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On the inertial motion of a homogeneous ocean
Institution:1. AC2T research GmbH, Viktor-Kaplan-Straße 2C, 2700 Wiener Neustadt, Austria;2. voestalpine Stahl GmbH, voestalpine-Straße 3, 4020 Linz, Austria;1. Tecnologico de Monterrey, School of Engineering and Sciences, Monterrey, 64849, Mexico;2. Department of Environmental Microbiology, School for Environmental Sciences, Babasaheb Bhimrao Ambedkar (A Central) University, Lucknow 226 025, Uttar Pradesh, India;3. Plant Molecular Biology Laboratory, Department of Botany, Dayanand Anglo-Vedic (PG) College, Chhatrapati Shahu Ji Maharaj University, Kanpur-208 001, India;4. Brazil University, Street Carolina Fonseca, Number 584, 08230-030 São Paulo, São Paulo, Brazil;5. School of Life Science and Food Engineering, Huaiyin Institute of Technology, Huaian 223003, China;1. Department of Natural Resources and Environment, Islamic Azad University, Science and Research Branch, Tehran, Iran;2. Department of Marine Science and Technology, Islamic Azad University, North Tehran Branch, Tehran, Iran;3. Institute of Geophysics, University of Tehran, Tehran, Iran
Abstract:An investigation of properties of the solutions of the steady state inviscid barotropic vorticity equation in a rectangular basin was performed for various functional relationships between potential vorticity and the streamfunction. All computed solutions which have slow interior flow and satisfy Arnol'd-Blumen condition are qualitatively similar to Fofonoff's inertial gyre. A new class of solutions with a small vortex near the boundary current is described. Such solutions are not stable under finite amplitude perturbations and instability is manifested in the drift of the vortex. It is shown that the vortex is robust and decays only after collision with the boundary or under the influence of very large perturbations. We also show that the inertial boundary current may be much wider than in Fofonoff's model due to the appearance of a countercurrent on its seaward side.
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