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This detailed outline covers the convergence theory and issues in solving integral equations using finite element and basis function approaches. It discusses the difficulties and methods for achieving stability and consistency, with examples and practical problems analyzed for both first and second-kind equations. The document outlines approaches like Galerkin and collocation, Nystrom methods, and strategies for minimizing residuals. It includes theoretical analyses and numerical results to illustrate the convergence properties and challenges in discretization. Additionally, it offers insights into the basic assumptions and derivations related to second-kind integral equations, emphasizing the importance of accuracy in approximating integrals and the implications for solving complex equations.
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Generalized Finite Element Methods Integral Equation Methods Discretization Convergence Theory Suvranu De
Outline Integral Equation Methods Reminder about Galerkin and Collocation Example of convergence issues in 1-D First and second kind integral Equations Develop some intuition about the difficulties Convergence for second-kind equations Show consistency and stability issues Nystrom Methods High Order Convergence
Basis Function Approach Integral Equation Basics Basic Idea Integral Equation: Example Basis Represent circle with straight lines
Basis Function Approach Integral Equation Basics Piecewise Constant Straight Sections Example. 1) Pick a set of n Points on the surface 2) Define a new surface by connecting points with n lines.
Basis Function Approach Integral Equation Basics Residual Definition and minimization
Basis Function Approach Laplace’s Equation in 2-D Residual minimization using test functions
Basis Function Approach Laplace’s Equation in 2-D Collocation
Basis Function Approach Laplace’s Equation in 2-D Galerkin A is symmetric
Example Problems Convergence Analysis 1-D First Kind Equation The potential is given The density must be computed Solution = 3x
Example Problems Convergence Analysis Collocation Discretization of 1-D Equation Centroid Collocated Piecewise Constant Scheme
Example Problems Convergence Analysis Collocation Discretization of 1-D Equation - The Matrix One column for each density value One row for each collocation point
Numerical Results with increasing n n = 40 n = 10 n = 20 Answers Are Getting Worse!!!
Example Problems Convergence Analysis 1-D Second Kind Equation The potential is given The density must be computed Solution = 3x
Example Problems Convergence Analysis Collocation Discretization of 1-D Equation Centroid Collocated Piecewise Constant Scheme
Example Problems Convergence Analysis Collocation Discretization of 1-D Equation - The Matrix
Numerical Results with increasing n n = 40 n = 10 n = 20 Answers Are Improving!!!
Example Problems Convergence Analysis 1-D First Kind Equation Difficulty Denote the integral operator as K The integral operator is singular 0 -1 1
Example Problems Convergence Analysis 1-D First Kind Difficulty from the Matrix Collocation Generates a Discrete form of K Solution = 3x
Numerical Results with increasing n n = 10 n = 40 n = 20 Eigenvalues accumulating at zero.
Example Problems Convergence Analysis Intuition about the Eigenvalues As the discretization is refined, K’s null space can be more accurately represented
-1 1 -1 1 Example Problems Convergence Analysis 2-D Kind Equation has fewer problems The second Kind equation + = -1 1
Numerical Results with increasing n n = 10 n = 40 n = 20 Eigenvalues do not get closer to zero.
Second Kind Theory Convergence Analysis Basic Assumptions General 2nd-Kind Integral Equation Assume the equation is uniquely solvable Then a discretization method converges if consistent
Second Kind Theory Convergence Analysis Kn for collocation. Aim: Derive a semidiscrete form of the second kind equation The point collocation equation for the ith collocation point Let us denote This is the projection of s(x) onto the basis function space
Second Kind Theory Convergence Analysis Kn for collocation. Hence Let us define the interpolation operator for any function u(x) Hence
Second Kind Theory Convergence Analysis Kn for collocation. From last slide We will define the semidiscrete operator Kn such that Hence
Second Kind Theory Convergence Analysis Rough Proof Operator Form for the integral equation Semidiscrete Integral Equation Subtracting And neglecting (Y-V Y)
Second Kind Theory Convergence Analysis Rough Proof continued The equation for the solution error (previous slide) Taking norms Error which should go to zero as n increases Needs a bound, this is discrete stability Goes to zero with n by consistency
Second Kind Theory Convergence Analysis Stability Bound Norm of Solution error Deriving the stability bound Taking Norms Bounded by C by Assumption
Second Kind Theory Convergence Analysis Stability Bound Continued Repeating from last slide Bounded by C by Assumption Bounding Terms Less than for n larger than n0, by consistency
Second Kind Theory Convergence Analysis Rough Proof completed Final Result What does it mean? The discretization convergence of a second kind integral equation solver depends only on how well the integral is approximated.
1-D Second Kind Example Nystrom Method Collocation Discretization of 1-D Equation Integral Equation Apply Quadrature to Collocation Equation Now set quadrature points = collocation points
1-D Second Kind Example Nystrom Method Collocation Discretization of 1-D Equation Continued Set quadrature points = collocation points System of n equations in n unknowns Collocation equation per quad/colloc point Unknown density per quad/colloc point
1-D Second Kind Example Nystrom Method 1-D Discretization - Matrix Comparison Nystrom Matrix Piecewise constant collocation Matrix
1-D Second Kind Example Nystrom Method 1-D Discretization - Matrix Comparison Continued Nystrom Matrix Just Green’s function evals - No integrals Entries each have a quadrature weight Collocation points are quadrature points High order quadrature = faster convergence? Piecewise constant collocation Matrix Integrals of Green’s functions over line sections Distant terms equal Green’s function Collocation points are basis function centriods Low order method always
1-D Second Kind Example Nystrom Method Convergence Theorem What does this mean? The discretization error for the Nystrom method applied to a second kind integral equation converges AT THE SAME RATE as the underlying quadrature! Gauss Quad ->Exponential Convergence!
1-D Second Kind Example Nystrom Method Convergence Comparison Piecewise-Constant Centroid Collocation E r r o r Gauss-Quad Nystrom n
1-D Second Kind Example Nystrom Method Convergence Caveat If Nystrom methods can have exponential convergence, why use anything else? Gaussian Quadrature has exponential convergence only for nonsingular kernels Most physical problems of interest have singular kernels (1/r, e^ikr/r, etc)
Summary Integral Equation Methods Reviewed Galerkin and Collocation Example of convergence issues in 1-D First and second kind integral Equations Examined by example operator null spaces Convergence for second-kind equations Show consistency and stability issues Nystrom Methods High Order Convergence Did not touch on singular integrands, the most common case in practice.