 Solution

The zero Dirichlet boundary condition must be part of the definition. Thus $u\in H^1(B)$ is a weak solution precisely when $u\in H_0^1(B)$, equivalently its Sobolev trace vanishes on $\partial B$, andHere ${\chi }_E$ is the indicator function of the measurable set $E$. One may initially require the identity only for test functions $\varphi \in C_c^{\infty }(B)$: both sides are continuous in the Sobolev norm, and the definition of the zero-trace Sobolev space then extends it to all $H_0^1(B)$. This formulation uses first weak derivatives and encodes $-\Delta u={\chi }_E$ without assuming classical second derivatives.