Methods to evaluate $ \int _{a }^{b }\!{\frac {\ln \left( tx + u \right) }{m{x}^{2}+nx +p}}{dx} $
Related problems: (I), (II). You can use the partial fraction technique combined with the use the dilogarithm function $\operatorname{Li}_{2}(x)$, which is defined by
$$\operatorname{Li}_{2}(x) = \int_{1}^{x} \frac{\ln(t)}{1-t} \,dt \,.$$
Here is an example,
$$ \int_{a}^{b} \frac{\ln(x)}{cx+d}dx =- \frac{1}{d}\left( \operatorname{Li}_{2}\left( {\frac {c+da}{c}} \right) +\ln \left(a\right) \ln \left( {\frac {c+da}{c}} \right) -\operatorname{Li}_{2} \left( { \frac {c+bd}{c}} \right) -\ln \left( b \right) \ln \left( {\frac {c+ bd}{c}} \right) \right) $$
Note that the above integral is undefined for $$ \left(a < -\frac{c}{d}, -\frac{c}{d} < b \right) $$
Have you seen http://www.recreatiimatematice.ro/arhiva/articole/RM12011DICU.pdf
For partial response
The answer below will restrict itself to the evaluation of integrals of the form $\int_{a}^{b}\mathrm{d}x\,\frac{\ln{\left(cx+d\right)}}{px^{2}+qx+r}$ for the case in which $q^{2}-4pr<0$ since the alternative cases are more than adequately addressed elsewhere.
Define the function $\mathcal{I}:\mathbb{R}\times\mathbb{R}_{>0}\times\mathbb{R}_{\ge0}\times\mathbb{R}_{>0}\rightarrow\mathbb{R}$ via the definite integral
$$\begin{align} \mathcal{I}{\left(a,b,c,z\right)} &:=\int_{0}^{z}\mathrm{d}x\,\frac{2b\ln{\left(x+c\right)}}{\left(x+a\right)^{2}+b^{2}}.\\ \end{align}$$
Also, define the Clausen function (of order 2) for real arguments by the integral representation
$$\operatorname{Cl}_{2}{\left(\theta\right)}:=-\int_{0}^{\theta}\mathrm{d}\varphi\,\ln{\left(\left|2\sin{\left(\frac{\varphi}{2}\right)}\right|\right)};~~~\small{\theta\in\mathbb{R}}.$$
We show below that the integral $\mathcal{I}$ can be evaluated in terms of Clausen functions and elementary functions.
Suppose $\left(a,b,c,z\right)\in\mathbb{R}\times\mathbb{R}_{>0}\times\mathbb{R}_{\ge0}\times\mathbb{R}_{>0}$, and set
$$\alpha:=\arctan{\left(\frac{a}{b}\right)}\in\left(-\frac{\pi}{2},\frac{\pi}{2}\right),$$
$$\beta:=\arctan{\left(\frac{z+a}{b}\right)}\in\left(-\frac{\pi}{2},\frac{\pi}{2}\right),$$
$$\gamma:=\arctan{\left(\frac{c-a}{b}\right)}\in\left(-\frac{\pi}{2},\frac{\pi}{2}\right).$$
Then,
$$\begin{align} \mathcal{I}{\left(a,b,c,z\right)} &=\left[\arctan{\left(\frac{z+a}{b}\right)}-\arctan{\left(\frac{a}{b}\right)}\right]\ln{\left(\left(a-c\right)^{2}+b^{2}\right)}\\ &~~~~~+\operatorname{Cl}_{2}{\left(2\alpha+2\gamma\right)}-\operatorname{Cl}_{2}{\left(2\beta+2\gamma\right)}+\operatorname{Cl}_{2}{\left(\pi-2\alpha\right)}-\operatorname{Cl}_{2}{\left(\pi-2\beta\right)}.\\ \end{align}$$
Proof:
$$\begin{align} \mathcal{I}{\left(a,b,c,z\right)} &=\int_{0}^{z}\mathrm{d}x\,\frac{2b\ln{\left(x+c\right)}}{\left(x+a\right)^{2}+b^{2}}\\ &=\int_{0}^{z}\mathrm{d}x\,\frac{2b\ln{\left(\left|x+c\right|\right)}}{\left(x+a\right)^{2}+b^{2}}\\ &=\int_{\frac{a}{b}}^{\frac{z+a}{b}}\mathrm{d}y\,\frac{2b^{2}\ln{\left(\left|by-a+c\right|\right)}}{\left(by-a+a\right)^{2}+b^{2}};~~~\small{\left[x=by-a\right]}\\ &=\int_{\frac{a}{b}}^{\frac{z+a}{b}}\mathrm{d}y\,\frac{2\ln{\left(\left|by+c-a\right|\right)}}{y^{2}+1}\\ &=\int_{\tan{\left(\alpha\right)}}^{\tan{\left(\beta\right)}}\mathrm{d}y\,\frac{2\ln{\left(\left|by+b\tan{\left(\gamma\right)}\right|\right)}}{y^{2}+1}\\ &=\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\frac{2\sec^{2}{\left(\varphi\right)}\ln{\left(\left|b\tan{\left(\varphi\right)}+b\tan{\left(\gamma\right)}\right|\right)}}{\tan^{2}{\left(\varphi\right)}+1};~~~\small{\left[y=\tan{\left(\varphi\right)}\right]}\\ &=2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|b\tan{\left(\varphi\right)}+b\tan{\left(\gamma\right)}\right|\right)}\\ &=2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(b\right)}+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|\tan{\left(\varphi\right)}+\tan{\left(\gamma\right)}\right|\right)}\\ &=2\ln{\left(b\right)}\int_{\alpha}^{\beta}\mathrm{d}\varphi+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|\frac{\sin{\left(\varphi\right)}\cos{\left(\gamma\right)}+\cos{\left(\varphi\right)}\sin{\left(\gamma\right)}}{\cos{\left(\varphi\right)}\cos{\left(\gamma\right)}}\right|\right)}\\ &=2\left(\beta-\alpha\right)\ln{\left(b\right)}+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|\frac{\sin{\left(\varphi+\gamma\right)}}{\cos{\left(\varphi\right)}\cos{\left(\gamma\right)}}\right|\right)}\\ &=2\left(\beta-\alpha\right)\ln{\left(b\right)}+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|\frac{1}{\cos{\left(\gamma\right)}}\right|\right)}\\ &~~~~~+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|\frac{\sin{\left(\varphi+\gamma\right)}}{\cos{\left(\varphi\right)}}\right|\right)}\\ &=2\left(\beta-\alpha\right)\ln{\left(b\right)}+2\left(\beta-\alpha\right)\ln{\left(\left|\frac{1}{\cos{\left(\gamma\right)}}\right|\right)}\\ &~~~~~+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|\frac{2\sin{\left(\varphi+\gamma\right)}}{2\cos{\left(\varphi\right)}}\right|\right)}\\ &=\left(\beta-\alpha\right)\ln{\left(b^{2}\right)}+\left(\beta-\alpha\right)\ln{\left(\frac{1}{\cos^{2}{\left(\gamma\right)}}\right)}\\ &~~~~~+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\frac{\left|2\sin{\left(\varphi+\gamma\right)}\right|}{\left|2\cos{\left(\varphi\right)}\right|}\right)}\\ &=\left(\beta-\alpha\right)\ln{\left(b^{2}\right)}+\left(\beta-\alpha\right)\ln{\left(\sec^{2}{\left(\gamma\right)}\right)}\\ &~~~~~+2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|2\sin{\left(\varphi+\gamma\right)}\right|\right)}\\ &~~~~~-2\int_{\alpha}^{\beta}\mathrm{d}\varphi\,\ln{\left(\left|2\cos{\left(\varphi\right)}\right|\right)}\\ &=\left(\beta-\alpha\right)\ln{\left(b^{2}\right)}+\left(\beta-\alpha\right)\ln{\left(1+\tan^{2}{\left(\gamma\right)}\right)}\\ &~~~~~+2\int_{\alpha+\gamma}^{\beta+\gamma}\mathrm{d}\varphi\,\ln{\left(\left|2\sin{\left(\varphi\right)}\right|\right)};~~~\small{\left[\varphi\mapsto\varphi-\gamma\right]}\\ &~~~~~+2\int_{\frac{\pi}{2}-\beta}^{\frac{\pi}{2}-\alpha}\mathrm{d}\varphi\,(-1)\ln{\left(\left|2\sin{\left(\varphi\right)}\right|\right)};~~~\small{\left[\varphi\mapsto\frac{\pi}{2}-\varphi\right]}\\ &=\left(\beta-\alpha\right)\ln{\left(b^{2}\right)}+\left(\beta-\alpha\right)\ln{\left(1+\left(\frac{c-a}{b}\right)^{2}\right)}\\ &~~~~~+\int_{2\beta+2\gamma}^{2\alpha+2\gamma}\mathrm{d}\varphi\,(-1)\ln{\left(\left|2\sin{\left(\frac{\varphi}{2}\right)}\right|\right)}\\ &~~~~~+\int_{\pi-2\beta}^{\pi-2\alpha}\mathrm{d}\varphi\,(-1)\ln{\left(\left|2\sin{\left(\frac{\varphi}{2}\right)}\right|\right)};~~~\small{\left[\varphi\mapsto\frac{\varphi}{2}\right]}\\ &=\left(\beta-\alpha\right)\ln{\left(\left(a-c\right)^{2}+b^{2}\right)}\\ &~~~~~+\operatorname{Cl}_{2}{\left(2\alpha+2\gamma\right)}-\operatorname{Cl}_{2}{\left(2\beta+2\gamma\right)}\\ &~~~~~+\operatorname{Cl}_{2}{\left(\pi-2\alpha\right)}-\operatorname{Cl}_{2}{\left(\pi-2\beta\right)}\\ &=\left[\arctan{\left(\frac{z+a}{b}\right)}-\arctan{\left(\frac{a}{b}\right)}\right]\ln{\left(\left(a-c\right)^{2}+b^{2}\right)}\\ &~~~~~+\operatorname{Cl}_{2}{\left(2\alpha+2\gamma\right)}-\operatorname{Cl}_{2}{\left(2\beta+2\gamma\right)}+\operatorname{Cl}_{2}{\left(\pi-2\alpha\right)}-\operatorname{Cl}_{2}{\left(\pi-2\beta\right)}\blacksquare.\\ \end{align}$$