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Vorticity and Circulation Questions and Answers

71.

Match each theorem with its content.

List I

A. Stokes

B. Kelvin

C. Ertel

List II

P. circulation conserved in a barotropic fluid

Q. circulation equals the flux of vorticity

R. potential vorticity conserved for adiabatic motion

Select the correct match.

Answer: C

Stokes' theorem is the mathematical identity relating circulation to the flux of vorticity, Kelvin's theorem is the dynamical statement of conservation in a barotropic fluid, and Ertel's theorem generalises conservation to stratified adiabatic flow. Bjerknes' theorem completes the family by giving the rate of change of circulation in the baroclinic case.

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Answer: D

Helicity is the integral of the dot product of velocity and vorticity, so it is large when the flow moves along its own vortex lines. Storm relative helicity, computed over the lowest few kilometres, is the standard measure of the potential for rotating updraughts in severe storm forecasting. The other options describe the stretching term, the vorticity magnitude and the mean vorticity respectively. Working one numerical case through both cases side by side fixes the distinction better than any rule of thumb.

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Answer: A

Values of storm relative helicity above about 150 square metres per square second in the lowest three kilometres indicate an environment favourable for rotating updraughts. The quantity captures the streamwise vorticity that the updraught will tilt and stretch. Tropical cyclone intensity, frontogenesis and boundary layer depth are assessed by quite different diagnostics.

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Answer: B

Curvature of the hodograph means the shear vector turns with height, which produces vorticity aligned with the storm relative flow and hence large helicity. A straight hodograph gives crosswise vorticity and split storms rather than a dominant rotating updraught. A hodograph of zero length means no shear at all, and a closed hodograph implies no net shear across the layer.

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Answer: C

Divergence measures the fractional rate of increase of the area of a horizontal fluid element, so positive divergence means the element is spreading out. Rotation is vorticity, circulation is the loop integral of velocity, and shape change at constant area is deformation. Together these four describe every way a fluid element can be affected by the local velocity gradient.

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Answer: D

Surface pressure measures the weight of the overlying column, so if more mass leaves the top than enters at the bottom the column lightens and the pressure falls. This is the mass budget argument behind the deepening of surface lows beneath upper divergence. Static stability affects the vertical motion profile but not the sign of this relationship.

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Answer: A

In a typical developing system convergence occupies the lower troposphere and divergence the upper, with the change of sign at a level of non-divergence around 500 to 600 hectopascals. That level is where the barotropic vorticity equation is most nearly valid, which is why 500 hectopascals was chosen for the first numerical forecasts. The tropopause is well above the divergence maximum rather than at the transition. A single measurement chosen to respond to the one asymmetry beats several that respond to shared behaviour.

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Answer: B

The barotropic model assumes non-divergent flow, so it is most nearly valid at the level where the divergence actually vanishes, and 500 hectopascals is close to that level. It is also the level with half the atmospheric mass beneath it, which reinforces the choice. The strongest winds are near 250 hectopascals, and observational convenience did not drive the decision.

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Answer: C

Convergence in the frictional boundary layer forces air upward out of it, and the associated divergence within the layer reduces the vorticity, spinning the vortex down over about four days. The inward turning of the wind is the mechanism by which this happens rather than a source of vorticity. Planetary and relative vorticity are exchanged by the beta effect rather than by friction.

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Answer: D

The spin-down time is the depth of the troposphere divided by the Ekman pumping velocity, which works out at roughly 4 days for typical mid-latitude values. That is far shorter than molecular diffusion would give and matches the observed lifetime of decaying systems, which is the empirical check that makes the theory convincing. Boundary layer adjustment and turbulent mixing operate on much shorter timescales. The shared properties explain why these belong to one family, and the differences explain why more than one exists.

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