Section 3.9, example 3.12, page 126:
In equations 3.132--3.135, the prefactor
\(\tau\) should be \(\tau^{-1}\).
The last line of equation 3.135 is then
\begin{equation*}
L(t) ={}
\frac{\sin(\omega t) - \omega \tau \cos(\omega t)}
{1 + (\omega\tau)^2}.
\end{equation*}
Chapter 11, section 11.48, equation 11.397:
In the third equation, \( \Gamma^0_{22} \)
should be \( \Gamma^0_{33} \);
in equation 11.410, \(3p\) should be \( 3p/c^2 \);
in equation 11.411, \( p \) should be \( p/c^2 \);
in equations 11.411, 412, 414, 417, 419, & 422,
\( k \) should be \( c^2 k \);
Chapter 11, section 11.49, each \( p \) should be
\( p/c^2 \), and each \( k \) should be \( c^2 k \)
Section 3.9, example 3.12, page 126:
In equations 3.132--3.135, the prefactor
\(\tau\) should be \(\tau^{-1}\).
The last line of equation 3.135 is then
\begin{equation*}
L(t) ={}
\frac{\sin(\omega t) - \omega \tau \cos(\omega t)}
{1 + (\omega\tau)^2}.
\end{equation*}
Chapter 11, section 11.48: in equation 11.397
(third subequation) \( \Gamma^0_{22} \)
should be \( \Gamma^0_{33} \);
in equation 11.401, \( \Gamma^3_{23} = \cot \theta =
\Gamma^3_{32} \);
in equation 11.403, \( \dot a/a \) should be \( \dot
a/ca \) ;
in equations 11.404 and 11.405, \( \dot a/a \) should be \( \dot
a/ca \) and \(\ddot a/a \) should be \(\ddot a/c^2 a \);
in equation 11.407, \( \ddot a \) should be \( \ddot a/c^2 \)
and \( \dot a^2 \) should be \( \dot a^2 / c^2 \);
in equation 11.408, \( \rho \) should be \( c^2 \rho \);
in equation 11.410, \(3p\) should be \( 3p/c^2 \);
in equation 11.411, \( p \) should be \( p/c^2 \);
in equations 11.411, 412, 414, 417, 419, & 422,
\( k \) should be \( c^2 k \);