Alternative proof for $\zeta\left(2,\frac14\right)=\psi^{(1)}\left(\frac14\right)=\pi^2+8G$ On the German Wikipedia page of the Hurwitz Zeta Function I have come across the following formula

$$\zeta\left(2,\frac14\right)~=~\pi^2+8G\tag1$$

Where $G$ is Catalan's Constant. Even though I was able proving $(1)$ I am dissatisfied with my own attempt since it is heavily relying on several relatives of the Riemann Zeta Functions. However, first of all I will present my own solution. Starting with the series representation of $\zeta(2)$ we get
$$\begin{align*}
\zeta(2)=\sum_{n=1}^\infty \frac1{n^2}&=\frac1{1^2}+\frac1{2^2}+\frac1{3^2}+\sum_{n=1}^\infty\frac1{(4n)^2}+\frac1{(4n+1)^2}+\frac1{(4n+2)^2}+\frac1{(4n+3)^2}\\
&=\frac1{16}\zeta(2)+\sum_{n=0}^\infty \frac1{4(2n+1)^2}+\frac1{(4n+1)^2}+\frac1{(4n+3)^2}\\
&=\frac1{16}\zeta(2)+\frac14\lambda(2)+\sum_{n=0}^\infty \frac1{(4n+1)^2}+\frac12\left[\frac1{(2n+1)^2}-\frac{(-1)^n}{(2n+1)^2}\right]\\
&=\frac1{16}\zeta(2)+\frac14\lambda(2)+\frac12[\lambda(2)-\beta(2)]+\sum_{n=0}^\infty \frac1{(4n+1)^2}\\
\therefore~\sum_{n=0}^\infty \frac1{(4n+1)^2}&=\frac{15}{16}\zeta(2)-\frac34\lambda(2)+\frac12\beta(2)\\
&=\frac{15}{16}\zeta(2)-\frac34\frac34\zeta(2)+\frac12 G\\&=\frac1{16}\pi^2+\frac12 G
\end{align*}$$

$$\therefore~\zeta\left(2,\frac14\right)~=~\sum_{n=0}^\infty\frac1{\left(n+\frac14\right)^2}~=~\pi^2+8G$$

Where $\zeta(s)$ dnotes the Riemann Zeta Function, $\lambda(s)$ the Dirichlet Lambda Function, $\beta(s)$ the Dirichlet Beta Function. Moreover the relation $\lambda(s)=(1-2^{-s})\zeta(s)$ and the well-known values $\zeta(2)=\frac{\pi^2}6$ and $\beta(2)=G$ were used.

I am suspicious about the heavy usage of the whole Zeta Function machinery and I am curious if there exists a shorter and more elegant way of proving $(1)$?

Thanks in advance!
EDIT
As Zacky pointed out within the comments this special value of the Hurwitz Zeta Function can also be interpreted as a particular value of the Trigamma Function since in general we got a the following series expansion of the Polygamma Function
$$\begin{align*}
\psi^{(n)(z)}&=(-1)^{n+1}n!\sum_{k=0}^\infty\frac1{(z+k)^{n+1}}\\
&=(-1)^{n+1}n!\zeta(n+1,z)
\end{align*}$$
So for $n=1$ and $z=\frac14$ it directly follows that
$$(-1)^{1+1}(1!)\psi^{(1)}\left(\frac14\right)=\zeta\left(1+1,\frac14\right)\Rightarrow \psi^{(1)}\left(\frac14\right)=\zeta\left(2,\frac14\right)$$
 A: We can use the following representation of the digamma function from here, namely:
$$\psi(s+1)=-\gamma+\int_0^1 \frac{1-x^s}{1-x}dx\Rightarrow \psi_1(s+1)=\int_0^1 \frac{x^{s}\ln x}{x-1}dx$$
Above follows since $\frac{d}{dz}\psi(z)=\psi_1{(z)} $, so we can rewrite our desired value as:
$$\psi_1\left(\frac14\right)=\int_0^1 \frac{x^{1/4-1} \ln x}{x-1}dx$$
Notice that $\frac{d}{dx}\left(4x^{\frac{1}{4}}\right)=x^{\frac14-1}$, so we can easily substitute $x^{\frac14}=t\Rightarrow x=t^4$ to get: $$\psi_1\left(\frac14\right)=16\int_0^1 \frac{\ln t}{t^4-1}dt$$
We might already recall that we saw before something similar, $\int_0^1 \frac{\ln x}{1+x^2}dx=-G$, thus let's try to get there.
$$\frac{1}{x^4-1}=\frac12 \frac{(x^2+1)-(x^2-1)}{(x^2+1)(x^2-1)}=\frac12 \left(\frac1{x^2-1}-\frac{1}{x^2+1}\right)$$
$$\Rightarrow \psi_1\left(\frac14\right)=8\int_0^1\frac{\ln t}{t^2-1}dt -8\int_0^1 \frac{\ln t}{t^2+1}dt=\boxed{\pi^2 +8G}$$
I am pretty sure you can prove that the first integral equals to $\frac{\pi^2}{8}$, but here are found many proofs.
A: Inspired by Zacky's comment on the integral representation of the Hurwitz Zeta Function I have found another pretty straightforward way. First we notice that

$$\zeta(s,q)~=~\frac1{\Gamma(s)}\int_0^\infty \frac{t^{s-1}e^{-qt}}{1-e^{-t}}\mathrm dt\tag1$$

Now substitute $s=2$ and $q=\frac14$ followed by $u=e^{-t}$ to get
$$\mathfrak I=\int_0^{\infty}\frac{te^{-t/4}}{1-e^{-t}}\mathrm dt=\int_0^1\frac{u^{1/4-1}\cdot \log(u)}{u-1}\mathrm du$$
And now we are at the same point from where Zacky deduced the right value via well-known integrals. Hence his method was quite elegant I will not repeat his solution but just refer to it. Basically using $(1)$ does not force us to rely on the Trigamma Function but instead leaves us all along with the Hurwitz Zeta Function and some nice integrals.
A: We can use the generalization identity 
$$\psi^{(n)}(a)=-\int_0^1\frac{x^{a-1}\ln^n(x)}{1-x}\ dx$$
set $n=1$ and $a=1/4$ we get
$$\psi^{(1)}\left(\frac14\right)=-\int_0^1\frac{x^{1/4-1}\ln(x)}{1-x}\ dx$$
which is the same integral @Zacky got.
