mirror of
https://github.com/wassname/simpeg.git
synced 2026-07-23 13:10:51 +08:00
Updates to the notes.
This commit is contained in:
+7
-6
@@ -203,11 +203,12 @@ Multiplying $\mathbf{J}$ onto a vector can be broken into three steps
|
||||
\begin{align}
|
||||
\vec{p}^{(n)} = \left[
|
||||
\begin{array}{c}
|
||||
0 \\
|
||||
\vec{p}_b^{(n)} \\
|
||||
\vec{p}_e^{(n)}
|
||||
\end{array}
|
||||
\right] \\
|
||||
\vec{p}_e^{(n)} = - \diag{\e^{(n)}} \Ace \diag{V} m
|
||||
\vec{p}_b^{(n)} = 0 \\
|
||||
\vec{p}_e^{(n)} = - \diag{\e^{(n)}} \Ace \diag{V} m
|
||||
\end{align}
|
||||
\end{subequations}
|
||||
|
||||
@@ -215,14 +216,14 @@ Multiplying $\mathbf{J}$ onto a vector can be broken into three steps
|
||||
|
||||
\begin{subequations}
|
||||
\begin{align}
|
||||
\dcurl \vec{y}_{e}^{(1)} + \frac{1}{\delta t} \vec{y}_{b}^{(1)} = 0 \\
|
||||
\dcurl \vec{y}_{e}^{(1)} + \frac{1}{\delta t} \vec{y}_{b}^{(1)} = \vec{p}_b^{(1)} \\
|
||||
\dcurl^\top \MfMui \vec{y}_b^{(1)} - \MeSig \vec{y}_e^{(1)} = \vec{p}_e^{(1)}
|
||||
\end{align}
|
||||
\end{subequations}
|
||||
|
||||
\begin{subequations}
|
||||
\begin{align}
|
||||
\left( \MfMui \dcurl \MeSig^{-1} \dcurl^\top \MfMui + \frac{1}{\delta t} \MfMui \right) \vec{y}_{b}^{(1)} = \MfMui \dcurl \MeSig^{-1} \vec{p}_e^{(1)} \\
|
||||
\left( \MfMui \dcurl \MeSig^{-1} \dcurl^\top \MfMui + \frac{1}{\delta t} \MfMui \right) \vec{y}_{b}^{(1)} = \MfMui \dcurl \MeSig^{-1} \vec{p}_e^{(1)} + \MfMui \vec{p}_b^{(1)} \\
|
||||
\vec{y}_e^{(1)} = \MeSig^{-1} \dcurl^\top \MfMui \vec{y}_b^{(1)} - \MeSig^{-1} \vec{p}_e^{(1)}
|
||||
\end{align}
|
||||
\end{subequations}
|
||||
@@ -233,7 +234,7 @@ Multiplying $\mathbf{J}$ onto a vector can be broken into three steps
|
||||
\begin{align}
|
||||
\dcurl \vec{y}_{e}^{(t+1)} + \frac{1}{\delta t} \vec{y}_{b}^{(t+1)}
|
||||
{\color{red}- \frac{1}{\delta t} \vec{y}_{b}^{(t)} }
|
||||
= 0 \\
|
||||
= \vec{p}_b^{(t+1)} \\
|
||||
\dcurl^\top \MfMui \vec{y}_b^{(t+1)} - \MeSig \vec{y}_e^{(t+1)} = \vec{p}_e^{(t+1)}
|
||||
\end{align}
|
||||
\end{subequations}
|
||||
@@ -242,7 +243,7 @@ Multiplying $\mathbf{J}$ onto a vector can be broken into three steps
|
||||
\begin{align}
|
||||
\left( \MfMui \dcurl \MeSig^{-1} \dcurl^\top \MfMui + \frac{1}{\delta t} \MfMui \right) \vec{y}_{b}^{(t+1)} =
|
||||
{\color{red} \frac{1}{\delta t} \MfMui \vec{y}_b^{(t)} }
|
||||
+ \MfMui \dcurl \MeSig^{-1} \vec{p}_e^{(t+1)} \\
|
||||
+ \MfMui \dcurl \MeSig^{-1} \vec{p}_e^{(t+1)} + \MfMui \vec{p}_b^{(t+1)} \\
|
||||
\vec{y}_e^{(t+1)} = \MeSig^{-1} \dcurl^\top \MfMui \vec{y}_b^{(t+1)} - \MeSig^{-1} \vec{p}_e^{(t+1)}
|
||||
\end{align}
|
||||
\end{subequations}
|
||||
|
||||
Reference in New Issue
Block a user