If a continuous function \( h: \Omega \to \mathbb{R} \) satisfies \( \int_{B(x_0,r)} h(x) \, dx = 0 \) for all balls \( B(x_0,r) \subseteq \Omega \), then it must be that \( h(x) = 0 \) for all \( x \in \Omega \). The discussion suggests proving the contrapositive: if \( h \) is not identically zero, then there exists a point \( x_0 \) and radius \( r \) such that the integral is non-zero. By continuity, if \( h(x_0) \neq 0 \), one can find a neighborhood around \( x_0 \) where \( h(x) \) remains bounded away from zero, leading to a non-zero integral. This establishes the necessary condition that if the integral is zero everywhere, the function must be zero everywhere.