Differential geometry MOC

Vector field

Let (𝑀,𝒜) be a 𝐶𝛼-manifold. A 𝐶𝛼-vector field formalizes the idea of assigning a vector smoothly to every point in 𝑀. The set of all vector fields on 𝑀 is denoted 𝔛(𝑀), #m/def/geo/diff which forms a module over 𝐶𝛼(𝑀) and thus in particular a (usually infinite-dimensional) vector space over . One can also consider a more general Tensor field. See also Smooth field.

Intrinsic manifold

The following characterizations of vector fields and 𝔛(𝑀) are both useful.

As a section of 𝑇𝑀

A vector field may be characterized as a smooth section of the Tangent bundle 𝑇𝑀, thus

𝔛(𝑀):=Γ𝛼(𝑀,𝑇𝑀).
As a derivation on 𝐶𝛼(𝑀)

A 𝐶𝛼-vector field is a derivation on the algebra of smooth (scalar-valued) functions 𝐶𝛼(𝑀), thus

𝔛(𝑀):=𝔡𝔢𝔯(𝐶𝛼(𝑀)).

The evaluation 𝑣𝑝 of a vector field 𝑣 Vect(𝑀) at a point 𝑝 𝑀 is then the derivation

𝑣𝑝:𝐶𝛼(𝑀)𝑓𝑣(𝑓)(𝑝)

which gives a map 𝔛(𝑀) Γ(𝑇𝑀).

Equivalence of charactrerizations

#missing/proof

When we wish to emphasize the latter view, we write 𝑣 for the derivation corresponding to 𝑣 𝔛(𝑀).

Euclidean space

A vector field 𝐅 is a function assigning a vector to every point in space

𝐅:𝔼𝑛𝑛

Importantly, the domain represents Euclidean space whereas the codomain represents vectors in the physical sense of directional quantities (tangent space). There may also be a time dependence, which is treated separately.

Two special kinds of field are

However, any vector field can be decomposed into conservative and incompressible parts, so that for any field there exists 𝑉 and Ψ such that1

𝐅=𝑉+×𝚿

This is due to the Helmholtz theorem, and is consequently called the Helmholtz decomposition.


#state/tidy | #lang/en | #SemBr

Footnotes

  1. 2013. Introduction to electrodynamics, p. 54 (eqn. 1.105)