Vibrating Plate. Let \(\Omega \subset \mathbb {R}^n\) be a smooth bounded domain. Let \(\varphi ,\psi \in C^\infty _0(\Omega )\). Suppose that there exists a solution \(u(x,t)\in C^4(\overline {\Omega }\times [0,T])\) to the initial-boundary value problem for the vibrating clamped plate equation \[ \begin {cases} \dfrac {\partial ^2u}{\partial t^2}+\Delta \Delta u=0, & \text {if }x\in \Omega \text { and }t\ge 0,\\ u(x,0)=\varphi (x),\\ \dfrac {\partial u}{\partial t}(x,0)=\psi (x), & \text {for }x\in \Omega ,\\ u(x,t)=\dfrac {\partial u}{\partial n}(x,t)=0, & \text {if }x\in \partial \Omega \text { and }0\le t\le T. \end {cases} \tag {4.} \]
- Show that the total energy \[ \mathcal {E}(t)=\int _\Omega \left \{\left (\frac {\partial u}{\partial t}(x,t)\right )^2+ \left (\Delta u(x,t)\right )^2\right \}\,dx \] is bounded in terms of \(\varphi \), \(\psi \) and \(t\).
- Show that such a solution of (4.) is unique.