$$z=\frac{a+b+c}{b-a}=1+\frac{2a+c}{b-a}>1.$$
This prevents us from defining our Gauss hypergeometric function by either its primary infinite series definition or Euler integral definition. Also complicating matters is the integer nature of the parameters.
The complete definition for the Gauss hypergeometric function includes the following two cases:
$$\begin{align}
{_2F_1}{\left(\alpha,\beta;\gamma;z\right)}
&:=\frac{\operatorname{B}{\left(\beta-\alpha,\gamma-\beta\right)}\,\left(-z\right)^{-\alpha}}{\operatorname{B}{\left(\beta,\gamma-\beta\right)}}\sum_{k=0}^{\infty}\frac{\left(\alpha\right)_{k}\,\left(\alpha-\gamma+1\right)_{k}\,z^{-k}}{\left(\alpha-\beta+1\right)_{k}\,k!}\\
&~~~~~+\frac{\operatorname{B}{\left(\beta,\alpha-\beta\right)}\,\left(-z\right)^{-\beta}}{\operatorname{B}{\left(\beta,\gamma-\beta\right)}}\sum_{k=0}^{\infty}\frac{\left(\beta\right)_{k}\,\left(\beta-\gamma+1\right)_{k}\,z^{-k}}{\left(\beta-\alpha+1\right)_{k}\,k!};~~~\small{\left|z\right|>1\land\alpha-\beta\notin\mathbb{Z}},\tag{3a}\\
\end{align}$$
and
$${_2F_1}{\left(\alpha,\beta;\gamma;z\right)}:=\lim_{\epsilon\to0}{_2F_1}{\left(\alpha,\beta+\epsilon;\gamma;z\right)};~~~\small{\left|z\right|>1\land\alpha-\beta\in\mathbb{Z}}.\tag{3b}$$
Letting $\left(m,n\right)\in\mathbb{Z}_{\ge0}\times\mathbb{N}\land z\in\left(1,\infty\right)$,
$$\begin{align}
{_2F_1}{\left(m+n,n;n+1;z\right)}
&=\lim_{\epsilon\to0}{_2F_1}{\left(m+n,n+\epsilon;n+1;z\right)}\\
&=\lim_{\epsilon\to0}\bigg{[}\frac{\operatorname{B}{\left(\epsilon-m,1-\epsilon\right)}\,\left(-z\right)^{-m-n}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\sum_{k=0}^{\infty}\frac{\left(m+n\right)_{k}\,\left(m\right)_{k}\,z^{-k}}{\left(m-\epsilon+1\right)_{k}\,k!}\\
&~~~~~+\frac{\operatorname{B}{\left(n+\epsilon,m-\epsilon\right)}\,\left(-z\right)^{-n-\epsilon}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\sum_{k=0}^{\infty}\frac{\left(n+\epsilon\right)_{k}\,\left(\epsilon\right)_{k}\,z^{-k}}{\left(\epsilon-m+1\right)_{k}\,k!}\bigg{]}\\
&=\lim_{\epsilon\to0}\bigg{[}\frac{\operatorname{B}{\left(\epsilon-m,1-\epsilon\right)}\,\left(-z\right)^{-m-n}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\,{_2F_1}{\left(m+n,m;m-\epsilon+1;\frac{1}{z}\right)}\\
&~~~~~+\frac{\operatorname{B}{\left(n+\epsilon,m-\epsilon\right)}\,\left(-z\right)^{-n-\epsilon}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\,{_2F_1}{\left(n+\epsilon,\epsilon;\epsilon-m+1;\frac{1}{z}\right)}\bigg{]}\\
&=\lim_{\epsilon\to0}\bigg{[}\frac{\operatorname{B}{\left(\epsilon-m,1-\epsilon\right)}\,\left(-z\right)^{-m-n}\left(1-\frac{1}{z}\right)^{-m-n}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\,{_2F_1}{\left(n+m,1-\epsilon;1-\epsilon+m;\frac{1}{1-z}\right)}\\
&~~~~~+\frac{\operatorname{B}{\left(n+\epsilon,m-\epsilon\right)}\,\left(-z\right)^{-n-\epsilon}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\,{_2F_1}{\left(n+\epsilon,\epsilon;\epsilon-m+1;\frac{1}{z}\right)}\bigg{]}.\\
\end{align}$$
At this point it will be convenient to consider the $m=0$ and $m>0$ cases separately.
Consider first the $m>0$ case, where $\left(m,n\right)\in\mathbb{N}^{2}\land z\in\left(1,\infty\right)$.
$$\begin{align}
{_2F_1}{\left(m+n,n;n+1;z\right)}
&=\lim_{\epsilon\to0}\bigg{[}\frac{\operatorname{B}{\left(\epsilon-m,1-\epsilon\right)}\,\left(-z\right)^{-m-n}\left(1-\frac{1}{z}\right)^{-m-n}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\\
&~~~~~\times\,{_2F_1}{\left(n+m,1-\epsilon;1-\epsilon+m;\frac{1}{1-z}\right)}\\
&~~~~~+\frac{\operatorname{B}{\left(n+\epsilon,m-\epsilon\right)}\,\left(-z\right)^{-n-\epsilon}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\,{_2F_1}{\left(n+\epsilon,\epsilon;\epsilon-m+1;\frac{1}{z}\right)}\bigg{]}\\
&=\lim_{\epsilon\to0}\bigg{[}\frac{1}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\cdot\frac{\sin{\left(m\pi\right)}\Gamma{\left(1-\epsilon\right)}}{\left(m-\epsilon\right)\sin{\left(\pi\left(\epsilon-m\right)\right)}}\cdot\frac{\Gamma{\left(m\right)}}{\Gamma{\left(m-\epsilon\right)}}\\
&~~~~~\times\left(1-z\right)^{-m-n}\,{_2F_1}{\left(n+m,1-\epsilon;1-\epsilon+m;\frac{1}{1-z}\right)}\\
&~~~~~+\frac{\operatorname{B}{\left(n+\epsilon,m-\epsilon\right)}\,\left(-z\right)^{-n-\epsilon}}{\operatorname{B}{\left(n+\epsilon,1-\epsilon\right)}}\,{_2F_1}{\left(n+\epsilon,\epsilon;\epsilon-m+1;\frac{1}{z}\right)}\bigg{]}\\
&=-\frac{n}{m}\left(1-z\right)^{-m-n}\,{_2F_1}{\left(n+m,1;1+m;\frac{1}{1-z}\right)}\\
&~~~~~+\frac{n\,\operatorname{B}{\left(m,n\right)}}{\left(-z\right)^{n}}\lim_{\epsilon\to0}{_2F_1}{\left(n+\epsilon,\epsilon;\epsilon-m+1;\frac{1}{z}\right)}\\
&=\frac{n\operatorname{B}{\left(m,n\right)}}{\left(-z\right)^{n}}-\frac{n}{m}\left(1-z\right)^{-m-n}\,{_2F_1}{\left(n+m,1;1+m;\frac{1}{1-z}\right)}\\
&=n\left(-z\right)^{-n}\operatorname{B}{\left(m,n\right)}-n\left(-z\right)^{-n}\left(1-z\right)^{-m}\sum_{k=0}^{n-1}\frac{\left(1-n\right)_{k}\,\left(-1\right)^{k}}{\left(k+m\right)\,k!\,\left(z-1\right)^{k}}\\
&=n\left(-z\right)^{-n}\operatorname{B}{\left(m,n\right)}-n\left(-z\right)^{-n}\left(1-z\right)^{-m}\sum_{k=0}^{n-1}\frac{\binom{n-1}{k}}{\left(k+m\right)\,\left(z-1\right)^{k}}\\
&=n\left(-z\right)^{-n}\left[\operatorname{B}{\left(m,n\right)}-\left(-1\right)^{m}\sum_{k=0}^{n-1}\frac{\binom{n-1}{k}}{\left(m+k\right)\,\left(z-1\right)^{m+k}}\right].\\
\end{align}$$
It remains to consider the $m=0$ special case, but for the time being I prefer to leave this as an exercise to the reader...