|
Exterior
In mathematics, the exterior derivative operator of differential geometry extends the concept of the differential of a function to differential forms of higher degree. more...
Home
ATV Parts
Apparel & Merchandise
Automotive Tools
Aviation Parts
Boat Parts
Car & Truck Parts
Car Audio, Video
Manuals & Literature
Motorcycle Parts
Other Vehicle Parts
Commercial Truck Parts
Go Kart Parts
Other
RV, Trailer & Camper Parts
Engine and Components
Exterior
Interior
Other
Tires and Wheels
Towing Systems
Scooter Parts
Personal Watercraft Parts
Racing Parts
Services & Installation
Snowmobile Parts
Vintage Car & Truck Parts
Wholesale Lots
It is important in the theory of integration on manifolds, and is the differential (coboundary) used to define de Rham and Alexander-Spanier cohomology. Its current form was invented by Élie Cartan.
Definition
The exterior derivative of a differential form of degree k is a differential form of degree k + 1.
For a k-form ω = fI dxI over Rn, the definition is as follows:
-
For general k-forms ΣI fI dxI (where the multi-index I runs over all ordered subsets of {1, ..., n} of cardinality k), we just extend linearly. Note that if i = I above then
Properties
Exterior differentiation satisfies three important properties:
linearity;
the wedge product rule (see antiderivation);
-
and d2 = 0, a formula encoding the equality of mixed partial derivatives, so that always;
-
It can be shown that the exterior derivative is uniquely determined by these properties and its agreement with the differential on 0-forms (functions).
The kernel of d consists of the closed forms, and the image of the exact forms (cf. exact differentials).
The exterior derivative is natural. If f: M → N is a smooth map and Ωk and Ωk+1 are the contravariant smooth functors that assign correspondingly to each manifold the space of k- and k+1-forms on the manifold, then the following diagram commutes
so d(f*ω) = f*dω, where f* denotes the pullback of f. Thus d is a natural transformation from Ωk to Ωk+1.
Invariant formula
Given a k-form ω and arbitrary smooth vector fields V0,V1, …, Vk we have
Read more at Wikipedia.org
|
|