ELASTOPLASTIC ANALYSIS OF PLATE WITH BOUNDARY ELEMENT METHOD
|
|
- Delphia Harrington
- 5 years ago
- Views:
Transcription
1 Intrntionl Journl of chnicl nginring nd Tchnology (IJT) olum 9, Issu 6, Jun 18, , Articl ID: IJT_9_6_97 Avilbl onlin t htt://.im.com/ijmt/issus.s?jty=ijt&ty=9&ity=6 IN Print: nd IN Onlin: IA Publiction cous Indxd LATOPLATIC ANALYI OF PLAT WITH BOUNDARY LNT THOD Drtmnt of chnicl nginring, Fkults Tknik, Univrsits uhmmdiyh urkrt. ABTRACT This ork is th dvlomnt of boundry lmnt mthod for lstolstic lt nlysis to includ lstic-linr hrdning mtril. Th lt is subjctd to bnding, in-ln nd combind bnding nd in-ln. Th lstic zon is vlutd by using von iss critrion. Th cll discrtiztion is imlmntd to solv numriclly th domin intgrl cusd by lsticity. To vlut th nonlinr trm in th formultion of th boundry lmnt, totl incrmntl tchniqu is imlmntd. Th cbility of th dvlomnt in this ork ill b rsntd by hving numricl xmls. Kyords: Boundry lmnt mthods, lsticity, shr dformbl lt, totl incrmnt mthod. Cit this Articl:, lstolstic Anlysis of Plt ith Boundry lmnt thod, Intrntionl Journl of chnicl nginring nd Tchnology, 9(6), 18, htt://.im.com/ijt/issus.s?jty=ijt&ty=9&ity=6 1. INTRODUCTION Th y to nlyz lt ill dnd on th lods orking on it. Th lods cn b idntifid s bnding, in-ln or combind bnding nd in-ln. Whn th lod is in-ln, th lt is trtd s D roblm nd it cn b nlyzd by th ln strss thory[1]. In th cs of bnding, th lt is solvd using lt bnding thory. Thr r to kinds of lt bnding thory i.. th clssicl[] nd shr dformbl thory[]. For th combind on, th surosition of lt bnding thory nd D ln strss thory r considrd. As fr s Author knos, th lstolstic nlysis of lt by B cn b sn in [4], [5], [6], [7], [8], [9], [1] nd [11]. All th orks only considrd n lstic-rfctly lstic mtril. In this r, th ork by uriyono[9] is xtndd to includ lstic-linr hrdning mtril. Th rltionshi btn strsss nd strins is shon in Fig. 1 hn th mtril ith linr hrdning bhvior is lodd unixilly. Th totl strin is considrd s sum of th lstic nd lstic comonnts s follos: ε + = ε ε 1 htt://.im.com/ijt/indx.s 864 ditor@im.com
2 lstolstic Anlysis of Plt ith Boundry lmnt thod σ hr ε = is th lstic rt of th totl strin nd ε rrsnts th lstic rt. Figur 1 Linr hrdning mtril bhvior For initil loding, lstic bhvior is obtind for σ Y < Onc th strss hs xcdd th initil yild strss Y, on cn hv σ σ < hr σ is subsqunt yild strss nd its vlu dnds on th lstic flo rul. Th strss-strin rltionshi for monotonic loding in tnsion hs th form hich my b rittn s σ = Y + ε, if σ > Y 4 σ = Y + Tε 5 By considring qution (1), It llos qution (5) to b xrssd s σ = Y + ( ε + ε ) 6 ubstituting qution (4) into qution (6) yilds T σ Y σ = Y + Tε + T 7 vntully, th folloing qution is obtind: σ T = Y + ε = Y + H ' ε 8 T 1 hr H is th lstic modulus dfind s th slo of th hrdning curv, no xrssd in trms of strss vrsus lstic strin. For th cs of linr hrdning, H is constnt, but in gnrl, it chngs continuously long th hrdning curv, i.. htt://.im.com/ijt/indx.s 865 ditor@im.com
3 dσ H ' = 9 dε In this r, shr dformbl lt thory is considrd instd of clssicl lt thory. Th totl incrmntl tchniqu is usd to vlut th nonlinr systm of qution. Th cll discrtiztion mthod using 9-nods qudriltrl cll is lid to nlyz th domin intgrls hich mrg in th formultion. In this r, th nottion of Crtsin tnsor is mloyd, ith Grk indics chnging from 1 to nd th Ltin indics chnging from 1 to.. B FORULATION.1. Govrning qution Gnrl formul for lstolstic lt nlysis is dtrmind by considring lstic strins tht r du to bnding nd mmbrn lodings, thrfor th totl strin rts cn b xrssd s χ ε = χ + χ ; 1 = ε + ε ; 11 And γ γ = 1 Whr, χ r th rts of th totl bnding strins, ε r th rts of th totl in-ln strins, nd γ th rts of th shr strin rts. Th rts of th totl bnding nd in-ln strins comris linr nd nonlinr comonnts. Th nonlinr comonnts of qutions (1) nd (11) r du to lsticity () nd thy cn b rittn s nd χ = χ 1 ε = ε 14 On th othr hnd, th rts of th rsultnts of th strss cn lso b rittn s = ; 15 for momnt rsultnts = Q ; 16 Q for shr rsultnts nd N = N N 17 for mmbrn strss rsultnts. Th rltionshis btn th strsss nd dislcmnts cn b sttd s htt://.im.com/ijt/indx.s 866 ditor@im.com
4 lstolstic Anlysis of Plt ith Boundry lmnt thod υ = D (, β+ β, γ, γ δ) ; 18 nd = (, Q C + ); 19 N υ = B( u, β + u β, uγ, γ δ ) N ; hr, D = h, B = h nd xrssd s: C = kh. Th quilibrium qution cn b (1 + υ) Q = ; 1 nd Q, q = ; N, β =.. Dislcmnt nd trss Intgrl qution As rsntd in [9] th dislcmnt intgrl qution for lstolstic nlysis cn b xrssd in qution (4) for rottion nd dflction nd qution (5) for in-ln dislcmnt. Th qutions r th xrssion of dislcmnt rts of ny oints X in th domin to th vlus of th rts of dislcmnt nd th rts of th trction on th boundry. nd = ij j &( X') W ( X', & ( d P ( X', ( d + W X ', X ) q ( X ) d + i i ( X ', X ) ( X ) ij j i ( & χ & d 4 = u ( X') U ( X', t ( d T ( X', u j ( d+ θ ( ', X ) N ε X ( X ) d 5 Whr, W ij (X,, P ij (X,, χ ij (X,X), U ij (X,, T ij (X,, nd ε ij (X,X) r nmd fundmntl solutions. Thy cn b found nd xlind in [7]. qution (4) nd (5) r th solution for ny oint in th domin, to hv solutions on th boundry oints, th limiting rocss s X x Є is conductd to hv: = ij j C & ( x') W ( x', & ( d P ( x', ( d+ W x', X ) q ( X ) d + nd ij i i ( x ', X ) ( X ) ij j i ( & χ & d 6 = C u ( x') U ( x', t ( d T ( x', u j( d+ θ ( ', X ) N ε x ( X ) d 7 htt://.im.com/ijt/indx.s 867 ditor@im.com
5 hr, C ij (x ) r clld fr trm. In th cs of smooth boundry, th vlu of th fr trm is.5. qution (4), (5), (6), nd (7) r dislcmnt intgrl qutions. On th othr hnd, th intgrl strss qutions r & ( X ') = W ( X ', & ( d P ( X ', & ( d + + k k k k k l χ ( X ', X ) & γθ γθ ( X ) d 1 l [ (1 + υ ) (1 υ ) & θθ δ ] for momnt rsultnts, Q X ') = W ( X ', ( d P ( X ', ( d + β ( k k k + l βγθ ( X ', X ) γθ ( X ) 8 W ( X ', X ) q& ( X ) d 8 k W ( X ) d βk ( X ', ) q χ & d 9 for shr rsultnts, nd N ( X') = U ( X', t ( d T ( X', u ( d + γ γ γ γ 1 8 [ (1 + υ ) N (1 υ )N δ ] θθ ε γθ ( ', X ) N γθ X ( X ) d for mmbrn rsultnts... Discrtiztion nd ystm of qution Numricl mthod is usd to solv qutions of (6), (7), (8), (9) nd (). Discrtiztion is conductd on th boundry nd rt of th domin hich is xctd to yild. Qudrtic is ormtric lmnts r lid to discrtiz th boundry nd 9 nods qudriltrl clls r imlmntd in th domin. Aftr discrtiztion, th mtrix form of th qutions (6) nd (7) cn b obtind s H G = u H u + b T + u G t u T N 1 hr [H] nd [G] r clld th influnc mtrics of boundry lmnt, [T] is th influnc mtrix of lsticity. Th surscrit nd u indict th mod of lt nd D rsctivly. { }, { u }, { } nd { t } r th rt vctors of th dislcmnt nd th trction on th boundry. { b } is th rt vctors of th lod on th domin nd { } nd { N } r th lsticity trms. Onc boundry conditions r imosd, qutions (1) cn b rsntd s T & = + u T N [ A]{ x} { f } hr, [A] is th cofficint mtrix, { x } is th column mtrix of th unknon nd {f } is th column mtrix of rscribd boundry vlus. In th sm y, th strss intgrl qutions of qution (8), (9) nd () cn b xrssd in mtrix form s htt://.im.com/ijt/indx.s 868 ditor@im.com
6 lstolstic Anlysis of Plt ith Boundry lmnt thod htt://.im.com/ijt/indx.s = u u u N T T T b b u H H H t G G G N Q Th totl incrmntl tchniqu is usd to solv th nonlinr systm of qutions of () nd (). Th dtil lgorithm of th tchniqu cn b sn in [9] s this ork is xtndd from tht ork. Hovr hn vluting th lstic zon, lstic-rfctly lstic or lsticlinr hrdning mtril r considrd.. NURICAL XAPL To sho th cbility of this ork to tk into ccount lstic-linr hrdning mtril, xmls r rsntd. Th first xml is squr lt of simly suortd lt (s Fig. ). Ths xmls hv bn rortd in [5], [9] nd [11] for lstic-rfctly lstic mtril. Figur imly suortd squr lt In this r th sm lt is rsntd ith linr hrdning mtrils of H =.7 nd H =.15. Th rortis of th lt r = 1.9 GP, ν =., σ Y = 16 P nd h/ =.1. Th nondimnsionl rmtrs r introducd s follos. Q q = nd 1 D W = hr = σ y h /4, is th cntr lt dflction nd D=h /1(1-ν ). Th rsult of th hrdning mtrils for squr lt cn b sn in Fig.. As it cn b sn tht th biggr vlu of H mk th mtril hrdns during th lstic flo, it mns t th sm lod ftr lstic, mtril ith biggr vlu of H hs lss dflction. Figur Dflction t cntr lt for vrious H. h q q imly uortd
7 Th scond xml is rctngulr lt ith cntr hol subjctd to unixil tnsion of σ. Th gomtry nd loding condition is shon in Fig. 4(). This is tyicl ln strss roblm nd hs lso bn studid using th B by Alibdi [1]. Th mtril is ssumd to hrdn linrly nd hs rortis of = 7GP, ν =., σ Y = 4 P nd H =.. Du to th symmtry conditions nd to sss th snsitivity solution to th discrtiztion, only qurtr of th lt is discrtizd s follos: odl A, 6 lmnts on th boundry ith 1 domin clls (s Fig. 4(b)) odl B, 6 lmnts on th boundry ith domin clls (s Fig. 4(c)) odl C, 8 lmnts on th boundry ith 41 domin clls (s Fig. 4(d)) Fig. 5 shos th comrison of th dislcmnt in x-dirction of oint A btn th currnt nlysis of th thr modls nd th on obtind in [1]. Th currnt nlysis of th thr modls r crrid out in 6 lod sts to chiv th finl lod hich is found to giv convrgd solution. In this figur th nondimnsionl rmtrs of U x nd Q r dfind s U x = u x /r 1 nd Q=σ/σ yild. It cn b sn tht odl B nd C giv convrgd rsults. trss comonnt σ xx t th nt sction of th lt is lottd in Fig. 6. Th rmtr of Dist is dfind s Dist = y/r. Th rsults r comrd ith th on obtind in [1]. Onc gin, convrgd solutions r givn by odl B nd C. At lst, th dvlomnt of th lstic zon is rsntd in Fig. 7. Figur 4 Gomtry nd discrtiztion of th rctngulr lt. Figur 5 Dislcmnt t osition of oint A htt://.im.com/ijt/indx.s 87 ditor@im.com
8 lstolstic Anlysis of Plt ith Boundry lmnt thod Figur 6 trss vrition on th nt sction of th lt. Figur 7 Dvlomnt of th lstic zon for vrious lod lvl. Thirdly, th sm lt s th scond on is lodd by combind tnsion nd bnding, hr th tnsion is σ = 5 P nd th bnding is q =.184 P. Th rsult of von iss strss is rsntd in Fig.8 in comrison ith F rsult. Figur 8 on iss trss contour t finl lod 4. CONCLUION From th xmls nd rsults rsntd in this ork, it cn b concludd tht th dvlomnt in this ork hs cbility to simult both lstic-rfctly lstic nd lsticlinr hrdning mtril. ACKNOWLDGNT Th uthors ould lik to thnk to th Dirctort Gnrl of Rsrch, Tchnology nd Highr duction, inistry of Rsrch, Tchnology nd Highr duction, Rublic of Indonsi for th finncil suort. This rsrch is finncilly suortd by Pnlitin Ungguln Prgurun Tinggi ith th contrct of 11.71/A.-III/LPP//17. htt://.im.com/ijt/indx.s 871 ditor@im.com
9 RFRNC [1]. Timoshnko nd J. N. Goodir, Thory of lsticity, Third. ingor: cgr-hill Intrntionl ditions, 197. [] G. Kirchhoff, Ubr ds glichgicht und di bgung inr lstischn schib, J. Rin Ang th, no. 4, , 185. []. Rissnr, On vritionl thorm in lsticity, J. th. Phys., no. 9,. 9 95, 195. [4]. J. Krm nd J. C. F. Tlls, On boundry lmnts for Rissnr s lt thory, ng. Anl., vol. 5, no. 1,. 1 7, [5]. J. Krm nd J. C. F. Tils, Th B lid to lt bnding lstolstic nlysis using Rissnr s thory, ng. Anl., vol. 9, , 199. [6]. J. Krm nd J. C. F. Tlls, Nonlinr mtril nlysis of Rissnr s lts, in Plt Bnding Anlysis ith Boundry lmnt, 1998, [7] uriyono nd. H. Alibdi, Boundry lmnt thod for hr Dformbl Plt ith Combind Gomtric nd tril Nonlinritis, ng. Anl. Bound. lm., vol.,. 1 4, 6. [8] uriyono nd. H. Alibdi, Anlysis of shr dformbl lts ith combind gomtric nd mtril nonlinritis by boundry lmnt mthod, Int. J. olids truct., vol. 44, , 7. [9] uriyono, Boundry lmnt thod for hr Dformbl Plt ith tril Nonlinrity, ARPN J. ng. Al. ci., vol. 11, no. 8, , 16. [1]. R. C. Olivir nd. J. Krm, lstolstic nlysis of Rissnr s lts by th boundry lmnt mthod, ng. Anl. Bound. lm., vol. 64, , 16. [11] uriyono,. ffndy, nd Wijinto, tril nonlinrity lt bnding nlysis ith boundry lmnt mthod, in AIP Confrnc Procdings, 17, vol [1]. H. Alibdi, Th Boundry lmnt thod, liction to solids nd structurs. Chichstr: Wily, 1. htt://.im.com/ijt/indx.s 87 ditor@im.com
CIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7
CIVL / -D Boundr Vlu Prolms - Rctngulr Elmnts / RECANGULAR ELEMENS - In som pplictions, it m mor dsirl to us n lmntl rprsnttion of th domin tht hs four sids, ithr rctngulr or qudriltrl in shp. Considr
More informationThe Angular Momenta Dipole Moments and Gyromagnetic Ratios of the Electron and the Proton
Journl of Modrn hysics, 014, 5, 154-157 ublishd Onlin August 014 in SciRs. htt://www.scir.org/journl/jm htt://dx.doi.org/.436/jm.014.51415 Th Angulr Momnt Diol Momnts nd Gyromgntic Rtios of th Elctron
More informationMiscellaneous open problems in the Regular Boundary Collocation approach
Miscllnous opn problms in th Rgulr Boundry Colloction pproch A. P. Zilińsi Crcow Univrsity of chnology Institut of Mchin Dsign pz@mch.p.du.pl rfftz / MFS Confrnc ohsiung iwn 5-8 Mrch 0 Bsic formultions
More informationInstructions for Section 1
Instructions for Sction 1 Choos th rspons tht is corrct for th qustion. A corrct nswr scors 1, n incorrct nswr scors 0. Mrks will not b dductd for incorrct nswrs. You should ttmpt vry qustion. No mrks
More informationElliptical motion, gravity, etc
FW Physics 130 G:\130 lctur\ch 13 Elliticl motion.docx g 1 of 7 11/3/010; 6:40 PM; Lst rintd 11/3/010 6:40:00 PM Fig. 1 Elliticl motion, grvity, tc minor xis mjor xis F 1 =A F =B C - D, mjor nd minor xs
More informationStress and Strain Analysis of Notched Bodies Subject to Non-Proportional Loadings
World Acdmy of Scinc Enginring nd Tchnology Intrntionl Journl of Mchnicl nd Mchtronics Enginring Strss nd Strin Anlysis of Notchd Bodis Subjct to Non-Proportionl Lodings A. Inc Intrntionl Scinc Indx Mchnicl
More informationINTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)
Chptr 7 INTEGRALS 7. Ovrviw 7.. Lt d d F () f (). Thn, w writ f ( ) d F () + C. Ths intgrls r clld indfinit intgrls or gnrl intgrls, C is clld constnt of intgrtion. All ths intgrls diffr y constnt. 7..
More informationCh 1.2: Solutions of Some Differential Equations
Ch 1.2: Solutions of Som Diffrntil Equtions Rcll th fr fll nd owl/mic diffrntil qutions: v 9.8.2v, p.5 p 45 Ths qutions hv th gnrl form y' = y - b W cn us mthods of clculus to solv diffrntil qutions of
More informationTheoretical Study on the While Drilling Electromagnetic Signal Transmission of Horizontal Well
7 nd ntrntionl Confrnc on Softwr, Multimdi nd Communiction Enginring (SMCE 7) SBN: 978--6595-458-5 Thorticl Study on th Whil Drilling Elctromgntic Signl Trnsmission of Horizontl Wll Y-huo FAN,,*, Zi-ping
More information, between the vertical lines x a and x b. Given a demand curve, having price as a function of quantity, p f (x) at height k is the curve f ( x,
Clculus for Businss nd Socil Scincs - Prof D Yun Finl Em Rviw vrsion 5/9/7 Chck wbsit for ny postd typos nd updts Pls rport ny typos This rviw sht contins summris of nw topics only (This rviw sht dos hv
More informationChapter 16. 1) is a particular point on the graph of the function. 1. y, where x y 1
Prctic qustions W now tht th prmtr p is dirctl rltd to th mplitud; thrfor, w cn find tht p. cos d [ sin ] sin sin Not: Evn though ou might not now how to find th prmtr in prt, it is lws dvisl to procd
More informationLecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9
Lctur contnts Bloch thorm -vctor Brillouin zon Almost fr-lctron modl Bnds ffctiv mss Hols Trnsltionl symmtry: Bloch thorm On-lctron Schrödingr qution ch stt cn ccommo up to lctrons: If Vr is priodic function:
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium
.65, MHD Thory of usion Systms Prof. ridrg Lctur 8: Effct of Vrticl ild on Tokmk Equilirium Toroidl orc lnc y Mns of Vrticl ild. Lt us riw why th rticl fild is imortnt. 3. or ry short tims, th cuum chmr
More informationVSMN30 FINITA ELEMENTMETODEN - DUGGA
VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional
More informationLecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:
Lctur 11 Wvs in Priodic Potntils Tody: 1. Invrs lttic dfinition in 1D.. rphicl rprsnttion of priodic nd -priodic functions using th -xis nd invrs lttic vctors. 3. Sris solutions to th priodic potntil Hmiltonin
More informationMulti-Section Coupled Line Couplers
/0/009 MultiSction Coupld Lin Couplrs /8 Multi-Sction Coupld Lin Couplrs W cn dd multipl coupld lins in sris to incrs couplr ndwidth. Figur 7.5 (p. 6) An N-sction coupld lin l W typiclly dsign th couplr
More informationTOPIC 5: INTEGRATION
TOPIC 5: INTEGRATION. Th indfinit intgrl In mny rspcts, th oprtion of intgrtion tht w r studying hr is th invrs oprtion of drivtion. Dfinition.. Th function F is n ntidrivtiv (or primitiv) of th function
More informationPARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION
ICSV4 Cns Australia 9- July, 007 PARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION Jin Woo L and Yoon Young Kim National Crativ
More informationAS 5850 Finite Element Analysis
AS 5850 Finit Elmnt Analysis Two-Dimnsional Linar Elasticity Instructor Prof. IIT Madras Equations of Plan Elasticity - 1 displacmnt fild strain- displacmnt rlations (infinitsimal strain) in matrix form
More informationCHAPTER 12. Finite-Volume (control-volume) Method-Introduction
CHAPR 12 Finit-Volum (control-volum) Mthod-Introduction 12-1 Introduction (1) In dvloing ht hs bcom knon s th finit-volum mthod, th consrvtion rincils r lid to fixd rgion in sc knon s control volum, r
More informationtemperature T speed v time t density ρ scalars may be constant or may be variable yes distributive a(b+c) = ab+ac
Mthmtics Riw. Sclr mthmticl ntity tht hs mgnitud only.g.: tmprtur T spd tim t dnsity ρ sclrs my constnt or my ril Lws of Algr for Sclrs: ys commutti ys ssociti (c) ()c ys distriuti (c) c Fith A. Morrison,
More informationBOUNDARY ELEMENT METHOD FOR SHEAR DEFORMABLE PLATE WITH MATERIAL NONLINEARIRTY
OL., O. 8, APRIL 6 I 89-668 ARP Jornl of Engnrng Ald cncs 6-6 Asn Rsrch Pblshng tor ARP). All rghts rsrvd..rnornls.com BOUDARY ELEET ETHOD FOR HEAR DEFORABLE PLATE WITH ATERIAL OLIEARIRTY ryono Drtmnt
More informationIntegration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals
Intgrtion Continud Intgrtion y Prts Solving Dinit Intgrls: Ar Undr Curv Impropr Intgrls Intgrtion y Prts Prticulrly usul whn you r trying to tk th intgrl o som unction tht is th product o n lgric prssion
More informationChapter 11 Calculation of
Chtr 11 Clcultion of th Flow Fild OUTLINE 11-1 Nd for Scil Procdur 11-2 Som Rltd Difficultis 11-3 A Rmdy : Th stggrd Grid 11-4 Th Momntum Equtions 11-5 Th Prssur nd Vlocity Corrctions 11-6 Th Prssur-Corrction
More informationLimits Indeterminate Forms and L Hospital s Rule
Limits Indtrmint Forms nd L Hospitl s Rul I Indtrmint Form o th Tp W hv prviousl studid its with th indtrmint orm s shown in th ollowin mpls: Empl : Empl : tn [Not: W us th ivn it ] Empl : 8 h 8 [Not:
More informationCIE3109 : Structural Mechanics 4
CI3109 CI3109 : Structural echanics 4 13-14 Unsmmetrical and/or inhomogeneous cross sections Introduction General theor for extension and bending Unsmmetrical cross sections example : curvature versus
More informationAn Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method
Amrican Journal of Applid Scincs 4 (1): 95-956, 7 ISSN 1546-939 7 Scinc Publications An Invstigation on th Effct of th Coupld and Uncoupld Formulation on Transint Spag by th Finit Elmnt Mthod 1 Ahad Ouria,
More informationSection 3: Antiderivatives of Formulas
Chptr Th Intgrl Appli Clculus 96 Sction : Antirivtivs of Formuls Now w cn put th is of rs n ntirivtivs togthr to gt wy of vluting finit intgrls tht is ct n oftn sy. To vlut finit intgrl f(t) t, w cn fin
More informationFINITE ELEMENT ANALYSIS OF CONSOLIDATION PROBLEM IN SEVERAL TYPES OF COHESIVE SOILS USING THE BOUNDING SURFACE MODEL
ARPN Journl of Enginring nd Alid Sins 006-008 Asin Rsrh Publishing Ntwork (ARPN). All rights rsrvd. www.rnjournls.om FINITE ELEMENT ANALYSIS OF CONSOLIDATION PROBLEM IN SEVERAL TYPES OF COHESIVE SOILS
More informationLast time: introduced our first computational model the DFA.
Lctur 7 Homwork #7: 2.2.1, 2.2.2, 2.2.3 (hnd in c nd d), Misc: Givn: M, NFA Prov: (q,xy) * (p,y) iff (q,x) * (p,) (follow proof don in clss tody) Lst tim: introducd our first computtionl modl th DFA. Tody
More informationStrength of Materials
Strngth of Matrials Sssion Column 08 ctur not : ramudiyanto, M.Eng. Strngth of Matrials STBIITY OF STRUCTURE In th dsign of columns, oss-sctional ara is slctd such that - allowabl strss is not xcdd all
More informationNon-Linear Analysis of Interlaminar Stresses in Composite Beams with Piezoelectric Layers
7TH ITERATIOA OFEREE O OMPOSITE SIEE AD TEHOOGY on-inar Analysis of Intrlaminar Strsss in omosit Bams with Piolctric ayrs MASOUD TAHAI 1, AMIR TOOU DOYAMATI 1 Dartmnt of Mchanical Enginring, Faculty of
More informationJOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (JMET)
JOURNAL OF MECHANICAL ENGINEERING AND ECHNOLOGY (JME) Journl of Mchnicl Enginring nd chnology (JME) ISSN 47-94 (Print) ISSN 47-9 (Onlin) Volum Issu July -Dcmbr () ISSN 47-94 (Print) ISSN 47-9 (Onlin) Volum
More informationJournal of System Design and Dynamics
Journl of Systm Dsign nd Dynmics Vol. 1, No. 3, 7 A Numricl Clcultion Modl of Multi Wound Foil Bring with th Effct of Foil Locl Dformtion * Ki FENG** nd Shighiko KANEKO** ** Dprtmnt of Mchnics Enginring,
More informationFinite Strain Elastic-Viscoplastic Model
Finit Strain Elastic-Viscoplastic Modl Pinksh Malhotra Mchanics of Solids,Brown Univrsity Introduction Th main goal of th projct is to modl finit strain rat-dpndnt plasticity using a modl compatibl for
More informationI. The Connection between Spectroscopy and Quantum Mechanics
I. Th Connction twn Spctroscopy nd Quntum Mchnics On of th postults of quntum mchnics: Th stt of systm is fully dscrid y its wvfunction, Ψ( r1, r,..., t) whr r 1, r, tc. r th coordints of th constitunt
More informationPage 1. Question 19.1b Electric Charge II Question 19.2a Conductors I. ConcepTest Clicker Questions Chapter 19. Physics, 4 th Edition James S.
ConTst Clikr ustions Chtr 19 Physis, 4 th Eition Jms S. Wlkr ustion 19.1 Two hrg blls r rlling h othr s thy hng from th iling. Wht n you sy bout thir hrgs? Eltri Chrg I on is ositiv, th othr is ngtiv both
More informationAnalysis of Dynamics of Boundary Shape Perturbation of a Rotating Elastoplastic Radially Inhomogeneous Plane Circular Disk: Analytical Approach
Alid Mtmtics 3 45-456 tt://dxdoiorg/436/m3568 Pulisd Onlin My (tt://wwwscirporg/journl/m) Anlysis of Dynmics of Boundry S Prturtion of Rotting Elstolstic Rdilly Inomognous Pln Circulr Disk: Anlyticl Aroc
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
More informationMathematics. Mathematics 3. hsn.uk.net. Higher HSN23000
Highr Mthmtics UNIT Mthmtics HSN000 This documnt ws producd spcilly for th HSN.uk.nt wbsit, nd w rquir tht ny copis or drivtiv works ttribut th work to Highr Still Nots. For mor dtils bout th copyright
More informationEinstein Equations for Tetrad Fields
Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for
More informationMASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS SEMESTER TWO 2014 WEEK 11 WRITTEN EXAMINATION 1 SOLUTIONS
MASTER CLASS PROGRAM UNIT SPECIALIST MATHEMATICS SEMESTER TWO WEEK WRITTEN EXAMINATION SOLUTIONS FOR ERRORS AND UPDATES, PLEASE VISIT WWW.TSFX.COM.AU/MC-UPDATES QUESTION () Lt p ( z) z z z If z i z ( is
More informationME311 Machine Design
ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform
More informationu 3 = u 3 (x 1, x 2, x 3 )
Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.
More informationCSE 373: AVL trees. Warmup: Warmup. Interlude: Exploring the balance invariant. AVL Trees: Invariants. AVL tree invariants review
rmup CSE 7: AVL trs rmup: ht is n invrint? Mihl L Friy, Jn 9, 0 ht r th AVL tr invrints, xtly? Disuss with your nighor. AVL Trs: Invrints Intrlu: Exploring th ln invrint Cor i: xtr invrint to BSTs tht
More informationMECHANICS OF MATERIALS
00 Th McGraw-Hill Companis, Inc. ll rights rsrvd. T Edition CHTER MECHNICS OF MTERIS Frdinand. Br E. Russll Johnston, Jr. John T. DWolf Columns ctur Nots: J. Walt Olr Txas Tch Univrsit 00 Th McGraw-Hill
More informationThe Theory of Small Reflections
Jim Stils Th Univ. of Knss Dt. of EECS 4//9 Th Thory of Smll Rflctions /9 Th Thory of Smll Rflctions Rcll tht w nlyzd qurtr-wv trnsformr usg th multil rflction viw ot. V ( z) = + β ( z + ) V ( z) = = R
More informationChem 104A, Fall 2016, Midterm 1 Key
hm 104A, ll 2016, Mitrm 1 Ky 1) onstruct microstt tl for p 4 configurtion. Pls numrt th ms n ml for ch lctron in ch microstt in th tl. (Us th formt ml m s. Tht is spin -½ lctron in n s oritl woul writtn
More informationME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002
3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or
More information6-6 Linear-Elastic Fracture Mechanics Method. Stress Life Testing: R. R. Moore Machine
6-6 Linr-Elstic Frctur Mchnics Mthod tg I Initition o micro-crck du to cyclic plstic dormtion tg II Progrsss to mcrocrck tht rptdly opns nd closs, crting nds clld ch mrks tg III Crck hs propgtd r nough
More informationThis Week. Computer Graphics. Introduction. Introduction. Graphics Maths by Example. Graphics Maths by Example
This Wk Computr Grphics Vctors nd Oprtions Vctor Arithmtic Gomtric Concpts Points, Lins nd Plns Eploiting Dot Products CSC 470 Computr Grphics 1 CSC 470 Computr Grphics 2 Introduction Introduction Wh do
More informationEconomics 201b Spring 2010 Solutions to Problem Set 3 John Zhu
Economics 20b Spring 200 Solutions to Problm St 3 John Zhu. Not in th 200 vrsion of Profssor Andrson s ctur 4 Nots, th charactrization of th firm in a Robinson Cruso conomy is that it maximizs profit ovr
More informationELECTRON-MUON SCATTERING
ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional
More informationCoupled Pendulums. Two normal modes.
Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron
More informationDesign/Modeling for Periodic Nano Structures t for EMC/EMI. Outline
/4/00 Dsign/Modling for Priodic Nno Structurs t for EMC/EMI Ji Chn Dprtmnt of ricl nd Computr Enginring Houston, TX, 7704 Outlin Introduction Composit Mtrils Dsign with Numricl Mixing-Lw FDTD dsign of
More informationBasic 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 informationNONLINEAR ANALYSIS OF PLATE BENDING
NONLINEAR ANALYSIS OF PLATE BENDING CONTENTS Govrning Equations of th First-Ordr Shar Dformation thor (FSDT) Finit lmnt modls of FSDT Shar and mmbran locking Computr implmntation Strss calculation Numrical
More informationFloating Point Number System -(1.3)
Floting Point Numbr Sstm -(.3). Floting Point Numbr Sstm: Comutrs rrsnt rl numbrs in loting oint numbr sstm: F,k,m,M 0. 3... k ;0, 0 i, i,...,k, m M. Nottions: th bs 0, k th numbr o igts in th bs xnsion
More informationNTHU ESS5850 Micro System Design F. G. Tseng Fall/2016, 7-2, p1. Lecture 7-2 MOSIS/SCNA Design Example- Piezoresistive type Accelerometer II
F. G. Tsng Fall/016, 7-, p1 ctur 7- MOSIS/SCNA Dsign Exampl-!! Pizorsistivity Pizorsistiv typ Acclromtr II a Considr a conductiv lock of dimnsion a as shown in th figur. If a currnt is passd through th
More informationFloating Point Number System -(1.3)
Floting Point Numbr Sstm -(.3). Floting Point Numbr Sstm: Comutrs rrsnt rl numbrs in loting oint numbr sstm: F,k,m,M 0. 3... k ;0, 0 i, i,...,k, m M. Nottions: th bs 0, k th numbr o igits in th bs xnsion
More informationThat is, we start with a general matrix: And end with a simpler matrix:
DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss
More informationHIGHER ORDER DIFFERENTIAL EQUATIONS
Prof Enriqu Mtus Nivs PhD in Mthmtis Edution IGER ORDER DIFFERENTIAL EQUATIONS omognous linr qutions with onstnt offiints of ordr two highr Appl rdution mthod to dtrmin solution of th nonhomognous qution
More informationCONTINUITY AND DIFFERENTIABILITY
MCD CONTINUITY AND DIFFERENTIABILITY NCERT Solvd mpls upto th sction 5 (Introduction) nd 5 (Continuity) : Empl : Chck th continuity of th function f givn by f() = + t = Empl : Emin whthr th function f
More informationMiddle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis
Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 4 Introduction to Finit Elmnt Analysis Chaptr 4 Trusss, Bams and Frams Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS
VSRT MEMO #05 MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS 01886 Fbrury 3, 009 Tlphon: 781-981-507 Fx: 781-981-0590 To: VSRT Group From: Aln E.E. Rogrs Subjct: Simplifid
More informationSolution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:
APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding
More informationLinear Algebra Existence of the determinant. Expansion according to a row.
Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit
More informationThe 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 informationCOMPUTATIONAL NUCLEAR THERMAL HYDRAULICS
COMPUTTIONL NUCLER THERML HYDRULICS Cho, Hyoung Kyu Dpartmnt of Nuclar Enginring Soul National Univrsity CHPTER4. THE FINITE VOLUME METHOD FOR DIFFUSION PROBLEMS 2 Tabl of Contnts Chaptr 1 Chaptr 2 Chaptr
More informationPerformance analysis of some CFAR detectors in homogeneous Pearson-distributed clutter
SETIT 5 3 rd Intrnational Confrnc: Scincs of Elctronic, Tchnologis of Information and Tlcommunications arch 7-31, 5 TNISIA Prformanc analysis of som CFAR dtctors in homognous Parson-distributd cluttr iani
More informationINCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS. xy 1 (mod p), (x, y) I (j)
INCOMPLETE KLOOSTERMAN SUMS AND MULTIPLICATIVE INVERSES IN SHORT INTERVALS T D BROWNING AND A HAYNES Abstract W invstigat th solubility of th congrunc xy (mod ), whr is a rim and x, y ar rstrictd to li
More information(2) If we multiplied a row of B by λ, then the value is also multiplied by λ(here lambda could be 0). namely
. DETERMINANT.. Dtrminnt. Introution:I you think row vtor o mtrix s oorint o vtors in sp, thn th gomtri mning o th rnk o th mtrix is th imnsion o th prlllppi spnn y thm. But w r not only r out th imnsion,
More informationAnalysis of Cantilever beams in Liquid Media: A case study of a microcantilever
Intrntionl Journl of Enginring Scinc Invntion (IJESI) ISSN (Onlin): 9 67, ISSN (Prin: 9 676 www.ijsi.org ǁ PP.57-6 Anlysis of Cntilvr bms in iquid Mdi: A cs study of microcntilvr S. Mnojkumr * nd J. Srinivs
More informationQuantum Mechanics & Spectroscopy Prof. Jason Goodpaster. Problem Set #2 ANSWER KEY (5 questions, 10 points)
Chm 5 Problm St # ANSWER KEY 5 qustios, poits Qutum Mchics & Spctroscopy Prof. Jso Goodpstr Du ridy, b. 6 S th lst pgs for possibly usful costts, qutios d itgrls. Ths will lso b icludd o our futur ms..
More informationCONIC SECTIONS. MODULE-IV Co-ordinate Geometry OBJECTIVES. Conic Sections
Conic Sctions 16 MODULE-IV Co-ordint CONIC SECTIONS Whil cutting crrot ou might hv noticd diffrnt shps shown th dgs of th cut. Anlticll ou m cut it in thr diffrnt ws, nml (i) (ii) (iii) Cut is prlll to
More informationErrata for Second Edition, First Printing
Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 71: Eqution (.3) should rd B( R) = θ R 1 x= [1 G( x)] pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1
More informationAnalysis of Convection-Diffusion Problems at Various Peclet Numbers Using Finite Volume and Finite Difference Schemes Anand Shukla
Mathmatical Thory and Modling.iist.org ISSN 4-5804 (apr) ISSN 5-05 (Onlin) Vol., No.6, 01-Slctd from Intrnational Confrnc on Rcnt Trnds in Applid Scincs ith nginring Applications Analysis of Convction-iffusion
More informationUNIT # 08 (PART - I)
. r. d[h d[h.5 7.5 mol L S d[o d[so UNIT # 8 (PRT - I CHEMICL INETICS EXERCISE # 6. d[ x [ x [ x. r [X[C ' [X [[B r '[ [B [C. r [NO [Cl. d[so d[h.5 5 mol L S d[nh d[nh. 5. 6. r [ [B r [x [y r' [x [y r'
More informationFSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, *
CmSc 365 Thory of Computtion Finit Stt Automt nd Rgulr Exprssions (Chptr 2, Sction 2.3) ALPHABET oprtions: U, conctntion, * otin otin Strings Form Rgulr xprssions dscri Closd undr U, conctntion nd * (if
More informationC-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)
An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...
More informationDETERMINATION OF THE DISTORTION COEFFICIENT OF A 500 MPA FREE-DEFORMATION PISTON GAUGE USING A CONTROLLED-CLEARANCE ONE UP TO 200 MPA
XX IMEKO World Congrss Mtrology for Grn Growth Stmbr 9 14, 2012, Busan, Rublic of Kora DETERMINATION OF THE DISTORTION COEFFICIENT OF A 500 MPA FREE-DEFORMATION PISTON GAUGE USING A CONTROLLED-CLEARANCE
More informationErrata for Second Edition, First Printing
Errt for Scond Edition, First Printing pg 68, lin 1: z=.67 should b z=.44 pg 1: Eqution (.63) should rd B( R) = x= R = θ ( x R) p( x) R 1 x= [1 G( x)] = θp( R) + ( θ R)[1 G( R)] pg 15, problm 6: dmnd of
More informationCOMP108 Algorithmic Foundations
Grdy mthods Prudn Wong http://www.s.liv..uk/~pwong/thing/omp108/01617 Coin Chng Prolm Suppos w hv 3 typs of oins 10p 0p 50p Minimum numr of oins to mk 0.8, 1.0, 1.? Grdy mthod Lrning outoms Undrstnd wht
More informationWalk Like a Mathematician Learning Task:
Gori Dprtmnt of Euction Wlk Lik Mthmticin Lrnin Tsk: Mtrics llow us to prform mny usful mthmticl tsks which orinrily rquir lr numbr of computtions. Som typs of problms which cn b on fficintly with mtrics
More informationThe Z transform techniques
h Z trnfor tchniqu h Z trnfor h th rol in dicrt yt tht th Lplc trnfor h in nlyi of continuou yt. h Z trnfor i th principl nlyticl tool for ingl-loop dicrt-ti yt. h Z trnfor h Z trnfor i to dicrt-ti yt
More informationThe model proposed by Vasicek in 1977 is a yield-based one-factor equilibrium model given by the dynamic
h Vsick modl h modl roosd by Vsick in 977 is yild-bsd on-fcor quilibrium modl givn by h dynmic dr = b r d + dw his modl ssums h h shor r is norml nd hs so-clld "mn rvring rocss" (undr Q. If w u r = b/,
More informationPH427/PH527: Periodic systems Spring Overview of the PH427 website (syllabus, assignments etc.) 2. Coupled oscillations.
Dy : Mondy 5 inuts. Ovrviw of th PH47 wsit (syllus, ssignnts tc.). Coupld oscilltions W gin with sss coupld y Hook's Lw springs nd find th possil longitudinl) otion of such syst. W ll xtnd this to finit
More informationStrain-softening in continuum damage models: Investigation of MAT_058
9th Euroan LS-DYNA Confrnc 2013 Strain-softning in continuum damag modls: Invstigation of MAT_058 Karla Simon Gmkow, Rad Vignjvic School of Enginring, Cranfild Univrsity, Cranfild, Bdfordshir, MK43 0AL,
More informationNonlinear analysis of under-deck cable-stayed bridges Z.W. CHEN, X.C. CHEN & Z.Z. BAI, X.C. CHEN*
5th Intrnational Confrnc on Civil, Architctural and Hydraulic Enginring (ICCAHE 016) Nonlinar analysis of undr-dck cabl-stayd bridgs Z.W. CHEN, X.C. CHEN & Z.Z. BAI, X.C. CHEN* Dartmnt of Bridg Enginring,
More informationDESIGNING WITH ANISOTROPY.
DESIGNING WITH ANISOTOPY. PAT : QUASI-HOMOGENEOUS ANISOTOPIC LAMINATES. P. Vannucci, X. J. Gong & G. Vrchry. ISAT - Institut Suériur d l Automobil t ds Transorts, LMA - Laboratoir d chrch n Mécaniqu t
More informationAn analytical model for instant design of an LCD cell with photospacers under gravity and local loading. Reprint. Journal
An analytical modl for instant dsign of an LCD cll ith hotosacrs undr gravity and local loading Ling-Yi Ding Wn-Pin Shih Mao-Hsing Lin Yuh-Chung Hu Pi-Zn Chang Abstract An analytical modl of an LCD cll
More informationFundamentals of Continuum Mechanics. Seoul National University Graphics & Media Lab
Fndmntls of Contnm Mchncs Sol Ntonl Unvrsty Grphcs & Md Lb Th Rodmp of Contnm Mchncs Strss Trnsformton Strn Trnsformton Strss Tnsor Strn T + T ++ T Strss-Strn Rltonshp Strn Enrgy FEM Formlton Lt s Stdy
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationIsogeometric Analysis of Soil Plasticity
Gomatrials, 207, 7, 96-6 htt://www.scir.org/journal/gm ISSN Onlin: 26-7546 ISSN Print: 26-7538 Isogomtric Analysis of Soil Plasticity Alx Stz *, Erika Tudisco, Ralf Dnzr 2, Ola Dahlblom Gotchnical Enginring,
More information2.3 Matrix Formulation
23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,
More informationCSE 373: More on graphs; DFS and BFS. Michael Lee Wednesday, Feb 14, 2018
CSE 373: Mor on grphs; DFS n BFS Mihl L Wnsy, F 14, 2018 1 Wrmup Wrmup: Disuss with your nighor: Rmin your nighor: wht is simpl grph? Suppos w hv simpl, irt grph with x nos. Wht is th mximum numr of gs
More informationNonlinear Bending of Strait Beams
Nonlinar Bnding of Strait Bams CONTENTS Th Eulr-Brnoulli bam thory Th Timoshnko bam thory Govrning Equations Wak Forms Finit lmnt modls Computr Implmntation: calculation of lmnt matrics Numrical ampls
More informationDivision of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.
Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationMATH 1080 Test 2-SOLUTIONS Spring
MATH Tst -SOLUTIONS Spring 5. Considr th curv dfind by x = ln( 3y + 7) on th intrval y. a. (5 points) St up but do not simplify or valuat an intgral rprsnting th lngth of th curv on th givn intrval. =
More information