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Tangent vector

Vector tangent to a curve or surface at a given point

In mathematics, a tangent vector is a vector that is tangent to a curve or surface at a given point. Tangent vectors are described in the differential geometry of curves in the context of curves in Rn. More generally, tangent vectors are elements of a tangent space of a differentiable manifold. Tangent vectors can also be described in terms of germs. Formally, a tangent vector at the point x is a linear derivation of the algebra defined by the set of germs at x.

01Motivation

Before proceeding to a general definition of the tangent vector, we discuss its use in calculus and its tensor properties.

Calculus

Let \mathbf {r} (t) be a parametric smooth curve. The tangent vector is given by \mathbf {r} '(t) provided it exists and provided \mathbf {r} '(t)\neq \mathbf {0}, where we have used a prime instead of the usual dot to indicate differentiation with respect to parameter t. The unit tangent vector is given by \mathbf {T} (t)={\frac {\mathbf {r} '(t)}{|\mathbf {r} '(t)|}}\,.

Example

Given the curve \mathbf {r} (t)=\left\{\left(1+t^{2},e^{2t},\cos {t}\right)\mid t\in \mathbb {R} \right\} in \mathbb {R} ^{3}, the unit tangent vector at t=0 is given by \mathbf {T} (0)={\frac {\mathbf {r} '(0)}{\|\mathbf {r} '(0)\|}}=\left.{\frac {(2t,2e^{2t},-\sin {t})}{\sqrt {4t^{2}+4e^{4t}+\sin ^{2}{t}}}}\right|_{t=0}=(0,1,0)\,. Where the components of the tangent vector are found by taking the derivative of each corresponding component of the curve with respect to t.

Contravariance

If \mathbf {r} (t) is given parametrically in the n-dimensional coordinate system xi (here we have used superscripts as an index instead of the usual subscript) by \mathbf {r} (t)=(x^{1}(t),x^{2}(t),\ldots ,x^{n}(t)) or \mathbf {r} =x^{i}=x^{i}(t),\quad a\leq t\leq b\,, then the tangent vector field \mathbf {T} =T^{i} is given by T^{i}={\frac {dx^{i}}{dt}}\,. Under a change of coordinates u^{i}=u^{i}(x^{1},x^{2},\ldots ,x^{n}),\quad 1\leq i\leq n the tangent vector {\bar {\mathbf {T} }}={\bar {T}}^{i} in the ui-coordinate system is given by {\bar {T}}^{i}={\frac {du^{i}}{dt}}={\frac {\partial u^{i}}{\partial x^{s}}}{\frac {dx^{s}}{dt}}=T^{s}{\frac {\partial u^{i}}{\partial x^{s}}} where we have used the Einstein summation convention. Therefore, a tangent vector of a smooth curve will transform as a contravariant tensor of order one under a change of coordinates.

02Definition

Let f:\mathbb {R} ^{n}\to \mathbb {R} be a differentiable function and let \mathbf {v} be a vector in \mathbb {R} ^{n}. We define the directional derivative in the \mathbf {v} direction at a point \mathbf {x} \in \mathbb {R} ^{n} by \nabla _{\mathbf {v} }f(\mathbf {x} )=\left.{\frac {d}{dt}}f(\mathbf {x} +t\mathbf {v} )\right|_{t=0}=\sum _{i=1}^{n}v_{i}{\frac {\partial f}{\partial x_{i}}}(\mathbf {x} )\,. The tangent vector at the point \mathbf {x} may then be defined as \mathbf {v} (f(\mathbf {x} ))\equiv (\nabla _{\mathbf {v} }(f))(\mathbf {x} )\,.

03Properties

Let f,g:\mathbb {R} ^{n}\to \mathbb {R} be differentiable functions, let \mathbf {v} ,\mathbf {w} be tangent vectors in \mathbb {R} ^{n} at \mathbf {x} \in \mathbb {R} ^{n}, and let a,b\in \mathbb {R}. Then

  1. (a\mathbf {v} +b\mathbf {w} )(f)=a\mathbf {v} (f)+b\mathbf {w} (f)
  2. \mathbf {v} (af+bg)=a\mathbf {v} (f)+b\mathbf {v} (g)
  3. \mathbf {v} (fg)=f(\mathbf {x} )\mathbf {v} (g)+g(\mathbf {x} )\mathbf {v} (f)\,.

04Tangent vector on manifolds

Let M be a differentiable manifold and let A(M) be the algebra of real-valued differentiable functions on M. Then the tangent vector to M at a point x in the manifold is given by the derivation D_{v}:A(M)\rightarrow \mathbb {R} which shall be linear , i.e., for any f,g\in A(M) and a,b\in \mathbb {R} we have

D_{v}(af+bg)=aD_{v}(f)+bD_{v}(g)\,.

Note that the derivation will by definition have the Leibniz property

D_{v}(f\cdot g)(x)=D_{v}(f)(x)\cdot g(x)+f(x)\cdot D_{v}(g)(x)\,.
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Sources and credits

This article is adapted from the Wikipedia article Tangent vector, written by its contributors and licensed under CC BY-SA 4.0. Fathomly has changed the layout, removed citation markers, navigation and maintenance notices, and adjusted punctuation. This adapted version is shared under the same license. For references, see the original article.

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