scholarly journals Numerical simulation of the wind wave fields in Lake Dianshan

2011 ◽  
Vol 23 (5) ◽  
pp. 783-788
Author(s):  
ZHANG Hongsheng ◽  
◽  
GU Junbo ◽  
WEN Wujian
2016 ◽  
Vol 41 (2) ◽  
pp. 130-135 ◽  
Author(s):  
A. A. Kubryakov ◽  
V. G. Polnikov ◽  
F. A. Pogarskii ◽  
S. V. Stanichnyi

2008 ◽  
Vol 38 (9) ◽  
pp. 2038-2055 ◽  
Author(s):  
Guillemette Caulliez ◽  
Vladimir Makin ◽  
Vladimir Kudryavtsev

Abstract The specific properties of the turbulent wind stress and the related wind wave field are investigated in a dedicated laboratory experiment for a wide range of wind speeds and fetches, and the results are analyzed using the wind-over-waves coupling model. Compared to long-fetch ocean wave fields, wind wave fields observed at very short fetches are characterized by higher significant dominant wave steepness but a much smaller macroscale wave breaking rate. The surface drag dependence on fetch and wind then closely follows the dominant wave steepness dependence. It is found that the dimensionless roughness length z*0 varies not only with wind forcing (or inverse wave age) but also with fetch. At a fixed fetch, when gravity waves develop, z*0 decreases with wind forcing according to a −1/2 power law. Taking into account the peculiarities of laboratory wave fields, the WOWC model predicts the measured wind stress values rather well. The relative contributions to surface drag of the equilibrium-range wave-induced stress and the airflow separation stress due to wave breaking remain small, even at high wind speeds. At moderate to strong winds, the form drag resulting from dominant waves represents the major wind stress component.


1986 ◽  
Vol 1 (20) ◽  
pp. 47
Author(s):  
W.L. Neu ◽  
S.H. Kwon

This study is concerned with the operation of spectral wind wave models. Many spectral wind wave models use a growth mechanism which operates on the point spectrum with directionality being introduced after the fact by the use of a spreading function. It is recognized here that this approach leads to errors whenever the wind and wave fields are not aligned. This is demonstrated by comparing the performance of two first generation models under various conditions. One makes use of a point spectral growth mechanism and follows the operation of the Spectral Ocean Wave Model (SOWM). The other uses a directional growth mechanism but is otherwise the same as the first. A large difference between the models is noted for swell corrupted seas.


Author(s):  
M. Spies ◽  
G. Hubschen ◽  
N.K. Batra ◽  
K.E. Simmonds ◽  
R.B. Mignogna

2008 ◽  
Vol 55 (11) ◽  
pp. 894-905 ◽  
Author(s):  
Witold Cieślikiewicz ◽  
Barbara Paplińska-Swerpel

2020 ◽  
Vol 65 (1) ◽  
pp. 33-50
Author(s):  
Alexander A. Kovtun ◽  
◽  
Eugenia L. Lyskova ◽  
Konstantin Yu. Sannikov ◽  
◽  
...  

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