Upload
alta
View
165
Download
1
Tags:
Embed Size (px)
DESCRIPTION
§3.1 Laplace’s equation. Christopher Crawford PHY 311 2014-02-19. Outline. Overview Summary of Ch. 2 Intro to Ch. 3, Ch. 4 Laplacian – cur vature (X-ray) operator PDE’s in physics with Laplacian Laplacian in 1-d, 2-d, 3-d - PowerPoint PPT Presentation
Citation preview
§3.1 Laplace’s equation
Christopher CrawfordPHY 311
2014-02-19
Outline• Overview
Summary of Ch. 2Intro to Ch. 3, Ch. 4
• Laplacian – curvature (X-ray) operatorPDE’s in physics with LaplacianLaplacian in 1-d, 2-d, 3-d
• Boundary conditionsClassification of hyperbolic, elliptic, parabolic PDE’sExternal boundaries: uniqueness theorem Internal boundaries: continuity conditions
• Numerical solution – real-life problems solved on computerRelaxation methodFinite differenceFinite element analysis – HW5
2
Summary of Ch. 2
3
Laplacian in physics• The source of a conservative flux
– Example: electrostatic potential, electric flux, and charge
4
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– 2nd derivative: curvature– Flux: spreads out on surface– 2nd order elliptic PDE– No trivial integration
• Depends on boundary cond.
– Mean field theorem• No local extrema
5
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:
6
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– Timelike (initial) and spacelike (edges) boundaries– 1 initial condition in time, 1 boundary condition at each edge
7
External boundary conditions• Uniqueness theorem – difference between any two solutions of
Poisson’s equation is determined by values on the boundary
• External boundary conditions:
8
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:
9
Solution: relaxation method1. Discretize Laplacian2. Fix boundary values3. Iterate adjusting potentials on the grid until solution settles
10
Solution: finite difference method1. Discretize Laplacian2. Fix boundary values3. Solve matrix equation for potential on grid
11
Solution: finite element method1. Weak formulation: integral equation2. Approximate potential by basis functions on a mesh3. Integrate basis functions; solve matrix equation
12