$\newcommand{\bbx}[1]{\,\bbox[8px,border:1px groove navy]{\displaystyle{#1}}\,}
\newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack}
\newcommand{\dd}{\mathrm{d}}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,}
\newcommand{\ic}{\mathrm{i}}
\newcommand{\mc}[1]{\mathcal{#1}}
\newcommand{\mrm}[1]{\mathrm{#1}}
\newcommand{\pars}[1]{\left(\,{#1}\,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,}
\newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}}
\newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$
\begin{align}
\sin^{2}\pars{\pi\root{n^{2} + n}} & =
\sin^{2}\pars{\pi n\root{1 + {1 \over n}}} =
\sin^{2}\pars{\pi n + \pi n\bracks{\root{1 + {1 \over n}} - 1}}
\\[5mm] & =
\bracks{\pars{-1}^{n}\sin\pars{\pi n\bracks{\root{1 + {1 \over n}} - 1}}}^{2}
\\[5mm] & =
\sin^{2}\pars{\pi \over \root{1 + 1/n} + 1}
\,\,\,\stackrel{\mrm{as}\ n\ \to\ \infty}{\to}\,\,\, \sin^{2}\pars{\pi \over 2} = \bbx{\ds{1}}
\end{align}