Another view for a posteriori error estimates for variational inequalities of the second kind
|
|
- Lenard Smith
- 6 years ago
- Views:
Transcription
1 Accptd by Applid Numrical Mathmatics in July 2013 Anothr viw for a postriori rror stimats for variational inqualitis of th scond kind Fi Wang 1 and Wimin Han 2 Abstract. In this papr, w giv anothr viw to undrstand a postriori rror analysis for finit lmnt solutions of lliptic variational inqualitis of th scond kind. This point of viw maks it simplr to driv rliabl rror stimators in solving variational inqualitis of th scond kind from th thory for rlatd linar variational quations. Rliabl rsidual-basd and gradint rcovry-basd stimators ar dducd. Efficincy of th stimators is also provd. ywords. Variational inquality; a postriori rror stimators; rliability; fficincy AMS Classification. 65N15, 65N30 1 Introduction Adaptiv finit lmnt mthods basd on a postriori rror stimats ar an activ rsarch fild. Many rror stimators can b classifid as rsidual typ or rcovry typ. Various rsidual quantitis ar usd to captur lost information going from u to u h, such as rsidual of th quation, rsidual from drivativ discontinuity and so on. In a gradint rcovry rror stimator, G h u h u h is usd to approximat u u h, whr a gradint rcovry oprator G h is applid to th numrical solution u h to rconstruct th gradint of th tru solution u. Th thory of a postriori rror stimation is wll stablishd for linar quations, and w rfr th radr to [1, 2, 16]. It is mor difficult to dvlop a postriori rror stimators for variational inqualitis (VIs) du to th inquality fatur. Nvrthlss, numrous paprs can b found on a postriori rror 1 School of Mathmatics and Statistics, Huazhong Univrsity of Scinc and Tchnology, Wuhan , China. Dpartmnt of Mathmatics, Univrsity of Iowa, Iowa City, Iowa 52242, USA. wangfitwo@163.com. Th work of this author was substantially supportd by th Chins National Scinc Foundation (Grant No ), and partially supportd by th Fundamntal Rsarch Funds for th Cntral Univrsity, HUST (Grant No. 2011QN169). 2 Dpartmnt of Mathmatics & Program in Applid Mathmatical and Computational Scincs, Univrsity of Iowa, Iowa City, Iowa 52242, USA. Th work of this author was supportd by th Simons Foundation. 1
2 stimation of finit lmnt mthods for obstacl problms, which is a rprsntativ lliptic variational inquality (EVI) of th first kind,.g., [3,10,13 15,17]. For VIs of th scond kind, in [4 7], th authors studid a postriori rror stimats and stablishd a framwork through th duality thory, but th sharpr stimation of on trm in th lowr bound is still an opn problm, i.., th fficincy was not compltly provd. In [8], Brass dmonstratd that a postriori rror stimators for finit lmnt solutions of th obstacl problm can b asily drivd by applying a postriori rror stimators for a rlatd linar lliptic problm. In this papr, w xtnd th idas thrin to giv anothr look at a postriori rror analysis for VIs of th scond kind. Morovr, w accomplish th proof for th fficincy of th rror stimators. W tak a stady stat frictional contact problm as an xampl to illustrat th drivation procss of a postriori rror stimators. Th idas and tchniqus prsntd hr for this modl problm can b xtndd to othr VIs of th scond kind. A frictional contact problm. Lt Ω R d (d 1) b a boundd domain with Lipschitz boundary Γ, Γ 1 a rlativly closd subst of Γ, and Γ 2 = Γ\Γ 1. Assum f L 2 (Ω), and g > 0 is a constant. Thn a frictional contact problm is to find u V = {v H 1 (Ω) : v = 0 a.. on Γ 1 } such that a(u, v u) + j(v) j(u) (f, v u) Ω v V, (1.1) whr (, ) Ω dnots th L 2 innr product in th domain Ω and a(u, v) = u v dx + u v dx, Ω Ω j(v) = g v ds. Γ 2 It was provd ( [12, Thorm 5.3], [11]) that this problm has a uniqu solution u V, and thr xists a uniqu Lagrang multiplir λ L (Γ 2 ) such that a(u, v) + g λ v ds = (f, v) Ω v V, (1.2) Γ 2 λ 1, λ u = u a.. on Γ 2. (1.3) It follows from (1.2) and (1.3) that th solution u of (1.1) is th wak solution of th boundary valu problm u + u = f in Ω, u = 0 on Γ 1, u n g, u n u + g u = 0 on Γ 2, whr n is th unit outward normal vctor. For any v V, st l(v) = (f, v) Ω g λ v ds. Γ 2 2
3 Thn (1.2) bcoms a(u, v) = l(v) v V. (1.4) For a Lipschitz subdomain ω Ω, lt v 2 1,ω := a ω (v, v) = ( v 2 + v 2 ) dx. For a masurabl subst γ ω Γ 2, dfin { } λ,γ := sup g λ v ds : v H 1 (ω), v 1,ω = 1. (1.5) Th subscript γ and ω ar omittd if γ = Γ 2 and ω = Ω. W hav γ ω λ,γ = w 1,ω, (1.6) whr w H 1 (ω) is th solution of th auxiliary quation a ω (w, v) = g λ v ds v H 1 (ω). (1.7) Th rlation (1.6) is provd as follows. First, g λ v ds = a ω (w, v) w 1,ω v 1,ω. Thus, γ λ,γ = Ltting v = w in (1.7), w hav w 1,ω = γ sup g λ v ds/ v 1,ω w 1,ω. 0 v H 1 (ω) γ γ g λ w ds/ w 1,ω λ,γ. W introduc a family of finit lmnt spacs V h V corrsponding to partitions T h of Ω into triangular or ttrahdral lmnts (othr kinds of lmnts, such as quadrilatral lmnts, or hxahdral or pntahdral lmnts, can b considrd as wll). Th partitions T h ar compatibl with th dcomposition of Γ into Γ 1 and Γ 2. Thn th finit lmnt mthod for th VI (1.1) is: Find u h V h such that a(u h, v h u h ) + j(v h ) j(u h ) (f, v h u h ) Ω v h V h. (1.8) Similar to th continuous problm, th discrt problm has a uniqu solution u h V h and thr xists a uniqu Lagrang multiplir λ h L (Γ 2 ) such that ( [6, 12]) a(u h, v h ) + g λ h v h ds = (f, v h ) Ω v h V h, (1.9) Γ 2 λ h 1, λ h u h = u h a.. on Γ 2. (1.10) 3
4 For any v h V h, lt l h (v h ) = (f, v h ) Ω g λ h v h ds. Γ 2 From Hahn-Banach xtnsion thorm, th boundd linar functional l h, originally dfind on V h, can b xtndd to a boundd linar functional on V with th norm prsrvd. Thn (1.9) bcoms a(u h, v h ) = l h (v h ) v h V h. (1.11) Obviously, u h is also th finit lmnt approximation of th solution z V of th linar problm: a(z, v) = l h (v) v V, (1.12) which is th wak formulation of th boundary valu problm z + z = f in Ω, (1.13) z = 0 on Γ 1, z n = gλ h on Γ 2. Now w prsnt th procss to driv a postriori rror stimators for th finit lmnt mthod (1.8). From (1.4) and (1.12), for all v V, w hav a(u h u, v) = a(u h z, v) + a(z u, v) = a(u h z, v) + l h (v) l(v) = a(u h z, v) + g(λ λ h )v ds. Γ 2 Tak v = u h u in th abov rlation. Not that by (1.3) and (1.10), w hav g(λ λ h )v ds = g λ u h ds g λ u ds g λ h u h ds + g λ h u ds Γ 2 Γ 2 Γ 2 Γ 2 Γ 2 g u h ds g u ds g u h ds + g u ds Γ 2 Γ 2 Γ 2 Γ 2 Thn w obtain Thrfor, = 0. u h u 2 1 = a(u h u, u h u) a(u h z, u h u) u h z 1 u h u 1. (1.14) u h u 1 u h z 1. (1.15) 4
5 Rcalling (1.6), w hav λ λ h = u z 1 u u h 1 + u h z 1 2 u h z 1. W summariz th abov rsults in th following thorm. Thorm 1.1 Lt u and z b th solutions of th problm (1.1) and (1.12), and lt u h b th finit lmnt solution of u. Thn, u h u 1 + λ λ h 3 u h z 1. This rsult is th starting point for drivation of a postriori rror stimators, whn combind with th standard rsults ( [1]) on rror stimators for th trm u h z 1. Basd on this obsrvation, w discuss rsidual typ rror stimators and gradint rcovry typ rror stimators in th nxt two sctions. Rliability and fficincy ar provd for both typs of rror stimators. 2 Rsidual typ rror stimators First, w introduc som notations. Givn a boundd st D R d and a positiv intgr m, H m (D) is th usual Sobolv spac with th corrsponding norm m,d and smi-norm m,d, which ar abbrviatd by m and m, rspctivly, whn D coincids with Ω. For convninc, w rwrit 0,D as D. W assum Ω is a polyhdral domain and dnot by {T h } h a family of partitions of Ω. For a partition T h, dnot all th dgs of T h by E h, and Eh i = E h\γ, E h,γ2 = E h Γ 2. Lt h = diam() for T h and h = diam() for E h. For any lmnt T h, dfin th patch st ω := {T T h, T }, and for any dg shard by two lmnts and, dfin ω :=. For a givn lmnt T h, N () and E() dnot th sts of th nods of and sids of, rspctivly; n dnots th unit outward normal vctor to th boundary of and n a unit vctor on. Throughout th papr, C dnots a gnric positiv constant indpndnt of th lmnt siz, which may tak diffrnt valus at diffrnt occurrncs. Dfin th intrior rsiduals and dg-basd jumps R := u h + u h f for ach T h, { [ u h R := ] if E i n h, u h + g λ n h if E h,γ2. 5
6 Hr [ u h ] = u n h n + u h n rprsnts th discontinuity of th gradint of u h across th dg shard by th nighboring lmnts and. Thy lad to th local stimators 1/2 η R, = h 2 k R h R 2 + h R 2 for any T h. (2.1) 2 E() E h,γ2 E() E i h It follows from [1] that th rsidual-typ a postriori rror stimator for th lliptic quation (1.13) satisfis ( ) 1/2 u h z 1 C. Hnc, w hav th following thorm. T h η 2 R, Thorm 2.1 Lt u V and u h V h b th solutions of th problms (1.1) and (1.8). Thn, u h u 1 + λ λ h Cη R, η 2 R := T h η 2 R,. Now w turn to considr lowr bounds with rsidual rror stimators. This can b achivd by following th standard argumnt for lowr bounds with rsidual rror stimators for linar lliptic problms, s [1, pp ]. Dfin ( ) a (u, v) = u v + uv dx, so that for u, v H 1 (Ω), a(u, v) = T h a (u, v). For any v V, by intgration by parts, w hav a (u h u, v) = a (u h z, v) + a(z u, v) T h T h = R v dx + R v ds + T h E i h E h,γ 2 E h,γ2 g(λ λ h )v ds. (2.2) W will us th bubbl functions. For ach T h, lt λ 1, λ 2 and λ 3 b th barycntric coordinats on. Thn th intrior bubbl function ϕ is dfind by ϕ = 27λ 1 λ 2 λ 3, and th thr dg bubbl functions ar givn by τ 1 = 4λ 2 λ 3, τ 2 = 4λ 1 λ 3, τ 3 = 4λ 1 λ 2. W rcall som proprtis of th bubbl functions ( [1, Thorms 2.2 and 2.3]). 6
7 Lmma 2.2 For ach T h, E(), lt ϕ and τ b th corrsponding intrior and dg bubbl functions. Lt P () H 1 () and P () H 1 () b finit-dimnsional spacs of functions dfind on and. Thn thr xists a constant C, indpndnt of h, such that for all v P (), C 1 v 2 ϕ v 2 dx C v 2, (2.3) C 1 v ϕ v + h ϕ v 1, C v, (2.4) C 1 v 2 τ v 2 ds C v 2, (2.5) h 1/2 τ v + h 1/2 τ v 1, C v. (2.6) For ach T h, ϕ and τ ar rspctivly th intrior and dg bubbl functions on or E i h E h,γ 2, and R is an approximation to th intrior rsidual R from a suitabl finit lmnt spac containing u h and u h. In (2.2), choosing v = R ϕ on lmnt and using an argumnt similar to that in [1, pp ], w obtain R C ( R R + h 1 u h u 1, ). For E i h, lt R b an approximation to th jump R from a suitabl finit-dimnsional spac and lt v = R τ in (2.2). W hav R C ( h 1/2 u h u 1,ω + h 1/2 R R ω + R R ). For E h,γ2, w obtain a ω (u h u, R τ ) = R R τ dx + R R τ ds + g(λ λ h )R τ ds. ω Thrfor, R 2 τ ds = R (R R )τ ds + a ω (u h u, R τ ) R R τ dx g(λ λ h )R τ ds. ω Applying Lmma 2.2, w bound th trms in th abov rlation as follows: R 2 τ ds C 1 R 2, R (R R )τ ds R τ R R C R R R, a ω (u h u, R τ ) u h u 1,ω R τ 1,ω Ch 1/2 u h u 1,ω R, R R τ dx R ω R τ ω Ch 1/2 R ω R, ω g(λ λ h )R τ ds λ λ h, R τ 1,ω Ch 1/2 λ λ h, R. 7
8 Hnc, R R + R R C ( h 1/2 u h u 1,ω + h 1/2 λ λ h + h 1/2 R R ω + R R ). (2.7) Not that u h +u h in and u h / n on ar polynomials. Hnc, th trms R R and R R can b rplacd by f f and λ h λ h, with discontinuous picwis polynomial approximations f and λ h. Thn w obtain th fficincy bound of th local rror indicator η R, (s also [5, 6]). Thorm 2.3 Lt u and u h b th solutions of (1.1) and (1.8), rspctivly, and lt η R, b th stimator (2.1). Thn ηr, 2 C u u h 2 1,ω + λ λ h 2, + h 2 f f 2 ω + h λ h λ h 2. (2.8) E() E h,γ2 Du to th inquality natur of th variational inqualitis, in th fficincy bound (2.8) of η R,, thr is a trm involving λ and λ h. In [5, 6], bcaus of th prsnc of this trm, th fficincy of th stimators was not provd compltly. From Thorm 2.1, w s that th involvmnt of th trm λ λ h, in th bound (2.8) is vry natural. This commnt is also valid for th cas of gradint rcovry typ rror stimators. 3 Gradint rcovry typ rror stimators In this sction, w study a gradint rcovry typ rror stimator for th linar finit lmnt solution of th frictional contact problm (1.1). Som additional notations ar ndd in this sction. W dnot by N h th st of nods of T h, and N h,0 is th st of fr nods, i.., thos nods that do not li on Γ 1. Lt N v N h b th st of th lmnt vrtics of th partition T h, N v,γ1 N v th subst of th lmnt vrtics lying on Γ 1, N v,i N v th st of th intrior vrtics, and N v,0 = N v N h,0. Lt {ϕ a : a N v } dnot th nodal basis functions of th linar lmnts for all th vrtics. Dfin an quivalnc rlation { a, if a Nv,0 ; ξ(a) := b, b N v,i and T h, s.t. a, b if a N v,γ1. Thn w can classify th st of vrtics N v into card(n v,0 ) classs of quivalnc, that is, I(a) = {ã N v : ξ(ã) = a} for ach nod a N v,0. W st ψ a = ϕã for vry nod a N v,0. ã I(a) 8
9 Not that {ψ a : a N v,0 } is a partition of unity. Lt a = supp(ψ a ) and h a = diam( a ). For a givn v L 1 (Ω), lt v a = vψ a dx ϕ a dx, a N v,0. Thn a Clémnt typ intrpolation oprator Π h : V V h is dfind as follows: Π h v = a N v,0 v a ϕ a. Th nxt thorm summarizs som basic stimats for Π h. Its proof can b found in [9]. Thorm 3.1 Thr xists an h-indpndnt positiv constant C such that for all v V and f L 2 (Ω), v Π h v 2 1,Ω C v 2 1,Ω, f(v Π h v) dx C v 1,Ω h 2 a min f f a 2 Ω f a R 0, a a N v,0 h 1 (v Π hv) 2 C v 2 1,Ω, T h h 1/2 (v Π h v) 2 C v 2 1,Ω. E h Thr ar many typs of gradint rcovry oprators G h. For G h u h to b a good approximation of th tru gradint u, a st of sufficint conditions can b found in [1, Lmma 4.5]. Considr a gradint rcovry oprator G h : V h (V h ) d dfind as follows: G h v h (x) = G h v h (a)ϕ a (x), G h v h (a) = 1 a N v v h dx. a a From (1.11) and (1.12), w gt th Galrkin orthogonality a(u h z, v h ) = 0 v h V h. Using th abov quation, for any v V, w gt 1/2, whr a(u h z, v) = a(u h z, v Π h v) = I 0 + G h u h (v Π h v) dx + u h (v Π h v) dx a(z, v Π h v) Ω Ω I 0 = ( u h G h u h ) (v Π h v) dx C u h G h u h Ω v 1,Ω. Ω 9
10 Prform lmnt-wis intgration by parts, G h u h (v Π h v) dx = G h u h (v Π h v) dx T h Ω = div(g h u h ) (v Π h v) dx + (G h u h n ) (v Π h v) ds. T h T h E() Th first summation is rwrittn as div( u h G h u h ) (v Π h v) dx + u h (v Π h v) dx. T h T h Sinc G h u h is continuous across th lmnt boundaris, (G h u h n ) (v Π h v) ds = (G h u h n )(v Π h v) ds. T E() h E h,γ2 Applying th abov rlations and using th quation (1.12), w obtain that a(u h z, v) = I 0 + I 1 + I 2 + I 3, (3.1) whr I 1 = div( u h G h u h )(v Π h v) dx, T h I 2 = ( u h + u h f)(v Π h v) dx = R (v Π h v) dx, T h T h I 3 = E h,γ2 (G h u h n + gλ h )(v Π h v) ds. It is shown in [6] (s also [4]) that I 1 C v 1,Ω ( T h u h G h u h 2 ) 1/2, I 2 C v 1,Ω a N v,0 ( ) h 4 a u h 2 a + h 2 a min f f a 2 a, f a R I 3 C v 1,Ω h G h u h n + gλ h 2 E h,γ2 Taking v = u h z in (3.1) and rcalling Thorm 1.1, w obtain th nxt rsult. 10 1/2.
11 Thorm 3.2 Lt u and u h b th solutions of (1.1) and (1.8), rspctivly. Thn u u h λ λ h 2 CηG 2 + C ( ) h 4 a u h 2 a + h 2 a min f f a 2 a, (3.2) f a R whr a N h,0 η 2 G = T h η 2 G,, η 2 G, = u h G h u h 2 + E() E h,γ2 h G h u h n + gλ h 2. (3.3) Th trm 1/2 h 4 a u h 2 a is boundd by O(h 2 ), and 1/2 h 2 a min f f a 2 a f a R a N h,0 a N h,0 is boundd by o(h) if f L 2 (Ω) or boundd by O(h 2 ) if f H 1 (Ω) (s [6]), which guarants th rliability of stimator η G. For th fficincy of th stimator, it is shown in Lmma 3.1 in [6] that ηg, 2 C h R 2 + h R 2, E() E h,γ2 E ω whr E ω dnots th st of innr sids of th patch ω corrsponding to th lmnt. Using th rlation (2.7), w obtain th following rsults. Thorm 3.3 Lt u and u h b th solutions of (1.1) and (1.8), rspctivly, and lt η G, b th stimator (3.3). Thn ηg, 2 C u u h 2 1,ω + λ λ h 2, + h 2 f f 2 ω + h λ h λ h 2. (3.4) E() E h,γ2 This thorm shows th fficincy of gradint rcovry typ stimators η G,. Th inquality (3.4) is comparabl to (2.8). 4 Summary In this papr, w study a postriori rror stimation of finit lmnt mthods for a frictional contact problm, and stablish a compact framwork to driv rliabl rsidual typ and gradint rcovry typ rror stimators by applying a postriori rror analysis for a rlatd linar lliptic problm. Furthrmor, w prov th fficincy of th rror stimators, which was an opn problm statd in [6]. This framwork can also b usd to driv rliabl and fficint a postriori rror stimators for othr variational inqualitis of th scond kind. Acknowldgmnt. W thank th anonymous rfrs for thir valuabl commnts that lad to an improvmnt of th papr. 11
12 Rfrncs [1] M. Ainsworth and T. J. Odn, A Postriori Error Estimation in Finit Elmnt Analysis, Wily, Chichstr, [2] I. Babuška and T. Strouboulis, Th Finit Elmnt Mthod and its Rliability, Oxford Univrsity Prss, [3] S. Bartls and C. Carstnsn, Avraging tchniqus yild rliabl a postriori finit lmnt rror control for obstacl problms, Numr. Math. 99 (2004), [4] V. Bostan and W. Han, Rcovry-basd rror stimation and adaptiv solution of lliptic variational inqualitis of th scond kind, Communications in Mathmatical Scincs 2 (2004), [5] V. Bostan and W. Han, A postriori rror analysis for a contact problm with friction, Computr Mthods in Applid Mchanics and Enginring 195 (2006), [6] V. Bostan and W. Han, Adaptiv finit lmnt solution of variational inqualitis with application in contact problm, in Advancs in Applid Mathmatics and Global Optimization, ds. D. Y. Gao and H. D. Shrali, Springr, Nw York, 2009, [7] V. Bostan, W. Han and B. D. Rddy, A postriori rror stimation and adaptiv solution of lliptic variational inqualitis of th scond kind, Applid Numrical Mathmatics 52 (2004), [8] D. Brass, A postriori rror stimators for obstacl problms anothr look, Numr. Math. 101 (2005), [9] C. Carstnsn, Quasi-intrpolation and a postriori rror analysis in finit lmnt mthods, RAIRO Math. Modl. Num. 33 (1999), [10] Z. Chn and R. H. Nochtto, Rsidual typ a postriori rror stimats for lliptic obstacl problms, Numr. Math. 84 (2000), [11] G. Duvaut and J.-L. Lions, Inqualitis in Mchanics and Physics, Springr-Vrlag, Brlin, [12] R. Glowinski, Numrical Mthods for Nonlinar Variational Problms, Springr-Vrlag, Nw York, 1984 [13] R. ornhubr, A postriori rror stimats for lliptic variational inqualitis, Comput. Math. Appl. 31 (1996),
13 [14] R. H. Nochtto,. G. Sibrt and A. Vsr, Pointwis a postriori rror control for lliptic obstacl problm, Numr. Math. 95 (2003), [15] A. Vsr, Efficint and rliabl a postriori rror stimators for lliptic obstacl problms, SIAM J. Numr. Anal. 39 (2001), [16] R. Vrfürth, A Rviw of a Postriori Error Estimation and Adaptiv Msh-rfinmnt Tchniqus, Wily-Tubur, [17] N. Yan, A postriori rror stimators of gradint rcovry typ for lliptic obstacl problms, Adv. Comput. Math. 15 (2001),
RELIABLE AND EFFICIENT A POSTERIORI ERROR ESTIMATES OF DG METHODS FOR A SIMPLIFIED FRICTIONAL CONTACT PROBLEM
INTERNATIONAL JOURNAL OF NUMERICAL ANALYSIS AND MODELING Volum 16, Numbr 1, Pags 49 62 c 2019 Institut for Scintific Computing and Information RELIABLE AND EFFICIENT A POSTERIORI ERROR ESTIMATES OF DG
More informationDerangements and Applications
2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir
More informationarxiv: v1 [math.na] 3 Mar 2016
MATHEMATICS OF COMPUTATION Volum 00, Numbr 0, Pags 000 000 S 0025-5718(XX)0000-0 arxiv:1603.01024v1 [math.na] 3 Mar 2016 RESIDUAL-BASED A POSTERIORI ERROR ESTIMATE FOR INTERFACE PROBLEMS: NONCONFORMING
More informationUNIFIED A POSTERIORI ERROR ESTIMATOR FOR FINITE ELEMENT METHODS FOR THE STOKES EQUATIONS
UNIFIED A POSTERIORI ERROR ESTIMATOR FOR FINITE ELEMENT METHODS FOR THE STOKES EQUATIONS JUNPING WANG, YANQIU WANG, AND XIU YE Abstract. This papr is concrnd with rsidual typ a postriori rror stimators
More informationA Weakly Over-Penalized Non-Symmetric Interior Penalty Method
Europan Socity of Computational Mthods in Scincs and Enginring (ESCMSE Journal of Numrical Analysis, Industrial and Applid Mathmatics (JNAIAM vol.?, no.?, 2007, pp.?-? ISSN 1790 8140 A Wakly Ovr-Pnalizd
More information1 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 informationIntroduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013
18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:
More informationHomotopy 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 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 informationRECOVERY-BASED ERROR ESTIMATORS FOR INTERFACE PROBLEMS: MIXED AND NONCONFORMING FINITE ELEMENTS
SIAM J. NUMER. ANAL. Vol. 48 No. 1 pp. 30 52 c 2010 Socity for Industrial Applid Mathmatics RECOVERY-BASED ERROR ESTIMATORS FOR INTERFACE PROBLEMS: MIXED AND NONCONFORMING FINITE ELEMENTS ZHIQIANG CAI
More informationThe 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 informationDeift/Zhou Steepest descent, Part I
Lctur 9 Dift/Zhou Stpst dscnt, Part I W now focus on th cas of orthogonal polynomials for th wight w(x) = NV (x), V (x) = t x2 2 + x4 4. Sinc th wight dpnds on th paramtr N N w will writ π n,n, a n,n,
More informationThe 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 informationBINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES
BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit
More informationInference Methods for Stochastic Volatility Models
Intrnational Mathmatical Forum, Vol 8, 03, no 8, 369-375 Infrnc Mthods for Stochastic Volatility Modls Maddalna Cavicchioli Cá Foscari Univrsity of Vnic Advancd School of Economics Cannargio 3, Vnic, Italy
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 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 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 informationc 2009 Society for Industrial and Applied Mathematics
SIAM J. NUMER. ANAL. Vol. 47 No. 3 pp. 2132 2156 c 2009 Socity for Industrial and Applid Mathmatics RECOVERY-BASED ERROR ESTIMATOR FOR INTERFACE PROBLEMS: CONFORMING LINEAR ELEMENTS ZHIQIANG CAI AND SHUN
More informationConstruction 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 informationSymmetric Interior Penalty Galerkin Method for Elliptic Problems
Symmtric Intrior Pnalty Galrkin Mthod for Elliptic Problms Ykatrina Epshtyn and Béatric Rivièr Dpartmnt of Mathmatics, Univrsity of Pittsburgh, 3 Thackray, Pittsburgh, PA 56, U.S.A. Abstract This papr
More informationInstitut für Mathematik
U n i v r s i t ä t A u g s b u r g Institut für Mathmatik Ditrich Brass, Ronald H.W. Hopp, and Joachim Schöbrl A Postriori Estimators for Obstacl Problms by th Hyprcircl Mthod Prprint Nr. 02/2008 23.
More informationAn interior penalty method for a two dimensional curl-curl and grad-div problem
ANZIAM J. 50 (CTAC2008) pp.c947 C975, 2009 C947 An intrior pnalty mthod for a two dimnsional curl-curl and grad-div problm S. C. Brnnr 1 J. Cui 2 L.-Y. Sung 3 (Rcivd 30 Octobr 2008; rvisd 30 April 2009)
More informationBINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES. 1. Statement of results
BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim and n a positiv intgr, lt ν p (n dnot th xponnt of p in n, and u p (n n/p νp(n th unit part of n. If α
More informationOn the irreducibility of some polynomials in two variables
ACTA ARITHMETICA LXXXII.3 (1997) On th irrducibility of som polynomials in two variabls by B. Brindza and Á. Pintér (Dbrcn) To th mmory of Paul Erdős Lt f(x) and g(y ) b polynomials with intgral cofficints
More informationc 2007 Society for Industrial and Applied Mathematics
SIAM J. NUMER. ANAL. Vol. 45, No. 3, pp. 1269 1286 c 2007 Socity for Industrial and Applid Mathmatics NEW FINITE ELEMENT METHODS IN COMPUTATIONAL FLUID DYNAMICS BY H (DIV) ELEMENTS JUNPING WANG AND XIU
More informationSCHUR S THEOREM REU SUMMER 2005
SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation
More informationA Family of Discontinuous Galerkin Finite Elements for the Reissner Mindlin plate
A Family of Discontinuous Galrkin Finit Elmnts for th Rissnr Mindlin plat Douglas N. Arnold Franco Brzzi L. Donatlla Marini Sptmbr 28, 2003 Abstract W dvlop a family of locking-fr lmnts for th Rissnr Mindlin
More informationApplication of Vague Soft Sets in students evaluation
Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt
More informationPROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS
Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra
More information3 Finite Element Parametric Geometry
3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,
More informationCOUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM
COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM Jim Brown Dpartmnt of Mathmatical Scincs, Clmson Univrsity, Clmson, SC 9634, USA jimlb@g.clmson.du Robrt Cass Dpartmnt of Mathmatics,
More informationChapter 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 informationL ubomír Baňas 1 and Robert Nürnberg Introduction A POSTERIORI ESTIMATES FOR THE CAHN HILLIARD EQUATION WITH OBSTACLE FREE ENERGY
ESAIM: MAN 43 (009) 1003 106 DOI: 10.1051/man/009015 ESAIM: Mathmatical Modlling and Numrical Analysis www.saim-man.org A POSERIORI ESIMAES FOR HE CAHN HILLIARD EQUAION WIH OBSACLE FREE ENERGY L ubomír
More informationA posteriori estimators for obstacle problems by the hypercircle method
Computing and Visualization in Scinc manuscript No. (will b insrtd by th ditor) A postriori stimators for obstacl problms by th hyprcircl mthod Ditrich Brass, Ronald H.W. Hopp 2,3, and Joachim Schöbrl
More informationProperties of Phase Space Wavefunctions and Eigenvalue Equation of Momentum Dispersion Operator
Proprtis of Phas Spac Wavfunctions and Eignvalu Equation of Momntum Disprsion Oprator Ravo Tokiniaina Ranaivoson 1, Raolina Andriambololona 2, Hanitriarivo Rakotoson 3 raolinasp@yahoo.fr 1 ;jacqulinraolina@hotmail.com
More informationOn spanning trees and cycles of multicolored point sets with few intersections
On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W
More informationData Assimilation 1. Alan O Neill National Centre for Earth Observation UK
Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal
More informationON A SECOND ORDER RATIONAL DIFFERENCE EQUATION
Hacttp Journal of Mathmatics and Statistics Volum 41(6) (2012), 867 874 ON A SECOND ORDER RATIONAL DIFFERENCE EQUATION Nourssadat Touafk Rcivd 06:07:2011 : Accptd 26:12:2011 Abstract In this papr, w invstigat
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 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationA POSTERIORI ERROR ESTIMATION FOR AN INTERIOR PENALTY TYPE METHOD EMPLOYING H(DIV) ELEMENTS FOR THE STOKES EQUATIONS
A POSTERIORI ERROR ESTIMATION FOR AN INTERIOR PENALTY TYPE METHOD EMPLOYING H(DIV) ELEMENTS FOR THE STOKES EQUATIONS JUNPING WANG, YANQIU WANG, AND XIU YE Abstract. This papr stablishs a postriori rror
More informationLINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM
Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL
More informationDifference -Analytical Method of The One-Dimensional Convection-Diffusion Equation
Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing
More informationCPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming
CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of
More informationNEW 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 information1 Minimum Cut Problem
CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms
More informationA LOCALLY DIVERGENCE-FREE INTERIOR PENALTY METHOD FOR TWO-DIMENSIONAL CURL-CURL PROBLEMS
A LOCALLY DIVERGENCE-FREE INTERIOR PENALTY METHOD FOR TWO-DIMENSIONAL CURL-CURL PROBLEMS SUSANNE C. BRENNER, FENGYAN LI, AND LI-YENG SUNG Abstract. An intrior pnalty mthod for crtain two-dimnsional curl-curl
More informationH(curl; Ω) : n v = n
A LOCALLY DIVERGENCE-FREE INTERIOR PENALTY METHOD FOR TWO-DIMENSIONAL CURL-CURL PROBLEMS SUSANNE C. BRENNER, FENGYAN LI, AND LI-YENG SUNG Abstract. An intrior pnalty mthod for crtain two-dimnsional curl-curl
More informationFourier 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 informationAnalysis of a Discontinuous Finite Element Method for the Coupled Stokes and Darcy Problems
Journal of Scintific Computing, Volums and 3, Jun 005 ( 005) DOI: 0.007/s095-004-447-3 Analysis of a Discontinuous Finit Elmnt Mthod for th Coupld Stoks and Darcy Problms Béatric Rivièr Rcivd July 8, 003;
More information(Upside-Down o Direct Rotation) β - Numbers
Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg
More informationABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS
Novi Sad J. Math. Vol. 45, No. 1, 2015, 201-206 ABEL TYPE THEOREMS FOR THE WAVELET TRANSFORM THROUGH THE QUASIASYMPTOTIC BOUNDEDNESS Mirjana Vuković 1 and Ivana Zubac 2 Ddicatd to Acadmician Bogoljub Stanković
More informationCramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter
WHEN THE CRAMÉR-RAO INEQUALITY PROVIDES NO INFORMATION STEVEN J. MILLER Abstract. W invstigat a on-paramtr family of probability dnsitis (rlatd to th Parto distribution, which dscribs many natural phnomna)
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 informationRecall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1
Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1
More informationDiscontinuous Galerkin and Mimetic Finite Difference Methods for Coupled Stokes-Darcy Flows on Polygonal and Polyhedral Grids
Discontinuous Galrkin and Mimtic Finit Diffrnc Mthods for Coupld Stoks-Darcy Flows on Polygonal and Polyhdral Grids Konstantin Lipnikov Danail Vassilv Ivan Yotov Abstract W study locally mass consrvativ
More informationAPPROXIMATION THEORY, II ACADEMIC PRfSS. INC. New York San Francioco London. J. T. aden
Rprintd trom; APPROXIMATION THORY, II 1976 ACADMIC PRfSS. INC. Nw York San Francioco London \st. I IITBRID FINIT L}ffiNT }ffithods J. T. adn Som nw tchniqus for dtrmining rror stimats for so-calld hybrid
More informationSupplementary Materials
6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic
More informationRational Approximation for the one-dimensional Bratu Equation
Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in
More informationLimiting value of higher Mahler measure
Limiting valu of highr Mahlr masur Arunabha Biswas a, Chris Monico a, a Dpartmnt of Mathmatics & Statistics, Txas Tch Univrsity, Lubbock, TX 7949, USA Abstract W considr th k-highr Mahlr masur m k P )
More informationON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS
INTEGERS: ELECTRONIC JOURNAL OF COMBINATORIAL NUMBER THEORY 8 2008, #A3 ON THE DISTRIBUTION OF THE ELLIPTIC SUBSET SUM GENERATOR OF PSEUDORANDOM NUMBERS Edwin D. El-Mahassni Dpartmnt of Computing, Macquari
More informationA LOCALLY CONSERVATIVE LDG METHOD FOR THE INCOMPRESSIBLE NAVIER-STOKES EQUATIONS
A LOCALLY CONSERVATIVE LDG METHOD FOR THE INCOMPRESSIBLE NAVIER-STOES EQUATIONS BERNARDO COCBURN, GUIDO ANSCHAT, AND DOMINI SCHÖTZAU Abstract. In this papr, a nw local discontinuous Galrkin mthod for th
More informationME469A Numerical Methods for Fluid Mechanics
ME469A Numrical Mthods for Fluid Mchanics Handout #5 Gianluca Iaccarino Finit Volum Mthods Last tim w introducd th FV mthod as a discrtization tchniqu applid to th intgral form of th govrning quations
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 informationA Family of Discontinuous Galerkin Finite Elements for the Reissner Mindlin Plate
Journal of Scintific Computing, Volums 22 and 23, Jun 2005 ( 2005) DOI: 10.1007/s10915-004-4134-8 A Family of Discontinuous Galrkin Finit Elmnts for th Rissnr Mindlin Plat Douglas N. Arnold, 1 Franco Brzzi,
More informationA generalized attack on RSA type cryptosystems
A gnralizd attack on RSA typ cryptosystms Martin Bundr, Abdrrahman Nitaj, Willy Susilo, Josph Tonin Abstract Lt N = pq b an RSA modulus with unknown factorization. Som variants of th RSA cryptosystm, such
More informationA Propagating Wave Packet Group Velocity Dispersion
Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to
More informationLegendre Wavelets for Systems of Fredholm Integral Equations of the Second Kind
World Applid Scincs Journal 9 (9): 8-, ISSN 88-495 IDOSI Publications, Lgndr Wavlts for Systs of Frdhol Intgral Equations of th Scond Kind a,b tb (t)= a, a,b a R, a. J. Biazar and H. Ebrahii Dpartnt of
More informationSymmetric Interior penalty discontinuous Galerkin methods for elliptic problems in polygons
Symmtric Intrior pnalty discontinuous Galrkin mthods for lliptic problms in polygons F. Müllr and D. Schötzau and Ch. Schwab Rsarch Rport No. 2017-15 March 2017 Sminar für Angwandt Mathmatik Eidgnössisch
More informationFunction Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0
unction Spacs Prrquisit: Sction 4.7, Coordinatization n this sction, w apply th tchniqus of Chaptr 4 to vctor spacs whos lmnts ar functions. Th vctor spacs P n and P ar familiar xampls of such spacs. Othr
More informationAbstract Interpretation. Lecture 5. Profs. Aiken, Barrett & Dill CS 357 Lecture 5 1
Abstract Intrprtation 1 History On brakthrough papr Cousot & Cousot 77 (?) Inspird by Dataflow analysis Dnotational smantics Enthusiastically mbracd by th community At last th functional community... At
More informationMapping properties of the elliptic maximal function
Rv. Mat. Ibroamricana 19 (2003), 221 234 Mapping proprtis of th lliptic maximal function M. Burak Erdoğan Abstract W prov that th lliptic maximal function maps th Sobolv spac W 4,η (R 2 )intol 4 (R 2 )
More informationAddition of angular momentum
Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat
More informationA ROBUST NONCONFORMING H 2 -ELEMENT
MAHEMAICS OF COMPUAION Volum 70, Numbr 234, Pags 489 505 S 0025-5718(00)01230-8 Articl lctronically publishd on Fbruary 23, 2000 A ROBUS NONCONFORMING H 2 -ELEMEN RYGVE K. NILSSEN, XUE-CHENG AI, AND RAGNAR
More informationTwo Products Manufacturer s Production Decisions with Carbon Constraint
Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint
More informationElements of Statistical Thermodynamics
24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,
More informationMutually Independent Hamiltonian Cycles of Pancake Networks
Mutually Indpndnt Hamiltonian Cycls of Pancak Ntworks Chng-Kuan Lin Dpartmnt of Mathmatics National Cntral Univrsity, Chung-Li, Taiwan 00, R O C discipl@ms0urlcomtw Hua-Min Huang Dpartmnt of Mathmatics
More informationFinding low cost TSP and 2-matching solutions using certain half integer subtour vertices
Finding low cost TSP and 2-matching solutions using crtain half intgr subtour vrtics Sylvia Boyd and Robrt Carr Novmbr 996 Introduction Givn th complt graph K n = (V, E) on n nods with dg costs c R E,
More informationA Simple Formula for the Hilbert Metric with Respect to a Sub-Gaussian Cone
mathmatics Articl A Simpl Formula for th Hilbrt Mtric with Rspct to a Sub-Gaussian Con Stéphan Chrétin 1, * and Juan-Pablo Ortga 2 1 National Physical Laboratory, Hampton Road, Tddinton TW11 0LW, UK 2
More informationEXISTENCE OF POSITIVE ENTIRE RADIAL SOLUTIONS TO A (k 1, k 2 )-HESSIAN SYSTEMS WITH CONVECTION TERMS
Elctronic Journal of Diffrntial Equations, Vol. 26 (26, No. 272, pp. 8. ISSN: 72-669. URL: http://jd.math.txstat.du or http://jd.math.unt.du EXISTENCE OF POSITIVE ENTIRE RADIAL SOLUTIONS TO A (k, k 2 -HESSIAN
More informationA SPLITTING METHOD USING DISCONTINUOUS GALERKIN FOR THE TRANSIENT INCOMPRESSIBLE NAVIER-STOKES EQUATIONS
ESAIM: MAN Vol. 39, N o 6, 005, pp. 5 47 DOI: 0.05/man:005048 ESAIM: Mathmatical Modlling and Numrical Analysis A SPLITTING METHOD USING DISCONTINUOUS GALERKIN FOR THE TRANSIENT INCOMPRESSIBLE NAVIER-STOKES
More informationMORTAR ADAPTIVITY IN MIXED METHODS FOR FLOW IN POROUS MEDIA
INTERNATIONAL JOURNAL OF NUMERICAL ANALYSIS AND MODELING Volum 2, Numbr 3, Pags 241 282 c 25 Institut for Scintific Computing and Information MORTAR ADAPTIVITY IN MIXED METHODS FOR FLOW IN POROUS MEDIA
More informationProcdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is
Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,
More informationOn the number of pairs of positive integers x,y H such that x 2 +y 2 +1, x 2 +y 2 +2 are square-free
arxiv:90.04838v [math.nt] 5 Jan 09 On th numbr of pairs of positiv intgrs x,y H such that x +y +, x +y + ar squar-fr S. I. Dimitrov Abstract In th prsnt papr w show that thr xist infinitly many conscutiv
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 informationDevelopments in Geomathematics 5
~~": ~ L " r. :.. ~,.!.-. r,:... I Rprintd from I Dvlopmnts in Gomathmatics 5 Procdings of th Intrnational Symposium on Variational Mthods in ' Goscincs hld at th Univrsity of Oklahoma, Norman, Oklahoma,
More informationNumerische Mathematik
Numr. Math. 04 6:3 360 DOI 0.007/s00-03-0563-3 Numrisch Mathmatik Discontinuous Galrkin and mimtic finit diffrnc mthods for coupld Stoks Darcy flows on polygonal and polyhdral grids Konstantin Lipnikov
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 informationExponential inequalities and the law of the iterated logarithm in the unbounded forecasting game
Ann Inst Stat Math (01 64:615 63 DOI 101007/s10463-010-03-5 Exponntial inqualitis and th law of th itratd logarithm in th unboundd forcasting gam Shin-ichiro Takazawa Rcivd: 14 Dcmbr 009 / Rvisd: 5 Octobr
More informationNONCONFORMING FINITE ELEMENTS FOR REISSNER-MINDLIN PLATES
NONCONFORMING FINITE ELEMENTS FOR REISSNER-MINDLIN PLATES C. CHINOSI Dipartimnto di Scinz Tcnologi Avanzat, Univrsità dl Pimont Orintal, Via Bllini 5/G, 5 Alssandria, Italy E-mail: chinosi@mfn.unipmn.it
More information16. Electromagnetics and vector elements (draft, under construction)
16. Elctromagntics (draft)... 1 16.1 Introduction... 1 16.2 Paramtric coordinats... 2 16.3 Edg Basd (Vctor) Finit Elmnts... 4 16.4 Whitny vctor lmnts... 5 16.5 Wak Form... 8 16.6 Vctor lmnt matrics...
More informationSOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.
SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. K VASUDEVAN, K. SWATHY AND K. MANIKANDAN 1 Dpartmnt of Mathmatics, Prsidncy Collg, Chnnai-05, India. E-Mail:vasu k dvan@yahoo.com. 2,
More informationUNIFIED ERROR ANALYSIS
UNIFIED ERROR ANALYSIS LONG CHEN CONTENTS 1. Lax Equivalnc Torm 1 2. Abstract Error Analysis 2 3. Application: Finit Diffrnc Mtods 4 4. Application: Finit Elmnt Mtods 4 5. Application: Conforming Discrtization
More informationInternational Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN
Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan
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 informationMath 102. Rumbos Spring Solutions to Assignment #8. Solution: The matrix, A, corresponding to the system in (1) is
Math 12. Rumbos Spring 218 1 Solutions to Assignmnt #8 1. Construct a fundamntal matrix for th systm { ẋ 2y ẏ x + y. (1 Solution: Th matrix, A, corrsponding to th systm in (1 is 2 A. (2 1 1 Th charactristic
More informationJournal of Computational and Applied Mathematics. An adaptive discontinuous finite volume method for elliptic problems
Journal of Computational and Applid Matmatics 235 (2011) 5422 5431 Contnts lists availabl at ScincDirct Journal of Computational and Applid Matmatics journal ompag: www.lsvir.com/locat/cam An adaptiv discontinuous
More informationc 2005 Society for Industrial and Applied Mathematics
SIAM J. NUMER. ANAL. Vol. 43, No. 4, pp. 1728 1749 c 25 Socity for Industrial and Applid Mathmatics SUPERCONVERGENCE OF THE VELOCITY IN MIMETIC FINITE DIFFERENCE METHODS ON QUADRILATERALS M. BERNDT, K.
More informationEEO 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 informationA UNIFIED A POSTERIORI ERROR ESTIMATOR FOR FINITE VOLUME METHODS FOR THE STOKES EQUATIONS
A UNIFIED A POSTERIORI ERROR ESTIMATOR FOR FINITE VOLUME METHODS FOR THE STOKES EQUATIONS JUNPING WANG, YANQIU WANG, AND XIU YE Abstract. In tis papr, t autors stablisd a unifid framwork for driving and
More information