I've recently started studying differential forms and have been looking at differential forms. I'm struggling to understand the motivation for introducing the notion of the wedge product. Does it simply arise when generalising the notion of a "signed area/volume" in higher dimensional spaces, or is there a deeper reasoning behind it?
If it is just a generalisation of a "signed area/volume" in higher dimensional spaces then my understanding is that the "area" spanned by two tangent vectors $X,Y$ is given by the wedge product between their associated differential forms. Thus, in one-dimension, if we have a one-form $\omega$ expressed in a local coordinate basis as $\omega =f_{i}(x)dx^{i}$, then $$\omega\wedge\omega = f_{i}(x)f_{j}(x)dx^{i}\wedge dx^{j}$$ and so from this, if X=Y, then the "area" spanned by them should be zero and so, $$\omega\wedge\omega (X,X)=0=f_{i}(x)f_{j}(x)dx^{i}(X)\wedge dx^{j}(X)\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\\ \quad\;\;=\frac{1}{2}\left[f_{i}(x)f_{j}(x)dx^{i}(X)\wedge dx^{j}(X)+f_{j}(x)f_{i}(x)dx^{j}(X)\wedge dx^{i}(X)\right]$$ and this implies that $$dx^{i}(X)\wedge dx^{j}(X)=-dx^{j}(X)\wedge dx^{i}(X)$$ I'm unsure whether my understanding here is correct or not?