Difference between revisions of "Lyapunov surfaces and curves"
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A class of surfaces and curves that have quite good smoothness properties; it was introduced in potential theory by A.M. Lyapunov at the turn into the 20th century. | A class of surfaces and curves that have quite good smoothness properties; it was introduced in potential theory by A.M. Lyapunov at the turn into the 20th century. | ||
| − | A surface | + | A surface $ S $ |
| + | in the three-dimensional Euclidean space $ \mathbf R ^ {3} $ | ||
| + | is called a Lyapunov surface if it satisfies the following three conditions (Lyapunov's conditions): 1) at every point of $ S $ | ||
| + | there is a well-defined tangent plane, and consequently a well-defined normal; 2) there is a number $ r > 0 $, | ||
| + | the same for all points of $ S $, | ||
| + | such that if one takes the part $ \Sigma $ | ||
| + | of $ S $ | ||
| + | lying inside the Lyapunov sphere $ B ( y _ {0} , r ) $ | ||
| + | with centre at an arbitrary point $ y _ {0} \in S $ | ||
| + | and radius $ r $, | ||
| + | then the lines parallel to the normal to $ S $ | ||
| + | at $ y _ {0} $ | ||
| + | meet $ \Sigma $ | ||
| + | at most once; and 3) there are two numbers $ A > 0 $ | ||
| + | and $ \lambda $, | ||
| + | $ 0 < \lambda \leq 1 $, | ||
| + | the same for the whole of $ S $, | ||
| + | such that for any two points $ y _ {1} , y _ {2} \in S $, | ||
| − | < | + | $$ \tag{* } |
| + | | \theta | < A | y _ {1} - y _ {2} | ^ \lambda , | ||
| + | $$ | ||
| − | where | + | where $ \theta $ |
| + | is the angle between the normals to $ S $ | ||
| + | at $ y _ {1} $ | ||
| + | and $ y _ {2} $. | ||
| + | Sometimes these three conditions are supplemented by the requirement that $ S $ | ||
| + | is closed and that the solid angle under which any part $ \sigma $ | ||
| + | of $ S $ | ||
| + | is visible at an arbitrary point $ x \in \mathbf R ^ {3} $ | ||
| + | is uniformly bounded. | ||
| − | The Lyapunov conditions can be generalized to hypersurfaces in | + | The Lyapunov conditions can be generalized to hypersurfaces in $ \mathbf R ^ {n} $, |
| + | $ n \geq 3 $. | ||
| − | Similarly, a simple continuous curve | + | Similarly, a simple continuous curve $ L $ |
| + | in the plane $ \mathbf R ^ {2} $ | ||
| + | is called a Lyapunov curve if it satisfies the following conditions: $ 1 ^ \prime $) | ||
| + | at every point of $ L $ | ||
| + | there is a well-defined tangent, and consequently a well-defined normal; and $ 3 ^ \prime $) | ||
| + | there are two numbers $ A > 0 $ | ||
| + | and $ \lambda $, | ||
| + | $ 0 < \lambda \leq 1 $, | ||
| + | the same for the whole of $ L $, | ||
| + | such that for any two points $ y _ {1} , y _ {2} \in L $(*) | ||
| + | holds, where $ \theta $ | ||
| + | is the angle between the tangents or normals to $ L $ | ||
| + | at $ y _ {1} $ | ||
| + | and $ y _ {2} $. | ||
| + | Here Lyapunov's condition 2) follows from $ 1 ^ \prime $) | ||
| + | and $ 3 ^ \prime $). | ||
| + | The Lyapunov curves are a subclass of the simple smooth curves. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> A.M. Lyapunov, "On certain questions connected with the Dirichlet problem" , ''Collected works'' , '''1''' , Moscow (1954) pp. 45–47; 48–100 (In Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> S.L. Sobolev, "Partial differential equations of mathematical physics" , Pergamon (1964) (Translated from Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) pp. Chapt. 5 (Translated from Russian)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> N.I. Muskhelishvili, "Singular integral equations" , Wolters-Noordhoff (1972) pp. Chapt. 1 (Translated from Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> A.M. Lyapunov, "On certain questions connected with the Dirichlet problem" , ''Collected works'' , '''1''' , Moscow (1954) pp. 45–47; 48–100 (In Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> S.L. Sobolev, "Partial differential equations of mathematical physics" , Pergamon (1964) (Translated from Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) pp. Chapt. 5 (Translated from Russian)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> N.I. Muskhelishvili, "Singular integral equations" , Wolters-Noordhoff (1972) pp. Chapt. 1 (Translated from Russian)</TD></TR></table> | ||
| − | |||
| − | |||
====Comments==== | ====Comments==== | ||
| − | A Lyapunov surface is necessarily | + | A Lyapunov surface is necessarily $ C ^ {1} $, |
| + | and on the other hand a compact surface of class $ C ^ {2} $ | ||
| + | is a Lyapunov surface. Lyapunov surfaces are used in the study of simple- and double-layer potentials. | ||
Latest revision as of 04:11, 6 June 2020
A class of surfaces and curves that have quite good smoothness properties; it was introduced in potential theory by A.M. Lyapunov at the turn into the 20th century.
A surface $ S $ in the three-dimensional Euclidean space $ \mathbf R ^ {3} $ is called a Lyapunov surface if it satisfies the following three conditions (Lyapunov's conditions): 1) at every point of $ S $ there is a well-defined tangent plane, and consequently a well-defined normal; 2) there is a number $ r > 0 $, the same for all points of $ S $, such that if one takes the part $ \Sigma $ of $ S $ lying inside the Lyapunov sphere $ B ( y _ {0} , r ) $ with centre at an arbitrary point $ y _ {0} \in S $ and radius $ r $, then the lines parallel to the normal to $ S $ at $ y _ {0} $ meet $ \Sigma $ at most once; and 3) there are two numbers $ A > 0 $ and $ \lambda $, $ 0 < \lambda \leq 1 $, the same for the whole of $ S $, such that for any two points $ y _ {1} , y _ {2} \in S $,
$$ \tag{* } | \theta | < A | y _ {1} - y _ {2} | ^ \lambda , $$
where $ \theta $ is the angle between the normals to $ S $ at $ y _ {1} $ and $ y _ {2} $. Sometimes these three conditions are supplemented by the requirement that $ S $ is closed and that the solid angle under which any part $ \sigma $ of $ S $ is visible at an arbitrary point $ x \in \mathbf R ^ {3} $ is uniformly bounded.
The Lyapunov conditions can be generalized to hypersurfaces in $ \mathbf R ^ {n} $, $ n \geq 3 $.
Similarly, a simple continuous curve $ L $ in the plane $ \mathbf R ^ {2} $ is called a Lyapunov curve if it satisfies the following conditions: $ 1 ^ \prime $) at every point of $ L $ there is a well-defined tangent, and consequently a well-defined normal; and $ 3 ^ \prime $) there are two numbers $ A > 0 $ and $ \lambda $, $ 0 < \lambda \leq 1 $, the same for the whole of $ L $, such that for any two points $ y _ {1} , y _ {2} \in L $(*) holds, where $ \theta $ is the angle between the tangents or normals to $ L $ at $ y _ {1} $ and $ y _ {2} $. Here Lyapunov's condition 2) follows from $ 1 ^ \prime $) and $ 3 ^ \prime $). The Lyapunov curves are a subclass of the simple smooth curves.
References
| [1] | A.M. Lyapunov, "On certain questions connected with the Dirichlet problem" , Collected works , 1 , Moscow (1954) pp. 45–47; 48–100 (In Russian) |
| [2] | S.L. Sobolev, "Partial differential equations of mathematical physics" , Pergamon (1964) (Translated from Russian) |
| [3] | V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) pp. Chapt. 5 (Translated from Russian) |
| [4] | N.I. Muskhelishvili, "Singular integral equations" , Wolters-Noordhoff (1972) pp. Chapt. 1 (Translated from Russian) |
Comments
A Lyapunov surface is necessarily $ C ^ {1} $, and on the other hand a compact surface of class $ C ^ {2} $ is a Lyapunov surface. Lyapunov surfaces are used in the study of simple- and double-layer potentials.
Lyapunov surfaces and curves. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Lyapunov_surfaces_and_curves&oldid=47731