1cs542g-term1-2007 Notes  No extra class tomorrow.

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Presentation transcript:

1cs542g-term Notes  No extra class tomorrow

2cs542g-term PDE’s  Subject of Partial Differential Equations is vast  We’ll focus on one particularly important equation: Called Poisson’s equation (if right hand side is zero, Laplace’s equation)  Arises almost everywhere Minimization of norm of gradient (see RBF’s) Gravitational/electrostatic potential Steady state of heat flow and other diffusion processes Stochastic processes (Brownian motion) Fluid dynamics

3cs542g-term Reduce to 1D first  Typical Boundary Value Problem (BVP):  Boundary conditions: specify solution value: “Dirichlet” specify solution derivative: “Neumann”  Can’t directly solve as a time integration

4cs542g-term Finite Difference Method  Discretize unknown solution on a grid:  Use Taylor series to estimate derivatives from values on grid

5cs542g-term Discretized Boundary Conditions  Dirichlet: substitute in known values  Neumann: discretize boundary condition, use it to extrapolate

6cs542g-term Solve!  At each grid point we have a linear equation  Combine into one large linear system (solve for all solution values simultaneously)  Resulting matrix is symmetric (negative) definite, and sparse In fact, in 1D, just tridiagonal…

7cs542g-term Higher dimensions  Lay down a regular grid as before  Matrices get even bigger, but not quite as simple structure  Notion of stencil: shorthand for matrix

8cs542g-term Stability  The preceding methods work, but not every stencil does  Need a notion of stability ~ conditioning  Example problem with central differences Matrix could be singular, or worse  Example problem with one-sided differences Information propagation is wrong

9cs542g-term Finite Difference Limitations  Accurately treating boundary conditions that don’t line up with the grid  Adaptivity