Conserved quantities in the Korteweg-de Vries equation

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Homework Help Overview

The discussion revolves around the Korteweg-de Vries (KdV) equation, specifically focusing on finding a relationship between coefficients in a conserved quantity involving integrals of derivatives and powers of the function ψ.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the formulation of a local conservation law and the conditions under which a specific quantity remains conserved. There are attempts to compute temporal derivatives and express integrands as perfect derivatives. Some participants question the placement of coefficients in the integrand and suggest using trial functions for further exploration.

Discussion Status

The discussion is ongoing, with various approaches being explored. Some participants have offered suggestions for trial functions and expressed concerns about the formulation of the integrand. There is no explicit consensus on the correct approach or solution at this time.

Contextual Notes

Participants are navigating the complexities of the KdV equation and its conservation laws, with some expressing uncertainty about the definitions and roles of coefficients in the integrals. There is mention of external resources that may provide insights, but no definitive conclusions have been reached.

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Homework Statement


Consider the Kortweg-de Vires Equation in the form

$$\frac{\partial \psi}{\partial t}+\frac{\partial^3 \psi}{\partial x^3}+6\psi\frac{\partial \psi}{\partial x}=0$$

Find the relation between the coefficients ##c## and ##d## , such that the following quantity is conserved:

$$c\; \int_{-\infty}^\infty\left(\frac{\partial\psi}{\partial x}\right)^2 \mathrm{d}x+d\;\int_{-\infty}^{\infty}\psi ^3 \mathrm{d}x$$

Homework Equations


A local conservation law is of the form ##D_t+F_x=0##.

The Attempt at a Solution


Usually, I would try to create a local conservation law, s.t. the quantity in question is conserved. But I really don't know how to do this in the given case. Thanks!
 
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Hey, I've attempted to do the following:

Since the quantity in question needs to be conserved, it follows that

$$\frac{\partial}{\partial t}\left( \; \int_{-\infty}^\infty c\left(\frac{\partial\psi}{\partial x}\right)^2 \mathrm{d}x+d\;\int_{-\infty}^{\infty}\psi ^3 \mathrm{d}x \right) =0$$.

Thus, I have computed the temporal derivation, which yields

$$-c\int_{-\infty}^\infty \mathrm{d}x \left( 2c\frac{\partial^4 \psi}{\partial x^4}\frac{\partial\psi}{\partial x}+12c\left(\frac{\partial \psi}{\partial x}\right)^2+12c \psi\frac{\partial\psi}{\partial x}\frac{\partial^2 \psi}{\partial x^2}+3d\psi^2\frac{\partial^3\psi}{\partial x^3}+18\psi ^3 \frac{\partial \psi}{\partial x} \right)=0 $$

if I define ##d:=-c##.

If I can show that the integrand is a perfect derivative, I am finished. However, I can't seem to show that this is the case. Can anyone help me?
 
I don't think you should have the factor of c outside the integral, but you need a factor of d in the last term of the integrand. (But I'm also one of those that deplore using d as a constant in anything involving calculus.)

It looks as though the integrand should be expressible in terms of an operator polynomial; something like (a + D)(D2 + D)(ψ3), where a is a constant and D is ∂/∂x, but I haven't been able to make it work.

I can only suggest putting in trial functions like ψ = sinx and seeing what happens.
Good luck.
 
Why reinvent the wheel when Google is your friend? The Wikipedia page on the KdV equation has c=-1, d=2. Check it out.
 
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