$\newcommand{\bbx}[1]{\,\bbox[8px,border:1px groove navy]{\displaystyle{#1}}\,}
\newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack}
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\newcommand{\ds}[1]{\displaystyle{#1}}
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\newcommand{\mrm}[1]{\mathrm{#1}}
\newcommand{\pars}[1]{\left(\,{#1}\,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,}
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\begin{align}
\int{\dd \theta \over a + \cos\pars{\theta}} & =
\int{\dd \theta \over a + \bracks{2\cos^{2}\pars{\theta/2} - 1}} =
\int{\sec^{2}\pars{\theta/2} \over \pars{a - 1}\sec^{2}\pars{\theta/2} + 2}
\,\dd \theta
\\[5mm] & =
\int{\sec^{2}\pars{\theta/2} \over \pars{a - 1}\tan^{2}\pars{\theta/2} + a + 1}
\,\dd \theta
\\[5mm] & =
{1 \over a + 1}\int{\sec^{2}\pars{\theta/2} \over
\bracks{\pars{a - 1}/\pars{a + 1}}\tan^{2}\pars{\theta/2} + 1}
\,\dd \theta
\end{align}
With $\ds{t \equiv \root{a - 1 \over a + 1}\tan\pars{\theta \over 2}\quad}$ and
$\quad\left\{\begin{array}{rcl}
\ds{\theta} & \ds{=} &
\ds{2\arctan\pars{\root{a + 1 \over a - 1}\,t}}
\\[2mm]
\ds{\quad\sec^{2}\pars{\theta \over 2}\,\dd\theta} & \ds{=} &
\ds{2\root{a + 1 \over a - 1}\dd t}
\end{array}\right.
$:
\begin{align}
\int{\dd \theta \over a + \cos\pars{\theta}} & =
{1 \over a + 1}\bracks{2\root{a + 1 \over a - 1}}\int{\dd t \over t^{2} + 1}
=
{2 \over \root{a^{2} - 1}}\,\arctan\pars{t}
\\[5mm] & =
\bbx{\ds{{2 \over \root{a^{2} - 1}}\arctan\pars{\root{a - 1 \over a + 1}
\tan\pars{\theta \over 2}} + \pars{~\mbox{a constant}~}}}
\end{align}