Differential geometry MOC

Tangent space

The tangent space 𝑇𝑝𝑋 of a differentiable manifold 𝑋 at a point 𝑝 βˆˆπ‘‹ is a vector space corresponding to possible velocities when moving through π‘₯. #m/def/geo/diff A number of equivalent characterizations are useful. See also Tangent map, Tangent bundle.

Intrinsic manifold

The following characterizations of 𝑇𝑝𝑀 are all useful.

As derivations at a point

Let 𝑝 βˆˆπ‘€, and suppose 𝔛(𝑀) is the set of vector fields viewed as derivations. We define the tangent space 𝑇𝑝𝑋 βŠ†β„πΆπ›Ό(𝑀) as the image of the map

𝔛(𝑀)↠𝑇𝑝𝑀𝑣↦𝑣𝑝,

i.e. the set of all derivations evaluated at 𝑝.

Chart-free characterization as velocities

Let 𝑝 βˆˆπ‘€, π‘₯ βˆˆπ’œ be a chart at 𝑝, and

Θ=𝖬𝖺𝗇𝛼‒(((βˆ’πœ–,πœ–),0),(𝑋,π‘₯))

be the set of all 𝐢𝛼 paths πœ” :( βˆ’1,1) →𝑋 such that πœ”(0) =𝑝. We define an equivalence relation ( ∼) on Θ so that two paths πœ”,πœ— ∈Θ are equivalent iff

(π‘₯βˆ˜πœ”)β€²(0)=(π‘₯βˆ˜πœ—)β€²(0)

which is easily shown to be independent of choice of π‘₯.

Via the cotangent space

The cotangent space π‘‡βˆ—π‘π‘€ admits an intrinsic characterization, which is applicable in other (non-differentiable) settings. The tangent space is simply the dual vector space (π‘‡βˆ—π‘π‘€)βˆ—.

Equivalence of characterizations

#missing/proof

Real embedded manifold

Both the following characterizations of the tangent space of a real embedded manifold is useful.

Fixed chart characterization

Let 𝑋 βŠ†β„π‘ be a Real embedded manifold and π‘₯ βˆˆπ‘‹. Let

πœ‘βˆ’1:π‘‰βŠ†β„π‘›β†’π‘ˆβŠ†π‘‹βŠ†β„π‘π‘£β†¦π‘₯

be a local parameterization at π‘₯, and π·πœ‘βˆ’1(𝑣) :ℝ𝑛 →ℝ𝑁 be its Total derivative. Then 𝑇π‘₯𝑋 =π·πœ‘βˆ’1(𝑣)(ℝ𝑛) is the tangent space at π‘₯.

Chart-free characterization as velocities

Let 𝑋 βŠ†β„π‘ be a Real embedded manifold and π‘₯ βˆˆπ‘‹. Let

Ξ©πœ–=π–¬π–Ίπ—‡βˆžβ€’(((βˆ’πœ–,πœ–),0),(𝑋,π‘₯))

be the set of all 𝐢∞ differentiable paths πœ” :( βˆ’πœ–,πœ–) →𝑋 such that πœ”(0) =π‘₯. Then the set of all β€œvelocities at π‘₯”

𝑇π‘₯𝑋={Λ™πœ”(0):πœ”βˆˆΞ©πœ–,πœ–>0}

is the tangent space at π‘₯.

The primary advantage of the fixed chart characterization is that its vector space status is clear, whereas the chart-free characterization is more intuitive and establishes chart-independence.

Equivalence of characterizations

Take a coΓΆrdinate chart πœ‘ :π‘ˆ →𝑉 βŠ†β„π‘› with πœ‘(π‘₯) =𝑣. Let π‘₯ βˆˆπ‘‹ and let 𝑇π‘₯𝑋 denote the fixed-chart characterization and Λœπ‘‡π‘₯𝑋 denote the chart-free characterization.

Let Λ™πœ”(0) βˆˆΛœπ‘‡π‘₯𝑋 for some 𝐢∞ differentiable πœ” :( βˆ’πœ–,πœ–) β†’π‘ˆ with πœ”(0) =π‘₯. Then

π·πœ”(0)=𝐷[πœ‘βˆ’1πœ‘πœ”](0)=π·πœ‘βˆ’1(𝑣)𝐷[πœ‘πœ”](0)βˆˆπ‘‡π‘₯𝑋

Herefore Λœπ‘‡π‘₯𝑋 βŠ†π‘‡π‘₯𝑋.

Now let π·πœ‘βˆ’1(𝑣)(βƒ—πš) βˆˆπ‘‡π‘₯𝑋 for some βƒ—πš βˆˆβ„π‘›. Define

Λœπœ”:(βˆ’πœ–,πœ–)→ℝ𝑛𝑑↦𝑣+π‘‘βƒ—πš

and let πœ” =πœ‘βˆ’1Λœπœ” :( βˆ’πœ–,πœ–) β†’π‘ˆ (we choose πœ– so that πœ” remains in π‘ˆ). It follows Λ™πœ”(0) =𝐷[πœ‘βˆ’1Λœπœ”](0) =π·πœ‘βˆ’1(𝑣)(βƒ—πš) and Λ™πœ”(0) βˆˆΛœπ‘‡π‘₯𝑋. Herefore 𝑇π‘₯𝑋 βŠ†Λœπ‘‡π‘₯𝑋.

Thus 𝑇π‘₯𝑋 =Λœπ‘‡π‘₯𝑋.


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