If \( f \) and \( g \) are the solutions of Laplace equation then \( \nabla \cdot \{(f \nabla g) - (g \nabla f)\ = \)}
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This expression is the integrand used in Green's Second Identity:
\( \int_V (f\nabla^2 g - g\nabla^2 f) dV = \oint_S (f\nabla g - g\nabla f) \cdot d\mathbf{\hat{n}} \). Since both functions satisfy Laplace's equation, both sides of the identity are identically zero.