Proof. If $E$ is constant, then $\sigma_u$ is constant, analogue $G$ constant then $\sigma_v$ is constant.
$F$ constant then the angle between $\sigma_u$ and $\sigma_v$ is contant.
Now
$L=-\sigma_u\cdot{\textbf{N}_u}$, $M=-\sigma_u\cdot{\textbf{N}_v}=-\sigma_v\textbf{N}_u$ and $N=-\sigma_v\cdot{\textbf{N}_v}$ are also constant, ie. $$\textbf{N}_u=cte_1$$ $$\textbf{N}_v=cte_2$$.
Since $d\textbf{N}$ is ortogonal a $\textbf{N}$, the vector $$\textbf{W}=cte_1\frac{du}{ds}+cte_2\frac{dv}{ds}$$ lies the tangent plane in a point $p$ in the surface and the constant direction fixed $u, v.$.
Proof. If $E$ is constant, then $\sigma_u$ is constant, analogue $G$ constant then $\sigma_v$ is constant.
$F$ constant then the angle between $\sigma_u$ and $\sigma_v$ is contant.
Now
$L=-\sigma_u\cdot{\textbf{N}_u}$, $M=-\sigma_u\cdot{\textbf{N}_v}=-\sigma_v\textbf{N}_u$ and $N=-\sigma_v\cdot{\textbf{N}_v}$ are also constant, ie. $$\textbf{N}_u=cte_1$$ $$\textbf{N}_v=cte_2$$.
Therefore
$$\frac{d\textbf{N}}{ds}=\textbf{N}_u\frac{du}{ds}+\textbf{N}_v\frac{dv}{ds}v=cte_1\frac{du}{ds}+cte_2\frac{dv}{ds}.$$
Since $d\textbf{N}$ is ortogonal a $\textbf{N}$, the vector $$\textbf{W}=cte_1\frac{du}{ds}+cte_2\frac{dv}{ds}$$ lies the tangent plane in a point $p$ in the surface and the constant direction fixed $u, v.$.
Then define the surface (Cylinder)
$$\sigma(u, v)=\sigma(u)+v\textbf{W}.$$