let : $$\frac{\partial f}{\partial x}=f _{x}\,,\qquad\frac{\partial f}{\partial t}=f _{t}\,,\qquad\frac{\partial}{\partial t}\frac{\partial f}{\partial x}=f_{tx}\,,\qquad\frac{\partial}{\partial x}\frac{\partial f}{\partial x}=f_{xx} $$ And: $\,f=f(x,t)$
We have the PDE : $$\left(1-2\hspace{0.3ex}f_{x}^{2}\right)f_{t}\hspace{0.5ex}f_{xx}+2\hspace{0.3ex}f_{x}\hspace{0.4ex}f_{tx}\left(1+f_{x}^{2}\right)=0$$ Which can be written as : $$\big(2\hspace{0.3ex}f_{x}\hspace{0.3ex}f_{tx}+f_{t}\hspace{0.4ex}f_{xx}\big) \big(1+f_{x}^{2}\big)=3\hspace{0.3ex}f_{x}^{2\hspace{0.2ex}}f_{t}\hspace{0.4ex}f_{xx}$$ And we have the Dirchlet boundary data : $$ f(x,t_{i})=g_{i}(x)\;,\;\;f(x,t_{j})=g_{j}(x)$$
I am having a hard time trying to solve the problem. Any help is highly appreciated.
$$(1-2f_x^2)f_tf_{xx}+2f_xf_{tx}(1+f_x^2)=0$$ This is a second order non-linear PDE.
Below, it is shown how to reduce it to the first order. Of course this is far to be the full solving, but I hope that it will help.
$$\frac{(1-2f_x^2)f_{xx}}{(1+f_x^2)f_x}+2\frac{f_{tx}}{f_t}=0$$ $\begin{cases} \frac{(1-2f_x^2)f_{xx}}{(1+f_x^2)f_x}=\frac{\partial}{\partial x}\left(\ln|f_x|-\frac{3}{2}\ln|1+f_x^2| \right)\\ \frac{f_{tx}}{f_t}=\frac{\partial}{\partial x}\left(\ln|f_t| \right) \end{cases} \quad\to\quad \frac{\partial}{\partial x}\left(\ln|f_x|-\frac{3}{2}\ln|1+f_x^2| +2\ln|f_t|\right)=0$
$$\frac{\partial}{\partial x}\left(\ln\left(\frac{f_x^2f_t^4}{(1+f_x^2)^3} \right)\right)=0$$ $\frac{f_x^2f_t^4}{(1+f_x^2)^3}=$ function of $t$ only.
$$(1+f_x^2)^3-f_x^2f_t^4 \varphi(t)=0 \quad \text{any function }\varphi(t)$$ This is a first order non-linear PDE.
Another simplification can be done :
Change of variable $\theta=\int \varphi(t)^{-1/4}dt \quad\to\quad dt=\varphi(t)^{1/4}d\theta \quad\to\quad f_\theta=f_t \: \varphi(t)^{1/4}$ $$(1+f_x^2)^3-f_x^2f_\theta^4 =0$$ where the unknown function is $f(x,\theta)$
Since $\varphi(t)$ is any function of $t$ then $\theta(t)$ is any function of $t$. So, one can forget the intermediate notation $\varphi$.
$f(x,t)=f\left(x,\theta(t)\right) \quad$ any function $\theta(t)$. This is consistent with the judicious comment of Andrew.