A form-field of rank n is an operator that takes n vector fields to a real-valued function on the manifold. A one-form field takes a single vector field.
We can extract the components function for a form, given a coordinate system.
To get the elements of a coordinate basis for the 1-form fields:
Given component functions defined on manifold points and a 1-form basis, to produce the 1-form field as a linear combination.
Now we transition to wedge.
Higher rank forms can be constructed from 1forms by wedging them together. This antisymmetric tensor product is computed as a determinant. The purpose of this is to allow us to use the construction dx^dy to compute the area described by the vectors that are given to it.
One-form fields multiply by [[wedge]].
Alternative definition in terms of alternation.
A form field is a function of a place and a number of vector fields. The exterior derivative of this form field is a derivative of the form with respect to the place, removing any dependence on place of the vector fields.
Consider w(v)(x), where b is the coefficient function for w in coordinates X:
v1(w(v2))(x) - v2(w(v1))(x) = v1(b v2(X))(x) - v2(b v1(X))(x) = v1(b)(x) v2(X)(x) + b(x) v1(v2(X))(x)
We define exterior derivative as follows:
dw(v1, v2)(x) = v1(b)(x) v2(X)(x) - v2(b)(x) v1(X)(x) = v1(w(v2))(x) - v2(w(v1))(x) - w([v1, v2])(x)
It is not obvious that this is equivalent to the standard definition. See page 91 in Spivak.
Another way to think about this is that if we were able to define constant vector fields (v1_bar, v2_bar) that have constant coefficient functions equal to the value of the coefficient function at the point, then dw(v1, v2)(x) would be just v1_bar(w(v2_bar))(x) - v2_bar(w(v1_bar))(x).
This definition is a generalization to k-forms, by recursion on the vector argument list.
The test for k<n is best if the n is the dimension of the manifold under study. However, if the manifold is embedded in a higher dimensional manifold n will be the dimension of the bigger manifold, making this test less effective (cutting off fewer branches).
Formula is from Spivak Vol. 1 p289.
NOTE: This is an excessively complicated program. Another, more elementary program would, for a k-form, extract the cofficient functions relative to a literal basis, by applying it to the basis vectors, do the derivatives of the coefficients, to make one forms, and form the sum of the wedges of the new 1-forms with the wedges of the corresponding dual basis elements.