Difference between revisions of "Method of Characteristics for Linear Equations"

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m (Created page with '{{nonlinear waves course | chapter title = Method of Characteristics for Linear Equations | next chapter = Traffic Waves | previous chapter = }} We present here a brief …')
 
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<center>
 
<center>
 
<math>
 
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\partial_t u + \partial_x u = 0,\,\,-\infty<x<\infty,\,\,t>0
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\partial_t u + \partial_x u = 0,\,\,-\infty<x<\infty,\,\,t>0,
 
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subject to the initial conditions
 
subject to the initial conditions
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  \left. u \right|_{t=0} = f(x)
 
  \left. u \right|_{t=0} = f(x)
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We consider the solution along the curve <math>(x,t) = (X(t),t)</math>. We then have
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\frac{d U}{d t} = \partial_t u + \frac{d X}{dt}\partial_x u = \partial_x u \left(\frac{d X}{dt} + 1 \right)
 
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Revision as of 02:00, 23 July 2010

Nonlinear PDE's Course
Current Topic Method of Characteristics for Linear Equations
Next Topic Traffic Waves
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We present here a brief account of the method of characteristic for linear waves.

Introduction

The method of characteristics is an important method for hyperbolic PDE's which applies to both linear and nonlinear equations.

We begin with the simplest wave equation

[math]\displaystyle{ \partial_t u + \partial_x u = 0,\,\,-\infty\lt x\lt \infty,\,\,t\gt 0, }[/math]

subject to the initial conditions

[math]\displaystyle{ \left. u \right|_{t=0} = f(x) }[/math]

We consider the solution along the curve [math]\displaystyle{ (x,t) = (X(t),t) }[/math]. We then have

[math]\displaystyle{ \frac{d U}{d t} = \partial_t u + \frac{d X}{dt}\partial_x u = \partial_x u \left(\frac{d X}{dt} + 1 \right) }[/math]