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− | ''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 $E$ of a Euclidean space at a point $a\in E$'' |
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− | 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. |
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| ====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=43561
This article was adapted from an original article by L.D. Ivanov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098.
See original article