- V. Bjerknes's circulation theorem: 1) With reference to an absolute coordinate system, the rate of change of the absolute circulation dCa/dt of a closed individual fluid curve, that is, one that will consist always of the same fluid particles, is equal to the number of pressure–volume solenoids Nα,-p embraced by the curvewhere the circulation has the same sense as the solenoids, the sense of the rotation from volume ascendent to pressure gradient.
2) With reference to a relative coordinate system (specifically, the rotating earth), the rate of change of circulation relative to the earth dC/dt of an arbitrary closed individual fluid curve is determined by two effects: a) the solenoid effect that tends to change the circulation in the sense of the solenoids by an amount per unit time equal to the number of solenoids embraced by the curve; and b) the inertial effect that tends to decrease the circulation by an amount per unit time proportional to the rate at which the projected area of the curve in the equatorial plane expands:where Ω is the angular speed of the earth's rotation and A is the equatorial projection of the curve. This is the most useful form of Bjerknes's circulation theorem. It permits the qualitative examination of many types of frictionless atmospheric motion that are too complicated for complete analytic treatment, for example, the sea breeze.
- Höiland's circulation theorem: An arbitrary closed tubular fluid filament with constant cross section has a total mass acceleration along itself equal to the resultant of the force of gravitation along the filament:where ρ is the fluid density,is the absolute vector acceleration, and dφa is the variation of the gravitational potential from the initial to the terminal point of the vector element dr. This theorem is particularly useful in the study of the stability of fluid flow.
Gill, A. E. 1982. Atmosphere–Ocean Dynamics. Academic Press, . 226–231, 237–241.
Holton, J. R. 1992. An Introduction to Dynamic Meteorology. 3d edition, Academic Press, . 87–92.
Copyright 2022 American Meteorological Society (AMS). For permission to reuse any portion of this work, please contact firstname.lastname@example.org. Any use of material in this work that is determined to be “fair use” under Section 107 of the U.S. Copyright Act (17 U.S. Code § 107) or that satisfies the conditions specified in Section 108 of the U.S.Copyright Act (17 USC § 108) does not require AMS’s permission. Republication, systematic reproduction, posting in electronic form, such as on a website or in a searchable database, or other uses of this material, except as exempted by the above statement, require written permission or a license from AMS. Additional details are provided in the AMS Copyright Policy statement.