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A harmonic function with a normal derivative of 0 on the boundary of an area is constant within that area. The Dirichlet problem is: ∇2 u(x ) = −f (x ) , x ∈ R , u(x ) = g(x ) for all x ∈ S. It has a unique solution. The Neumann problem is: ∇2 u(x ) = −f (x ) , x ∈ R , ∂u(x ) = h(x ) for all x ∈ S. ∂n 32 Mathematics Formulary by ir. A. Wevers The solution is unique except for a constant. The solution exists if: f (x )d3 V = − R h(x )d2 A S A fundamental solution of the Laplace equation satisfies: ∇2 u(x ) = −δ(x ) This has in 2 dimensions in polar coordinates the following solution: u(r) = ln(r) 2π This has in 3 dimensions in spherical coordinates the following solution: u(r) = 1 4πr The equation ∇2 v = −δ(x − ξ ) has the solution v(x ) = 1 4π|x − ξ | After substituting this in Green’s 2nd theorem and applying the sieve property of the δ function one can derive Green’s 3rd theorem: u(ξ ) = − ∇2 u 3 1 d V + r 4π 1 4π R 1 ∂u ∂ −u r ∂n ∂n 1 r d2 A S The Green function G(x, ξ ) is defined by: ∇2 G = −δ(x − ξ ), and on boundary S holds G(x, ξ ) = 0.

2. Introduce: x˙ = u and y˙ = v, this leads to x ¨ = u˙ and y¨ = v. ˙ This transforms a n-dimensional set of second order equations into a 2n-dimensional set of first order equations. 44 Mathematics Formulary by ir. A. 1 Quadratic forms in IR2 The general equation of a quadratic form is: xT Ax + 2xT P + S = 0. Here, A is a symmetric matrix. , λn ) holds: uT Λu + 2uT P + S = 0, so all cross terms are 0. u = (u, v, w) should be chosen so that det(S) = +1, to maintain the same orientation as the system (x, y, z).

We define the notations Cρ+ = {z||z| = ρ, (z) ≥ 0} and Cρ− = {z||z| = ρ, (z) ≤ 0} and M + (ρ, f ) = max+ |f (z)|, M − (ρ, f ) = max− |f (z)|. We assume that z∈Cρ z∈Cρ f (z) is analytical for (z) > 0 with a possible exception of a finite number of singular points which do not lie on the real axis, lim ρM + (ρ, f ) = 0 and that the integral exists, than ρ→∞ ∞ f (x)dx = 2πi Resf (z) in (z) > 0 −∞ Replace M + by M − in the conditions above and it follows that: ∞ f (x)dx = −2πi Resf (z) in (z) < 0 −∞ Jordan’s lemma: let f be continuous for |z| ≥ R, (z) ≥ 0 and lim M + (ρ, f ) = 0.

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