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Benedict Irwin edited Electromagnetism.tex
about 10 years ago
Commit id: 68d6406c19723ffa809d963566de7558300daa15
deletions | additions
diff --git a/Electromagnetism.tex b/Electromagnetism.tex
index 7eafd8e..8ffa24a 100644
--- a/Electromagnetism.tex
+++ b/Electromagnetism.tex
...
\end{bmatrix}
\end{equation}
This would require perhaps a normalisation of $\frac{1}{\sqrt{2}}$ on each matrix.
For the potential 4 vector \begin{equation}
A^{\mu}=(\varphi/c,A_x,A_y,A_z)
\end{equation}
Then \begin{equation}
A_{\mu}=eta_{\mu \nu}A^{\nu}
\end{equation}
Which gives \begin{equation}
A_\mu = \begin{bmatrix}
\frac{\varphi}{c} +A_xi+A_yj+A_zk \\
\frac{\varphi i}{c} -A_x +A_yk -A_zj \\
\frac{\varphi j}{c} -A_xk -A_y +A_zi \\
\frac{\varphi k}{c} +A_xj +A_yi-A_z
\end{bmatrix}
=
\begin{bmatrix}
\frac{\varphi}{c} \\
-A_x \\
-A_y \\
-A_z
\end{bmatrix}
+
\begin{bmatrix}
A_x \\
\frac{\varphi}{c} \\
A_z \\
-A_y
\end{bmatrix}
i
+
\begin{bmatrix}
A_y \\
-A_z \\
\frac{\varphi}{c} \\
A_x
\end{bmatrix}
j
+
\begin{bmatrix}
A_z \\
A_y \\
-A_x \\
\frac{\varphi}{c}
\end{bmatrix}
k
\end{equation}