$\newcommand{\+}{^{\dagger}}%
\newcommand{\angles}[1]{\left\langle #1 \right\rangle}%
\newcommand{\braces}[1]{\left\lbrace #1 \right\rbrace}%
\newcommand{\bracks}[1]{\left\lbrack #1 \right\rbrack}%
\newcommand{\ceil}[1]{\,\left\lceil #1 \right\rceil\,}%
\newcommand{\dd}{{\rm d}}%
\newcommand{\ds}[1]{\displaystyle{#1}}%
\newcommand{\equalby}[1]{{#1 \atop {= \atop \vphantom{\huge A}}}}%
\newcommand{\expo}[1]{\,{\rm e}^{#1}\,}%
\newcommand{\fermi}{\,{\rm f}}%
\newcommand{\floor}[1]{\,\left\lfloor #1 \right\rfloor\,}%
\newcommand{\half}{{1 \over 2}}%
\newcommand{\ic}{{\rm i}}%
\newcommand{\iff}{\Longleftrightarrow}
\newcommand{\imp}{\Longrightarrow}%
\newcommand{\isdiv}{\,\left.\right\vert\,}%
\newcommand{\ket}[1]{\left\vert #1\right\rangle}%
\newcommand{\ol}[1]{\overline{#1}}%
\newcommand{\pars}[1]{\left( #1 \right)}%
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\pp}{{\cal P}}%
\newcommand{\root}[2][]{\,\sqrt[#1]{\,#2\,}\,}%
\newcommand{\sech}{\,{\rm sech}}%
\newcommand{\sgn}{\,{\rm sgn}}%
\newcommand{\totald}[3][]{\frac{{\rm d}^{#1} #2}{{\rm d} #3^{#1}}}
\newcommand{\ul}[1]{\underline{#1}}%
\newcommand{\verts}[1]{\left\vert\, #1 \,\right\vert}$
Let's check what Euler-Maclaurin says:
\begin{align}
&\color{#0000ff}{\large\sum_{k = 1}^{n}{1 \over \root{n^{2} + n - k^{2}}}}={1 \over \root{n}} +
\sum_{k = 1}^{n - 1}{1 \over \root{n^{2} + n - k^{2}}}
\\[3mm]&=
{1 \over \root{n}} + \overbrace{\int_{0}^{n}{\dd k \over \root{n^{2} + n - k^{2}}}}^{\ds{\arcsin\pars{n \over\root{n^{2} + n}}}}
-
\half\pars{{1 \over \root{n^{2} + n}} + {1 \over \root{n}}}
+ {1 \over 12}\,{1 \over \root{n}}\\[3mm]&
- {1 \over 720}\pars{{15 \over \root{n}} + {9 \over n\root{n}}} + \cdots
\color{#0000ff}{\large\stackrel{n \to \infty}{\to} {\pi \over 2}}
\end{align}
It seems $\pi/2$ is the correct result but the convergence, in the numerical side, is very slow. Even with $n = 10^{8}$, the difference respect of $\pi/2$ is $\approx -0.00135758$.