VISCOSITY {SUTHERLAND | WILKE | KEYE | CONSTANT vis}
|
This keyword allows you to specify the method of computing the
transport properties.
The equations shown below are for the laminar viscosity coefficient
mu.
For all the options except WILKE, in WIND the laminar thermal
conductivity coefficient k is equal to the viscosity coefficient,
when non-dimensionalized.
For WILKE, the form of the equations used for k is the
same as those used for mu, but with different constants from the
chemistry data (.chm) file.
| SUTHERLAND | Use Sutherland's law, designed for ideal gases with
T > 180 °R, as follows:
mu = 2.329 × 10-8 T3/2 / (T + 216) | ||
| WILKE | Use Wilke's law, designed for multi-species flow (real gases).
First, the viscosity coefficient is computed for each individual
species n using Sutherland's law, as follows:
mun / mu0 = (T / T0)3/2 (T0 + S) / (T + S) where T is the local static temperature, and mu0, T0, and S are constants read from the chemistry data (.chm) file for species n. For N total species, the individual viscosity coefficients are combined using mu = sumNi=1 [ Xi mui / sumNj=1 ( Xj phii,j ) ] where phii,j is a mixing coefficient computed as phii,j = [ 8 ( 1 + Mi / Mj ) ] -1/2 [ 1 + ( mui / muj ) 1/2 ( Mj / Mi ) 1/4 ] 2 X is the species mole fraction, and M is the species molecular weight. | ||
| KEYE | Use Sutherland's law for T >= 180 °R, Keyes' law
for T < 160 °R, and a linear combination of the two
for 160 °R < T < 180 °R.
Sutherland's law is written as above.
Keyes' law is given by:
mu = 2.32 × 10-8 T1/2 / (1 + (220/T) × 10-9/T) And the linear combination is given by mu = f muS + (1 - f) muK where muS and muK are the viscosity coefficients from Sutherland's and Keyes' laws, and f = (T - 160) / 20. | ||
| CONSTANT | Use a constant molecular viscosity of vis (slug/ft-sec) |
In all of the above equations, mu is in slug/ft-sec and T is in °R.