By definition of the inverse image, $f^{-1}(p) = \{(x,y,z) : f(x,y,z) = p\}$, so $f(x,y,z) - p = 0$. Now, since p is a regular value, it means that one of its partial derivatives is nonzero. Without loss of generality, we can assume that the partial derivative with respect to z is nonzero.
And by the implicit function theorem, there exists $\phi: U \subset \mathbb{R}^2 \rightarrow \mathbb{R}^3$ such that $\phi(u,v) = (u,v,h(u,v))$, where h(u,v) is a local parameterization at a point.
If we consider the composition $f \circ \phi = f(u,v,h(u,v)) = p$,
Now, differentiating partially with respect to u and using the chain rule $f \circ \phi$ , we obtain
$\frac{\partial h}{\partial u} = \frac{-\frac{\partial f}{\partial x}}{\frac{\partial f}{\partial z}}$
and
$\frac{\partial h}{\partial v} = \frac{-\frac{\partial f}{\partial y}}{\frac{\partial f}{\partial z}}$
and if I do the partial derivative of $\phi$
$\frac{\partial \phi}{\partial u} = (1,0,\frac{\partial h}{\partial u}) = (1,0,\frac{-\frac{\partial f}{\partial x}}{\frac{\partial f}{\partial z}})$
and
$\frac{\partial \phi}{\partial v} = (0,1,\frac{\partial h}{\partial v}) = (0,1,\frac{-\frac{\partial f}{\partial y}}{\frac{\partial f}{\partial z}})$
And the coefficients would be equal to
$E = \langle \frac{\partial \phi}{\partial u} \cdot \frac{\partial \phi}{\partial u} \rangle = 1 + \left(\frac{-\frac{\partial f}{\partial x}}{\frac{\partial f}{\partial z}}\right)^2$
$F = \langle \frac{\partial \phi}{\partial u} \cdot \frac{\partial \phi}{\partial v} \rangle = \frac{\frac{\partial f}{\partial x}}{\frac{\partial f}{\partial z}} \cdot \frac{\frac{\partial f}{\partial y}}{\frac{\partial f}{\partial z}}$
$G = \langle \frac{\partial \phi}{\partial v} \cdot \frac{\partial \phi}{\partial v} \rangle = 1 + \left(\frac{-\frac{\partial f}{\partial y}}{\frac{\partial f}{\partial z}}\right)^2$