$\newcommand{\bbx}[1]{\,\bbox[8px,border:1px groove navy]{\displaystyle{#1}}\,}
\newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack}
\newcommand{\dd}{\mathrm{d}}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,}
\newcommand{\ic}{\mathrm{i}}
\newcommand{\mc}[1]{\mathcal{#1}}
\newcommand{\mrm}[1]{\mathrm{#1}}
\newcommand{\pars}[1]{\left(\,{#1}\,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,}
\newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}}
\newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$
\begin{align}
&\mbox{P.V.}\int_{-\infty}^{\infty}{\dd x \over \pars{2 - x}\pars{x^{2} + 4}}
\\[5mm] \stackrel{\mbox{def.}}{=}\,\,\,&\
-\lim_{\epsilon \to 0^{+}}\bracks{%
\int_{-\infty}^{2 - \epsilon}{\dd x \over \pars{x - 2}\pars{x^{2} + 4}} +
\int_{2 + \epsilon}^{\infty}{\dd x \over \pars{x - 2}\pars{x^{2} + 4}}}
\\[5mm] = &\
-\lim_{\epsilon \to 0^{+}}
\bracks{\oint_{\mc{C}}{\dd z \over \pars{z - 2}\pars{z^{2} + 4}} -
\int_{\pi}^{0}{\epsilon\expo{\ic\theta}\ic\,\dd\theta \over \epsilon\expo{\ic\theta}\times 8}}
\\[5mm] = &\
-\lim_{\epsilon \to 0^{+}}\bracks{2\pi\ic\,{1 \over \pars{2\ic - 2}\pars{4\ic}} + {1 \over 8}\,\pi\ic} = \bbx{\ds{{1 \over 8}\,\pi}}
\end{align}
$\mc{C}$ 'closes' the integration in the upper complex plane with and additional indent around $\ds{z = 2}$. There is a simple pole, inside $\ds{\,\mc{C}}$, at $\ds{z = 2\ic}$.