Consider the wave equation \[ \frac {\partial ^2\phi }{\partial t^2}=\frac {\partial ^2\phi }{\partial x^2}, \qquad 0\le x\le l \] with the following boundary conditions \[ \begin {gathered} \phi (x,0)=0,\qquad \frac {\partial \phi }{\partial t}(x,0)=0,\\ \phi (0,t)=0,\qquad \phi (l,t)=f(t). \end {gathered} \]
- Show that the Laplace transform of the solution \(\widehat {\Phi }(x,s)\) is given by \[ \widehat {\Phi }(x,s)=\frac {\widehat {F}(s)\sinh sx}{\sinh sl} \] where \(\widehat {F}(s)\) is the Laplace transform of \(f(t)\).
- Suppose that \(\phi _0(x,t)\) is the solution when \(f(t)=1\). Show that the solution for general \(f\) is given by \[ \phi (x,t)=\int _0^t \frac {\partial \phi _0}{\partial t'}(x,t')f(t-t')\,dt'. \]