If $C_o,C_1...$ are the binomial coefficents in the expansion of $(1+x)^n$ and $$\sum_{r=0}^{n} (-1)^r \binom{n}{r} \frac{1}{(r+1)^2} = k \sum_{r=0}^{n} \frac{1}{r+1}$$ Find a k such that the above equation is satisfied
My attempt: $$ (1+x)^n = \sum_{k=0}^{k=n} \binom{n}{k} x^k$$
integrate both sides
$$ \frac{ (1+x)^{n+1} }{n+1} =\sum_{k=0}^{n} \binom{n}{k} \frac{x^{k+1}}{k+1} +C$$
$$ x= 0 $$
$$ \implies \frac{-n}{n+1} = C$$
Divide both sides by 'x' and integrate
$$ \int \frac{ (1+x)^{n+1} }{ (x) n+1} dx = \sum_{k=0}^{n} \binom{n}{k} \frac{x^{k+1}}{(k+1)^2} - \frac{n}{n+1} \ln(x)+ C'$$
Or,
$$ \int \frac{ (1+x)^{n+1} }{ (x) n+1} dx - \frac{n}{n+1} \ln(x)+ C' = \sum_{k=0}^{n} \binom{n}{k} \frac{x^{k+1}}{(k+1)^2}$$
Not so sure what do here, like what to put as bounds. Slightly concerned I may have to evaluate a negative logarithm
$\newcommand{\bbx}[1]{\,\bbox[15px,border:1px groove navy]{\displaystyle{#1}}\,} \newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace} \newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack} \newcommand{\dd}{\mathrm{d}} \newcommand{\ds}[1]{\displaystyle{#1}} \newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,} \newcommand{\ic}{\mathrm{i}} \newcommand{\mc}[1]{\mathcal{#1}} \newcommand{\mrm}[1]{\mathrm{#1}} \newcommand{\pars}[1]{\left(\,{#1}\,\right)} \newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}} \newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,} \newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}} \newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$ \begin{align} &\bbox[5px,#ffd]{\sum_{r = 0}^{n}\pars{-1}^{r}{n \choose r} {1 \over \pars{r + 1}^{2}}} = \sum_{r = 0}^{n}\pars{-1}^{r}{n \choose r}\ \overbrace{\bracks{-\int_{0}^{1}\ln\pars{x}\, x^{r}\,\dd x}} ^{\ds{1 \over \pars{r + 1}^{2}}} \\[5mm] = &\ -\int_{0}^{1}\ln\pars{x}\sum_{r = 0}^{n}{n \choose r}\pars{-x}^{r}\,\dd x = -\int_{0}^{1}\ln\pars{x}\pars{1 - x}^{n}\,\dd x \\[5mm] = &\ -\bracks{\xi^{1}}\int_{0}^{1}x^{\xi}\pars{1 - x}^{n}\,\dd x = -\bracks{\xi^{1}}\bracks{\Gamma\pars{\xi + 1}\Gamma\pars{n + 1} \over \Gamma\pars{\xi + n + 2}} \\[5mm] = &\ -n!\bracks{\xi^{1}}\bracks{% \Gamma\pars{1} + \Gamma\, '\pars{1}\xi \over \Gamma\pars{n + 2} + \Gamma\, '\pars{n + 2}\xi} \\[5mm] = &\ -\,{1 \over n + 1}\bracks{\xi^{1}}\bracks{% 1 - \gamma\xi \over 1 + \Psi\pars{n + 2}\xi} \\[5mm] = &\ -\,{1 \over n + 1}\bracks{\xi^{1}}\braces{\vphantom{\Large A}% \pars{\vphantom{\large A}1 - \gamma\xi}\bracks{\vphantom{\large A}1 - \Psi\pars{n + 2}\xi}} \\[5mm] = &\ -\,{1 \over n + 1}\bracks{-\gamma - \Psi\pars{n + 2}} = -\,{1 \over n + 1}\pars{-H_{n + 1}} = \\[5mm] = &\ {1 \over n + 1}\sum_{r = 0}^{n}{1 \over r + 1} \implies \bbx{k = {1 \over n + 1}} \\ & \end{align}
$\ds{\bracks{\xi^{m}}}$ is the Coefficient Extraction Operator.
$\ds{\Gamma}$ is the Gamma Function.
$\ds{\gamma}$ is the Euler-Mascheroni Constant.
$\ds{\Psi}$ is the Digamma Function.
$\ds{H_{z}}$ is a Harmonic Number.