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Dr. Guy Tel-Zur Computational Physics Differential Equations Autumn Colors, by Bobby Mikul, Mikul Autumn Colors,

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Presentation on theme: "Dr. Guy Tel-Zur Computational Physics Differential Equations Autumn Colors, by Bobby Mikul, Mikul Autumn Colors,"— Presentation transcript:

1 Dr. Guy Tel-Zur Computational Physics Differential Equations Autumn Colors, by Bobby Mikul, http://www.publicdomainpictures.netBobby Mikul Autumn Colors, by Bobby Mikul, http://www.publicdomainpictures.netBobby Mikul Version 10-11-2010 18:30

2 Agenda MHJ Chapter 13 & Koonin Chapter 2 How to solve ODE using Matlab Scilab

3 Topics Defining the scope of the discussion Simple methods Multi-Step methods Runge-Kutta Case Studies - Pendulum

4 The scope of the discussion For a higher order ODE  a set of coupled 1 st order equations:

5 Simple methods Euler method: Integration using higher order accuracy: Taylor series expansion:

6 Local error! Better than Euler’s method but useful only when it is easy to differentiate f(x,y)

7 Example Let’s solve:

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9 FORTRAN code

10 Multi-Step methods

11 Adams-Bashforth 2 steps: 4 steps:

12 (So far) Explicit methods Future = Function(Present && Past) Implicit methods Future = Function(Future && Present && Past)

13 Let’s calculate dy/dx at a mid way between lattice points: Rearrange: This is a recursion relation! Let’s replace:

14 A simplification occurs if f(x,y)=y*g(x), then the recursion equation becomes: An example, suppose g(x)=-x y n+1 =(1-x n h/2)/(1+x n+1 h/2)y n This can be easily calculated, for example: Calculate y(x=1) for h=0.5 X0=0, y(0)=1 X1=0.5, y(0.5)=? x2=1.0, y(1.0)=?

15 The solution:

16 Predictor-Corrector method

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18 Runge-Kutta

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21 Proceed to: Physics examples: Ideal harmonic oscillator – section 13.6.1

22 Physics Project – The pendulum, 13.7 I use a modified the C++ code from: http://www.fys.uio.no/compphys/cp/programs/FYS3150/chapter13/cpp/program2.cpp fout.close  fout.close() Demo on folder: C:\Users\telzur\Documents\BGU\Teaching\ComputationalPhysics\2011A\Lectures\05\CPP

23 ODEs in Matlab function dydt = odefun(t,y) a=0.001; b=1.0; dydt -=b*t*sin(t)+a*t*t; function dydt = odefun(t,y) a=0.001; b=1.0; dydt -=b*t*sin(t)+a*t*t; Usage: [t1, y1]=ode23(@odefun,[0 100],0); Plot(t1,y1,’r’); hold on plot(t2,y2,’b’); hold off Usage: [t1, y1]=ode23(@odefun,[0 100],0); Plot(t1,y1,’r’); hold on plot(t2,y2,’b’); hold off Demo folder: Users\telzur\Documents\BGU\Teaching\ComputationalPhysics\2011A\Lectures\05\Matlab

24 Output

25 http://www.scilab.org

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30 Parallel tools for Multi-Core and Distributed Parallel Computing

31 In preparation Parallel execution A new function (parallel_run) allows parallel computations and leverages multicore architectures and their capacities. Parallel execution A new function (parallel_run) allows parallel computations and leverages multicore architectures and their capacities.

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37 Xcos demo


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