On the numerical solution of the elastodynamic problem by a boundary integral equation method
Roman Chapko, Leonidas Mindrinos
TL;DR
This paper addresses the Dirichlet initial boundary value problem for the time-dependent elastodynamic equation in an unbounded 2D exterior domain, $u_{tt}=\\Delta^*u$ in $D\\times(0,\\infty)$, with $u|_\\Gamma=f$ and zero initial data. A Laguerre-transform-based semi-discretization in time yields a sequence of stationary Navier problems $\\Delta^*u_n-\\kappa^2u_n=\\sum_{m=0}^{n-1}\\beta_{n-m}u_m$ coupled through $\\beta_n=\\kappa^2(n+1)$ and $u_n|_\\Gamma=f_n$. These are solved with a boundary integral equation framework using explicit fundamental solutions $E_n$ and layer potentials, leading to first-kind and second-kind systems for densities $q_n$ on $\\Gamma$, with well-posedness in Hölder spaces. A fully discrete scheme employing trig quadrature and a spectral-type Laguerre expansion demonstrates exponential convergence for analytic data and accurate exterior elastodynamics simulations without domain truncation.
Abstract
A numerical method for the Dirichlet initial boundary value problem for the elastic equation in the exterior and unbounded region of a smooth closed simply connected 2-dimensional domain, is proposed and investigated. This method is based on a combination of a Laguerre transformation with respect to the time variable and a boundary integral equation approach in the spatial variables. Using the Laguerre transformation in time reduces the time-depended problem to a sequence of stationary boundary value problems, which are solved by a boundary layer approach resulting to a sequence of boundary integral equations of the first kind. The numerical discretization and solution are obtained by a trigonometrical quadrature method. Numerical results are included.
