(a) If one solution u exists for the equation on a finite connected graph), then all other solutions are of the form \
(b) If a solution \( u \) exists for the equation then
(c) If is satisfied, then a solution \( u \) exists for the equation
(a) The equationrepresents a linear partial differential equation. If \( u \) is a solution, then any function of the form is also a solution because the Laplace operator is linear. Let Then, which implies that \( v \) is also a solution.
(b) Taking the sum of both sides of over all vertices \( x \) in \( V \) weighted by gives. By the divergence theorem, the left side simplifies to \( 0 \), leading to
(c) If \( \sum_{x \in V} f(x) \mu(x) = 0 \), we can construct a function \( u \) such that \( \Delta_{\mu}u = f \). One way to find \( u \) is to solve the discrete Poisson equation by defining \( u(x) = \frac{1}{\mu(x)}\sum_{y \in N(x)}\mu(y)u(y) + \frac{f(x)}{\Delta_{\mu}x} \), where \( N(x) \) is the set of neighbors of \( x \) in \( V \). This construction ensures that \( \Delta_{\mu}u = f \).
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