On a MM, the exterior derivative is the unique family of R\mathbb R-linear maps

d:Ωk(M)→Ωk+1(M)(k≥0)d:\Omega^k(M)\to \Omega^{k+1}(M)\qquad (k\ge 0)

satisfying the following axioms:

  1. (On functions) If f∈Ω0(M)=C∞(M)f\in\Omega^0(M)=C^\infty(M), then dfdf is the usual differential (a 1-form) given by dfp(v)=v(f)df_p(v)=v(f).
  2. (Graded Leibniz rule) For α∈Ωk(M)\alpha\in\Omega^k(M) and β∈Ωℓ(M)\beta\in\Omega^\ell(M),
    d(α∧β)=dα∧β+(−1)k α∧dβ.d(\alpha\wedge\beta)=d\alpha\wedge\beta + (-1)^k\,\alpha\wedge d\beta.
  3. (Nilpotence) d∘d=0d\circ d = 0.
Naturality

A key naturality property is that for any F:M→NF:M\to N, the satisfies

F∗(dω)=d(F∗ω)F^*(d\omega)=d(F^*\omega)

for every ω∈Ωk(N)\omega\in\Omega^k(N).

The notions of and forms are defined using dd, and their quotient defines the .

Local coordinate formula

In a coordinate chart (x1,…,xn)(x^1,\dots,x^n), write a kk-form as

α=∑IaI dxi1∧⋯∧dxik,\alpha=\sum_{I} a_I\, dx^{i_1}\wedge\cdots\wedge dx^{i_k},

where I=(i1<⋯<ik)I=(i_1<\cdots<i_k) and aIa_I are smooth functions. Then

dα=∑I∑j=1n∂aI∂xj dxj∧dxi1∧⋯∧dxik.d\alpha=\sum_I \sum_{j=1}^n \frac{\partial a_I}{\partial x^j}\, dx^j \wedge dx^{i_1}\wedge\cdots\wedge dx^{i_k}.
Examples
  1. A function on R2\mathbb{R}^2. For f(x,y)f(x,y), the exterior derivative is
    df=∂f∂x dx+∂f∂y dy.df = \frac{\partial f}{\partial x}\,dx + \frac{\partial f}{\partial y}\,dy.
  1. A 1-form on R2\mathbb{R}^2. Let α=P(x,y) dx+Q(x,y) dy\alpha = P(x,y)\,dx + Q(x,y)\,dy. Then
    dα=(∂Q∂x−∂P∂y) dx∧dy.d\alpha = \left(\frac{\partial Q}{\partial x}-\frac{\partial P}{\partial y}\right)\,dx\wedge dy.
  1. A 2-form on R3\mathbb{R}^3. If ω=f(x,y,z) dx∧dy\omega = f(x,y,z)\,dx\wedge dy, then
    dω=df∧dx∧dy=∂f∂z dz∧dx∧dy,d\omega = df\wedge dx\wedge dy = \frac{\partial f}{\partial z}\,dz\wedge dx\wedge dy,
    since the terms involving dx∧dxdx\wedge dx and dy∧dydy\wedge dy vanish by alternation.