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Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao ([email protected] ) Department of Mathematics The University of Texas – Pan American Sept 2, 2008
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Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao ([email protected])[email protected] Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

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Page 1: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Soliton for PDEsMath 6399 – Lec 2

Zhijun Qiao

([email protected])

Department of Mathematics

The University of Texas – Pan American

Sept 2, 2008

Page 2: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Solitons along a boundary

This is the way you usually see solitons in shallow water,

scurrying along like mice in the gutter, at a scale of a only a few inches in width and height.

Page 3: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Synthetic Aperture Radar Image of Soliton Formation at Gibraltar

Solitons at Gibraltar Strait are 2D

Page 4: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Technology Seeks to Control Turbulence Turbulence Challenges Weather

Prediction at All Scales

Turbulence appears at all scales in the weather. Turbulence affects weather prediction at all scales.

Turbulence Causes Uncertainty in Numerical Weather Prediction

Turbulence Challenges the Prediction of Global Ocean Circulation & Climate

Page 5: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Aircraft turbulence is just one of the phenomena that Fluid Dynamics seeks to explain. By solving suitable equations, mathematicians can create computer simulations of observed cases of turbulence.

Page 6: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Examples of fluids include gases and liquids. Typically, liquids are considered to be incompressible,whereas gases are considered to be compressible. Fluid flow is dominated by the governing equation- NS. There are a bunch of applications in engineering and DoD Prog.

Page 7: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

BACKGROUND

Here is the example. There is a well known PDE that arises in the modeling of various fluid flows, from shock waves to turbulence, known as Burgers equation.

It is, roughly speaking, a one-dimensional caricature of the Navier-Stokes equation, so central to fluid mechanics. Burgers equation concerns a field u depending on one spatial coordinate, x, and time, t. The PDE is as written.

Page 8: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Traveling Wave:

• This is the Riemann equation (also called inviscid Burgers’, Hopf etc.)

Page 9: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Other type solution

Page 10: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

plot3d((2*x-3)/(2*t-7),x=-10..10,t=3.3..3.7); A=2,B=-3,C=-7;

Page 11: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

General Solution

Page 12: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 13: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Burgers Equation: Traveling Shock Wave

Page 14: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 15: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 16: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 17: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

plot((2*x-7)/(x-4),x=3.01..3.99);t=1,a=2,c=4,B=0; plot((2*x-7)/(x-4),x=4.01..4.99);t=1,a=2,c=4,B=0;

Page 18: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

plot3d((2*x-8*t+1)/(x-4*t),x=-10..10,t=0..2);a=2,c=4,B=0;Singular Traveling Wave Solution

Page 19: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 20: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 21: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 22: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

plot3d(1+tanh(x-2*t),x=-10..10,t=0..3);B=0,a=2,b=0,c=2;plot(1+tanh(x-2*1),x=-10..10);B=0,a=2,b=0,c=2,t=1;

Shock wave solution for the Burgers equation

Page 23: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.
Page 24: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

plot3d(1+1/tanh(x-2*t),x=-1..1,t=0..0.5);B=0,a=2,b=0,c=2;plot(1+1/tanh(x-2),x=1.5..1.99);B=0,a=2,b=0,c=2,t=1;plot(1+1/tanh(x-2),x=2.01..2.5);B=0,a=2,b=0,c=2,t=1;

Page 25: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Assignment: find traveling wave solution or other explicit

solution

• MKdV equation

• Fisher equation

Page 26: Soliton for PDEs Math 6399 – Lec 2 Zhijun Qiao (qiao@utpa.edu)qiao@utpa.edu Department of Mathematics The University of Texas – Pan American Sept 2, 2008.

Thanks

• Any Questions/Comments?

• Welcome to discuss with me anytime.

My email: [email protected]