2017
DOI: 10.1016/s1001-6058(16)60786-2
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BEM for wave interaction with structures and low storage accelerated methods for large scale computation

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Cited by 14 publications
(2 citation statements)
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“…In each time step, the radiation-velocity potential that satisfies the Laplace equation is calculated using an integral-equation method. By applying Green's second identity in the fluid domain, the boundary-value problem described above is converted into the following boundary integral equation in a conventional manner (Teng et al [23]).…”
Section: Integral Equationmentioning
confidence: 99%
“…In each time step, the radiation-velocity potential that satisfies the Laplace equation is calculated using an integral-equation method. By applying Green's second identity in the fluid domain, the boundary-value problem described above is converted into the following boundary integral equation in a conventional manner (Teng et al [23]).…”
Section: Integral Equationmentioning
confidence: 99%
“…where the summation ranges over all panels and F p (r) and U p (r) denote induced potential and velocity from the p-th element with unit singularity distribution to the field point r; see, e.g., [30] and the references cited there. We mention here that a minimum number of 10-20 elements per wavelength is used in discretizing the free surface, in order to eliminate errors due to damping and dispersion associated with the above discrete scheme.…”
Section: A Novel Bem For the Diffraction And Radiation Problems In 3dmentioning
confidence: 99%