Dr. College of Civil & Hydroelectric Engineering of China Three Gorges University, Yichang,, China 2

Size: px
Start display at page:

Download "Dr. College of Civil & Hydroelectric Engineering of China Three Gorges University, Yichang,, China 2"

Transcription

1 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna Study on th Flud-Sold Intracton Mchanm o Caoh Aquduct n South-to-North Watr Dvron Mddl Ln Projct Undr Condton o Smc Load PENG Hu 1 LIU D-u 2 IAN Bn 3 1 Dr. Collg o Cvl & Hydrolctrc Engnrng o Chna hr Gorg Unvrty, Ychang,, Chna 2 Proor, Collg o Cvl & Hydrolctrc Engnrng o Chna hr Gorg Unvrty, Ychang,, Chna 3 Proor, Collg o Cvl & Hydrolctrc Engnrng o Chna hr Gorg Unvrty, Ychang,, Chna E-mal:hpng1976@163.com ABSRAC: Bad on condrng th lud-old couplng problm n aquduct, th dynamc FEM modl o lud-old ntracton wa tablhd by u o Galrkn Mthod. And th mc rpon o Caoh aquduct tructur n th South-to-North Watr Dvron Mddl Ln Projct wa calculatd. h rult ndcat that mc rpon o th aquduct tructur ncra wth th r o watr lvl, and o th lud-old ntracton wa o grat nlunc on th mc rpon o th aquduct tructur. h calculatd rult could provd good ntructon to orthcomng aquduct contructon and opratonal managmnt and aty montorng. KEYWORDS: aquduct; lud-old ntracton; mc rpon; dynamc charactrtc; South-to-North Watr Dvron Projct 1.INRODUCION In ngnrng communty, th lud-old ntracton btwn om tructur n lud and lud tl a common problm that w otn ncountr. hr an xtnv manng or projct contructon to tudy th problm o lud-old ntracton. h problm o lud-old ntracton wa rtly put orward by H. M. Wtrgaard n th 193[1]. In Chna, Pro. Zhng Zh-mn took om rarch on coupld vbraton btwn watr and plat and cantlvr n 195[2~3].In th prod o 196 to 197, th tudy on lud-old ntracton n ovra wa actv and th man rarch objct concntratd on hydraulc tructur and drnt hp whch occurrd coupld vbraton caud by watr wav. h thory o hydrolatcty wa tablhd by a Brth pcalt R. E. D.Bhop at that tm[5~7]. At prnt, gnrally thr ar two mthod whch can b ud to rarch th problm o lud-old ntracton. h rt on analytcal-numrcal mulaton, Gr doubl aymptotc approxmaton(daa) commonly ud o ar[8]; th cond on numrcal mthod, ncludng FEM, BEM, Lagrang-Eulran Mthod and o on. In lnar lud-old ntracton ytm(lnar latc tructur and dal ncomprbl lud), thr ar alo two mthod otn ud to tudy lud-old ntracton problm. h rt on through takng dplacmnt vctor o tructur and lud a ld varabl to rarch lud-old ntracton problm, uch a dplacmnt-dplacmnt chm[9~1]; th cond on to u hybrd chm whch com rom tructur dplacmnt vctor and lud ld varabl, uch dplacmnt-prur chm, dplacmnt-vlocty potntal chm and o on[11~12]. In FEM, th lud ar ncomprbl th mthod o Numrcal Computng Mthod o Addtonal Watr Ma otn appld [13~14]. Whn w condr th charactr o lud comprblty, th Galrkn Mthod appld to contruct lud-old ntracton FEM ormula btwn aquduct and watr n th papr. h rarch ndcat that numrcal mthod can mulat th couplng ntracton btwn watr and hug watr-rtanng tructur and mc rpon wll. 2.CALCULAION PRINCIPLE Flud-old ntracton problm vry complcatd and t nvolv n tructur dynamc and lud dynamc. Uually, om uppo can b mad accordng to practcal ngnrng problm. A a rult, th calculaton modl wll b mpld and cncy wll b mprovd ctvly. In th papr, w not only condr bg tructur coupld vbraton, but alo condr th ntracton btwn watr and bg tructur undr condton o mall luctuaton. In practcal calculaton, n ordr to mak calculaton convnnt w otn uppo that lud ar nvcd and rrotatonal low. Howvr, n mot condton, vn though w mak om uppo w can not obtan analytcal oluton. So w can not but tnd to numrcal mulaton mthod. Actually, om tructur wth rgular hap lk cylndr mayb u pcal uncton uch a Bl uncton to gt dal analytcal oluton. Accordng to rrnc 8, through comprhnvly condrng Nav-Stok quaton and contnuty quaton th FEM quaton wth dplacmnt-prur chm ( u, p) o unorm, nvcd and

2 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna comprbl lud undr condton o mall luctuaton ar contructd. 2.1 h dynamc modl o lud-old ntracton ytm and t bac quaton and boundary condton Hr w uppo that watr nvcd, comprbl and ur mall dturbanc. At th am tm, w can know that watr r urac appar mall luctuaton bcau aquduct locat n low mc ntnty ara. W tak aquduct tructur a lnar latc body bcau durng th cour o opraton th aquduct tructur don t allow crackng. Hr, VandV rpctvly rprnt old doman and lud doman. tand or ntrac btwn old and lud. S b lud rgd xd ntrac. S dnd a watr r urac. Su old dplacmnt boundar. S σ tand or orc boundar mpod on old. ln unt vctor o lud boundar. ntrac btwn old and lud 2.1.1Flud doman ( V ) h quaton or lud ld ar ltd a ollow: n xtrnal normal n xtrnal normal ln unt vctor o old boundar. Any pont at nand n ar oppot drcton. p 1 && p= (1), 2 c Hr p lud prur and ctand or ound vlocty n lud h boundary condton o lud p On rgd xd boundary condton ( S b) : = n (2) On watr r urac ( S ) : p 1 + && p = (3) z g 2.1.3Sold doman ( V ) h quaton or old ld ar xprd a ollow: σ + = ρ u&& (4) j, j Hr σj ar old tr componnt, u ar old dplacmnt componnt, ar old body orc componnt, ρtand or old dnty Sold body boundary condton h orc boundary condton ( S σ ) can b xprd a ollow: σ n = (5) j j h dplacmnt boundary condton ( Su) can b wrttn a ollow: u = u (6) Hr and u rpctvly rprnt th known urac orc componnt and dplacmnt componnt Condton on ntrac btwn old and lud Kntc condton on th ntrac ( ) ar that normal vlocty hould kp contnuou:

3 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna v = v n = v n = v n = v (7) n n By man o moton quaton o nvcd, wakly dturbd lud, th quaton 7 can b changd a ollow: p + ρ u&& n = (on ntrac S ) (8) n Hr utand or old dplacmnt vctor, ρ lud dnty. h contnuou condton o orc on ntrac ( ) ar xprd a ollow: σ n = τ n = τ n (9) j j j j j j h quaton 9 man that normal orc on ntrac ar contnuou. Hr componnt. I th lud ar nvcd thnτ j can b wrttn a ollow: τ j tand or lud tr tnor τ j = pδ (1) j By ubttuton quaton 1 nto quaton 9 w can gt: σ jnj = pn (on ntrac S ) (11) 2.2 Etablhmnt o lud-old ntracton FEM quaton bad on Galrkn Mthod 2.2.1Contructng ntrpolaton uncton For lud prur pattrn appld and prur dtrbuton n lud lmnt can b xprd a ollow: m pxyzt (,,,) N ( xyz,, ) p () t = Np (12) = 1 Hr mar nod numbr o lud lmnt, p ar nod prur vctor o lud lmnt, N ntrpolaton uncton corrpondng to nod No., N ntrpolaton uncton matrx. For old bod dplacmnt pattrn ud and dplacmnt dtrbuton n old lmnt can b ltd a ollow: u u m m u ( xyzt,,,) = v N( xyz,, ) v = N( xyz,, ) a () t = Na (13) = 1 = 1 w w Hr mar nod numbr o old lmnt, a ar nod dplacmnt vctor o old lmnt, N ntrpolaton uncton corrpondng to nod No., N ntrpolaton uncton matrx Drvd olvng quaton by man o Galrkn Mthod h wghtd rdual oluton o Galrkn Mthod or bac quaton and boundary condton o lud-old ntracton n lud doman can b wrttn a ollow: 1 p 1 p p δ p( p && pdv ) δ p( ) ds δ p( && p+ ) ds δ p( + ρ && ) ds = (14) u n, 2 c n V Sb g z n S For old doman uppod that dplacmnt boundary condton hav bn atd and thn th ormula n old doman can b xprd:

4 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna δu ( σ + ρ u&& ) dv δu ( σ n ) ds δu ( σ n pn ) ds = (15) j, j j j j j V Sσ hrough applcaton o ntgraton by part to rt tm δp( p, ) dv o ormula (14), w can obtan ormula (16):,, 2 c g V S V 1 1 [( δ p ) p + && pdv ] + δ p( && pds ) + δ p( ρ && ) ds = (16) u n Smlarly by u o ntgraton by part to rt tm δu ( σ, ) dv o ormula (15) and ubttutng t nto phycal quaton, thn w can gt ormula: j jkl kl V Sσ V j j [ δε D ε + δu ( ρ u&& )] dv δuds + δu ( pn ) ds = (17) By ubttuton ormula (12) and ormula (13) nto ormula (16) and ormula (17) rpctvly and at th am tm condrng th arbtrarn o ollow: δpandδ u, th FEM quaton o lud-old ntracton can b xprd a 1 M && a KS Q ρ a F + = Q M p&& p K (18) Hr par prur vctor on lud nod, aar dplacmnt vctor on old nod, Q lud-old couplng matrx, M and Kar global lud ma matrx and global lud tn matrx rpctvly, Mand Kar global old ma matrx and global old tn matrx rpctvly, Far xtrnal load vctor mpod on old. Each lmnt matrx corrpondng to global matrx can b xprd: M 1 1 = NN dv + NN ds ; = N N K dv ; Q ρ ds x x = NnN ; M = ρnn dv ; 2 c g V S = V K BDB dv ; F = N dv + N ds,hr B dplacmnt-tran rlaton matrx o old. From V V Sσ V abov calculaton proc w can that M cont o two part. h rt part MV and th cond part M.So w can know that M = M + M.Hr V MV lmnt ma matrx caud by comprbl lud, M lmnt ma matrx caud by r urac wav problm. Whn condrng th rpon o aquduct undr condton o arthquak, th FEM quaton o lud-old ntracton can b wrttn a ollow: 1 1 M && a M a& KS Q S ρ a& K Q α β ρ a F = Q M p&& Q M p& p & p K K (19)

5 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna 1 M a& KS Q Hr α ρ a& C= + β dampng matrx, αand βar proportonal ma and Q M p& p & K tn dampng cocnt rpctvly. 3.FEM MODEL OF AQUEDUC Caoh Aquduct locat n Shnxng own, Manchng County, Baodng Cty, Hb Provnc. h aquduct a larg pan cro tructur n South-to-North Watr Dvron Mddl Ln Projct. h dgnd dcharg 125 m 3 /,th maxmum dgnd dcharg 15 m 3 /.h pan o aquduct 3m and th tructur o ngl conncton o thr lum wth mult-d wall appld. Each lum cro cton z m and th thckn o d wall.6m. At th top o d wall 2m thck pdtran plat ar pavd. h thckn o mddl wall btwn ach lum.7m. Smlarly, 2.7m thck pdtran plat ar pavd on th top o mddl wall. Longtudnal prtrd tructur ar ud by d wall and mddl wall. Sd rb and bottom rb ar xd n aquduct body. On th top o th d wall and mddl wall, pull rod ar alo contructd. h pacng o d rb 2.5m, th wdn and hght o d rb ar.5m and.7m rpctvly. h pacng o bottom rb alo 2.5m, th wdn and hght o bottom rb ar.5m and 1.1m rpctvly. h wdn and hght o pull rod ar.3m and.4m rpctvly. h matral o aquduct C5 grad rnorcd concrt whch maxmum comprv trngth about 5MPa. Fgur on h cro cton o aquduct 3.1 h 3-D FEM modl h ngl-pan aquduct 3m long and 22m wd. In th papr ttrahdron lmnt ud to calculat aquduct tructur. h rod lmnt appld to mulat tl trand and om tl bar. A total numbr o lmnt ar ubdvdd. h X-coordnat n th am drcton wth watr low. h Y-coordnat paralll to aquduct wd drcton. h Z-coordnat n th am drcton wth lvaton o aquduct. h 3-D FEM modl obtand by ot ANSYS. ELEMENS NOV :4:3 Y Z X Fgur two h 3-D FEM modl o aquduct

6 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna 3.2 Calculaton ca In ordr to nur a opraton and obtan rlabl conomc bnt, t ncary to tak numrcal mulaton on hgh trngth and larg pan aquduct tructur. Accordng to ngnrng practc and projct contructon plannng, x calculaton ca ar chon n th papr. 1thr lum pang watr undr condton o dgnd watr dpth(4.15m) and condrng aquduct gravty; 2thr lum pang watr undr condton o ncrad watr dpth(4.792m) and condrng aquduct gravty; 3thr lum pang watr undr condton o bankull watr dpth(5.4m) and condrng aquduct gravty; 4thr lum pang watr undr condton o bankull watr dpth(5.4m) and condrng aquduct gravty and wnd load; 5only mddl lum pang watr undr condton o ncrad watr dpth(4.792m) and condrng aquduct gravty; 6only two d lum pang watr undr condton o ncrad watr dpth(4.792m) and condrng aquduct gravty. h calculaton otwar wa l-dvlopd and th otwar could ntrac wth ANSYS and Autocad. In th pat v yar, th otwar hav bn uccully appld to om hug hydropowr projct n Chna, uch a hr Gorg Projct, Jnpng arch dam and Xaowan arch dam. 3.3 h choong o mc wav Whn takng mc rpon calculaton on aquduct, t ncary to choo raonabl mc wav bcau wavorm hav proound ct on mc rpon o aquduct. Accordng to t condton o aquduct, or th ak o thoroughly rlctng mc rpon o aquduct undr condton o drnt mc wav, n th papr EL-Cntro wav, at wav, Paadna wav ar chon a ground acclraton. h mc wav nput mthod ltd a ollow: whn tranvr xctaton ourc happnng thn EW componnt o EL-Cntro wav, at wav, Paadna wav hould b nputtd. I vrtcal xctaton ourc takng plac, thn NS componnt o EL-Cntro wav, at wav hav to b nputtd. h concrt numrcal valu and maxmum ampltud ar conrmd accordng to rrnc [15]. 3.4 Calculaton rult Bor undrtakng dynamc analy watr can b takn a a knd o addtonal ma o aquduct tructur. Whn calculaton w can know that n th ntak and outlt o aquduct watr r and th boundary condton n ntak and outlt o aquduct ar p/ n=. Calculaton rult manly nclud thr part. h rt part tranvr dplacmnt n bottom plat n th mddl o thr lum rpctvly. h cond part longtudnal dplacmnt n bottom plat n th mddl o thr lum rpctvly. h thr part rotaton angl o mddl cro cton ntrwnng ax o thr lum rpctvly (bcau o mor calculaton ca, th calculatd tr and dplacmnt contour plot ar canclld). Man calculaton rult ar ltd a ollow: 3.4.1ranvr dplacmnt n bottom plat n th mddl o thr lum h maxmum tranvr dplacmnt n bottom plat n th mddl o thr lum rpctvly ar ltd n tabl on undr condton o EW componnt xctaton o EL-Cntro wav, at wav, Paadna wav. From tabl on w can know that th dtrbuton law and changng trnd o tranvr dplacmnt n bottom plat n th mddl o thr lum ar mlar. Howvr, tranvr dplacmnt n bottom plat n th mddl lum bggr than that o n two d lum. Wth watr dpth ncrang, th ma o aquduct ncra too. A a rult, tranvr dplacmnt n bottom plat n th mddl o thr lum gradually ncrad. Furthrmor, undr condton o cro-wnd load acton, tranvr dplacmnt n bottom plat n th mddl o thr lum a lttl largr than that o wthout condrng cro-wng load acton. h ncrang ampltud not obvou whch ndcat that watr can ctvly rduc tranvr mc rpon. Fgur 1 th maxmum tranvr dplacmnt n bottom plat n th mddl o thr lum Maxmum tranvr dplacmnt(mm) poton ca1 ca2 ca3 ca4 ca5 ca6 Bottom plat n th mddl o rght lum Bottom plat n mddl lum Bottom plat n th mddl o lt lum Rotaton angl o mddl cro cton ntrwnng ax o thr lum

7 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna h maxmum rotaton angl o mddl cro cton ntrwnng ax o thr lum rpctvly ar ltd n tabl two undr condton o EW componnt xctaton o EL-Cntro wav, at wav, Paadna wav. From calculaton rult, th dtrbuton law and changng trnd o rotaton angl o mddl cro cton ntrwnng ax o thr lum ar am. Actually, rotaton angl n th mddl lum bggr than that o two d lum. Smlarly, condrng cro-wnd load acton th maxmum rotaton angl o mddl cro cton ntrwnng ax o thr lum rpctvly ar largr that that o wthout condrng cro-wnd load. Wth watr dpth ncrang, th ma o aquduct ncra too. A a rult, th maxmum rotaton angl o mddl cro cton ntrwnng ax o thr lum rpctvly ncra too. In act, th dtrbuton law and changng trnd o rotaton angl o mddl cro cton ntrwnng ax o thr lum bor and atr watr lvl changng ar am. So w can know that lud-old ntracton obvouly act th valu o rotaton angl but l obvouly act dtrbuton law o rotaton angl. Flud-old ntracton calculaton alo ndcat that mc rpon aroud by longtudnal wav l than that o tranvr wav. abl 2 h maxmum rotaton angl o mddl cro cton ntrwnng ax o thr lum Maxmum rotaton angl(rad) poton ca1 ca2 ca3 ca4 ca5 ca6 Cro cton n th mddl o rght lum Cro cton n mddl lum Cro cton n th mddl o lt lum Longtudnal dplacmnt n bottom plat n th mddl o thr lum h maxmum longtudnal dplacmnt n bottom plat n th mddl o thr lum rpctvly ar ltd n tabl thr undr condton o NS componnt xctaton o EL-Cntro wav, at wav. From calculaton rult w can know that th maxmum longtudnal dplacmnt tak plac n artht pont on aquduct along mc tranmon drcton (rght lum ar rom that o mc ourc). Howvr, no mattr whthr condrng lud-old ntracton or not, wth watr dpth ncrang, th ma o aquduct ncra too. A a rult, longtudnal dplacmnt n bottom plat n th mddl o thr lum gradually ncrad. Furthrmor, undr condton o cro-wnd load acton, longtudnal dplacmnt n bottom plat n th mddl o thr lum a lttl largr than that o wthout condrng cro-wng load acton. h ncrang ampltud not obvou whch ndcat that watr can ctvly rduc longtudnal mc rpon. ranvr wav mpo lttl ct on longtudnal dplacmnt. abl 3 th maxmum longtudnal dplacmnt n bottom plat n th mddl o thr lum Maxmum longtudnal dplacmnt(mm) poton ca1 ca2 ca3 ca4 ca5 ca6 Bottom plat n th mddl o rght lum Bottom plat n mddl lum Bottom plat n th mddl o lt lum Vrtcal dplacmnt n bottom plat n th mddl o thr lum h maxmum vrtcal dplacmnt n bottom plat n th mddl o thr lum aroud by tranvr wav and longtudnal wav ar vry mall rpctvly. Calculaton ndcat that no mattr whthr condrng lud-old ntracton or not th vrtcal dplacmnt chang a lttl. It how that lud-old ntracton ha lttl nlunc on aquduct vrtcal dplacmnt. 4.CONCLUSIONS (1) Rult o drnt calculaton ca ndcat that condrng lud-old ntracton n aquduct and drnt watr dpth hav clo rlaton wth aquduct mc rpon. It ncary to tudy lud-old ntracton mchanm undr condton o mc wav acton[15]. (2) Drnt mc rpon can b obtan undr condton o drnt mc wav xctaton. Although calculaton rult changng trnd ar mlar th valu o rult ar drnt. So, n practcal projct w mut

8 h 14 th World Conrnc on Earthquak Engnrng Octobr 12-17, 28, Bjng, Chna condr raonabl xctaton drcton and mc wav. (3) Undr condton o cro-wnd load acton th maxmum longtudnal and tranvr dplacmnt ar a lttl largr than that o wthout cro-wnd acton. It ndcat that watr body can ctvly rduc mc rpon o aquduct. (4) h maxmum longtudnal dplacmnt aroud by tranvr wav vry mall. h mc rpon o aquduct brought by longtudnal wav acton l than that o tranvr wav acton. ACKNOWLEDGEMEN: h rarch wa upportd by Natonal Natural Scnc Foundaton o Chna (NSFC, wth grantd numbr: ). W thank Proor Huang Da-ha or commnt on th manucrpt. REFERENCES [1]Wtrgaard H M. Watr prur on dam durng arthquak[j].ran. o Amrcan Socty o Cvl Engnrng,1933,59 (3) : [2]Zhng Zh-mn. h vbraton o plat undr condton o lud acton[j].acta Mchanca Snca, 958,2 (1) : [3]Zhng Zh-mn, Ma Zong-ku. Fr vbraton o cantlvr undr condton o latral lud acton[j]. Acta Mchanca Snca,1959,3 (2) : [4]Gpanpan J E. Flud-old ntracton[a].h Wntr Annual Mtng o th ASME[C].Pttbrgh, Pnnylvana, [5]Bhop R E D, Prc W G. Hydrolatcty o Shp[M].Cambrdg :Cambrdg Unvrty Pr,1979. [6]Znkwcz O C, Btt P. Flud-tructur dynamc ntracton and wav orc: An Introducton to numrcal tratmnt [J]. Intrnatonal Journal or Numrcal Mthod n Engnrng, 1978,13 (1) :1-16. [7]FENG Zhn2xng, Hung C.h coupld BE/ FE algorthm or lud2tructur ntracton : 2-D and 3-D numrcal rult[j]. Acta Mchanca and Scnta, 1987,7(2). [8]Lu Xn-n.Advancd Structural Dynamc[M].Shangha: Shangha Jaotong Unvrty Pr, [9]2Alrdo B, Rodolo R. Fnt lmnt computaton o th vbraton mod o a lud-old ytm, [J]. Comput Mthod, Appl Mh Eugrg, 1994, [1]Alrdo B, Rodolo R, Rodrguz R. Fnt lmnt oluton o ncomp rbl lud-trucur vbraton p roblm [J]. Intrnatonal Journal or numrcalmthod n ngnrng, 1997:4-42. [11]Lu W K, Chang H G. Multdcp lnary and ntracton problm: A mthod o computaton or lud tructur ntracton,[j] Computr & Structur, 1985, 2 :1-3. [12]Da Da-nong, Wang Xu-chng, Du Qng-hua.A modl analy or th dynamc rpon o lud-tructur ytm[j].acta Mchnca Solda Snca, 199, 11 (4) : [13]Jn Zhan-l,Wang Zong-l,L Hong-yun. Numrcal Computng Mthod o Addtonal Watr Ma whn th Structur Vbrat n th Innt Lqud[J]. Journal o Shangha Jaotong Unvrty, 2, 34 (8). [14]Wang Xu-chng. Fnt Elmnt Mthod[M].Bjng: nghua Unvrty Pr,July,23 [15]Wang Bo, Chn Hua, Xu W. Nonlnar mc rpon analy o aquduct contructd wth lad rubbr barng or vbraton olaton [J].Watr Rourc and Hydropowr Engnrng, Jun,25,Vol.25 No.3:5-7.

Exercises for lectures 7 Steady state, tracking and disturbance rejection

Exercises for lectures 7 Steady state, tracking and disturbance rejection Exrc for lctur 7 Stady tat, tracng and dturbanc rjcton Martn Hromčí Automatc control 06-3-7 Frquncy rpon drvaton Automatcé řízní - Kybrnta a robota W lad a nuodal nput gnal to th nput of th ytm, gvn by

More information

MECH321 Dynamics of Engineering System Week 4 (Chapter 6)

MECH321 Dynamics of Engineering System Week 4 (Chapter 6) MH3 Dynamc of ngnrng Sytm Wk 4 (haptr 6). Bac lctrc crcut thor. Mathmatcal Modlng of Pav rcut 3. ompl mpdanc Approach 4. Mchancal lctrcal analogy 5. Modllng of Actv rcut: Opratonal Amplfr rcut Bac lctrc

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved.

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved. Journal o Thortcal and Appld Inormaton Tchnology th January 3. Vol. 47 No. 5-3 JATIT & LLS. All rghts rsrvd. ISSN: 99-8645 www.att.org E-ISSN: 87-395 RESEARCH ON PROPERTIES OF E-PARTIAL DERIVATIVE OF LOGIC

More information

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION CHAPTER 7d. DIFFERENTIATION AND INTEGRATION A. J. Clark School o Engnrng Dpartmnt o Cvl and Envronmntal Engnrng by Dr. Ibrahm A. Assakka Sprng ENCE - Computaton Mthods n Cvl Engnrng II Dpartmnt o Cvl and

More information

Static/Dynamic Deformation with Finite Element Method. Graphics & Media Lab Seoul National University

Static/Dynamic Deformation with Finite Element Method. Graphics & Media Lab Seoul National University Statc/Dynamc Dormaton wth Fnt Elmnt Mthod Graphcs & Mda Lab Sol Natonal Unvrsty Statc/Dynamc Dormaton Statc dormaton Dynamc dormaton ndormd shap ntrnal + = nrta = trnal dormd shap statc qlbrm dynamc qlbrm

More information

Challenges and Experiences in Model Reduction for Mechanical Systems Illustrated for the Reduction of a Crankshaft

Challenges and Experiences in Model Reduction for Mechanical Systems Illustrated for the Reduction of a Crankshaft ODRED 010 Challng and Exrnc n odl Rducton for chancal Sytm Illutratd for th Rducton of a Crankhaft Chrtn Gchwndr, Jörg Fhr und tr Ebrhard Inttut of Engnrng and Comutatonal chanc Unvrty of Stuttgart, Grmany

More information

A Note on Estimability in Linear Models

A Note on Estimability in Linear Models Intrnatonal Journal of Statstcs and Applcatons 2014, 4(4): 212-216 DOI: 10.5923/j.statstcs.20140404.06 A Not on Estmablty n Lnar Modls S. O. Adymo 1,*, F. N. Nwob 2 1 Dpartmnt of Mathmatcs and Statstcs,

More information

From Structural Analysis to FEM. Dhiman Basu

From Structural Analysis to FEM. Dhiman Basu From Structural Analyss to FEM Dhman Basu Acknowldgmnt Followng txt books wr consultd whl prparng ths lctur nots: Znkwcz, OC O.C. andtaylor Taylor, R.L. (000). Th FntElmnt Mthod, Vol. : Th Bass, Ffth dton,

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach Unv.Prof. r. J. FrankVbach WS 067: Intrnatonal Economcs ( st xam prod) Unvrstät Sgn Fakultät III Unv.Prof. r. Jan FrankVbach Exam Intrnatonal Economcs Wntr Smstr 067 ( st Exam Prod) Avalabl tm: 60 mnuts

More information

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES 13 th World Confrnc on Earthquak Engnrng Vancouvr, B.C., Canada August 1-6, 4 Papr No. 485 ORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WIT VARIABLE PROPERTIES Mngln Lou 1 and Wnan Wang Abstract:

More information

The Hyperelastic material is examined in this section.

The Hyperelastic material is examined in this section. 4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):

More information

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd

More information

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 6: Heat Conduction: Thermal Stresses

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 6: Heat Conduction: Thermal Stresses 16.512, okt Proulon Prof. Manul Martnz-Sanhz Ltur 6: Hat Conduton: Thrmal Str Efft of Sold or Lqud Partl n Nozzl Flow An u n hhly alumnzd old rokt motor. 3 2Al + O 2 Al 2 O 2 3 m.. 2072 C, b.. 2980 C In

More information

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS COMPUTTION FUID DYNMICS: FVM: pplcatons to Scalar Transport Prolms ctur 3 PPICTIONS OF FINITE EEMENT METHOD TO SCR TRNSPORT PROBEMS 3. PPICTION OF FEM TO -D DIFFUSION PROBEM Consdr th stady stat dffuson

More information

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions 9 Strss-Basd Fnt Elmnt Mthods for Dynamcs Analyss of Eulr-Brnoull Bams wth Varous Boundary Condtons Abstract In ths rsarch, two strss-basd fnt lmnt mthods ncludng th curvatur-basd fnt lmnt mthod (CFE)

More information

167 T componnt oftforc on atom B can b drvd as: F B =, E =,K (, ) (.2) wr w av usd 2 = ( ) =2 (.3) T scond drvatv: 2 E = K (, ) = K (1, ) + 3 (.4).2.2

167 T componnt oftforc on atom B can b drvd as: F B =, E =,K (, ) (.2) wr w av usd 2 = ( ) =2 (.3) T scond drvatv: 2 E = K (, ) = K (1, ) + 3 (.4).2.2 166 ppnd Valnc Forc Flds.1 Introducton Valnc forc lds ar usd to dscrb ntra-molcular ntractons n trms of 2-body, 3-body, and 4-body (and gr) ntractons. W mplmntd many popular functonal forms n our program..2

More information

Modeling and Simulation Analysis of Power Frequency Electric Field of UHV AC Transmission Line

Modeling and Simulation Analysis of Power Frequency Electric Field of UHV AC Transmission Line (IJACSA) Intrnatonal Journal of Advancd Computr Scnc and Applcatons, Vol., o., Modlng and Smulaton Analyss of Powr Frquncy Elctrc Fld of UHV AC Transmsson Ln Chn Han Collg of Elctronc and Elctrcal Engnrng

More information

Engineering Circuit Analysis 8th Edition Chapter Nine Exercise Solutions

Engineering Circuit Analysis 8th Edition Chapter Nine Exercise Solutions Engnrng rcu naly 8h Eon hapr Nn Exrc Soluon. = KΩ, = µf, an uch ha h crcu rpon oramp. a For Sourc-fr paralll crcu: For oramp or b H 9V, V / hoo = H.7.8 ra / 5..7..9 9V 9..9..9 5.75,.5 5.75.5..9 . = nh,

More information

EE750 Advanced Engineering Electromagnetics Lecture 17

EE750 Advanced Engineering Electromagnetics Lecture 17 EE75 Avan Engnrng Eltromagnt Ltur 7 D EM W onr a D ffrntal quaton of th form α α β f ut to p on Γ α α. n γ q on Γ whr Γ Γ Γ th ontour nlong th oman an n th unt outwar normal ot that th ounar onton ma a

More information

Equil. Properties of Reacting Gas Mixtures. So far have looked at Statistical Mechanics results for a single (pure) perfect gas

Equil. Properties of Reacting Gas Mixtures. So far have looked at Statistical Mechanics results for a single (pure) perfect gas Shool of roa Engnrng Equl. Prort of Ratng Ga Mxtur So far hav lookd at Stattal Mhan rult for a ngl (ur) rft ga hown how to gt ga rort (,, h, v,,, ) from artton funton () For nonratng rft ga mxtur, gt mxtur

More information

Outline. Types of Experimental Designs. Terminology. EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Lecture 12

Outline. Types of Experimental Designs. Terminology. EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Lecture 12 EEC 686/785 Modlng & Prformanc Evaluaton of Computr Sytm Lctur Outln Rvw of lctur r Factoral Dgn wth Rplcaton Dpartmnt of Elctrcal and Computr Engnrng Clvland Stat Unvrty wnbng@.org (bad on Dr. Ra Jan

More information

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd

More information

Logistic Regression I. HRP 261 2/10/ am

Logistic Regression I. HRP 261 2/10/ am Logstc Rgrsson I HRP 26 2/0/03 0- am Outln Introducton/rvw Th smplst logstc rgrsson from a 2x2 tabl llustrats how th math works Stp-by-stp xampls to b contnud nxt tm Dummy varabls Confoundng and ntracton

More information

Polytropic Process. A polytropic process is a quasiequilibrium process described by

Polytropic Process. A polytropic process is a quasiequilibrium process described by Polytropc Procss A polytropc procss s a quasqulbrum procss dscrbd by pv n = constant (Eq. 3.5 Th xponnt, n, may tak on any valu from to dpndng on th partcular procss. For any gas (or lqud, whn n = 0, th

More information

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM Avalabl onln at www.scncdrct.com Procda Engnrng 9 () 373 377 Intrnatonal Workshop on Informaton and Elctroncs Engnrng (IWIEE) Thr-Nod Eulr-Brnoull Bam Elmnt Basd on Postonal FEM Lu Jan a *,b, Zhou Shnj

More information

Naresuan University Journal: Science and Technology 2018; (26)1

Naresuan University Journal: Science and Technology 2018; (26)1 Narsuan Unvrsty Journal: Scnc and Tchnology 018; (6)1 Th Dvlopmnt o a Corrcton Mthod or Ensurng a Contnuty Valu o Th Ch-squar Tst wth a Small Expctd Cll Frquncy Kajta Matchma 1 *, Jumlong Vongprasrt and

More information

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization THE UNIVERSITY OF MARYLAND COLLEGE PARK, MARYLAND Economcs 600: August, 007 Dynamc Part: Problm St 5 Problms on Dffrntal Equatons and Contnuous Tm Optmzaton Quston Solv th followng two dffrntal quatons.

More information

Hidden variable recurrent fractal interpolation function with four function contractivity factors

Hidden variable recurrent fractal interpolation function with four function contractivity factors Hddn varabl rcurrnt fractal ntrpolaton functon wth four functon contractvt factor Chol-Hu Yun Facult of Mathmatc Km Il ung Unvrt Pongang Dmocratc Popl Rpublc of Kora Abtract: In th papr w ntroduc a contructon

More information

ME 200 Thermodynamics I Spring 2014 Examination 3 Thu 4/10/14 6:30 7:30 PM WTHR 200, CL50 224, PHY 112 LAST NAME FIRST NAME

ME 200 Thermodynamics I Spring 2014 Examination 3 Thu 4/10/14 6:30 7:30 PM WTHR 200, CL50 224, PHY 112 LAST NAME FIRST NAME M 00 hrodynac Sprng 014 xanaton 3 hu 4/10/14 6:30 7:30 PM WHR 00, CL50 4, PHY 11 Crcl your dvon: PHY 11 WHR 00 WHR 00 CL50 4 CL50 4 PHY 11 7:30 Joglkar 9:30 Wagrn 10:30 Gor 1:30 Chn :30 Woodland 4:30 Srcar

More information

ARCH DAM OPTIMIZATION CONSIDERING FLUID-STRUCTURE INTERACTION WITH FREQUENCY CONSTRAINTS USING ARTIFICIAL INTELLIGENCE METHODS

ARCH DAM OPTIMIZATION CONSIDERING FLUID-STRUCTURE INTERACTION WITH FREQUENCY CONSTRAINTS USING ARTIFICIAL INTELLIGENCE METHODS Th 4 th World Confrnc on Earthqak Engnrng Octobr -7, 008, Bjng, Chna ARCH DAM OPTIMIZATION CONSIDERING FLUID-STRUCTURE INTERACTION WITH FREQUENCY CONSTRAINTS USING ARTIFICIAL INTELLIGENCE METHODS J. Salajghh,

More information

Lecture 4: Parsing. Administrivia

Lecture 4: Parsing. Administrivia Adminitrivia Lctur 4: Paring If you do not hav a group, pla pot a rqut on Piazzza ( th Form projct tam... itm. B ur to updat your pot if you find on. W will aign orphan to group randomly in a fw day. Programming

More information

Source code. where each α ij is a terminal or nonterminal symbol. We say that. α 1 α m 1 Bα m+1 α n α 1 α m 1 β 1 β p α m+1 α n

Source code. where each α ij is a terminal or nonterminal symbol. We say that. α 1 α m 1 Bα m+1 α n α 1 α m 1 β 1 β p α m+1 α n Adminitrivia Lctur : Paring If you do not hav a group, pla pot a rqut on Piazzza ( th Form projct tam... itm. B ur to updat your pot if you find on. W will aign orphan to group randomly in a fw day. Programming

More information

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges Physcs of Vry Hgh Frquncy (VHF) Capactvly Coupld Plasma Dschargs Shahd Rauf, Kallol Bra, Stv Shannon, and Kn Collns Appld Matrals, Inc., Sunnyval, CA AVS 54 th Intrnatonal Symposum Sattl, WA Octobr 15-19,

More information

1- Summary of Kinetic Theory of Gases

1- Summary of Kinetic Theory of Gases Dr. Kasra Etmad Octobr 5, 011 1- Summary of Kntc Thory of Gass - Radaton 3- E4 4- Plasma Proprts f(v f ( v m 4 ( kt 3/ v xp( mv kt V v v m v 1 rms V kt v m ( m 1/ v 8kT m 3kT v rms ( m 1/ E3: Prcntag of

More information

MODELLING OF LAMINATE COMPOSITES WITH EMBEDDED PIEZOELECTRIC ACTUATORS AND SENSORS UDC : :62-521

MODELLING OF LAMINATE COMPOSITES WITH EMBEDDED PIEZOELECTRIC ACTUATORS AND SENSORS UDC : :62-521 FACA UNIRSIAIS Sr: Mchanc, Automatc Control and Robotc ol.4, N o 6, 24, pp. 5-2 MODLLING OF LAMINA COMPOSIS WIH MDDD PIZOLCRIC ACUAORS AND SNSORS UDC 57.6.86:5.82.7:62-52 Dragan Marnovć,2, Ulrch Gabbrt

More information

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY Stud of Dnamc Aprtur for PETRA III Rng K. Balws, W. Brfld, W. Dcng, Y. L DESY FLS6 Hamburg PETRA III Yong-Jun L t al. Ovrvw Introducton Dnamcs of dampng wgglrs hoc of machn tuns, and optmzaton of stupol

More information

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Ch. 9 Common Emitter Amplifier

Ch. 9 Common Emitter Amplifier Ch. 9 Common mttr mplfr Common mttr mplfr nput and put oltags ar 180 o -of-phas, whl th nput and put currnts ar n-phas wth th nput oltag. Output oltag ( V ) V V V C CC C C C C and V C ar -of-phas 10 μ

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

Period vs. Length of a Pendulum

Period vs. Length of a Pendulum Gaphcal Mtho n Phc Gaph Intptaton an Lnazaton Pat 1: Gaphng Tchnqu In Phc w u a vat of tool nclung wo, quaton, an gaph to mak mol of th moton of objct an th ntacton btwn objct n a tm. Gaph a on of th bt

More information

ANALYTICAL FUNCTIONAL FORM AND FITTING PROCEDURE

ANALYTICAL FUNCTIONAL FORM AND FITTING PROCEDURE Elctronc Supplmntary Matral (ESI) for Phycal Chmtry Chmcal Phyc. Th journal th Onr Soct 6 Supplmntary Informaton Ttl: at contant calculaton of th GH + OH/O GH + H O/HO racton ung an ab nto bad full-dmnonal

More information

Volume Scattering. Our challenge is to determine how a monochromatic plane wave might scatter and propagate through such a medium.

Volume Scattering. Our challenge is to determine how a monochromatic plane wave might scatter and propagate through such a medium. 11/3/4 Volum Scattrng 1/4 Volum Scattrng In many radar rmot nng applcaton, th llumnatd targt a random collcton of rrgular partcl or lmnt, dprd throughout om 3- dmnonal volum. Our challng to dtrmn how a

More information

Neural Network Control for the Linear Motion of a Spherical Mobile Robot

Neural Network Control for the Linear Motion of a Spherical Mobile Robot Nural Ntwork Control for th Lnar Moton of a Sphrcal Mobl Robot Rgular Papr Yao Ca, Qang Zhan * and X X Robotc Inttut, Bjng Unvrty of Aronautc and Atronautc, Bjng *Corrpondng author E-mal: qzhan@buaa.du.cn

More information

Study interaction between intensive circularly polarized laser and hydrogen atom using a matrix method

Study interaction between intensive circularly polarized laser and hydrogen atom using a matrix method ISBN 978-1-84626-020-9 Procdngs of 3 rd Intrnatonal Workshop on Matrx Analyss angzhou,p.r.chna.july 9-13, 2009, pp. 199-202 ( Wll st y th pulshr ) Study ntracton twn ntnsv crcularly polarzd lasr and hydrogn

More information

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn.

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn. Modul 10 Addtonal Topcs 10.1 Lctur 1 Prambl: Dtrmnng whthr a gvn ntgr s prm or compost s known as prmalty tstng. Thr ar prmalty tsts whch mrly tll us whthr a gvn ntgr s prm or not, wthout gvng us th factors

More information

JEE-2017 : Advanced Paper 2 Answers and Explanations

JEE-2017 : Advanced Paper 2 Answers and Explanations DE 9 JEE-07 : Advancd Papr Answrs and Explanatons Physcs hmstry Mathmatcs 0 A, B, 9 A 8 B, 7 B 6 B, D B 0 D 9, D 8 D 7 A, B, D A 0 A,, D 9 8 * A A, B A B, D 0 B 9 A, D 5 D A, B A,B,,D A 50 A, 6 5 A D B

More information

APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF 3D DIFFUSION IN SOLIDS

APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF 3D DIFFUSION IN SOLIDS Cênca/Scnc APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF D DIFFUSION IN SOLIDS E C Romão a, M D d Campos c, J A Martns b, and L F M d Moura a Unvrsdad Estadual d Campnas Faculdad d Engnhara

More information

A Study on Nonlinear Forced Vibration of an Axial Moving Viscoelasticity Beam using the Multi-Scale Approach

A Study on Nonlinear Forced Vibration of an Axial Moving Viscoelasticity Beam using the Multi-Scale Approach BAO-FU KOU t al: A STUDY ON NONLINEAR FORCED VIBRATION OF AN AXIAL MOVING A Study on Nonlnar Forcd Vbraton of an Axal Movng Vscolastcty Bam usng th Mult-Scal Approach Bao-Fu Kou *, Xao-L Hu Collg of Mchancal

More information

3.4 Properties of the Stress Tensor

3.4 Properties of the Stress Tensor cto.4.4 Proprts of th trss sor.4. trss rasformato Lt th compots of th Cauchy strss tsor a coordat systm wth bas vctors b. h compots a scod coordat systm wth bas vctors j,, ar gv by th tsor trasformato

More information

Α complete processing methodology for 3D monitoring using GNSS receivers

Α complete processing methodology for 3D monitoring using GNSS receivers 7-5-5 NATIONA TECHNICA UNIVERSITY OF ATHENS SCHOO OF RURA AND SURVEYING ENGINEERING DEPARTMENT OF TOPOGRAPHY AORATORY OF GENERA GEODESY Α complt procssng mthodology for D montorng usng GNSS rcvrs Gorg

More information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS

More information

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline Introucton to Ornar Dffrntal Equatons Sptmbr 7, 7 Introucton to Ornar Dffrntal Equatons Larr artto Mchancal Engnrng AB Smnar n Engnrng Analss Sptmbr 7, 7 Outln Rvw numrcal solutons Bascs of ffrntal quatons

More information

Performance assessment of the window-wall interface. PhD-meeting Nathan Van Den Bossche - 04/06/2010 Department of Architecture Ghent University

Performance assessment of the window-wall interface. PhD-meeting Nathan Van Den Bossche - 04/06/2010 Department of Architecture Ghent University Prformanc assssmnt of th wndow-wall ntrfac Start: 04/2007 Stop: 01/2012 Nathan Van Dn Bossch Suprvsor: Arnold Janssns Hstory of Enrgy cods n Flandrs: 1992: Vntlaton and nsulaton dcr nsulaton lvl K65 1993:

More information

Journal of Chemical and Pharmaceutical Research, 2014, 6(7): Research Article

Journal of Chemical and Pharmaceutical Research, 2014, 6(7): Research Article Avalabl onln www.ocpr.com Journal of Chmcal and Pharmacutcal Rsarch, 214, 6(7):1394-14 Rsarch Artcl ISSN : 975-7384 COEN(USA) : JCPRC5 Rsarch on fatgu damag of suckr rod basd on damag mchancs Ru-fn Zhou,

More information

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC

More information

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP ISAHP 00, Bal, Indonsa, August -9, 00 COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP Chkako MIYAKE, Kkch OHSAWA, Masahro KITO, and Masaak SHINOHARA Dpartmnt of Mathmatcal Informaton Engnrng

More information

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك FEM FOR HE RNSFER PROBLEMS 1 Fild problms Gnral orm o systm quations o D linar stady stat ild problms: For 1D problms: D D g Q y y (Hlmholtz quation) d D g Q d Fild problms Hat transr in D in h h ( D D

More information

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D Comp 35 Introducton to Machn Larnng and Data Mnng Fall 204 rofssor: Ron Khardon Mxtur Modls Motvatd by soft k-mans w dvlopd a gnratv modl for clustrng. Assum thr ar k clustrs Clustrs ar not rqurd to hav

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 6

ECE Spring Prof. David R. Jackson ECE Dept. Notes 6 ECE 6345 Spring 2015 Prof. David R. Jackon ECE Dpt. Not 6 1 Ovrviw In thi t of not w look at two diffrnt modl for calculating th radiation pattrn of a microtrip antnna: Elctric currnt modl Magntic currnt

More information

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m hy3: Gnral hyscs III 4/0/008 haptr Worksht lctrc Flds: onsdr a fxd pont charg of 0 µ (q ) q = 0 µ d = 0 a What s th agntud and drcton of th lctrc fld at a pont, a dstanc of 0? q = = 8x0 ˆ o d ˆ 6 N ( )

More information

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,

More information

Improvements on Waring s Problem

Improvements on Waring s Problem Imrovement on Warng Problem L An-Png Bejng 85, PR Chna al@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th aer, we wll gve ome mrovement for Warng roblem Keyword: Warng Problem, Hardy-Lttlewood

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

Incorporating Subjective Characteristics in Product Design and Evaluations. Web Appendix

Incorporating Subjective Characteristics in Product Design and Evaluations. Web Appendix Incorporatng ubctv Charactrtc n Product Dgn and Evaluaton Lan Luo, P.K. Kannan, and Bran T. Ratchford Wb Appndx A. TEP I MARKOV CHAI MOTE CARLO IMULATIO Our MCMC procdur carrd out by quntally gnratng draw

More information

EXTENDED MULTISCALE FINITE ELEMENT METHOD FOR GEOMETRICALLY NONLINEAR ANALYSIS OF THIN COMPOSITE PLATES ON BENDING PROBLEMS

EXTENDED MULTISCALE FINITE ELEMENT METHOD FOR GEOMETRICALLY NONLINEAR ANALYSIS OF THIN COMPOSITE PLATES ON BENDING PROBLEMS 21 st Intrnatonal Confrnc on Compost Matrals X an, 20-25 th August 2017 XTNDD MULTISCAL FINIT LMNT MTHOD FOR GOMTRICALLY NONLINAR ANALYSIS OF THIN COMPOSIT PLATS ON BNDING PROBLMS Mngfa Rn 1, J Cong 1

More information

Folding of Regular CW-Complexes

Folding of Regular CW-Complexes Ald Mathmatcal Scncs, Vol. 6,, no. 83, 437-446 Foldng of Rgular CW-Comlxs E. M. El-Kholy and S N. Daoud,3. Dartmnt of Mathmatcs, Faculty of Scnc Tanta Unvrsty,Tanta,Egyt. Dartmnt of Mathmatcs, Faculty

More information

LARGE DISPLACEMENT ANALYSIS OF SLENDER ARCHES

LARGE DISPLACEMENT ANALYSIS OF SLENDER ARCHES Arch Brdg ARCH P. Roca and E. Oñat Ed CIMNE, Barclona, LARGE DISPLACEMEN ANALSIS OF SLENDER ARCHES M. Arc * and M. F. Granata * * Unvrtà dgl Std d Palrmo Dpartmnto d Inggnra Strttral Gotcnca Val dll Scnz

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

Journal of Chemical and Pharmaceutical Research, 2014, 6(5): Research Article

Journal of Chemical and Pharmaceutical Research, 2014, 6(5): Research Article Avalabl onln www.jocpr.com Journal of Chmcal and Pharmacutcal sarch, 4, 6(5):66-73 sarch Artcl SSN : 975-7384 CDN(SA) : JCPC5 Gap lmnt mthod and ts applcaton on forc analyss of tubng strngs Lu ka #, Song

More information

Equivalent Signal Theory for Frequency Domain Modeling of Linear Time-Periodic Systems: PWM Application

Equivalent Signal Theory for Frequency Domain Modeling of Linear Time-Periodic Systems: PWM Application Equvalnt Sgnal Thory for Frquncy Doman Modlng of Lnar Tm-Prodc Sytm: PWM Applcaton Mohamd Abdl-Rahman, Abnr Ramrz Abtract Equvalnt Sgnal Thory prov that a ampld gnal can b rprntd by a ynthtc contnuou functon

More information

WEEK 3 Effective Stress and Pore Water Pressure Changes

WEEK 3 Effective Stress and Pore Water Pressure Changes WEEK 3 Effctiv Str and Por Watr Prur Chang 5. Effctiv tr ath undr undraind condition 5-1. Dfinition of ffctiv tr: A rvi A you mut hav larnt that th ffctiv tr, σ, in oil i dfind a σ σ u Whr σ i th total

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

Advances in the study of intrinsic rotation with flux tube gyrokinetics

Advances in the study of intrinsic rotation with flux tube gyrokinetics Adans n th study o ntrns rotaton wth lux tub gyroknts F.I. Parra and M. arns Unrsty o Oxord Wolgang Paul Insttut, Vnna, Aprl 0 Introduton In th absn o obous momntum nput (apart rom th dg), tokamak plasmas

More information

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS ACOUSTIC WAE EQUATION Contnts INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS INTRODUCTION As w try to vsualz th arth ssmcally w mak crtan physcal smplfcatons that mak t asr to mak and xplan our obsrvatons.

More information

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University xtrnal quvalnt 5 Analyss of Powr Systms Chn-Chng Lu, ong Dstngushd Profssor Washngton Stat Unvrsty XTRNAL UALNT ach powr systm (ara) s part of an ntrconnctd systm. Montorng dvcs ar nstalld and data ar

More information

CHAPTER 4. The First Law of Thermodynamics for Control Volumes

CHAPTER 4. The First Law of Thermodynamics for Control Volumes CHAPTER 4 T Frst Law of Trodynacs for Control olus CONSERATION OF MASS Consrvaton of ass: Mass, lk nrgy, s a consrvd proprty, and t cannot b cratd or dstroyd durng a procss. Closd systs: T ass of t syst

More information

CHAPTER 33: PARTICLE PHYSICS

CHAPTER 33: PARTICLE PHYSICS Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

FINITE ELEMENT METHOD II Autumn 2015

FINITE ELEMENT METHOD II Autumn 2015 FEM II - Lctur Pag of 4 FINITE ELEMENT METHOD II Autumn 05 Lcturs (5h):. Accuracy, rror stmaton and adaptv rmshng. Hat flow and thrmal strsss n FEM 3. Introducton to structural dynamcs, fr vbratons 4.

More information

Optimal Ordering Policy in a Two-Level Supply Chain with Budget Constraint

Optimal Ordering Policy in a Two-Level Supply Chain with Budget Constraint Optmal Ordrng Polcy n a Two-Lvl Supply Chan wth Budgt Constrant Rasoul aj Alrza aj Babak aj ABSTRACT Ths papr consdrs a two- lvl supply chan whch consst of a vndor and svral rtalrs. Unsatsfd dmands n rtalrs

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

Finite Element Models for Steady Flows of Viscous Incompressible Fluids

Finite Element Models for Steady Flows of Viscous Incompressible Fluids Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod

More information

Optimal Topology Design for Replaceable of Reticulated Shell Based on Sensitivity Analysis

Optimal Topology Design for Replaceable of Reticulated Shell Based on Sensitivity Analysis Optmal Topology Dsgn for Rplacabl of Rtculatd Shll Basd on Snstvty Analyss Yang Yang Dpartmnt of Naval Archtctur, Dalan Unvrsty of Tchnology, Laonng, CN Ma Hu Collg of Rsourc and Cvl Engnrng, Northastrn

More information

Variational Approach in FEM Part II

Variational Approach in FEM Part II COIUUM & FIIE ELEME MEHOD aratonal Approach n FEM Part II Prof. Song Jn Par Mchancal Engnrng, POSECH Fnt Elmnt Mthod vs. Ralgh-Rtz Mthod On wants to obtan an appromat solton to mnmz a fnctonal. On of th

More information

Integration of Predictive Display and Aircraft Flight Control System

Integration of Predictive Display and Aircraft Flight Control System ATE Wb of onfrnc 99, 03005 (07 DOI: 005/ matcconf/079903005 TAI06 Intgraton of Prdctv Dplay and Arcraft Flght ontrol Sytm AV Efrmov, *, S Tjaglk, IH Irgalv and VG Tpnko ocow Avaton Inttut, Aronautcal chool,

More information

PREDICTION OF STRESS CONCENTRATION FACTORS IN UNLAPPED SQUARE HOLLOW "K" JOINTS BY THE FINITE ELEMENT METHOD

PREDICTION OF STRESS CONCENTRATION FACTORS IN UNLAPPED SQUARE HOLLOW K JOINTS BY THE FINITE ELEMENT METHOD Ngran Journal of chnology, Vol. 5, No., March 006 Jk 5 PREDICION OF SRESS CONCENRAION FACORS IN UNLAPPED SQUARE HOLLOW "K" JOINS BY HE FINIE ELEMEN MEHOD DR.P.N.JIKI Dpartmnt of Cvl Engnrng, Unvrsty of

More information

10/24/2013. PHY 113 C General Physics I 11 AM 12:15 PM TR Olin 101. Plan for Lecture 17: Review of Chapters 9-13, 15-16

10/24/2013. PHY 113 C General Physics I 11 AM 12:15 PM TR Olin 101. Plan for Lecture 17: Review of Chapters 9-13, 15-16 0/4/03 PHY 3 C General Physcs I AM :5 PM T Oln 0 Plan or Lecture 7: evew o Chapters 9-3, 5-6. Comment on exam and advce or preparaton. evew 3. Example problems 0/4/03 PHY 3 C Fall 03 -- Lecture 7 0/4/03

More information

Improvements on Waring s Problem

Improvements on Waring s Problem Improvement on Warng Problem L An-Png Bejng, PR Chna apl@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th paper, we wll gve ome mprovement for Warng problem Keyword: Warng Problem,

More information

Direct Approach for Discrete Systems One-Dimensional Elements

Direct Approach for Discrete Systems One-Dimensional Elements CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:

More information

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI 2017 2nd Internatonal Conference on Electrcal and Electroncs: echnques and Applcatons (EEA 2017) ISBN: 978-1-60595-416-5 Study on Actve Mcro-vbraton Isolaton System wth Lnear Motor Actuator Gong-yu PAN,

More information

DETERMINATION OF INTERMEDIATE ORBIT AND POSITION OF GLONASS SATELLITES BASED ON THE GENERALIZED PROBLEM OF TWO FIXED CENTERS

DETERMINATION OF INTERMEDIATE ORBIT AND POSITION OF GLONASS SATELLITES BASED ON THE GENERALIZED PROBLEM OF TWO FIXED CENTERS Acta Goyn. Gomatr. Vol. 9 No. (7) 9 DTRMINATION OF INTRMDIAT ORBIT AND POSITION OF GLONASS SATLLITS BASD ON TH GNRALIZD PROBLM OF TWO FIXD CNTRS Włayław GÓRAL ) * an Bogan SKORUPA ) ) Bronław Marwcz Stat

More information

Finite Element Based Implementation of Fiala s Thermal Manikin in THESEUS-FE

Finite Element Based Implementation of Fiala s Thermal Manikin in THESEUS-FE Fnt Elmnt Basd Implmntaton of Fala s hrmal Mankn n HESEUS-FE Author: Dr. Stfan Paulk (chncal Managr) VMS, 3.05.007 Global Modllng Mankn Implmntaton Global Human Hat Fluxs Human mpratur Valdaton Global

More information

Lecture 3: Phasor notation, Transfer Functions. Context

Lecture 3: Phasor notation, Transfer Functions. Context EECS 5 Fall 4, ctur 3 ctur 3: Phasor notaton, Transfr Functons EECS 5 Fall 3, ctur 3 Contxt In th last lctur, w dscussd: how to convrt a lnar crcut nto a st of dffrntal quatons, How to convrt th st of

More information

ANALYSIS: The mass rate balance for the one-inlet, one-exit control volume at steady state is

ANALYSIS: The mass rate balance for the one-inlet, one-exit control volume at steady state is Problm 4.47 Fgur P4.47 provds stady stat opratng data for a pump drawng watr from a rsrvor and dlvrng t at a prssur of 3 bar to a storag tank prchd 5 m abov th rsrvor. Th powr nput to th pump s 0.5 kw.

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

Operating conditions of a mine fan under conditions of variable resistance

Operating conditions of a mine fan under conditions of variable resistance Paper No. 11 ISMS 216 Operatng condtons of a mne fan under condtons of varable resstance Zhang Ynghua a, Chen L a, b, Huang Zhan a, *, Gao Yukun a a State Key Laboratory of Hgh-Effcent Mnng and Safety

More information

Fakultät III Wirtschaftswissenschaften Univ.-Prof. Dr. Jan Franke-Viebach

Fakultät III Wirtschaftswissenschaften Univ.-Prof. Dr. Jan Franke-Viebach Unvrstät Sgn Fakultät III Wrtschaftswssnschaftn Unv.-rof. Dr. Jan Frank-Vbach Exam Intrnatonal Fnancal Markts Summr Smstr 206 (2 nd Exam rod) Avalabl tm: 45 mnuts Soluton For your attnton:. las do not

More information