Tangent space: Difference between revisions

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==Definition==
==Definition==


Although it is tempting to define a tangent space as a "space where tangent vectors live", without a definition of a tangent space there is no definition of a tangent vector. Instead, one can define the tangent space in terms of ''directional derivatives'', and that the space <math>T_pM</math> is the space identified with directional derivatives of curves through p.
Although it is tempting to define a tangent space as a "space where tangent vectors live", without a definition of a tangent space there is no definition of a tangent vector. There are various ways in which a tangent space can be defined, the most intuitive of which is in terms of ''directional derivatives''; the space <math>T_pM</math> is the space identified with directional derivatives at p.


===Directional derivative===
===Directional derivative===


A ''curve'' on the manifold is defined as a [[differentiable]] map <math>\scriptstyle \gamma: (a,b) \rightarrow M</math>. Let <math>\scriptstyle \gamma(t_0) \, = \, p</math>. If one defines <math>\scriptstyle \mathcal{F}_p</math> to be all the functions <math>\scriptstyle f:M \rightarrow \mathbb{R}^n</math> that are differentiable at the point p, then one can interpret <math>\scriptstyle \gamma'(t_0): \, \mathcal{F}_p \rightarrow \mathbb{R}</math> to be an operator such that
A ''curve'' on the manifold is defined as a [[differentiable]] map <math>\scriptstyle \gamma: (a,b) \rightarrow M</math>. Let <math>\scriptstyle \gamma(t_0) \, = \, p</math>. If one defines <math>\scriptstyle \mathcal{F}_p</math> to be all the functions <math>\scriptstyle f:M \rightarrow \mathbb{R}^n</math> that are differentiable at the point p, then one can interpret  
:<math> \gamma'(t_0)(f) = (f \circ \gamma)'(t_0)   </math>
:<math>\gamma'(t_0): \, \mathcal{F}_p \rightarrow \mathbb{R}</math>
to be an operator such that
:<math> \gamma'(t_0)(f) = (f \circ \gamma)'(t_0) = \lim_{h \rightarrow 0} \frac{f(\gamma(t_0+h)) - f(\gamma(t_0))}{h}  </math>
and is a '''directional derivative''' of f in the direction of the curve <math>\scriptstyle \gamma</math>. This operator can be interpreted as a ''tangent vector''.
 
The tangent space is then the set of all directional derivatives of curves at the point p.
 
 
 
 
 


[[category:CZ Live]]
[[category:CZ Live]]
[[category:Mathematics Workgroup]]
[[category:Mathematics Workgroup]]

Revision as of 18:32, 21 July 2007

The tangent space of a differentiable manifold M is a vector space at a point p on the manifold whose elements are the tangent vectors (or velocities) to the curves passing through that point p. The tangent space at this point p is usually denoted .

The tangent space is necessary for a manifold because it offers a way in which tangent vectors at different points on the manifold can be compared (via an affine connection). If the manifold is a submanifold of , then the tangent space at a point can be thought of as an n-dimensional hyperplane at that point. However, this ambient Euclidean space is unnecessary to the definition of the tangent space.

The tangent space at a point has the same dimension as the manifold, and the union of all the tangent spaces of a manifold is called the tangent bundle, which itself is a manifold of twice the dimension of M.

Definition

Although it is tempting to define a tangent space as a "space where tangent vectors live", without a definition of a tangent space there is no definition of a tangent vector. There are various ways in which a tangent space can be defined, the most intuitive of which is in terms of directional derivatives; the space is the space identified with directional derivatives at p.

Directional derivative

A curve on the manifold is defined as a differentiable map . Let . If one defines to be all the functions that are differentiable at the point p, then one can interpret

to be an operator such that

and is a directional derivative of f in the direction of the curve . This operator can be interpreted as a tangent vector.

The tangent space is then the set of all directional derivatives of curves at the point p.