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Matteo Cantiello edited MLT.tex
over 9 years ago
Commit id: 3d34941180c580ef816de196d7e2493ebacf46c8
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index b4423dc..2385eb9 100644
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\end{equation}
where the factor 1/2 comes from the fact that at each level approximately one-half of the matter is rising and one-half is descending. Here $\rho$, $\bar{v}$ and $\cp$ are averages along the distance $\lambda$ of density, velocity and specific heat at constant pressure of upward and downward moving fluid elements.
Using equation~\ref{eq:deltat} we can write
\begin{equation} \begin{equation}\label{eq:convectiveflux}
F_{c} = \frac{1}{2} \rho \bar{v}\, \cp \, T \frac{\lambda}{\hp} ( \nabla - \nabla') ,
\end{equation}