flowfanno
Fanno line flow relations
Syntax
Description
Default Input Mode
Examples
Input Arguments
Output Arguments
Limitations
This function assumes that variables vary only in one dimension. It also assumes that the main mechanism for the change of flow variables is the change of cross-sectional area of the flow stream tubes.
If the temperature experiences large fluctuations, the perfect gas assumption might be invalid. 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. Consider it a thermally perfect gas. For thermally perfect gas correction factors, see [2]. If the temperature is so high that molecules dissociate and ionize (static temperature 5000 K for air), you cannot assume a 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
| flowrayleigh