deletions | additions       diff --git a/subsubsection_Kinetic_Fractionation_Factor_One__.tex b/subsubsection_Kinetic_Fractionation_Factor_One__.tex  index 4ea686d..f76b2f0 100644  --- a/subsubsection_Kinetic_Fractionation_Factor_One__.tex  +++ b/subsubsection_Kinetic_Fractionation_Factor_One__.tex 
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B^{-1} = 2/k (inverse of the Dalton number of interfacial sublayer - paramterisation of mass transfer coefficient). Canopy resistance inferred from P-M sensitive to B.\\  $\phi_m$ and $\phi_h$ are the integral of the MOST functions for momentum and heat - this is where the profile will be useful as we need gradient to derive these \cite{1988}:  \[\phi_m = \frac{kz}{u_*}\Bigg[\bigg(\frac{\partial \bar U}{\partial z}\bigg)^2 + \bigg(\frac{\partial \bar V}{\partial z}\bigg)^2\Bigg]^{1/2}\]  \\  \\  \[\phi_H = \frac{kz}{\theta_*^SL}\frac{\partial \bar \theta}{\partial z}\]