An ocean current of speed flows towards a broad seamount of horizontal width rising…

PHYSICS · Multi-part · Fermi University Physics · Fluids & Continuum Physics · Convection, rotation and geophysical flows · Convection, rotation and geophysical flows

Fluid Dynamics, Ch Rotating fluids: geostrophy, Taylor columns and Ekman layers

Problem

An ocean current of speed U=0.05 m s−1U = 0.05\,\mathrm{m\,s^{-1}} flows towards a broad seamount of horizontal width L=20 kmL = 20\,\mathrm{km} rising from a sea floor at depth H=4000 mH = 4000\,\mathrm{m}, at latitude 30∘N30^\circ\mathrm{N}. Take the ocean's turbulent eddy viscosity as ν=1.0×10−2 m2 s−1\nu = 1.0\times10^{-2}\,\mathrm{m^2\,s^{-1}} and Ω=7.292×10−5 s−1\Omega = 7.292\times10^{-5}\,\mathrm{s^{-1}}. The sea surface rises and falls so little that it may be treated as a rigid lid. ((a)) Compute the Rossby number Ro=U/(fL)Ro = U/(fL) and the Ekman number Ek=ν/(fH2)Ek = \nu/(fH^2) for this flow. ((b)) Predict, with a reason based on these two numbers, what the current does as it approaches the seamount: does the water near the sea surface flow straight over the top, or is it steered around it? Describe the pattern you expect at every depth.

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