Numerical simulation of mass transport in internal solitary waves

2012 ◽  
Vol 24 (1) ◽  
pp. 016602 ◽  
Author(s):  
Maher Salloum ◽  
Omar M. Knio ◽  
Alan Brandt
2016 ◽  
Vol 114 ◽  
pp. 250-258 ◽  
Author(s):  
Haibin LÜ ◽  
Jieshuo Xie ◽  
Jiexin Xu ◽  
Zhiwu Chen ◽  
Tongya Liu ◽  
...  

2019 ◽  
Vol 873 ◽  
pp. 1-17 ◽  
Author(s):  
Yangxin He ◽  
Kevin G. Lamb ◽  
Ren-Chieh Lien

Large internal solitary waves with subsurface cores have recently been observed in the South China Sea. Here fully nonlinear solutions of the Dubreil–Jacotin–Long equation are used to study the conditions under which such cores exist. We find that the location of the cores, either at the surface or below the surface, is largely determined by the sign of the vorticity of the near-surface background current. The results of a numerical simulation of a two-dimensional shoaling internal solitary wave are presented which illustrate the formation of a subsurface core.


2016 ◽  
Vol 35 (1) ◽  
pp. 1-10
Author(s):  
Haibin Lü ◽  
Jieshuo Xie ◽  
Yuan Yao ◽  
Jiexin Xu ◽  
Zhiwu Chen ◽  
...  

2016 ◽  
Vol 58 ◽  
pp. 118-134 ◽  
Author(s):  
Hai Zhu ◽  
Lingling Wang ◽  
E.J. Avital ◽  
Hongwu Tang ◽  
J.J.R. Williams

MATEMATIKA ◽  
2018 ◽  
Vol 34 (2) ◽  
pp. 333-350 ◽  
Author(s):  
Mun Hoe Hooi ◽  
Wei King Tiong ◽  
Kim Gaik Tay ◽  
Kang Leng Chiew ◽  
San Nah Sze

In this paper, we look at the propagation of internal solitary waves overthree different types of slowly varying region, i.e. a slowly increasing slope, a smoothbump and a parabolic mound in a two-layer fluid flow. The appropriate mathematicalmodel for this problem is the variable-coefficient extended Korteweg-de Vries equation.The governing equation is then solved numerically using the method of lines. Ournumerical simulations show that the internal solitary waves deforms adiabatically onthe slowly increasing slope. At the same time, a trailing shelf is generated as theinternal solitary wave propagates over the slope, which would then decompose intosecondary solitary waves or a wavetrain. On the other hand, when internal solitarywaves propagate over a smooth bump or a parabolic mound, a trailing shelf of negativepolarity would be generated as the results of the interaction of the internal solitarywave with the decreasing slope of the bump or the parabolic mound. The secondarysolitary waves is observed to be climbing the negative trailing shelf.


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