Limit definition of the exterior derivative In most treatments of differential geometry, the exterior derivative is defined in a purely algebraic fashion, as map on the exterior algebra of a manifold satisfying certain properties, from which one can show it is well defined and unique.
I am curious if there is any way to define the exterior derivative as a limit. I am mainly interested in this, since "limit definitions" usually carry more geometric meaning than algebraic definitions. Case in point, one could define the Lie derivative $\mathcal{L}_X$ as the unique derivation of the tensor algebra satisfying $\mathcal{L}_Xf=Xf$ and $\mathcal{L}_XY=[X,Y]$ and that it commutes with contractions, however the definition $$\mathcal{L}_XT=\lim_{t\rightarrow 0}\frac{(\phi^X_{t})^*T-T}{t}$$ is far more enlightening in terms of geometric meaning.
Question: Is there any way to define the exterior derivative of a differential form as a limit?
 A: I don't have time to write out the details, but if $\omega$ is a $k$-form, you can write out a formula for $d\omega(v_1,\dots,v_{k+1})$ as a limit of integrals of $\omega$ over boundaries of smaller and smaller $(k+1)$-dimensional parallelepipeds determined by the $v_i$'s. For example, since $d\omega(v_1,\dots,v_{k+1})$ depends only on the values of the $v_i$'s at one point, you could extend the $v_i$'s to commuting vector fields and then define the parallelpiped using their flows. 
A: Here's Jack Lee's argument applied to the exterior derivative of a $1$-form. The argument extends easily to $k$-forms.
First, recall that the fundamental theorem of calculus (or line integrals) says
$$
  \int_{t=a}^{t=b} \langle c'(t), df(c(t))\rangle\,dt = f(c(b)) - f(c(a)).
$$
Given $p \in M$ and $v_1, v_2 \in T_pM$, Let $\Phi: E \rightarrow M$ satisfy $\Phi(0,0) = p$, where $R = [0,\delta]\times [0,\delta]$, $\partial_1\Phi(0,0) = v_1$, and $\partial\Phi_2(0,0) = v_2$. Given a $1$-form $\theta$, consider the line integral
\begin{align*}
  \int_{\partial R} \theta
  &= \int_{x^1=0}^{x^1=\delta} \langle \partial_1, \theta(x^1,0)\rangle\,dx^1
  + \int_{x^2=\delta}^{x^2=0} \langle \partial_2, \theta(\delta,x^2)\rangle\,dx^2\\
  &\quad+ \int_{x^1=\delta}^{x^1=0} \langle \partial_1, \theta(x^1,\delta)\rangle\,dx^1
  + \int_{x^2=\delta}^{x^2=0} \langle \partial_2, \theta(0,x^2)\rangle\,dx^2\\
  &=\int_{x^2=0}^{x^2=\delta} \langle \partial_2,\theta(\delta,x^2) - \theta(0,x^2)\rangle\,dx^2\\
  &\quad- \int_{x^1=0}^{x^1=\delta} \langle \partial_1, \theta(x^1,\delta) - \theta(x^1,0)\rangle\,dx^1\\
  &=\int_{x^2=0}^{x^2=\delta} \int_{x^1=0}^{x^1=\delta}
    \langle \partial_1, d\langle \partial_2, \theta(x^1,x^2)\rangle\rangle\,dx^1\,dx^2\\
  &\quad
    - \int_{x^1=0}^{x^1=\delta} \int_{x^2=0}^{x=\delta}
    \langle \partial_2, d\langle \partial_1, \theta(x^1,x^2)\rangle\rangle\,dx^2\,dx^1\\
  &=\int_{x^2=0}^{x^2=\delta} \int_{x^1=0}^{x^1=\delta}
    \langle \partial_1, d\langle \partial_2, \theta(x^1,x^2)\rangle\rangle
    - \langle \partial_2, d\langle \partial_1, \theta(x^1,x^2)\rangle\rangle\,dx^1\,dx^2.
\end{align*}
Therefore,
\begin{align*}
  \lim_{\delta\rightarrow 0}  \frac{1}{\delta^2}\int_{\partial R} \theta
  &= \langle \partial_1, d\langle \partial_2, \theta\rangle\rangle
  - \langle \partial_2, d\langle \partial_1, \theta\rangle\rangle\\
& = \langle \partial_1\otimes\partial_1,d\theta\rangle\\
  &= \langle v_1\otimes v_2,d\theta\rangle.
\end{align*}
