1990
DOI: 10.1061/(asce)0733-950x(1990)116:2(191)
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Time‐Domain Solution for Second‐Order Wave Diffraction

Abstract: In presenting this thesis in partial fulfilment of the requirements for an advanced degree at the University of British Columbia, I agree that the Library shall make it freely available for reference and study. I further agree that permission for extensive copying of this thesis for scholarly purposes may be granted by the head of my department or by his or her representatives. It is understood that copying or publication of this thesis for financial gain shall not be allowed without my written permission.

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Cited by 27 publications
(5 citation statements)
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“…, ) , d can be discretized to finite quadrilateral panels. According to some existing studies [17,26], the discretization of Equation ( 11) can be expressed as below when the source point is located on the body surface:…”
Section: Fundamentalsmentioning
confidence: 99%
“…, ) , d can be discretized to finite quadrilateral panels. According to some existing studies [17,26], the discretization of Equation ( 11) can be expressed as below when the source point is located on the body surface:…”
Section: Fundamentalsmentioning
confidence: 99%
“…Compared to the first one, the Rankine source method removes the explicit memory effect from the integral equation. Typical works of this method are finished by Isaacson and Cheung [15,16] calculating the second-order wave loads on a single cylinder. Nevertheless, the solution requires truncating the fluid field at some finite distance.…”
Section: Introductionmentioning
confidence: 99%
“…A lot of researches have been done on the time-domain problems. Using the Boundary Element Method (BEM) [1][2][3][4][5] , BAI and TENG [6] have solved the linear and second order wave radiation and diffraction problem. WANG and WU [7] , using the Finite Element Method (FEM), have done fully nonlinear and second-order wave-body interaction problems.…”
Section: Introductionmentioning
confidence: 99%