After some algebra we rewrite the equation as
\begin{equation*}
\sin 2\theta=\frac{2}{3}
\end{equation*}
or
\begin{equation}
\sin u=\frac{2}{3}\text{,}\tag{2.127}
\end{equation}
where
\(u=2\theta\text{.}\) Since
\(u_0=\arcsin(2/3)\) is a solution to
(2.127), according to
Procedure 2.19.5 the general solution is
\begin{equation*}
u=\arcsin(2/3)+2\pi n \text{ or } u=(\pi-\arcsin(2/3))+2\pi n\text{.}
\end{equation*}
Since \(u=2\theta\text{,}\) we conclude that the general solution to the original equation is
\begin{equation*}
\theta=\frac{1}{2}\arcsin(2/3)+\pi n \text{ or } \theta=\frac{1}{2}(\pi-\arcsin(2/3))+\pi n\text{.}
\end{equation*}
Which of these infinitely-many solutions lies in the prescribed interval \([0,2\pi]\text{?}\) Since \(\arcsin(2/3)\in [0,\pi/2]\text{,}\) we have \(\frac{1}{2}\arcsin(2/3)\in [0,\pi/4]\) and \(\frac{1}{2}(\pi-\arcsin(2/3)\in [\pi/4, \pi/2]\text{.}\) It follows that the solutions lying in \([0,2\pi]\) are
\begin{equation*}
\theta=\frac{1}{2}\arcsin(2/3), \frac{1}{2}\arcsin(2/3)+\pi, \frac{1}{2}(\pi-\arcsin(2/3)), \frac{1}{2}(\pi-\arcsin(2/3))+\pi\text{.}
\end{equation*}