Let be the difference of two sufficiently regular solutions of the wave equation with the prescribed data. By linearity, has zero initial displacement, zero initial velocity, and homogeneous Dirichlet boundary conditions. Define its wave energy by
For , differentiation under the integral sign and integration by parts yield
The boundary term vanishes because at both fixed endpoints implies there. The zero initial data give , so for all times. Thus is spatially constant, and its zero boundary values give . This proves uniqueness for the undamped wave equation.
Use the same difference and wave energy as in part (i). The damped wave equation now gives the energy dissipation identity for a linearly damped string
Because and , the energy remains zero. Hence , and the homogeneous Dirichlet boundary conditions force . Therefore the solution of a differential equation is unique also for ; positive damping can only decrease this energy.

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