The Kuramoto–Sivashinsky Equation (Part 5)

In Parts 3 and 4, I showed some work of Cheyne Weis on the ‘derivative form’ of the Kuramoto–Sivashinksy equation, namely

u_t + u_{xx} + u_{xxxx} + u u_x = 0

Steve Huntsman’s picture of a solution above gives you a good feel for how this works.

Now let’s turn to the ‘integral form’, namely

h_t + h_{xx} + h_{xxxx} + \frac{1}{2} (h_x)^2 = 0

This has rather different behavior, though it’s closely related, since if h is any solution of the integral form then

u = h_x

is a solution of the derivative form.

Cheyne drew a solution of the integral form:



You’ll immediately see the most promi...

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Published on October 23, 2021 18:53
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