The Discretization Process
|
|
- Gwenda Williams
- 5 years ago
- Views:
Transcription
1 FMIA F Moukalled L Mangan M Darwsh An Advanced Introducton wth OpenFOAM and Matlab Ths textbook explores both the theoretcal foundaton of the Fnte Volume Method (FVM) and ts applcatons n Computatonal Flud Dynamcs (CFD) Readers wll dscover a thorough explanaton of the FVM numercs and algorthms used n the smulaton of ncompressble and compressble flud flows, along wth a detaled examnaton of the components needed for the development of a collocated unstructured pressure-based CFD solver Two partcular CFD codes are explored The frst s ufvm, a three-dmensonal unstructured pressure-based fnte volume academc CFD code, mplemented wthn Matlab The second s OpenFOAM, an open source framework used n the development of a range of CFD programs for the smulaton of ndustral scale flow problems Moukalled Mangan Darwsh Flud Mechancs and Its Applcatons 113 Seres Edtor: A Thess The Fnte Volume Method n Computatonal Flud Dynamcs Wth over 220 fgures, numerous examples and more than one hundred exercses on FVM numercs, programmng, and applcatons, ths textbook s sutable for use n an ntroductory course on the FVM, n an advanced course on CFD algorthms, and as a reference for CFD programmers and researchers Flud Mechancs and Its Applcatons F Moukalled L Mangan M Darwsh The Fnte Volume Method n Computatonal Flud Dynamcs The Fnte Volume Method n Computatonal Flud Dynamcs An Advanced Introducton wth OpenFOAM and Matlab Engneerng ISBN The Dscretzaton Process Chapter 04
2 The Dscretzaton Process
3 The Process Physcal Doman Physcal Phenomena Doman Modelng Physcal Modelng Set of Governng Equatons Defned on omputatonal Doman Doman Dscretzaton Equaton Dscretzaton Structured Grds Cartesan, Non-Orthogonal) Block Structured grds Unstructured Grds Chmera Grds System of Algebrac Equatons Fnte Dfference Fnte Volume Fnte Element Boundary Element Numercal Solutons Soluton Method Combnatons of Multgrd Methods Iteratve Solvers Coupled-Uncoupled 3
4 Doman Modelng Physcal Modelng heat snk heat spreader base Tsnk Insulated ( k T ) = Q Q smk mcroprocessor Tmcroprocessor Q source Doman Dscretzaton Equatons Dscretzaton ρφ + ( ρvφ) t = ( Γ φ ) + Q transent term convecton term φ C + dffuson term NB( C) source term a NB φ NB = b P Soluton Method = 4
5 Doman Dscretzaton T snk nsulated T mcroprocessor 5
6 Numberng F 2 F 3 C F 4 F 1 Element 9 Connectvty Neghbours Faces Vertces [ ] [ ] [ ] E S 1 f E f 2 owner neghbour Face 12 Connectvty Element1 9 Element2 10 Vertces [19 12] Vertex Connectvty Elements [ ] Faces [ ] 6
7 Sparse Matrx Equaton Element 3 Neghbors 1 local element equaton s assemble for element 3 element connectvty s used to transform local ndces to global ndces T C + a F1 T F1 + a F2 T F2 + a F3 T F3 = b C a F 1 F 2 F 3 33 T 3 + a 32 T 2 + a 35 T 5 + a 31 T 1 = b a N3 a N1 a N2 element equaton s assembled nto global matrx 3 = 7
8 Element Felds Element Feld nteror patch#1 patch#2 patch#
9 Equaton Dscretzaton x F 2 f 2 F F 3 C f 3 f 1 F f 1 4 δ y f 2 S f F 4 F 3 f 3 C S f1 F 1 y S f3 f 1 S f4 f 4 F 4 δ x ( k T ) = 0 ( k T ) ds ( k T ) f S f = 0 S C! = 0 f C S f1 δ x f1 T f1 = y f1 = x N1 x C = T x + T y j ( k T ) f1 S f1 ( k T ) f2 S f2 ( k T ) f3 S f3 ( k T ) f4 S f4 = 0 9
10 Coeffcents x F 2 T f1 S f1 = T x + T y j y f1 f 1 δ y F 3 f 3 S f3 f 2 C S f2 S f1 f 1 F 1 y = T x y f1 f 1 S f4 F 4 f 4 δ x T x f 1 = T N1 T C δ x f1 T f1 S f1 = T F 1 T C y f1 ( k T ) δ x f1 S f1 = a F1 T F1 T C f1 a F1 = k y f 1 δ x f1 10
11 Algebrac Equaton F 2 a F2 = k x f 2 δ y f2 f 2 4 S f2 a F3 = k y f 3 δ x f3 F 3 8 f 3 S f3 C 9 S f1 f 1 10 F 1 S f4 f 4 a F4 = k x f 4 δ y f4 F = ( k T ) f S f = a NB T NB T C f C NB C = ( a F1 + a F2 + a F3 + a F4 )T C + a F1 T F1 + a F2 T F2 + a F3 T F3 + a F4 T F4 T C + a NB T NB = 0 NB C = NB C a NB = ( a F1 + a F2 + a F3 + a F4 ) 11
12 System of Equatons Element 3 Neghbors 1 local element equaton s assemble for element 3 element connectvty s used to transform local ndces to global ndces T C + a F1 T F1 + a F2 T F2 + a F3 T F3 2 = b C a F 1 F 2 F 3 33 T 3 + a 32 T 2 + a 35 T 5 + a 31 T 1 = b 3 a N3 a N1 a N2 element equaton s assembled nto global matrx 3 = 12
13 Solvng the Equatons 13 T C = a NB T NB NB(C ) + b C =
14 Face Feld Face Feld nteror patch#1 patch#2 patch# S f d CF g CF S f 14
15 Node feld Vertex Feld nteror patch#1 patch#2 patch#
The Finite Volume Mesh
FMIA F Moukalled L Mangani M Darwish An Advanced Introduction with OpenFOAM and Matlab This textbook explores both the theoretical foundation of the Finite Volume Method (FVM) and its applications in Computational
More informationThe Finite Volume Method in
FMIA F Moukalled L Mangani M Darwish An Advanced Introduction with OpenFOAM and Matlab This textbook explores both the theoretical oundation o the Finite Volume Method (FVM) and its applications in omputational
More informationTransient, Source Terms and Relaxation
F. Moukalled L. Mangani M. Darwish An Advanced Introduction with OpenFOAM and Matlab This textbook explores both the theoretical foundation of the Finite Volume Method (FVM) and its applications in Computational
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 informationSolving the Navier-Stokes Equations
FMIA F. Moukalled L. Mangani M. Darwish An Advanced Introduction with OpenFOAM and Matlab This textbook explores both the theoretical oundation o the Finite Volume Method (FVM) and its applications in
More informationPART 8. Partial Differential Equations PDEs
he Islamc Unverst of Gaza Facult of Engneerng Cvl Engneerng Department Numercal Analss ECIV 3306 PAR 8 Partal Dfferental Equatons PDEs Chapter 9; Fnte Dfference: Ellptc Equatons Assocate Prof. Mazen Abualtaef
More informationIntroduction to Computational Fluid Dynamics
Introducton to Computatonal Flud Dynamcs M. Zanub 1, T. Mahalakshm 2 1 (PG MATHS), Department of Mathematcs, St. Josephs College of Arts and Scence for Women-Hosur, Peryar Unversty 2 Assstance professor,
More informationFTCS Solution to the Heat Equation
FTCS Soluton to the Heat Equaton ME 448/548 Notes Gerald Recktenwald Portland State Unversty Department of Mechancal Engneerng gerry@pdx.edu ME 448/548: FTCS Soluton to the Heat Equaton Overvew 1. Use
More informationRelaxation Methods for Iterative Solution to Linear Systems of Equations
Relaxaton Methods for Iteratve Soluton to Lnear Systems of Equatons Gerald Recktenwald Portland State Unversty Mechancal Engneerng Department gerry@pdx.edu Overvew Techncal topcs Basc Concepts Statonary
More informationA new integrated-rbf-based domain-embedding scheme for solving fluid-flow problems
Home Search Collectons Journals About Contact us My IOPscence A new ntegrated-rbf-based doman-embeddng scheme for solvng flud-flow problems Ths artcle has been downloaded from IOPscence. Please scroll
More informationResearch & Reviews: Journal of Engineering and Technology
Research & Revews: Journal of Engneerng and Technology Case Study to Smulate Convectve Flows and Heat Transfer n Arcondtoned Spaces Hussen JA 1 *, Mazlan AW 1 and Hasanen MH 2 1 Department of Mechancal
More informationLecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES
COMPUTATIONAL FLUID DYNAMICS: FDM: Appromaton of Second Order Dervatves Lecture APPROXIMATION OF SECOMD ORDER DERIVATIVES. APPROXIMATION OF SECOND ORDER DERIVATIVES Second order dervatves appear n dffusve
More informationCalculation of Aerodynamic Characteristics of NACA 2415, 23012, Airfoils Using Computational Fluid Dynamics (CFD)
Calculaton of Aerodynamc Characterstcs of NACA 2415, 23012, 23015 Arfols Usng Computatonal Flud Dynamcs (CFD) Hmanshu Parashar Abstract A method of solvng the flow over arfols of Natonal Advsory Commttee
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 informationGrid Generation around a Cylinder by Complex Potential Functions
Research Journal of Appled Scences, Engneerng and Technolog 4(): 53-535, 0 ISSN: 040-7467 Mawell Scentfc Organzaton, 0 Submtted: December 0, 0 Accepted: Januar, 0 Publshed: June 0, 0 Grd Generaton around
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 informationElectrical Circuits 2.1 INTRODUCTION CHAPTER
CHAPTE Electrcal Crcuts. INTODUCTION In ths chapter, we brefly revew the three types of basc passve electrcal elements: resstor, nductor and capactor. esstance Elements: Ohm s Law: The voltage drop across
More informationA Numerical Study of Heat Transfer and Fluid Flow past Single Tube
A Numercal Study of Heat ransfer and Flud Flow past Sngle ube ZEINAB SAYED ABDEL-REHIM Mechancal Engneerng Natonal Research Center El-Bohos Street, Dokk, Gza EGYP abdelrehmz@yahoo.com Abstract: - A numercal
More information2.29 Numerical Fluid Mechanics Fall 2011 Lecture 12
REVIEW Lecture 11: 2.29 Numercal Flud Mechancs Fall 2011 Lecture 12 End of (Lnear) Algebrac Systems Gradent Methods Krylov Subspace Methods Precondtonng of Ax=b FINITE DIFFERENCES Classfcaton of Partal
More informationSTUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS
Blucher Mechancal Engneerng Proceedngs May 0, vol., num. www.proceedngs.blucher.com.br/evento/0wccm STUDY ON TWO PHASE FLOW IN MICRO CHANNEL BASED ON EXPERI- MENTS AND NUMERICAL EXAMINATIONS Takahko Kurahash,
More informationIC Engine Flow Simulation using KIVA code and A Modified Reynolds Stress Turbulence Model
IC Engne Flow Smulaton usng KIVA code and A Modfed Reynolds Stress Turbulence Model Satpreet Nanda and S.L. Yang Mechancal Engneerng-Engneerng Mechancs Department Mchgan Technologcal Unversty Houghton,
More informationNew Method for Solving Poisson Equation. on Irregular Domains
Appled Mathematcal Scences Vol. 6 01 no. 8 369 380 New Method for Solvng Posson Equaton on Irregular Domans J. Izadan and N. Karamooz Department of Mathematcs Facult of Scences Mashhad BranchIslamc Azad
More informationAdditional Codes using Finite Difference Method. 1 HJB Equation for Consumption-Saving Problem Without Uncertainty
Addtonal Codes usng Fnte Dfference Method Benamn Moll 1 HJB Equaton for Consumpton-Savng Problem Wthout Uncertanty Before consderng the case wth stochastc ncome n http://www.prnceton.edu/~moll/ HACTproect/HACT_Numercal_Appendx.pdf,
More informationFMIA. Fluid Mechanics and Its Applications 113 Series Editor: A. Thess. Moukalled Mangani Darwish. F. Moukalled L. Mangani M.
FMIA F. Moukalled L. Mangani M. Darwish An Advanced Introduction with OpenFOAM and Matlab This textbook explores both the theoretical foundation of the Finite Volume Method (FVM) and its applications in
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 information1-Dimensional Advection-Diffusion Finite Difference Model Due to a Flow under Propagating Solitary Wave
014 4th Internatonal Conference on Future nvronment and nergy IPCB vol.61 (014) (014) IACSIT Press, Sngapore I: 10.776/IPCB. 014. V61. 6 1-mensonal Advecton-ffuson Fnte fference Model ue to a Flow under
More information2.29 Numerical Fluid Mechanics Fall 2011 Lecture 6
REVIEW of Lecture 5 2.29 Numercal Flud Mechancs Fall 2011 Lecture 6 Contnuum Hypothess and conservaton laws Macroscopc Propertes Materal covered n class: Dfferental forms of conservaton laws Materal Dervatve
More informationFinding The Rightmost Eigenvalues of Large Sparse Non-Symmetric Parameterized Eigenvalue Problem
Fndng he Rghtmost Egenvalues of Large Sparse Non-Symmetrc Parameterzed Egenvalue Problem Mnghao Wu AMSC Program mwu@math.umd.edu Advsor: Professor Howard Elman Department of Computer Scences elman@cs.umd.edu
More informationNodal analysis of finite square resistive grids and the teaching effectiveness of students projects
2 nd World Conference on Technology and Engneerng Educaton 2 WIETE Lublana Slovena 5-8 September 2 Nodal analyss of fnte square resstve grds and the teachng effectveness of students proects P. Zegarmstrz
More informationTHE STURM-LIOUVILLE EIGENVALUE PROBLEM - A NUMERICAL SOLUTION USING THE CONTROL VOLUME METHOD
Journal of Appled Mathematcs and Computatonal Mechancs 06, 5(), 7-36 www.amcm.pcz.pl p-iss 99-9965 DOI: 0.75/jamcm.06..4 e-iss 353-0588 THE STURM-LIOUVILLE EIGEVALUE PROBLEM - A UMERICAL SOLUTIO USIG THE
More informationINTERROGATING THE FLOW BEHAVIOUR IN A NOVEL MAGNETIC DESICCANT VENTILATION SYSTEM USING COMPUTATIONAL FLUID DYNAMICS (CFD)
INTERROGATING THE FLOW BEHAVIOUR IN A NOVEL MAGNETIC DESICCANT VENTILATION SYSTEM USING COMPUTATIONAL FLUID DYNAMICS (CFD) Auwal Dodo*, Valente Hernandez-Perez, Je Zhu and Saffa Rffat Faculty of Engneerng,
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 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 information2.29 Numerical Fluid Mechanics
REVIEW Lecture 10: Sprng 2015 Lecture 11 Classfcaton of Partal Dfferental Equatons PDEs) and eamples wth fnte dfference dscretzatons Parabolc PDEs Ellptc PDEs Hyperbolc PDEs Error Types and Dscretzaton
More informationInterconnect Modeling
Interconnect Modelng Modelng of Interconnects Interconnect R, C and computaton Interconnect models umped RC model Dstrbuted crcut models Hgher-order waveform n dstrbuted RC trees Accuracy and fdelty Prepared
More informationHigher Order Wall Boundary Conditions for Incompressible Flow Simulations
THE 5 TH ASIAN COMPUTAITIONAL FLUID DYNAMICS BUSAN KOREA OCTOBER 7-30 003 Hgher Order Wall Boundary Condtons for Incompressble Flow Smulatons Hdetosh Nshda. Department of Mechancal and System Engneerng
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 informationImprovement of the numerical framework for selective catalytic reduction applications
Improvement of the numercal framework for selectve catalytc reducton applcatons J. Baleta,1, M. Vuanovć 1, N. Duć 1, K. Pachler, D. Schellander 1 Faculty of Mechancal Engneerng and Naval Archtecture, Unversty
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 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 informationSimulation of Turbulent Flow Using FEM
Internatonal Journal of Engneerng and Technology Volume 2 No. 8, August, 2012 Smulaton of Turbulent Flow Usng FEM Sabah Tamm College of Computng, AlGhurar Unversty, Duba, Unted Arab Emrates. ABSTRACT An
More informationTHE NEAR-WALL INFLUENCE ON THE FLOW AROUND A SINGLE SQUARE CYLINDER.
THE NEAR-WALL INFLUENCE ON THE FLOW AROUND A SINGLE SQUARE CYLINDER. Campregher, Rubens Faculty of Mechancal Engneerng, FEMEC Federal Unversty of Uberlânda, UFU 38400-902 Uberlânda - Brazl campregher@mecanca.ufu.br
More informationImposition of the essential boundary conditions in transient heat conduction problem based on Isogeometric analysis
Imposton of the essental boundary condtons n transent heat conducton problem based on Isogeometrc analyss S. Shojaee, E. Izadpanah, S. Nazar Department of Cvl Engneerng, Shahd Bahonar Unversty, Kerman,
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 informationOn a direct solver for linear least squares problems
ISSN 2066-6594 Ann. Acad. Rom. Sc. Ser. Math. Appl. Vol. 8, No. 2/2016 On a drect solver for lnear least squares problems Constantn Popa Abstract The Null Space (NS) algorthm s a drect solver for lnear
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 informationSolution of the Navier-Stokes Equations
Numercal Flud Mechancs Fall 2011 Lecture 25 REVIEW Lecture 24: Soluton of the Naver-Stokes Equatons Dscretzaton of the convectve and vscous terms Dscretzaton of the pressure term Conservaton prncples Momentum
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 two dimensional coupled viscous Burgers Equation using the Modified Cubic B-Spline Differential Quadrature Method
umercal Soluton of two dmensonal coupled vscous Burgers Equaton usng the odfed Cubc B-Splne Dfferental Quadrature ethod H. S. Shukla 1, ohammad Tamsr 1*, Vneet K. Srvastava, Ja Kumar 3 1 Department of
More informationApplication of Finite Element Method (FEM) Instruction to Graduate Courses in Biological and Agricultural Engineering
Sesson: 08 Applcaton of Fnte Element Method (FEM) Instructon to Graduate Courses n Bologcal and Agrcultural Engneerng Chang S. Km, Terry H. Walker, Caye M. Drapcho Dept. of Bologcal and Agrcultural Engneerng
More informationU.C. Berkeley CS278: Computational Complexity Professor Luca Trevisan 2/21/2008. Notes for Lecture 8
U.C. Berkeley CS278: Computatonal Complexty Handout N8 Professor Luca Trevsan 2/21/2008 Notes for Lecture 8 1 Undrected Connectvty In the undrected s t connectvty problem (abbrevated ST-UCONN) we are gven
More informationMaejo International Journal of Science and Technology
Maejo Int. J. Sc. Technol. () - Full Paper Maejo Internatonal Journal of Scence and Technology ISSN - Avalable onlne at www.mjst.mju.ac.th Fourth-order method for sngularly perturbed sngular boundary value
More informationNumerical Transient Heat Conduction Experiment
Numercal ransent Heat Conducton Experment OBJECIVE 1. o demonstrate the basc prncples of conducton heat transfer.. o show how the thermal conductvty of a sold can be measured. 3. o demonstrate the use
More informationApplication of the lattice Boltzmann method for solving conduction problems with heat flux boundary condition.
November 5-7, 9 - Sousse Tunsa Applcaton of the lattce Boltzmann method for solvng conducton problems wth heat flux boundary condton. Raoudha CHAABANE, Faouz ASKRI, Sass Ben NASRALLAH Laboratore d Etudes
More informationTHE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD
Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS
More informationField computation with finite element method applied for diagnosis eccentricity fault in induction machine
Proceedngs of the Internatonal Conference on Recent Advances n Electrcal Systems, Tunsa, 216 Feld computaton wth fnte element method appled for dagnoss eccentrcty fault n nducton machne Moufd Mohammed,
More informationCOMPUTATIONAL METHODS AND ALGORITHMS Vol. II - Finite Element Method - Jacques-Hervé SAIAC
COMPUTATIONAL METHODS AND ALGORITHMS Vol. II - Fnte Element Method - Jacques-Hervé SAIAC FINITE ELEMENT METHOD Jacques-Hervé SAIAC Départment de Mathématques, Conservatore Natonal des Arts et Méters, Pars,
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 informationAn Experimental and Numerical Study on Pressure Drop Coefficient of Ball Valves
A. Ozdomar, K. Turgut Gursel, Y. Pekbey, B. Celkag / Internatonal Energy Journal 8 (2007) An Expermental and Numercal Study on Pressure Drop Coeffcent of Ball Valves www.serd.at.ac.th/rerc A. Ozdamar*
More informationTurbulence and its Modelling
School of Mechancal Aerospace and Cvl Engneerng 3rd Year Flud Mechancs Introducton In earler lectures we have consdered how flow nstabltes develop, and noted that above some crtcal Reynolds number flows
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 informationComputational Fluid Dynamics. Smoothed Particle Hydrodynamics. Simulations. Smoothing Kernels and Basis of SPH
Computatonal Flud Dynamcs If you want to learn a bt more of the math behnd flud dynamcs, read my prevous post about the Naver- Stokes equatons and Newtonan fluds. The equatons derved n the post are the
More informationNUMERICAL MODEL FOR NON-DARCY FLOW THROUGH COARSE POROUS MEDIA USING THE MOVING PARTICLE SIMULATION METHOD
THERMAL SCIENCE: Year 2018, Vol. 22, No. 5, pp. 1955-1962 1955 NUMERICAL MODEL FOR NON-DARCY FLOW THROUGH COARSE POROUS MEDIA USING THE MOVING PARTICLE SIMULATION METHOD Introducton by Tomok IZUMI a* and
More informationNumerical Simulation of One-Dimensional Wave Equation by Non-Polynomial Quintic Spline
IOSR Journal of Matematcs (IOSR-JM) e-issn: 78-578, p-issn: 319-765X. Volume 14, Issue 6 Ver. I (Nov - Dec 018), PP 6-30 www.osrournals.org Numercal Smulaton of One-Dmensonal Wave Equaton by Non-Polynomal
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 informationSolving Fractional Nonlinear Fredholm Integro-differential Equations via Hybrid of Rationalized Haar Functions
ISSN 746-7659 England UK Journal of Informaton and Computng Scence Vol. 9 No. 3 4 pp. 69-8 Solvng Fractonal Nonlnear Fredholm Integro-dfferental Equatons va Hybrd of Ratonalzed Haar Functons Yadollah Ordokhan
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 informationAirflow and Contaminant Simulation with CONTAM
Arflow and Contamnant Smulaton wth CONTAM George Walton, NIST CHAMPS Developers Workshop Syracuse Unversty June 19, 2006 Network Analogy Electrc Ppe, Duct & Ar Wre Ppe, Duct, or Openng Juncton Juncton
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 informationSurvey of applications of discrete vortex method in civil engineering
Budownctwo Archtektura 5 (2009) 29-38 Survey of applcatons of dscrete vortex method n cvl engneerng Tomasz Nowck Lubln Unversty of Technology, Faculty of Cvl Engneerng and Archtecture, Department of Structural
More informationA Cartesian-grid integrated-rbf method for viscoelastic flows
Home Search Collectons Journals About Contact us My IOPscence A Cartesan-grd ntegrated-rbf method for vscoelastc flows Ths artcle has been downloaded from IOPscence. Please scroll down to see the full
More informationComputational Electromagnetics in Antenna Analysis and Design
Computatonal Electromagnetcs n Antenna Analyss and Desgn Introducton It s rare for real-lfe EM problems to fall neatly nto a class that can be solved by the analytcal methods presented n the precedng lectures.
More informationDESIGN OF CONTROL PROCESSES IN DPS BLOCKSET FOR MATLAB & SIMULINK
DESIGN OF CONTROL PROCESSES IN DPS BLOCKSET FOR MATLAB & SIMULINK C. Belavý, G. Hulkó, M. Mchalečko, V. Ivanov Department of Automaton, Informatcs and Instrumentaton, Faculty of Mechancal Engneerng, Slovak
More informationDynamic Programming 4/5/12. Dynamic programming. Fibonacci numbers. Fibonacci: a first attempt. David Kauchak cs302 Spring 2012
Dynamc Programmng Davd Kauchak cs32 Sprng 212 Dynamc programmng l One of the most mportant algorthm tools! l Very common ntervew queston l Method for solvng problems where optmal solutons can be defned
More informationImplicit Integration Henyey Method
Implct Integraton Henyey Method In realstc stellar evoluton codes nstead of a drect ntegraton usng for example the Runge-Kutta method one employs an teratve mplct technque. Ths s because the structure
More informationA large scale tsunami run-up simulation and numerical evaluation of fluid force during tsunami by using a particle method
A large scale tsunam run-up smulaton and numercal evaluaton of flud force durng tsunam by usng a partcle method *Mtsuteru Asa 1), Shoch Tanabe 2) and Masaharu Isshk 3) 1), 2) Department of Cvl Engneerng,
More informationHybrid FDTD/FETD Technique Using Parametric Quadratic Programming for Nonlinear Maxwell s Equations
Progress In Electromagnetcs Research M, Vol. 54, 113 123, 217 Hybrd FDTD/FETD Technque Usng Parametrc Quadratc Programmng for Nonlnear Maxwell s Equatons Hongxa L 1,BaoZhu 2 and Jefu Chen 3, * Abstract
More informationCOMPUTATIONAL STUDY OF SUPERSONIC FLOW THROUGH A CONVERGING DIVERGING NOZZLE
Engneerng e-transacton (ISSN 183-6379) Vol. 6, No. 1, June 011, pp 37-4 Onlne at http://eum.fsktm.um.edu.my Receved 5 October, 010; Accepted 30 December, 010 COMPUTATIONAL STUDY OF SUPERSONIC FLOW THROUGH
More informationHigh resolution entropy stable scheme for shallow water equations
Internatonal Symposum on Computers & Informatcs (ISCI 05) Hgh resoluton entropy stable scheme for shallow water equatons Xaohan Cheng,a, Yufeng Ne,b, Department of Appled Mathematcs, Northwestern Polytechncal
More informationA constant recursive convolution technique for frequency dependent scalar wave equation based FDTD algorithm
J Comput Electron (213) 12:752 756 DOI 1.17/s1825-13-479-2 A constant recursve convoluton technque for frequency dependent scalar wave equaton bed FDTD algorthm M. Burak Özakın Serkan Aksoy Publshed onlne:
More informationNUMERICAL MODELLING OF TSUNAMI WAVE EQUATIONS MASTER OF SCIENCE IN MATHEMATICS
NUMERICAL MODELLING OF TSUNAMI WAVE EQUATIONS A thess submtted n partal fulfllment of the requrements for the award of the degree of MASTER OF SCIENCE IN MATHEMATICS submtted by HARI SHANKAR SHAW Roll
More informationME 501A Seminar in Engineering Analysis Page 1
umercal Solutons of oundary-value Problems n Os ovember 7, 7 umercal Solutons of oundary- Value Problems n Os Larry aretto Mechancal ngneerng 5 Semnar n ngneerng nalyss ovember 7, 7 Outlne Revew stff equaton
More informationCOMPUTATIONAL FLUID DYNAMICS ME G515
BITS Plan Duba Campus COMPUTATIONAL FLUID DYNAMICS ME G515 BASICS OF COMPUTATIONAL FLUID DYNAMICS ANALYSIS BITS Plan, Duba Campus Overvew Introducton Hstory of CFD Basc concepts CFD Process Dervaton of
More informationMultigrid Methods and Applications in CFD
Multgrd Metods and Applcatons n CFD Mcael Wurst 0 May 009 Contents Introducton Typcal desgn of CFD solvers 3 Basc metods and ter propertes for solvng lnear systems of equatons 4 Geometrc Multgrd 3 5 Algebrac
More informationNUMERICAL SIMULATION OF TURBULENT FLOW AROUND A BUILDING COMPLEX
BBAA VI Internatonal Colloquum on: Bluff Bodes Aerodynamcs & Applcatons lano, Italy, July, 0-4 008 NUEICAL SIULATION OF TUBULENT FLOW AOUND A BUILDING COPLEX Sungsu Lee, Choon-Bum Cho, Kyung-Soo Yang and
More informationLecture 2: Numerical Methods for Differentiations and Integrations
Numercal Smulaton of Space Plasmas (I [AP-4036] Lecture 2 by Lng-Hsao Lyu March, 2018 Lecture 2: Numercal Methods for Dfferentatons and Integratons As we have dscussed n Lecture 1 that numercal smulaton
More informationAnalytical Gradient Evaluation of Cost Functions in. General Field Solvers: A Novel Approach for. Optimization of Microwave Structures
IMS 2 Workshop Analytcal Gradent Evaluaton of Cost Functons n General Feld Solvers: A Novel Approach for Optmzaton of Mcrowave Structures P. Harscher, S. Amar* and R. Vahldeck and J. Bornemann* Swss Federal
More informationA Spline based computational simulations for solving selfadjoint singularly perturbed two-point boundary value problems
ISSN 746-769 England UK Journal of Informaton and Computng Scence Vol. 7 No. 4 pp. 33-34 A Splne based computatonal smulatons for solvng selfadjont sngularly perturbed two-pont boundary value problems
More informationNumerical Studies on Supersonic Turbulent Flow over a Backward Facing Sharp Edge Step Using Hybrid RANS-LES
www.eter.everscence.org Numercal Studes on Supersonc Turbulent Flow over a Bacward Facng Sharp Edge Step Usng Hybrd RANS-LES Dr. Nrmal Kumar Kund Assocate Professor, Department of Producton Engneerng,
More informationFORCED CONVECTION HEAT TRANSFER FROM A RECTANGULAR CYLINDER: EFFECT OF ASPECT RATIO
ISTP-,, PRAGUE TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA FORCED CONVECTION HEAT TRANSFER FROM A RECTANGULAR CYLINDER: EFFECT OF ASPECT RATIO Mohammad Rahnama*, Seyed-Mad Hasheman*, Mousa Farhad**
More informationMMA and GCMMA two methods for nonlinear optimization
MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons
More informationConduction Shape Factor Models for Three-Dimensional Enclosures
JOURNAL OF THERMOPHYSICS AND HEAT TRANSFER Vol. 19, No. 4, October December 005 Conducton Shape Factor Models for Three-Dmensonal Enclosures P. Teertstra, M. M. Yovanovch, and J. R. Culham Unversty of
More informationConsideration of 2D Unsteady Boundary Layer Over Oscillating Flat Plate
Proceedngs of the th WSEAS Internatonal Conference on Flud Mechancs and Aerodynamcs, Elounda, Greece, August -, (pp-) Consderaton of D Unsteady Boundary Layer Over Oscllatng Flat Plate N.M. NOURI, H.R.
More informationNUMERICAL ANALYSIS OF METAL TRANSFER IN GAS METAL ARC WELDING
Unversty of Kentucky UKnowledge Unversty of Kentucky Doctoral Dssertatons Graduate School 007 NUMERICAL ANALYSIS OF METAL TRANSFER IN GAS METAL ARC WELDING Ge Wang Unversty of Kentucky gwang@engr.uky.edu
More informationAcceleration of Gas Bubble-Free Surface Interaction Computation Using Basis Preconditioners
Acceleraton of Gas Bubble-Free Surface Interacton Computaton Usng Bass Precondtoners K. L. Tan, B. C. Khoo and J. K. Whte ABSTRACT The computaton of gas bubble-free surface nteracton entals a tme-steppng
More informationComputer-Aided Circuit Simulation and Verification. CSE245 Fall 2004 Professor:Chung-Kuan Cheng
Computer-Aded Crcut Smulaton and Verfcaton CSE245 Fall 24 Professor:Chung-Kuan Cheng Admnstraton Lectures: 5:pm ~ 6:2pm TTH HSS 252 Offce Hours: 4:pm ~ 4:45pm TTH APM 4256 Textbook Electronc Crcut and
More informationNumerical Studies on Flow Features past a Backward Facing Sharp Edge Step Introducing Hybrid RANS-LES
ISSN NO : 49-7455 Numercal Studes on Flow Features past a Backward Facng Sharp Edge Step Introducng Hybrd RANS-LES Abstract Dr. Nrmal Kumar Kund Assocate Professor, Department of Producton Engneerng Veer
More informationJournal of Fluid Science and Technology
Journal of Flud Scence and Technology Numercal Smulaton of Incompressble Flows around a Fsh Model at Low Reynolds Number Usng Seamless Vrtual Boundary Method * Hdetosh NISHIDA ** and Kyohe TAJIRI ** **Department
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 informationModeling acoustic transducer surface waves by Transmission Line Matrix method
Modelng acoustc transducer surface waves by Transmsson Lne Matrx method Andreas Wlde Fraunhofer Insttut für Integrerte Schaltungen, Außenstelle EAS Peter-Chrstan Eccardt Semens AG, CT MS, München Wllam
More information