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Signed-off-by: jtneedels <jneedels@stanford.edu>
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_docs_v7/Thermochemical-Nonequilibrium.md

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@@ -221,6 +221,19 @@ The Wilkes-Blottner-Eucken model is generally efective up to temperatures of 10,
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## Gupta-Yos ##
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Aother model develped by Gupta focuses on the transport properties of weakly ionized flows, and is generally more accurate than the Wilkes-Blottner-Eucken model at temperatures above 10,000 K.
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The mixutre viscoisty is computed as
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$$
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\mu = \sum_{s \neq e} \frac{m_s \gamma_s}{\sum_{r \neq e} \gamma_r \Delta_{s,r}^{(2)}(T_{tr}) + \gamma_r \Delta_{e,r}^{(2)}(T_{ve})} + \frac{m_e \gamma_e}{\sum_r \gamma_r \Delta_{e,r}^{(2)}(T_{ve}) }
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$$
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where
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$$
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\gamma_s = \frac{\rho_s}{\rho M_s}
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$$
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