(a) At latitude , a steady geostrophic flow of water, with molecular viscosity ,…

PHYSICS · Subjective · Fermi University Physics · Fluids & Continuum Physics · Kinematics, conservation laws and ideal flow · Convection, rotation and geophysical flows

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

Problem

(a) At latitude 35∘N35^\circ\mathrm{N}, a steady geostrophic flow of water, with molecular viscosity ν=1.0×10−6 m2 s−1\nu = 1.0\times10^{-6}\,\mathrm{m^2\,s^{-1}}, produces a bottom Ekman layer of thickness δE=2ν/f\delta_E = \sqrt{2\nu/f}. Set beside it, as a formal comparison, a plate oscillating in the same water in a tank that does not rotate, at an angular frequency ω\omega chosen equal to that ff; it produces a Stokes layer of thickness δs=2ν/ω\delta_s = \sqrt{2\nu/\omega}. Compute the two thicknesses, and explain from the balance of terms in each layer's momentum equation why they come out equal. (b) In the rotating fluid at 35∘N35^\circ\mathrm{N}, a column of water of height h1=2.0 mh_1 = 2.0\,\mathrm{m} with zero relative vorticity flows over a submerged ridge that reduces its height to h2=1.4 mh_2 = 1.4\,\mathrm{m}. Using conservation of the shallow-water potential vorticity (ωz+f)/h(\omega_z+f)/h, find the relative vorticity ωz\omega_z of the column after it crosses the ridge, state whether the resulting spin is cyclonic or anticyclonic, and relate the result to the stretching of frozen-in vortex lines.

Browse the problem library