deletions | additions       diff --git a/subsubsection_Kinetic_Fractionation_Factor_One__.tex b/subsubsection_Kinetic_Fractionation_Factor_One__.tex  index 0122d30..1a86a29 100644  --- a/subsubsection_Kinetic_Fractionation_Factor_One__.tex  +++ b/subsubsection_Kinetic_Fractionation_Factor_One__.tex 
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z_o = 0.1h, $z_q = \frac{z_0}{exp^{(kB^{-1})}}$\\  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:  \[\phi_m = \frac{kz}{u_*}\big[\frac{\partial \frac{kz}{u_*}\bigg[\frac{\partial  \bar U}{\partial z}^2 + \frac{\partial \bar V}{\partial z}^2\bigg]^{1/2}\]