I am trying to prove the existence of a weak solution of the problem: $$ -\Delta^2 u = f \in L^2(U)\\ \\ u|_{\partial U}=\Delta u|_{\partial U} = 0 $$ on the bounded open set $U\subset\mathbb{R}^n$ which has smooth boundary. The weak formulation follows from multiplying by the test function $v$ and integration by parts:
$$ \int_U fv\,dx= \int_U \, (\Delta^2 u) v\, dx= \int_U \Delta u \Delta v \, dx + \int_{\partial U} (v \frac{\partial \Delta u}{\partial n} - \frac{\partial v}{\partial n}\Delta u)dS. $$ The second boundary vanishes for $\Delta u|_{\partial U} = 0$ and to make the first boundary term vanish we require $v$ to be in the Sobolev space $H^1_0(U)\cap H^2(U)$, so that $v=0$ on the boundary.
Therefore $u\in H^1_0(U)\cap H^2(U)$ is a weak solution if: $$ \int_U \Delta u \Delta v \, dx = \int_U fv\,dx\,\,\,\, \forall v\in H^1_0(U)\cap H^2(U). $$
Now I want to use the Lax-Milgram theorem on the bilinear form $B[u,v]=\int_U \Delta u \Delta v \, dx$. My problem is: what norm on $H^1_0(U)\cap H^2(U)$ should I use? At first I thought I could use either one of the norms of $H^1_0(U)$ or $H^2(U)$, since clearly $H^1_0(U)\cap H^2(U)$ is a closed subspace of both spaces. However I realized that this argument must be wrong, otherwise I might as well use the norm of the subspace $H^{8}(U)$ and conclude there exists a weak solution in that space.
Or should I use Lax Milgram for both $H^1_0(U)$ and $H^2(U)$ and conclude that the weak solution is in their intersection?
My second problem: when proving the coercivity of $B[u,v]$, I think I need an inequality like $\int_U |\Delta u|^2 dx \geq C\int_U u^2 dx$ for some constant $C$. I know this holds for $u\in H^2_0(U)$ but I don't see why this should hold in $H^1_0(U)\cap H^2(U)$?
A sequence $(u_n)$ in $H^2\cap H^1_0$ which converges to $u$ in the $H^2$ norm is naturally in $H^2$ and hence $H^1$. But why could we choose all $u_n$ to be in $C^{\infty}_c$, so that $u$ is in $H^1_0$?
– ScroogeMcDuck Apr 08 '13 at 17:54