Christopher Crawford PHY

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Christopher Crawford PHY 416 2014-10-20 §3.1 Laplace’s equation Christopher Crawford PHY 416 2014-10-20

Outline Overview Summary of Ch. 2 Intro to Ch. 3, Ch. 4 Laplacian – curvature (X-ray) operator PDEs in physics with Laplacian Laplacian in 1-d, 2-d, 3-d Boundary conditions Classification of hyperbolic, elliptic, parabolic PDE’s External boundaries: uniqueness theorem Internal boundaries: continuity conditions Numerical solution – real-life problems solved on computer Relaxation method Finite difference Finite element analysis – HW6

Summary of Ch. 2

Laplacian in physics Derivative chain: potential to conservative flux to source Example: electrostatic potential, electric flux, and charge

Laplacian in lower dimensions 1-d Laplacian 2nd derivative: curvature Flux: doesn’t spread out in space Solution: Boundary conditions: Mean field theorem 2-d Laplacian Flux: spreads out on surface 2nd order elliptic PDE No trivial integration Depends on boundary cond. No local extrema

Laplacian in 3-d Laplace equation: Now curvature in all three dimensions – harder to visualize All three curvatures must add to zero Unique solution is determined by fixing V on boundary surface Mean value theorem:

Classification of Conic Sections Quadratic bilinear form: matrix of coefficients Elliptic – 2 positive eigenvalues, det > 0 Hyperbolic – 1 negative eigenvalue, det < 0 Parabolic – 1 null eigenvalue, det = 0

Classification of 2nd order PDEs Same as conic sections (where ) Elliptic – Laplacian Spacelike boundary everywhere 1 boundary condition at each point on the boundary surface Hyperbolic – wave equation Timelike (initial) and spacelike (edges) boundaries 2 initial conditions in time, 1 boundary condition at each edge Parabolic – diffusion equation 1 initial condition in time, 1 boundary condition at each edge

External boundary conditions Uniqueness theorem – difference between any two solutions of Poisson’s equation is determined by values on the boundary External boundary conditions:

Internal boundary conditions Possible singularities (charge, current) on the interface between two materials Boundary conditions “sew” together solutions on either side of the boundary External: 1 condition on each side Internal: 2 interconnected conditions General prescription to derive any boundary condition: