What is the general formula for the Area of a 2-D surface in a 3-D manifold? Suppose we have a flat 3-D manifold $ ds^2=\delta_{ab}dx^{a}dx^{b},$ which contains a 2-D surface given by a parametric relationship $r^{a}\left(u,v\right)=x^{a}\left(u,v\right).$ Where $ u $ and $ v $ are two independent parameters.
I know that the Area of this surface is the magnitude of a 3-D vector
$$
dA_{a}=\varepsilon_{abc}\dfrac{\partial x^{b}}{\partial u}\dfrac{\partial x^{c}}{\partial v} du dv
$$
$$dA^2=\delta^{ef}dA_{e}dA_{f}$$
How can I generalize this formula to an arbitrary 3-D manifold given by $ ds^2=g_{ab}dx^{a}dx^{b}$, where:
$$
dA^2=g^{ab}dA_{b}dA_{a}?
$$
That is, is it possible to write
$$
dA_{a}=\kappa_{abc}\dfrac{\partial x^{b}}{\partial u}\dfrac{\partial x^{c}}{\partial v} du dv
$$
and, if so, what is $\kappa_{abc}$ ?
 A: @Solenodon Paradoxus may be has answered your question already. But let me do it in more detail. 
Suppose we have a 3-dim manifold $\mathfrak{M}_3$ with metric function $g_{\alpha\beta}$. Note that manifolds does not contain any vectors itself. Vectors emerges in tangent spaces. But we will not be so specific. So we will say that $\mathfrak{M}_3$ contains vectors, metric and etc. bearing in mind that this elements belong to its ($\mathfrak{M}_3$'s) tangent space. OK. Let us suppose also we have 2-dim manifold say $\mathfrak{M}_2\in\mathfrak{M}_3$. But $\mathfrak{M}_2$ can be considered individually with its own metric say $G_{\mu\nu}$. So you are asking the following question:
How do I know $G_{\mu\nu}$ if I know $g_{\alpha\beta}$?
Suppose $\mathfrak{M}_2$ represents some surface $M_2$ in your space. Or like you say $\mathfrak{M}_2$ can be parametrized by two variables $u, v$ (in the rest we will call it $u^1$ and $u^2$) in the following way:
$$x_1 = x_1(u^1, u^2),\, x_2 = x_2(u^1, u^2),\,x_3 = x_3(u^1, u^2);$$
If we planed to calculate arc length $ds^2$ on our surface $M_2$ we could do it absolutely in the same way as we would do if this arc belonged $\mathfrak{M}_3$ but with the only specialty: $\vec{x}$ is a function of $u$ nd $v$. Let's do this.
$$ds^2 = g_{\alpha\beta}(u^1,u^2)dx^\alpha(u^1, u^2) dx^\beta(u^1, u^2) = g_{\alpha\beta}\frac{dx^\alpha}{du^\mu}\frac{dx^\beta}{du^\nu}du^\mu du^\nu$$ 
But on the other hand 
$$ds^2 = G_{\mu\nu}du^\mu du^\nu$$
So we have eventually 
$$G_{\mu\nu} = g_{\alpha\beta}\frac{dx^\alpha}{du^\mu}\frac{dx^\beta}{du^\nu}$$
A: Given an embedding of smooth differentiable manifolds $M \rightarrow N$, it is always possible to pull-back covariant tensors from $N$ to $M$. In physicist's notation:
$$ A_{\mu \nu \dots} (x) = \frac{\partial y^{\alpha}}{\partial x^{\mu}} \frac{\partial y^{\beta}}{\partial x^{\nu}} A_{\alpha \beta \dots} (y(x)). $$
To answer your question: pull back the 3D metric to obtain a 2D induced metric on the surface. In your case $\mu, \nu, \dots$ range through $\{1, 2\}$ and $\alpha, \beta, \dots$ range through $\{1, 2, 3\}$. Integrate the volume form of the induced metric over the surface:
$$ \text{Area} = \int d^2 x \sqrt{\det g_{\text{induced}}}. $$
