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Fourier filtering and coefficient tapering at the North Pole in OGCMs
Institution:1. School of Earth Sciences, University of Melbourne, Melbourne, Parkville, 3010, Vic., Australia;2. Departments of EGS and Oceanography, University of Cape Town, Cape Town, South Africa;1. Dr. B. C. Roy College of Pharmacy and Allied Health Sciences, Division of Pharmacognosy and Phytochemistry, Bidhan Nagar, Durgapur 713206, India;2. Department of Pharmaceutical Technology, Pharmacognosy and Phytotherapy Research Laboratory, Jadavpur University, Kolkata 700032, India;1. School of Traditional Chinese Materia Medica, Shenyang Pharmaceutical University, Shenyang 110016, China;2. Jiangsu Key Laboratory of Bioactive Natural Product Research and State Key Laboratory of Natural Medicines, Department of Natural Medicinal Chemistry, China Pharmaceutical University, Nanjing 210009, China;1. Institute of Bioengineering and Nanotechnology, 31 Biopolis Way, The Nanos, #04-01, Singapore 138669, Singapore;2. Department of Biology and Chemistry, City University of Hong Kong, 83 Tat Chee Ave, Kowloon, Hong Kong SAR;3. Department of Neurosciences, Lerner Research Institute, Cleveland Clinic, 9500 Euclid Avenue, Cleveland, OH 44120, USA;4. Research and Development Center for Novel Pharmaceuticals, Guangxi Botanical Garden of Medicinal Plants, 189 Changgang Road, Nanning, Guangxi, China
Abstract:This article considers how some of the measures used to overcome numerical problems near the North Pole affect the ocean solution and computational time step limits. The distortion of the flow and tracer contours produced by a polar island is obviated by implementing a prognostic calculation for a composite polar grid cell, as has been done at NCAR. The severe limitation on time steps caused by small zonal grid spacing near the pole is usually overcome by Fourier filtering, sometimes supplemented by the downward tapering of mixing coefficients as the pole is approached; however, filtering can be expensive, and both measures adversely affect the solution. Fourier filtering produces noise, which manifests itself in such effects as spurious static instabilities and vertical motions; this noise can be due to the separate and different filtering of internal and external momentum modes and tracers, differences in the truncation at different latitudes, and differences in the lengths of filtering rows, horizontally and vertically. Tapering has the effect of concentrating tracer gradients and velocities near the pole, resulting in some deformation of fields. In equilibrium ocean models, these effects are static and localised in the polar region, but with time-varying forcings or coupling to atmosphere and sea ice it is possible that they may seriously affect the global solution. The marginal stability curve in momentum and tracer time-step space should have asymptotes defined by diffusive, viscous, and internal gravity wave stability criteria; at large tracer time steps, tracer advection stability may become limiting. Tests with various time-step combinations and a flat-bottomed Arctic Ocean have confirmed the applicability of these limits and the predicted effects of filtering and tapering on them. They have also shown that the need for tapering is obviated by substituting a truncation which maintains a constant time step limit rather than a constant minimum wave number over the filtering range.
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