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Seismic analysis of a district heating pipeline

Abstract

The effect of seismic loading is not contemplated in any of the current design standards of District Heating and Cooling (DHC) networks, since this technology has been originally adopted in northern Europe, characterized by low earthquake vulnerability. Nevertheless, an increasing number of countries, including those in seismic areas like Italy, Turkey, China, Japan, and Chile are using DHC solutions due to the higher energy efficiency, compared to individual heating systems. Seismic regions are one of the most hostile environments for buried pipelines due to the effects of Transient Ground Deformation (TGD) caused by seismic wave propagation, and Permanent Ground Deformation (PGD), like faulting, landsliding, lateral spreading and buoyancy due to liquefaction. Most of research publications on the seismic analysis and design of buried steel pipelines have been motivated by the need of safeguarding the integrity of hydrocarbon pipelines, and there are no actual studies on the seismic vulnerability of DHC pipelines. This highlights the need to carefully evaluate the seismic performance of DHC pipelines, considering their typical composite cross-section and soil-pipe interaction under service loading. The present paper analyses the effect of diverse earthquake hazards on an operating District Heating (DH) pipe bend, usually susceptible to stress concentrations due to the greater flexibility, as well as the ability to accommodate thermal expansions, and absorb other externally-induced loading. The response of the operating DH pipeline subjected to different seismic loading is evaluated taking into account the geometric and mechanical properties of the system, including the soil-pipeline interaction. In conclusion, the obtained results give a better understanding on the seismic behavior of DH pipelines, highlighting important research ground for assessing their earthquake performance in operating conditions.

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Seismic analysis of a district heating pipeline

Author: Banushi, Gersena,Weidlich, Ingo
Publisher: Elsevier
DOI: 10.1016/j.egypro.2018.08.186
Source: https://repos.hcu-hamburg.de/bitstream/hcu/807/1/1-s2.0-S187661021830482X-main.pdf
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1876-6102 © 2017The Au ho s. Published by Else ie L d.
Pee - e iew unde esponsibili y o he Scien i ic Commi ee o The 15 h In e na ional Symposium on Dis ic Hea ing and Cooling.
The 15 h In e na ional Symposium on Dis ic Hea ing and Cooling
Assessing he easibili y o using he hea demand-ou doo
empe a u e unc ion o a long- e m dis ic hea demand o ecas
I. And ića,b,c*, A. Pinaa, P. Fe ãoa, J. Fou nie b., B. Laca iè ec, O. Le Co ec
aIN+ Cen e o Inno a ion, Technology and Policy Resea ch -Ins i u o Supe io Técnico,A . Ro isco Pais 1, 1049-001 Lisbon, Po ugal
bVeolia Reche che & Inno a ion,291 A enue D ey ous Daniel, 78520 Limay, F ance
cDépa emen Sys èmes Éne gé iques e En i onnemen -IMT A lan ique, 4 ue Al ed Kas le , 44300 Nan es, F ance
Abs ac
Dis ic hea ing ne wo ks a e commonly add essed in he li e a u e as one o he mos e ec i e solu ions o dec easing he
g eenhouse gas emissions om he building sec o . These sys ems equi e high in es men s which a e e u ned h ough he hea
sales. Due o he changed clima e condi ions and building eno a ion policies, hea demand in he u u e could dec ease,
p olonging he in es men e u n pe iod.
The main scope o his pape is o assess he easibili y o using he hea demand –ou doo empe a u e unc ion o hea demand
o ecas . The dis ic o Al alade, loca ed in Lisbon (Po ugal), was used as a case s udy. The dis ic is consis ed o 665
buildings ha a y in bo h cons uc ion pe iod and ypology. Th ee wea he scena ios (low, medium, high) and h ee dis ic
eno a ion scena ios we e de eloped (shallow, in e media e, deep). To es ima e he e o , ob ained hea demand alues we e
compa ed wi h esul s om a dynamic hea demand model, p e iously de eloped and alida ed by he au ho s.
The esul s showed ha when only wea he change is conside ed, he ma gin o e o could be accep able o some applica ions
( he e o in annual demand was lowe han 20% o all wea he scena ios conside ed). Howe e , a e in oducing eno a ion
scena ios, he e o alue inc eased up o 59.5% (depending on he wea he and eno a ion scena ios combina ion conside ed).
The alue o slope coe icien inc eased on a e age wi hin he ange o 3.8% up o 8% pe decade, ha co esponds o he
dec ease in he numbe o hea ing hou s o 22-139h du ing he hea ing season (depending on he combina ion o wea he and
eno a ion scena ios conside ed). On he o he hand, unc ion in e cep inc eased o 7.8-12.7% pe decade (depending on he
coupled scena ios). The alues sugges ed could be used o modi y he unc ion pa ame e s o he scena ios conside ed, and
imp o e he accu acy o hea demand es ima ions.
© 2017 The Au ho s. Published by Else ie L d.
Pee - e iew unde esponsibili y o he Scien i ic Commi ee o The 15 h In e na ional Symposium on Dis ic Hea ing and
Cooling.
Keywo ds: Hea demand; Fo ecas ; Clima e change
Ene gy P ocedia 149 (2018) 216–225
1876-6102 © 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic Hea ing
and Cooling, DHC2018.
10.1016/j.egyp o.2018.08.186
10.1016/j.egyp o.2018.08.186
© 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic Hea ing
and Cooling, DHC2018.
1876-6102
A ailable online a www.sciencedi ec .com
ScienceDi ec
Ene gy P ocedia 00 (2018) 000–000
www.else ie .com/loca e/p ocedia
1876-6102 © 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic Hea ing and Cooling,
DHC2018.
16 h In e na ional Symposium on Dis ic Hea ing and Cooling, DHC2018,
9–12 Sep embe 2018, Hambu g, Ge many
Seismic analysis o a dis ic hea ing pipeline
Ge sena Banushia*, Ingo Weidlicha
aHa enCi y Uni e si y, Übe seesallee 16, Hambu g, 20457, Ge many
Abs ac
The e ec o seismic loading is no con empla ed in any o he cu en design s anda ds o Dis ic Hea ing and Cooling (DHC)
ne wo ks, since his echnology has been o iginally adop ed in no he n Eu ope, cha ac e ized by low ea hquake ulne abili y.
Ne e heless, an inc easing numbe o coun ies, including hose in seismic a eas like I aly, Tu key, China, Japan, and Chile a e
using DHC solu ions due o he highe ene gy e iciency, compa ed o indi idual hea ing sys ems.
Seismic egions a e one o he mos hos ile en i onmen s o bu ied pipelines due o he e ec s o T ansien G ound De o ma ion
(TGD) caused by seismic wa e p opaga ion, and Pe manen G ound De o ma ion (PGD), like aul ing, landsliding, la e al
sp eading and buoyancy due o lique ac ion.
Mos o esea ch publica ions on he seismic analysis and design o bu ied s eel pipelines ha e been mo i a ed by he need o
sa egua ding he in eg i y o hyd oca bon pipelines, and he e a e no ac ual s udies on he seismic ulne abili y o DHC
pipelines. This highligh s he need o ca e ully e alua e he seismic pe o mance o DHC pipelines, conside ing hei ypical
composi e c oss-sec ion and soil-pipe in e ac ion unde se ice loading.
The p esen pape analyses he e ec o di e se ea hquake haza ds on an ope a ing Dis ic Hea ing (DH) pipe bend, usually
suscep ible o s ess concen a ions due o he g ea e lexibili y, as well as he abili y o accommoda e he mal expansions, and
abso b o he ex e nally-induced loading.
The esponse o he ope a ing DH pipeline subjec ed o di e en seismic loading is e alua ed aking in o accoun he geome ic
and mechanical p ope ies o he sys em, including he soil-pipeline in e ac ion.
In conclusion, he ob ained esul s gi e a be e unde s anding on he seismic beha io o DH pipelines, highligh ing impo an
esea ch g ound o assessing hei ea hquake pe o mance in ope a ing condi ions.
© 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic
Hea ing and Cooling, DHC2018.
Keywo ds: Seismic analysis; T ansien G ound De o ma ion; Pe manen G ound De o ma ion; Dis ic Hea ing Pipeline
* Co esponding au ho
E-mail add ess: [email p o ec ed]
A ailable online a www.sciencedi ec .com
ScienceDi ec
Ene gy P ocedia 00 (2018) 000–000
www.else ie .com/loca e/p ocedia
1876-6102 © 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic Hea ing and Cooling,
DHC2018.
16 h In e na ional Symposium on Dis ic Hea ing and Cooling, DHC2018,
9–12 Sep embe 2018, Hambu g, Ge many
Seismic analysis o a dis ic hea ing pipeline
Ge sena Banushia*, Ingo Weidlicha
aHa enCi y Uni e si y, Übe seesallee 16, Hambu g, 20457, Ge many
Abs ac
The e ec o seismic loading is no con empla ed in any o he cu en design s anda ds o Dis ic Hea ing and Cooling (DHC)
ne wo ks, since his echnology has been o iginally adop ed in no he n Eu ope, cha ac e ized by low ea hquake ulne abili y.
Ne e heless, an inc easing numbe o coun ies, including hose in seismic a eas like I aly, Tu key, China, Japan, and Chile a e
using DHC solu ions due o he highe ene gy e iciency, compa ed o indi idual hea ing sys ems.
Seismic egions a e one o he mos hos ile en i onmen s o bu ied pipelines due o he e ec s o T ansien G ound De o ma ion
(TGD) caused by seismic wa e p opaga ion, and Pe manen G ound De o ma ion (PGD), like aul ing, landsliding, la e al
sp eading and buoyancy due o lique ac ion.
Mos o esea ch publica ions on he seismic analysis and design o bu ied s eel pipelines ha e been mo i a ed by he need o
sa egua ding he in eg i y o hyd oca bon pipelines, and he e a e no ac ual s udies on he seismic ulne abili y o DHC
pipelines. This highligh s he need o ca e ully e alua e he seismic pe o mance o DHC pipelines, conside ing hei ypical
composi e c oss-sec ion and soil-pipe in e ac ion unde se ice loading.
The p esen pape analyses he e ec o di e se ea hquake haza ds on an ope a ing Dis ic Hea ing (DH) pipe bend, usually
suscep ible o s ess concen a ions due o he g ea e lexibili y, as well as he abili y o accommoda e he mal expansions, and
abso b o he ex e nally-induced loading.
The esponse o he ope a ing DH pipeline subjec ed o di e en seismic loading is e alua ed aking in o accoun he geome ic
and mechanical p ope ies o he sys em, including he soil-pipeline in e ac ion.
In conclusion, he ob ained esul s gi e a be e unde s anding on he seismic beha io o DH pipelines, highligh ing impo an
esea ch g ound o assessing hei ea hquake pe o mance in ope a ing condi ions.
© 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic
Hea ing and Cooling, DHC2018.
Keywo ds: Seismic analysis; T ansien G ound De o ma ion; Pe manen G ound De o ma ion; Dis ic Hea ing Pipeline
* Co esponding au ho
E-mail add ess: ge [email protected]
2 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
1. In oduc ion
Dis ic Hea ing and Cooling (DHC) consis o an unde g ound pipe ne wo k connec ing buildings in an u ban
a ea o cen alized plan s o a numbe o dis ibu ed hea p oducing uni s, allowing o hea ecycling and enewable
ene gy supply. Due o he highe ene gy e iciency, an inc easing numbe o coun ies including hose in seismic
a eas like I aly, Tu key, China, Japan, a e adop ing dis ic hea ing solu ions. The e ec o seismic loading is no
con empla ed in any o he cu en design s anda ds o DH ne wo ks, since his echnology has been o iginally
adop ed in no he n Eu opean coun ies, cha ac e ized by low ea hquake ulne abili y.
Seismic egions a e one o he mos hos ile en i onmen s o bu ied pipelines due o he e ec s o T ansien
G ound De o ma ion (TGD) caused by seismic wa e p opaga ion, and Pe manen G ound De o ma ion (PGD), like
aul ing, landsliding, la e al sp eading and buoyancy due o lique ac ion [1].
Mos o esea ch publica ions on he seismic analysis and design o bu ied s eel pipelines ha e been mo i a ed by
he need o sa egua ding he in eg i y o hyd oca bon pipelines [2], and he e a e no ac ual s udies on he seismic
ulne abili y o DHC pipelines. This highligh s he need o ca e ully e alua e he seismic pe o mance o DHC
pipelines, conside ing hei ypical composi e c oss-sec ion and soil-pipe in e ac ion unde se ice loading.
To minimize hea losses, DHC pipes ha e a composi e c oss-sec ion o h ee di e en ma e ial laye s, including
he s eel pipe o he wa e supply, he insula ion oam o polyu e hane (PUR), and an ou e coa ing o High Densi y
Polye hylene (HDPE), in e ac ing wi h he su ounding soil. The s i ness o he PUR oam and i s cons an adhesion
o he s eel pipe a e essen ial o p ope ly ansmi a he HDPE coa ing he ic ion s esses om he su ounding soil.
The axial expansion o he ope a ing pipeline, is coun e ac ed by he soil ic ion a he ou e HDPE coa ing
in e ace, un il he o al ic ion eac ion equilib a es he pipe axial o ce a he ancho poin , whe e he he mal
expansion is ully es ained. Mo eo e , he he mal expansion is coun e ac ed a he bend by he la e al soil eac ion,
inducing high s ess le els in his c i ical egion, as schema ically illus a ed in Fig. 1. Addi ionally, he PUR
insula ion is e y sensi i e o axial shea s ess and la e al p essu es, inducing high s esses associa ed wi h ma e ial
ailu e and loss o he bond; in a wo se case, i can lose i s insula ion e ec i he s eel se ice pipe c acks and he
oam is mois u ed. [3].
Fig. 1. De o ma ion o bu ied ope a ing DH pipeline a he bend (adap ed om [4] and [5])
The e o e, a co ec design o DHC pipelines equi es an accu a e conside a ion o he ele a ed s esses and
de o ma ions due o he ope a ing loads like in e nal p essu e and empe a u e, as well as he e alua ion o he soil-
pipeline in e ac ion.
Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225 217
A ailable online a www.sciencedi ec .com
ScienceDi ec
Ene gy P ocedia 00 (2018) 000–000
www.else ie .com/loca e/p ocedia
1876-6102 © 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic Hea ing and Cooling,
DHC2018.
16 h In e na ional Symposium on Dis ic Hea ing and Cooling, DHC2018,
9–12 Sep embe 2018, Hambu g, Ge many
Seismic analysis o a dis ic hea ing pipeline
Ge sena Banushia*, Ingo Weidlicha
aHa enCi y Uni e si y, Übe seesallee 16, Hambu g, 20457, Ge many
Abs ac
The e ec o seismic loading is no con empla ed in any o he cu en design s anda ds o Dis ic Hea ing and Cooling (DHC)
ne wo ks, since his echnology has been o iginally adop ed in no he n Eu ope, cha ac e ized by low ea hquake ulne abili y.
Ne e heless, an inc easing numbe o coun ies, including hose in seismic a eas like I aly, Tu key, China, Japan, and Chile a e
using DHC solu ions due o he highe ene gy e iciency, compa ed o indi idual hea ing sys ems.
Seismic egions a e one o he mos hos ile en i onmen s o bu ied pipelines due o he e ec s o T ansien G ound De o ma ion
(TGD) caused by seismic wa e p opaga ion, and Pe manen G ound De o ma ion (PGD), like aul ing, landsliding, la e al
sp eading and buoyancy due o lique ac ion.
Mos o esea ch publica ions on he seismic analysis and design o bu ied s eel pipelines ha e been mo i a ed by he need o
sa egua ding he in eg i y o hyd oca bon pipelines, and he e a e no ac ual s udies on he seismic ulne abili y o DHC
pipelines. This highligh s he need o ca e ully e alua e he seismic pe o mance o DHC pipelines, conside ing hei ypical
composi e c oss-sec ion and soil-pipe in e ac ion unde se ice loading.
The p esen pape analyses he e ec o di e se ea hquake haza ds on an ope a ing Dis ic Hea ing (DH) pipe bend, usually
suscep ible o s ess concen a ions due o he g ea e lexibili y, as well as he abili y o accommoda e he mal expansions, and
abso b o he ex e nally-induced loading.
The esponse o he ope a ing DH pipeline subjec ed o di e en seismic loading is e alua ed aking in o accoun he geome ic
and mechanical p ope ies o he sys em, including he soil-pipeline in e ac ion.
In conclusion, he ob ained esul s gi e a be e unde s anding on he seismic beha io o DH pipelines, highligh ing impo an
esea ch g ound o assessing hei ea hquake pe o mance in ope a ing condi ions.
© 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic
Hea ing and Cooling, DHC2018.
Keywo ds: Seismic analysis; T ansien G ound De o ma ion; Pe manen G ound De o ma ion; Dis ic Hea ing Pipeline
* Co esponding au ho
E-mail add ess: [email p o ec ed]
A ailable online a www.sciencedi ec .com
ScienceDi ec
Ene gy P ocedia 00 (2018) 000–000
www.else ie .com/loca e/p ocedia
1876-6102 © 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic Hea ing and Cooling,
DHC2018.
16 h In e na ional Symposium on Dis ic Hea ing and Cooling, DHC2018,
9–12 Sep embe 2018, Hambu g, Ge many
Seismic analysis o a dis ic hea ing pipeline
Ge sena Banushia*, Ingo Weidlicha
aHa enCi y Uni e si y, Übe seesallee 16, Hambu g, 20457, Ge many
Abs ac
The e ec o seismic loading is no con empla ed in any o he cu en design s anda ds o Dis ic Hea ing and Cooling (DHC)
ne wo ks, since his echnology has been o iginally adop ed in no he n Eu ope, cha ac e ized by low ea hquake ulne abili y.
Ne e heless, an inc easing numbe o coun ies, including hose in seismic a eas like I aly, Tu key, China, Japan, and Chile a e
using DHC solu ions due o he highe ene gy e iciency, compa ed o indi idual hea ing sys ems.
Seismic egions a e one o he mos hos ile en i onmen s o bu ied pipelines due o he e ec s o T ansien G ound De o ma ion
(TGD) caused by seismic wa e p opaga ion, and Pe manen G ound De o ma ion (PGD), like aul ing, landsliding, la e al
sp eading and buoyancy due o lique ac ion.
Mos o esea ch publica ions on he seismic analysis and design o bu ied s eel pipelines ha e been mo i a ed by he need o
sa egua ding he in eg i y o hyd oca bon pipelines, and he e a e no ac ual s udies on he seismic ulne abili y o DHC
pipelines. This highligh s he need o ca e ully e alua e he seismic pe o mance o DHC pipelines, conside ing hei ypical
composi e c oss-sec ion and soil-pipe in e ac ion unde se ice loading.
The p esen pape analyses he e ec o di e se ea hquake haza ds on an ope a ing Dis ic Hea ing (DH) pipe bend, usually
suscep ible o s ess concen a ions due o he g ea e lexibili y, as well as he abili y o accommoda e he mal expansions, and
abso b o he ex e nally-induced loading.
The esponse o he ope a ing DH pipeline subjec ed o di e en seismic loading is e alua ed aking in o accoun he geome ic
and mechanical p ope ies o he sys em, including he soil-pipeline in e ac ion.
In conclusion, he ob ained esul s gi e a be e unde s anding on he seismic beha io o DH pipelines, highligh ing impo an
esea ch g ound o assessing hei ea hquake pe o mance in ope a ing condi ions.
© 2018 The Au ho s. Published by Else ie L d.
This is an open access a icle unde he CC BY-NC-ND license (h ps://c ea i ecommons.o g/licenses/by-nc-nd/4.0/)
Selec ion and pee - e iew unde esponsibili y o he scien i ic commi ee o he 16 h In e na ional Symposium on Dis ic
Hea ing and Cooling, DHC2018.
Keywo ds: Seismic analysis; T ansien G ound De o ma ion; Pe manen G ound De o ma ion; Dis ic Hea ing Pipeline
* Co esponding au ho
E-mail add ess: ge [email protected]
2 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
1. In oduc ion
Dis ic Hea ing and Cooling (DHC) consis o an unde g ound pipe ne wo k connec ing buildings in an u ban
a ea o cen alized plan s o a numbe o dis ibu ed hea p oducing uni s, allowing o hea ecycling and enewable
ene gy supply. Due o he highe ene gy e iciency, an inc easing numbe o coun ies including hose in seismic
a eas like I aly, Tu key, China, Japan, a e adop ing dis ic hea ing solu ions. The e ec o seismic loading is no
con empla ed in any o he cu en design s anda ds o DH ne wo ks, since his echnology has been o iginally
adop ed in no he n Eu opean coun ies, cha ac e ized by low ea hquake ulne abili y.
Seismic egions a e one o he mos hos ile en i onmen s o bu ied pipelines due o he e ec s o T ansien
G ound De o ma ion (TGD) caused by seismic wa e p opaga ion, and Pe manen G ound De o ma ion (PGD), like
aul ing, landsliding, la e al sp eading and buoyancy due o lique ac ion [1].
Mos o esea ch publica ions on he seismic analysis and design o bu ied s eel pipelines ha e been mo i a ed by
he need o sa egua ding he in eg i y o hyd oca bon pipelines [2], and he e a e no ac ual s udies on he seismic
ulne abili y o DHC pipelines. This highligh s he need o ca e ully e alua e he seismic pe o mance o DHC
pipelines, conside ing hei ypical composi e c oss-sec ion and soil-pipe in e ac ion unde se ice loading.
To minimize hea losses, DHC pipes ha e a composi e c oss-sec ion o h ee di e en ma e ial laye s, including
he s eel pipe o he wa e supply, he insula ion oam o polyu e hane (PUR), and an ou e coa ing o High Densi y
Polye hylene (HDPE), in e ac ing wi h he su ounding soil. The s i ness o he PUR oam and i s cons an adhesion
o he s eel pipe a e essen ial o p ope ly ansmi a he HDPE coa ing he ic ion s esses om he su ounding soil.
The axial expansion o he ope a ing pipeline, is coun e ac ed by he soil ic ion a he ou e HDPE coa ing
in e ace, un il he o al ic ion eac ion equilib a es he pipe axial o ce a he ancho poin , whe e he he mal
expansion is ully es ained. Mo eo e , he he mal expansion is coun e ac ed a he bend by he la e al soil eac ion,
inducing high s ess le els in his c i ical egion, as schema ically illus a ed in Fig. 1. Addi ionally, he PUR
insula ion is e y sensi i e o axial shea s ess and la e al p essu es, inducing high s esses associa ed wi h ma e ial
ailu e and loss o he bond; in a wo se case, i can lose i s insula ion e ec i he s eel se ice pipe c acks and he
oam is mois u ed. [3].
Fig. 1. De o ma ion o bu ied ope a ing DH pipeline a he bend (adap ed om [4] and [5])
The e o e, a co ec design o DHC pipelines equi es an accu a e conside a ion o he ele a ed s esses and
de o ma ions due o he ope a ing loads like in e nal p essu e and empe a u e, as well as he e alua ion o he soil-
pipeline in e ac ion.
218 Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 3
Repo ed expe imen al esea ch on he esponse o bu ied DH pipe sys ems subjec ed o g ound mo emen is e y
limi ed, equi ing u he analysis o he soil-pipe in e ac ion o bu ied DH pipes, while aking in o accoun eal
ope a ing condi ions and mode n pipe laying echnologies [6-10]. On he o he hand, he seismic esponse o bu ied
pipelines has been in es iga ed by many esea che s in he las 50 yea s, using expe imen al in es iga ions as well as
simple analy ical o mo e complex nume ical app oaches [11-17].
Du ing ex eme e en s like ea hquakes, he pipeline needs o plas ically s e ch, bend and comp ess in o de o
accommoda e local o global mo emen o he su ounding soil, equi ing s ain-based pe o mance c i e ia o a
sa e and cos -e ec i e pipeline design [18-19]. E iden ly, s ess-based pe o mance limi s a es, like hose
ecommended in Eu opean s anda d EN 13941 [20] o in he Eu ocode 3 - Pa 4-3 [21] a e o e conse a i e o
pipelines cons uc ed in ha sh en i onmen s, like seismic egions.
The p esen pape analyses he e ec o seismic induced g ound mo emen on an ope a ing Dis ic Hea ing (DH)
pipe bend, ypically suscep ible o highes momen s and s ess concen a ions due o he g ea e lexibili y, as well as
he abili y o accommoda e he mal expansions, and abso b o he ex e nally-induced loading. [22].
The esponse o he ope a ing DH pipeline subjec ed o seismic loading is e alua ed aking in o accoun he
geome ic and mechanical p ope ies o he sys em, including he soil-pipeline in e ac ion. In conclusion, he
ob ained esul s gi e a be e unde s anding on he seismic beha iou o DH pipelines, highligh ing impo an
esea ch g ound o assessing hei ea hquake pe o mance in ope a ing condi ions.
Nomencla u e
Ds ou e diame e o he s eel pipe
s hickness o he s eel pipe
D ou e diame e o ex e nal HDPE coa ing
PUR hickness o he PUR insula ion
Rbend adius o he pipe bend
L leng h o he pipe legs
Lc leng h o he expansion cushion a each bend leg
H soil co e dep h
E elas ici y modulus o he s eel pipe
ν
Poisson's a io o he s eel pipe
σ
y yield s eng h he s eel pipe
α
linea he mal expansion coe icien o he s eel pipe
φ
soil ic ion angle
γ
soil densi y
Ti, T ins alla ion and ope a ing empe a u e
Pi, ope a ing in e nal p essu e in he s eel pipe
Ug,
ε
g,
λ
g ea hquake induced g ound displacemen , g ound s ain, and seismic wa e leng h
FR soil ic ion eac ion
Pu maximum la e al soil eac ion
k elas ic la e al soil s i ness
kc equi alen la e al s i ness in he pipe co ne wi h expansion cushion
My yielding momen o he s eel pipe sec ion
2. Me hodology
This pape in es iga es he pe o mance o p einsula ed bonded DH pipelines, subjec ed o TGD due o seismic
wa e p opaga ion. Clea ly, his haza d a ec s DH ne wo ks, conside ably mo e han does PGD, h ea ening mainly
ansmission hyd oca bon pipelines.
4 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
The in es iga ed pipe bend DN 150/250 is composed o a cen al P235GH s eel pipe o ex e nal diame e Ds =
168.3 mm and hickness s = 4 mm, a oam insula ion o hickness PUR = 37 mm, and ex e nal plas ic man le wi h
ou e diame e D = 250 mm. The adius o he pipe bend is Rbend = 1 m, he leng h o he expansion cushion a he
co ne is Lc = 2 m, while he leng h o bo h bend legs is L = 40 m, ancho ed a he ends. The pipe is assumed bu ied
in loose sand soil wi h a co e dep h H = 0.8 m, as schema ically illus a ed in Fig. 1.
The soil-pipeline sys em subjec ed o seismic loading has been analyzed nume ically wi hin beam on Winkle
ounda ion heo y, using he ini e elemen so wa e ABAQUS/S anda d [23].
The pipeline is modeled using he PIPE31 beam elemen ype, allowing he possibili y o speci y ex e nal o
in e nal p essu e. The soil-pipeline in e ac ion is modeled wi h he sp ing-like pipe-soil in e ac ion elemen s PSI34,
ep esen ing he soil eac ion o he soil mo emen in he axial, la e al, and e ical di ec ion. One edge o he
elemen sha es nodes wi h he unde lying pipe elemen while he nodes on he o he edge a e assigned he a - ield
g ound mo ion h ough he bounda y condi ions.
The P235GH s eel pipe ma e ial model is de ined wi hin he on Mises plas ici y heo y wi h nonlinea
ha dening. The ma e ial pa ame e s a e de e mined as a unc ion o he ope a ing empe a u e T, acco ding o EN
13941 [19]. The elas ici y modulus, yield s eng h, and he linea he mal expansion coe icien a he ope a ing
empe a u e T = 90°C a e E = 208857 MPa ,
σ
y = 215.8 MPa and
α
= 12.098 10-06 1/K espec i ely, while he
Poisson's a io is ν = 0.3. A loose sand ma e ial is assumed as soil back ill, wi h he same p ope ies epo ed in he
calcula ion example o he Ge man s anda d FW 401 [4], cha ac e ized by a ic ion angle
φ
= 32.5°, and a soil
densi y
γ
= 18 kN/m3. The o ce-displacemen ela ionship is conside ed bilinea elas o-plas ic, and e alua ed
acco ding o FW 401 [5]. Speci ically, he calcula ed soil ic ion eac ion is FR = 3944 N/m, while he maximum
la e al soil eac ion is Pu = 49750 N/m, wi h an elas ic la e al soil s i ness k = 35 MPa beyond he expansion
cushion, whe e he equi alen elas ic la e al s i ness is kc = 0.247 MPa [5].
The seismic-induced g ound mo emen is applied a he ee nodes o he pipe-soil in e ac ion elemen s, as a
sinusoidal wa e p opaga ing ho izon ally in he di ec ion o he longi udinal leg.
The nume ical analysis o assessing he seismic pe o mance o he ope a ing DH pipeline a e conduc ed in wo
consecu i e s eps. A i s , a s a ic analysis is pe o med o es ablish he s ess and s ain s a e in he soil-pipeline
sys em in ope a ing condi ions wi h in e nal p essu e Pi = 12 Ba , ins alla ion and se ice empe a u e Ti = 10°C and
T = 90°C, espec i ely. In he second s ep, a ho izon al displacemen is applied quasi-s a ically a he ee nodes
ends o he pipe-soil in e ac ion elemen s, ma ching he sinusoidal pa e n de ined by:
( )
⎟
⎠
⎞
⎜
⎝
⎛
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛
=
λ
π
π
λ
ε
y
xU
g
gg
2
sin
2
(1)
whe e εg = 0.0041 is he soil s ain and
λ =
500 m is he seismic wa e leng h. Thus, he maximum alue o he
g ound displacemen esul s Ug = 0.33 m
On each loading s ep, he global equilib ium equa ions a e sol ed i e a i ely by he New on-Raphson me hod
pe mi ing o assess he pipe and soil de o ma ion s a e a each inc emen .
3. Resul s and discussion
This sec ion p esen s he s uc u al esponse o he bu ied DH pipeline e alua ed using he p oposed
me hodology. Fi s ly, he pipeline esponse is in es iga ed in ope a ing condi ions, unde he e ec o in e nal
p essu e and empe a u e a ia ion. Then he seismic pe o mance o he pipeline is analyzed in e ms o loading and
de o ma ions, o di e en alues o he maximum seismic-induced g ound displacemen Ug, as discussed u he in
his sec ion.
3.1. S uc u al esponse o he pipeline in ope a ing condi ions
The expansion o he ope a ing pipeline is coun e ac ed by he bene icial e ec o he soil ic ion, and he
bea ing o ce on he ans e se leg (Fig. 1). The maximum axial elonga ion o he pipeline in ope a ion condi ions,
Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225 219
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 3
Repo ed expe imen al esea ch on he esponse o bu ied DH pipe sys ems subjec ed o g ound mo emen is e y
limi ed, equi ing u he analysis o he soil-pipe in e ac ion o bu ied DH pipes, while aking in o accoun eal
ope a ing condi ions and mode n pipe laying echnologies [6-10]. On he o he hand, he seismic esponse o bu ied
pipelines has been in es iga ed by many esea che s in he las 50 yea s, using expe imen al in es iga ions as well as
simple analy ical o mo e complex nume ical app oaches [11-17].
Du ing ex eme e en s like ea hquakes, he pipeline needs o plas ically s e ch, bend and comp ess in o de o
accommoda e local o global mo emen o he su ounding soil, equi ing s ain-based pe o mance c i e ia o a
sa e and cos -e ec i e pipeline design [18-19]. E iden ly, s ess-based pe o mance limi s a es, like hose
ecommended in Eu opean s anda d EN 13941 [20] o in he Eu ocode 3 - Pa 4-3 [21] a e o e conse a i e o
pipelines cons uc ed in ha sh en i onmen s, like seismic egions.
The p esen pape analyses he e ec o seismic induced g ound mo emen on an ope a ing Dis ic Hea ing (DH)
pipe bend, ypically suscep ible o highes momen s and s ess concen a ions due o he g ea e lexibili y, as well as
he abili y o accommoda e he mal expansions, and abso b o he ex e nally-induced loading. [22].
The esponse o he ope a ing DH pipeline subjec ed o seismic loading is e alua ed aking in o accoun he
geome ic and mechanical p ope ies o he sys em, including he soil-pipeline in e ac ion. In conclusion, he
ob ained esul s gi e a be e unde s anding on he seismic beha iou o DH pipelines, highligh ing impo an
esea ch g ound o assessing hei ea hquake pe o mance in ope a ing condi ions.
Nomencla u e
Ds ou e diame e o he s eel pipe
s hickness o he s eel pipe
D ou e diame e o ex e nal HDPE coa ing
PUR hickness o he PUR insula ion
Rbend adius o he pipe bend
L leng h o he pipe legs
Lc leng h o he expansion cushion a each bend leg
H soil co e dep h
E elas ici y modulus o he s eel pipe
ν
Poisson's a io o he s eel pipe
σ
y yield s eng h he s eel pipe
α
linea he mal expansion coe icien o he s eel pipe
φ
soil ic ion angle
γ
soil densi y
Ti, T ins alla ion and ope a ing empe a u e
Pi, ope a ing in e nal p essu e in he s eel pipe
Ug,
ε
g,
λ
g ea hquake induced g ound displacemen , g ound s ain, and seismic wa e leng h
FR soil ic ion eac ion
Pu maximum la e al soil eac ion
k elas ic la e al soil s i ness
kc equi alen la e al s i ness in he pipe co ne wi h expansion cushion
My yielding momen o he s eel pipe sec ion
2. Me hodology
This pape in es iga es he pe o mance o p einsula ed bonded DH pipelines, subjec ed o TGD due o seismic
wa e p opaga ion. Clea ly, his haza d a ec s DH ne wo ks, conside ably mo e han does PGD, h ea ening mainly
ansmission hyd oca bon pipelines.
4 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
The in es iga ed pipe bend DN 150/250 is composed o a cen al P235GH s eel pipe o ex e nal diame e Ds =
168.3 mm and hickness s = 4 mm, a oam insula ion o hickness PUR = 37 mm, and ex e nal plas ic man le wi h
ou e diame e D = 250 mm. The adius o he pipe bend is Rbend = 1 m, he leng h o he expansion cushion a he
co ne is Lc = 2 m, while he leng h o bo h bend legs is L = 40 m, ancho ed a he ends. The pipe is assumed bu ied
in loose sand soil wi h a co e dep h H = 0.8 m, as schema ically illus a ed in Fig. 1.
The soil-pipeline sys em subjec ed o seismic loading has been analyzed nume ically wi hin beam on Winkle
ounda ion heo y, using he ini e elemen so wa e ABAQUS/S anda d [23].
The pipeline is modeled using he PIPE31 beam elemen ype, allowing he possibili y o speci y ex e nal o
in e nal p essu e. The soil-pipeline in e ac ion is modeled wi h he sp ing-like pipe-soil in e ac ion elemen s PSI34,
ep esen ing he soil eac ion o he soil mo emen in he axial, la e al, and e ical di ec ion. One edge o he
elemen sha es nodes wi h he unde lying pipe elemen while he nodes on he o he edge a e assigned he a - ield
g ound mo ion h ough he bounda y condi ions.
The P235GH s eel pipe ma e ial model is de ined wi hin he on Mises plas ici y heo y wi h nonlinea
ha dening. The ma e ial pa ame e s a e de e mined as a unc ion o he ope a ing empe a u e T, acco ding o EN
13941 [19]. The elas ici y modulus, yield s eng h, and he linea he mal expansion coe icien a he ope a ing
empe a u e T = 90°C a e E = 208857 MPa ,
σ
y = 215.8 MPa and
α
= 12.098 10-06 1/K espec i ely, while he
Poisson's a io is ν = 0.3. A loose sand ma e ial is assumed as soil back ill, wi h he same p ope ies epo ed in he
calcula ion example o he Ge man s anda d FW 401 [4], cha ac e ized by a ic ion angle
φ
= 32.5°, and a soil
densi y
γ
= 18 kN/m3. The o ce-displacemen ela ionship is conside ed bilinea elas o-plas ic, and e alua ed
acco ding o FW 401 [5]. Speci ically, he calcula ed soil ic ion eac ion is FR = 3944 N/m, while he maximum
la e al soil eac ion is Pu = 49750 N/m, wi h an elas ic la e al soil s i ness k = 35 MPa beyond he expansion
cushion, whe e he equi alen elas ic la e al s i ness is kc = 0.247 MPa [5].
The seismic-induced g ound mo emen is applied a he ee nodes o he pipe-soil in e ac ion elemen s, as a
sinusoidal wa e p opaga ing ho izon ally in he di ec ion o he longi udinal leg.
The nume ical analysis o assessing he seismic pe o mance o he ope a ing DH pipeline a e conduc ed in wo
consecu i e s eps. A i s , a s a ic analysis is pe o med o es ablish he s ess and s ain s a e in he soil-pipeline
sys em in ope a ing condi ions wi h in e nal p essu e Pi = 12 Ba , ins alla ion and se ice empe a u e Ti = 10°C and
T = 90°C, espec i ely. In he second s ep, a ho izon al displacemen is applied quasi-s a ically a he ee nodes
ends o he pipe-soil in e ac ion elemen s, ma ching he sinusoidal pa e n de ined by:
( )
⎟
⎠
⎞
⎜
⎝
⎛
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛
=
λ
π
π
λ
ε
y
xU
g
gg
2
sin
2
(1)
whe e εg = 0.0041 is he soil s ain and
λ =
500 m is he seismic wa e leng h. Thus, he maximum alue o he
g ound displacemen esul s Ug = 0.33 m
On each loading s ep, he global equilib ium equa ions a e sol ed i e a i ely by he New on-Raphson me hod
pe mi ing o assess he pipe and soil de o ma ion s a e a each inc emen .
3. Resul s and discussion
This sec ion p esen s he s uc u al esponse o he bu ied DH pipeline e alua ed using he p oposed
me hodology. Fi s ly, he pipeline esponse is in es iga ed in ope a ing condi ions, unde he e ec o in e nal
p essu e and empe a u e a ia ion. Then he seismic pe o mance o he pipeline is analyzed in e ms o loading and
de o ma ions, o di e en alues o he maximum seismic-induced g ound displacemen Ug, as discussed u he in
his sec ion.
3.1. S uc u al esponse o he pipeline in ope a ing condi ions
The expansion o he ope a ing pipeline is coun e ac ed by he bene icial e ec o he soil ic ion, and he
bea ing o ce on he ans e se leg (Fig. 1). The maximum axial elonga ion o he pipeline in ope a ion condi ions,
220 Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 5
calcula ed nume ically (31.1 mm) is consis en wi h he heo e ical alue o he maximum axial elonga ion umax,
acco ding o he o mula epo ed in he s anda ds FW 401 [5] and EN 13941 [20]:
mmL
EA
F
L
DP
EA
Tu
s
R
s
si
s
T29.4
10
7
4
)21( 2
max ≈⋅
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛⋅−⋅
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛−
+Δ=
ν
α
(2)
Clea ly, he i s addend in Eq. (2) indica es he pipeline expansion due o he posi i e empe a u e a ia ion
Δ
T =
80°C, and in e nal p essu e Pi = 12 Ba , while he second nega i e e m ep esen s he pipeline con ac ion due o
he soil esis ance a he ou e HDPE coa ing.
The a o emen ioned alues o he maximum axial elonga ion a e consis en wi h he es ima ions using he me hod
p oposed in [22, 24-26], conside ing he bend ei he igid (30.8 mm) o lexible (31.4 mm).
The pipeline esponse in e ms o longi udinal de o ma ions does depend on he geome ical and mechanical
pa ame e s o he sys em, like he ope a ing empe a u e T , he pipe leng h L, and he bend adius Rbend.
Clea ly, he maximum longi udinal s ain in ope a ing condi ions occu s a he elbow (
ε
max = 0.42%, o T =
90°C, L = 40 m and Rbend = 1 m). A small pa ame ic s udy has shown ha he pipeline de o ma ion is accen ua ed
o g ea e ope a ing empe a u es (
ε
max = 1.03%, o T = 130°C), la ge pipe leng h (
ε
max = 0.91%, L = 80 m),
smalle bending adius (
ε
max = 0.68%, o Rbend = 0.5 m), all o he pa ame e s emaining he same, as shown in Fig.
2. These c i ical ac o s need o be ca e ully e alua ed in he design phase in o de o a oid excessi e s ess-s ain
concen a ion in he ope a ing pipeline, associa ed wi h ma e ial damage.
Fig. 2. Longi udinal s ain con ou and de o med shape o pipeline a he bend egion, unde ope a ing condi ions,
o di e en alues o he sys em pa ame e s: a) T = 90°C, L = 40 m, Rbend = 1 m; b) T = 130°C, L = 40 m, Rbend = 1
m; c) T = 90°C, L = 80 m, Rbend = 1 m; d) T = 90°C, L = 40 m, Rbend = 0.5 m.
E iden ly, he axial o ce in ope a ing condi ions is comp essi e and in he elas ic ange, wi h i s magni ude
inc easing linea ly along he pipeline om he bend egion owa ds he ancho poin s, whe e i eaches i s maximum
6 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
alue (162507 N). The obse ed linea a ia ion o he axial o ce beyond he bend egion is caused by he cons an
soil ic ion (FR = 3944 N/m) opposing he he mal expansion. Ins ead, close o he bend, he pipe axial o ce
dec eases due o he bea ing o ce on he ans e se leg (Fig. 3a).
Con e sely, he bending momen unde se ice loads is maximum a he bend (22163 Nm), exceeding he
yielding momen o he pipe sec ion (My = 18804 Nm), associa ed wi h plas ic bending s ains (Fig. 4), leading o
comp essi e plas ic longi udinal s ains (-0.3%). The la e mus be ca e ully e i ied in o de o p e en he onse o
local buckling limi s a e in he ope a ing pipeline.
Fig. 3 Va ia ion o he loads along he pipeline axis o di e en alues o he g ound displacemen Ug: a) axial
o ce; b) shea o ce; c) bending momen .

Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225 221
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 5
calcula ed nume ically (31.1 mm) is consis en wi h he heo e ical alue o he maximum axial elonga ion umax,
acco ding o he o mula epo ed in he s anda ds FW 401 [5] and EN 13941 [20]:
mmL
EA
F
L
DP
EA
Tu
s
R
s
si
s
T29.4
10
7
4
)21( 2
max ≈⋅
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛⋅−⋅
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛−
+Δ=
ν
α
(2)
Clea ly, he i s addend in Eq. (2) indica es he pipeline expansion due o he posi i e empe a u e a ia ion
Δ
T =
80°C, and in e nal p essu e Pi = 12 Ba , while he second nega i e e m ep esen s he pipeline con ac ion due o
he soil esis ance a he ou e HDPE coa ing.
The a o emen ioned alues o he maximum axial elonga ion a e consis en wi h he es ima ions using he me hod
p oposed in [22, 24-26], conside ing he bend ei he igid (30.8 mm) o lexible (31.4 mm).
The pipeline esponse in e ms o longi udinal de o ma ions does depend on he geome ical and mechanical
pa ame e s o he sys em, like he ope a ing empe a u e T , he pipe leng h L, and he bend adius Rbend.
Clea ly, he maximum longi udinal s ain in ope a ing condi ions occu s a he elbow (
ε
max = 0.42%, o T =
90°C, L = 40 m and Rbend = 1 m). A small pa ame ic s udy has shown ha he pipeline de o ma ion is accen ua ed
o g ea e ope a ing empe a u es (
ε
max = 1.03%, o T = 130°C), la ge pipe leng h (
ε
max = 0.91%, L = 80 m),
smalle bending adius (
ε
max = 0.68%, o Rbend = 0.5 m), all o he pa ame e s emaining he same, as shown in Fig.
2. These c i ical ac o s need o be ca e ully e alua ed in he design phase in o de o a oid excessi e s ess-s ain
concen a ion in he ope a ing pipeline, associa ed wi h ma e ial damage.
Fig. 2. Longi udinal s ain con ou and de o med shape o pipeline a he bend egion, unde ope a ing condi ions,
o di e en alues o he sys em pa ame e s: a) T = 90°C, L = 40 m, Rbend = 1 m; b) T = 130°C, L = 40 m, Rbend = 1
m; c) T = 90°C, L = 80 m, Rbend = 1 m; d) T = 90°C, L = 40 m, Rbend = 0.5 m.
E iden ly, he axial o ce in ope a ing condi ions is comp essi e and in he elas ic ange, wi h i s magni ude
inc easing linea ly along he pipeline om he bend egion owa ds he ancho poin s, whe e i eaches i s maximum
6 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
alue (162507 N). The obse ed linea a ia ion o he axial o ce beyond he bend egion is caused by he cons an
soil ic ion (FR = 3944 N/m) opposing he he mal expansion. Ins ead, close o he bend, he pipe axial o ce
dec eases due o he bea ing o ce on he ans e se leg (Fig. 3a).
Con e sely, he bending momen unde se ice loads is maximum a he bend (22163 Nm), exceeding he
yielding momen o he pipe sec ion (My = 18804 Nm), associa ed wi h plas ic bending s ains (Fig. 4), leading o
comp essi e plas ic longi udinal s ains (-0.3%). The la e mus be ca e ully e i ied in o de o p e en he onse o
local buckling limi s a e in he ope a ing pipeline.
Fig. 3 Va ia ion o he loads along he pipeline axis o di e en alues o he g ound displacemen Ug: a) axial
o ce; b) shea o ce; c) bending momen .
222 Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 7
The bending momen dec eases mono onically beyond he bend, in e ing i s di ec ion un il eaching wo local
peaks (17981 Nm) in he elas ic ange, loca ed symme ically a a dis ance o 2.5 m om he bend. A e wa ds, he
magni ude o he bending momen dec eases apidly o ze o, so ha beyond a dis ance o 5m om he bend, he
pipeline unde goes only axial loading (Fig. 4).
Fig. 4 Va ia ion o he s ains along he mos s essed gene a o o he pipeline o di e en alues o he g ound
displacemen Ug: a) longi udinal s ain; b) axial s ain; c) bending s ain.
8 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
3.2. S uc u al esponse o he pipeline in ope a ing condi ions
The seismic wa e p opaga ing pa allel o one longi udinal leg, e e ses he di ec ion o he ac i a ed soil ic ion
unde se ice loads (Fig. 5), subjec ing he pipeline o inc easing ensile o ces, as shown in Fig. 4 (a).
E iden ly, pipe axial o ce a ies linea ly along he pipeline axis beyond he bend egion, due o he soil ic ion
eac ion (FR = 3944 N/m), ha is assumed cons an h oughou he analysis, despi e he cyclic loading.
The pipe axial o ce is maximum a he ancho poin in he longi udinal leg, pa allel o he di ec ion o he
seismic wa e p opaga ion, dec easing linea ly he eupon, un il he bend egion whe e i inc eases sligh ly, due o he
la e al soil eac ion in ans e se leg. The linea a ia ion o he axial o ce along he pipe axis is due o he soil
ic ion eac ion (FR = 3944 N/m), ha is assumed cons an h oughou he analysis, despi e he cyclic loading.
Fig. 5. Con ou o he soil ic ion eac ion along he pipeline (N/m): a) in ope a ing condi ions; b) unde seismic
loading.
The bending momen along he pipeline in e s i s di ec ion wi h espec o he ope a ing condi ions (Fig. 4),
exceeding he elas ic limi (My = 18804 Nm), a he bending poin in he ans e se leg, loca ed a 2.4 m om he
bend. Consequen ly, wo plas ic hinges de elop a hese bending poin s du ing seismic loading, cha ac e ized by a
localiza ion o excessi e bending and longi udinal s ains, as shown in Fig. 4 and Fig. 6.
Fig. 6 Longi udinal s ain con ou and de o med shape o he pipeline a he bend egion: a) in ope a ing condi ions;
b) unde seismic loading.
Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225 223
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 7
The bending momen dec eases mono onically beyond he bend, in e ing i s di ec ion un il eaching wo local
peaks (17981 Nm) in he elas ic ange, loca ed symme ically a a dis ance o 2.5 m om he bend. A e wa ds, he
magni ude o he bending momen dec eases apidly o ze o, so ha beyond a dis ance o 5m om he bend, he
pipeline unde goes only axial loading (Fig. 4).
Fig. 4 Va ia ion o he s ains along he mos s essed gene a o o he pipeline o di e en alues o he g ound
displacemen Ug: a) longi udinal s ain; b) axial s ain; c) bending s ain.
8 Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000
3.2. S uc u al esponse o he pipeline in ope a ing condi ions
The seismic wa e p opaga ing pa allel o one longi udinal leg, e e ses he di ec ion o he ac i a ed soil ic ion
unde se ice loads (Fig. 5), subjec ing he pipeline o inc easing ensile o ces, as shown in Fig. 4 (a).
E iden ly, pipe axial o ce a ies linea ly along he pipeline axis beyond he bend egion, due o he soil ic ion
eac ion (FR = 3944 N/m), ha is assumed cons an h oughou he analysis, despi e he cyclic loading.
The pipe axial o ce is maximum a he ancho poin in he longi udinal leg, pa allel o he di ec ion o he
seismic wa e p opaga ion, dec easing linea ly he eupon, un il he bend egion whe e i inc eases sligh ly, due o he
la e al soil eac ion in ans e se leg. The linea a ia ion o he axial o ce along he pipe axis is due o he soil
ic ion eac ion (FR = 3944 N/m), ha is assumed cons an h oughou he analysis, despi e he cyclic loading.
Fig. 5. Con ou o he soil ic ion eac ion along he pipeline (N/m): a) in ope a ing condi ions; b) unde seismic
loading.
The bending momen along he pipeline in e s i s di ec ion wi h espec o he ope a ing condi ions (Fig. 4),
exceeding he elas ic limi (My = 18804 Nm), a he bending poin in he ans e se leg, loca ed a 2.4 m om he
bend. Consequen ly, wo plas ic hinges de elop a hese bending poin s du ing seismic loading, cha ac e ized by a
localiza ion o excessi e bending and longi udinal s ains, as shown in Fig. 4 and Fig. 6.
Fig. 6 Longi udinal s ain con ou and de o med shape o he pipeline a he bend egion: a) in ope a ing condi ions;
b) unde seismic loading.
224 Ge sena Banushi e al. / Ene gy P ocedia 149 (2018) 216–225
Ge sena Banushi / Ene gy P ocedia 00 (2018) 000–000 9
Pa icula ly, he la ge comp essi e s ains a he plas ic hinges may lead o local buckling and consequen pipe
ailu e, equi ing p ope mi iga ion measu es in he design phase.
Fu he mo e, he axial s ains a y linea ly along he pipeline in he elas ic ange, apa wo local peaks
de eloping a he bending poin s (Fig. 4). The la e a e p oduced by he in e ac ion be ween bending and axial
s ains as a esul o he elas oplas ic esponse o he pipe sec ion [27, 28]. Once he maximum longi udinal s ain
exceeds he yielding limi , axial s ains inc ease locally so ha he in eg al o he co esponding longi udinal s esses
is equal o he con inuously inc easing axial o ce due o he g ound displacemen .
E iden ly, he c i ical pipe egion unde going excessi e plas ic de o ma ions is de e mined by he la ge bending
momen , dissipa ing wi hin a ew pipe diame e s a ound he bend (5 m), while beyond i he pipeline is subjec ed
only o axial loading in he elas ic ange.
4. Conclusions
The p esen pape analyses he pe o mance o an ope a ing DH pipeline subjec ed o seismic loading wi hin he
ini e elemen me hodology, aking in o accoun he geome ic and mechanical p ope ies o he sys em, including
he soil-pipeline in e ac ion.
The analyzed pipeline bend su e ed plas ic s ains due o p edominan bending induced by he imposed seismic
g ound displacemen , leading o la ge comp essi e s ains associa ed wi h local buckling in a b i le ailu e mode.
The pipeline pe o mance depends on he geome ical and mechanical p ope ies o he sys em, like he ope a ing
empe a u e, he pipe leng h, and he bend adius, equi ing accu a e e alua ion in he design phase, in o de o
p e en ma e ial damage, unde se ice and seismic loading.
Mo eo e , despi e he simplis ic assump ions ega ding he adop ed nume ical model, including he
ep esen a ion o seismic loading as a sinusoidal wa e, he ob ained esul s gi e a be e unde s anding on he
ea hquake esponse o ope a ing DH pipelines. The la e is cha ac e ized by a cyclic soil-pipe in e ac ion du ing
seismic wa e p opaga ion (Fig. 7), equi ing p ope conside a ion in he enginee ing design p ac ice.
Fig. 7 Pipeline beha iou du ing: a) ope a ing condi ions; b) seismic g ound de o ma ion.
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