Proceedings of the ... International Conference on Offshore Mechanics and Arctic Engineering, Volume 18, Part 5American Society of Mechanical Engineers, 1999 - Arctic regions |
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Page 173
The potential function should also satisfy the Sommerfeld's radiation condition at the far field from the structure . tion on the wet surface of the structure , Sw , therefore we can call it the general solution for the problem when a ...
The potential function should also satisfy the Sommerfeld's radiation condition at the far field from the structure . tion on the wet surface of the structure , Sw , therefore we can call it the general solution for the problem when a ...
Page 174
( 13 ) h where , the function r , ( z ) in Eq . ( 9 ) is a function of z defined by the following Eq . ( 11 ) . The function n . ( z ) in Eq . ( 10 ) is the rcomponent of the unit normal vector on the wet surface , Sw , at z The complex ...
( 13 ) h where , the function r , ( z ) in Eq . ( 9 ) is a function of z defined by the following Eq . ( 11 ) . The function n . ( z ) in Eq . ( 10 ) is the rcomponent of the unit normal vector on the wet surface , Sw , at z The complex ...
Page 329
The spectrum is a function of wave process dispersion mo the wave number of spectral maximum kmar and main direction of wave propagation ß . It has been shown that kmar is a function of m , i.e. kmar = kmar ( m . ) ...
The spectrum is a function of wave process dispersion mo the wave number of spectral maximum kmar and main direction of wave propagation ß . It has been shown that kmar is a function of m , i.e. kmar = kmar ( m . ) ...
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Contents
OMAE99PA1135 | 19 |
OMAE99PA1141 | 39 |
PROPELLERICE INTERACTION | 53 |
Copyright | |
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