2021
DOI: 10.1016/j.compgeo.2021.104364
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A direct time-domain procedure for the seismic analysis of dam–foundation–reservoir systems using the scaled boundary finite element method

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Cited by 23 publications
(8 citation statements)
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“…The radiation damping of an infinite foundation is an important factor affecting the structure-foundation interaction, which can be simulated by setting artificial boundary conditions at the foundation truncation. Various artificial boundaries have been proposed to date, such as viscous boundary [10,11], viscous-spring boundary [12,13], scaled boundary finite element method [14,15], infinite elements [7,16], and perfectly matched layers [17]. Hariri-Ardebili and Saouma [18] investigated the effect of different foundation numerical models and corresponding boundary conditions on the seismic responses of arch dam-foundation systems under near-fault and far-field ground motions.…”
Section: Introductionmentioning
confidence: 99%
“…The radiation damping of an infinite foundation is an important factor affecting the structure-foundation interaction, which can be simulated by setting artificial boundary conditions at the foundation truncation. Various artificial boundaries have been proposed to date, such as viscous boundary [10,11], viscous-spring boundary [12,13], scaled boundary finite element method [14,15], infinite elements [7,16], and perfectly matched layers [17]. Hariri-Ardebili and Saouma [18] investigated the effect of different foundation numerical models and corresponding boundary conditions on the seismic responses of arch dam-foundation systems under near-fault and far-field ground motions.…”
Section: Introductionmentioning
confidence: 99%
“…The equivalent nodal forces resulting from the free-field motion can be determined from the shape function and the unit surface traction (Bazyar and Song, 2017;Huang et al, 2017;Qu et al, 2021).…”
Section: > mentioning
confidence: 99%
“…The scaled boundary finite element method (SBFEM) is a numerical method developed gradually in the course of simulation studies of elastic dynamics problems in infinite domains (Song, 2018;Wolf, 2003), which has the advantages of semi-analytical, high accuracy, reduced dimensional solution, and mesh flexibility. At present, the SBFEM has many applications to the problem of elastic wave scattering in half-space (Bazyar and Song, 2017;Chen et al, 2015b;Qu et al, 2021). Based on the theory of soil-structure interaction, the site with an open trench is decomposed into a near-field system and an infinite far-field system.…”
Section: Introductionmentioning
confidence: 99%
“…}mQD "OQ=O |QDq=@ CkO '=yx@U=Lt sHL Vy=m ut[ |a@ Q |v=t}rU 'p=Ft u=wvax@ [4] "CU= xOwRi= u=v; |=}= Rt x@ R}v |a@ Q OvJ `@=D =@ |OOa hqDN= VwQ =@ |a@ Q OvJ `@=D VwQ ? }mQD uw}UqwtQi '2021 u= Q=mty w jDWt p}Uv=Qi}O CqO=at QO =yjDWt `=wv= |R=UxDUUo |= Q@ = Q 4 FD OwOLt |=yxRwL QO 'OwW|t xO}t=v R}v 5 = Rv=m VwQ xm 'QwmPt VwQ [5] "Ov=xOQm x=Q= |RH Q=Wi `} RwD |x@U=Lt 'lR=v C=LiY w =yQ}D R}r=v; pt=W '|UOvyt swra R= |a}Uw [7w6] "CU= xOW xO=O xaUwD C}kiwt =@ """ w '?rY |=yOU uR=Nt QO |m}t=v}OwQO}y u} wv |WwQ '|a=aW |x}=B `@=wD R= xO=iDU= =@ '2019 u= Q=mty w 6 w}r 'xwqa x@ u= Q=mty w |Q}Y=@ O}y=m u}vJty [8] "Ov=xO=O O=yvW}B =yxR=U |m}D=DU= R}r=v; |= Q@ pwUt xOvU}wv "1401 3 28 VQ}PB '1401 3 18 x}LqY= '1400 12 24 Ci=} QO %M}Q=D DOI:10.24200/J30.2022.60113.3085 """ |a@ Q OvJ |xm@W uwO@ VwQ |xaUwD |=yVwQ QO xOWu=wva |=yha[ R= |NQ@ Cra x@ 'OW xQ=W= xm Qw]u=ty |= Q@ |WywSB |=yVqD 'OvQ=O R}v xm@W R= xO=iDU= QO xW} Q , =[a@ xm u}W}B |OOa QO |B uRNt OU sDU}U |}xRQr VvmQOv= p=Ut p}rLD QO xm@W R= ?=vDH= |a@ Q OvJ |xm@W uwO@ VwQ 'Q[=L VywSB QO '=DU= Q u}= QO "OvDUy u=}QH l} O=H}= 1 %Ovv=t |}=y|oS} w |= Q=O xm CU= xOW xO=O xaUwD Q=@ u}rw= |= Q@ Rm = Qt u}@ X=N |]=@DQ= w |oDUw}B sOa 2 &xvt=O QU=QU QO xDUw}B MU=B `@=D |xv}Ry Vy=m 4 &xO}J}B |=yxUOvy |R=Ux}@W QO q=@ C}r@=k 3 &|D=@U=Lt """ w &QDq=@ Oa ) @ =@ p=Ut x@ u=U; s}taD 5 &T=}ktnQR@ p=Ut pL QO C=@U=Lt "OvyO|t VWwB = Q xm@W =@ |=yVwQ ha[ \=kv R= |NQ@ 'Q}N= |=y|oS}w "CU= |= Q@ w |WQ@ Q}D |xrO=at R= |B w OU Q=DiQ |R=Ux}@W |= Q@ 'Q[=L |xar=]t QO 'VvmQOv= p=ta= |= Q@ "CU= xOW xO=iDU= 22 RDrwytry |Oa ) @wO |xrO=at R= uRNt l=N w p=}U 'xR=U |= Q@ = RHt |xvt=OQ}R xU h} QaD =@ xvt=O |x}RHD u} wv ui l} |xvt=OQ}R xU u}@ VvmQOv= |R=Ux}@W u=mt= sy 'ui u}= =@ "CU= xOW O=yvW}B O=H}= pm ? }=Q[ T} QD=t QO QiY |x}= QO |yHwD p@=k O=OaD sy w sy=Qi OwHwt xrRrR Q=@ Ot=U@ T=U= Q@ |O}OH \@=wQ R}v xv}y@ pmW Q}eDt u}}aD |= Q@ "OwW|t x@ C=@U=Lt sHL '=yu; R= xO=iDU= OL=w |xvt=O =@ |ki= l}vwtQ=y |xrRrR uDiQo Q_vQO =@ Ot=U@ |xRwL QO uRNt 1 |x]@= Q RDrwytry |xrO=at j@=]t u g (!…”
mentioning
confidence: 99%
“…; VvmQOv= p=Ut |OOa |R=Ux}@W QO uwvm=D w =DU=Q u}= QO "CU= xDiQv Q=m x@ |B uRNt OU |=ysDU}U XwYNr=|ra |Qo}O O}it |=yVwQ '|B uRNt OU VvmQOv= p=Ut R}r=v; |= Q@ , =YNWt Q}eDt `]kt =@ Q}D l} =@ = Q OU |xvO@ '2005 O=UQi w O=SvQ=]a "Ov=xDi=} xaUwD |xrO=at pL R= xm Ow@ |O}OH pmW `@=wD h} QaD =yu; Q=m |=v@t "OvOQm |R=Ux}@W Q}F -=D OvDUv=wD OwN pOt =@ =yu; "Ot;|t CUOx@ |rwvQ@ Qr} w= Q}D p}Uv=Qi}O Q@ OQ=w |m}t=v}OwQO}y Q=Wi `} RwD w OvyO u=Wv = Q uRNt OU u}@ VvmQOv= pL l} R}v 2013 |v=w}m [17] "OvQw; CUOx@ |rw@kp@=k CkO =@ = Q OU |xvO@ |Oa@wO C}=yv|@xt}v uRNt pt=W uRNt OU sDU}U |}xRQr R}r=v; |= Q@ xDU@ xO=O x=Q= Ot=U@ |xRwL QO |ki= l}vwtQ=y |xrRrR Q=@ CLD |WQ@ Q}D pOt w OU p=Ut `=wv= R= |Y=N Cr=L xJQo = 'u=W}= VywSB j}kO pLx=Q "CU= |OOa |=yVwQ |}=tR;|DU=Q |= Q@ |@ wN |=v@t Ov=wD|t |rw 'CU= uRNt |= Q@ O=}R |xv}Ry 1 %Ovv=t '|DqmWt OwOLt u=tr= Ovtv=wD VwQ [18] "OW=@ O}OH CkO Vy=m xH}DvQO w QDCWQO |=yxm@W O=H}= CQwQ[ 2 &=yxm@W CN=U Q=wWO s}taD 3 &|B uRNt OU Ovv=t 'T=}ktnQR@ |=yu=O}t |R=Ux}@W QO x= Qty x@ OwN =@ = Q """ w xO}J}B |=yxUOvy QO , =YwYNt |Oa@xU p=Ut x@ [19] "OQ=O OQ=O R=}v |mtm `]=kDt \w]N R= |t_vt |xm@W x@ OwOLt p[=iD VwQ p}rOx@ xwqax@ "OQ=O OQ@Q=m s_vt |RQt \}=QW w xUOvy |= Q@ \ki , qwtat w u=tr= VwQ QO [20] "OQ=O p=@vOx@ R}v |}q=@ |D=@U=Lt |xv}Ry '=[i pm |R=UpOt |Ov@xm@W |D=@U=Lt u=O}t |=yRQt \ki 'xm@W R= ?=vDH= hOy =@ 15 BE |RQt 16 |U=U= pL x@ R=}v BE |RQt u=tr= VwQ ha[x]kv u} QDxDUHQ@ "OvwW|t 17 SBFE xOW T=}kt OwOLt |RQt u=tr= VwQ [21] "CU= xrUt \}=QW x@ xDU@=w xO=iDU= "OQ@|t xQy@ |RQt u=tr= w OwOLt u=tr= VwQ |=y|oS}w R= u=tRty Qw] x@ VwQ u; CqmWt R= |NQ@ Ov=wD|t OwOLt |=yu=tr= VwQ l}Uqm pmW `@=wD R= CqO=at x=oDUO l} pL x@ VwQ u}= u}vJty "OW=@ xDW=O x= Qty x@ OwN =@ = Q |xv}Ry w |U=U= pL OvtR=}v xm OwW|t QHvt QB ? }=Q[ T} QD=t =@ p}Uv=Qi}O 18 DSBFE = RHt |xOWT=}kt OwOLt |RQt u=tr= VwQ [22] "CUq=@ C=@U=Lt = Q sm =L p}Uv=Qi}O CqO=at x=oDUO T} QD=t CU= xDUv=wD O}OH |=y|oS}w O=H}= =@ [23] "OyO Vy=m |Q}otWJ Qw] x@ = Q C=@U=Lt sHL w Ovm O}rwD |Q]k CQwYx@ O}=@ =yRQt |xty uwJ 'OQ=O ha[ xO}J}B |=yxUOvy |R=Ux}@W QO Q}N= VwQ 'u= Q=mty w 20 w} "OvW=@ C} -wQp@=k u; 19 LCO |rLt C=YDNt RmQt pLt R= |xO}OB R}r=v; |= Q@ = Q 21 SPH Q=wty C= QP l}t=v}OwQO}y |xm@W uwO@ VwQ 'Ov=xOQ@ Q=m x@ OU |xvO@ Q@ l}t=v}OwQO}y Q=Wi QF= uOQm ^=Lr =@ OU CUmW |= Q@ w xOW xO=iDU= uRNt |Q=Wi G=wt= |R=Ux}@W |= Q@ \ki xOWQmP VwQ |rw "Ov=xOQ@ xQy@ |mtm |=yVwQ Q}=U R= OU |R=Ux}@W %CU= xOW xO=iDU= 14 |r= 12 \@=wQ =@ j@=]t |a@ Q OvJ u}tND `@=wD R= uRNt QO u (y; !…”
mentioning
confidence: 99%