Crocco's Theorem
Crocco's theorem is a fluid dynamics theorem relating the velocity, vorticity, and stagnation pressure (or entropy) of a potential flow. The theorem was first written by Italian scientist Luigi Crocco, a son of Gaetano Crocco.
Because stagnation pressure loss and entropy generation can be viewed as essentially the same thing, there are two popular forms for writing Crocco's theorem:
- Stagnation pressure\[ V \times \omega = \frac{1}{\rho} \nabla p_0 \] [1]
- Entropy\[ T \frac{ds}{dn} = \frac{dh_0}{dn} + ||V||\omega \] [2]
- quantity of movement\[ \frac{\partial \mathbf{v}}{\partial t} + \nabla \left(\frac{\mathbf{v}^2}{2} + h \right) = \mathbf{v} \times \mathbf{\omega} + T \nabla s + \mathbf{f},\]
In the above equations, \( V \) is velocity, \( \omega \) is vorticity, \( \rho \) is density, \( p_0 \) is stagnation pressure, \( T \) is temperature, \( s \) is entropy, and \( n \) is the direction normal to the streamlines.
References
- ↑ Shapiro, Ascher H. "National Committee for Fluid Mechanics Films Film Notes for 'Vorticity,'" 1969. Encyclopaedia Britannica Educational Corporation, Chicago, Illinois. (retrieved from http://web.mit.edu/hml/ncfmf/09VOR.pdf (5/29/11)
- ↑ Liepmann, H. W. and Roshko, A. "Elements of Gasdynamics" 2001. Dover Publications, Mineola, NY.