210 |
$v=\frac{Dy}{Dt}=r \frac{D \phi}{Dt}$ |
$v=\frac{Dy}{Dt}=r \frac{D \phi}{Dt}$ |
211 |
are the zonal and meridional components of the |
are the zonal and meridional components of the |
212 |
flow vector, $\vec{u}$, on the sphere. As described in |
flow vector, $\vec{u}$, on the sphere. As described in |
213 |
MITgcm Numerical Solution Procedure \cite{MITgcm_Numerical_Scheme}, the time |
MITgcm Numerical Solution Procedure \ref{chap:discretization}, the time |
214 |
evolution of potential temperature, $\theta$, equation is solved prognostically. |
evolution of potential temperature, $\theta$, equation is solved prognostically. |
215 |
The total pressure, $p$, is diagnosed by summing pressure due to surface |
The total pressure, $p$, is diagnosed by summing pressure due to surface |
216 |
elevation $\eta$ and the hydrostatic pressure. |
elevation $\eta$ and the hydrostatic pressure. |