Consider the equation \[ \frac {\partial u}{\partial t} +\frac {\partial }{\partial x}\left (\frac {u^2}{2}\right ) =\epsilon \frac {\partial ^2u}{\partial x^2}, \] for \(-\infty <x<\infty \) and \(t>0\).
- Look for a traveling wave solution \(u(x,t)=U(z)\), \(z=(x-Vt)/\epsilon \), with velocity \(V>0\) and \(U(z)\to U_\pm \) as \(z\to \pm \infty \). Solve the resulting ODE for \(U(z)\) and deduce that \[ V=\frac {[U^2/2]_{-\infty }^{\infty }}{[U]_{-\infty }^{\infty }} \]
- Discuss how the traveling wave solution relates to shock solutions of the quasilinear equation obtained by setting \(\epsilon =0\).
- Using phase-plane analysis, show that the wave profile \(U\) is monotonically decreasing, that is, \(dU/dz<0\).