flowrayleigh
Rayleigh line flow relations
Syntax
Description
Examples
Input Arguments
Output Arguments
Limitations
This function assumes that:
The medium is a calorically perfect gas in a constant area duct.
The flow is steady, frictionless, and one dimensional.
The main mechanism for the change of flow variables is heat transfer.
This function assumes that the environment is a perfect gas. In the following instances, it cannot assume a perfect gas environment.
If there is a large change in either temperature or pressure without a proportionally large change in the other.
If the stagnation temperature is above 1500 K, do not assume constant specific heats. In this case, the medium ceases to be a calorically perfect gas; you must then consider it a thermally perfect gas. For thermally perfect gas correction factors, see [2]. The local static temperature might be so high that molecules dissociate and ionize (static temperature 5000 K for air). In this case, you cannot assume a calorically or thermally perfect gas.
More About
References
[1] James, John E. A. Gas Dynamics. 2nd ed. Boston: Allyn and Bacon 1984.
[2] Ames Research Staff. NACA Technical Report 1135. Moffett Field, CA: National Advisory Committee on Aeronautics, 1953. 667–671.
Version History
Introduced in R2010a
See Also
flowisentropic
| flownormalshock
| flowprandtlmeyer
| flowfanno