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The boundary particle method (BPM) is a boundary-only discretization of an inhomogeneous partial differential equation by combining the RC-MRM with strong-form meshless boundary collocation discretization schemes, such as the [[method of fundamental solution]] (MFS), [[boundary knot method]] (BKM), [[regularized meshless method]] (RMM), [[singular boundary method]] (SBM), and [[Trefftz method]] (TM). The BPM has been applied to problems such as nonhomogeneous [[Helmholtz]] and [[convection-diffusion equation]]. The BPM interpolation representation is of a [[wavelet]] series.
For the application of the BPM to [[Helmholtz]],<ref name="Chena" /> [[Siméon Denis Poisson|Poisson]]<ref name="Chenb" /> and [[plate bending]] problems,<ref>Fu ZJ, Chen W, Yang W, Winkler plate bending problems by a truly boundary-only boundary particle method. Computational Mechanics 2009,44(6): 757–563</ref> the high-order [[fundamental solution]] or general solution, harmonic function<ref>Hon YC, Wu ZM, A numerical computation for inverse boundary determination problem. Engineering Analysis with Boundary Elements 2000,24(7–8): 599–606</ref> or [[Trefftz]] function (T-complete functions)<ref>Chen W, Fu ZJ, Qin QH, Boundary particle method with high-order Trefftz functions. CMC: Computers, Materials & Continua 2010,13(3): 201–217</ref> are often used, for instance, those of [[Marcel Berger|Berger]]
==Further comments==
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