KdV equation: Difference between revisions

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This is the Korteweg de Vries equation for a quantity <math>A(x,t)</math> in physical form
This is the Korteweg de Vries equation for a quantity <math>A(x,t)</math> in physical form
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<math>A_t = -c A_x + \alpha A A_x + \beta A_{xxx}</math>
<math>A_t = -c A_x + \alpha A A_x + \beta A_{xxx}\,</math>
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where subscripts denote partial derivatives.
where subscripts denote partial derivatives.
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To understand the meaning of the nonlinear and dispersive terms consider them one at a time.  First the nonlinear term
To understand the meaning of the nonlinear and dispersive terms consider them one at a time.  First the nonlinear term
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<math>A_t = -(c-\alpha A) A_x. </math>
<math>A_t = -(c-\alpha A) A_x.\, </math>
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You can see that if <math>A>0</math> and <math>\alpha</math> is negative then larger waves have faster propagation speeds.  For the dispersive term we need to Fourier transform to see that
You can see that if <math>A>0</math> and <math>\alpha</math> is negative then larger waves have faster propagation speeds.  For the dispersive term we need to Fourier transform to see that

Revision as of 15:21, 1 June 2011

This is the Korteweg de Vries equation for a quantity in physical form

where subscripts denote partial derivatives.

The parameter c denotes the linear advective wave speed, the parameter denotes the nonlinear effects while the parameter denotes the dispersive effect. In practice these parameters depend on the physical situation considered.

To understand the meaning of the nonlinear and dispersive terms consider them one at a time. First the nonlinear term

You can see that if and is negative then larger waves have faster propagation speeds. For the dispersive term we need to Fourier transform to see that

where is the wavenumber. Thus when is positive shorter waves (with larger k) propagate slower.