Finite Difference Discretization of Elliptic Equations: 1D Problem Lectures 2 and 3.

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Presentation transcript:

Finite Difference Discretization of Elliptic Equations: 1D Problem Lectures 2 and 3

Model Problem Poisson Equation in 1D Boundary Value Problem (BVP) Describes many simple physical phenomena (e.g.): Deformation of an elastic bar Deformation of a string under tension Temperature distribution in a bar

Model Problem Poisson Equation in 1D Solution Properties The solution always exists is always smoother then the data If for all, then for all Given the solution is unique

Numerical Finite Differences Discretization Subdivide interval into equal subintervals for

Numerical Solution Finite Differences Approximation For example … forsmall

Numerical Solution Finite Differences Equations suggests …

Numerical Solution Finite Differences ….Equations (Symmetric)

Numerical Solution Finite Differences Solution Isnon-singular ? For any Hence for any ( Is APD) exists and is unique

Numerical Solution Finite Differences Example … with Take

Numerical Solution Finite Differences … Example

Numerical Solution Finite Differences Convergence ? 1. Does the discrete solution retain the qualitative propeties of the continuous solution ? 2. Does the solution become more accurate when ? 3. Can we make for arbierarily small ?

Discretization Error Analysis Properties of A -1 Let Non-negativity for Boundedness for

Discretization Error Analysis Qualitative Properties of If for Then for

Discretization Error Analysis Qualitative Properties of Discrete Stability

Discretization Error Analysis Truncation Error For any we can show that Take

Discretization Error Analysis Error Equation Let be the discretization error Subtracting and

Discretization Error Analysis Error Equation

Discretization Error Analysis Convergence Using the discrete stability estimate on or A-priori Error Estimate

Discretization Error Analysis Numerical Example

EXAMPLE : Asymptotically,

Discretization Error Analysis Summary For a simple model problem we can produce numerical approximations of arbitrary accuracy. An a-priori error estimate gives the asymptotic dependence of the solution error on the discretization size.

Generalizations Definitions Consider a linear elliptic differential equation and a difference scheme

Generalizations Consistency The difference scheme is consistent with the differential equation if: For all smooth functions for when for all is order of accuracy

Generalizations Truncation Error or, for The truncation error results from inserting the exact solution into the difference scheme. Consistency

Generalizations Error Equation Original scheme Consistercy The errorsatisfies

Generalizations Stability Matrix norm The difference scheme is stable if (independent of )

Generalizations Stability (max row sum)

Generalizations Convergence Error equation Taking norms

Generalizations Summary Consistency + Stability Convergence ConvergenceStability Consistency

The Eigenvalue Problem Model Problem Statement Find nontrivial such that denote solutions with

The Eigenvalue Problem Application Axially Loaded Beam Small Deflection External Force Equilibrium

The Eigenvalue Problem Exact Solution or

The Eigenvalue Problem Exact Solution Thus (choose ) Larger more oscillatory larger

The Eigenvalue Problem Exact Solution

The Eigenvalue Problem Discrete Equations Difference Formulas

The Eigenvalue Problem Discrete Equations Matrix Form

The Eigenvalue Problem Error Analysis Analytical Solution: Claim that Notesince

The Eigenvalue Problem Error Analysis Analytical Solution:

What are ?

The Eigenvalue Problem Error Analysis Analytical Solution: Thus:

The Eigenvalue Problem Error Analysis Conclusions … Low modes For fixed, : second-order convergence

The Eigenvalue Problem Error Analysis … Conclusions … High modes : For as High modes ( ) are not accurate.

The Eigenvalue Problem Error Analysis … Conclusions … Low modes vs. high modes Example :

The Eigenvalue Problem Error Analysis … Conclusions … Low modes vs. high modes resolved accurate not resolved not accurate is BUT: as,, so any fixed mode converges.

The Eigenvalue Problem Error Analysis … Conclusions …

The Eigenvalue Problem Condition Number of A For a SPD matrix, the condition number is given by = maximum eigenvalue of minimum eigenvalue of Thus, for our matrix, as grows (in ) as number of grid points squared. Importance: understanding solution procedures.

The Eigenvalue Problem Link to … Discretization … Recall : or

The Eigenvalue Problem Link to … Discretization … Error equation : for as(consistency)

The Eigenvalue Problem Link to Norm Discretization We will use the modified norm for Thus, from consistency

The Eigenvalue Problem Link to ||.|| Discretization … Ingredients: 1. Rayleigh Quotient : 2. Cauchy-Schwarz Inequality : for all

The Eigenvalue Problem Link to ||.|| Discretization … Convergence proof:

The Eigenvalue Problem Link to ||.|| Discretization …

Alternative Derivation Since From error equation Multiplying by