There is a beautiful generalization. We will define something called a k-dimensional parametrized-manifold in R^n, that is analogous to say, a 2-dimensional parametrized-surface in R^3.
Here is the definition of a parametrized-manifold:
Let k <= n. Let A be open in R^k, and let g: A ---> R^n be a map of class C^r. The set Y = g(A), together with the map g, constitute what is called a parametrized-manifold of dimension k. We denote this parametrized-manifold by Y_g; and we define the k-dimensional volume of Y_g by the equation [tex]v(Y_g) = \int_A V(Dg)[/tex], provided the integral exists.
Here, Dg is the derivative of g, and [tex]V(Dg) = \sqrt{det[Dg^{tr}Dg]}[/tex].
Note that if f is a continuous map from Y_g to R then the integral of f over Y_g, with respect to volume, is defined by [tex]\int_{Y_g} f dV = \int_A (f \circ g) V(Dg)[/tex]
We use the notation dV in the integral to denote integral with respect to volumeEDIT: Also note that [tex]Dg^{tr}Dg [/tex[ is <b> always </b> a square matrix, so taking the determinant of it is never a problem.[/tex]