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Section 9: Vorticity and circulation | ||||||||||||
9.1 | Vorticity and its physical significance. Vortex lines and vortex tubes. The solenoidal nature of vortex lines. Examples. | |||||||||||
9.2 | Circulation G: its definition and relationship to vorticity. Vorticity as a "source" of circulation (Biot-Savart's law). | |||||||||||
9.3 | Kelvin's
theorem on circulation in barotropic flows in irrotational force fields:
For inviscid flows:
Examples: steady sink vortex, tornado or cyclone, bathtub vortex. |
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9.4 |
Three vortex theorems for inviscid, barotropic flow in an irrotational force field (corollaries of Kelvin's theorem): (a) Vortex lines move with the fluid. Examples: behavior of vortex rings; instability of shear layer or vortex sheet; secondary flow induced in bends. (b) Once irrotational( ), a fluid particle will remain so forever. Consequence: Potential flows. Example: solution of steady sink vortex based on constraint that . (c) For vortex "tube",
Example: accelerating inviscid flow with transverse velocity gradient. |
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9.5 | Vorticity transport equation in differential form. The effect on vorticity of vortex line stretching and turning; the role of kinematic viscosity as the diffusivity of vorticity. | |||||||||||
Reading | ||||||||||||
Fay, pp 271-276
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Problem Set Section 9 (from Shapiro and Sonin) | ||||||||||||
Problem 10.3 | ||||||||||||
Problem 10.4 | ||||||||||||
Problem 10.5 | ||||||||||||
Problem 10.8 | ||||||||||||
Problem 10.11 | ||||||||||||