Namespaces
Variants
Actions

Friedrichs inequality

From Encyclopedia of Mathematics
Revision as of 19:40, 5 June 2020 by Ulf Rehmann (talk | contribs) (tex encoded by computer)
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)
Jump to: navigation, search


An inequality of the form

$$ \tag{1 } \int\limits _ \Omega f ^ { 2 } \ d \Omega \leq C \left \{ \int\limits _ \Omega \sum _ {i = 1 } ^ { n } \left ( \frac{\partial f }{\partial x _ {i} } \right ) ^ {2} \ d \Omega + \int\limits _ \Gamma f ^ { 2 } d \Gamma \right \} , $$

where $ \Omega $ is a bounded domain of points $ x = x ( x _ {1} \dots x _ {n} ) $ in an $ n $- dimensional Euclidean space with an $ ( n - 1) $- dimensional boundary $ \Gamma $ satisfying a local Lipschitz condition, and the function $ f \equiv f ( x) \in W _ {2} ^ {1} ( \Omega ) $( a Sobolev space).

The right-hand side of the Friedrichs inequality gives an equivalent norm in $ W _ {2} ^ {1} ( \Omega ) $. Using another equivalent norm in $ W _ {2} ^ {1} ( \Omega ) $, one obtains (see [2]) a modification of the Friedrichs inequality of the form

$$ \tag{2 } \int\limits _ \Omega f ^ { 2 } \ d \Omega \leq C \left \{ \int\limits _ \Omega \sum _ {i = 1 } ^ { n } \left ( \frac{\partial f }{\partial x _ {i} } \right ) ^ {2} d \Omega + \left ( \int\limits _ \Gamma f d \Gamma \right ) ^ {2} \right \} . $$

There are generalizations (see [3][5]) of the Friedrichs inequality to weighted spaces (see Weighted space; Imbedding theorems). Suppose that $ \Gamma \subset C ^ {(} l) $ and that the numbers $ r $, $ p $ and $ \alpha $ are real, with $ r $ being a natural number and $ 1 \leq p < \infty $. One says that $ f \in W _ {p, \alpha } ^ {r} ( \Omega ) $ if the norm

$$ \| f \| _ {W _ {p, \alpha } ^ {r} ( \Omega ) } = \ \| f \| _ {L _ {p} ( \Omega ) } + \| f \| _ {\omega _ {p, \alpha } ^ {r} ( \Omega ) } $$

is finite, where

$$ \| f \| _ {L _ {p} ( \Omega ) } = \ \left ( \int\limits _ \Omega | f | ^ {p} \ d \Omega \right ) ^ {1/p} , $$

$$ \| f \| _ {\omega _ {p, \alpha } ^ {r} ( \Omega ) } = \sum _ {| k | = r } \| \rho ^ \alpha f ^ {(} k) \| _ {L _ {p} ( \Omega ) } , $$

$$ f ^ { ( k) } = \frac{\partial ^ {| k | } f }{\partial x _ {1} ^ {k _ {1} } \dots \partial x _ {n} ^ {k _ {n} } } ,\ \ | k | = \sum _ {i = 1 } ^ { n } k _ {i} , $$

and $ \rho = \rho ( x) $ is distance function from $ x \in \Omega $ to $ \Gamma $.

Suppose that $ s _ {0} $ is a natural number such that

$$ r - \alpha - { \frac{1}{p} } \leq \ s _ {0} < r - \alpha + 1 - { \frac{1}{p} } . $$

Then, if $ \Gamma \subset C ^ {( s _ {0} + 1) } $, $ - p ^ {-} 1 < \alpha < r - p ^ {-} 1 $, $ r/2 \leq s _ {0} $, for $ f \in W _ {p, \alpha } ^ {r} ( \Omega ) $ the following inequality holds:

$$ \| f \| _ {L _ {p} ( \Omega ) } \leq \ C \left \{ \sum _ {l + s < r/2 } \left \| \left ( \left . \frac{\partial ^ {s} f }{\partial n ^ {s} } \ \right | _ \Gamma \right ) ^ {(} l) \ \right \| _ {L _ {p} ( \Gamma ) } + \| f \| _ {\omega _ {p, \alpha } ^ {r} ( \Omega ) } \right \} , $$

where $ ( \partial ^ {s} f/ \partial n ^ {s} ) \mid _ \Gamma $ is the derivative of order $ s $ with respect to the interior normal to $ \Gamma $ at the points of $ \Gamma $.

One can also obtain an inequality of the type (2), which has in the simplest case the form

$$ \| f \| _ {L _ {p} ( \Omega ) } ^ {p} \leq \ C \left ( \| f \| _ {\omega _ {p, \alpha } ^ {1} ( \Omega ) } ^ {p} + \left | \int\limits _ \Gamma u \tau d \Gamma \ \right | ^ {p} \right ) , $$

where

$$ p , \gamma > 1,\ \ - \frac{1}{p} < \alpha < 1 - \frac{1}{p} - \frac{1} \gamma , $$

$$ \tau \in L _ \gamma ( \Gamma ),\ \int\limits _ \Gamma \tau d \Gamma \neq 0. $$

The constant $ C $ is independent of $ f $ throughout.

The inequality is named after K.O. Friedrichs, who obtained it for $ n = 2 $, $ f \in C ^ {(} 2) ( \overline \Omega \; ) $( see [1]).

References

[1] K.O. Friedrichs, "Eine invariante Formulierung des Newtonschen Gravititationsgesetzes und des Grenzüberganges vom Einsteinschen zum Newtonschen Gesetz" Math. Ann. , 98 (1927) pp. 566–575
[2] S.L. Sobolev, "Applications of functional analysis in mathematical physics" , Amer. Math. Soc. (1963) (Translated from Russian)
[3] S.M. Nikol'skii, P.I. Lizorkin, "On some inequalities for weight-class functions and boundary-value problems with a strong degeneracy at the boundary" Soviet Math. Dokl. , 5 (1964) pp. 1535–1539 Dokl. Akad. Nauk SSSR , 159 : 3 (1964) pp. 512–515
[4] S.M. Nikol'skii, "Approximation of functions of several variables and imbedding theorems" , Springer (1975) (Translated from Russian)
[5] D.F. Kalinichenko, "Some properties of functions in the spaces and " Mat. Sb. , 64 : 3 (1964) pp. 436–457 (In Russian)
[6] R. Courant, D. Hilbert, "Methods of mathematical physics. Partial differential equations" , 2 , Interscience (1965) (Translated from German)
[7] L. Nirenberg, "On elliptic partial differential equations" Ann. Scuola Norm. Sup. Pisa Ser. 3 , 13 : 2 (1959) pp. 115–162
[8] L. Sandgren, "A vibration problem" Medd. Lunds Univ. Mat. Sem. , 13 (1955) pp. 1–84
How to Cite This Entry:
Friedrichs inequality. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Friedrichs_inequality&oldid=46991
This article was adapted from an original article by D.F. KalinichenkoN.V. Miroshin (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article