PARALEL PREDICTOR-CORRECTOR SCHEMES FOR PARABOLIC PROBLEMS ON GRAPHS
|
|
- Ethan Wade
- 5 years ago
- Views:
Transcription
1 COMPUTATIONAL METHODS IN APPLIED MATHEMATICS, Vol. 10(2010, No. 3, pp c 2010 Istitute of Matematics of te Natioal Academy of Scieces of Belarus PARALEL PREDICTOR-CORRECTOR SCHEMES FOR PARABOLIC PROBLEMS ON GRAPHS R.ČIEGIS1 AND N.TUMANOVA 1 Abstract We cosider a predictor-corrector type fiite differece sceme for solvig oe-dimesioal parabolic problems. Tis algoritm decouples computatios o differet subdomais ad tus ca be efficietly implemeted o parallel computers ad used to solve problems o grap structures. Te stability ad covergece of te discrete solutio is proved i te special eergy ad maximum orms. Te results of computatioal experimets are preseted Matematics Subject Classificatio: 65N20; 65M55. Keywords: parabolic problem, braced structures, fiite differece metod, predictor corrector algoritm, stability, covergece, parallel algoritms. 1. Itroductio May applied problems are described by reactio - diffusio equatios o braced structures. Te well-kow examples are give by euro simulatio models based o te Hodgki Huxley (HH reactio diffusio system [4]. I order to describe te fuctioig of te brai we must take ito accout te complex arcitecture of te syaptic coectios betwee euros, te spatial distributio of te membrae caels witi te braced structure of euros, ad te igly oliear electrical properties of te euros. Te amout of computatios eeded to make a matematical model fit experimetal data by explorig exaustively te parameter space grows expoetially wit te umber of parameters. Numerical algoritms for solvig HH type problems were proposed ad ivestigated i [1, 6, 7, 11]. Tey use te fiite differece metod for te approximatio of space derivatives ad apply differet teciques for umerical itegratio i time. I costructig umerical approximatios of reactio-diffusio systems o braced structures, very importat problem arises due to te approximatio of flux coservatio equatios at brac poits. Recetly, te predictor-corrector splittig ad domai decompositio metods ave bee widely used to solve elliptic ad parabolic PDEs i multidimesioal domais [3, 10, 16]. Importat results for domai decompositio metods are described i [5]. A geeral framework for te costructio ad aalysis of various classes of splittig ad domai decompositio algoritms is preseted i [13]. Very iterestig developmets of tese ideas are preseted i [15], were ew domai decompositio metods wit overlappig subdomais are ivestigated. Te mai idea is to coose a simple geeratig sceme for te classical approximatio of te cotiuous problem, te to icrease its stability by addig te regularizatio operator at te secod stage of developig a efficiet discrete sceme. Geeral operator stability coditios [12] ca be used to prove te stability of te ew discrete scemes tat are obtaied. 1 Vilius Gedimias Tecical Uiversity, Saulėtekio al. 11, Vilius, Lituaia. rc@vgtu.lt Uauteticated
2 276 R. Čiegis ad N. Tumaova Suc algoritms are well suited for parallel implemetatio. Similar teciques ca also be used for problems o grap structures (see [11, 14] for related discussios. Equatios o differet edges of te grap are decoupled ad ca be solved i parallel. Parallelizatio of te algoritm is very importat i solvig real-world problems we te amout of computatios icreases, ad te applicatio of parallel algoritms eables us to reduce substatially te CPU time. I tis paper, we cosider predictor ad predictor corrector type fiite differece scemes for solutig parabolic problems. Tese results ca be geeralized to problems o graps quite straigtforwardly. Te mai goal is to ivestigate te stability of te obtaied discrete algoritms wit respect to te approximatio errors itroduced at te predictor step of te algoritm. Stability aalysis i te maximum orm was performed i [2], but oly te coditioal stability ca be proved by tis metod ad o ifluece of te corrector step o te stability is obtaied. I te preset paper, we ave ivestigated te stability of te proposed discrete sceme i te eergy ad maximum orms. For ease of presetatio, we restrict ourselves to a detailed aalysis of oe-dimesioal liear parabolic problems. Te mai goal is to ivestigate te stability of te obtaied discrete algoritms wit respect to te approximatio errors itroduced at te predictor step of te algoritm. Te rest of te paper is orgaized as follows. Te matematical model of a liear parabolic problem ad te predictor-corrector algoritm are preseted i Sectio 2. Te covergece of te discrete solutio i te eergy ad maximum orms is ivestigated i Sectio 3. Some umerical results are preseted i Sectio 4, tey cofirm te obtaied teoretical results. Fially, some coclusios are give i Sectio Problem formulatio We cosider a oe-dimesioal liear parabolic problem u t = ( a(x u x x 0 < a 0 a(x a M, q(x 0, u(x,0 = u 0 (x, 0 x 1, q(xu(x,t+f(x,t, 0 < x < 1, t > 0, (2.1 u(0,t = µ L (t, u(1,t = µ R (t, 0 < t T Predictor corrector discrete sceme We costruct uiform grids for te x ad t variables, respectively, ω = {x j : x j = j, j = 1,...,N 1}, = 1/N, ω = ω {x 0,x N }, ω τ = {t : t = τ, = 0,...,N, Nτ = T}. O ω ω τ wedefietediscretefuctiou j = U(x j,t approximatigtesolutiou(x j,t at time t. Te backward time, te forward ad backward space differece quotiets wit respect to t ad x are defied by U t = U U 1, x Uj = U j+1 Uj τ, x Uj = U j Uj 1. Uauteticated
3 Parallel Predictor-corrector Scemes for Parabolic Problems o Graps 277 Let U, V be grid fuctios, te we defie te discrete ier product (U,V, te discrete L 2 orm U, ad te discrete H 1 semiorm U b by J 1 (U,V = U j V j, U = (U,U, U 2 b = j=1 J ( 2, b j 1/2 x U j j=1 were b(x is a give positive fuctio b(x > 0, x [0,1]. Recetly, te predictor-corrector splittig ad domai decompositio metods ave bee widely used to solve elliptic ad parabolic PDEs i multidimesioal regios ad o grap structures (see [11, 14] for related discussios. Te preseted algoritm is based o te stadard decompositio of te problem ito simple 1D problems o eac edge. New values of te solutio at brac poits are predicted by usig a explicit algoritm. I order to improve te stability of te domai decompositio algoritms, a ew approac was proposed i [9]. Te mai idea is to drop te values of te solutio at te iterface of two domais computed by te predictor algoritm ad compute ew values by usig te basic implicit discrete algoritm (correctio step. We ote tat predictor-corrector splittig fits well wit te geeral framework from [15], sice te predictor step implemeted as te explicit Euler algoritm ca be take as a geeratig sceme, ad te implicit Euler sceme at te corrector step ca be regarded as a regularized algoritm i tis framework. Problem (2.1 is approximated by te followig sceme. First, te domai Ω = [0,1] is divided ito K subdomais Ω = K Ω k, Ωk = [l k 1,l k ], l 0 = 0, l K = 1. I accordace wit tis domai decompositio, te space grid is decomposed ito subgrids ω = K ω k, were ω k = {x j : x j = j, j = j k 1,...,j k }, x = l k. Predictor step. First, we compute i parallel te ew values of te solutio at te boudary poits of te subdomais. Te explicit-implicit Euler approximatio is used to discretize te differetial equatio (2.1: Ũ j k U 1 j k τ = x ( a x U 1 j q k Ũj k +f 1 j k, k = 1,...,K 1. (2.2 Domai decompositio step. Secod, te solutios o eac subdomai are computed i parallel usig te implicit fiite differece sceme (2.3. Te predicted values Ũ j k are used as te iterface boudary coditios. ( U t = x aj+ 1 2 x Uj qj Uj +fj, x j ω, k k = 1,...,K 1, (2.3 U j k 1 = Ũ j k 1, U j k = Ũ j k, U 0 = µ L (t, U J = µ R (t. Uauteticated
4 278 R. Čiegis ad N. Tumaova Corrector step. Tird, usig te implicit fiite differece sceme (2.3 ad takig te solutio U computed at te secod step, we update i parallel te values of te solutio at te boudary poits of te subdomais Uj k, t = x( a + 1 x Uj q Uj k +fj k, k = 1,...,K 1. (2.4 Our goal is to ivestigate te stability ad te accuracy of te discrete algoritm. 3. Covergece aalysis Let us deote te error fuctios of te discrete solutio as Zj = Uj u(x j,t, Z j = Ũj u(x j,t, x j ω. By puttig tem ito te fiite-differece sceme we get a discrete problem for te error fuctios Zj, t = x( aj+ 1 2 x Zj qj Z j +ψ j, x j ω \{x ±1, k = 1,...,K 1}, (3.1 Zj k ±1, t = x( a ± x Zj k ±1 q ±1Zj k ±1 +a ± 1 2 Z j k Z 1 j k τ Z j k Z j k 2 +ψ j k ±1, (3.2 ( = x a + 1 x Z 1 j q Z ++ϕ j k, k = 1,...,K 1, (3.3 Z 0 = 0, Z J = 0, Z 0 j = 0, j = 0,...,J, (3.4 were ψ ad ϕ are te trucatio errors of te implicit ad explicit-implicit Euler scemes ψj = u + x( ( j, t aj+ 1 2 x uj qj u j +fj, ϕ j = u j, t + x aj+ 1 x u 1 j qj u j +f 1 j. 2 Let us assume tat te iitial data, te coefficiets, ad te exact solutio of problem (2.1 are smoot eoug. Usig te Taylor formula, we ca eatimate te trucatio errors of te fiite differece sceme (2.2 (2.4 as ψ j C(τ + 2, 1 j J, ϕ j k ψ j k Cτ, 1 k < K. (3.5 Next, we ivestigate te stability of te discrete solutio of te fiite differece sceme (2.2 ( Stability i H 1 Ourstabilityaalysisusesteresultsof[14]. Letā = (a 1/2+a +1/2/2, k = 1,...,K 1. Lemma 3.1. Let Z satisfy problem (3.1 (3.4. Te E E 0 +τ l=1 { K ψl 2 + [ 2τ olds, were te fuctioal E is defied as E = Z 2 a + qz 2 + 2τ2 ( a ā (ψl j k M (K 1τ + (ϕ l a 0 2 j ψj l 2 k ]}, (3.6 K 1 ā 1+τq ( x (a 1/2 x Z j k 2. Uauteticated
5 Parallel Predictor-corrector Scemes for Parabolic Problems o Graps 279 Proof. Multiplyig equatios (3.1 (3.2, respectively, by 2τ tz j, j = 1,...,J 1 ad addig te resultig equalities, we get 2τ tz 2 = 2τ ( ( tz, x aj 1 Z 2 x j 2τ + K 1 ( Z j k Zj k (a 1 tz j 1 +a + 2 tz 1 j k +1 2τ ( qz, tz +2τ ( ψ, tz. (3.7 Applyig equality 2Z = Z +Z 1 +τ tz ad te well-kow formula of summatio by parts, we obtai 2τ ( ( tz, x aj 1 Z 2 x j = Z 2 a + Z 1 2 a τ 2 tz 2 a, (3.8 2τ ( qz, tz = qz 2 qz 1 2 +τ 2 q tz 2. (3.9 Usig te Scwarz iequality ad te ε iequality, we ave 2τ ( ψ, tz 2τ tz 2 + τ 2 ψ 2. (3.10 It remais to estimate te error itroduced at te predictor step. From (3.1, (3.3 it follows tat We ote tat (1+τq ( Z j k Z j k = τ 2 t x ( a 1 2 x Z j k +τ(ϕ ψ j k. ( a 1 tz j 1 +a + 1 tz j +1 = 2 t x a 2 x 1 Zj +2ā k tz j k ( ( ( = 2 t x a 1 x Zj +2ā x a 1 x Zj +ψ. Applyig te Scwarz iequality, te ε iequality, ad te a priori estimate q j 0, we get te followig estimates: T 1 = 2τ3 ( ( t x a 1+τq 1 x Zj 2, T 2 = 4τ3 ā (1+τq ( ( x a 2 x 1 Zj k t x a 1 x Zj = 2τ2 ā (1+τq ( ( x ( a 2 x 1 Zj 2 ( ( k x a 1 x Z ( 1 2 ( j +τ 2 t x a 1 x Zj 2, T 3 = 4τ3 ā (1+τq t ( x a 1 x Zj ψ 2τ4 ā [ ( ] t x a (1+τq 1 x Zj 2 2τ 2 ā ( + ψ 2, T 4 = 2τ2 ( t x a 1+τq 1 x Zj (ϕ ψj k 2τ3 ( ( t x a 1+τq 1 x Zj 2 τ( + ϕ 2. 2 ψj k Now we will estimate te last term i a differet way ta it was doe i [14]. Te followig imbeddig teorem Z j 1 2 a 0 Z a is used. Te we obtai T 5 = 4τ2 ā (1+τq (ϕ j k ψj k tz j k 4τ2 a M ϕ j k ψ j k tz j k τ2 K 1 tz 2 a + a2 M (K 1τ2( ϕ 2. a 0 2 ψj k Uauteticated
6 280 R. Čiegis ad N. Tumaova Substitutig (3.8 (3.10 ito (3.7 ad usig te resultig iequalities T m, m = 1,...,5, we obtai E E 1 +τ{ 1 2 ψ 2 + K 1 [ 2τ Repeated applicatio yields te desired result (3.6. ( a ā (ψ j k M (K 1τ + (ϕ a 0 2 j ψj 2 k ]}. Remark 3.1. It follows from Lemma 3.1 tat te fiite differece sceme (2.2 (2.4 is ucoditioally A-stable. Note tat i [14] oly te ρ-stability wit ρ = 1+cτ was proved. Usig te stability estimate give i Lemma 3.1 ad te estimates of te trucatio errors (3.5, we get te followig covergece result i te H 1 orm. Teorem 1. Let U be te solutio of te fiite differece sceme (2.2 (2.4 ad u(x, t be te solutio of te differetial problem (2.1. Te 3.2. Stability i L U u a Ct ( τ τ τ. (3.11 I tis sectio, we ivestigate te asymptotic optimality of te error estimate (3.11. For simplicity of otatios, we restrict ourselves to te case K = 1 ad assume tat a(x 1, q(x = 0. Let us deote m = j 1 ad defie g = max 1 N max x j ω ψ j, g = max 1 N ϕ m ψ m, G = g +g. Te we cosider te statioary aalogue of te predictor-corrector algoritm x x W j = g, 1 j < m, W 0 = 0, Wm p = W m, x x W j = g, m < j < J, Wm p = W m, W J = 0, (3.12 W m W m τ = x x W m +G, x x W m = g, j = m. Te solutio of (3.12 ca be writte i explicit form A x j + g x m 2 x j(1 x j, 0 j m, W j = A 1 x j + g 1 x m 2 x j(1 x j, m < j J, We see tat te fuctio W is bouded by W j C (τ τ2, A = 2τ(x m x 2 m /2 ad tis estimate predicts a better covergece rate ta it follows from te a priori error estimate (3.11. g. Uauteticated
7 Parallel Predictor-corrector Scemes for Parabolic Problems o Graps Numerical experimets We ave applied te developed fiite differece sceme (2.2 (2.4 to te model problem (2.1, were we take T = 1 ad te followig coefficiets a(x 1, q(x = 0. Te source term f is cose suc tat te exact solutio is give by u = exp(texp(2x. Te computatioal domai is decomposed ito four subdomais at poits l 1 = 0.25, l 2 = 0.5, l 3 = 0.8. I te umerical experimets we ave tested te covergece of te algoritm for differet values of ad τ. Te error of te solutio is preseted i te uiform orm Te results are give i Table 4.1. Z N = max 1 j<j UN j u(x j,t. Table 4.1. Error of te solutio of te predictor corrector sceme at T = 1 N τ = 0.02 τ = 0.01 τ = τ = τ = Te results sow tat te global error i most cases coverges as O(τ 2 /, i.e., te error itroduced at te predictio step domiates te total error. It follows from Teorem 1 tat te predictor corrector sceme is ucoditioally stable wit respect to te iitial coditio i te eergy orm, i.e., E for te test problem 3 E = Z 2 a ++ 2τ2 ( 2. x x Zj k E 1 for > 0, were 1500 = 0.01, tau= 0.01 = 0.005, tau=0.005 = 0.005, tau = t Fig Dyamics of te error Z i time Uauteticated
8 282 R. Čiegis ad N. Tumaova But i te case of oliear problems we are iterested to get error estimates also i te uiform orm. I Fig. 4.1, we plot te dyamics of te error Z i time, we zero iitial coditios are disturbed oly at oe grid poit ZJ/2 0 = 1 ad te source term f Coclusios Te predictor corrector algoritm splits te computatios for eac time step ito a set of discrete oe-dimesioal parabolic problems wic ca be solved efficietly by te stadard factorizatio algoritm. Tis leads to a good parallelism of te algoritm. It is wellkow tat te simple predictio strategy loses te ucoditioal stability of te backward Euler algoritm. By te eergy estimates metod we ave proved tat te predictor-corrector algoritm is ucoditioally stable. Te relatio betwee te space ad time steps is still required i order to get te covergece of te discrete solutio, sice te trucatio error itroduced at te predictio step is of order O(τ 2 /. Ackowledgmets. We are grateful to te aoymous reviewer for te costructive remarks wic eabled us to improve te paper. Refereces 1. R. Cegis, Ivestigatio of differece scemes for a class of models of excitability, Comput. Mats. Mat. Pys., 32 (1992, o. 6, pp R. Čiegis ad N. Tumaova, Fiite-differece scemes for parabolic problems o graps, Lit. Mat. Joural, 50 (2010, o. 2, pp M. Dryja ad X. Tu, A domai decompositio of parabolic problems, Numer. Mat., 107 (2007, pp A. Hodgki ad A. Huxley, A quatitative descriptio of membrae curret ad its applicatio to coductio ad excitatio i erve, J. Pysiol. Lodo, 117 (1952, pp Y. Laevsky, Domai decompositio metods for te solutio of two-dimesioal parabolic equatios, i: Variatioal-differece metods i problems of umerical aalysis., vol. 2, Comp. Cetr. Sib. Brac, USSR Acad. Sci., 1987, pp M. Mascagi, Te backward Euler metod for umerical simulatio of te Hodgki Huxley equatios of erve coductio, SIAM J. Numer. Aal., 27 (1990, pp M. Mascagi, A parallelizig algoritm for computig solutios to arbitrarily braced cable euro models, J. Neurosci. Metods, 36 (1991, pp T. Matew, Domai Decompositio Metods for te Numerical Solutio of Partial Differetial Equatios, Lecture Notes i Computatioal Sciece ad Egieerig 61. Berli: Spriger, H. Qia ad J. Zu, O te efficiet parallel algoritm for solvig time depedet partial differetial equatios, i: Proceedigs of te 1998 Iteratioal Coferece o Parallel ad Distributed Processig Teciques ad Applicatios, CSREA Press, Las Vegas, NV, 1998, pp A. Quarteroi ad A. Valli, Domai Decompositio Metods for Partial Differetial Equatios. Numerical Matematics ad Scietific Computatio, Oxford Uiversity Press, USA, M. Rempe ad D. Copp, A predictor-corrector algoritm for reactio diffusio equatios associated wit eural activity o braced structures, SIAM J. Sci. Comput., 28 (2006, o. 6, pp A. Samarskii, Te Teory of Differece Scemes, Marcel Dekker, Ic., New York Basel, A. Samarskii, P. Matus, ad P. Vabiscevic, Differece Scemes wit Operator Factors, Matematics ad its Applicatios (Dordrect Dordrect: Kluwer Academic Publisers, H. Si ad H. Liao, Ucoditioal stability of corrected explicit-implicit domai decompositio algoritms for parallel approximatio of eat equatios, SIAM J. Numer. Aal., 44 (2006, o. 4, pp P. Vabiscevic, Domai decompositio metods wit overlappig subdomais for te time-depedet problems of matematical pysics, CMAM, 8 (2008, o. 4, pp Y. Zuag ad X. Su, Stabilized explicit implicit domai decompositio metods for te umerical solutio of parabolic equatios, SIAM J. Sci. Comput., 24 (2002, o. 1, pp Uauteticated
Finite Difference Method for the Estimation of a Heat Source Dependent on Time Variable ABSTRACT
Malaysia Joural of Matematical Scieces 6(S): 39-5 () Special Editio of Iteratioal Worsop o Matematical Aalysis (IWOMA) Fiite Differece Metod for te Estimatio of a Heat Source Depedet o Time Variable, Allabere
More informationx x x 2x x N ( ) p NUMERICAL METHODS UNIT-I-SOLUTION OF EQUATIONS AND EIGENVALUE PROBLEMS By Newton-Raphson formula
NUMERICAL METHODS UNIT-I-SOLUTION OF EQUATIONS AND EIGENVALUE PROBLEMS. If g( is cotiuous i [a,b], te uder wat coditio te iterative (or iteratio metod = g( as a uique solutio i [a,b]? '( i [a,b].. Wat
More informationThe Advection-Diffusion equation!
ttp://www.d.edu/~gtryggva/cf-course/! Te Advectio-iffusio equatio! Grétar Tryggvaso! Sprig 3! Navier-Stokes equatios! Summary! u t + u u x + v u y = P ρ x + µ u + u ρ y Hyperbolic part! u x + v y = Elliptic
More informationOn Exact Finite-Difference Scheme for Numerical Solution of Initial Value Problems in Ordinary Differential Equations.
O Exact Fiite-Differece Sceme for Numerical Solutio of Iitial Value Problems i Ordiar Differetial Equatios. Josua Suda, M.Sc. Departmet of Matematical Scieces, Adamawa State Uiversit, Mubi, Nigeria. E-mail:
More informationStability analysis of numerical methods for stochastic systems with additive noise
Stability aalysis of umerical metods for stoctic systems wit additive oise Yosiiro SAITO Abstract Stoctic differetial equatios (SDEs) represet pysical peomea domiated by stoctic processes As for determiistic
More informationA Pseudo Spline Methods for Solving an Initial Value Problem of Ordinary Differential Equation
Joural of Matematics ad Statistics 4 (: 7-, 008 ISSN 549-3644 008 Sciece Publicatios A Pseudo Splie Metods for Solvig a Iitial Value Problem of Ordiary Differetial Equatio B.S. Ogudare ad G.E. Okeca Departmet
More informationOn the convergence, consistence and stability of a standard finite difference scheme
AMERICAN JOURNAL OF SCIENTIFIC AND INDUSTRIAL RESEARCH 2, Sciece Huβ, ttp://www.sciub.org/ajsir ISSN: 253-649X, doi:.525/ajsir.2.2.2.74.78 O te covergece, cosistece ad stabilit of a stadard fiite differece
More informationNUMERICAL SOLUTIONS OF THE FRACTIONAL KdV-BURGERS-KURAMOTO EQUATION
S5 NUMERICAL SOLUTIONS OF THE FRACTIONAL KdV-BURGERS-KURAMOTO EQUATION by Doga KAYA a*, Sema GULBAHAR a, ad Asif YOKUS b a Departmet of Matematics, Istabul Commerce Uiversity, Uskudar, Istabul, Turkey
More informationA NEW CLASS OF 2-STEP RATIONAL MULTISTEP METHODS
Jural Karya Asli Loreka Ahli Matematik Vol. No. (010) page 6-9. Jural Karya Asli Loreka Ahli Matematik A NEW CLASS OF -STEP RATIONAL MULTISTEP METHODS 1 Nazeeruddi Yaacob Teh Yua Yig Norma Alias 1 Departmet
More informationFinite Difference Approximation for First- Order Hyperbolic Partial Differential Equation Arising in Neuronal Variability with Shifts
Iteratioal Joural of Scietific Egieerig ad Research (IJSER) wwwiseri ISSN (Olie): 347-3878, Impact Factor (4): 35 Fiite Differece Approimatio for First- Order Hyperbolic Partial Differetial Equatio Arisig
More informationME 501A Seminar in Engineering Analysis Page 1
Accurac, Stabilit ad Sstems of Equatios November 0, 07 Numerical Solutios of Ordiar Differetial Equatios Accurac, Stabilit ad Sstems of Equatios Larr Caretto Mecaical Egieerig 0AB Semiar i Egieerig Aalsis
More informationNumerical Method for Blasius Equation on an infinite Interval
Numerical Method for Blasius Equatio o a ifiite Iterval Alexader I. Zadori Omsk departmet of Sobolev Mathematics Istitute of Siberia Brach of Russia Academy of Scieces, Russia zadori@iitam.omsk.et.ru 1
More informationNumerical Solution of the Two Point Boundary Value Problems By Using Wavelet Bases of Hermite Cubic Spline Wavelets
Australia Joural of Basic ad Applied Scieces, 5(): 98-5, ISSN 99-878 Numerical Solutio of the Two Poit Boudary Value Problems By Usig Wavelet Bases of Hermite Cubic Splie Wavelets Mehdi Yousefi, Hesam-Aldie
More informationTHE ENERGY BALANCE ERROR FOR CIRCUIT TRANSIENT ANALYSIS
THE ENERGY BALANCE ERROR FOR CIRCUIT TRANSIENT ANALYSIS FLORIN CONSTANTINESCU, ALEXANDRU GABRIEL GHEORGHE, MIRUNA NIŢESCU Key words: Trasiet aalysis, Eergy balace error, Time step coice. Two algoritms
More informationUniformly Consistency of the Cauchy-Transformation Kernel Density Estimation Underlying Strong Mixing
Appl. Mat. If. Sci. 7, No. L, 5-9 (203) 5 Applied Matematics & Iformatio Scieces A Iteratioal Joural c 203 NSP Natural Scieces Publisig Cor. Uiformly Cosistecy of te Caucy-Trasformatio Kerel Desity Estimatio
More informationFinite Difference Approximation for Transport Equation with Shifts Arising in Neuronal Variability
Iteratioal Joural of Sciece ad Research (IJSR) ISSN (Olie): 39-764 Ide Copericus Value (3): 64 Impact Factor (3): 4438 Fiite Differece Approimatio for Trasport Equatio with Shifts Arisig i Neuroal Variability
More informationTaylor polynomial solution of difference equation with constant coefficients via time scales calculus
TMSCI 3, o 3, 129-135 (2015) 129 ew Treds i Mathematical Scieces http://wwwtmscicom Taylor polyomial solutio of differece equatio with costat coefficiets via time scales calculus Veysel Fuat Hatipoglu
More informationA note on the modified Hermitian and skew-hermitian splitting methods for non-hermitian positive definite linear systems
A ote o the modified Hermitia ad skew-hermitia splittig methods for o-hermitia positive defiite liear systems Shi-Liag Wu Tig-Zhu Huag School of Applied Mathematics Uiversity of Electroic Sciece ad Techology
More informationA collocation method for singular integral equations with cosecant kernel via Semi-trigonometric interpolation
Iteratioal Joural of Mathematics Research. ISSN 0976-5840 Volume 9 Number 1 (017) pp. 45-51 Iteratioal Research Publicatio House http://www.irphouse.com A collocatio method for sigular itegral equatios
More informationExplicit Group Methods in the Solution of the 2-D Convection-Diffusion Equations
Proceedigs of the World Cogress o Egieerig 00 Vol III WCE 00 Jue 0 - July 00 Lodo U.K. Explicit Group Methods i the Solutio of the -D Covectio-Diffusio Equatios a Kah Bee orhashidah Hj. M. Ali ad Choi-Hog
More informationResearch Article Nonautonomous Discrete Neuron Model with Multiple Periodic and Eventually Periodic Solutions
Discrete Dyamics i Nature ad Society Volume 21, Article ID 147282, 6 pages http://dx.doi.org/1.11/21/147282 Research Article Noautoomous Discrete Neuro Model with Multiple Periodic ad Evetually Periodic
More informationMonte Carlo Optimization to Solve a Two-Dimensional Inverse Heat Conduction Problem
Australia Joural of Basic Applied Scieces, 5(): 097-05, 0 ISSN 99-878 Mote Carlo Optimizatio to Solve a Two-Dimesioal Iverse Heat Coductio Problem M Ebrahimi Departmet of Mathematics, Karaj Brach, Islamic
More informationA New Hybrid in the Nonlinear Part of Adomian Decomposition Method for Initial Value Problem of Ordinary Differential Equation
Joural of Matematics Researc; Vol No ; ISSN - E-ISSN - Publised b Caadia Ceter of Sciece ad Educatio A New Hbrid i te Noliear Part of Adomia Decompositio Metod for Iitial Value Problem of Ordiar Differetial
More informationGoal. Adaptive Finite Element Methods for Non-Stationary Convection-Diffusion Problems. Outline. Differential Equation
Goal Adaptive Fiite Elemet Methods for No-Statioary Covectio-Diffusio Problems R. Verfürth Ruhr-Uiversität Bochum www.ruhr-ui-bochum.de/um1 Tübige / July 0th, 017 Preset space-time adaptive fiite elemet
More informationComparison Study of Series Approximation. and Convergence between Chebyshev. and Legendre Series
Applied Mathematical Scieces, Vol. 7, 03, o. 6, 3-337 HIKARI Ltd, www.m-hikari.com http://d.doi.org/0.988/ams.03.3430 Compariso Study of Series Approimatio ad Covergece betwee Chebyshev ad Legedre Series
More informationNEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE
UPB Sci Bull, Series A, Vol 79, Iss, 207 ISSN 22-7027 NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE Gabriel Bercu We itroduce two ew sequeces of Euler-Mascheroi type which have fast covergece
More informationNUMERICAL METHOD FOR SINGULARLY PERTURBED DELAY PARABOLIC PARTIAL DIFFERENTIAL EQUATIONS
THERMAL SCIENCE, Year 07, Vol., No. 4, pp. 595-599 595 NUMERICAL METHOD FOR SINGULARLY PERTURBED DELAY PARABOLIC PARTIAL DIFFERENTIAL EQUATIONS by Yula WANG *, Da TIAN, ad Zhiyua LI Departmet of Mathematics,
More informationAn efficient time integration method for extra-large eddy simulations
A efficiet time itegratio method for extra-large eddy simulatios M.A. Scheibeler Departmet of Mathematics Master s Thesis A efficiet time itegratio method for extra-large eddy simulatios M.A. Scheibeler
More informationModified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations
Noliear Aalysis ad Differetial Equatios, Vol. 5, 27, o. 4, 57-7 HIKARI Ltd, www.m-hikari.com https://doi.org/.2988/ade.27.62 Modified Decompositio Method by Adomia ad Rach for Solvig Noliear Volterra Itegro-
More informationNumerical Solutions of Second Order Boundary Value Problems by Galerkin Residual Method on Using Legendre Polynomials
IOSR Joural of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 319-765X. Volume 11, Issue 6 Ver. IV (Nov. - Dec. 15), PP 1-11 www.iosrjourals.org Numerical Solutios of Secod Order Boudary Value Problems
More informationStability Analysis of the Euler Discretization for SIR Epidemic Model
Stability Aalysis of the Euler Discretizatio for SIR Epidemic Model Agus Suryato Departmet of Mathematics, Faculty of Scieces, Brawijaya Uiversity, Jl Vetera Malag 6545 Idoesia Abstract I this paper we
More informationScientific Research of the Institute of Mathematics and Computer Science
Scietific Researc of te Istitute of Matematics ad Computer Sciece ON THE TOLERANCE AVERAGING FOR DIFFERENTIAL OPERATORS WITH PERIODIC COEFFICIENTS Jolata Borowska, Łukasz Łaciński 2, Jowita Ryclewska,
More informationAN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC MAPS
http://www.paper.edu.c Iteratioal Joural of Bifurcatio ad Chaos, Vol. 1, No. 5 () 119 15 c World Scietific Publishig Compay AN OPEN-PLUS-CLOSED-LOOP APPROACH TO SYNCHRONIZATION OF CHAOTIC AND HYPERCHAOTIC
More informationMore Elementary Aspects of Numerical Solutions of PDEs!
ttp://www.d.edu/~gtryggva/cfd-course/ Outlie More Elemetary Aspects o Numerical Solutios o PDEs I tis lecture we cotiue to examie te elemetary aspects o umerical solutios o partial dieretial equatios.
More informationEstimating the Population Mean using Stratified Double Ranked Set Sample
Estimatig te Populatio Mea usig Stratified Double Raked Set Sample Mamoud Syam * Kamarulzama Ibraim Amer Ibraim Al-Omari Qatar Uiversity Foudatio Program Departmet of Mat ad Computer P.O.Box (7) Doa State
More information-ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION
NEW NEWTON-TYPE METHOD WITH k -ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION R. Thukral Padé Research Cetre, 39 Deaswood Hill, Leeds West Yorkshire, LS7 JS, ENGLAND ABSTRACT The objective
More informationSolving third order boundary value problem with fifth order block method
Matematical Metods i Egieerig ad Ecoomics Solvig tird order boudary value problem wit it order bloc metod A. S. Abdulla, Z. A. Majid, ad N. Seu Abstract We develop a it order two poit bloc metod or te
More informationNumerical solution of Bagley-Torvik equation using Chebyshev wavelet operational matrix of fractional derivative
It. J. Adv. Appl. Math. ad Mech. () (04) 83-9 ISSN: 347-59 Available olie at www.iaamm.com Iteratioal Joural of Advaces i Applied Mathematics ad Mechaics Numerical solutio of Bagley-Torvik equatio usig
More informationApplication of a Two-Step Third-Derivative Block Method for Starting Numerov Method
Iteratioal Joural of eoretical ad Applied Matematics 7; (: -5 ttp://wwwsciecepublisiroupcom//itam doi: 648/itam75 Applicatio of a wo-step ird-derivative Block Metod for Starti Numerov Metod Oluwaseu Adeyeye
More informationA STUDY ON MHD BOUNDARY LAYER FLOW OVER A NONLINEAR STRETCHING SHEET USING IMPLICIT FINITE DIFFERENCE METHOD
IRET: Iteratioal oural of Research i Egieerig ad Techology eissn: 39-63 pissn: 3-7308 A STUDY ON MHD BOUNDARY LAYER FLOW OVER A NONLINEAR STRETCHING SHEET USING IMPLICIT FINITE DIFFERENCE METHOD Satish
More informationChapter 7 Isoperimetric problem
Chapter 7 Isoperimetric problem Recall that the isoperimetric problem (see the itroductio its coectio with ido s proble) is oe of the most classical problem of a shape optimizatio. It ca be formulated
More informationμ are complex parameters. Other
A New Numerical Itegrator for the Solutio of Iitial Value Problems i Ordiary Differetial Equatios. J. Suday * ad M.R. Odekule Departmet of Mathematical Scieces, Adamawa State Uiversity, Mubi, Nigeria.
More informationwavelet collocation method for solving integro-differential equation.
IOSR Joural of Egieerig (IOSRJEN) ISSN (e): 5-3, ISSN (p): 78-879 Vol. 5, Issue 3 (arch. 5), V3 PP -7 www.iosrje.org wavelet collocatio method for solvig itegro-differetial equatio. Asmaa Abdalelah Abdalrehma
More informationDECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS. Park Road, Islamabad, Pakistan
Mathematical ad Computatioal Applicatios, Vol. 9, No. 3, pp. 30-40, 04 DECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS Muhammad Aslam Noor, Khalida Iayat Noor ad Asif Waheed
More informationH05 A 3-D INVERSE PROBLEM IN ESTIMATING THE TIME-DEPENDENT HEAT TRANSFER COEFFICIENTS FOR PLATE FINS
Proceedigs of te 5 t Iteratioal Coferece o Iverse Problems i Egieerig: Teory ad Practice, Cambridge, UK, 11-15 t July 005 A 3-D INVERSE PROBLEM IN ESTIMATING THE TIME-DEPENDENT HEAT TRANSFER COEFFICIENTS
More informationALLOCATING SAMPLE TO STRATA PROPORTIONAL TO AGGREGATE MEASURE OF SIZE WITH BOTH UPPER AND LOWER BOUNDS ON THE NUMBER OF UNITS IN EACH STRATUM
ALLOCATING SAPLE TO STRATA PROPORTIONAL TO AGGREGATE EASURE OF SIZE WIT BOT UPPER AND LOWER BOUNDS ON TE NUBER OF UNITS IN EAC STRATU Lawrece R. Erst ad Cristoper J. Guciardo Erst_L@bls.gov, Guciardo_C@bls.gov
More informationSolution of Differential Equation from the Transform Technique
Iteratioal Joural of Computatioal Sciece ad Mathematics ISSN 0974-3189 Volume 3, Number 1 (2011), pp 121-125 Iteratioal Research Publicatio House http://wwwirphousecom Solutio of Differetial Equatio from
More informationDefinition 4.2. (a) A sequence {x n } in a Banach space X is a basis for X if. unique scalars a n (x) such that x = n. a n (x) x n. (4.
4. BASES I BAACH SPACES 39 4. BASES I BAACH SPACES Sice a Baach space X is a vector space, it must possess a Hamel, or vector space, basis, i.e., a subset {x γ } γ Γ whose fiite liear spa is all of X ad
More informationComputation of Hahn Moments for Large Size Images
Joural of Computer Sciece 6 (9): 37-4, ISSN 549-3636 Sciece Publicatios Computatio of Ha Momets for Large Size Images A. Vekataramaa ad P. Aat Raj Departmet of Electroics ad Commuicatio Egieerig, Quli
More informationResearch Article Two Expanding Integrable Models of the Geng-Cao Hierarchy
Abstract ad Applied Aalysis Volume 214, Article ID 86935, 7 pages http://d.doi.org/1.1155/214/86935 Research Article Two Epadig Itegrable Models of the Geg-Cao Hierarchy Xiurog Guo, 1 Yufeg Zhag, 2 ad
More informationIN many scientific and engineering applications, one often
INTERNATIONAL JOURNAL OF COMPUTING SCIENCE AND APPLIED MATHEMATICS, VOL 3, NO, FEBRUARY 07 5 Secod Degree Refiemet Jacobi Iteratio Method for Solvig System of Liear Equatio Tesfaye Kebede Abstract Several
More informationFive Steps Block Predictor-Block Corrector Method for the Solution of ( )
Applied Mathematics, 4,, -66 Published Olie May 4 i SciRes. http://www.scirp.org/oural/am http://dx.doi.org/.46/am.4.87 Five Steps Block Predictor-Block Corrector y = f x, y, y Method for the Solutio of
More informationOptimized interface conditions for the compressible Euler equations
Optimized iterface coditios for the compressible Euler equatios Victorita Dolea 1 ad Frédéric Nataf 2 1 UMR 6621 CNRS, Uiversité de Nice Sophia-Atipolis dolea@math.uice.fr 2 CMAP, UMR 7641 CNRS, École
More information1. Linearization of a nonlinear system given in the form of a system of ordinary differential equations
. Liearizatio of a oliear system give i the form of a system of ordiary differetial equatios We ow show how to determie a liear model which approximates the behavior of a time-ivariat oliear system i a
More informationHALF-SWEEP GAUSS-SEIDEL ITERATION APPLIED TO TIME-FRACTIONAL DIFFUSION EQUATIONS
Jural Karya Asli Loreka Ahli Matematik Vol. 8 No. () Page 06-0 Jural Karya Asli Loreka Ahli Matematik HALF-SWEEP GAUSS-SEIDEL ITERATION APPLIED TO TIME-FRACTIONAL DIFFUSION EQUATIONS A. Suarto J. Sulaima
More informationStreamfunction-Vorticity Formulation
Streamfuctio-Vorticity Formulatio A. Salih Departmet of Aerospace Egieerig Idia Istitute of Space Sciece ad Techology, Thiruvaathapuram March 2013 The streamfuctio-vorticity formulatio was amog the first
More information62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 +
62. Power series Defiitio 16. (Power series) Give a sequece {c }, the series c x = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + is called a power series i the variable x. The umbers c are called the coefficiets of
More informationON POINTWISE BINOMIAL APPROXIMATION
Iteratioal Joural of Pure ad Applied Mathematics Volume 71 No. 1 2011, 57-66 ON POINTWISE BINOMIAL APPROXIMATION BY w-functions K. Teerapabolar 1, P. Wogkasem 2 Departmet of Mathematics Faculty of Sciece
More informationExact Solutions for a Class of Nonlinear Singular Two-Point Boundary Value Problems: The Decomposition Method
Exact Solutios for a Class of Noliear Sigular Two-Poit Boudary Value Problems: The Decompositio Method Abd Elhalim Ebaid Departmet of Mathematics, Faculty of Sciece, Tabuk Uiversity, P O Box 741, Tabuki
More informationNumerical Conformal Mapping via a Fredholm Integral Equation using Fourier Method ABSTRACT INTRODUCTION
alaysia Joural of athematical Scieces 3(1): 83-93 (9) umerical Coformal appig via a Fredholm Itegral Equatio usig Fourier ethod 1 Ali Hassa ohamed urid ad Teh Yua Yig 1, Departmet of athematics, Faculty
More informationFourier Techniques lecture by Håkon Hoel
CSC Nada DN55 Sprig - Differetial Equatios II JOp p (7) Fourier Teciques lecture by Håo Hoel Fourier series... Applicatios to liear PDE... 3 Numerical metods...3 3. Vo Neuma aalysis...4 3. Spectral metods...6
More informationPAijpam.eu ON TENSOR PRODUCT DECOMPOSITION
Iteratioal Joural of Pure ad Applied Mathematics Volume 103 No 3 2015, 537-545 ISSN: 1311-8080 (prited versio); ISSN: 1314-3395 (o-lie versio) url: http://wwwijpameu doi: http://dxdoiorg/1012732/ijpamv103i314
More informationWeighted Approximation by Videnskii and Lupas Operators
Weighted Approximatio by Videsii ad Lupas Operators Aif Barbaros Dime İstabul Uiversity Departmet of Egieerig Sciece April 5, 013 Aif Barbaros Dime İstabul Uiversity Departmet Weightedof Approximatio Egieerig
More informationLecture 8: Solving the Heat, Laplace and Wave equations using finite difference methods
Itroductory lecture otes o Partial Differetial Equatios - c Athoy Peirce. Not to be copied, used, or revised without explicit writte permissio from the copyright ower. 1 Lecture 8: Solvig the Heat, Laplace
More informationA RANK STATISTIC FOR NON-PARAMETRIC K-SAMPLE AND CHANGE POINT PROBLEMS
J. Japa Statist. Soc. Vol. 41 No. 1 2011 67 73 A RANK STATISTIC FOR NON-PARAMETRIC K-SAMPLE AND CHANGE POINT PROBLEMS Yoichi Nishiyama* We cosider k-sample ad chage poit problems for idepedet data i a
More informationImproved Estimation of Rare Sensitive Attribute in a Stratified Sampling Using Poisson Distribution
Ope Joural of Statistics, 06, 6, 85-95 Publised Olie February 06 i SciRes ttp://wwwscirporg/joural/ojs ttp://dxdoiorg/0436/ojs0660 Improved Estimatio of Rare Sesitive ttribute i a Stratified Samplig Usig
More informationUniform Strict Practical Stability Criteria for Impulsive Functional Differential Equations
Global Joural of Sciece Frotier Research Mathematics ad Decisio Scieces Volume 3 Issue Versio 0 Year 03 Type : Double Blid Peer Reviewed Iteratioal Research Joural Publisher: Global Jourals Ic (USA Olie
More informationGenerating Functions for Laguerre Type Polynomials. Group Theoretic method
It. Joural of Math. Aalysis, Vol. 4, 2010, o. 48, 257-266 Geeratig Fuctios for Laguerre Type Polyomials α of Two Variables L ( xy, ) by Usig Group Theoretic method Ajay K. Shula* ad Sriata K. Meher** *Departmet
More informationDetermination of Energy Involved In a Stepwise Size Reduction of Maize, Using a Numerical Approach.
IOSR Joural of Matematics (IOSR-JM) e-issn: 78-578, p-issn: 9-765X. Volume, Issue Ver. V (Ja - Feb. 5), PP 6-65 www.iosrourals.org Determiatio of ergy Ivolved I a Stepwise Size Reductio of Maize, Usig
More informationThe picture in figure 1.1 helps us to see that the area represents the distance traveled. Figure 1: Area represents distance travelled
1 Lecture : Area Area ad distace traveled Approximatig area by rectagles Summatio The area uder a parabola 1.1 Area ad distace Suppose we have the followig iformatio about the velocity of a particle, how
More information1. Introduction. 2. Numerical Methods
America Joural o Computatioal ad Applied Matematics, (5: 9- DOI:.59/j.ajcam.5. A Stud o Numerical Solutios o Secod Order Iitial Value Problems (IVP or Ordiar Dieretial Equatios wit Fourt Order ad Butcer
More informationPOWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS
Joural of Applied Mathematics ad Computatioal Mechaics 4 3(3) 3-8 POWER SERIES SOLUION OF FIRS ORDER MARIX DIFFERENIAL EQUAIONS Staisław Kukla Izabela Zamorska Istitute of Mathematics Czestochowa Uiversity
More informationSome New Iterative Methods for Solving Nonlinear Equations
World Applied Scieces Joural 0 (6): 870-874, 01 ISSN 1818-495 IDOSI Publicatios, 01 DOI: 10.589/idosi.wasj.01.0.06.830 Some New Iterative Methods for Solvig Noliear Equatios Muhammad Aslam Noor, Khalida
More informationSome Variants of Newton's Method with Fifth-Order and Fourth-Order Convergence for Solving Nonlinear Equations
Copyright, Darbose Iteratioal Joural o Applied Mathematics ad Computatio Volume (), pp -6, 9 http//: ijamc.darbose.com Some Variats o Newto's Method with Fith-Order ad Fourth-Order Covergece or Solvig
More informationA numerical Technique Finite Volume Method for Solving Diffusion 2D Problem
The Iteratioal Joural Of Egieerig d Sciece (IJES) Volume 4 Issue 10 Pages PP -35-41 2015 ISSN (e): 2319 1813 ISSN (p): 2319 1805 umerical Techique Fiite Volume Method for Solvig Diffusio 2D Problem 1 Mohammed
More informationDiscrete Orthogonal Moment Features Using Chebyshev Polynomials
Discrete Orthogoal Momet Features Usig Chebyshev Polyomials R. Mukuda, 1 S.H.Og ad P.A. Lee 3 1 Faculty of Iformatio Sciece ad Techology, Multimedia Uiversity 75450 Malacca, Malaysia. Istitute of Mathematical
More informationLECTURE 2 LEAST SQUARES CROSS-VALIDATION FOR KERNEL DENSITY ESTIMATION
Jauary 3 07 LECTURE LEAST SQUARES CROSS-VALIDATION FOR ERNEL DENSITY ESTIMATION Noparametric kerel estimatio is extremely sesitive to te coice of badwidt as larger values of result i averagig over more
More informationA NOTE ON BOUNDARY BLOW-UP PROBLEM OF u = u p
A NOTE ON BOUNDARY BLOW-UP PROBLEM OF u = u p SEICK KIM Abstract. Assume that Ω is a bouded domai i R with 2. We study positive solutios to the problem, u = u p i Ω, u(x) as x Ω, where p > 1. Such solutios
More informationMath 257: Finite difference methods
Math 257: Fiite differece methods 1 Fiite Differeces Remember the defiitio of a derivative f f(x + ) f(x) (x) = lim 0 Also recall Taylor s formula: (1) f(x + ) = f(x) + f (x) + 2 f (x) + 3 f (3) (x) +...
More informationNICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) =
AN INTRODUCTION TO SCHRÖDER AND UNKNOWN NUMBERS NICK DUFRESNE Abstract. I this article we will itroduce two types of lattice paths, Schröder paths ad Ukow paths. We will examie differet properties of each,
More informationMost text will write ordinary derivatives using either Leibniz notation 2 3. y + 5y= e and y y. xx tt t
Itroductio to Differetial Equatios Defiitios ad Termiolog Differetial Equatio: A equatio cotaiig the derivatives of oe or more depedet variables, with respect to oe or more idepedet variables, is said
More informationSOME RELATIONS ON HERMITE MATRIX POLYNOMIALS. Levent Kargin and Veli Kurt
Mathematical ad Computatioal Applicatios, Vol. 18, No. 3, pp. 33-39, 013 SOME RELATIONS ON HERMITE MATRIX POLYNOMIALS Levet Kargi ad Veli Kurt Departmet of Mathematics, Faculty Sciece, Uiversity of Adeiz
More informationLinear Elliptic PDE s Elliptic partial differential equations frequently arise out of conservation statements of the form
Liear Elliptic PDE s Elliptic partial differetial equatios frequetly arise out of coservatio statemets of the form B F d B Sdx B cotaied i bouded ope set U R. Here F, S deote respectively, the flux desity
More informationTMA4205 Numerical Linear Algebra. The Poisson problem in R 2 : diagonalization methods
TMA4205 Numerical Liear Algebra The Poisso problem i R 2 : diagoalizatio methods September 3, 2007 c Eiar M Røquist Departmet of Mathematical Scieces NTNU, N-749 Trodheim, Norway All rights reserved A
More informationSimilarity Solutions to Unsteady Pseudoplastic. Flow Near a Moving Wall
Iteratioal Mathematical Forum, Vol. 9, 04, o. 3, 465-475 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.988/imf.04.48 Similarity Solutios to Usteady Pseudoplastic Flow Near a Movig Wall W. Robi Egieerig
More informationSome properties of Boubaker polynomials and applications
Some properties of Boubaker polyomials ad applicatios Gradimir V. Milovaović ad Duša Joksimović Citatio: AIP Cof. Proc. 179, 1050 (2012); doi: 10.1063/1.756326 View olie: http://dx.doi.org/10.1063/1.756326
More informationUniversity of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015
Uiversity of Wasigto Departmet of Cemistry Cemistry 453 Witer Quarter 15 Lecture 14. /11/15 Recommeded Text Readig: Atkis DePaula: 9.1, 9., 9.3 A. Te Equipartitio Priciple & Eergy Quatizatio Te Equipartio
More informationb i u x i U a i j u x i u x j
M ath 5 2 7 Fall 2 0 0 9 L ecture 1 9 N ov. 1 6, 2 0 0 9 ) S ecod- Order Elliptic Equatios: Weak S olutios 1. Defiitios. I this ad the followig two lectures we will study the boudary value problem Here
More informationNew Version of the Rayleigh Schrödinger Perturbation Theory: Examples
New Versio of the Rayleigh Schrödiger Perturbatio Theory: Examples MILOŠ KALHOUS, 1 L. SKÁLA, 1 J. ZAMASTIL, 1 J. ČÍŽEK 2 1 Charles Uiversity, Faculty of Mathematics Physics, Ke Karlovu 3, 12116 Prague
More informationHigher-order iterative methods by using Householder's method for solving certain nonlinear equations
Math Sci Lett, No, 7- ( 7 Mathematical Sciece Letters A Iteratioal Joural http://dxdoiorg/785/msl/5 Higher-order iterative methods by usig Householder's method for solvig certai oliear equatios Waseem
More informationDEGENERACY AND ALL THAT
DEGENERACY AND ALL THAT Te Nature of Termodyamics, Statistical Mecaics ad Classical Mecaics Termodyamics Te study of te equilibrium bulk properties of matter witi te cotext of four laws or facts of experiece
More informationarxiv: v2 [math.na] 1 Feb 2016
A Aalysis of Galerki Proper Ortogoal Decompositio for Subdiffusio Bagti Ji Zi Zou arxiv:58.634v2 [mat.a] Feb 26 October 9, 28 Abstract I tis work, we develop a ovel Galerki-L-POD sceme for te subdiffusio
More informationTime-Domain Representations of LTI Systems
2.1 Itroductio Objectives: 1. Impulse resposes of LTI systems 2. Liear costat-coefficiets differetial or differece equatios of LTI systems 3. Bloc diagram represetatios of LTI systems 4. State-variable
More informationCO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS
CO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS C.PRAX ad H.SADAT Laboratoire d'etudes Thermiques,URA CNRS 403 40, Aveue du Recteur Pieau 86022 Poitiers Cedex,
More informationq-durrmeyer operators based on Pólya distribution
Available olie at wwwtjsacom J Noliear Sci Appl 9 206 497 504 Research Article -Durrmeyer operators based o Pólya distributio Vijay Gupta a Themistocles M Rassias b Hoey Sharma c a Departmet of Mathematics
More informationMETHOD OF FUNDAMENTAL SOLUTIONS FOR HELMHOLTZ EIGENVALUE PROBLEMS IN ELLIPTICAL DOMAINS
Please cite this article as: Staisław Kula, Method of fudametal solutios for Helmholtz eigevalue problems i elliptical domais, Scietific Research of the Istitute of Mathematics ad Computer Sciece, 009,
More informationRiesz-Fischer Sequences and Lower Frame Bounds
Zeitschrift für Aalysis ud ihre Aweduge Joural for Aalysis ad its Applicatios Volume 1 (00), No., 305 314 Riesz-Fischer Sequeces ad Lower Frame Bouds P. Casazza, O. Christese, S. Li ad A. Lider Abstract.
More informationNumerical Solution of the First-Order Hyperbolic Partial Differential Equation with Point-Wise Advance
Iteratioal oural of Sciece ad Research (ISR) ISSN (Olie): 39-74 Ide Copericus Value (3): 4 Impact Factor (3): 4438 Numerical Solutio of the First-Order Hyperbolic Partial Differetial Equatio with Poit-Wise
More informationResearch Article A New Second-Order Iteration Method for Solving Nonlinear Equations
Abstract ad Applied Aalysis Volume 2013, Article ID 487062, 4 pages http://dx.doi.org/10.1155/2013/487062 Research Article A New Secod-Order Iteratio Method for Solvig Noliear Equatios Shi Mi Kag, 1 Arif
More informationTR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT
TR/46 OCTOBER 974 THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION by A. TALBOT .. Itroductio. A problem i approximatio theory o which I have recetly worked [] required for its solutio a proof that the
More information