In this paper, a new indirect boundary element formulation for two-dimensional elastodynamic problems is
presented. The formulation makes use of a static fundamental solution. For accurate solution, the location of the
fictitious boundary is chosen to be the same as problem boundary. The relevant fundamental solution is integrated
over lines. The method is combined with the Dual Reciprocity Method (DRM), for handling the domain
integral concerning to the domain inertia terms. A suitable approximation (traditional function C-R is used) for
the inertia terms (or, domain accelerations), is used to transform the domain integral to the boundary. The
discretization is performed on the boundary, or a boundary-like geometry. The method is easy to code and
efficient as presented by the numerical examples.