Observations and Parametrization of the Turbulent Energy Dissipation Beneath Non-Breaking Waves

Here, for non-breaking short surface waves, we have experimentally determined the value of the turbulent eddy viscosity νT or its ratio ν∗T≡ νT/ν, where ν is the water kinematic viscosity. The non-breaking wave-generated turbulent eddy viscosity νT was found to depend on the ratio of the wave period...

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Bibliographic Details
Main Authors: Barzegar, M. (Author), Bogucki, D.J (Author), Haus, B.K (Author)
Format: Article
Language:English
Published: MDPI 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 01795nam a2200193Ia 4500
001 10.3390-fluids7070216
008 220718s2022 CNT 000 0 und d
020 |a 23115521 (ISSN) 
245 1 0 |a Observations and Parametrization of the Turbulent Energy Dissipation Beneath Non-Breaking Waves 
260 0 |b MDPI  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.3390/fluids7070216 
520 3 |a Here, for non-breaking short surface waves, we have experimentally determined the value of the turbulent eddy viscosity νT or its ratio ν∗T≡ νT/ν, where ν is the water kinematic viscosity. The non-breaking wave-generated turbulent eddy viscosity νT was found to depend on the ratio of the wave period, T, to the microscale Kolmogorov time scale, τη. Our observations were consistent with ν∗T= 1.46·(T/τη)−2.6 when (T/τη) < 0.9. That implied that the ν∗T∝ɛ−1.3, where ɛ is the background turbulent energy dissipation rate. The near-surface turbulent flow associated with non-breaking waves was characterized by a short inertial subrange. The background turbulence appears to modulate the amount of energy the non-breaking waves dissipate locally and, consequently, the wave’s decay rate. Our results imply that the background turbulent flow acts as a lubricant, permitting waves to propagate further when traveling over a more energetic turbulent background flow. Our results have implications for the modeling of oceanic wave propagation or the air–sea exchange processes. © 2022 by the authors. Licensee MDPI, Basel, Switzerland. 
650 0 4 |a near-surface turbulence 
650 0 4 |a non-breaking waves 
650 0 4 |a surface gravity waves 
700 1 |a Barzegar, M.  |e author 
700 1 |a Bogucki, D.J.  |e author 
700 1 |a Haus, B.K.  |e author 
773 |t Fluids