In Kirchhoff-Love Plate Theory, the vertical displacement \(w(x)\) of an isotropic static plate under pure bending satisfies \[ Lw:=D\left (\frac {\partial ^4w}{\partial x_1^4} +2\frac {\partial ^4w}{\partial x_1^2\partial x_2^2} +\frac {\partial ^4w}{\partial x_2^4}\right )=-f, \] where \(D>0\) is a known constant bending stiffness, and \(-f(x)\) is a given applied transverse load. Assume that the plate lies within a simply connected bounded region \(U\subset \mathbb {R}^2\) with smooth boundary \(\partial U\). Define the bilinear form \[ B(w,v)=\int _U (Lw)v\dd x. \]
- Suppose that the boundary of the plate is clamped, that is, the displacement \(w\) satisfies \[ \begin {aligned} w &= 0, && \text {on }\partial U,\\ \frac {\partial w}{\partial \eta } &= 0, && \text {on }\partial U, \end {aligned} \] where \(\eta \) is the unit outward normal. Let \(X\) be the space of smooth functions satisfying the above boundary conditions. Show that \(B\) is symmetric and positive semidefinite over \(X\times X\).
- Using an elementary estimate for solutions of Poisson’s equation, show that \(B\) is bounded and coercive over \(X\times X\) in a well-chosen norm.
- By extending \(X\) appropriately, use the Lax-Milgram Theorem to prove that the boundary value problem above admits a unique weak solution for all sufficiently smooth \(f\).