CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 5 Numerical Integration Spring 2010 Prof. Chung-Kuan Cheng 1.

Slides:



Advertisements
Similar presentations
Courant and all that Consistency, Convergence Stability Numerical Dispersion Computational grids and numerical anisotropy The goal of this lecture is to.
Advertisements

Formal Computational Skills
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 5 Numerical Integration Prof. Chung-Kuan Cheng 1.
Ordinary Differential Equations
Lecture 18 - Numerical Differentiation
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 2: State Equations Prof. Chung-Kuan Cheng 1.
1 EE 616 Computer Aided Analysis of Electronic Networks Lecture 12 Instructor: Dr. J. A. Starzyk, Professor School of EECS Ohio University Athens, OH,
CSE245:Lec4 02/24/2003. Integration Method Problem formulation.
Numerical Integration CSE245 Lecture Notes. Content Introduction Linear Multistep Formulae Local Error and The Order of Integration Time Domain Solution.
Lecture on Stiff Systems (Section 1-6 of Chua and Lin) ECE 546 Jan. 15, 2008.
Solutions for Nonlinear Equations
1 EE 616 Computer Aided Analysis of Electronic Networks Lecture 12 Instructor: Dr. J. A. Starzyk, Professor School of EECS Ohio University Athens, OH,
CSE245:Lecture12 Advisor: C.K. Cheng Date: 02/13/03.
UCSD CSE245 Notes -- Spring 2006 CSE245: Computer-Aided Circuit Simulation and Verification Lecture Notes Spring 2006 Prof. Chung-Kuan Cheng.
Ordinary Differential Equations (ODEs) 1Daniel Baur / Numerical Methods for Chemical Engineers / Implicit ODE Solvers Daniel Baur ETH Zurich, Institut.
CISE301_Topic8L31 SE301: Numerical Methods Topic 8 Ordinary Differential Equations (ODEs) Lecture KFUPM (Term 101) Section 04 Read , 26-2,
Numerical Solution of Ordinary Differential Equation
MATH 685/ CSI 700/ OR 682 Lecture Notes Lecture 10. Ordinary differential equations. Initial value problems.
1 Chapter 6 Numerical Methods for Ordinary Differential Equations.
Numerical Solutions to ODEs Nancy Griffeth January 14, 2014 Funding for this workshop was provided by the program “Computational Modeling and Analysis.
Professor Walter W. Olson Department of Mechanical, Industrial and Manufacturing Engineering University of Toledo Solving ODE.
Ch 8.1 Numerical Methods: The Euler or Tangent Line Method
Boyce/DiPrima 9th ed, Ch 8.4: Multistep Methods Elementary Differential Equations and Boundary Value Problems, 9th edition, by William E. Boyce and Richard.
Lecture 35 Numerical Analysis. Chapter 7 Ordinary Differential Equations.
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 2: State Equations Prof. Chung-Kuan Cheng.
EE3561_Unit 8Al-Dhaifallah14351 EE 3561 : Computational Methods Unit 8 Solution of Ordinary Differential Equations Lesson 3: Midpoint and Heun’s Predictor.
Numerical Methods for Partial Differential Equations CAAM 452 Spring 2005 Lecture 3 AB2,AB3, Stability, Accuracy Instructor: Tim Warburton.
1 EEE 431 Computational Methods in Electrodynamics Lecture 4 By Dr. Rasime Uyguroglu
Modelling & Simulation of Chemical Engineering Systems Department of Chemical Engineering King Saud University 501 هعم : تمثيل الأنظمة الهندسية على الحاسب.
Integration of 3-body encounter. Figure taken from
Scientific Computing Numerical Solution Of Ordinary Differential Equations - Euler’s Method.
Copyright © 2006 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. ~ Ordinary Differential Equations ~ Stiffness and Multistep.
7. Introduction to the numerical integration of PDE. As an example, we consider the following PDE with one variable; Finite difference method is one of.
+ Numerical Integration Techniques A Brief Introduction By Kai Zhao January, 2011.
Engineering Analysis – Computational Fluid Dynamics –
Large Timestep Issues Lecture 12 Alessandra Nardi Thanks to Prof. Sangiovanni, Prof. Newton, Prof. White, Deepak Ramaswamy, Michal Rewienski, and Karen.
© Imperial College London Numerical Solution of Differential Equations 3 rd year JMC group project ● Summer Term 2004 Supervisor: Prof. Jeff Cash Saeed.
Circuits Theory Examples Newton-Raphson Method. Formula for one-dimensional case: Series of successive solutions: If the iteration process is converged,
Numerical Analysis – Differential Equation
Introduction to the Runge-Kutta algorithm for approximating derivatives PHYS 361 Spring, 2011.
1 EE 616 Computer Aided Analysis of Electronic Networks Lecture 12 Instructor: Dr. J. A. Starzyk, Professor School of EECS Ohio University Athens, OH,
Announcements Read Chapters 11 and 12 (sections 12.1 to 12.3)
CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 2: State Equations Spring 2010 Prof. Chung-Kuan Cheng.
Ch 8.2: Improvements on the Euler Method Consider the initial value problem y' = f (t, y), y(t 0 ) = y 0, with solution  (t). For many problems, Euler’s.
Today’s class Ordinary Differential Equations Runge-Kutta Methods
Lecture 40 Numerical Analysis. Chapter 7 Ordinary Differential Equations.
ECE 576 – Power System Dynamics and Stability Prof. Tom Overbye Dept. of Electrical and Computer Engineering University of Illinois at Urbana-Champaign.
Ordinary Differential Equations
1/14  5.2 Euler’s Method Compute the approximations of y(t) at a set of ( usually equally-spaced ) mesh points a = t 0 < t 1
Lecture 39 Numerical Analysis. Chapter 7 Ordinary Differential Equations.
NUMERICAL DIFFERENTIATION or DIFFERENCE APPROXIMATION Used to evaluate derivatives of a function using the functional values at grid points. They are.
Solving Ordinary Differential Equations
Lecture 11 Alessandra Nardi
Numerical Methods for Partial Differential Equations
ECE 576 – Power System Dynamics and Stability
CSE245: Computer-Aided Circuit Simulation and Verification
Class Notes 18: Numerical Methods (1/2)
SE301: Numerical Methods Topic 8 Ordinary Differential Equations (ODEs) Lecture KFUPM (Term 101) Section 04 Read , 26-2, 27-1 CISE301_Topic8L4&5.
CSE 245: Computer Aided Circuit Simulation and Verification
CSE245: Computer-Aided Circuit Simulation and Verification
Chapter 26.
Sec 21: Analysis of the Euler Method
CSE245: Computer-Aided Circuit Simulation and Verification
SE301: Numerical Methods Topic 8 Ordinary Differential Equations (ODEs) Lecture KFUPM (Term 101) Section 04 Read , 26-2, 27-1 CISE301_Topic8L2.
ECE 576 POWER SYSTEM DYNAMICS AND STABILITY
Chapter 2 A Survey of Simple Methods and Tools
EE 616 Computer Aided Analysis of Electronic Networks Lecture 12
Presentation transcript:

CSE245: Computer-Aided Circuit Simulation and Verification Lecture Note 5 Numerical Integration Spring 2010 Prof. Chung-Kuan Cheng 1

Numerical Integration: Outline One-step Method for ODE (IVP) –Forward Euler –Backward Euler –Trapezoidal Rule –Equivalent Circuit Model Convergence Analysis Linear Multi-Step Method Time Step Control 2

Ordinary Difference Equaitons N equations, n x variables, n dx/dt. Typically analytic solutions are not available  solve it numerically 3

Numerical Integration Forward Euler Backward Euler Trapezoidal 4

Numerical Integration: State Equation Forward Euler Backward Euler 5

Numerical Integration: State Equation Trapezoidal 6

7 Equivalent Circuit Model-BE Capacitor + C

8 Equivalent Circuit Model-BE Inductor + L

9 Equivalent Circuit Model-TR Capacitor + C

10 Equivalent Circuit Model-TR Inductor + L

Trap Rule, Forward-Euler, Backward-Euler All are one-step methods x k+1 is computed using only x k, not x k-1, x k-2, x k-3... Forward-Euler is the simplest No equation solution explicit method. Backward-Euler is more expensive Equation solution each step implicit method most stable (FE/BE/TR) Trapezoidal Rule might be more accurate Equation solution each step implicit method More accurate but less stable, may cause oscillation Summary of Basic Concepts 11

12 Stabilities Froward Euler

Difference Eqn Stability region 1 Im(z) Re(z) Forward Euler ODE stability region Region of Absolute Stability FE region of absolute stability 13

14 Stabilities Backward Euler

Difference Eqn Stability region 1 Im(z) Re(z) Backward Euler Region of Absolute Stability BE region of absolute stability 15

16 Stabilities Trapezoidal

Convergence Consistency: A method of order p (p>1) is consistent if Stability: A method is stable if: Convergence: A method is convergent if: Consistency + Stability Convergence 17

A-Stable Dahlqnest Theorem: –An A-Stable LMS (Linear MultiStep) method cannot exceed 2nd order accuracy The most accurate A-Stable method (smallest truncation error) is trapezoidal method. 18

Convergence Analysis: Truncation Error Local Truncation Error (LTE): –At time point t k+1 assume x k is exact, the difference between the approximated solution x k+1 and exact solution x * k+1 is called local truncation error. –Indicates consistancy –Used to estimate next time step size in SPICE Global Truncation Error (GTE): –At time point t k+1, assume only the initial condition x 0 at time t 0 is correct, the difference between the approximated solution x k+1 and the exact solution x * k+1 is called global truncation error. –Indicates stability 19

LTE Estimation: SPICE Taylor Expansion of x n+1 about the time point t n : Taylor Expansion of dx n+1 /dt about the time point t n : Eliminate term in above two equations we get the trapezoidal rule LTE 20

Time Step Control: SPICE We have derived the local truncation error the unit is charge for capacitor and flux for inductor Similarly, we can derive the local truncation error in terms of (1) the unit is current for capacitor and voltage for inductor Suppose E D represents the absolute value of error that is allowed per time point. That is together with (1) we can calculate the time step as 21

Time Step Control: SPICE (cont ’ d) DD 3 (t n+1 ) is called 3rd divided difference, which is given by the recursive formula 22