A wind-wave tank study of the azimuthal response of a Ka-band scatterometer

1991 ◽  
Vol 29 (1) ◽  
pp. 143-148 ◽  
Author(s):  
J.-P. Giovanangeli ◽  
L.F. Bliven ◽  
O. Le Calve
Keyword(s):  
Author(s):  
C-A. Guerin ◽  
O. Boisot ◽  
S. Pioch ◽  
A. Bringer ◽  
G. Caulliez ◽  
...  
Keyword(s):  
Ka Band ◽  

2015 ◽  
Vol 120 (5) ◽  
pp. 3261-3285 ◽  
Author(s):  
Olivier Boisot ◽  
Sébastien Pioch ◽  
Christophe Fatras ◽  
Guillemette Caulliez ◽  
Alexandra Bringer ◽  
...  

1999 ◽  
Author(s):  
Christian M. Senet ◽  
Nicole Braun ◽  
Philipp A. Lange ◽  
Joerg Seemann ◽  
Heiko Dankert ◽  
...  

2017 ◽  
Vol 34 (10) ◽  
pp. 2129-2139 ◽  
Author(s):  
Naohisa Takagaki ◽  
Satoru Komori ◽  
Mizuki Ishida ◽  
Koji Iwano ◽  
Ryoichi Kurose ◽  
...  

AbstractIt is important to develop a wave-generation method for extending the fetch in laboratory experiments, because previous laboratory studies were limited to the fetch shorter than several dozen meters. A new wave-generation method is proposed for generating wind waves under long-fetch conditions in a wind-wave tank, using a programmable irregular-wave generator. This new method is named a loop-type wave-generation method (LTWGM), because the waves with wave characteristics close to the wind waves measured at the end of the tank are reproduced at the entrance of the tank by the programmable irregular-wave generator and the mechanical wave generation is repeated at the entrance in order to increase the fetch. Water-level fluctuation is measured at both normal and extremely high wind speeds using resistance-type wave gauges. The results show that, at both wind speeds, LTWGM can produce wind waves with long fetches exceeding the length of the wind-wave tank. It is observed that the spectrum of wind waves with a long fetch reproduced by a wave generator is consistent with that of pure wind-driven waves without a wave generator. The fetch laws between the significant wave height and the peak frequency are also confirmed for the wind waves under long-fetch conditions. This implies that the ideal wind waves under long-fetch conditions can be reproduced using LTWGM with the programmable irregular-wave generator.


1984 ◽  
Vol 89 (C1) ◽  
pp. 627 ◽  
Author(s):  
Jung-Tai Lin ◽  
Mohamed Gad-el-Hak
Keyword(s):  

2018 ◽  
Vol 2018 (0) ◽  
pp. GS2-4
Author(s):  
Shunsaku TAKAHATA ◽  
Naohisa TAKAGAKI ◽  
Naoya SUZUKI ◽  
Keita TAKANE ◽  
Yuhei SHIMIZU ◽  
...  
Keyword(s):  

1999 ◽  
Vol 104 (C2) ◽  
pp. 3243-3263 ◽  
Author(s):  
William J. Plant ◽  
William C. Keller ◽  
Vahid Hesany ◽  
Tetsu Hara ◽  
Erik Bock ◽  
...  
Keyword(s):  

2008 ◽  
Vol 38 (7) ◽  
pp. 1597-1606 ◽  
Author(s):  
T. Lamont-Smith ◽  
T. Waseda

Abstract Wave wire data from the large wind wave tank of the Ocean Engineering Laboratory at the University of California, Santa Barbara, are analyzed, and comparisons are made with published data collected in four other wave tanks. The behavior of wind waves at various fetches (7–80 m) is very similar to the behavior observed in the other tanks. When the nondimensional frequency F* or nondimensional significant wave height H* is plotted against nondimensional fetch x*, a large scatter in the data points is found. Multivariate regression to the dimensional parameters shows that significant wave height Hsig is a function of U2x and frequency F is a function of U1.25x, where U is the wind speed and x is the horizontal distance, with the result that in general for wind waves at a particular fetch in a wave tank, approximately speaking, the wave frequency is inversely proportional to the square root of the wind speed and the wavelength is proportional to the wind speed. Similarly, the wave height is proportional to U1.5 and the orbital velocity is proportional to U. Comparison with field data indicates a transition from this fetch law to the conventional one [the Joint North Sea Wave Project (JONSWAP)] for longer fetch. Despite differences in the fetch relationship for the wave tank and the field data, the wave height and wave period satisfy Toba’s 3/2 power law. This law imposes a strong constraint on the evolution of wind wave energy and frequency; consequently, the energy and momentum retention rate are not independent. Both retention rates grow with wind speed and fetch at the short fetches present in the wave tank. The observed retention rates are completely different from those typically observed in the field, but the same constraint (Toba’s 3/2 law) holds true.


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