Growth of Digamma function 
For $1\le \sigma \le 2$ and $t\ge 2$, $s=\sigma+it$ prove that $\displaystyle \frac{\Gamma'(s)}{\Gamma(s)}=O(\log t)$.

From Stirling's formula we have, $\displaystyle \Gamma(s)\approx \sqrt{2\pi}\exp\{s\log s-s-\frac 12 \log s\}$.
Then, $\displaystyle \frac{\Gamma'(s)}{\Gamma(s)}\approx\log s-\frac{1}{2s}$. From here I'm unable to estimate !! Any hint. ?
Where can I get rigorous proof ? 
Edit: Wikipedia links below the question are NOT clear enough to me.

Let's use the following formula, from Abramowitz and Stegun, valid everywhere in the strip of interest:
$$
\psi(z)=-\gamma+\sum_{n=1}^{\infty}\frac{z-1}{n(n+z-1)}.
$$
Letting $a=\sigma-1\in[0,1]$,
$$
\psi(\sigma+it)+\gamma=\sum_{n=1}^{\infty}\frac{a+it}{n(n+a+it)}=\sum_{n=1}^{\infty}\frac{\left(a+it\right)(n+a-it)}{n\left((n+a)^2+t^2\right)}=\sum_{n=1}^{\infty}\frac{a(n+a)+int+t^2}{n\left((n+a)^2+t^2\right)}=\sum_{n=1}^{\infty}\frac{a(n+a)}{n\left((n+a)^2+t^2\right)}+i\sum_{n=1}^{\infty}\frac{t}{(n+a)^2+t^2}+\sum_{n=1}^{\infty}\frac{t^2}{n\left((n+a)^2 + t^2\right)}.
$$
The first term is no more than $2a\sum_{n=1}^{\infty}1/n^2=\pi^2/3$, independent of $t$.  The second and third terms can be bounded by integrals; the third integral must be split into two sums first.  Specifically,
$$
\sum_{n=1}^{\infty}\frac{t}{(n+a)^2+t^2}\le \sum_{n=1}^{\infty}\frac{1/t}{(n/t)^2+1}\le\int_{0}^{\infty}\frac{dx}{x^2+1}=\frac{\pi}{2},
$$
and
$$
\sum_{n=t+1}^{\infty}\frac{t^2}{n\left((n+a)^2+t^2\right)}\le \sum_{n=t+1}^{\infty}\frac{1/t}{(n/t)\left((n/t)^2+1\right)}\le\int_{1}^{\infty}\frac{dx}{x(x^2+1)}=\log\left(\frac{x}{\sqrt{x^2+1}}\right)\Bigg\vert_{1}^{\infty}=\frac{1}{2}\log 2.
$$
Note the restricted range of summation.  Finally,
$$
\sum_{n=1}^{t}\frac{t^2}{n\left((n+a)^2+t^2\right)}\le\sum_{n=1}^{t}\frac{1}{n}=O(\log t),
$$
so we conclude that $\psi(\sigma+it)$ is $O(\log t)$, with bounded imaginary part.
