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 | ||
<br> | <br> | ||
<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> | ||
<br> | <br> | ||
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> | ||
<br> | <br> | ||
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 14:21, 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.