Repository landing page

We are not able to resolve this OAI Identifier to the repository landing page. If you are the repository manager for this record, please head to the Dashboard and adjust the settings.

Fast integral equation methods for the modified Helmholtz equation

Abstract

Many problems in physics and engineering require the solution of the forced heat equation, utβˆ’Deltau=F(xx,u,t)u_{t}-Delta u = F(xx,u,t), with Dirichlet boundary conditions. In this thesis, we solve such PDEs in two-dimensional, multiply-connected domains, with a twice continuously differentiable boundary. We discretize the partial differential equation (PDE) in time, known as Rothe\u27s method, leading to the modified Helmholtz equation, u(xx)βˆ’alpha2Deltau(xx)=g(xx,t)u(xx)-alpha^{2}Delta u(xx)=g(xx,t). At each time step, solutions are written as the sum of a volume potential and a solution of u(xx)βˆ’alpha2Deltau(xx)=0u(xx)-alpha^{2} Delta u(xx)=0 with appropriate boundary conditions. The solution of the homogeneous PDE is written as a double layer potential with unknown density function. The density function satisfies a Fredholm integral equation of the second kind. Some advantages of integral equation methods are: the unknown function is defined only on the boundary of the domain, complex physical boundaries are easy to incorporate, the ill-conditioning associated with discretizing the governing equations is avoided, high-order accuracy is easy to attain, and far-field boundary conditions are handled naturally. The integral equation is discretized at NN points with a high-order, hybrid Gauss-trapezoidal rule resulting in a dense NtimesNN times N linear system. The linear system is solved using the generalized minimal residual method (GMRES). If the required matrix-vector multiplication is done directly, mathcalO(N2)mathcal{O}(N^{2}) operations are required. This is reduced to mathcalO(N)mathcal{O}(N) or mathcalO(NlogN)mathcal{O}(N log N) using the fast multipole method (FMM). To demonstrate the versatility of integral equation methods, the homogeneous problem is solved in bounded and unbounded, as well as simply- and multiply-connected domains. The volume integral is computed using a previously developed fast multipole-accelerated fourth-order method. This work is extended to general bounded domains and is coupled with the double layer potential. Applying Rothe\u27s method coupled with integral equation methods is tested on a collection of forced heat equation problems. This includes the homogeneous heat equation, a forced linear heat equation, and the Allen-Cahn equation

Similar works

Full text

thumbnail-image

Simon Fraser University Institutional Repository

redirect
Last time updated on 12/11/2016

Having an issue?

Is data on this page outdated, violates copyrights or anything else? Report the problem now and we will take corresponding actions after reviewing your request.