Paint flowing down a wall has thickness \(u(x,t)\) satisfying (for \(t>0\)) \[ \frac {\partial u}{\partial t}+u^2\frac {\partial u}{\partial x}=0. \]
- Show that the characteristics are straight lines and that the Rankine–Hugoniot condition on a shock \(x=S(t)\) is \[ \frac {dS}{dt}=\frac {\left [u^3/3\right ]_-^+}{[u]_-^+}. \]
- A stripe of paint is applied at \(t=0\) so that \[ u(x,0)= \begin {cases} 0, & x<0\text { or }x>1\\ 1, & 0<x<1 \end {cases} \] For sufficiently small \(t\), determine \(u\) in the domains \(x<0\), \(0<x<t\), \(t<x<S(t)\) and \(S(t)<x\), where the shock is \(x=S(t)=1+t/3\)
- Explain why the solution changes at \(t=3/2\) and show that thereafter \(\dot {S}=S/3t\).