Differential form

Exterior derivative

The exterior derivative generalizes the concept of differential to general differential forms on a 𝐢𝛼-manifold (𝑀,π’œ). For 𝑝 β‰₯0, we have a map

d:Ω𝑝(𝑀)→Ω𝑝+1(𝑀).

Note that to any 0-form, i.e. continuous function 𝑓 βˆˆπΆπ›Ό(𝑀), we can naturally associate a 1-form by the

(d𝑓)π‘Žπ‘£π‘Ž=βˆ‡π‘£π‘“.

The general exterior derivative is then the unique extension of this operation to a graded derivation Ξ©βˆ™(𝑀) β†’Ξ©βˆ™(𝑀) such that d2 =0, i.e. if πœ” βˆˆΞ©π‘(𝑀) and πœ‡ βˆˆΞ©π‘ž(𝑀) we have

d(πœ”βˆ§πœ‡)=dπœ”βˆ§πœ‡+(βˆ’1)π‘πœ”βˆ§dπœ‡.

Local coΓΆrdinates

Let π‘₯ :π‘ˆ β†’β„π‘š be a chart. Then for

πœ”=1𝑝!πœ”πœ‡1β‹―πœ‡π‘dπ‘₯πœ‡1βˆ§β‹―βˆ§dπ‘₯πœ‡π‘

we have

dπœ”=1𝑝!πœ•πœ‡π‘+1πœ”πœ‡1β‹―πœ‡π‘dπ‘₯πœ‡π‘+1∧dπ‘₯πœ‡1βˆ§β‹―βˆ§dπ‘₯πœ‡π‘

This can be seen as a special case of From a covariant derivative.

From a covariant derivative

Let βˆ‡ denote a torsion-free affine connexion on 𝑀. Then for πœ”π‘Ž1β‹―π‘Žπ‘ βˆˆΞ©π‘(𝑀), the covariant derivative gives

(dπœ”)π‘π‘Ž1β‹―π‘Žπ‘=(𝑝+1)βˆ‡[π‘πœ”π‘Ž1β‹―π‘Žπ‘]

which is independent of the choice of βˆ‡.1

See also


develop | en | SemBr

Footnotes

  1. 2009. General relativity, Β§B.1, pp. 428–429. ↩