I have $2$ approaches, both of which rely on the result
$$\int_0^1\frac{\ln x}{x^2-1}~\mathrm dx=\frac{\pi^2}8$$
\begin{align}\int_0^1\frac{\ln x}{x^2-1}~\mathrm dx&\overset{x\mapsto\tanh x}=\int_0^\infty\ln(\coth x)~\mathrm dx\\&=\frac12\int_0^\infty\ln\left(\frac{2\cosh^2x}{2\sinh^2x}\right)~\mathrm dx\\&=\frac12\int_0^\infty\ln\left(\frac{\cosh2x+1}{\cosh2x-1}\right)~\mathrm dx\\&\overset{2x\mapsto x}=\frac14\int_0^\infty\ln\left(\frac{\cosh x+1}{\cosh x-1}\right)\mathrm dx\\&=\frac14\int_0^\infty\int_{-1}^1\frac{\mathrm dy}{\cosh x+y}~\mathrm dx\\&=\frac14\int_0^\infty\left(\int_0^1\frac1{\cosh x+y}~\mathrm dy+\underbrace{\int_{-1}^0\frac1{\cosh x+y}~\mathrm dy}_{y\mapsto-y}\right)~\mathrm dx\\&=\frac14\int_0^\infty\int_0^1\frac1{\cosh x+y}+\frac1{\cosh x-y}~\mathrm dy~\mathrm dx\\&=\frac12\int_0^1\int_0^\infty\frac{\cosh x}{\sinh^2x+1-y^2}~\mathrm dx~\mathrm dy\\&=\frac\pi4\int_0^1\frac{\mathrm dy}{\sqrt{1-y^2}}\\&=\frac{\pi^2}8\end{align}
$\textbf{Method 1:}$ Consider $I_\pm=\int_0^1\frac{\ln x}{1\pm x}~\mathrm dx$. Then, IBP,
$$I_\pm=\pm\int_0^1\frac{\ln(1\pm x)}x~\mathrm dx$$
Now, utilizing the identity $(1+x)(1-x)=1-x^2$,
\begin{align}I_+-I_-&=\int_0^1\frac{\ln(1-x^2)}x~\mathrm dx\\&\overset{x^2\mapsto x}=-\frac{I_-}2\\\implies I_+&=\frac{I_-}2\end{align}
And since
\begin{align}\int_0^1\frac{\ln x}{x^2-1}~\mathrm dx&=\frac12\int_0^1\ln x\left(\frac1{1+x}+\frac1{1-x}\right)~\mathrm dx\\&=\frac{I_++I_-}2\\&=\frac{3I_-}4\\\implies I_-&=\frac{\pi^2}6\end{align}
as desired.
$\textbf{Method 2:}$ Consider $I=\int_0^1\frac{x\ln x}{x^2-1}~\mathrm dx$, $J=\int_0^1\frac{\ln x}{x^2-1}~\mathrm dx$.
Note that on adding both these integrals, a factor of $(x+1)$ gets cancelled:
$$I+J=\int_0^1\frac{\ln x}{x-1}\mathrm dx$$
But substituting $x^2\mapsto x$ in $I$ gives:
$$I=\frac14\int_0^1\frac{\ln x}{x-1}~\mathrm dx$$
Hence,
$$I=\frac{J}3=\frac{\pi^2}{24}$$
$$\implies\int_0^1\frac{\ln x}{x-1}~\mathrm dx=4I=\frac{\pi^2}6$$
as desired.