scholarly journals Relationship of Internal Waves with Tide and Wind Drift Effects and Propagation of Internal Kelvin Waves in Brackish Lake Nakaumi.

1997 ◽  
Vol 58 (3) ◽  
pp. 241-260
Author(s):  
Tomoyasu FUJII
2001 ◽  
Vol 17 ◽  
pp. 111-116 ◽  
Author(s):  
Tomoyasu FUJII ◽  
Akira NISHIMURA ◽  
Nobuo SHIMIZU ◽  
Hidenori TANAKA

Limnology ◽  
2019 ◽  
Vol 21 (2) ◽  
pp. 197-205
Author(s):  
Ja Yeong Park ◽  
Shogo Sugahara ◽  
Michiko Egawa ◽  
Yasushi Seike

AbstractHighly concentrated dissolved silicate was detected in pore water from anoxic-reducing sediment in Lake Nakaumi, a brackish lake. Silicate concentration also simultaneously increased with total hydrogen sulfide concentration during the summer. Generally, dissolved silicate is readily adsorbed onto ferric hydroxide and precipitates in an oxidative environment. In this study, we focused on the behavior of ferric hydroxide adsorbing silicate in sediment and determined that hydrogen sulfide was the main cause of dissolved silicate elution from ferric hydroxide adsorbing silicate because the hydrogen sulfide produced via microbiological processes in the anoxic-reducing environment was reducible for other metal oxides. According to laboratory experiments, silicate was released from ferric hydroxide by reacting with sodium sulfide, causing increasing elution of dissolved silicate from anoxic-reducing sediments with increasing concentration of sodium sulfide in the solutions. This result shows that hydrogen sulfide is very crucial for silicate release under a reducing environment. Therefore, in Lake Nakaumi, silicate would be released from the bottom after ferric hydroxide adsorbing silicate reacted with hydrogen sulfide in a summer reductive environment.


Limnology ◽  
2000 ◽  
Vol 1 (3) ◽  
pp. 151-157
Author(s):  
O. Mitamura ◽  
N. Ishida ◽  
Y. Seike ◽  
K. Kondo ◽  
M. Okumura

Limnology ◽  
2002 ◽  
Vol 3 (1) ◽  
pp. 21-27 ◽  
Author(s):  
Y. Senga ◽  
K. Mochida ◽  
N. Okamoto ◽  
R. Fukumori ◽  
Y. Seike

1992 ◽  
Vol 241 ◽  
pp. 23-57 ◽  
Author(s):  
G. G. Tomasson ◽  
W. K. Melville

We consider the general problem of geostrophic adjustment in a channel in the weakly nonlinear and dispersive (non-hydrostatic) limit. Governing equations of Boussinesq-type are derived, based on the assumption of weak nonlinear, dispersive and rotational effects, both for surface waves on a homogeneous fluid and internal waves in a two-layer system. Numerical solutions of the Boussinesq equations are presented, giving examples of the geostrophic adjustment in a channel for two different kinds of initial disturbances, both with non-zero perturbation potential vorticity. The timescales of rotational separation (that is, the separation of the Kelvin and Poincaré waves due to their dispersive properties) and that of nonlinear evolution are considered, with particular concern for the resonant interactions of nonlinear Kelvin waves and linear Poincaré waves described by Melville, Tomasson & Renouard (1989). A parameter measuring the ratio of the two timescales is used to predict when the free and forced Poincaré waves may be separated in the solution. It also distinguishes the cases in which the linear solutions are valid for the rotational separation from those requiring the full Boussinesq equations. Finally, solutions for the evolution of nonlinear internal waves in a sea strait are presented, and the effects of friction on the wavefront curvature of the nonlinear Kelvin waves are briefly considered.


2009 ◽  
Vol 30 (7) ◽  
pp. 1073-1076 ◽  
Author(s):  
Yasushi Seike ◽  
Makoto Murakami ◽  
Ryoko Fukumori ◽  
Yukiko Senga ◽  
Kazuhiro Ayukawa ◽  
...  

1970 ◽  
Vol 43 (1) ◽  
pp. 165-176 ◽  
Author(s):  
M. J. Manton ◽  
L. A. Mysak ◽  
R. E. Mcgorman

We discuss the diffraction of internal waves by a semi-infinite vertical barrier in a uniformly rotating, stably stratified fluid of constant depth and Brunt–Väisälä frequency. N, For the frequency passband f < σ < N, where f and σ are respectively the inertial and wave frequencies, the presence of rotation gives rise to internal Kelvin waves which propagate without attenuation along the barrier. For the passband N < σ < f, however, the barrier generates waves which propagate without attenuation away from the barrier and which have amplitudes that fall off exponentially in the direction along the barrier.


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