|
|
Line 1: |
Line 1: |
− | ''of a subset <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255101.png" /> of a Euclidean space at a point <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255102.png" />'' | + | {{TEX|done}} |
| + | ''of a subset of a Euclidean space at a point a\in E'' |
| | | |
− | The union of rays <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255103.png" /> with origin <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255104.png" /> for which there exists a sequence of points <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255105.png" /> converging to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255106.png" /> such that the sequence of rays <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255107.png" /> converges to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255108.png" />. It is denoted by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c0255109.png" />. For an <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551010.png" />-dimensional differentiable manifold <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551011.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551012.png" /> is the same as the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551013.png" />-dimensional tangent plane to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551014.png" /> at <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551015.png" />. This concept proves useful in the study of differentiability properties of functions. If for every point <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551016.png" /> of a set <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551017.png" /> in the plane, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551018.png" /> is not the whole plane, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551019.png" /> can be partitioned into a countable number of parts situated on rectifiable curves. This theorem has been repeatedly generalized and refined. For example, a set of finite Hausdorff <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551021.png" />-measure, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551022.png" />, located in an <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551023.png" />-dimensional Euclidean space partitions into a countable number of parts, one of which has zero Favard measure of order <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551024.png" />, while each of the remaining parts is situated on some Lipschitz surface of dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551025.png" />; for almost-all <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551026.png" /> (in the sense of the Hausdorff <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551027.png" />-measure), <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551028.png" /> is a plane of dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551029.png" /> if all variations of the set <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551030.png" /> are finite and, beginning with the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c025/c025510/c02551031.png" />-th, vanish. | + | The union of rays \vec{ab} with origin a for which there exists a sequence of points b_n\in E converging to a such that the sequence of rays \vec{ab_n} converges to \vec{ab}. It is denoted by \operatorname{contg}(E,a). For an m-dimensional differentiable manifold E, $\operatorname{contg}(E,a)$ is the same as the m-dimensional tangent plane to E at a. This concept proves useful in the study of differentiability properties of functions. If for every point a of a set E in the plane, \operatorname{contg}(E,a) is not the whole plane, then E can be partitioned into a countable number of parts situated on rectifiable curves. This theorem has been repeatedly generalized and refined. For example, a set of finite Hausdorff p-measure, $p=1,\dots,n-1$, located in an n-dimensional Euclidean space partitions into a countable number of parts, one of which has zero Favard measure of order p, while each of the remaining parts is situated on some Lipschitz surface of dimension p; for almost-all x\in E (in the sense of the Hausdorff p-measure), \operatorname{contg}(E,a) is a plane of dimension p if all variations of the set E are finite and, beginning with the (p+1)-th, vanish. |
| | | |
| ====References==== | | ====References==== |
Revision as of 15:34, 29 December 2018
of a subset E of a Euclidean space at a point a\in E
The union of rays \vec{ab} with origin a for which there exists a sequence of points b_n\in E converging to a such that the sequence of rays \vec{ab_n} converges to \vec{ab}. It is denoted by \operatorname{contg}(E,a). For an m-dimensional differentiable manifold E, \operatorname{contg}(E,a) is the same as the m-dimensional tangent plane to E at a. This concept proves useful in the study of differentiability properties of functions. If for every point a of a set E in the plane, \operatorname{contg}(E,a) is not the whole plane, then E can be partitioned into a countable number of parts situated on rectifiable curves. This theorem has been repeatedly generalized and refined. For example, a set of finite Hausdorff p-measure, p=1,\dots,n-1, located in an n-dimensional Euclidean space partitions into a countable number of parts, one of which has zero Favard measure of order p, while each of the remaining parts is situated on some Lipschitz surface of dimension p; for almost-all x\in E (in the sense of the Hausdorff p-measure), \operatorname{contg}(E,a) is a plane of dimension p if all variations of the set E are finite and, beginning with the (p+1)-th, vanish.
References
[1] | G. Bouligand, "Introduction à la géometrie infinitésimale directe" , Vuibert (1932) |
[2] | S. Saks, "Theory of the integral" , Hafner (1952) (Translated from French) |
[3] | H. Federer, "Geometric measure theory" , Springer (1969) |
[4] | L.D. Ivanov, "Variations of sets and functions" , Moscow (1975) (In Russian) |
More on contingents (and the related notion of paratingent) can be found in G. Choquet's monograph [a1]. Contingents are useful in optimization problems nowadays.
References
[a1] | G. Choquet, "Outils topologiques et métriques de l'analyse mathématiques" , Centre Docum. Univ. Paris (1969) (Rédigé par C. Mayer) |
[a2] | J.P. Aubin, I. Ekeland, "Applied nonlinear analysis" , Wiley (Interscience) (1984) |
How to Cite This Entry:
Contingent. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Contingent&oldid=12121
This article was adapted from an original article by L.D. Ivanov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098.
See original article