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Torsional analysis of the engine computational model

Abstract

The paper deals with basic behaviour and torsional analysis of the engine computational model. This computational model is assembled from own blocks which are created using the basic elements of Simulink software. The paper describes individual blocks and whole assembly of the engine computational model. The simulation of this diesel model was done to verify its function. In conclusion, torsional analysis was carried out.

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Torsional analysis of the engine computational model

Author: Kučera, Pavel; Píštěk, Václav
Publisher: JVE Intenational
Year: 2017
DOI: 10.21595/vp.2017.19499
Source: https://dspace.vut.cz/bitstreams/21569fab-ddcb-4aa8-aabf-90d4bc1497d8/download
© JVE INTERNATIONAL LTD. VIBROENGINEERING PROCEDIA. DEC 2017, VOL. 16. ISSN 2345-0533
25
To sional analysis o he engine compu a ional model
Pa el Kuče a1, Václa Píš ěk2
B no Uni e si y o Technology, Technicka 2896/2, 616 69, B no, Czech Republic
1Co esponding au ho
E-mail: 1kuce a@ me. u b .cz, 2pis ek. @ me. u b .cz
R
ecei ed 22 No embe 2017; accep ed 3 Decembe 2017
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Abs ac . The pape deals wi h basic beha iou and o sional analysis o he engine compu a ional
model. This compu a ional model is assembled om own blocks which a e c ea ed using he basic
elemen s o Simulink so wa e. The pape desc ibes indi idual blocks and whole assembly o he
engine compu a ional model. The simula ion o his diesel model was done o e i y i s unc ion.
In conclusion, o sional analysis was ca ied ou .
Keywo ds: compu a ional model, engine, Simulink, o sional ib a ion.
1. In oduc ion
Di e en so wa e is used o de elopmen o engine compu a ional model and i is i s s ep
o he engine p o o ype de elopmen . Howe e , some pa s o in e nal s uc u e o he p epa ed
compu a ional model canno be ully modi ied. The e o e, i is necessa y o c ea e a cus om engine
compu a ion model.
This pape is ocused on de elopmen o own lib a y wi h blocks. They desc ibe indi idual
pa s o he engine and a e c ea ed in Simulink so wa e. Then he use can assemble di e en
ypes o engine cons uc ion. Fo he ep esen o he eal engine, indica ed p essu e measu emen
we e used. F om his da a, he o que map is assembled and implemen o he engine compu a ional
model. The model includes lexible elemen s; he e o e, o sional ib a ions can be simula ed. The
pape also desc ibes an example o a compu a ional model o he eigh -cylinde diesel engine. I s
simula ion o maximum load was compa ed wi h measu emen o he engine o que and engine
powe cu es. O he simula ion desc ibes he o sional ib a ions which we e e alua ed by FFT
analysis.
The aim was o c ea e a compu a ional engine model wi h possibili y o eal ime simula ion.
In he u u e, his will allow using o hese models o de eloping and es ing o ECU p o o ypes.
2. Inpu alue o he compu a ional model
Fo ge ing inpu alues o he engine compu a ional model, engine o que and o ces ac ing
on he c ank mechanism mus be calcula ed. The e o e, inpu alues o he engine compu a ional
model a e cu es o indica ed p essu e in he engine cylinde . The ange o he engine speed,
ep esen ing p essu e cu e, is om 800 pm o 2000 pm. The cylinde diame e o 120 mm, he
engine s oke o 140 mm and he leng h o he connec ing od o 260 mm we e also used o he
calcula ion and he equa ions a e desc ibed in [1]. To ob ain he whole engine o que map, he
indi idual cu es o p essu e we e ecalcula ed o he o que and we e placed o he
h ee-dimensional ma ices wi h he dimensions o 13×720×2 o each cylinde . Some dimensions
o he ma ices could be di e en because i depends on he measu ed da a which a e a ailable.
He e a e example ma ices used o simula ion. Fi s dimension has alue o 2, i ep esen s
wo-dimensional a ays o maximum and minimum uel supply. The 13 ma ix ows con ain he
engine speed ange om 800 pm o 2000 pm and he 720 ma ix columns ep esen he c ank
angle. The ma ices o indi idual cylinde we e shi ed acco ding o cylinde igni ions. Fig. 1
shows he o que map o a maximum and a minimum uel supply. Be ween hese s a uses, he e
is ange o engine o que which can be used o a d i e o powe ain. In he new e sion o blocks,
he e is also a possibili y o using s aigh away indica ed p essu e, because blocks con ain
equa ion o calcula ion o he o que.
TORSIONAL ANALYSIS OF THE ENGINE COMPUTATIONAL MODEL.
PAV EL KUČERA, VÁCLAV PÍŠTĚK
26 © JVE INTERNATIONAL LTD. VIBROENGINEERING PROCEDIA. DEC 2017, VOL. 16. ISSN 2345-0533
Fig. 1. To que map
3. Compu a ional model o he engine
The compu a ional engine model is c ea ed in Simulink so wa e and uses own lib a y wi h
blocks. Fo he c ea ion o compu a ional models, he li e a u e [2, 3, 4] was used. This lib a y
includes blocks desc ibing he indi idual pa s o engine. Basic p inciple o blocks is based on
lexible elemen s; he e o e, use can simula e o sional ib a ions. The engine compu a ional
model is ep esen ed by a o sional model. The assembly o he compu a ional engine model
includes blocks o pis on, sha , lywheel, o sion dampe , o name bu a ew. The compu a ional
model is shown in Fig. 2. The e is o sional model wi h se en educed ine ia alues and six
s i ness blocks be ween discs. In gene al, o sional sys em is desc ibed by using Lag angian
me hod [5]:

󰇘
+󰇗+=(), (1)
whe e  is mass ma ix,  – damping ma ix,  – s i ness ma ix,  – ec o o engine o que,
 – ec o o gene alised coo dina es (󰇘 is he angula accele a ion, 󰇗 – angula eloci y,
 – angle o de o ma ion) and  – ime.
Fig. 2. In e n blocks o he engine compu a ional model
Du ing he simula ion, he compu a ional model gene a es c anksha angle and engine speed.
And he use con ols he engine model by an inpu signal o a h o le pedal. I s alue has he
ange o 0-100 %. These h ee alues de e mine he alue o ac ual engine o que om o que map.
The acqui ed engine o que is applied on he indi idual ine ia block o he o sional model. These
pis on blocks a e connec ed oge he using by lexible blocks, he e o e, hey a ec each o he .
Then o sional ib a ion can be simula ed. The compu a ional model o he dynamome e is also
assembled as a o sional model. I s block is shown in Fig. 3. This dynamome e block gene a es a
o que which coun e ac s he engine o que o achie e he desi ed engine speed.
TORSIONAL ANALYSIS OF THE ENGINE COMPUTATIONAL MODEL.
PAV EL KUČERA, VÁCLAV PÍŠTĚK
© JVE INTERNATIONAL LTD. VIBROENGINEERING PROCEDIA. DEC 2017, VOL. 16. ISSN 2345-0533 27
Fig. 3. Compu a ional model o engine and dynamome e
4. Simula ion
In he simula ion, he compu a ional model simula ed maximum load o diesel engine. The
simula ion was di ided in o se e al s eps. In each s ep o engine speed, he mean o que was
ob ained. F om hese alues we e c ea ed cu es o he engine o que and powe . Then hey we e
compa ed wi h he speed cha ac e is ics o he eal engine. The esul s a e shown in Fig. 4. The
esul s show ha he cu es o o que and powe a e simila in main ange o engine speed. In his
engine load s a e, he compu a ional model can be conside ed wo king p ope ly. In he u u e,
o he simula ions will be ca ied ou o e i y o o he condi ions.
a
)
b)
Fig. 4. Resul o he engine speed cha ac e is ics
5. To sional ib a ion
I is an eigh -cylinde engine and igni ion occu a e 90° o he c anksha . The e o e, i can
be assumed ha he 4 h and 8 h ha monics o he engine speed a e e lec ed in o sional ib a ions.
This equency  can be calcula ed using he ollowing equa ion:

=
60
,  = 1, 2, 3 … , (2)
whe e n is he engine speed wi h he uni pm and  – ha monic o de o engine speed. The
equency co esponding o he 4 h and 8 h ha monic o de o he engine speed is calcula ed a
800 pm and esul s a e 53.33 Hz and 106.66 Hz.
Fo he analysis o o sional ib a ions, he simula ions om he p e ious chap e we e used.
Thei o al o que om each engine cycle was used o e alua e he FFT analysis [6] o he engine
speed ange om 800 o 2000 pm. In his FFT spec um in Fig. 5, he 4 h and 8 h ha monic o de
o he engine speed a e clea ly isible. I co esponds o he calcula ions in Eq. (2). These ha monic
o de s can exci e o sional sys em o he engine o he ehicle powe ain. This occu s when he
ac ual o sional equency is equal o he ha monic o de o he engine speed. In he g aph in Fig. 5,
he e is e y li le isible ansi ion o e he 2nd own engine equency (282.73 Hz) because he
TORSIONAL ANALYSIS OF THE ENGINE COMPUTATIONAL MODEL.
PAV EL KUČERA, VÁCLAV PÍŠTĚK
28 © JVE INTERNATIONAL LTD. VIBROENGINEERING PROCEDIA. DEC 2017, VOL. 16. ISSN 2345-0533
o sional ib a ion is damped. Resul s o o sional ib a ion analyses shows ha he model wo ks
p ope ly and can be used o analyses o o he engines o exci a ion o he whole i ual ehicle
powe ain.
Fig. 5. FFT spec um o he engine compu a ional model
6. Conclusions
The aim was o assemble he compu a ional engine model which desc ibes he unc ions o he
eal engine, can be simula ed in he eal ime and can be used o analyse o he o sional ib a ion.
The compu a ional model was assembled om own lib a y wi h blocks. They ep esen indi idual
pa s o he engine.
The esul s o engine speed cha ac e is ics in he i s simula ion we e compa ed o he eal
engine and he i ual engine can be used o a simula ion wi h maximum load o an engine.
Howe e , o he simula ions mus be done o e i y o he ope a ing modes o he engine. The
esul s o he o sional ib a ion analysis show gene a ed ha monic o de o he engine speed and
i co espond wi h heo e ical assump ions. In he u u e, measu emen o o sional ib a ion mus
be done o e i y o esul s.
This engine compu a ional model can be also used o eal- ime simula ions in he Ha dwa e
in he Loop sys ems. I is impo an o u u e de elopmen and es ing o ECU p o o ypes.
Acknowledgemen s
This wo k is an ou pu o he in e nal BUT Resea ch P ojec Reg. No. FSI-S-17-4104.
Re e ences
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1992.
[3] Budynas R. G. Shigley’s Mechanical Enginee ing Design. McG aw-Hill, New Yo k, 2006.
[4] Kuče a P. Mecha onic App oach o Vehicle Dynamics. Doc o al Thesis, BUT B no. 2015
[5] Nes o ides E. J. A Handbook on To sional Vib a ion. Camb idge Uni e si y P ess¸ Camb idge, 1958.
[6] Tůma J. Vehicle Gea box Noise and Vib a ion. Wiley, Chiches e , 2014.