Proceedings of the ... International Conference on Offshore Mechanics and Arctic Engineering, Volume 14, Part 4American Society of Mechanical Engineers, 1995 - Arctic regions |
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Page 124
The first is how much spray is generated during a ship / wave collision and how is it distributed over the topside of the ship . Panov ( 1971 ) proposed an empirical formula for the frequency of spraying of a medium - sized fishing ...
The first is how much spray is generated during a ship / wave collision and how is it distributed over the topside of the ship . Panov ( 1971 ) proposed an empirical formula for the frequency of spraying of a medium - sized fishing ...
Page 125
The spray droplet trajectory begins at the spray source point , S ( x , y ) , with a vertical velocity v , and zero horizontal velocity relative to the ship . It ends at the centre of the grid cell at O ' . Chung ( 1994b ) describes how ...
The spray droplet trajectory begins at the spray source point , S ( x , y ) , with a vertical velocity v , and zero horizontal velocity relative to the ship . It ends at the centre of the grid cell at O ' . Chung ( 1994b ) describes how ...
Page 126
3 SPRAY THERMODYNAMICS MODULE Figure 4a exhibits similar power law behaviour for the dependence of total spray mass on wave height and ship speed , as does Equation 1. The model results are therefore consistent with the experiments .
3 SPRAY THERMODYNAMICS MODULE Figure 4a exhibits similar power law behaviour for the dependence of total spray mass on wave height and ship speed , as does Equation 1. The model results are therefore consistent with the experiments .
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Contents
139 | 95 |
Mechanical Behavior of Ice Loaded Optical Ground Wires | 107 |
Influence of the Surface Liquid Film on Cylinder Icing Under Marine Conditions | 115 |
Copyright | |
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