One of the characteristics of similarity of heat processes in fluids and gasses. The Prandtl number depends only on the thermodynamical state of the medium, and is defined by
$$ \mathop{\rm Pr} = \frac \nu {a} = \ \frac{\mu c _ {p} } \lambda , $$
where $ \nu = \mu / \rho $ is the kinematic coefficient of viscosity, $ \mu $ is the dynamic coefficient of viscosity, $ \rho $ is the density, $ \lambda $ is the coefficient of heat conductivity, $ a = \lambda / \rho c _ {p} $ is the coefficient of thermal diffusion, and $ c _ {p} $ is the specific heat capacity of the medium at constant pressure.
The Prandtl number is connected with other characteristics of similarity, the Péclet number and the Reynolds number, by the relation $ \mathop{\rm Pr} = \mathop{\rm Pe} / \mathop{\rm Re} $.
The Prandtl number is named after L. Prandtl.
Comments
The Prandtl number is sometimes also called the Darcy–Prandtl number.
References
| [a1] | N. Curle, H.J. Davies, "Modern fluid dynamics" , II , v. Nostrand-Reinhold (1971) |
| [a2] | S. Chandrasekhar, "Hydrodynamics and hydrodynamic stability" , Dover, reprint (1981) pp. Chapt. VII |
| [a3] | C.-S. Yih, "Stratified flows" , Acad. Press (1980) |
| [a4] | L.D. Landau, E.M. Lifshitz, "Fluid mechanics" , Pergamon (1959) pp. 203, 208 (Translated from Russian) |
Prandtl number. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Prandtl_number&oldid=48274