How to prove that
$$4\int_0^1\frac{\chi_2(x)\operatorname{Li}_2(x)}{x}\ dx+\int_0^1\frac{\log(1-x)\log^2(x)\log(1+x)}{x}\ dx=\frac{29}4\zeta(2)\zeta(3)-\frac{91}8\zeta(5)$$
Where $\chi_2(x)=\sum_{n=1}^\infty\frac{x^{2n-1}}{(2n-1)^2}$ is the Legendre Chi function and $ \operatorname{Li}_2(x)=\sum_{n=1}^\infty\frac{x^n}{n^2}$ is the Dilogarithm function.
This integral was proposed by Cornel.
Using the relation between the Chi function and Dilogarithm we can rewrite the first integral as: $$4\int_0^1\frac{\chi_2(x)\operatorname{Li}_2(x)}{x}dx=2\int_0^1\frac{\operatorname{Li}^2_2(x)}{x} dx-2\int_0^1\frac{\operatorname{Li}_2(x)\operatorname{Li}_2(-x)}{x} dx$$ You solved the first part here. $$\int_0^1\frac{\operatorname{Li}_2^2(x)}{x}dx=2\zeta(2)\zeta(3)-3\zeta(5)$$ And the second one is found here: $$\int_0^1\frac{\operatorname{Li}_2(x){\operatorname{Li}_2(-x)}}{x}dx =-\frac54\zeta(2)\zeta(3)+\frac{59}{32}\zeta(5)$$ Combinging the two results from above yields: $$\boxed{4\int_0^1\frac{\chi_2(x)\operatorname{Li}_2(x)}{x}dx=\frac{13}{2}\zeta(2)\zeta(3)-\frac{155}{16}\zeta(5)}$$ The second integral is solved here. $$\boxed{\int_0^1\frac{\ln(1-x)\ln^2 x\ln(1+x)}{x}dx=\frac34 \zeta(2)\zeta(3)-\frac{27}{16}\zeta(5)}$$ Combining the two boxed results gives: $$4\int_0^1\frac{\chi_2(x)\operatorname{Li}_2(x)}{x} dx+\int_0^1\frac{\ln(1-x)\ln^2(x)\ln(1+x)}{x} dx=\frac{29}4\zeta(2)\zeta(3)-\frac{91}8\zeta(5)$$
Remark.
We know from above that: $$\int_0^1\frac{\chi_2(x)\operatorname{Li}_2(x)}{x}dx=\frac{13}{8}\zeta(2)\zeta(3)-\frac{155}{64}\zeta(5)$$ But integating by parts also gives us: $$\sum_{n=0}^\infty \frac{1}{(2n+1)^2}\int_0^1 x^{2n}\operatorname{Li}_2 (x)dx$$$$\overset{IBP}=\sum_{n=0}^\infty \frac{\operatorname{Li}_2(1)}{(2n+1)^3}+\sum_{n=0}^\infty \frac{1}{(2n+1)^3}\int_0^1 x^{2n}\ln(1-x)dx$$ $$=\frac{7}{8}\zeta(2)\zeta(3) +\sum_{n=0}^\infty \frac{H_{2n+1}}{(2n+1)^4}$$ Which results in: $$\sum_{n=0}^\infty \frac{H_{2n+1}}{(2n+1)^4}=\frac34\zeta(2)\zeta(3)-\frac{155}{64}\zeta(5)$$ Alteratively one can compute that sum in a different way to find the value of the first integral.