Overflows in the ocean occur when dense water flows down a continental slope into less dense ambient water. It is important to study idealized and small-scale models, which allow for confidence and control of parameters. The work presented here is a direct qualitative and quantitative comparison between physical laboratory experiments and lab-scale numerical simulations. Physical parameters are varied, including the Coriolis parameter, the inflow density, and the inflow volumetric flow rate. Laboratory experiments are conducted using a rotating square tank and high-resolution camera mounted on the table in the rotating reference frame. Video results are digitized in order to compare directly to numerical simulations. The MIT General Circulation Model (MITgcm), a three-dimensional ocean model, is used for the direct numerical simulations corresponding to the specific laboratory experiments. It was found that the MITgcm was not a good match to laboratory experiments when physical parameters fell within the high eddy activity regime. However, a more extensive resolution study is needed to understand this fully. The MITgcm simulations did provide a good qualitative and quantitative match to laboratory experiments run in a low eddy activity regime. In all cases, the MITgcm simulations had more eddy activity than the laboratory experiments.
Funding
An Integrated Program for Recruitment, Retention and Graduation of Academically Talented Low Income Engineering Students | Funder: National Science Foundation | Grant ID: DUE-1644182
UIC Breakthrough Tech Chicago | Funder: Cornell University | Grant ID: 91229-11352
WiTNY National Expansion | Funder: Cornell University | Grant ID: 90620-11335
History
Citation
Reckinger, S. M., Gibson, T. H., Hohman, F. M., Morrison, T. J., Reckinger, S. J.Carvalho, M. (2019). The effect of numerical parameters on eddies in oceanic overflows: A laboratory and numerical study. International Journal of Computational Methods and Experimental Measurements, 7(2), 142-153. https://doi.org/10.2495/CMEM-V7-N2-142-153