Show that the directional derivative of $F:H^1(\mathbb{R})\to \mathbb{R}, u\mapsto \int_{\Omega} \sqrt{1+|\nabla u|^2}$ is $$\partial_e F(u)=\int_{\Omega} \frac{\nabla{u} \cdot \nabla{e}}{\sqrt{1+|\nabla u|^2}}.$$
By definition of directional derivative I think we have $$\partial_e F(u)=\lim_{t\to0}\frac{F(u+te)-F(u)}{t}=\lim_{t\to0}\frac{F(u+te)-F(u)}{te}e=F'(u)e$$ or rather $F'(u)\cdot e$?
Differentiating naively I get $F'(u)=\int_\Omega\frac{\nabla{u}}{\sqrt{1+|\nabla u|^2}}$ and so I would have $\partial_e F(u)=\int_{\Omega} \frac{\nabla{u} \cdot e}{\sqrt{1+|\nabla u|^2}}$, missing a gradient.
I also tried to expand $F(u+te)$ but I am not sure how to simply $F(u+te)-F(u)= \sqrt{1+|\nabla{u}+t\nabla{e}|^2}-\sqrt{1+|\nabla{u}|^2}$.
As noted by @mattos, the first variation of a functional gives the Gateaux derivative (directional derivative): $$\partial F_e(u)=\lim_{t\to 0} \frac{F(u+te)-F(u)}{t}= \frac{d}{dt} F(u+te)\bigg\rvert_{t=0}=\frac{d}{dt} \int_{\Omega}\sqrt{1+|\nabla{u}+t\nabla{e}|^2}dx\bigg\rvert_{t=0}$$
Taking the derivative inside the integral and using the chain rule we get $$ \partial F_e(u)=\int_{\Omega} \frac{(\nabla{u}+t\nabla{e})\cdot \nabla{e}}{\sqrt{1+|\nabla{u}+t\nabla{e}|^2}}dx\bigg\rvert_{t=0}=\int_{\Omega} \frac{(\nabla{u}+t\nabla{e})\cdot \nabla{e}}{\sqrt{1+|\nabla{u}+t\nabla{e}|^2}}dx\bigg\rvert_{t=0}=\int_{\Omega} \frac{\nabla{u}\cdot \nabla{e}}{\sqrt{1+|\nabla{u}|^2}}dx.$$