Dual frame in Riemannian metrics. Suppose that we have a Riemannian metric $ds^2=Edu^2+2Fdudv+Gdv^2$ on a local coordinate neighborhood $(U;(u,v))$ prove that for the following vector fields:
$$e_{1}=\frac{1}{\sqrt{E}}\frac{\partial}{\partial u},\quad e_{2}=\frac{-1}{\sqrt{EG-F^2}}\left(\frac{F}{\sqrt{E}}\frac{\partial}{\partial u}-\sqrt{E}\frac{\partial}{\partial v}\right)$$
The $1-$forms:
$$\omega_1=\sqrt{E}\left(du+\frac{F}{E}dv\right),\quad \omega_2=\sqrt{\frac{EG-F^2}{E}}dv$$ 
satisfies:
$$\omega_i(e_k)=\delta_{ik}$$
My work: Let $p(u,v)$ a differentiable function, I think that I must show fisrtly that $\omega_1(e_1(p))=p$, i.e. $\omega_1(e_1)=1$ the identity function. 
$$\omega_1\left(\tfrac{1}{\sqrt{E}}\tfrac{\partial}{\partial u}(p)\right)=\tfrac{1}{\sqrt{E}}\tfrac{\partial}{\partial u}(\omega_1(p))$$
I do this beacuse an $1-form$ $\alpha$ is such that $\alpha(fX)=f\alpha(X)$. Then It is correct that
$\omega_1(p)=\sqrt{E}\left(pdu+\frac{F}{E}pdv\right)?$
and then apply the partial derivative, my problem is that I don't know ho operate the $1$-form. Anyone can guide me in how can I reach the result or a explicit form to operate with $\omega_1$ and $\omega_2$?
I'm using the book "Umehara, differential geometry of surfaces".
 A: I think you can do this by direct calculation. Fix $p\in U$. If $X_p\in TU_p$, then $X_p=a\partial_u+b\partial_v$ for some $a,b\in \mathbb R$, and by definition of the $1-$forms $du$ and $dv$, we have $du(X_p)=a$ and $dv(X_p)=b$. Now, apply this to the tangent vectors $e_1$ and $e_2$:
$\omega_1(e_1)=\sqrt{E}\left(du+\frac{F}{E}dv\right)\frac{1}{\sqrt{E}}\frac{\partial}{\partial u}=\sqrt E\frac{1}{\sqrt E}(\partial_uu)=\frac{\sqrt E}{\sqrt E}=1$
Similarly,
$\omega_1(e_2)=\sqrt{E}\left(du+\frac{F}{E}dv\right)\left(\frac{-1}{\sqrt{EG-F^2}}\left(\frac{F}{\sqrt{E}}\frac{\partial}{\partial u}-\sqrt{E}\frac{\partial}{\partial v}\right)\right )=-\frac{\sqrt E}{\sqrt{EG-F^2}}\left (\frac{F}{\sqrt E}-\frac{F\sqrt E}{E}\right )=0.$
$\omega_2(e_1)=\sqrt{\frac{EG-F^2}{E}}dv\left(\frac{1}{\sqrt{E}}\frac{\partial}{\partial u} \right)=\sqrt{\frac{EG-F^2}{E^2}}\partial_u v=0$
and
$\omega_2(e_2)=\sqrt{\frac{EG-F^2}{E}}dv\left(\frac{-1}{\sqrt{EG-F^2}}\left(\frac{F}{\sqrt{E}}\frac{\partial}{\partial u}-\sqrt{E}\frac{\partial}{\partial v}\right)\right)=\left(\sqrt{\frac{EG-F^2}{E}}\right)\cdot \left(\frac{\sqrt E}{\sqrt{EG-F^2}}\right)=1$
A: Note that $e_i$ is an orthonormal vector fields wrt $ds^2$. Hence we let $
\omega_i=ds^2(e_i,\cdot)$ which is dual frame. 
