The Mathematical Theory of RelativityEddington, Arthur Stanley, Sir
Science
The Mathematical Theory of Relativity
Eddington, Arthur Stanley, Sir
Relativity (Physics)
The determinants with which we are most concerned are the fundamental
determinant~$g$ and the Jacobian of a transformation
\index{Jacobian}%
\[
J = \frac{\dd(x_{1}', x_{2}', x_{3}', x_{4}')}{\dd(x_{1}, x_{2}, x_{3}, x_{4})}.
\]
By~\Eq{(48.2)}
\begin{align*}
4!\, g &= \epsilon_{\alpha\beta\gamma\delta}\, \epsilon_{\epsilon\zeta\eta\theta}\,
g_{\alpha\epsilon}\, g_{\beta\zeta}\, g_{\gamma\eta}\, g_{\delta\theta},
\Tag{(48.32)} \\
4!\, J &= \epsilon_{\alpha\beta\gamma\delta}\, \epsilon_{\epsilon\zeta\eta\theta}\,
\frac{\dd x_{\epsilon}'}{\dd x_{\alpha}}\,
\frac{\dd x_{\zeta}'}{\dd x_{\beta}}\,
\frac{\dd x_{\eta}'}{\dd x_{\gamma}}\,
\frac{\dd x_{\theta}'}{\dd x_{\delta}}.
\Tag{(48.33)}
\end{align*}
To illustrate the manipulations we shall prove that\footnote
{A shorter proof is given at the end of this section.}
\[
g = J^{2} g'.
\]
By \Eq{(48.32)} and~\Eq{(48.33)}
\begin{multline*}
(4!)^{3} J^{2} g'
= \epsilon_{\alpha\beta\gamma\delta}\, \epsilon_{\epsilon\zeta\eta\theta}\,
g_{\alpha\epsilon}'\, g_{\beta\zeta}'\, g_{\gamma\eta}'\, g_{\delta\theta}'
· \epsilon_{\iota\kappa\lambda\mu}\, \epsilon_{\nu\xi\omicron\varpi}\,
\frac{\dd x_{\nu}'}{\dd x_{\iota}}\,
\frac{\dd x_{\xi}'}{\dd x_{\kappa}}\,
\frac{\dd x_{\omicron}'}{\dd x_{\lambda}}\,
\frac{\dd x_{\varpi}'}{\dd x_{\mu}} \\
· \epsilon_{\rho\sigma\tau\upsilon}\, \epsilon_{\phi\chi\psi\omega}\,
\frac{\dd x_{\phi}'}{\dd x_{\rho}}\,
\frac{\dd x_{\chi}'}{\dd x_{\sigma}}\,
\frac{\dd x_{\psi}'}{\dd x_{\tau}}\,
\frac{\dd x_{\omega}'}{\dd x_{\upsilon}}.
\Tag{(48.41)}
\end{multline*}
There are about $280$~billion terms on the right, and we proceed to rearrange
those which do not vanish.
For non-vanishing terms the letters $\nu$, $\xi$, $\omicron$, $\varpi$ denote the same suffixes as
$\alpha$, $\beta$, $\gamma$, $\delta$, but (usually) in a different order. Permute the four factors in which
they occur so that they come into the same order; the suffixes of the denominators
will then come into a new order, say, $i$, $k$, $l$,~$m$. Thus
\[
\frac{\dd x_{\nu}'}{\dd x_{\iota}}\,
\frac{\dd x_{\xi}'}{\dd x_{\kappa}}\,
\frac{\dd x_{\omicron}'}{\dd x_{\lambda}}\,
\frac{\dd x_{\varpi}'}{\dd x_{\mu}}
= \frac{\dd x_{\alpha}'}{\dd x_{i}}\,
\frac{\dd x_{\beta}'}{\dd x_{k}}\,
\frac{\dd x_{\gamma}'}{\dd x_{l}}\,
\frac{\dd x_{\delta}'}{\dd x_{m}}.
\Tag{(48.42)}
\]
Public-domain text, read in full here on John Shaqi.
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