Duality in constitutive formulation of nite-strain elastoplasticity based on F ˆ F e F p and F ˆ F p F e decompositions

Size: px
Start display at page:

Download "Duality in constitutive formulation of nite-strain elastoplasticity based on F ˆ F e F p and F ˆ F p F e decompositions"

Transcription

1 Intrntionl Journl of Plticity 15 (1999) 1277±1290 Dulity in contitutiv formultion of nit-trin ltoplticity bd on F ˆ F F p nd F ˆ F p F dcompoition V.A. Lubrd Dprtmnt of Mchnicl nd Aropc Enginring, Univrity of Cliforni, Sn Digo, L Joll, CA , USA Rcivd in nl rvid form 19 July 1999 Abtrct A contitutiv thory for lrg ltic±pltic dformtion i prntd by mploying F=F p F dcompoition of th totl dformtion grdint. A dulity in contitutiv formultion bd on thi nd th wll-known L' dcompoition F=F F p i tblihd for iotropic polycrytllin nd ingl crytl plticity. # 1999 Publihd by Elvir Scinc Ltd. All right rrvd. Kyword: Elto-plticity; Contitutiv qution; Finit trin; Dformtion grdint; Multiplictiv dcompoition; Rvrd dcompoition 1. Introduction Th multiplictiv dcompoition of th dformtion grdint into it ltic nd pltic prt F=F F p, originlly introducd by L (1969), h bn frquntly mployd during th pt thr dcd to tudy th contitutiv bhvior of ltopltic polycrytllin mtril nd ingl crytl. Th dcompoition i introducd by d ning t ch tg of dformtion proc tr-fr intrmdit con gurtion B p, obtind from ltoplticlly dformd con gurtion B by concptul ltic unloding to zro tr. Sinc ltic dformtion i rvrd during thi unloding proc, th intrmdit con gurtion i dformd only plticlly, i.. it di r from th originl (undformd) con gurtion B 0 by pltic prt of th dformtion grdint F p. Thu, th multiplictiv dcompoition F=F F p, whr F rprnt ltic prt of th dformtion grdint from B p to B (Fig. 1 ). Th ltopltic dformtion proc i, thrfor, imgind to tk plc in two tg. Firt, thr i pltic ow of mtril, t zro tr, from th initil con gurtion B 0 to intrmdit con gurtion B p, followd by ltic dformtion from B p to B /99/$ - front mttr # 1999 Publihd by Elvir Scinc Ltd. All right rrvd. PII: S (99)00039-X

2 1278 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 Fig. 1. () Intrmdit con gurtion B p i obtind from ltoplticlly dformd con gurtion by ltic unloding to zro tr. L' dcompoition F=F F p rult. (b) Intrmdit con gurtion B i obtind from initil undformd con gurtion by ltic tring, kping frozn mchnim of pltic dformtion. Rvrd dcompoition F=F p F rult. du to totl pplid tr. Th rulting dcompoition of dformtion grdint, F=F F p, providd ound kinmtic nd kintic bi for ltopltic contitutiv nlyi of polycrytllin mtril (.g., Lubrd nd L, 1981, Lubrd nd Shih, 1994), nd ingl crytl (.g., Aro, 1983, Hvnr, 1985,1992). In th wk of F=F F p dcompoition, thr hv bn vrl uggtion for n ltrntiv, rvrd dcompoition F=F p F (.g. Clifton, 1972, Nmt-Nr, 1979), but thi dcompoition rmind virtully unmployd in ubqunt contitutiv nlyi of ltopltic bhvior. Th prnt ppr i rult of my rcnt tudy of F=F p F dcompoition, which I nvr ttmptd to invtigt bfor, bing intrtd in F=F F p dcompoition only. Intrtingly, but prhp not urpriingly, it turnd out tht th contitutiv nlyi of ltopltic bhvior cn b dvlopd by uing th rvrd dcompoition, quit nlogouly to uing L' dcompoition. Th two formultion cn, thu, b viwd dul to ch othr, both lding to th m nl tructur of contitutiv qution, lthough om of th drivtion nd intrprttion r implr in th c of L' dcompoition. Th dcompoition F=F p F i introducd follow. An rbitrry tt of ltopltic dformtion, corrponding to dformtion grdint F, i gin imgind to b rchd in two tg. Firt, it i umd tht ll intrnl mchnim rponibl for pltic dformtion r frozn, o tht, for xmpl, th criticl forc ndd to driv diloction, or criticl rolvd hr tr on crytllin lip ytm, r ignd in nitly lrg vlu. Th ppliction of totl tr to uch mtril, incpbl of pltic dformtion, rult in pur ltic dformtion F tht crri th mtril from initil con gurtion B 0 to intrmdit con gurtion B. Subquntly, th mtril i plticlly unlockd, by unfrzing th mchnim of pltic dformtion, which nbl mtril to ow t contnt tr. Th corrponding prt of th dformtion grdint, from intrmdit con gurtion B to nl con gurtion B, i th pltic prt of th dformtion grdint F p. Thu, th rvrd multiplictiv dcompoition F=F p F (Fig. 1b).

3 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277± Uniqun nd objctivity iu Th untrd intrmdit con gurtion B p of L' dcompoition i not uniqu, bcu uprimpod rottion Q lv thi con gurtion untrd, i.. F ˆ F F p ˆ F^ F^ p; F^ ˆ F Q T ; F^ p ˆ QF p : 1 Suprimpod T dnot th trnpo. If mtril i lticlly iotropic nd rmin uch in th cour of pltic dformtion, rottion of th intrmdit con- gurtion B p h no ct on th tr rpon. Th intrmdit con gurtion cn thn b pci d uniquly by chooing convnintly F =V (th ltic lft trtch tnor). Thu, F=V F p, which w bi of L' (1969) nd Lubrd nd L' (1981) contitutiv nlyi. In th c of rvrd dcompoition F=F p F, th intrmdit lticlly dformd con gurtion B i ncrily uniqu, bcu rottion uprimpod to it would rott th tr tt, wll, nd th pltic ow from B to B would not b t contnt tr ny mor. Furthrmor, if mtril i lticlly iotropic, n initil rottion t B 0 do not ct th tr rpon, nd th rlvnt prt of th totl dformtion grdint i F=F p V. Thrfor, for contitutiv nlyi w cn writ F ˆ V F p ˆ F p V : 2 If mtril i lticlly niotropic, thn, rltiv to givn orinttion of principl dirction of ltic niotropy, thr i uniqu F tht giv ri to totl tr in B or B, which ˆ F F T Hr, i th pci c trin nrgy, E =(1=2)(F T F I) i th Lgrngn ltic trin rltiv to it ground tt (B p in th c of L' dcompoition nd B 0 in th c of rvrd dcompoition, both hving th m orinttion of th principl x of niotropy rltiv to xd frm of rfrnc). Th Kirchho tr i = F, whr dignt th Cuchy tr, nd th dtrminnt. It i lo umd tht pltic ow i incompribl nd tht it do not ct th ltic proprti. Thrfor, w now hv F ˆ F F p ˆ F p F : 4 Not tht th m ltic dformtion grdint mtrix F ppr in both dcompoition. Th rltionhip btwn th two pltic prt of th dformtion grdint i conquntly F p ˆ F 1 F p F ; 5 whr 1 dignt th invr.

4 1280 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 It i hlpful for th ubqunt dvlopmnt to bri y dicu objctivity rquirmnt for th contitunt of th two dcompoition. If rigid-body rottion Q i uprimpod to ltoplticlly dformd con gurtion B, th dformtion grdint F chng to FÃ =QF, whil th Kirchho tr bcom ^=QQ T. Sinc pltic ow from B to B occur t contnt tr, B h to b rottd by Q, wll. Conquntly, F Ã p =QF p Q T nd F Ã =QF. On th othr hnd, F p rmin unchngd, F^ p ˆ F p. Morovr, inc F ˆ V R, th ltic trtch nd rottion tnor chng to V Ã =QV Q T nd R Ã =QR. For brvity, th objctivity rquirmnt corrponding to n indpndnt rottion of intrmdit con gurtion B p of L' dcompoition r not dicud hr, inc thy hv bn xmind in dtil by Lubrd (1991) nd Lubrd nd Shih (1994). 3. Eltic unloding During ltic loding from B p to B, or ltic unloding from B to B p, th pltic dformtion grdint F p of L' dcompoition F=F F p rmin contnt. Thi grtly impli drivtion of th corrponding contitutiv qution. Indd, th vlocity grdint in B i L ˆ F : F 1 ˆ F : F 1 F F : pf 1 p F 1 ; 6 o tht during ltic unloding F : p=0 nd L=F : F 1. Howvr, in th frmwork of rvrd dcompoition, F=F p F, th pltic prt of th dformtion grdint F p do not rmin contnt during ltic unloding. In fct, upon complt unloding from n ltopltic tt of dformtion to zro tr, th con gurtion B p i rchd, nd F p =F p t tht intnt (Fig. 2). Thrfor, F : p 6ˆ 0 during ltic unloding. Thi cn lo b rcognizd from th gnrl rltionhip btwn F p nd F p. By di rntiting Eq. (5), w obtin F : p ˆ F 1 F p F ; 7 Fig. 2. Pltic prt of dformtion grdint F p do not rmin contnt during ltic unloding. Upon complt unloding to zro tr, th con gurtion B p i rchd, nd F p =F p t tht intnt.

5 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277± whr F p ˆ F : p F : F 1 F p F p F : F 1 8 i convctd-typ drivtiv (Hill, 1978) of F p rltiv to ltic dformtion. Clrly, from Eq. (7), F p ˆ 0ifḞ p =0, o tht in tht c F : p ˆ F : F 1 F p F p F : F 1 : 9 Th lt xprion d n th chng of F p during ltic unloding. From Eq. (7), furthrmor, F : pf 1 p ˆ F 1 F p F p 1 F ; 10 nd ubtitution into Eq. (6) giv L ˆ F : F 1 F p F p 1 11 Thi i dul qution to Eq. (6) of L' thory, which will b frquntly ud in th ubqunt nlyi. 4. Polycrytllin plticity W now lbort on th contitutiv formultion of nit-trin ltoplticity within th tructur of rvrd dcompoition F=F p F. Phnomnologicl polycrytllin plticity i rt conidrd. For implicity, ltic iotropy i umd throughout th cour of dformtion. Th ltic tr rpon from B 0 to B i givn by Eq. (3) with F =V. Thu, upon di rntition ˆ K : V : V 1 ; ijkl ˆ V im V V pk V ql : pq Hr, tnd for th convctd-typ drivtiv of th Kirchho tr with rpct to ltic dformtion ˆ : V : V 1 V : T: V Th trc product in Eq. (12) i dnotd by : nd th ubcript tnd for th ymmtric prt.

6 1282 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 In trm of th Jumnn drivtiv ˆ V : V 1 V: V 1 ; 14 Eq. (12) cn b rwrittn ˆ L : V : V 1 ; L ijkl ˆ ijkl 1 2 ik jl il jk ik jl il jk : 15 Th componnt of th unit tnor r th Kronckr ij. By tking ymmtric nd ntiymmtric prt of Eq. (11), w hv: V : V 1 ˆ D V : V 1 ˆ W F p F p 1 F p F p 1 ; 16 : 17 Th trin rt nd pin tnor in th con gurtion B r dnotd by D nd W. Hnc, ˆ F p F p 1 F p F p 1 ; 18 whr ˆ t : W W i th Jumnn drivtiv of th Kirchho tr with rpct to W. Conquntly, ubtitution of Eq. (18) into Eq. (15) giv ˆ L : V : V 1 M : F p F p 1 F p F p 1 : 19 Th fourth-ordr tnor M =L 1 i th intntnou ltic complinc, th invr of th ltic ti n tnor L. Th ltic trin rt D, corrponding to tr rt, i vidntly D ˆ V : V 1 M : F p F p 1 F p F p 1 : 20 In viw of Eq. (16) nd dditiv dcompoition of th trin rt into it ltic nd pltic prt, th pltic prt of th trin rt bcom D p ˆ F p F p 1 M : F pf p 1 F p F p 1 : 21

7 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277± Clrly, during ltic unloding D p =0 nd D =(V V 1 ), inc F p ˆ 0 in th unloding proc. Furthr contitutiv nlyi procd in th c of L' dcompoition. From Eq. (19), th ltic trin rt, xprd in trm of th tr rt, i D ˆ M : : 22 Thi d n rvribl prt of th trin incrmnt, rcovrd upon unloding of th tr incrmnt ocitd with th Jumnn tr rt. Th rmining, pltic prt of th trin rt giv ridul prt of th trin incrmnt. Undr uul umption of clicl plticity, thi i codirctionl with th outwrd norml to loclly mooth yild urfc f in th tr pc. In th c of iotropic hrdning D p ˆ @ : whr th clr function h ccount for th pltic dformtion hitory. Thu, D ˆ M h : ; or, by invrion, ˆ L L : : L : D; whr h 0 =h+(@f/@):l :(@f/@) Strin rt xprion in trm of V,F p nd thir rt Th ltic nd pltic trin rt wr xprd in trm of th contitunt V nd F p of L' dcompoition F=V F p by Lubrd nd L (1981), nd in mor gnrl contxt by Lubrd (1991,b) nd Lubrd nd Shih (1994). In thi ction th corrponding rltion r drivd in th frmwork of rvrd dcompoition F=F p V. Agin, for implicity, only iotropic rpon i conidrd. Firt, introduc th pin th olution of th following mtrix qution W ˆ V : V 1 V V 1 : Th corrponding Jumnn drivtiv of th Kirchho tr nd th ltic trtch V r: 26 r ˆ : ; V r ˆ V : V V : 27

8 1284 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 Applying th drivtiv to Eq. (3), with F =V, thr follow r r ˆ V V 1 V r T V 1 : V r V 1 : 28 In viw of Eq. (26) nd (27) 2, th rltionhip hold V r V 1 ˆ V r V 1 W ; 29 nd ubtitution into Eq. (28) giv ˆ L : V r V 1 : Thi idnti th ltic trin rt D ˆ V r V 1 ˆ V : V 1 V V 1 : On th othr hnd, compring Eq. (17) nd (26) yild V V 1 ˆ F p F p 1 : 32 Thrfor, from Eq. (16) nd (31) th pltic trin rt i givn by D p ˆ D D ˆ F p F p 1 V V 1 : 33 Thi i idnticlly qul to D p ˆ F p F p 1 V V 1 ; 34 inc ntiymmtric prt of th di rnc on th right-hnd id of Eq. (34) vnih by Eq. (32). If hrdning i iotropic, th principl dirction of th tr nd th ltic trtch V r prlll to tho of th pltic trin rt D p. Thu by multiplying Eq. (34) by V 1 from th lft, nd by V from th right, it follow D p ˆ V 1 F p F p 1 V : 35 Tking ymmtric nd ntiymmtric prt of Eq. (35) nlly giv:

9 D p ˆ ˆ V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277± F p F p 1 ; 36 V 1 V 1 F p F p 1 V V : 37 Th xprion r in complt grmnt with th originl rult obtind by Lubrd nd L (1981) in th frmwork of L' dcompoition F=V F p. Indd, inc F p =V 1 F p V, on h V 1 F p F p 1 V ˆ F : pf 1 p ; 38 nd Eq. (36) nd (37) rduc to Lubrd nd L' rult D p ˆ F : pf 1 p ; ˆ F: pf 1 p : 39 Thi dmontrt dulity in contitutiv formultion for iotropic ltoplticity bd on th two ltrntiv dcompoition F=V F p nd F=F p V. 6. Singl crytl plticity W nxt conidr th contitutiv formultion for lrg ltopltic dformtion of ingl crytl, in which crytllogrphic lip i umd to b th only mchnim of pltic dformtion. Th rvr multiplictiv dcompoition F=F p F i mployd to compr th formultion with th wll-known formultion bd on th dcompoition F=F F p (.g. Aro, 1983, whr th nottion F=F F p i ud). Th totl tr i pplid to initil con gurtion B 0, conidring tht crytllogrphic lip i prvntd by igning in nit vlu to criticl rolvd hr tr on ch lip ytm. Th rulting dformtion F i purly ltic, nd cud by lttic trtching nd rottion tht crri B 0 into intrmdit con gurtion B. Subquntly, th criticl rolvd hr tr r rlxd to thir ctul nit vlu, which nbl mtril to ow through th crytllin lttic t contnt tr. Thi prt of dformtion grdint i th pltic prt F p, nd th dcompoition F=F p F hold. Dnot th unit lip dirction nd th norml to th corrponding lip pln in th undformd con gurtion B 0 by 0 nd m 0, whr dignt th lip ytm. Th vctor 0 i mbddd in th lttic, o tht it bcom =F. 0 in th intrmdit con gurtion B. Sinc th mtril ow through th lttic during th dformtion F p, th lip dirction rmin th m in th nl con gurtion B (Fig. 3). Th norml to th lip pln in th con gurtion B nd B i d nd by th rciprocl vctor m =m 0.F 1. In gnrl, nd m r not unit vctor, but r orthogonl to ch othr.

10 1286 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 Fig. 3. Unit lip dirction nd unit norml to lip pln in undformd con gurtion B 0 r 0 nd m 0. Th vctor 0 i mbddd in th lttic, bcoming =F. 0 in th intrmdit con gurtion B.A mtril ow through th lttic during dformtion F p, th lip dirction rmin th m. Th vlocity grdint in th dformd con gurtion B i conqunc of th lip rt : ovr n ctiv lip ytm, uch tht F p F p 1 ˆ n ˆ1 m : ; 40 whr dignt dydic product, nd F p i convctd-typ drivtiv d nd by Eq. (8). Thi convctd rt of F p ppr in Eq. (40) bcu, during ltopltic incrmnt of dformtion, both th currnt nd intrmdit con gurtion, with rpct to which pltic dformtion grdint F p i d nd, dform. Furthrmor, dicud in Sction 3, during ltic unloding from th currnt con gurtion, F p ˆ 0, o tht Eq. (40) i in ccord with th rquirmnt tht during ltic unloding th lip rt : mut lo b qul to zro. In viw of Eq. (10), Eq. (40) i quivlnt to th corrponding qution from th formultion bd on F=F F p dcompoition,whr th point of dprtur i n xprion for F : pf p 1 in trm of th um of lip contribution ( 0 m 0 ) : in th intrmdit con gurtion B p (Aro, 1983). Th ltic rpon of th lttic nd th mtril mbddd on it i dcribd by Eq. (3). It i umd tht crytllogrphic lip i n iochoric dformtion proc, nd tht ltic proprti of th crytl r un ctd by th lip. Thu,

11 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277± ˆ L : F : F 1 ; ˆ : F : F 1 F: F 1 Th componnt of th intntnou ltic ti n tnor of th crytl 2 L ijkl ˆ F im F pq : 41 F kp F lq 1 2 ik jl il jk ik jl il jk : 42 Th trin rt nd pin tnor cn b xprd from Eq. (11) nd (40) : D ˆ F : F 1 ˆ1 n P : ; 43 W ˆ F : F 1 ˆ1 n W : ; 44 whr th cond-ordr tnor r introducd: P ˆ 1 2 m m ; W ˆ 1 2 m m ; 45 commonly don in crytl plticity. Furthr nlyi procd idnticlly in th c of dcompoition F=F F p. Sinc ˆ n ˆ1 W W : ; 46 Eq. (41) bcom ˆ L : D n ˆ1 P M : W W Š : ; 47 which d n th pltic trin rt corrponding to D p ˆ n ˆ1 P M : W W Š : : 48 Phyiclly, D p yild th ridul trin incrmnt lft in th crytl upon n in nitiml loding/unloding cycl ocitd with th tr rt. Th rvribl prt i th ltic prt of th trin rt, D =M :. Th tructur of th trin rt xprion corrponding to othr choic of th tr rt h bn dicud by Lubrd (1994,1999). Eq. (47) cn b rwrittn

12 1288 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 ˆ L : D n ˆ1 K : ; K ˆ L : P W W : 49 To complt th contitutiv formultion, th lip rt : hv to b xprd in trm of th rt of dformtion or th rt of tr. Thi i don in tndrd mnnr. For rt-indpndnt mtril it i umd tht pltic ow occur on lip ytm whn th rolvd hr tr on tht ytm rch th criticl vlu ( ˆ cr ). Th gnrlizd Schmid tr cn b d nd th work conjugt to th lip rt :, uch tht (Hill nd Ric, 1972; Hill nd Hvnr, 1982; Aro, 1983) n ˆ1 : ˆ : n ˆ1 P : : 50 Thrfor, ˆ P :, it rt bing : ˆ K : F : F 1 : If th rt of chng of th criticl rolvd hr tr on givn lip ytm i d nd linr combintion of th lip rt :, th co cint bing th lippln hrdning rt h, th conitncy condition for th lip on th ytm i 51 : ˆ n h : : ˆ1 52 In viw of Eq. (51) nd (43), thi bcom K : D ˆ n g : ; g ˆ h K : P : 53 ˆ1 Thu, th lip rt cn b dtrmind from : ˆ n ˆ1 g 1 K : D; 54 providd tht th mtrix with componnt g i poitiv-d nit (Hill nd Ric, 1972). Subtitution of Eq. (54) into Eq. (49) nlly giv ˆ L n : D; 55 ˆ1ˆ1 n K g 1 K which i th m contitutiv tructur of ingl crytl plticity prntd by Aro (1983) in th frmwork of th dcompoition F=F F p. For prcribd componnt of vlocity grdint, th lip rt r dtrmind from Eq. (54), nd F by intgrtion from Eq. (11) with th incorportd Eq. (40). Th pltic dformtion grdint i thn F p =FF 1.

13 7. Concluion V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277± W hv dmontrtd in thi ppr dulity in contitutiv formultion of lrgdformtion ltoplticity bd on L' dcompoition F=F F p nd rvrd dcompoition F=F p F, t lt for th contitutiv modl conidrd in thi ppr. It i hown tht for mtril tht prrv ltic proprti during pltic dformtion, th m ltic dformtion grdint F ppr in both dcompoition, whil pltic dformtion grdint F p nd F p nturlly di r. Exprion for ltic nd pltic trin rt, drivd in th frmwork of rvrd dcompoition, r givn by Eq. (20) nd (21), nd Eq. (31) nd (36). A kinmtic rprnttion of th vlocity grdint in Eq. (11) w ud in thi drivtion. Th tructur of th obtind xprion i found to b mor involvd thn of tho bd on L' dcompoition, cf. Eq. (36) nd (39). Thi i prtly bcu during ltic unloding th pltic grdint F p of L' dcompoition rmin contnt, whil F p of rvrd dcompoition chng, lbit in d nit mnnr pci d by Eq. (9). Nonthl, within th m phyicl ingrdint, both formultion ld to th m nl tructur of ltopltic contitutiv qution for iotropic polycrytllin mtril nd ingl crytl. Th r givn by Eq. (25) nd (55). In ddition to concptul importnc of dmontrting dulity, th nlyi prntd in thi ppr my b of intrt bcu it i poibl tht in om ppliction th rvrd dcompoition h crtin dvntg. For xmpl, Clifton (1972) found it to b lightly mor convnint for th nlyi of on-dimnionl wv propgtion in ltic-vicopltic olid. It hould, howvr, b pointd out tht L' dcompoition h d nit dvntg in modling plticity with volving ltic proprti. In thi c, t of tructurl tnor cn b ttchd to th intrmdit con gurtion B p to rprnt it currnt tt of ltic niotropy. Th tructurl tnor volv during pltic dformtion, dpnding on th ntur of microcopic inltic proc, thir chng bing rprntd by pproprit volution qution. Th tr rpon t ch intnt of dformtion i givn in trm of th grdint of ltic trin nrgy with rpct to ltic trin, t th currnt vlu of th tructurl tnor. Thi typ of nlyi w ud by Lubrd (1994b) nd Lubrd nd Krjcinovic (1995) in thir tudy of dmg-ltoplticity. In th c of rvrd dcompoition, howvr, th ltic rpon i d nd rltiv to th initil con gurtion B 0, which do not contin ny informtion bout volving ltic proprti or ubquntly dvlopd ltic niotropy. Additionl rmdy h to b introducd to dl with th ftur of mtril rpon, which i likly to mk th rvrd dcompoition l ttrctiv thn th originl dcompoition. Acknowldgmnt Rrch funding providd by th Alco Cntr i kindly cknowldgd. I m in prticulr indbtd to Dr. Own Richmond for dicuion nd for hi long-tnding upport of my work.

14 1290 V.A. Lubrd / Intrntionl Journl of Plticity 15 (1999) 1277±1290 Rfrnc Aro, R.J., Crytl plticity. J. Appl. Mch. 50, 921. Clifton, R.J., On th quivlnc of F F p nd F p F. J. Appl. Mch. 39, 288. Hvnr, K.S., Comprion of crytl hrdning lw in multipl lip. Int. J. Plticity 2, 111. Hvnr, K.S., Finit pltic dformtion of crytllin olid. Int. J. Plticity 2, 111. Hill, R., Apct of invrinc in olid mchnic. In: Yih, C.-S. (Ed.), Advnc in Applid Mchnic. Acdmic Pr, Nw York, pp. 1±75. Hill, R., Hvnr, K.S., Prpctiv in th mchnic of ltopltic crytl. J. Mch. Phy. Solid 30, 5. Hill, R., Ric, J.R., Contitutiv nlyi of ltic-pltic crytl t rbitrry trin. J. Mch. Phy. Solid 20, 401. L, E.H., Eltic-pltic dformtion t nit trin. J. Appl. Mch. 36, 1. Lubrd, V.A., Contitutiv nlyi of lrg lto-pltic dformtion bd on th multiplictiv dcompoition of dformtion grdint. Int. J. Solid Struct. 27, 885. Lubrd, V.A., 1991b. Som pct of lto-pltic contitutiv nlyi of lticlly niotropic mtril. Int. J. Plticity 7, 625. Lubrd, V.A., Eltopltic contitutiv nlyi with th yild urfc in trin pc. J. Mch. Phy. Solid 42, 931. Lubrd, V.A., 1994b. An nlyi of lrg-trin dmg ltoplticity. Int. J. Solid Struct. 31, Lubrd, V.A., On th prtition of rt of dformtion in crytl plticity. Int. J. Plticity 15, 721. Lubrd, V.A., Krjcinovic, D., Som fundmntl iu in rt thory of dmg-ltoplticity. Int. J. Plticity 11, 763. Lubrd, V.A., L, E.H., A corrct d nition of ltic nd pltic dformtion nd it computtionl igni cnc. J. Appl. Mch. 48, 35. Lubrd, V.A., Shih, C.F., Pltic pin nd rltd iu in phnomnologicl plticity. J. Appl. Mch. 61, 524. Nmt-Nr, S., Dcompoition of trin mur nd thir rt in nit dformtion ltoplticity. Int. J. Solid Struct. 15, 155.

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9

Lecture 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 information

APPLICATIONS OF THE LAPLACE-MELLIN INTEGRAL TRANSFORM TO DIFFERNTIAL EQUATIONS

APPLICATIONS OF THE LAPLACE-MELLIN INTEGRAL TRANSFORM TO DIFFERNTIAL EQUATIONS Intrntionl Journl o Sintii nd Rrh Publition Volum, Iu 5, M ISSN 5-353 APPLICATIONS OF THE LAPLACE-MELLIN INTEGRAL TRANSFORM TO DIFFERNTIAL EQUATIONS S.M.Khirnr, R.M.Pi*, J.N.Slun** Dprtmnt o Mthmti Mhrhtr

More information

TOPIC 5: INTEGRATION

TOPIC 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 information

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:

Lecture 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 information

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)

INTEGRALS. 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 information

CIVL 8/ D Boundary Value Problems - Rectangular Elements 1/7

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 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

Instructions for Section 1

Instructions 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 information

Last time: introduced our first computational model the DFA.

Last 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 information

Chapter 16. 1) is a particular point on the graph of the function. 1. y, where x y 1

Chapter 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 information

The Z transform techniques

The 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 information

1 Finite Automata and Regular Expressions

1 Finite Automata and Regular Expressions 1 Fini Auom nd Rgulr Exprion Moivion: Givn prn (rgulr xprion) for ring rching, w migh wn o convr i ino drminiic fini uomon or nondrminiic fini uomon o mk ring rching mor fficin; drminiic uomon only h o

More information

Multi-Section Coupled Line Couplers

Multi-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 information

Algebraic theory of linear viscoelastic nemattodynamics Part 2: Linear viscoelastic nematic viscoelasticity

Algebraic theory of linear viscoelastic nemattodynamics Part 2: Linear viscoelastic nematic viscoelasticity Algbric thory of linr vicoltic nmttodynmic Prt : Linr vicoltic nmtic vicolticity Ardy I. Lonov Drtmnt of Polymr Enginring, Th Univrity of Aron, Aron, Ohio 4435-3, USA. Abtrct Thi cond rt of r dvlo thory

More information

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören ME 522 PINCIPLES OF OBOTICS FIST MIDTEM EXAMINATION April 9, 202 Nm Lst Nm M. Kml Özgörn 2 4 60 40 40 0 80 250 USEFUL FOMULAS cos( ) cos cos sin sin sin( ) sin cos cos sin sin y/ r, cos x/ r, r 0 tn 2(

More information

UNIT # 08 (PART - I)

UNIT # 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 information

Integration Continued. Integration by Parts Solving Definite Integrals: Area Under a Curve Improper Integrals

Integration 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 information

Ch 1.2: Solutions of Some Differential Equations

Ch 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 information

Engineering Differential Equations Practice Final Exam Solutions Fall 2011

Engineering Differential Equations Practice Final Exam Solutions Fall 2011 9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS

MASSACHUSETTS 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 information

Errata for Second Edition, First Printing

Errata 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 information

Einstein Equations for Tetrad Fields

Einstein 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 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

Errata for Second Edition, First Printing

Errata 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 information

PH427/PH527: Periodic systems Spring Overview of the PH427 website (syllabus, assignments etc.) 2. Coupled oscillations.

PH427/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 information

However, many atoms can combine to form particular molecules, e.g. Chlorine (Cl) and Sodium (Na) atoms form NaCl molecules.

However, many atoms can combine to form particular molecules, e.g. Chlorine (Cl) and Sodium (Na) atoms form NaCl molecules. Lctur 6 Titl: Fundmntls of th Quntum Thory of molcul formtion Pg- In th lst modul, w hv discussd out th tomic structur nd tomic physics to undrstnd th spctrum of toms. Howvr, mny toms cn comin to form

More information

Modeling of the Thermomechanical Behavior of Porous Shape Memory Alloys

Modeling of the Thermomechanical Behavior of Porous Shape Memory Alloys odling of th Thrmomchnicl Bhvior of orou hp mory Alloy uhmmd A. Qidwi 1 Go-Cntr Inc. Whington Oprtion ultifunctionl tril Brnch Nvl Rrch Lbortory 4555 Ovrlook Av. W Whington D.C. 2375 vlin B. Entchv 2 Dimitri

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,

, 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 information

The Angular Momenta Dipole Moments and Gyromagnetic Ratios of the Electron and the Proton

The 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 information

Quantum Phase Operator and Phase States

Quantum Phase Operator and Phase States Quantum Pha Oprator and Pha Stat Xin Ma CVS Halth Richardon Txa 75081 USA William Rhod Dpartmnt of Chmitry Florida Stat Univrity Tallaha Florida 3306 USA A impl olution i prntd to th long-tanding Dirac

More information

HIGHER ORDER DIFFERENTIAL EQUATIONS

HIGHER 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 information

Chapter 10 Time-Domain Analysis and Design of Control Systems

Chapter 10 Time-Domain Analysis and Design of Control Systems ME 43 Sytm Dynamic & Control Sction 0-5: Stady Stat Error and Sytm Typ Chaptr 0 Tim-Domain Analyi and Dign of Control Sytm 0.5 STEADY STATE ERRORS AND SYSTEM TYPES A. Bazoun Stady-tat rror contitut an

More information

WEAK VISCOELASTIC NEMATODYNAMICS OF MAXWELL TYPE

WEAK VISCOELASTIC NEMATODYNAMICS OF MAXWELL TYPE WEAK VISCOELASTIC NEMATODYNAMICS OF MAXWELL TYPE Ardy I. Lonov, Vlry S. Volov b ) Drtmnt of Polymr Enginring, Th Univrity of Aron, Aron, Ohio 445-, USA. b) Lbortory of Rhology, Intitut of Ptrochmicl Synthi,

More information

THE SPINOR FIELD THEORY OF THE PHOTON

THE SPINOR FIELD THEORY OF THE PHOTON Romnin Rports in Physics, Vol. 66, No., P. 9 5, 4 THE SPINOR FIELD THEORY OF THE PHOTON RUO PENG WANG Pking Univrsity, Physics Dprtmnt, Bijing 87, P.R. Chin E-mil: rpwng@pku.du.cn Rcivd Octobr 8, Abstrct.

More information

CSE303 - Introduction to the Theory of Computing Sample Solutions for Exercises on Finite Automata

CSE303 - Introduction to the Theory of Computing Sample Solutions for Exercises on Finite Automata CSE303 - Introduction to th Thory of Computing Smpl Solutions for Exrciss on Finit Automt Exrcis 2.1.1 A dtrministic finit utomton M ccpts th mpty string (i.., L(M)) if nd only if its initil stt is finl

More information

SCIENCE CHINA Physics, Mechanics & Astronomy. An energy-equilibrium model for complex stress effect on fatigue crack initiation

SCIENCE CHINA Physics, Mechanics & Astronomy. An energy-equilibrium model for complex stress effect on fatigue crack initiation SCIENCE CHINA Phyic, Mchnic & Atronoy Articl My 014 Vol.57 No.5: 916 96 doi: 10.1007/11433-013-541-z An nrgy-quilibriu odl or coplx tr ct on tigu crck initition ZHAO SiCong, XIE JiJi *, ZHAO AiGuo & WU

More information

This Week. Computer Graphics. Introduction. Introduction. Graphics Maths by Example. Graphics Maths by Example

This 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 information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

COMP108 Algorithmic Foundations

COMP108 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 information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

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

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here,

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here, Numrical Eampl In thi final chaptr, w tart b illutrating om known rult in th thor and thn procd to giv a fw novl ampl. All ampl conidr th quation F(u) = u f(u) = g, (-) with Dirichlt boundar condition

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 8: Effect of a Vertical Field on Tokamak Equilibrium

22.615, 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 information

Walk Like a Mathematician Learning Task:

Walk 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 information

A Quadratic Serendipity Plane Stress Rectangular Element

A Quadratic Serendipity Plane Stress Rectangular Element MAE 323: Chaptr 5 Putting It All Togthr A Quadratic Srndipity Plan Str Rctangular Elmnt In Chaptr 2, w larnd two diffrnt nrgy-bad mthod of: 1. Turning diffrntial quation into intgral (or nrgy) quation

More information

FSA. CmSc 365 Theory of Computation. Finite State Automata and Regular Expressions (Chapter 2, Section 2.3) ALPHABET operations: U, concatenation, *

FSA. 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 information

A Method for Interpolation Wavelet Construction Using Orthogonal Scaling Functions

A Method for Interpolation Wavelet Construction Using Orthogonal Scaling Functions A Mthod for Intrpoltion Wvlt Contruction Uing Orthogonl Scling Function higuo hng Collg of Autotion Univrity of Elctronic Scinc nd Tchnology of Chin Chngdu, Chin zhiguozhng@utc.du.cn Mr A. Kon Dprtnt of

More information

(1) Then we could wave our hands over this and it would become:

(1) Then we could wave our hands over this and it would become: MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

5.2 Plasticity I: Hypoelastic-Plastic Models

5.2 Plasticity I: Hypoelastic-Plastic Models 5. Platicity Hyolatic-Platic Modl h two main ty o claical laticity modl or larg train ar th hyolaticlatic modl and th hyrlatic-latic modl. h irt o th i dicud in thi ction. 5.. Hyolaticity n th hyolatic-latic

More information

Minimum Spanning Trees

Minimum Spanning Trees Minimum Spnning Trs Minimum Spnning Trs Problm A town hs st of houss nd st of rods A rod conncts nd only houss A rod conncting houss u nd v hs rpir cost w(u, v) Gol: Rpir nough (nd no mor) rods such tht:

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 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 information

Chapter 11 Calculation of

Chapter 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 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

( ) Geometric Operations and Morphing. Geometric Transformation. Forward v.s. Inverse Mapping. I (x,y ) Image Processing - Lesson 4 IDC-CG 1

( ) Geometric Operations and Morphing. Geometric Transformation. Forward v.s. Inverse Mapping. I (x,y ) Image Processing - Lesson 4 IDC-CG 1 Img Procssing - Lsson 4 Gomtric Oprtions nd Morphing Gomtric Trnsformtion Oprtions dpnd on Pil s Coordints. Contt fr. Indpndnt of pil vlus. f f (, ) (, ) ( f (, ), f ( ) ) I(, ) I', (,) (, ) I(,) I (,

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

(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 information

An Inventory Model with Change in Demand Distribution

An Inventory Model with Change in Demand Distribution Autralian Journal of Baic and Applid cinc, 5(8): 478-488, IN 99-878 An Invntory Modl with Chang in Dmand Ditribution P.. hik Uduman,. rinivaan, 3 Dowlath Fathima and 4 athyamoorthy, R. Aociat Profor, H.O.D

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

Self-interaction mass formula that relates all leptons and quarks to the electron

Self-interaction mass formula that relates all leptons and quarks to the electron Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris

More information

Collisions between electrons and ions

Collisions between electrons and ions DRAFT 1 Collisions btwn lctrons and ions Flix I. Parra Rudolf Pirls Cntr for Thortical Physics, Unirsity of Oxford, Oxford OX1 NP, UK This rsion is of 8 May 217 1. Introduction Th Fokkr-Planck collision

More information

The Relativistic Stern-Gerlach Force C. Tschalär 1. Introduction

The Relativistic Stern-Gerlach Force C. Tschalär 1. Introduction Th Rlativistic Strn-Grlach Forc C. Tschalär. Introduction For ovr a dcad, various formulations of th Strn-Grlach (SG) forc acting on a particl with spin moving at a rlativistic vlocity in an lctromagntic

More information

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting

More information

Miscellaneous open problems in the Regular Boundary Collocation approach

Miscellaneous 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 information

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon.

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon. PART I TRUE/FALSE/UNCERTAIN (5 points ach) 1. Lik xpansionary montary policy, xpansionary fiscal policy rturns output in th mdium run to its natural lvl, and incrass prics. Thrfor, fiscal policy is also

More information

L 1 = L G 1 F-matrix: too many F ij s even at quadratic-only level

L 1 = L G 1 F-matrix: too many F ij s even at quadratic-only level 5.76 Lctur #6 //94 Pag of 8 pag Lctur #6: Polyatomic Vibration III: -Vctor and H O Lat tim: I got tuck on L G L mut b L L L G F-matrix: too many F ij vn at quadratic-only lvl It obviou! Intrnal coordinat:

More information

DISCRETE TIME FOURIER TRANSFORM (DTFT)

DISCRETE TIME FOURIER TRANSFORM (DTFT) DISCRETE TIME FOURIER TRANSFORM (DTFT) Th dicrt-tim Fourir Tranform x x n xn n n Th Invr dicrt-tim Fourir Tranform (IDTFT) x n Not: ( ) i a complx valud continuou function = π f [rad/c] f i th digital

More information

CBSE 2015 FOREIGN EXAMINATION

CBSE 2015 FOREIGN EXAMINATION CBSE 05 FOREIGN EXAMINATION (Sris SSO Cod No 65//F, 65//F, 65//F : Forign Rgion) Not tht ll th sts hv sm qustions Onl thir squnc of pprnc is diffrnt M Mrks : 00 Tim Allowd : Hours SECTION A Q0 Find th

More information

Lecture 12 Quantum chromodynamics (QCD) WS2010/11: Introduction to Nuclear and Particle Physics

Lecture 12 Quantum chromodynamics (QCD) WS2010/11: Introduction to Nuclear and Particle Physics Lctur Quntum chromodynmics (QCD) WS/: Introduction to Nuclr nd Prticl Physics QCD Quntum chromodynmics (QCD) is thory of th strong intrction - bsd on color forc, fundmntl forc dscribing th intrctions of

More information

Mathematics. Mathematics 3. hsn.uk.net. Higher HSN23000

Mathematics. 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 information

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th

More information

CONTINUITY AND DIFFERENTIABILITY

CONTINUITY 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 information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

ELECTRON-MUON SCATTERING

ELECTRON-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 information

Asymptotic Behaviour of the Solutions. of the Falkner-Skan Equations. Governing the Swirling Flow

Asymptotic Behaviour of the Solutions. of the Falkner-Skan Equations. Governing the Swirling Flow Adv. Thor. Appl. Mch., Vol. 3,, no. 4, 5-58 Aymptotic Bhaviour o th Solution o th Falknr-Skan Equation Govrning th Sirling Flo J. Singh Dpartmnt o Civil Enginring, ntitut o Tchnology, Banara Hindu Univrity,

More information

1 Introduction to Modulo 7 Arithmetic

1 Introduction to Modulo 7 Arithmetic 1 Introution to Moulo 7 Arithmti Bor w try our hn t solvin som hr Moulr KnKns, lt s tk los look t on moulr rithmti, mo 7 rithmti. You ll s in this sminr tht rithmti moulo prim is quit irnt rom th ons w

More information

Stress and Strain Analysis of Notched Bodies Subject to Non-Proportional Loadings

Stress 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 information

Section 3: Antiderivatives of Formulas

Section 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 information

MASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS SEMESTER TWO 2014 WEEK 11 WRITTEN EXAMINATION 1 SOLUTIONS

MASTER 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 information

Garnir Polynomial and their Properties

Garnir Polynomial and their Properties Univrsity of Cliforni, Dvis Dprtmnt of Mthmtis Grnir Polynomil n thir Proprtis Author: Yu Wng Suprvisor: Prof. Gorsky Eugny My 8, 07 Grnir Polynomil n thir Proprtis Yu Wng mil: uywng@uvis.u. In this ppr,

More information

I. The Connection between Spectroscopy and Quantum Mechanics

I. 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 information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

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

Exp-function method to solve the nonlinear dispersive K(m,n) equations

Exp-function method to solve the nonlinear dispersive K(m,n) equations From th SlctdWork of Ji-Hn H 8 Exp-fnction mthod to olv th nonlinr dipriv K(mn qtion Xin-Wi Zho Yi-Xin Wn Ji-Hn H Dongh Univrity Avilbl t: http://work.bpr.com/ji_hn_h/9/ Frnd Pblihing Ho Ltd. Intrntionl

More information

Theoretical Study on the While Drilling Electromagnetic Signal Transmission of Horizontal Well

Theoretical 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

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

Oppgavesett kap. 6 (1 av..)

Oppgavesett kap. 6 (1 av..) Oppgvstt kp. 6 (1 v..) hns.brnn@go.uio.no Problm 1 () Wht is homognous nucltion? Why dos Figur 6.2 in th book show tht w won't gt homognous nucltion in th tmosphr? ˆ Homognous nucltion crts cloud droplts

More information

CONIC SECTIONS. MODULE-IV Co-ordinate Geometry OBJECTIVES. Conic Sections

CONIC 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 information

Chem 104A, Fall 2016, Midterm 1 Key

Chem 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 information

KOHN LUTTINGER SUPERCONDUCTIVITY IN GRAPHENE

KOHN LUTTINGER SUPERCONDUCTIVITY IN GRAPHENE KOHN LUTTINGER SUPERCONDUCTIITY IN GRAPHENE J. Gonzálz Instituto d Estructur d l Mtri, CSIC, Spin Is it possibl to hv suprconducting instbility in grphn (by suitbl doping)? Thr hv bn lrdy svrl proposls

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

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1

More information

Chapter 10. The singular integral Introducing S(n) and J(n)

Chapter 10. The singular integral Introducing S(n) and J(n) Chaptr Th singular intgral Our aim in this chaptr is to rplac th functions S (n) and J (n) by mor convnint xprssions; ths will b calld th singular sris S(n) and th singular intgral J(n). This will b don

More information

Sequence Mirroring Properties of Orthogonal Transforms Having Even and Odd Symmetric Vectors

Sequence Mirroring Properties of Orthogonal Transforms Having Even and Odd Symmetric Vectors ECT TANSACTONS ON COMPUTE AND NFOMATON TECNOLOGY VOL., NO. 2 NOVEMBE 2 Squnc Mirroring Proprti of Orthogonal Tranform aving Evn and Odd Symmtric Vctor Do Nyon Kim and K.. ao Dpartmnt of Elctrical Enginring,

More information

Laplace Transform. National Chiao Tung University Chun-Jen Tsai 10/19/2011

Laplace Transform. National Chiao Tung University Chun-Jen Tsai 10/19/2011 plc Trnorm Nionl Chio Tung Univriy Chun-Jn Ti /9/ Trnorm o Funcion Som opror rnorm uncion ino nohr uncion: d Dirniion: x x, or Dx x dx x Indini Ingrion: x dx c Dini Ingrion: x dx 9 A uncion my hv nicr

More information