The Solution of the Two-Dimensional Gross-Pitaevskii Equation Using Lattice-Boltzmann and He s Semi-Inverse Method
|
|
- Brice Rose
- 5 years ago
- Views:
Transcription
1 Internatonal Journal of Mathematcal Analyss Vol., 7, no., HIKARI Ltd, The Soluton of the Two-Dmensonal Gross-Ptaevsk Equaton Usng Lattce-Boltzmann and He s Sem-Inverse Method F. Fonseca Unversdad Naconal de Colomba Grupo de Cenca de Materales y Superfces Departamento de Físca Bogotá-Colomba Copyrght c 7 F. Fonseca. Ths artcle s dstrbuted under the Creatve Commons Attrbuton Lcense, whch permts unrestrkd use, dstrbuton, and reproducton n any medum, provded the orgnal work s properly cted. Abstract We solve the two-dmensonal tme ndependent Gross-Ptaevsk equaton usng the lattce-boltzmann technque for a dq9 lattce velocty scheme. Also, applyng the He s sem nverse method we fnd soltary wave soluton. We get stable densty profles. Keywords: d Bose-Ensten condensates, lattce-boltzmann, He s sem nverse method Introducton The Gross-Ptaevsk equaton, (GEq), descrbes the Bose-Condensates phenomena, whch s a very mportant nvestgaton feld n condensed matter physcs, at low temperature []. Ths nonlnear dfferental equaton s used, e.g., n nonlnear Optcs, quantum flud dynamcs, and the magnetc trap of Rubdum atoms at very low temperatures []-[3]. Research n pure and appled mathematcs has been done for GEq. For nstance, usng tme-splttng spectral [4], fnte-dfference scheme [5], doman truncaton technques [6]. Also, the use of the lattce-boltzmann (LB) technque, s wdely use n Physcs. For
2 7 F. Fonseca example, LB has been appled from research felds as dverse as magnetohydrodynamcs [7], tll the Posson equaton [8]. Also, the tme dependent GEq had been solved usng LB, obtanng good results, [9] (and references theren). Ths work solves the Gross-Ptaevsk equaton usng the lattce Boltzmann and He s sem nverse method. In secton ()-(3), we present the lattce-boltzmann technque and the moment dstrbuton functons appled to dervaton of the GEq. In secton (4), we get the GEq. Then, n secton (5), we obtan the equlbrum dstrbuton functons usng dq9 scheme. In secton (6), we use the He s sem nverse method. And at last, n secton (7), we present results and conclusons. The lattce Boltzmann model The lattce-boltzmann equaton s: f ( r + vδt, t + δt) f ( r, t) = Ω ( r, t) () Where Ω( r, t) s the collson term, and usng the B.G.K approxmaton []: Ω ( r, t) = [ fj ( r, t) f eq j ( r, v) ] () τ Expandng the one-partcle dstrbuton functon n a Taylor seres, we have: + ( f( r + δ r, t + δt) f ( r, t) = δt t + δx x + δy ) f (3) y ( δt t + δx x + δy ) + δxδt + δyδt y xt yt + δxδy f xy Consderng δ r = vδt, δx = δtv x and δy = δtv y, and replacng n eq.(4) f( r + vδt, t + δt) f ( r, t) = δt [ ] [ ] t + v f + δt t + v f (4) Dong a perturbatve expanson at frst order n the spatal dervatves, second order to the tme dervatve, and second order to the partcle dstrbuton functon, we have: x = ɛ x, y = ɛ, y t = ɛ + ɛ, f = f + ɛf + ɛ f (5) t t Assumng = x + y j and replacng eqs. (5) n eq. (4)
3 Soluton of the two-dmensonal Gross-Ptaevsk equaton 7 (( τ (f + ɛf + ɛ f f eq ) = (δt ɛ + ɛ ) + v [ɛ t t ] ) (6) [( + δt ɛ + ɛ ) + v [ ɛ t t ] ] ) ( ) f + ɛf + ɛ f The terms at order ɛ n eq. (6) and assumng f = f eq, we have: [( ) ] [ ] ɛf (f τ = ɛδt + v t ) The terms at order ɛ n eq (6), we get: (7) τ ɛ f + δt Replacng eq. (7) n eq. (8), we get: = ɛ δt f [ ] + ɛ (δt + v t t f (8) ( ) ( ) + v t (f δt + v t ) ) τ [ ] [ ] f ( ) = δt f t + δt + v t f ( ) τ (9) Summng eq. (7) to eq. (9), we have: τδt (ɛf + ɛ f ) = ( + v t [ ) ɛf + ɛ f 3 Moments of the dstrbuton ( )] + ɛ ( ) f τ t () Dong the next defntons for the statstcal meoments of f, we have: (ρ µρ ρ ρ) = f () ; u = v f () () Π () α,β = v,α v,β f () () f (k) =, (k ) (3) Where ρ and u are the densty feld an velocty feld of the physcal system. Besdes, we assume the dstrbuton functon f satsfy the probablty conservaton condton wth the equlbrum dstrbuton f eq, such that f = f eq
4 7 F. Fonseca 4 The Gross-Ptaevsk equaton Takng the summaton about () n eqs. () and () (v,α ), we get: (ρ µρ ρ ρ) t The tensor Π () s defned a dagonal matrx ( ) Π () ρ = t ρ t Replacng eq. (6) n eq. (5), we obtan: + u =. (4) u t + Π() =, (5) (6) Interchangng dervatves u t ( ρ t ) = (7) Applyng dvergence n eq. (8), we get: u t (ρ) = (8) u t (ρ) = (9) Fgure : The lattce veloctes dq9 scheme. Usng eq. (4) n eq. (9), we obtan: (ρ µρ ρ ρ) t t (ρ) = ()
5 Soluton of the two-dmensonal Gross-Ptaevsk equaton 73 Takng out the temporal dervatve and assumng zero the nteror term n the parenthess, we get the Gross-Ptaevsk equaton ρ + (ρ ρ ρ) = µρ () 5 The equlbrum dstrbuton functon usng dq9 velocty scheme. The dq9 scheme velocty lattce shown n fg. () s used. The drectons v and weghts w on each cell are defned as: w = { 4 9, f = ; 9, f =,, 3, 4; 36, f = 5, 6, 7, 8 } () Both, drectons v and weghts w, follow the next tensoral relatons: w v,α =, w v,α v,β = 3 δ α,β, The equlbrum functon used s: w v,α v,β v,γ = (3) { f (eq) w [A v = u + B] f > w C otherwse = (4) The A, B y C constants n the equlbrum functon f (eq), are proportonal to the macroscopc quanttes, and they are calculated usng eqs. (-) n combnaton wth eqs. (3), then: B = 3 (ρ) t, A = 3, C = 9 4 (ρ µρ ρ ρ) (ρ) t (5) Then, the equlbrum functon that satsfes the Gross-Ptaevsk equaton s, f (eq) = ( ) 3w v u (ρ) t 9 4 w (ρ µρ ρ ρ) f > (ρ) t and = (6) In order to mplement the dervatve operator of ρ(x, t) used n eq. (6), we appled the dfference dscretzaton scheme of the second dervatve as: ρ ρ(x, t + δt) ρ(x, t) + ρ(x, t δt) = (7) t δt
6 74 F. Fonseca 6 He s sem-nverse method, Soltary wave soluton Accordng to He s sem nverse method [9], we choose the energy functonal [9], that satsfy eqs. (). Then, we get: Or: J(φ) = ( ( ) φ ( φ ) + 4 φ 4 )da (8) J(φ) = (( φ x ) + ( φ y ) φ + 4 φ 4 )dxdy (9) Changng to polar coordnates ξ = x + y ; x = ξ cos (θ); y = ξ sn (θ) (3) Fgure : LB results, usng an ntal profle gven by eq. (3). Then, eq. (3) s: J(φ) = (( φ ξ ) + ξ (φ θ ) φ + 4 φ 4 )ξdξdθ (3) We choose as a soluton:
7 Soluton of the two-dmensonal Gross-Ptaevsk equaton 75 Then, the entre acton s: ρ = a sn(bξ ) exp( bξ ) (3) J(a, b) = a 6 a (µ ) + 3a 8b 5b (33) In order to make J statonary, we calculate: J b = a (µ ) 3a 8b 5b = ; a = 4 (µ ) (34) 3 J = a 6 µ 8b + 6a 5b = ; b = (µ ) 8 (35) Fgures () show the LB results produced by an ntal profle gven by (3). The boundary condtons are zero at all tmes. 7 Conclusons We have solved the Gross-Ptaevsk equaton usng the lattce-boltzmann method and the He s sem nverse method. In addton, we present results for an ntal profle showng stable solutons. Besdes, we gve an explct soluton of Gross-Ptaevsk equaton: ρ(x, y) = a sn(b(x + y )) exp( b(x + y )) (36) As a future work we can extend the method to three dmensons. Acknowledgements. Ths research was supported by Unversdad Naconal de Colomba n Hermes project (35). References [] S. N. Bose, Plancks Gesetz und Lchtquantenhypothese, Zetschrft fuer Physk, 6 (94), German translaton of Boses paper on Plancks law by Abert Ensten.
8 76 F. Fonseca [] M. H. Anderson, J. R. Ensher, M. R. Matthews, C. E. Weman and E. A. Cornell, Observaton of Bose-Ensten condensaton n a dlute atomc vapor, Scence, 69 (995), [3] K. B. Davs, M. O. Mewes, M. R. Andrews, N. J. van Druten, D. S. Durfee, D. M. Kurn, and W. Ketterle, Bose-ensten condensaton n a gas of sodum atoms, Phys. Rev. Lett., 75 (995), [4] W. Bao, S. Jn and P. A. Markowch, On tme-splttng spectral approxmaton for the Schrödnger equatons n the sem-classcal regme, Journal of Comput. Phys., 75 (), [5] M. M. Cermele, M. L. Chofalo, F. Pstella, S. Succ, and M. P. Tos, Numercal soluton of the Gross-Ptaevsk equaton usng an explct fntedfference scheme: An applcaton to trapped Bose-Ensten condensates, Phys. Rev. E, 6 (), no., [6] X. Antonea, C. Besseb and P. Klen, Numercal soluton of tmedependent nonlnear Schrödnger equatons usng doman truncaton technques coupled wth relaxaton scheme, Laser Physcs, (), no. 8, [7] P. J. Dellar, Lattce Boltzmann magnetohydrodynamcs wth currentdependent resstvty, Journal of Computatonal Physcs, 37 (3), [8] Z. Cha and B. Sh, A novel lattce Boltzmann model for the Posson equaton, Appled Mathematcal Modellng, 3 (8), [9] H. Wang and G. Yan, Lattce Boltzmann model for the nteracton of (+)-dmensonal soltons n generalzed GrossPtaevsk equaton, Appled Mathematcal Modellng, 4 (6), [] P. Bathnagar, E. Gross, A. Krook, A Model for Collson Processes n Gases. I. Small Ampltude Processes n Charged and Neutral One- Component Systems, Phys. Rev., 94 (954),
9 Soluton of the two-dmensonal Gross-Ptaevsk equaton 77 [] J-Huan He, A classcal varatonal model for mcropolar elastodynamcs, Internatonal Journal of Nonlnear Scence and Numercal Smulaton, (), no., Receved: January 7, 7; Publshed: January 4, 7
A Solution of the Harry-Dym Equation Using Lattice-Boltzmannn and a Solitary Wave Methods
Appled Mathematcal Scences, Vol. 11, 2017, no. 52, 2579-2586 HIKARI Ltd, www.m-hkar.com https://do.org/10.12988/ams.2017.79280 A Soluton of the Harry-Dym Equaton Usng Lattce-Boltzmannn and a Soltary Wave
More informationA Solution of Porous Media Equation
Internatonal Mathematcal Forum, Vol. 11, 016, no. 15, 71-733 HIKARI Ltd, www.m-hkar.com http://dx.do.org/10.1988/mf.016.6669 A Soluton of Porous Meda Equaton F. Fonseca Unversdad Naconal de Colomba Grupo
More information(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate
Internatonal Journal of Mathematcs and Systems Scence (018) Volume 1 do:10.494/jmss.v1.815 (Onlne Frst)A Lattce Boltzmann Scheme for Dffuson Equaton n Sphercal Coordnate Debabrata Datta 1 *, T K Pal 1
More informationResearch Article A Multilevel Finite Difference Scheme for One-Dimensional Burgers Equation Derived from the Lattice Boltzmann Method
Appled Mathematcs Volume 01, Artcle ID 9590, 13 pages do:10.1155/01/9590 Research Artcle A Multlevel Fnte Dfference Scheme for One-Dmensonal Burgers Equaton Derved from the Lattce Boltzmann Method Qaoe
More informationThe Order Relation and Trace Inequalities for. Hermitian Operators
Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence
More informationThe Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices
Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan
More informationResearch Article Green s Theorem for Sign Data
Internatonal Scholarly Research Network ISRN Appled Mathematcs Volume 2012, Artcle ID 539359, 10 pages do:10.5402/2012/539359 Research Artcle Green s Theorem for Sgn Data Lous M. Houston The Unversty of
More informationMagnetic Diffusion using Lattice-Boltzmann
Revsta Mexcana de Físca S 58 2 188 14 DICIEMBRE 212 Magnetc Dffuson usng Lattce-Boltzmann F. Fonseca Physcs Department, Unversdad Naconal de Colomba, Bogotá Colomba. e-mal: frfonsecaf@unal.edu.co Recbdo
More informationAsymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation
Nonl. Analyss and Dfferental Equatons, ol., 4, no., 5 - HIKARI Ltd, www.m-har.com http://dx.do.org/.988/nade.4.456 Asymptotcs of the Soluton of a Boundary alue Problem for One-Characterstc Dfferental Equaton
More informationThe Exact Formulation of the Inverse of the Tridiagonal Matrix for Solving the 1D Poisson Equation with the Finite Difference Method
Journal of Electromagnetc Analyss and Applcatons, 04, 6, 0-08 Publshed Onlne September 04 n ScRes. http://www.scrp.org/journal/jemaa http://dx.do.org/0.46/jemaa.04.6000 The Exact Formulaton of the Inverse
More informationA Hybrid Variational Iteration Method for Blasius Equation
Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method
More informationResearch Article Cubic B-Spline Collocation Method for One-Dimensional Heat and Advection-Diffusion Equations
Appled Mathematcs Volume 22, Artcle ID 4587, 8 pages do:.55/22/4587 Research Artcle Cubc B-Splne Collocaton Method for One-Dmensonal Heat and Advecton-Dffuson Equatons Joan Goh, Ahmad Abd. Majd, and Ahmad
More informationPhysics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1
P. Guterrez Physcs 5153 Classcal Mechancs D Alembert s Prncple and The Lagrangan 1 Introducton The prncple of vrtual work provdes a method of solvng problems of statc equlbrum wthout havng to consder the
More informationComparison of the Population Variance Estimators. of 2-Parameter Exponential Distribution Based on. Multiple Criteria Decision Making Method
Appled Mathematcal Scences, Vol. 7, 0, no. 47, 07-0 HIARI Ltd, www.m-hkar.com Comparson of the Populaton Varance Estmators of -Parameter Exponental Dstrbuton Based on Multple Crtera Decson Makng Method
More informationLagrangian Field Theory
Lagrangan Feld Theory Adam Lott PHY 391 Aprl 6, 017 1 Introducton Ths paper s a summary of Chapter of Mandl and Shaw s Quantum Feld Theory [1]. The frst thng to do s to fx the notaton. For the most part,
More informationThe Feynman path integral
The Feynman path ntegral Aprl 3, 205 Hesenberg and Schrödnger pctures The Schrödnger wave functon places the tme dependence of a physcal system n the state, ψ, t, where the state s a vector n Hlbert space
More informationOne-sided finite-difference approximations suitable for use with Richardson extrapolation
Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,
More informationPhysics 5153 Classical Mechanics. Principle of Virtual Work-1
P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal
More informationQuantum Particle Motion in Physical Space
Adv. Studes Theor. Phys., Vol. 8, 014, no. 1, 7-34 HIKARI Ltd, www.-hkar.co http://dx.do.org/10.1988/astp.014.311136 Quantu Partcle Moton n Physcal Space A. Yu. Saarn Dept. of Physcs, Saara State Techncal
More informationThe Tangential Force Distribution on Inner Cylinder of Power Law Fluid Flowing in Eccentric Annuli with the Inner Cylinder Reciprocating Axially
Open Journal of Flud Dynamcs, 2015, 5, 183-187 Publshed Onlne June 2015 n ScRes. http://www.scrp.org/journal/ojfd http://dx.do.org/10.4236/ojfd.2015.52020 The Tangental Force Dstrbuton on Inner Cylnder
More informationTensor Smooth Length for SPH Modelling of High Speed Impact
Tensor Smooth Length for SPH Modellng of Hgh Speed Impact Roman Cherepanov and Alexander Gerasmov Insttute of Appled mathematcs and mechancs, Tomsk State Unversty 634050, Lenna av. 36, Tomsk, Russa RCherepanov82@gmal.com,Ger@npmm.tsu.ru
More information14 The Postulates of Quantum mechanics
14 The Postulates of Quantum mechancs Postulate 1: The state of a system s descrbed completely n terms of a state vector Ψ(r, t), whch s quadratcally ntegrable. Postulate 2: To every physcally observable
More informationCHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE
CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng
More informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationGeorgia Tech PHYS 6124 Mathematical Methods of Physics I
Georga Tech PHYS 624 Mathematcal Methods of Physcs I Instructor: Predrag Cvtanovć Fall semester 202 Homework Set #7 due October 30 202 == show all your work for maxmum credt == put labels ttle legends
More informationCase Study of Markov Chains Ray-Knight Compactification
Internatonal Journal of Contemporary Mathematcal Scences Vol. 9, 24, no. 6, 753-76 HIKAI Ltd, www.m-har.com http://dx.do.org/.2988/cms.24.46 Case Study of Marov Chans ay-knght Compactfcaton HaXa Du and
More informationAmplification and Relaxation of Electron Spin Polarization in Semiconductor Devices
Amplfcaton and Relaxaton of Electron Spn Polarzaton n Semconductor Devces Yury V. Pershn and Vladmr Prvman Center for Quantum Devce Technology, Clarkson Unversty, Potsdam, New York 13699-570, USA Spn Relaxaton
More informationSUPPLEMENTARY INFORMATION
do: 0.08/nature09 I. Resonant absorpton of XUV pulses n Kr + usng the reduced densty matrx approach The quantum beats nvestgated n ths paper are the result of nterference between two exctaton paths of
More information2 Finite difference basics
Numersche Methoden 1, WS 11/12 B.J.P. Kaus 2 Fnte dfference bascs Consder the one- The bascs of the fnte dfference method are best understood wth an example. dmensonal transent heat conducton equaton T
More informationComparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy
Comparatve Studes of Law of Conservaton of Energy and Law Clusters of Conservaton of Generalzed Energy No.3 of Comparatve Physcs Seres Papers Fu Yuhua (CNOOC Research Insttute, E-mal:fuyh1945@sna.com)
More informationSIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME. Abstract
SIMULATION OF SOUND WAVE PROPAGATION IN TURBULENT FLOWS USING A LATTICE-BOLTZMANN SCHEME PACS REFERENCE: 43.20.Mv Andreas Wlde Fraunhofer Insttut für Integrerte Schaltungen, Außenstelle EAS Zeunerstr.
More informationAppendix B. The Finite Difference Scheme
140 APPENDIXES Appendx B. The Fnte Dfference Scheme In ths appendx we present numercal technques whch are used to approxmate solutons of system 3.1 3.3. A comprehensve treatment of theoretcal and mplementaton
More informationCanonical transformations
Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,
More informationTitle: Radiative transitions and spectral broadening
Lecture 6 Ttle: Radatve transtons and spectral broadenng Objectves The spectral lnes emtted by atomc vapors at moderate temperature and pressure show the wavelength spread around the central frequency.
More informationUniqueness of Weak Solutions to the 3D Ginzburg- Landau Model for Superconductivity
Int. Journal of Math. Analyss, Vol. 6, 212, no. 22, 195-114 Unqueness of Weak Solutons to the 3D Gnzburg- Landau Model for Superconductvty Jshan Fan Department of Appled Mathematcs Nanjng Forestry Unversty
More informationIntroduction to the lattice Boltzmann method
Introducton to LB Introducton to the lattce Boltzmann method Burkhard Dünweg Max Planck Insttute for Polymer Research Ackermannweg 10, D-55128 Manz, Germany duenweg@mpp-manz.mpg.de Introducton Naver-Stokes
More informationPhysics 607 Exam 1. ( ) = 1, Γ( z +1) = zγ( z) x n e x2 dx = 1. e x2
Physcs 607 Exam 1 Please be well-organzed, and show all sgnfcant steps clearly n all problems. You are graded on your wor, so please do not just wrte down answers wth no explanaton! Do all your wor on
More informationSharp integral inequalities involving high-order partial derivatives. Journal Of Inequalities And Applications, 2008, v. 2008, article no.
Ttle Sharp ntegral nequaltes nvolvng hgh-order partal dervatves Authors Zhao, CJ; Cheung, WS Ctaton Journal Of Inequaltes And Applcatons, 008, v. 008, artcle no. 5747 Issued Date 008 URL http://hdl.handle.net/07/569
More informationPerfect Fluid Cosmological Model in the Frame Work Lyra s Manifold
Prespacetme Journal December 06 Volume 7 Issue 6 pp. 095-099 Pund, A. M. & Avachar, G.., Perfect Flud Cosmologcal Model n the Frame Work Lyra s Manfold Perfect Flud Cosmologcal Model n the Frame Work Lyra
More informationExistence of Two Conjugate Classes of A 5 within S 6. by Use of Character Table of S 6
Internatonal Mathematcal Forum, Vol. 8, 2013, no. 32, 1591-159 HIKARI Ltd, www.m-hkar.com http://dx.do.org/10.12988/mf.2013.3359 Exstence of Two Conjugate Classes of A 5 wthn S by Use of Character Table
More informationLecture 12: Discrete Laplacian
Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly
More informationResearch Article Relative Smooth Topological Spaces
Advances n Fuzzy Systems Volume 2009, Artcle ID 172917, 5 pages do:10.1155/2009/172917 Research Artcle Relatve Smooth Topologcal Spaces B. Ghazanfar Department of Mathematcs, Faculty of Scence, Lorestan
More informationBianchi Type V String Cosmological Model with Variable Deceleration Parameter
September 013 Volume 4 Issue 8 pp. 79-800 79 Banch Type V Strng Cosmologcal Model wth Varable Deceleraton Parameter Kanka Das * &Tazmn Sultana Department of Mathematcs, Gauhat Unversty, Guwahat-781014,
More informationDETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM
Ganj, Z. Z., et al.: Determnaton of Temperature Dstrbuton for S111 DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM by Davood Domr GANJI
More informationChapter 4 The Wave Equation
Chapter 4 The Wave Equaton Another classcal example of a hyperbolc PDE s a wave equaton. The wave equaton s a second-order lnear hyperbolc PDE that descrbes the propagaton of a varety of waves, such as
More informationResearch Article Møller s Energy in the Kantowski-Sachs Space-Time
Advances n Hgh Energy Physcs Volume 2010, Artcle ID 379473, 6 pages do:10.1155/2010/379473 Research Artcle Møller s Energy n the Kantowsk-Sachs Space-Tme M. Abdel-Meged and Ragab M. Gad Mathematcs Department,
More informationNumerical Solutions of a Generalized Nth Order Boundary Value Problems Using Power Series Approximation Method
Appled Mathematcs, 6, 7, 5-4 Publshed Onlne Jul 6 n ScRes. http://www.scrp.org/journal/am http://.do.org/.436/am.6.77 umercal Solutons of a Generalzed th Order Boundar Value Problems Usng Power Seres Approxmaton
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationModule 1 : The equation of continuity. Lecture 1: Equation of Continuity
1 Module 1 : The equaton of contnuty Lecture 1: Equaton of Contnuty 2 Advanced Heat and Mass Transfer: Modules 1. THE EQUATION OF CONTINUITY : Lectures 1-6 () () () (v) (v) Overall Mass Balance Momentum
More informationA Note on Bound for Jensen-Shannon Divergence by Jeffreys
OPEN ACCESS Conference Proceedngs Paper Entropy www.scforum.net/conference/ecea- A Note on Bound for Jensen-Shannon Dvergence by Jeffreys Takuya Yamano, * Department of Mathematcs and Physcs, Faculty of
More informationPower law and dimension of the maximum value for belief distribution with the max Deng entropy
Power law and dmenson of the maxmum value for belef dstrbuton wth the max Deng entropy Bngy Kang a, a College of Informaton Engneerng, Northwest A&F Unversty, Yanglng, Shaanx, 712100, Chna. Abstract Deng
More informationNON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS
IJRRAS 8 (3 September 011 www.arpapress.com/volumes/vol8issue3/ijrras_8_3_08.pdf NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS H.O. Bakodah Dept. of Mathematc
More informationWei, Jianguo; Wang, Song; Hou, Qingz Author(s) Jianwu. Mathematical Problems in Engineering Article ID
JAIST Repos https://dspace.j Ttle Generalzed Fnte Dfference Tme D and Its Applcaton to Acoustcs We, Janguo; Wang, Song; Hou, Qngz Author(s Janwu Ctaton Mathematcal Problems n Engneerng Artcle ID 6435 Issue
More informationA PROCEDURE FOR SIMULATING THE NONLINEAR CONDUCTION HEAT TRANSFER IN A BODY WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY.
Proceedngs of the th Brazlan Congress of Thermal Scences and Engneerng -- ENCIT 006 Braz. Soc. of Mechancal Scences and Engneerng -- ABCM, Curtba, Brazl,- Dec. 5-8, 006 A PROCEDURE FOR SIMULATING THE NONLINEAR
More informationInternational Conference on Advanced Computer Science and Electronics Information (ICACSEI 2013) equation. E. M. E. Zayed and S. A.
Internatonal Conference on Advanced Computer Scence and Electroncs Informaton (ICACSEI ) The two varable (G'/G/G) -expanson method for fndng exact travelng wave solutons of the (+) dmensonal nonlnear potental
More informationSolutions for Euler and Navier-Stokes Equations in Powers of Time
Solutons for Euler and Naver-Stokes Equatons n Powers of Tme Valdr Montero dos Santos Godo valdr.msgodo@gmal.com Abstract We present a soluton for the Euler and Naver-Stokes equatons for ncompressble case
More informationRate of Absorption and Stimulated Emission
MIT Department of Chemstry 5.74, Sprng 005: Introductory Quantum Mechancs II Instructor: Professor Andre Tokmakoff p. 81 Rate of Absorpton and Stmulated Emsson The rate of absorpton nduced by the feld
More informationThermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)
hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In
More informationLinear Approximation with Regularization and Moving Least Squares
Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...
More informationResearch Article Exact Partition Function for the Random Walk of an Electrostatic Field
Hndaw Advances n Mathematcal Physcs Volume 2017, Artcle ID 6970870, 5 pages https://do.org/10.1155/2017/6970870 Research Artcle Exact Partton Functon for the Random Walk of an Electrostatc Feld Gabrel
More informationSIMULATION OF WAVE PROPAGATION IN AN HETEROGENEOUS ELASTIC ROD
SIMUATION OF WAVE POPAGATION IN AN HETEOGENEOUS EASTIC OD ogéro M Saldanha da Gama Unversdade do Estado do o de Janero ua Sào Francsco Xaver 54, sala 5 A 559-9, o de Janero, Brasl e-mal: rsgama@domancombr
More informationA NUMERICAL COMPARISON OF LANGRANGE AND KANE S METHODS OF AN ARM SEGMENT
Internatonal Conference Mathematcal and Computatonal ology 0 Internatonal Journal of Modern Physcs: Conference Seres Vol. 9 0 68 75 World Scentfc Publshng Company DOI: 0.4/S009450059 A NUMERICAL COMPARISON
More informationCOMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD
COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,
More informationLecture Notes on Linear Regression
Lecture Notes on Lnear Regresson Feng L fl@sdueducn Shandong Unversty, Chna Lnear Regresson Problem In regresson problem, we am at predct a contnuous target value gven an nput feature vector We assume
More informationA Computational Viewpoint on Classical Density Functional Theory
A Computatonal Vewpont on Classcal Densty Functonal Theory Matthew Knepley and Drk Gllespe Computaton Insttute Unversty of Chcago Department of Molecular Bology and Physology Rush Unversty Medcal Center
More informationOptimal Control of Temperature in Fluid Flow
Kawahara Lab. 5 March. 27 Optmal Control of Temperature n Flud Flow Dasuke YAMAZAKI Department of Cvl Engneerng, Chuo Unversty Kasuga -3-27, Bunkyou-ku, Tokyo 2-855, Japan E-mal : d33422@educ.kc.chuo-u.ac.jp
More informationHYBRID LBM-FVM AND LBM-MCM METHODS FOR FLUID FLOW AND HEAT TRANSFER SIMULATION
HYBRID LBM-FVM AND LBM-MCM METHODS FOR FLUID FLOW AND HEAT TRANSFER SIMULATION Zheng L a,b, Mo Yang b and Yuwen Zhang a* a Department of Mechancal and Aerospace Engneerng, Unversty of Mssour, Columba,
More informationPHYS 705: Classical Mechanics. Canonical Transformation II
1 PHYS 705: Classcal Mechancs Canoncal Transformaton II Example: Harmonc Oscllator f ( x) x m 0 x U( x) x mx x LT U m Defne or L p p mx x x m mx x H px L px p m p x m m H p 1 x m p m 1 m H x p m x m m
More informationThe Finite Element Method
The Fnte Element Method GENERAL INTRODUCTION Read: Chapters 1 and 2 CONTENTS Engneerng and analyss Smulaton of a physcal process Examples mathematcal model development Approxmate solutons and methods of
More informationTransfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system
Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng
More informationUPGRADE OF THE GSP GYROKINETIC CODE MID-YEAR PROGRESS REPORT
12/6/211 1 UPGRADE OF THE GSP GYROKINETIC CODE MID-YEAR PROGRESS REPORT George Wlke gwlke@umd.edu December 6, 211 Supersor: Wllam Dorland, Dept. of Physcs bdorland@umd.edu Abstract: Smulatons of turbulent
More informationLattice Boltzmann Method and its Application to Flow Analysis in Porous Media
Specal Issue Multscale Smulatons for Materals 7 Research Report Lattce Boltzmann Method and ts Applcaton to Flow Analyss n Porous Meda Hdemtsu Hayash Abstract Under the exstence of an external force, a
More informationLecture 20: Noether s Theorem
Lecture 20: Noether s Theorem In our revew of Newtonan Mechancs, we were remnded that some quanttes (energy, lnear momentum, and angular momentum) are conserved That s, they are constant f no external
More informationNon-interacting Spin-1/2 Particles in Non-commuting External Magnetic Fields
EJTP 6, No. 0 009) 43 56 Electronc Journal of Theoretcal Physcs Non-nteractng Spn-1/ Partcles n Non-commutng External Magnetc Felds Kunle Adegoke Physcs Department, Obafem Awolowo Unversty, Ile-Ife, Ngera
More informationA micro-macro decomposition based asymptotic-preserving scheme for the multispecies Boltzmann equation
A mcro-macro decomposton based asymptotc-preservng scheme for the multspeces Boltzmann equaton Sh Jn Yngzhe Sh Abstract In ths paper we extend the mcro-macro decomposton based asymptotc-preservng scheme
More informationA new Approach for Solving Linear Ordinary Differential Equations
, ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of
More informationApplication of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems
Mathematca Aeterna, Vol. 1, 011, no. 06, 405 415 Applcaton of B-Splne to Numercal Soluton of a System of Sngularly Perturbed Problems Yogesh Gupta Department of Mathematcs Unted College of Engneerng &
More informationDUE: WEDS FEB 21ST 2018
HOMEWORK # 1: FINITE DIFFERENCES IN ONE DIMENSION DUE: WEDS FEB 21ST 2018 1. Theory Beam bendng s a classcal engneerng analyss. The tradtonal soluton technque makes smplfyng assumptons such as a constant
More informationNumerical Solution of Boussinesq Equations as a Model of Interfacial-wave Propagation
BULLETIN of the Malaysan Mathematcal Scences Socety http://math.usm.my/bulletn Bull. Malays. Math. Sc. Soc. (2) 28(2) (2005), 163 172 Numercal Soluton of Boussnesq Equatons as a Model of Interfacal-wave
More informationTHEOREMS OF QUANTUM MECHANICS
THEOREMS OF QUANTUM MECHANICS In order to develop methods to treat many-electron systems (atoms & molecules), many of the theorems of quantum mechancs are useful. Useful Notaton The matrx element A mn
More informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationχ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body
Secton.. Moton.. The Materal Body and Moton hyscal materals n the real world are modeled usng an abstract mathematcal entty called a body. Ths body conssts of an nfnte number of materal partcles. Shown
More informationElectron-Impact Double Ionization of the H 2
I R A P 6(), Dec. 5, pp. 9- Electron-Impact Double Ionzaton of the H olecule Internatonal Scence Press ISSN: 9-59 Electron-Impact Double Ionzaton of the H olecule. S. PINDZOLA AND J. COLGAN Department
More informationCHAPTER 14 GENERAL PERTURBATION THEORY
CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves
More informationErrors in Nobel Prize for Physics (7) Improper Schrodinger Equation and Dirac Equation
Errors n Nobel Prze for Physcs (7) Improper Schrodnger Equaton and Drac Equaton u Yuhua (CNOOC Research Insttute, E-mal:fuyh945@sna.com) Abstract: One of the reasons for 933 Nobel Prze for physcs s for
More informationIntegrals and Invariants of Euler-Lagrange Equations
Lecture 16 Integrals and Invarants of Euler-Lagrange Equatons ME 256 at the Indan Insttute of Scence, Bengaluru Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng,
More informationLecture 21: Numerical methods for pricing American type derivatives
Lecture 21: Numercal methods for prcng Amercan type dervatves Xaoguang Wang STAT 598W Aprl 10th, 2014 (STAT 598W) Lecture 21 1 / 26 Outlne 1 Fnte Dfference Method Explct Method Penalty Method (STAT 598W)
More informationChapter 12. Ordinary Differential Equation Boundary Value (BV) Problems
Chapter. Ordnar Dfferental Equaton Boundar Value (BV) Problems In ths chapter we wll learn how to solve ODE boundar value problem. BV ODE s usuall gven wth x beng the ndependent space varable. p( x) q(
More informationStatistical inference for generalized Pareto distribution based on progressive Type-II censored data with random removals
Internatonal Journal of Scentfc World, 2 1) 2014) 1-9 c Scence Publshng Corporaton www.scencepubco.com/ndex.php/ijsw do: 10.14419/jsw.v21.1780 Research Paper Statstcal nference for generalzed Pareto dstrbuton
More informationLattice Boltzmann Method in Theory and in Application to Coupled Problems
Lattce Boltzmann Method n Theory and n Applcaton to Coupled Problems Master Thess Danel Heubes supervsng Prof. Dr. Mchael Günther Dr. Andreas Bartel Unversty of Wuppertal Faculty of Mathematcs and Natural
More information2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification
E395 - Pattern Recognton Solutons to Introducton to Pattern Recognton, Chapter : Bayesan pattern classfcaton Preface Ths document s a soluton manual for selected exercses from Introducton to Pattern Recognton
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION
Advanced Mathematcal Models & Applcatons Vol.3, No.3, 2018, pp.215-222 ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EUATION
More informationCONTROLLED FLOW SIMULATION USING SPH METHOD
HERI COADA AIR FORCE ACADEMY ROMAIA ITERATIOAL COFERECE of SCIETIFIC PAPER AFASES 01 Brasov, 4-6 May 01 GEERAL M.R. STEFAIK ARMED FORCES ACADEMY SLOVAK REPUBLIC COTROLLED FLOW SIMULATIO USIG SPH METHOD
More informationThe Two-scale Finite Element Errors Analysis for One Class of Thermoelastic Problem in Periodic Composites
7 Asa-Pacfc Engneerng Technology Conference (APETC 7) ISBN: 978--6595-443- The Two-scale Fnte Element Errors Analyss for One Class of Thermoelastc Problem n Perodc Compostes Xaoun Deng Mngxang Deng ABSTRACT
More informationarxiv: v1 [math.ho] 18 May 2008
Recurrence Formulas for Fbonacc Sums Adlson J. V. Brandão, João L. Martns 2 arxv:0805.2707v [math.ho] 8 May 2008 Abstract. In ths artcle we present a new recurrence formula for a fnte sum nvolvng the Fbonacc
More informationResearch Article The Solution of Two-Point Boundary Value Problem of a Class of Duffing-Type Systems with Non-C 1 Perturbation Term
Hndaw Publshng Corporaton Boundary Value Problems Volume 9, Artcle ID 87834, 1 pages do:1.1155/9/87834 Research Artcle The Soluton of Two-Pont Boundary Value Problem of a Class of Duffng-Type Systems wth
More informationVisco-Rubber Elastic Model for Pressure Sensitive Adhesive
Vsco-Rubber Elastc Model for Pressure Senstve Adhesve Kazuhsa Maeda, Shgenobu Okazawa, Koj Nshgch and Takash Iwamoto Abstract A materal model to descrbe large deformaton of pressure senstve adhesve (PSA
More informationSpin-rotation coupling of the angularly accelerated rigid body
Spn-rotaton couplng of the angularly accelerated rgd body Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 E-mal: louaelzen@gmal.com November 1, 2017 All Rghts Reserved. Abstract Ths paper s
More information