Galileo High Ga in Antenna
(HGA) to de ploy [ 11 ]. T he bond strength of cold
welding in high vacuum has been s hown to be
significant, at least an adhesion s trength equal
to the load app lied [ 12 ]. Adhesion forces in the
vicinity of 1 0s of Newto ns are reported and, i n
certain con ditions, as high as 100 N under h igh
vacuum launc h environm ent using silver m ati ng
pairs [ 13 ]. Other sof t m etals, such as Indi um ,
are excellent candidates for deliberate fusion as
the y have bee n shown to readil y f use in
atm ospheric conditions [ 14 ]. In general, a long
with m etal surfac e c onditions, the adhesion
forc e is a f unction of the rel ative m otion an d
m agnitude of the applie d c ontact forc e. In a
study carrie d out b y ESA in 2009 on the eff ects
of f retting and m etal ad h e sion, the maximum
adhesion forc e (9.5 N) was found to be 2.5
times the applied load (4 N) [ 15 ].
3. Operational framew ork
In Novem ber 2021, I nstitute of Technolog y
Carlow, Ire land, initiated a collabor ation wi th the
Malta Co llege of Arts, Sc ienc e, and T echno logy
(MCAST ), which i s c urrentl y developing th e f irst
hypervelocit y impact facility of Malta . This joint
research eff ort aim s at attr acting a nd invo lving
post an d un dergraduate gr adua te stud ents to a
space based project while boost ing the
competences of these res earch centres . The
two Institut ions a lso initiat ed a collaboration w it h
Luleå Universit y of Technolog y, in Sweden. The
focus is on stud y ing the p ayload integrat ion of
the pre viousl y desc ribed experiment on a rocket
for a sub-orb ital f light. The space researc h
centre of this Un iversit y has world- class
facilities and part ners w it h Esrange , a rocket
range and research centre located near Kirun a
in northern Sweden. C urre ntly a Mem orandum
of Understan ding is being f inalis ed.
4. Results
4.1. Preliminary desi gn
A conceptual design of an experimental la yout
has be gun . This includes four Alum inum alloy
cham bers (7075-T 651), her m itically sea led and
m ounted to th e roc k et sk in at the location of a
sim ulated hull breach. Spac e qualified bondi ng
age nt, such as Kry ptos m a y be used to f orm the
seal. E ach unit will in vestigate a s et of
experim ental param eters establishe d through
Phase 1 testing . This m ay include, material
type, surf ace f inish and s urfac e contac t
conditions . At ap ogee t he experim ent will
comm ence. Signals f rom ei ther gro und s tation
(SOD/SOE) or t im ers will initiate the exp erim ent
after Yo-Yo sta bilisation . A breac h in the rock et
skin is introduce d to eac h chamber and the
m aterial sam ples will be a ctuated b y s tepper
m otors or piezoelectric actuator s. T he
perform ance of the seal ed cham ber will be
m onitored usi ng welde d s tainless ste el
tem perature c om pensated differential pressure
transducers located in eac h cham ber a nd will
be m onitored dur ing r e-ent r y. Som e cham bers
m ay be press urized prior to re-entry t o examine
the joint integrit y in space ( aga i nst a vacuum
alone). A P C104 em bedded CP U will be used
to acqu ire the data. It w ill b e s tored locally, and
an onboard Service Module (SM) and
transm itter wil l b e us ed to tr ansit live data to
ground stat ion (sensors and housek eeping) .
Load cells or Li near Variab le D iff erential
Tr ans f orm er ( LV DT ) may be used to ver if y the
position of the sea ling patch and th e a pplied and
reaction f orces. Video data m ay also b e
acquired a nd st ored local ly as a m eans of
anomal y detection. A pr elim ina ry outline and
design of the experim ent h as been created. A
potential configuration f or multiple test
cham bers is offered but not f ixed. It is intended
for use a s a guide or tem plate for s tudents to
develop further into a proposal for a sp ace -
based e ducational rese arc h program . T he
preliminar y desi gn of the t est r ig is shown in
Figure 2. T his exp erim ent is designed within
356 m m diam eter and 237.5 mm in height , a
standard REXU S so unding rock et m odule.
Expected m as s (exc luding rock et sk in and
baseplate) is less than 4.5 k g.
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Figure 2 . Conceptual design of sounding rocket
experiment (mm).
This paper a lso details the basis of the t echnical
objectives required for the s tudent experim ent.
The ge neral t hem e of the research is presented
but the intention is that the student t eam will
develop this proj ect in more deta il.
5. Conclusions
This publication form s the f irst c ollaborative
eff ort towards ach ievin g the academic
objectives. It is designed as a n impetus f or
students to develop t his program m e. T here are
a number of funded student positions availab le.
Expressions of interest c an be emailed to either
of the authors before Novem ber 1 st 2022. T his
eff ort was conceived as a m eans to com bine
expertise and resourc es f rom multiple t hird-
level institutes with l imited space flight heri tage ,
to bolster th eir sp ace resea rch capab ilitie s and
to prom ote European co llaborations .
Acknow ledgements
The authors would l ike to thank I nstitute of
Tec hnology Car lo w and M alta Col lege of Arts,
Science & T echno logy for their support with this
research. W e would also lik e to thank LT U f or
providing the ir guidance a nd expert ise.
References
[1] W .P Schonberg, Charac terizin g
Secondar y Debris Ejecta, Intern ationa l
Journal of Impact Engineering , 26 (2001)
713 -724.
[2] S.Lemm ens, V . Braun, B . Bo nvois in .
Space Debris Mitigation: Methods (and
implem entation) MA STER8 , DRAMA3 &
ESTIMATE , European Space Agency ,
2008 .
[3] ESA’s Space Debris Office , F AQ.
https://www.esa. int/Safet y_Securit y/Spa
ce_Debris/FAQ_Fr equentl y_ask ed_ques
tions , 2021.
[4] C . Geb hardt, NA SAspacef light.com .
https://www.n asaspacefligh t.com /2018/0
8/soyuz-statio n-leak - no -thr eat-repairs -
continue/ , 20 18.
[5] H. W eiteri ng , “ Astronauts W or k to Seal
Air L eak on Space S tation. Here's How ” .
N. https:// www.space.com , 2018 .
[6] ISS On-Orbit Status ,
https://www.n asa.gov/direct orates/heo/r
eports/iss_rep orts/2012/1 1162012. htm l ,
2012 .
[7] M . W all, “ Small air leak on space station
traced to R uss ian ser vice m odule” .
https://www.space.c om /international -
space-station -air-leak - russian-m odule ,
2020 .
[8] L . Barilaro, “Measurem ent t echniques for
assessing and reducing the risk posed b y
Microm eteoroid and O rbit al D ebris t o
Space vehic les”. PhD T hesis , 2012.
[9] L. Barilaro., C. Fa lsetti, L. Olivieri.,
C. Giacom uzzo, A. Francesconi, P. Be ard,
R. Cam illeri: “ A concept ual stu dy to
characterize properti es of space debris
from h y p ervelocit y im pacts through T hin
Film Heat F lux Gauges ” . IE E
MetroAeroSpace (Na poli, Ital y ) , June
2021 .
[ 10 ] H. Pattee , R. Monroe, “Adhesion in
Space Environm ent” . R esearch Branc h
US Army Mi ssile Command , 1966.
[ 11 ] J . Ta y l or, K .M C heung, and D. Seo, ,
Deep Space Comm uni cations, Chapter
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4- Galileo Te lecomm unications , W i ley,
2016.
[ 12 ] H. Conrad, L. Rice , “T he cohesion of
previousl y frac tured FC C m etals in
ultrahigh vacuum ” , Metallurgica l
Transactions , pp. 3019 -302 9, 1970.
[ 13 ] A . Mers tallinger, R .H olzbauer and N .
Bams ey.” Cold W eldi n g in Hold Down
Points of Space Mec hani sm s Due to
Fretting W hen Om itting G rease ”.
Proceedings of the Institution of
Mechanical E ngineers , Part J: Journal of
Engineering Tribology , Vol um e 222 ( 8):
10, 2008.
[ 14 ] A.C Moore, D. Tabor, “ Som e Mechan ical
and Adhesion Properties of Ind ium ” ,
British Journa l of Appl ied Physics
3(9):299, 2002.
[ 15 ] A. M erstallinger, M. Sales, E. Semerad
and B.D. D unn. “Assessm ent of Cold
W elding between Separ able Contac t
Surfaces due to Im pact and F retting
under Vacuum ”. ESA STM- 279 , 2009.
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S u p p o r t i n g a n I S S e x p e r i m e n t a s P h D s t u d e n t s : a c a s e s t u d y o f t h e
P A R T I C L E V I B R A T I O N p r o j e c t
Georgie Crewdso n 1 * , Alessi o Boaro 1 , Monica Kerr 1 , Ma rcello Lappa 1
__________________________________________________________________________
Abstract
This paper provides an insi ght into t he involvem ent of t wo PhD students in the PARTICLE VIBRATIO N
project, a mu ltiphase fluid experimen t , a lso know n as, “T hermovibrat ionally -driven P article s elf-
Assembly an d Order ing mechan isms in L ow grAvity” ( T-PAOLA ) to be launch ed on th e Intern ational
Space Station by the end of 2022. The proj ect aims to id entify self- organizatio n phenomena in dispersed
phase flows when v ibrat ions are applied to th e system. It will therefore underpin the development of new
contactless particle m anip ul ations and materials proce ssing strategies. In this short paper, the work of
two Ph D c andidates, working within the T -PAOL A proj ect framework, is discussed. In doing so, t he
various research activit ies undertaken are highlighte d, bo th experimental a nd nu me rical, as is the
peripheral or supporting research being u ndertak en by both s tudents in order t o expand the sc ope of
the project and identify new lines of enquiry regardi ng conv ection - based contro l mechan isms.
Keywords
Microgravity , Thermovibrat ional co nv ec tion, Part icle ag gregation , ISS experi ment , T-PAOL A project
_________________________________________________________________________
1 Department of Mechanica l and Aerosp ace Eng ineering, Univers ity of Strathc lyde , Glasgow , UK
* Correspondi ng author: ge orgie.crewdson @strath.ac .uk
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Acronyms/Abbr eviations
E SA European Space Agenc y
E-USOC Spa nish User Su pport an d
Operations Centre
MSG Microgravity Sc ienc e Glove box
ISS International Space Station
SODI Selectable O ptical Diagnos tic
Instrument
T-PAOLA Thermovibrational ly- driven Partic le
self-Assembly a nd Order ing
mechanisms in L ow gr Avity
TVC Thermov ibrational C onvection
1. Introduction
Working on a sp ac e e x peri ment to be launched
on the I nternation al S pace Station (ISS) is the
dream of many mechan ical and a erospace
engineering stude nts. These opportunities are
however d ifficult to come- by as the leve l of
expertise required to undert ake such projects i s
significant, and often bey ond the sk i lls of
postgraduate students. Althou gh sig nificant
efforts have been made by organizat ions such
as E SA Academy to make altered gravity and
space platforms more acces sible to stu dents,
contributing effectively to projects of such a kind
and s cale rem ains a ch allenge. Th e T- PAOLA
project (Thermov ibrationally -driven Particle
self-Assembly and Ordering mechanisms in
Low grAvity , the c orresp onding N ASA/ES A
opsnom bei ng “Particle Vibration”) , however,
has enabled two PhD s tud en ts from th e
University of Strathclyde to immers e
themselves in a conc rete space experimen t,
leading to s ignif icant benef it s for both the
students a nd the projec t its elf. In the fol lowing,
first the scie ntific context of the ex per im ent [1 ]–
[4] , the str ucture of th e researc h team and the
other stake holders ( spac e agenc ies and
payload dev eloper) are introduced . Then, the
specific activit ies undert aken by the stu dents to
di rectly support th e project are described,
followed by a m ore ge neral presentation of their
respective r esearch inter ests and r esults .
These align w ith th e general goa ls of any
microgravity -related proj ect, na mely, a
meaningful extens ion of current state of
knowledge thro ugh th e ex ecution of a w ell-
defined ser ies of s pace experiment and the
definition o f oth er exp erim ents to b e ex ecuted in
the future to fill the rema ining gaps ( see e.g. refs
[5], [6]) .
2. Scientific objecti ve and t eam
2.1. Scientif ic objective
The T -PAOLA project consists of performing
multiphase fluid dynamic ex periments onboar d
the ISS. These experiments will inv estigate ho w
a set of particles dispersed i n a Ne wtonian liquid
can accumulate and form well - or dered
structur es. Ind eed, o n eart h, th e b ehaviour of
particle-fluid mixtures is constrained due to
gravity leading to flotati on or sediment ation of
the partic les. O nce gr avity is remove d, the
dispersed partic les are not forced to separate
and exp loring sel f-as sembly pri nciples
becomes poss ible . By stu dy ing these surpr ising
phenome na un der micro gravity con ditions ,
T-PAOLA aims to pave th e way to i nnovative
applications in chem istry, ph y sics, bi omater ials,
inorganic material scien ce and eventually
nanotechnolo gies.
The flo w th at faci litates t his parti c le aggregati on
is known as therm ov ibrationa l c onvection
(TVC). This type of c onvection is a varia nt o f
standard buoy ancy co nvection wh ere ste ady
gravitational acceleratio n is replaced with
vibrations (see Fi gure 1). When subjected to
TVC, the patterni ng beh aviour of t he flu id
becomes dependent on not only the m agnitude
of the i mposed temperatur e gradient bu t a lso on
the freq uency and am plitud e of the consid ered
vibrations and t he direction of t hese with
respect to the t emperature gradient
Figure 1: Mathematical model for (a)
thermogravitational convection and (b)
thermovibrational convection.
When parti c les are added t o the mix, in
microgravity condit ions ( where the only driv i ng
force present is due to vibratio ns), many
different patterning beh aviours are possibl e
when the space of para meters of TVC is
explored (frequency and amplitude of th e
vibrations ). The properti es of the particles a lso
contribute to the struc ture formatio ns, where
both the size, density and concen tratio n of
particles af fect the fina l s tr uctures . An ex ample
of possible pa tt erning co nfi gurations is dep icted
in Figure 2 (ad apted fro m Re f [7] ) .
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Figure 2: Example of particle aggregate
structures varying in shape due to varying
dif ferent thermo-vibrational conditions.
To k eep t he ISS experi ment as simp le as
possible an d ow ing t o the fact that the proj ect
utilises the ex isting ISS hardware Selectable
Optical Diag nostics Ins trumen t (SODI) in
combination w ith the Micrograv ity Science
Glovebox ( MSG), only the v ibrational
frequency, amplitude and te mperature
difference across the cavity are var ied and the
direction of vibratio ns is set in a p erpendicu lar
manner to the temperature gradient (as show n
in Figure 1 ).
However, keeping w ith t he ai m of exp anding the
project sc ope, the inv olved PhD s tudents (first
and second author of the prese nt paper ,
hereafter simply referred to as GC and A B ,
respectively ) have a lso co ns idered situations in
which the tem perature gradient has a diff erent
orientation and/or the liquid also p osses s es
elastic propert ies (non- Newtonian f luids).
2.2. Team co mposition
A nota ble asp ect o f the proj ect is the
composition of the team responsible for the
success ful completion and continuation o f the
Particle Vibration project. The team i s
composed of two sub- tea ms . The science te am
(based at the University of Strathclyde) inc ludes
the principa l investigat or (f ourth aut hor, ML), a
research associate ( third author , MK ) and the
two af oremention ed PhD s tudents . The t eam is
responsible for providing the exact scientific
requirements for t he series of experiments to be
conducted on b oard the ISS an d for expa nding
the project sc ope by pushing its bo undaries
further. The techn ical team i ncludes the
relevant pers onnel of th e compa ny in charge of
manufacturing the ex periment hardwar e
(QinetiQ), t he ESA project c oordinator, the E SA
Payload Integ ra tion Man ager and the User
Support and Operations Centre (E -USOC) in
charge of commanding remote ly the payload
and d evelop ing t he re lated proc edures . In
Figure 3 we schem atise the compositio n of both
teams.
Figure 3 : Composition of the Science an d the
Industry team.
3. Discussion
3.1. Projec t activities and team integrat ion
In th is section the v arious activit ies undertaken
by G C and AB , and direc tly re lated t o t he
T-PAOLA space experimen t, are d iscuss ed.
3.1.1. Experi mental ac tivities (G C )
We b egin this secti on with discuss ing the
plethora of ex perim ental a ctivities undertaken
GC . For brevity we focus on the two mos t
relevant tasks . Firstly, GC attend ed a weeklong
activity w here Qinet iQ had been contract ed to
carry out t he “c ell f illing proced ure”, wh ere t he
quartz cells to be used on t he ISS are f illed w ith
both th e f luid and the particles . Duri ng the filling
procedure, many foresee n (and u nf oreseen)
obstacles w here tackled. These obstacles
provided an ins ight into the d ifficulty of
monitoring and perform ing the high-prec ision
tasks required for the s uccess of th e
experiment. The second critical experimental
procedure to be carried o ut was th e degass ing
of the f luid in preparation for the experime nt
(shown in F igure 4) , whic h was supervised by
MK. The related rationale/c hallenges can be
described as fo llows.
Under atmos pheric pressur e a smal l a mount of
“air” is tr apped in the flu id. W he n the fl uid is
placed unde r vac uum, th is air is forced out of
the fluid cr eating un wanted air bu bbles in the
fluid c ell. Of course, this ca n ma k e any particle
formations imposs ible , therefore th e fluid must
be p urged of all r esidual air befor e it is inserte d
in th e c ell w ith the pa rt icles. Th is ac tivity
involves th e us e of both co mpressed gases and
liquid nitrogen tha t required GC taking short
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courses, henc e developing her s kill set , as wel l
as contributi ng to dev eloping bespoke
experimental prot ocols.
Figure 4: Nitrogen gas is bu bbled through the
ethanol to displace any remaining oxygen.
3.1.2. Data downlink a nd p ost processing
(A B)
In addition to the fu ndamental ex perimenta l
activities, anot her crucial part of t he proj ect h as
been the treatment of the experi ment al dat a
(signals and images) pr oduc ed i nitially during
ground testing . A proper description of t hese
aspects requires t he intr oduction of so me
details about the contro l parameters of t he
experiment ( as deve loped in the fo llowing ) .
As stated in the introducti on, TVC arises inside
a differentia lly heate d cavity when v ib rations are
applied. After selecting the propert ies of the
fluid an d t he particles, four other c ontrol
parameters r emain, n amely , the tempe rature at
the to p and bott om of the cell , the freque ncy of
the vibrati ons and their am plitud e. In a ddition ,
the a pplied temperature has to be var ied
sinusoidally in c ertain stages of the ex periment
in order to re -disperse t he particle s (after
particle structures are fo rmed f or a given
combination of the pa ramet ers , i nitial condit ions
with a uniform distribut ion of p artic les must be
established for th e ex ecution of the next
experiment de aling wi th a d ifferent combi nation
of them) .
In Autumn 2021 gro und te st s were carr ied out
by the a forement ioned E-USOC w ith two- fold
purpose to 1) assess the consistency of the
payload so ftware (exper iment “s cripts”) wi th the
specifications provided by the s cientific team
and 2) verify the ab ility of the h ardwar e to
support ade quately the ranges of temper ature
and v ibration al frequenci es specified t hrough
such a set of r equirements.
Here, t he support of AB w as funda mental. H e
developed a r obust a lgorithm capable of
automatically check ing the results of t he t ests
against the requirements in terms of dura tion of
every ste p and a mplitud e and fr equency of bot h
vi brations and temperatu re. More over , t he
algorithm w as also able to c lassify the pictures
recorded d uring e ach run and split them i nto
different subgroups accordin g to t he specific
step of the experiment in w hich t hey had bee n
generated . A s an example, Figu re 5 shows part
the algorith m output for a generic run.
This procedure reve aled an inconsistency
between the image number ing an d the rec orded
signals, w hich was ti mely c omm unicated to the
E-USOC an d f ixed accordingly. More over, t he
processed data proved that the hardware coul d
maintain the re quired therm al modulations .
a)
b)
c)
Figure 5 : Output of the algorithm. The vertical
dashed lines indicate the s ta rt of a new step. a)
Frequency and b) Amplitude of the vibrations,
and c) temperature of the pr imary cell.
3.2. Expansi on of pro ject s c ope throug h
peripheral research
We now turn t o the s pecific topics of the
students PhD thes es an d show how their
activities are contrib uting t o the legacy of the
Particle Vibration project not on ly from a
technical point of v iew, but a lso in terms of
scientific outcomes .
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References
[1]
BryceTech, “The 2 019 Global Sp ace
Economy at a Gla nce,” Oc tober 5, 2020.
[2]
The Institution of Engineering and
Technology, “ Satellite Co mmunicat ions
Systems Cours e,” [Online]. Available:
https://satcoms.the iet.org/.
[3]
Systems a nd Netw ork Ltd., “Ess ential
Satellite commun ications,” [Online].
Available:
https://www.snt.co. uk/traini ng_courses/N
etworking/Sate llite_commu nications_co ur
se.htm.
[4]
The Kno w ledge Aca demy, “Satellite
Communicati on Tra ining,” [Online].
Available:
https://www.th eknowledge academy.c om/
courses/advanced -tec hnologies-
courses/satel lite-comm unication -training/.
[5]
D. M. St einer, Lear ning, Construc tivist
Theories of, vo l. 276, 2014, pp. 319 -320.
[6]
D. C. P hillips, B ehaviorism and
Behaviorist Learn ing T heo ries. I n: Seel
N.M. (eds) Encycloped ia of the Sciences
of Learning, Spr inger, B oston, MA, 2012.
[7]
Y. Inoue, “ Learning a nd Co gnitive Theory
Applied to Educatio n,” College of
Education, U niversity of Gu am, 2000.
[8]
J. Utecht and D. Keller, “Becoming
Relevant Again: Applyi ng Connectivism
Learning Theory t o Today's Classrooms,”
Critical Questions i n E ducatio n, vol. 10,
pp. 107-119, 2019.
[9]
P. A. A lmeida, “ Kolb’s Experientia l
Learning The ory Revisi ted,” Advances in
Psychology Research, vol. 102, pp. 6 3-
76, 2015.
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DEAR project: Lunar Dust Surface interactions, Risk and Removal
investigations
C. Jalba , P . Milev 1 , P . Schulz , A. Pflug 2 , P . Ramm , O. Gusland , I. Ghitiu 1 , R: Jalba 1 , A.
1 2 2bis 3
Magureanu 1 , A. Molenta 1 , A. Pantea 1 , G. Pantea 1 , L. Jalba 1 , S. Özdemir -Fritz , G. Groemer 4 ,
4
A. Müller , H. Steininger 5 , D. McKeown , F . Gibson Kiely 6 , J .Hamilton
5 6 1
__________________________________________________________________________
Abstract
The DEAR project (Dusty Environment Application Research) investigates the interaction
between lunar regolith and surfaces and components relevant for lunar exploration. Based
on the TUBS regolith simulant which is representative in chemistry , size and shape
properties to Moon soils to study the regolith transport, adhesion and strategies for cleaning.
The regolith simulant will be applied to thermal, structural, optical sensor , sealing and other
astronautic systems, providing input for requirements, justification and verification.
The key applications are split in human space flight regolith investigations, wrinkled surface
with random movement and hardware surfaces, flat material defined movement. The paper
provides an overview of the DEAR project including a discussion of the first results, in
particular vibration, shock and micro-vibration on regolith bearing surfaces. The investigation
shall enable better understand the regolith layers interaction and the release mechanism, as
well as potential cross contamination and cleaning strategies. The research is complemented
by simulation of the regolith motion as parameter surface plasma interactions. The project is
funded and supported by the European Space Agency (ESA). DEAR specifically addresses
the development and testing of lunar dust removal strategies on optics, mechanisms and
human space flight hardware (e.g., space suits). As the Moons regolith is known to be highly
abrasive, electrically chargeable, and potentially chemically reactive, lunar dust might reduce
the performance of hardware, such as cameras, thermal control surfaces and solar cells. The
dust can cause malfunction on seals for on/of f mechanisms or space suits. Of particular
interest are risk assessment, avoidance, and cleaning techniques such as the use of electric
fields to remove lunar dust from surfaces. Representative dust (e.g., regolith analogues of
interesting landing sites) will be used in a dedicated test setup to evaluate risks and ef fects of
lunar dust. W e describe designs and methods developed by the DEAR consortium to deal
with the regolith-related issues, in particular an electrode design to deflect regolith particles,
cleaning of astronautical systems with CO2, design of a robotic arm for the testing within the
DEAR chamber , regolith removal via shock, and regolith interaction with cleanroom textiles.
Keywords
Astronaut space suit, Electrode design, Regolith (lunar dust), Robot arm, Specific cleaning
(CO2)
________________________________________________________________________
Microelectronica, Romania, [email protected]
1
Fraunhofer IST , Germany
2
Fraunhofer EMFT , Germany
2bis
Gusland Consulting, Norway
3
OeWF , Austria
4
OHB, Germany
5
University College of Dublin, Ireland
6
University of Hawaii
1
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1. Introduction
Interest in lunar exploration has regained
thrust in recent years around the world. ESA,
private industries, and the academic sector
strive to explore the Earth ! s satell ite with
a m b i t i o u s n e w t e c h n o l o g i e s . T h e h o s t i l e
e n v i r o n m e n t o f t h e M o o n , h o w e v e r , i s
generally perceived as a serious challenge, in
particular the lunar dust. T o minimise its impact
on optical surfaces and mechanisms, seals,
and in order to reduce operational risks during
future lunar missions, the European Space
A g e n c y h a s co n t r a c t e d th e DE A R (d u s t y
environment application research) consortium
to deal with regolith-related issues, catalysing
European moon surface exploration missions
in the near future.
1.1. Risks posed by Lunar Dust
Being highly abrasive, electrically chargeable,
and potentially chemically reactive, lunar dust
poses a high risk on the performance of hard-
ware, such as cameras, thermal control, and
solar cells. The dust can cause malfunctions
on seals and influence the optical, mechanical
and electrical as well as thermal properties of
surfaces including space suits. For instance,
during the sample processing on the lunar
s u r f a c e or in ai r lo c k s , r e l i a b l e s e a l s ar e
mandatory . Furthermore, lunar dust is likely to
be toxic and therefore needs to be avoided
inside the lunar habitats, motivating the work
on validated cleaning methods. T est setups
shall be used to measure potential
performance degradations within controlled
dusty loads. A programmable robotic arm is
used for repeated lifetime testing and for the
mimic of the movement of an astronaut arm.
1.2. Cleaning methods
Cleaning is possible due to the avoidance of
regolith dust built up or with active cleaning
pro ce sse s t o re mo ve t he d us t. P ro tec ti on
possibilities and cleaning efficiencies shall be
e x p e r i m e n t a l l y e x t r a c t e d . I n p a r t i c u l a r
electrode structures creating electric AC fields
for dust removal are in first order studied by
simulation and test. Another cleaning method
by applied vibration and shock is studied as
well. The cleaning of astronautic systems is
tested with CO 2 cleaning.
2. Discussion
2.1. Optical-Electrode simulation and Electrode
breadboard
This work includes a simulation of how to re-
move dust particles covering optical windows
e.g. photographic cameras, image sensors
etc., utilising an electrostatic (electrophoretic)
force on particles with inhomogeneous electric
fields. The implementation of inhomogeneous
electric fields is done via structured thin film
electrodes, either metal films or transparent
indium tin oxide (ITO) on a glass substrate. For
si mul at io n o f t he beha vi ou r r eg ar di ng t he
electrode, the following simulation codes are
used:
• The Particle-in-Cell Monte-Carlo (PIC-MC)
simulation code developed at IST
Fraunhofer , using the distributed, parallel
Poisson solver , which is based on the
Ga us s -S e id e l a lg o ri th m wit h s uc c es s iv e
over relaxation (SOR).
• A simulation tool named “P ALADIN”, for
modelling the transport of macro-particles
of variable sizes that considers particles of
sizes ranging from nanometers up to milli-
meters, and may include various physical
forces such as gravitation, gas friction, ther-
mophoresis, charging and decharging, as
well as electromagnetic field forces.
The combination of these tools allows the
computation of the trajectories of a diluted
ensemble of non-interacting nanoparticles on
electrode structures. For a higher density of
particles – as is the case of many dust layers
covering a window , different simulation
methods such as the Discrete Element Method
(DEM) would be needed.
2.1.1. Simulation of electrode structure
Our simulation test geometry consists of a
ceramic substrate material sized 10x10 mm 2
and a thickness of 1 mm (Fig.1). On the top
side, the electrode structure is integrated into
the substrate. It consists of metal lines with a
thickness of 100 µm and a lateral width of 200
µm.
Figure 1. Geometric test structure used in simulation
for various electrode designs
T wo metal wire systems are connected to the
positive and negative output of a voltage
source.
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T able 1. Basic parameters used for the electric field
computation of the test structures
The simulation volume for solving the electro-
static potential via the Poisson equation com-
prises the substrate plus a 10x10x10 mm 3
cube on top of the substrate, which is facing
the side with the electrode structure.
Th e com p u te d ele c t r ic fi el d , t h e r e s u lt i n g
particle trajectories and the dielectrophoretic
forces are shown in Fig. 2. For the P ALADIN
simulation, particles with a relative dielectric
permittivity of ε r = 3.0, mass density of ρ = 3.5
g/ c m³ , a n d h o mo g en e ou s siz e d i st r ib u ti o n
between 10 - 500 µm are used.
T h e i r s t a r t i n g p o s i t i o n s a r e r a n d o m l y
distributed on the substrate surface with the
electrode structure.
An important result is that on surface areas,
where alternating poles are entangled, high
electrophoretic forces up to several 100 g
occur , allowing for particles to drift away from
the electrodes. In contrast, in regions with only
one polarity of the electrode structure, the
d i e l e c t r o p h o r e t i c f o r c e s a r e s m a l l , a n d
particles have the tendency to remain sticking
there.
2.2. Astronautic systems. Cleaning with CO 2
This activity is mainly focused on space suit
materials but also equipment to be used by the
astronauts. Following the “AMADEE-20” Mars
analog field campaign in the Israeli Negev
desert, a carefully selected crew of analog
astronauts were deployed for one month.
Figure 2. (1) Electric potential in a cut-plane located
100 μ m a b o v e t h e s u bs t r at e w i t h t h e e l e c t r o de
structure;
(2) Central cut plane of the electric field showing the
inhomogeneous regions in between alt erna= ng poles;
(3) P ar =cle trajectories c omputed by P ALADIN;
(4) Computed dielectrophore=c forc e in units of the
gravita = onal fi eld
Parameter
Va l u e
Low
resolution
High
resolution
W afer thickness
1.0 mm
Simulation box
size
10 * 10 * 1 1 mm 3
Segmentation
4 * 4 * 2 = 32 segments up to
32 CPUs
Cell spacing
0.1 mm
0.05 mm
Number of cells
1.1 * 10 6
8.8 * 10 6
Electrode
voltage
± 1000 V
Substrate
material
Ceramic material ε r = 6.0
Solver
Poisson equation;
Distributed Gauss-Seidel with
SOR
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Their work included performing simulated
extra -veh icula r act ivity (EV A) – w ith ta sks
pertinent also to lunar exploration, such as
geosampling activities, maintaining critical
hardware infrastructure of surface translation.
In total, 61,35 EV A hours were conducted.
The spacesuits were representative of what is
to be expected for future lunar missions, with a
mass of 50 kg, 3 hour so donning time and a
complex technical infrastructure for satisfying
the needs of a human body , technical and
biomedical monitoring and human metabolite
management [2] and performing the EV A ’s in a
manner pertinent to what is expected during a
planetary surface operation [3].
Figure 3. Fiel d work with spacesui t simul ators
during the AMADEE-20 expedition in Israel. (Photo
courtesy of Florian V oggeneder (OeWF))
The surface textiles of the spacesuit simulators
accumulated “regolith simulant” in a realistic
fashion and were then transferred to a CO 2 -
cleaning facility to investigate the effectiveness
of the cleaning workflow .
2.2.1. DEAR T est T extile Selection
The outermost layer to be focused upon will be
in direct contact with regolith and the physical
environment of the Moon. Based upon the
parallel ESA project PExT ex where dozens of
candidate textiles were investigates, a shortlist
of potential candidates was selected based
upon the following criteria presented in T able 2:
The resistance to dust abrasion,
e l e c t r o m a g n e t i c c o m p a t i b i l i t y ( E M C ) a n d
discharge protection and dust mitigation were
pr io r it ie s for t h e c ho i ce . T h e s el e ct io n i s
Inventex F1 120Al, having following properties:
(Kevlar ® orthofabric)
• T ensile strength 5 times higher than steel
• Permanently non-inflammable
• The fiber starts to degrade at 420 °C, for
short duration can withstand higher
temperatures
• Panox ® preoxygenated polyacrylnitril fiber
with >60% carbon content very high LOI
(l i m i t ed ox y g e n i n d e x) of 45 s t a r t s t o
segregate graphite above 700°C and as
such has a very high thermal resistance
• low mechanical strength → Kevlar has been
combined
T able 2. Selection criteria
Several CO2 Cleaning Methods to remove
lunar dust from the space suits are being
tested, including blast cleaning with super-
critical CO2 jets.
2.2.2. Benefits of Cleaning with CO 2
The CO 2 Snow-Jet Cleaning method requires
80% less space than conventional power-wash
systems which are water-based. The time
which is needed for one cleaning cycle is as
well 80% shorter and the costs are reduced by
up to 40%. This cleaning method is not adding
any excess CO2 impact on the environment
because the used CO2 has been re-captured
from existing industrial emissions.
2.3. Robotic Arm
The objective is to develop a robotic arm
testbed for the DEAR chamber . The testbed
w i l l b e a b l e t o a r t i c u l a t e i n a n e a s i l y
programmable and repeatable manner with/
without the application of lunar regolith, based
u p o n a P i n c h e r X 1 5 0 r o b o t i c a r m f r o m
I n t e r b o t i x . T h e Pi n c h e r X 1 5 0 R o b o t A r m
f e a t u r e s , 5 d e g r e e s o f f r e e d o m u s i n g
D Y N A M IX E L X L 4 3 0- W 25 0- T s m ar t s e r v o s
motors, with a resolution of 4096 positions per
rotation and user definable PID parameters. It
allows the following parameters to be logged
• Cartesian Coordinate at end ef fecter (m)
• Angular Displacement of the joints (rad)
• Angular V elocity of the joints (rad/s)
• Ef fort produced by joints (Nm)
• T emperature of joints (°C)
• Present load of the joints (% of maximum
torque)
• Input V oltage of each joint (V)
Withstand Lunar
T emperature
Withstand and/or
reduce Lunar radiation
Compatible with lunar
vacuum
Must sustain pressure-
vacuum cycling (?)
EMC and discharge
protection
Resistance to wear by
abrasive regolith
Bendability (?)
Fatigue integrity over
the expected suit life
Shall not off-gas toxic
substances
Shall be non-flammable
Dust mitigation
Impermeability to water
and fluids
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Figure 4. CAD drawing of PincherX-150 robot arm
from Interbotix
The PincherX 150 is controlled by a Robotis
DYNAMIXEL U2D2 which interfaces with a
range of commonly available robotics software
such as ROS, Gazebo, Coppella Sim and
Move it.
It is of interest to measure the maximum
payload the arms can reliably perform typical
manoeuvers with. The Pincher- X150 is rated
for a 50g payload at its end ef fector but can
c a r r y l a r ge r m a s se s w h en t h e we i gh t i s
distributed over the full length of the arm, as it
the case when covered in textile. A series of
tests were performed by wrapping the arm in a
textile of known mass and measuring the
maximum effort in the joints, during an “arm
curl” movement repeated 50 time.
2.4. Regolith removal from surfaces using
vario us ex tern al fo rces (shock, v ibra tion ,
magnetic field)
One of the first choices to remove unwanted
dust is a shock or vibration mechanism. Apart
from the ef ficiency of the method, we bear in
mind, an example of spatial activities with
mechanical shock tasks as, for instance, the
crushing station, part of the ExoMars rover , is
equipped with a little hammer mechanism.
After a drill sample is crushed, the hammer is
applied to remove potential powder
contamination from the sensitive surfaces prior
to the next sample investigation.
2.4.1. Shock testing
Measure the displacement of dust applied to a
surface by means of mechanical shock. The
purpose of the experiment is to quantify the
displacement of dust particles as function of
the momentum transferred to the system. The
control parameter is mass displacement for a
well-defined mass, angle, and height of the
pendulum (linear momentum transfer).
Experimental set-up consists of a pendulum
with a rigid arm, a support, a Si wafer with
applied regolith on it. The camera was used for
recording of experiment. In a rectangular area
of 50 x 16 (= 800 mm 2 ), we are placing the five
types of particles, that differ by shape and
sizes. The chosen particles for the experiment
are: NaCl, anhydrous CaSO 4 , CaSO 4 *2H 2 O,
T alcum powder , regolith simulant TUBS-M.
Figure 5. Experimental setup
The set-up has been improved in the following
way:
• The arm of pendulum is rigid and without
torsion
• The area of particle covering is well defined
by using a “window” of sieving the powder;
• The applied concussive force is automatic,
excluding direct human intervention.
As control parameter , the mass of particles is
measured, that has crossed the line on the
side of the pendulum, by carefully removing
the particles with fine brush into a watch glass,
then measuring its weight. The control of the
accuracy of that operation is done by weighting
the remaining powder inside the initial area
and deciding whether the difference to the
original amount is within the limits of error
tolerance. Experimental results are presented
in T able 3.
T able 3. Experimental results for dust removal with
identical shocks, and distribution of dust on surface
Particles
type /%
of
displaced
powder
Exp.1
Exp.2
Exp.3
Exp.4
Exp.5
NaCl
19.34
31.53
39.74
32.98
36.06
CaSO 4
anh
24.65
20.91
40.86
27.45
66.60
CaSO 4 *
2H 2 O
29.68
37.75
28.07
29.91
38.86
Ta l c
29.61
38.86
20.06
26.13
25.9
Regolith
66.5
57.5
46.66
50.88
50.80
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2.5. Regolith interaction with textile
Motivation for this experiment is checking the
border conditions (high and low pressure) and
see how well cleanroom textiles can protect
against fine Regolith particles.
2.5.1. Regolith penetration through textile by
applying only gravitational force
Cleanroom textiles used in this experiment
were by Dastex: ION-NOST A T VI.2 without
Carbon, and PFG DAST A T I1800. Using
elastic bands, the textiles were tautly fixed on
the beakers. A certain amount of Regolith was
placed on the surface of textiles using a sieve.
Then the beakers were sealed for 7 days in a
ch a mb e r t o e x cl u de ext e rn a l d i st u rb a nc e s
suc h as stream ing air . Afte r 7 d ays , th e
chamber was unsealed and the beakers were
taken out of it. The regolith on the top of textile
s u r f a c e w a s c a r e f u l l y r e m o v e d , a v o i d i n g
particle shoehorning. After that, the textiles
were taken for an analysis. Observed range of
lengths of particles that penetrated the textiles:
ION -N OS T A T VI .2 with out Carb on : 6 ,09 -
51,72 µm; PFG DAST A T I1800: 1 1,06 - 49,09
µm.
Experimental results are presented in T able 4.
T able 4 Experimental Data for Regolith penetration
through textile by applying only gravitational force
2.5.2. Regolith penetration thorough textile by
applying additional pressure
T extile has been placed in a mortar , covering
all mortar ! s surface. Regolith was placed on
the surface of the textile, and then using a
pestle it was forcefully pressed into the textile.
W e have pressed 800 mg of Regolith against
26,5 cm 2 of both materials. The penetration
rate, visually detected is in-between 5-10%.
For calculation we have considered roughly 53
mg. The surface density of penetrated Regolith
through textile (the control parameter) is then
53mg/26,5cm 2 , resulting 2mg/cm 2 , or 0,02 kg/
m 2 .
3. Conclusions
The DEAR project has been successful in
a c h i e v i n g i t s o b j e c t i v e s . S i m u l a t i o n s o f
electrode structure suggests that on surface
areas where alternating poles are entangled
electrophoretic forces are pointing outward i.e.,
regolith will be removed outside of the covered
area. Next steps will be the manufacture of
p r o t o t y p e s t o e v a l u a t e t h e r e s u l t s o f
s i m u l a t i o n , i n v e s t i g a t i o n o f e f f e c t s f r o m
magnetic fields and adding the interaction
between particles in simulations. Cleaning with
CO 2 is also of particular interest because it can
be used on a variety of human space flight
hardware. Further investigations will be related
to cleaning with CO 2 of robotic arm for wear
issues and dust penetration. Robotic arm is an
a s s e t f o r d o i n g e x p e r i m e n t s i n r e g o l i t h
e n v i r o n m e n t s e . g . , t e s t i n g p o t e n t i a l
degradation of space suits exposed to regolith
an d te s t i n g me c h a ni c a l sy s t e m s i n du s t y
environments. Regolith removal using
mechanical shock is one of the simplest and
effe ct iv e me th od s , bu t f ur th er res ea rc h i s
required.
Acknowledgements
This project was supported by the European
Space Agency .
Following are the experts and contributors, as
w e l l as o u r r e f e r e n c e f o r t h e p r e s e n t e d
activities within the article: Andreas Pflug,
P h i l i p p S c h u l z ( I S T F r a u n h o f e r ) , G e r n o t
Groemer , Seda Özdemir-Fritz (OeWF), David
McKeown (UCD), Ole Gusland (Gusland
Consulting), Axel Mueller (OHB) and Christian
Schwartz (ESA), to whom we thank for their
wisdom, passion and patience shown to us.
References
[1] G.E. Groemer , M. Storrie-Lombardi, B.
Sattler , O. Hauser , K. Bickert, E. Hauth, S.
Hauth, U. Luger , D. Schild-Hammer , D.
Foeger , J. Klauck: " Reducing biological
contamination by a space suited astronaut:
Laboratory and field test results from
Aouda.X”, Acta Astronautica (2010),
doi:10.1016/j.actaastro.2010.08.018
[2] A. Soucek, L. Ostkamp, R. Paternesi:
" Suited versus Unsuited Analog Astronaut
Performance Using the Aouda.X Space Suit
Simulator: The DEL T A Experiment of
MARS2013”, Astrobiology , vol. 15, issue 4, pp.
283-290, April 2015. DOI: 10.1089/
ast.2013.1067
T extile
Mass of
Regolith
before
experiment
(mg)
Mass of
remained
Regolith
(mg)
Mass of
Regolith
penetrating
the textile
(mg)
ION –
NOST A T
without
Carbon
307,6
286,1
21,5
PFG
DAST A T
I1800
299,8
270,5
29,3
Page of 6 6
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M o n i t o r i n g n a t u r a l p h e n o m e n a f r o m t h e c l a s s r o o m wi t h E d u s a t .
P r o p o s a l f o r a t e a c h i n g g u i d e ( a n d s u p p o r t m a t e r i a l )
Rosa Olivel la 1 , Carla G ar cia 2 , Laura Olivas 1 , P ep Si tjar 1
__________________________________________________________________________
A bstr act
Satelli te images and rem ote sensing allow us t o identify the effects of natural and hu man-made
changes that occur on Earth: fires , f lood s, urban dev elopment, deforesta t ion , etc. Than k s t o
the Copernicus p r ogram me , satel lite ima g es of the entire w orld are now availab le, with a near-
daily frequency tha t all ow the identification and m oni t oring of all these natur al phenomena and
human activ ities that produce notable changes to the Earth’s sur f ace.
All t hese phenomena are forming part of the conce rn s of many young people who see the
future of their planet in danger. The Edusa t platfo rm expl ores these phenomena from space
and provides a didactic guide to understandin g the eff ects o f global environmen tal change,
right i n the classroom. In this way , we bring remote sensing cl oser t o a public that un til now
was rarely involv ed in this discipline. W e do it fr om a didacti c and pra ctical point of view ,
connected w ith real data from Sentinel satell ites and thanks to E O Brow ser appli cation.
Key w ords
Climate chan g e, Coperni cus, remote sensin g , satell ite images, teachin g material
__________________________________________________________________________
1 Geographic Inform ation System s and Rem ote Sensing Service (SIGTE) - University of Girona, Spain,
rosa.olivella@ud g.edu
2 Facult y of Science – Un ivers it y of Girona, Spain.
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1. Introduction - Remo te sensing as an
educational resou rce
The social, econom ic and terr itorial d yna m ics
that humanit y has adopted since the First
Industrial Re volutio n h ave led to t he
indiscrim inate consum ption of natural
resources. The exploitation of these resources
has put the well- being of the inh abitants of
planet Earth, as well as th e ph ysical s ystem s
that supp ort it, at s evere r isk . This process h as
been desc ribed as “ Global Env ironmenta l
Change” and results i n f our well -k nown
phenom ena: pollutio n, b iodiversit y loss, change
in land use an d land cover, and clim ate chan ge
[1] [2].
The scientific strength of the negative
consequences of clim ate c hange, pollution or
biodiversit y loss f urther intensif ies critical
reflection am ong citizens. This sense of protes t
and s truggle is es peciall y in tense among y oung
people, who are f ighting against the pas sivit y of
politicians f or po licies to m itigate clim ate
change. As s uch, these young people nee d t o
have th e necessar y com petences in order t o
evaluate and dissem inate the conseque nces of
global e nvironm ental chan ge in a c ritica l and
objective m anner.
The availab ility of sate llite im ager y f rom around
the world o n a dail y bas is (depending o n
weather conditions) m ak es i t eas y to identif y
and m onitor all of these n atural phenom ena and
anthropic proces ses th at in volve not able
changes to the land surface [3]. T hese images
taken f rom space m ake it possible t o stud y t he
evolution of natural an d anthropic episodes
such as wildf ires, floods, melting g laciers ,
deforestation or urbani zation [4].
Copernicus is the Earth obs ervatio n program
coordinated and m anaged by the Euro pean
Comm ission and the Eur opean Environm ent
Agenc y , wit h the aim of providing acc urate a nd
up - to -date i nform ation on six areas: c limate
change, s ecurit y, emergenc y, atm osphere,
m arine environment, and land surf ace [5].
All of this inform ation is especiall y designed to
provide a globa l view of the Earth ’s hea lth, wit h
the aim of helping governm ents to f ocus on
environmental p olicies and to eff ectivel y
m onitor their im plementation. Industri es,
organizations and re searc hers are also
encouraged to m ake use of this data in
conjunction with the ir ow n da ta in order to
develop new functi onalities and app lications .
Copernicus of fers a c om plete s et of open data,
including t he large v olum e of im ages captured
from Sentinel sate llites. T his data is a vailable
through various websites, applications and
services, a nd it is desi gned f or diff erent user
profiles, f rom highly s pecialized to less
experienced ones.
The Edusat project [6 ] pres ented in th is paper
aims to s et out, in an educat ional and interactive
way, the fundamentals of rem ote sensing in
order to make the process of col lecting a nd
processing sat ellite images unders tandable .
Theref ore, the m ain objecti ve of this reference
m aterial is to present rem ote s ensing to a n on -
sp ecialized a udience and to off er a user- friendl y
tool for the a nal y sis of land surface changes as
well as a tool f or the disse m ination of results .
2. Th e Edusat platform
Edusat is a web platform that contains
educational r esources f or explor ing satellite
images that are open to th e ent ire educati onal
comm unity.
The web s ite was launched in Ma y 2 021 and is
a multilingual (C atalan, Spanish and En glish)
platform . Edu sat offer resources in a dynam ic
way (images, videos, tim e lapses, m aps, gifs,
etc.) in ord er to clear ly explai n glo bal
environmental cha nge. The resources off ered
are:
- basic pri nciples of rem ote sensing,
- cas e s tudies (explaining various natural
and anthropo logical ph enom ena),
- exerc ises to work on with the EO
Browser teachi ng guide.
Using Edusat, we pro pose a teaching guide that
aims to bring rem ote sensin g to a non-
specialized au dience and t o provide teac hers,
students an d researc hers with support m ater ial.
This paper s ets out a t eac hing guide for a
classroom work shop.
The overall aim of Edusat is specif ied in these
three specif ic objectives :
- To introduce stude nts t o the fie ld of r em ote
sensing and to sho w them how t o ide ntify re al
natural phenom ena.
- To introduce stu dents to the C opernicus
programm e, givin g them acces s to f reel y
available satel lite images.
- T o enable studen ts to i dentif y the causes and
consequences of natural p henomena such as
floods, drought, def orestati on, etc.
Th e purpose of m aking t he materials openly
available is t o empo wer users to learn about a
resource, regardless of whether or not they
have c om pleted t he c ours es we off er. T he
dissem ination of the materials enable s an yone
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to bec om e f amiliar w it h th e applications an d the
usefulness of satellite im ager y.
At the mom ent of writing this paper there are
nine case s tudies developed that allow us t o
dem onstrate the usefulness of satellite images
to observe and anal y ze the current phenom ena
of global en vironm ental change. T he case
studies ar e accom panied by videos whic h
explain step by s tep how to obt ain the results
we s how f or each phenomenon studied so that
the user c an get the same res ults using th e
videos as a qu ick -start guide.
3. Th e learning material
The tea ching guide i s th e pr oposa l that w e off er
educators to use Edusat in order to work with
rem ote sensing and case studies in t he
classroom .
It is structured as a single s ession -or set of
sessions, depend ing on te aching context - wi th
different parts or b lock s (Figure 1).
3.1. Block 1. Con text and assumptions
Estimated dur ation: 2 ho urs
3.1.1. Context
The first block c omprises of a t heor y sessi on in
which th e teacher explains the principles of
rem ote sensing (satellites, sensors ,
electrom agnetic radiation an d ban d
combinations), sho wing students how th is
technolog y c an he lp to detect nat ural disasters
or human activit y resu lting f rom the climate
crisis. T he goal of this block is to provide the
students with co ntext on the issu e of gl obal
environmental change and t o exp lain the
principles of rem ote s ensing in a simple,
enjoyable wa y.
3.1.2. EO Bro wser [7]
This block also contains a s ect ion in which the
teacher s hows t he s tudents how to use the EO
Browser ap plication to s earch for s atellite
images and m ake band c om binations.
EO Brows er is an a pplication d eveloped b y the
Sentinel Hub com pany [ 8] which m ak es it
possible to view hi gh -reso lution images from
Sentinel, Landsat an d ot her satellites on a
single website.
Furtherm ore, the EO Br owser enables users to
create com parisons or time lapses of satellite
images so that the c hanges that h ave occurred
in the territor y ca n be easily identif ied by
comparing several images tak en on diff erent
dates.
For now, th is application is an open-acces s tool
that off ers basic functions such as displa ying
the natur al-colour images of satellites; as well
as advance d par am eters of ban d com binations
or th e app lication of m ulti ple indices through
inter-band algorit hm s.
Figure 1. Teaching gu ide infographic
3.1.3. Case s tudy
The students exp lore real exam ples of
phenom ena f rom around the wor ld t hat ca n be
studied using satellite i m ages and wel l-
docum ented case studies availab le in Edusat,
related to phenomena s uch as f ires, f loods,
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Figure 4. Absorb ent Pad s Test
2.5. Therma l
R EQ : The exp eriment s hall have nom inal
performance a t temperatur es of u p to 45 °C.
REQ: The exper iment shal l ma intain
functionality with nominal performance after
being exposed to a temper ature of almos t -30°C
before the fl ight.
Extreme tem peratures mus t be cons idered
before the operat ion of t he experiment . T he
launch wi ll take p lace fr o m the ESRANGE
launch site ins ide the Ar ctic Circle . s o, the
experiment co uld be ex posed for a long per iod
of time to very low temperatures before the
launch. Also, the heat coming gen erated during
the flight can drastica lly rise the temp erature
inside o ur exp eriment module before th e
milligravity perio d.
The proc edure cons isted in artificially ex posing
the experi ment to low ( using a house hold
freezer) and high (using a lab oven)
temperatures and running the fu ll pr inting
sequence immediate ly after (see Figure 5). T his
test is quite conservative as in reality, th ermal
insulation is use d ins ide the rocket modu le and
the org anizers can he at t he rock et to a desired
temperature bef ore the f light.
The succ ess c riteria was repres ented by the
success ful completion of the printing procedur e
after the cold/h eat exposur e.
Figure 5 . High (left) and L ow( right) temp.
tests
2.6. Vibrati on
REQ: T he experiment shall withstand the
vibration loads during the launch of REXU S
rocket.
Figure 6 . Vib ration Test Set - Up
The vibrati on test was the most conventional
test performed by o ur team c ompared with all
the others .
The procedure was entire ly specified by the
REXUS User Manual [4] and by t he
REXUS/BEXU S orga niser s. The exper iment
was mou nted on a shaker a nd differe nt vibra tion
input pro files were used while observin g an d
recording dat a from the accelerometers p laced
on different sp ots on the experim ent’s body .
One of the ch allenges of performing the test
was the d esign a nd ma nufacturing of the
interface bo ard to the s haker that was need ed
to match the shaker m echanical interfaces with
our experiment.
The success criteria was to have a functiona l
experiment after exposed t o vibratio ns.
2.7. Vacuum
REQ: The experim ent s hall have n ominal
performance in v acuum c onditions (pres sure
below 0.5 mbar) .
Most of t he electronics used are off - the -sh elf
components that w ill be ex posed t o vacu um for
a short t ime durin g operation in mi lligravity. For
this reason, a ll the electronics parts wer e teste d
while in operation insid e a vacuum chamb er at
a pressure of less than 0.5 mbar.
The proc edure consiste d in runn ing t he
electronics with the printing software inside the
vacuum chamber while measur ing and
recording tem perature dat a via the sensors
placed on the most critical p arts of th e assembly
(the s tepper- motor and the most p ower
consuming chips of the PCB). To command the
electronics while inside the cham ber, we
implemented a Bluetooth communication that
allowed us to c ontrol the pr ocess.
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The success criteria consisted of confirmin g full
functionality of th e electron ics while inside the
vacuum chamber and t o prove that t he
hotspots’ temperatures of the assembly were i n
line with the re quirements.
Figure 7 . El ectronics Vacuu m Test
3. Results
All the test procedures presented in S ection 2
were suc cessful ly carr ied out by the team in the
given t imefram e. The Therma l Test was
performed w ith some delay as the initial plan
was to acc ess a thermal chamber but given t he
high n umber o f CO VID i nfections at th at t ime,
we continued w ith the freez er/oven pr ocedure.
All th e suc cess criteria were achieved, an d
extensive test rep orts were delivered to the
campaign pane l. The test activities ende d with
a succes sful Experi ment Acceptance Review
and with the d elivery of th e experim ent to the
REXUS/BEXU S organiser s for the launch
campaign pe nding to take place in 202 3.
4. Conclusions
The test campaign execut ed by the ECRIDA
team p articipating i n th e REXUS/ BEXUS
framework is presented. O ur method of
designing th e camp aign, the constra ints we
faced, and a high-leve l des cription of every test
performed are described with focus on t he more
general aspects and w ithout digging i nto the
specifics of our experi ment . The purpose of t he
authors is to make a ll the informa tion val uable
to any stud ent proj ect that will be hosted by a
launch v ehicle a nd that must under go test
procedures.
Given the c ircumstance s of the CO VID
pandemic, our team faced v arious ch allenges
while p erforming the test p lan but eluded them
with c onfide nce resulting in a succ essful test
campaign. The experiment was delivered to the
REXUS/BEXU S org anizers and no w fi nal
preparations for the launch are perf ormed .
Acknowledgem ents
The team behind ECRIDA would like to
acknowledge the inva luable h elp duri ng the
testing campaign of prof. Bogdan Vasile and
prof. Bogdan Ionescu fro m CAM PUS Researc h
Centre, U niversity P olitehnica of Bucharest, and
Claudiu Cherci u from t he Roman ian Institute of
Space Sciences. T he team grati tude also goe s
to our advisors from t he R EXUS/B EXUS
framework : Koe n DeBeu le (ESA), Armelle
Frenea-Schmi dt ( SSC), Dieter Bischoff
(ZARM), and to al l the people involved in
organising and running this amazing campaig n.
The au t hors would also like to acknowledge th e
institutional and private sponsors of ECRIDA ,
namely: U niversity Politehnica of Bucharest,
Thales, GM V, RISE, T ech Lounge Ass ociation,
2Space, Fau lhaber, Top Metrology, SNS A, DLR
and ESA.
References
[1 ] Sacco, E., & Moon, S. K . (2 019). Additive
manufacturing for sp ace : status and
promises . The Internat ional Journ al of
Advanced Manuf acturi ng T echnology
[2 ] Haoyuan Quan, Tin g Zha n g, Ha ng Xu,
Shen Luo, J un Nie, X iaoqun Zhu , Photo-
curing 3D pri nting techn ique and its
challenges . Bioactive Materials, Volum e
5, Issue 1, 20 20
[3] Projec t ECRIDA Website : www. ecr ida-
rexus.github.io , last v isited: 21 st Marc h
2022.
[4] REX US User Ma nual:
www. rexusbexus.n et/rexus/r exus -us er-
manual , last v isited: 21 st M arch 202 2.
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D e v e l o p i n g a 3 U C u b e S a t E n g i n e e r i n g M o d e l - F l a t S a t & C h a s s i s D e s i g n
Willi am Crofts 1 , M att ias L anger 2 , Alex Bolland 2 , Ta hrim Uddin 2 , C hiara Biquet 2 , Edua rd
Hopkins 2 , Jai Bassi 2 , M yles Ing 2 , Julia Hunter - And erson 2
____________ _________ ________ ___________ ____ ____________ _________ ________ _
Abstract
WUSAT-3 is a 3U Cub eSat being designe d to c arry an experimental RF sig nal d irec tion fin ding pa yload
in Low Earth Orbit (LEO). Success ful outc ome of this experiment could l ead to significant benefits for
the f ield of wildlife mon itoring from Space. Commerc ial adoption of this proces s would enable the
development and use of muc h smaller, lighter RF t racking tags , which in tur n would co nsiderably
increase the potential r ange of spec ies that could be tr acked by S atellites.
The effect of the Covid- 19 pandem ic lockdowns has limited phys ical progress over the past 18 months,
but the team continues to g ain e normous experience and mot ivation fr om purs uing this exc it ing proj ect
with a very re al-w orld mission. A recent return to near - normal w orking p atterns has ena bled t he team to
fully engage w ith t he prac tical ities of pro gressing the previous ly prod uced WU SAT -3 C onfiguratio n
Model, towards a testable Engineering M odel.
This paper outlines t he dev elopment of both t he initial chass is prototype ( includin g mechan isms) a nd a
subsystem F latSat as a firs t stage towards building th e complete Engineer ing Mod el.
The c hassis prototype was required t o meet a ll the r e quirement s of t he FY S D esign Specification [1],
the NanoRacks Cub eSat ICD [2], the Cub eSat Desi gn Specificat ion [3] and thos e features iden tified by
the outcomes of the WU SAT -3 Configurati on Model.
The FlatS at w as required to include a ll subs ystems capable of be ing constructe d a nd t ested wi thout the
availability of c ertain proprietary items that will be purchased later. The function and interface of t hese
items, where it was necessary for the purpose of tes ting th e assembled s ubsystem units that were
available, was met by the design and inclusio n of temporary s ubstitute arrange ments that provided
similar performa nce.
Systems Engineer ing methodo logies were emp loyed throug hout as a means of e nsuring that th e design
features of both ch assis an d FlatSat me t all necess ary requireme nts.
Keywords
CubeSat , Engineering- Model , F latSat , S pace, System s,
____________ _________ ________ ___________ ____ ____________ _________ ________ _
1 William Crofts, Universi ty of Warw ick , United K ingdom , W. E.Crofts@warw ick.ac .uk ,
2 University of W arwick , Un ited Kin gdom
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Acronyms/Abbr eviations
ADC Analogue- to -D igital Co nver ter
DDD Direct Dis placeme nt Damage
DoD Depth of D ischarge
EEPROM Electr ically Er asable Programmable
Read-Only Me mory
EM Electroma gnetic
EPS Electr ical Power Sys tem
FlatSat Flat Sate llite, internal subsystems of
the satellite c onstructed an d
connected outs ide of the ch assis
FYS Fly Your Satellite
LDO Low -Drop out
LEO Low Earth Or bit
OBDH On -Board Data Handl ing
RF Radio Frequency
SEE Single Eve nt Effect
SEU Single Event Ups et
TID Total Ionizin g Dose
TMR Tr iple Modular Re dundanc y
WUSAT Warwick Un iversity Satellite
XCAM The CubeSat C amera & Co mpany
Figure 1. WU SAT-3 Cub eSat Di agram
1. Introduction
In prev ious years, work carried out has been
highly c oncept ual i n nature , ow ing in no small
part to the impact of t he Covid- 19 pandemic.
Building upon t he work of prev ious t eams, the
focus this ye ar was tra nslating con c eptual
designs into re ality – manuf acturing,
assembling, and testing as ma ny CubeSat
subsystems as possible in preparation for the
project’s am b ition of admiss ion to the Europe an
Space Agency’s S atellite P rogram [1 ].
2. Discussions
Detailed be low is a s ummary of each
subsystem develo ped this year by the WUSAT -
3 te am , outl ining the key design features, their
function , the ir testing an d v erification as w ell as
relevant major c onsider ations for each.
2.1 Chass is
The primary f unction of the chassis is to support
the pay load’s ability to fulfill the satel lite’s
mission. It provi des a stable ba s e to secur e
internal c ompo nents during launch fro m Earth ,
as well as to withstand the vibrations and large
forces experi enced. The ch assis c onsists of tw o
side pane ls whi c h i ncorporate four external
rails, nadir and back pa nels, top and botto m
plates alongs ide an additional intern al structura l
support . The panels act a s anchors to attac h
multiple patch antennas in addition to the s olar
panels requ ired to power the s ystem. W here
required, cut outs were implemen ted to facilitate
connections betw een exter nal compon ents and
internal sys tems, with al l de signs c onforming to
the dynam ic envelope spec ification [1] .
2.2 Chassis Testi ng
Static stress testing was conducte d using finite
element s oftware. Thro ug h Abaqus r elevant
parameters s uch as Von Mises str esses
highlight areas which may be prone to yielding
failures from lo ading and vibrati on during
launch. This information has be en used to
inform design on key loadbeari ng components
wh ere rein forcement or r edesign has been
required . Additional simulati on outputs
investigated c omponent deflect ion, wh ich is
presented as the displacement magnitude in
Abaqus.
The first simu lation for stres ses in th e X ax is
shows v alues lie we ll wit hin t olerate d levels
peaking at only 42.90 MPa. The maximu m
deflections of 0 .04 mm are also w ell within
reasonable s afety m argins. Similar results ar e
seen across the Y ax is w ith peak s tress at 68. 86
Nadir
facing
side
Deploya ble
patch
antennas
Fixed pa t ch
antennas
XCAM
Figure 2. Re sults of simu lation in Y axis
showing th e Von Misses stress in MPa
(left) and def lection in m m (right)
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MPa c ausing a 0.1 8 mm deflection, and over the
Z axis a pe ak 73. 18 MP a resulted again in a
small 0.18mm deforma tion. With the use of
aluminium 7075 as the material for the chas sis
construction t hese forc es are well b elow the 31 0
MPa yield limit.
Dynamic vibrational testing was al s o performed
to g ain insight on the natu ral fre quency of the
satellite chass is. Th is was carried o ut in s imilar
fashion by s imulat ion - with res ults yiel ding a
first natura l freq uency 547.77Hz, which is wel l
outside t he requ ired m inimum tolerated 130Hz
[1] . Th is testing however, indicated that large
deformations of the struct ure up t o 8.68m m
could occur, which could potentially dama ge
internal co mponents , whi lst also pot entially
exceeding the a llowable dy namic enve lope [ 1].
2.3 Internals
The i nternal compone nts are separated into
‘shelves’, each containing a m otherboard wi th
the PC/10 4 form factor. Sta ndoffs sit uated i n th e
corners of each s helf, allow them t o b e arr anged
into a stack con figuration ac ross the axial length
of the C ubeSat , a nd maintain c ontrolle d
separation between each internal com ponent .
This shelf stack fits wit hin the chassis and is
attached via the sta ndoffs at two mountin g
points, loc ated a t t he top and b ottom p lates
respectively.
Figure 3. Conf iguration of Component
Shelves
2.4 Patch Antenna Fr ame a nd Hing e
There are f our payload pat ch ant ennas on t he
CubeSat ( Abracon A RRT N5- 915.000 MHz ),
each receiving data fro m the freq uency of the
RFID tags. T wo are fixe d and located on th e
nadir (Y+) panel of the satellite, a nd two are
deployable from the side pane ls. The latt er are
constrained w ith a hinge to the X+ and X -
panels respect ively, where a de ploymen t
mechanism a llows them to rotate 9 0° about the
Y ax is to face th e Earth. Deployable ant enna
mechanisms were neces sary , as there is
insufficient s pace on the n adir panel to host al l
four of t he earth facin g an tennas re quired by the
payload – g iven the pos ition of the cam era
aperture. Give n th e thickne ss of 6.9 mm of the
antenna module, thes e could not be mounted
flush on to the s ide panels o f the chassis since it
will exceed the maximum 6.5 m m of a llowable
dynamic enve lope protrud ing fr om th e sid e.
Therefore, a recess in the aluminum chassis
was implemented to house the patch antenna in
its deployed conf iguration.
2.5 Deployment M echanisms
The r eliability of the deplo yment mechanisms
for the patch and TM/TC an tennas was a criti cal
factor for gu arantee ing the success of the
WUSAT-3 miss ion. For this reason, the
deployment mecha nisms underwent rigor ous
design, testing and valida tion to ensure the
designated mechan isms were s ufficient. Both
deployment mecha nisms utilize a nichro me
melt w ire d evice to release the appropriate
spring-loaded deployment mechanism for the
respective a ntenna system. In order t o increase
the effective ness of the burn wire break point, a
spring me c hanis m pul ls the melt wire in the
direction o f cutting across the respect ive b urn
wire. Collective ly this mechanism is k nown as a
“thermal knife”.
Figure 4 . WU SAT Deplo yment Mech anism s
To reduce th e likelihood o f deployment failure –
which would result in mission failure, redundant
pairs of t hermal knives were em ployed in the
deployment mechanisms for each an tenna .
During testing, it was discovered that a
sufficiently high curr ent of 2. 6 A would b e
required to ens ure a succes sful c ut within the
acceptable time fram e ( < 10 s ec onds). For this
reason, it wo uld be necessary to activate only a
single therma l kn ife at a ny gi v en mom ent, to
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DOI: 10.5821/conference-9788419184405.022
4 th Symposium on Space Educational Activities
Barcelona, April 2022
Page 4 of 6
remain withi n the limi ted p ower budget ava ilable
from the s atellite’s battery. Thus, a sensor
would be employed t o detect unsucc essful
antenna deployment and en able power to be re-
routed to the redundant thermal knife. In
addition, t his d esign cho ice elim inates the
possibility of burn wires be coming a sourc e o f
space debris.
2.6 Thermal Radiati on Conside rations
Despite the abu ndance of literature about
thermal radiation effects and shi elding
pertaining to C ubeSats, th ere is a significant
dearth of investigations into the effect of t hermal
radiation in space on t he temperat ures of
internal el ectronic co mponents . Th is lack of
analysis s eems str ange – giv en that the i nter nal
electronics are the co mponents for which a
suitable te mperature eq uilibrium must be
maintained. F or this reason, building on d ata
obtained throu gh prev ious thermal an alyses, a n
investigation into the effects of thermal radiation
– an d spec ifically – how they affect t he
temperatures of inter nal electronics, was
undertaken. T he data y ielded that, wit hout
insulation, the curr ent design of t he WU SAT - 3
CubeSat would not be capable of suff iciently
insulating its interna l e lectr onics, a nd that the
minimum and maxim um temperatures of at
least one or several compon ents would be
exceeded i n wors t case, eclipse, or m aximum
solar flux sc enarios.
Figure 5. Internal Operati on Temp erature
This resulted i n the i mp lementati on of
aluminumized mylar multi-l ayer insulation w ithin
the interior of the chassis pane ls betwe en the
outer fac es an d th e internal c omponents. With
the add ition of t his new insulat ion, res ults
determined that th e Cube Sat would be c apable
of e nsuring sufficient ther mal stab ility for the
duration of its deployment “surv ival” period, as
well as the e ntire mission.
2.7 Electrical Power Sy stem (EPS)
Figure 6 ill ustrates the block diagram of the
EPS, showin g the b asic layout for the power
network. Power is generated by photovoltaic
cells a nd su bsequent ly tra nsmitted t o th e EPS
control, which incl udes c omponents s uch as
buck converters and additi onal subsystems to
protect against un der and over voltages. After
this, the E PS c ontrol can proceed to distri bute
th is power to t he battery to charge it as well as
to sensin g subs ystems wi thin th e Cu beSat. The
On Board D ata Handling ( O BDH) contr ols t he
EPS sy stem and batt ery - distributi ng store d
charge when n eeded a nd with in the c orrect
operating conditions . The battery o utputs a
range of voltages depending on the a mount of
remaining stored char ge. I n id eal c onditions, i t
outputs 8.26 V DC, how ever this mus t s till be
reduc ed to a usable vo ltage for the range o f
components on t he sat ellite. This is achieve d
with two buck converter s ; one to deliver
regulated power to various subsys tems and the
other the delivered pow er to the O BDH
microcontroller. These buck c onverters are a
part of the pow er distribution in F igure 6. They
were success fully designed , man ufactured, and
tested and are able to provide sufficient power
to the satellite during opera tion .
Figure 6. E PS Block Diag ram
2.8 EPS Testing
The constructed buck converters, s een in
Figure 7 Error! R eference source no t foun d. ,
were test ed for the ir outpu t voltages a nd the ir
ripples to determ ine if the y were suitable a nd
could thus be accepted as feasible for further
development. The LM226 79 buck converter
was found to successfully supply 5 V a nd 3.3 V
power r ails for various s ubsy stem s, although
outputs were meas ured at 5.2 V and 3.6 V
respectively. The LM103 6 buck converter
delivers exactly 3.3 V to the microcontrol ler
(PIC16), as desired. The ripple of all t he po wer
rails was found t o be n egligible d ue to the Lo w
Dropout (LDO) regulato rs, names given
respectively for each buck convert er.
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