1.II.31E

Integrable Systems | Part II, 2006

(a) Let q(x,t)q(x, t) satisfy the heat equation

qt=2qx2\frac{\partial q}{\partial t}=\frac{\partial^{2} q}{\partial x^{2}}

Find the function XX, which depends linearly on q/x,q,k\partial q / \partial x, q, k, such that the heat equation can be written in the form

t(eikx+k2tq)+x(eikx+k2tX)=0,kC.\frac{\partial}{\partial t}\left(e^{-i k x+k^{2} t} q\right)+\frac{\partial}{\partial x}\left(e^{-i k x+k^{2} t} X\right)=0, \quad k \in \mathbb{C} .

Use this equation to construct a Lax pair for the heat equation.

(b) Use the above result, as well as the Cole-Hopf transformation, to construct a Lax pair for the Burgers equation

Qt2QQx=2Qx2\frac{\partial Q}{\partial t}-2 Q \frac{\partial Q}{\partial x}=\frac{\partial^{2} Q}{\partial x^{2}}

(c) Find the second-order ordinary differential equation satisfied by the similarity solution of the so-called cylindrical KdV\mathrm{KdV} equation:

qt+3qx3+qqx+q3t=0,t0\frac{\partial q}{\partial t}+\frac{\partial^{3} q}{\partial x^{3}}+q \frac{\partial q}{\partial x}+\frac{q}{3 t}=0, \quad t \neq 0

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