Doppler Sonar Observations of Langmuir Circulation

Author(s):  
Jerome A. Smith
1987 ◽  
Vol 82 (4) ◽  
pp. 1469-1469
Author(s):  
Robert L. Simmons ◽  
Clifton M. Wyant
Keyword(s):  

2017 ◽  
Vol 17 (18) ◽  
pp. 6056-6068 ◽  
Author(s):  
Ki-Seung Lee
Keyword(s):  

2015 ◽  
Vol 34 (5) ◽  
pp. 1-11 ◽  
Author(s):  
Guojing Li ◽  
Dongxiao Wang ◽  
Ju Chen ◽  
Jinglong Yao ◽  
Lili Zeng ◽  
...  

Author(s):  
R. Pinkel ◽  
H. Merrifield ◽  
J. Smith
Keyword(s):  

2012 ◽  
Vol 699 ◽  
pp. 79-93 ◽  
Author(s):  
A. E. Tejada-Martínez ◽  
C. E. Grosch ◽  
N. Sinha ◽  
C. Akan ◽  
G. Martinat

AbstractWe report on disruption of the log layer in the resolved bottom boundary layer in large-eddy simulations (LES) of full-depth Langmuir circulation (LC) in a wind-driven shear current in neutrally-stratified shallow water. LC consists of parallel counter-rotating vortices that are aligned roughly in the direction of the wind and are generated by the interaction of the wind-driven shear with the Stokes drift velocity induced by surface gravity waves. The disruption is analysed in terms of mean velocity, budgets of turbulent kinetic energy (TKE) and budgets of TKE components. For example, in terms of mean velocity, the mixing due to LC induces a large wake region eroding the classical log-law profile within the range $90\lt { x}_{3}^{+ } \lt 200$. The dependence of this disruption on wind and wave forcing conditions is investigated. Results indicate that the amount of disruption is primarily determined by the wavelength of the surface waves generating LC. These results have important implications for turbulence parameterizations for Reynolds-averaged Navier–Stokes simulations of the coastal ocean.


1989 ◽  
Vol 1 (2) ◽  
pp. 149-153
Author(s):  
K. V. Konyaev ◽  
E. A. Leont'eva ◽  
S. I. Muyakshin

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