Finite difference time domain

Slides:



Advertisements
Similar presentations
Partial Differential Equations
Advertisements

P. Venkataraman Mechanical Engineering P. Venkataraman Rochester Institute of Technology DETC2013 – 12269: Continuous Solution for Boundary Value Problems.
Basic Functions and Their Graphs
BVP Weak Formulation Weak Formulation ( variational formulation) where Multiply equation (1) by and then integrate over the domain Green’s theorem gives.
CHE/ME 109 Heat Transfer in Electronics LECTURE 12 – MULTI- DIMENSIONAL NUMERICAL MODELS.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 6 FLUID KINETMATICS.
Parabolic PDEs Generally involve change of quantity in space and time Equivalent to our previous example - heat conduction.
Chapter 4 Numerical Solutions to the Diffusion Equation.
1 Chapter 9 NUMERICAL SOLUTION OF PARTIAL DIFFERENTIAL EQUATIONS.
Finite Difference Time Domain Method (FDTD)
ME 595M J.Murthy1 ME 595M: Computational Methods for Nanoscale Thermal Transport Lecture 9: Boundary Conditions, BTE Code J. Murthy Purdue University.
Eigenvalues of Ordinary Differential Equations Jake Blanchard University of Wisconsin.
報 告 者:林 建 文 指導教授:陳 瑞 昇 博士 1 Jesús S. Pérez Guerrero · Todd H. Skaggs · M. Th. van Genuchten {Transp Porous Med (2010) 85:171–188.}
1.2 Functions and Graphs. Functions Domains and Ranges Viewing and Interpreting Graphs Even Functions and Odd functions - Symmetry Functions Defined in.
Graph 8 a. Graph b. Domain _________ c. Range __________
Numerical ElectroMagnetics & Semiconductor Industrial Applications Ke-Ying Su Ph.D. National Central University Department of Mathematics 12 2D-NUFFT &
Solidification / Melting Moving Boundary Problems: A finite difference method Final Project MANE 6640 – Fall 2009 Wilson Braz.
Scientific Computing Partial Differential Equations Poisson Equation.
Section 2.2 Functions  Functions & Graphs  Function Notation & Equations  Applications: Interpolation & Extrapolation 12.2.
1 EEE 431 Computational Methods in Electrodynamics Lecture 9 By Dr. Rasime Uyguroglu
Introduction to Level Set Methods: Part II
Remcom Inc. 315 S. Allen St., Suite 416  State College, PA  USA Tel:  Fax:   ©
Graphing Absolute Value Without a Calculator Objective: You should be able to graph absolute value functions (including their changes) without a calculator.
Discretization Methods Chapter 2. Training Manual May 15, 2001 Inventory # Discretization Methods Topics Equations and The Goal Brief overview.
Options, Futures, and Other Derivatives, 4th edition © 1999 by John C. Hull 18.1 Exotic Options Chapter 18.
Chapter 7 Finite element programming May 17, 2011.
1 EEE 431 Computational Methods in Electrodynamics Lecture 7 By Dr. Rasime Uyguroglu
For the sequence, describe the pattern and write the next term. 1.) 1, 6, 11, 16 2.) -4, 8, -12, 16 3.) 1.2, 4.2, 9.2, 16.2.
Simple numerical scheme for modelling of nonlinear pulse propagation in coupled microring resonators Anna Sterkhova, Jiří Petráček, Jaroslav Luksch ICTON.
Solving Partial Differential Equation Numerically Pertemuan 13 Matakuliah: S0262-Analisis Numerik Tahun: 2010.
14 - finite element method
Math – Exponential Functions
Model Anything. Quantity Conserved c  advect  diffuse S ConservationConstitutiveGoverning Mass, M  q -- M Momentum fluid, Mv -- F Momentum fluid.
Section 2.8 Distance and Midpoint Formulas; Circles.
The Finite Difference Time Domain Method FDTD Haythem H. abdullah ERI, Electronics Research Institute, Microwave Engineering Dept.
The Finite Difference Time Domain Method FDTD By Dr. Haythem H. Abdullah Researcher at ERI, Electronics Research Institute, Microwave Engineering Dept.
THERMO-STRUCTURAL ANALYSIS
EEE 431 Computational Methods in Electrodynamics
Modeling of Traffic Flow Problems
#2 Functions and Graphs.
Piecewise Functions.
Piecewise Functions At least 2 equations, each of which applies to a different part of the functions domain. It is like having 3 equations for 3 different.
Warm-Up.
CSE 245: Computer Aided Circuit Simulation and Verification
Warm Up State the domain and range of the following equations:
Objective Numerical methods.
Image Enhancement in the
Image Enhancement in the
פחת ורווח הון סוגיות מיוחדות תהילה ששון עו"ד (רו"ח) ספטמבר 2015
Objective 1A f(x) = 2x + 3 What is the Range of the function
finite element method node point based strong form
finite element method node point based strong form
Piecewise Functions At least 2 equations, each of which applies to a different part of the functions domain. It is like having 3 equations for 3 different.
Piecewise-defined Functions
Equation Review Given in class 10/4/13.
A least-squares method for the Monge-Ampère equation
Objective Numerical methods Finite volume.
Machine learning algorithms for nano-material characterization
topic16_cylinder_flow_relaxation
Finite element method.
Unit 3 Review (Calculator)
Relations, Domain and Range
Warm-up 1)
Diyu Yang Mentor: Xu Chen Advisor: José E. Schutt-Ainé Abstract
Equation Review.
Section 3.1 Functions.
Warm-Up Study the patterns below to determine the next five numbers in each sequence. You may use the calculator to check your answers. 2, 4, 6, 8, 10...
Calculate 9 x 81 = x 3 3 x 3 x 3 x 3 3 x 3 x 3 x 3 x 3 x 3 x =
Mathematics Unit 22: Staircase
Chapter 4 Review What quadrant is point (-3, 2) in?
Presentation transcript:

Finite difference time domain FDTD -- MATLAB

Development of the technique “advection” equation

Calculate the spatial distribution at the next increment in time Setup a mesh in time and in space. The mesh in position extends beyond the points of interest. Initial conditions @ t = 0 time Calculate the spatial distribution at the next increment in time @ t = 1 position

Invoke periodic boundary conditions

Foreword difference in time Central difference in space

Finite difference Time domain “fdtd”

This is valid only for the interior range 2  n  N – 1

Periodic boundary conditions

Time  #1 -3L/8 -1/2 #2 -1L/8 1 ½ #3 +1L/8 3/2 #4 +3L/8

Example of the FDTD using the above procedure Initial conditions Time  2 3 4 -3L/8 -1/2 ½ 5/2 z -1L/8 1 -3/2 +1L/8 3/2 +3L/8

Lax to the rescue!

Periodic boundary conditions

 #1 -3L/8 #2 -1L/8 1 #3 +1L/8 #4 +3L/8

Example of the FDTD using the Lax procedure. Initial conditions Time  2 3 4 -3L/8 1 z -1L/8 +1L/8 +3L/8

First iteration & 50th iteration

Movie to illustrate the calculation

Frasson

Lewandowski