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All tangent vectors in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220091.png" /> arise in this way. Identifying the vector (a2) with the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220092.png" />-vector <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220093.png" />, viewed as a directed line segment starting in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220094.png" />, one recovers the intuitive picture of the tangent space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220095.png" /> as the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220096.png" />-plane in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220097.png" /> tangent to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220098.png" /> in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220099.png" />.
 
All tangent vectors in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220091.png" /> arise in this way. Identifying the vector (a2) with the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220092.png" />-vector <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220093.png" />, viewed as a directed line segment starting in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220094.png" />, one recovers the intuitive picture of the tangent space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220095.png" /> as the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220096.png" />-plane in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220097.png" /> tangent to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220098.png" /> in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t09220099.png" />.
  
A vector field on a manifold <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200100.png" /> can be defined as a derivation (cf. [[Derivation in a ring|Derivation in a ring]]) in the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200101.png" />-algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200102.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200103.png" />. Composition with the evaluation mappings <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200104.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200105.png" />, yields a family of tangent vectors <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200106.png" />, so that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200107.png" /> "becomes" a section of the [[Tangent bundle|tangent bundle]]. Given local coordinates <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200108.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200109.png" /> can locally be written as
+
A vector field on a manifold <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200100.png" /> can be defined as a derivation (cf. [[Derivation in a ring|Derivation in a ring]]) in the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200101.png" />-algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200102.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200103.png" />. Composition with the evaluation mappings <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200104.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200105.png" />, yields a family of tangent vectors <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200106.png" />, so that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200107.png" /> "becomes" a section of the [[Tangent bundle|tangent bundle]]. Given local coordinates <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200108.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200109.png" /> can locally be written as
  
 
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200110.png" /></td> </tr></table>
 
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200110.png" /></td> </tr></table>
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<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200114.png" /></td> </tr></table>
 
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200114.png" /></td> </tr></table>
  
showing once more the convenience of the " / x" notation for tangent vectors. (Of course, in practice one uses a bit more abuse of notation and writes <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200115.png" /> instead of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200116.png" />.)
+
showing once more the convenience of the " / x" notation for tangent vectors. (Of course, in practice one uses a bit more abuse of notation and writes <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200115.png" /> instead of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200116.png" />.)
  
Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200117.png" /> be the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200118.png" />-algebra of germs of smooth functions at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200119.png" /> (cf. [[Germ|Germ]]). Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200120.png" /> be the ideal of germs that vanish at zero, and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200121.png" /> the ideal generated by all products <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200122.png" /> for <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200123.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200124.png" /> are local coordinates at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200125.png" /> so that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200126.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200127.png" /> is generated as an ideal in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200128.png" /> by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200129.png" />, and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200130.png" /> by the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200131.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200132.png" />. In fact, the quotient ring <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200133.png" /> is the power series ring in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200134.png" /> variables over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200135.png" />. Here <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200136.png" /> is the ideal of flat function germs. (A smooth function is flat at a point if it vanishes there with all its derivatives (an example is <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200137.png" /> at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200138.png" />); the "Taylor expansion mapping" <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200139.png" /> is surjective, a very special consequence of the [[Whitney extension theorem|Whitney extension theorem]].)
+
Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200117.png" /> be the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200118.png" />-algebra of germs of smooth functions at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200119.png" /> (cf. [[Germ|Germ]]). Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200120.png" /> be the ideal of germs that vanish at zero, and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200121.png" /> the ideal generated by all products <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200122.png" /> for <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200123.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200124.png" /> are local coordinates at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200125.png" /> so that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200126.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200127.png" /> is generated as an ideal in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200128.png" /> by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200129.png" />, and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200130.png" /> by the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200131.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200132.png" />. In fact, the quotient ring <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200133.png" /> is the power series ring in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200134.png" /> variables over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200135.png" />. Here <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200136.png" /> is the ideal of flat function germs. (A smooth function is flat at a point if it vanishes there with all its derivatives (an example is <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200137.png" /> at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200138.png" />); the "Taylor expansion mapping" <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200139.png" /> is surjective, a very special consequence of the [[Whitney extension theorem|Whitney extension theorem]].)
  
 
Now, let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200140.png" /> be a tangent vector of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200141.png" /> at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200142.png" />. Then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200143.png" /> by (a1) for all constant functions in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200144.png" />. Also <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200145.png" />, again by (a1). Thus, each <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200146.png" /> defines an element in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200147.png" />, which is of dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200148.png" /> because <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200149.png" /> has dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200150.png" /> (and that element uniquely determines <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200151.png" />). Moreover, the tangent vectors <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200152.png" /> clearly define <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200153.png" /> linearly independent elements in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200154.png" /> (because <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200155.png" />). Thus,
 
Now, let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200140.png" /> be a tangent vector of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200141.png" /> at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200142.png" />. Then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200143.png" /> by (a1) for all constant functions in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200144.png" />. Also <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200145.png" />, again by (a1). Thus, each <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200146.png" /> defines an element in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200147.png" />, which is of dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200148.png" /> because <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200149.png" /> has dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200150.png" /> (and that element uniquely determines <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200151.png" />). Moreover, the tangent vectors <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200152.png" /> clearly define <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200153.png" /> linearly independent elements in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200154.png" /> (because <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t092/t092200/t092200155.png" />). Thus,
Line 56: Line 56:
  
 
====References====
 
====References====
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> R. Hermann,   "Geometry, physics, and systems" , M. Dekker (1973)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> R.L. Bishop,   R.J. Crittenden,   "Geometry of manifolds" , Acad. Press (1964)</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> M.W. Hirsch,   "Differential topology" , Springer (1976) pp. 4, 78</TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> S.P. Novikov,   A.T. Fomenko,   "Basic elements of differential geometry and topology" , Kluwer (1991) (Translated from Russian)</TD></TR><TR><TD valign="top">[a5]</TD> <TD valign="top"> Yu. Borisovich,   N. Bliznyakov,   Ya. Izrailevich,   T. Fomenko,   "Introduction to topology" , Kluwer (1993) (Translated from Russian)</TD></TR></table>
+
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> R. Hermann, "Geometry, physics, and systems" , M. Dekker (1973) {{MR|0494183}} {{ZBL|0285.58001}} </TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> R.L. Bishop, R.J. Crittenden, "Geometry of manifolds" , Acad. Press (1964) {{MR|0169148}} {{ZBL|0132.16003}} </TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> M.W. Hirsch, "Differential topology" , Springer (1976) pp. 4, 78 {{MR|0448362}} {{ZBL|0356.57001}} </TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> S.P. Novikov, A.T. Fomenko, "Basic elements of differential geometry and topology" , Kluwer (1991) (Translated from Russian) {{MR|1135798}} {{ZBL|0711.53001}} </TD></TR><TR><TD valign="top">[a5]</TD> <TD valign="top"> Yu. Borisovich, N. Bliznyakov, Ya. Izrailevich, T. Fomenko, "Introduction to topology" , Kluwer (1993) (Translated from Russian) {{MR|1450091}} {{MR|0824983}} {{MR|0591670}} {{ZBL|0836.57001}} {{ZBL|0834.57001}} {{ZBL|0478.57001}} </TD></TR></table>

Revision as of 21:57, 30 March 2012

Let be a differentiable manifold, and let be the algebra of smooth real-valued functions on it. A tangent vector to at is an -linear mapping such that

(a1)

For this definition one can equally well (in fact, better) use the ring of germs of smooth functions on at .

The tangent vectors to at form a vector space over of dimension . It is denoted by .

Let , , where is a system of coordinates on near . The -th partial derivative at with respect to is the tangent vector

where the right hand-side is the usual partial derivative of the function in the variables , at the point . One has (the Kronecker delta) and the form a basis for .

This basis for determined by the coordinate system is often denoted by .

A cotangent vector at is an -linear mapping such that the cotangent space at is the dual vector space to . The dual basis to is denoted by . One has

The disjoint union of the tangent spaces , , together with the projection , if , can be given the structure of a differentiable vector bundle, the tangent bundle.

Similarly, the cotangent spaces form a vector bundle dual to , called the cotangent bundle. The sections of are the vector fields on , the sections of are differentiable -forms on .

Let be a mapping of differentiable manifolds and let be the induced mapping . For a tangent vector at , composition with gives an -linear mapping which is a tangent vector to at . This defines a homomorphism of vector spaces and a vector bundle morphism .

In case and with global coordinates and , respectively, is given by differentiable functions and at each ,

so that the matrix of with respect to the basis of and the basis of is given by the Jacobi matrix of at .

Now, let be an imbedded manifold. Let , be a smooth curve in , . Then

(a2)

All tangent vectors in arise in this way. Identifying the vector (a2) with the -vector , viewed as a directed line segment starting in , one recovers the intuitive picture of the tangent space as the -plane in tangent to in .

A vector field on a manifold can be defined as a derivation (cf. Derivation in a ring) in the -algebra , . Composition with the evaluation mappings , , yields a family of tangent vectors , so that "becomes" a section of the tangent bundle. Given local coordinates , can locally be written as

and if a function in local coordinates is given by , then is the function given in local coordinates by the expression

showing once more the convenience of the " / x" notation for tangent vectors. (Of course, in practice one uses a bit more abuse of notation and writes instead of .)

Let be the -algebra of germs of smooth functions at (cf. Germ). Let be the ideal of germs that vanish at zero, and the ideal generated by all products for . If are local coordinates at so that , is generated as an ideal in by , and by the , . In fact, the quotient ring is the power series ring in variables over . Here is the ideal of flat function germs. (A smooth function is flat at a point if it vanishes there with all its derivatives (an example is at ); the "Taylor expansion mapping" is surjective, a very special consequence of the Whitney extension theorem.)

Now, let be a tangent vector of at . Then by (a1) for all constant functions in . Also , again by (a1). Thus, each defines an element in , which is of dimension because has dimension (and that element uniquely determines ). Moreover, the tangent vectors clearly define linearly independent elements in (because ). Thus,

the dual space of . This point of view is more generally applicable and serves as the definition of tangent space in analytic and algebraic geometry, cf. Analytic space; Zariski tangent space.

References

[a1] R. Hermann, "Geometry, physics, and systems" , M. Dekker (1973) MR0494183 Zbl 0285.58001
[a2] R.L. Bishop, R.J. Crittenden, "Geometry of manifolds" , Acad. Press (1964) MR0169148 Zbl 0132.16003
[a3] M.W. Hirsch, "Differential topology" , Springer (1976) pp. 4, 78 MR0448362 Zbl 0356.57001
[a4] S.P. Novikov, A.T. Fomenko, "Basic elements of differential geometry and topology" , Kluwer (1991) (Translated from Russian) MR1135798 Zbl 0711.53001
[a5] Yu. Borisovich, N. Bliznyakov, Ya. Izrailevich, T. Fomenko, "Introduction to topology" , Kluwer (1993) (Translated from Russian) MR1450091 MR0824983 MR0591670 Zbl 0836.57001 Zbl 0834.57001 Zbl 0478.57001
How to Cite This Entry:
Tangent vector. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Tangent_vector&oldid=23991