Ladyzhenskaya's inequality
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In mathematics, Ladyzhenskaya's inequality is any of a number of related functional inequalities named after the
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Olga Aleksandrovna Ladyzhenskaya Olga Aleksandrovna Ladyzhenskaya (russian: Óльга Алекса́ндровна Лады́женская, link=no, p=ˈolʲɡə ɐlʲɪˈksandrəvnə ɫɐˈdɨʐɨnskəɪ̯ə, a=Ru-Olga Aleksandrovna Ladyzhenskaya.wav; 7 March 1922 – 12 Jan ...
. The original such inequality, for functions of two real variables, was introduced by Ladyzhenskaya in 1958 to prove the existence and uniqueness of long-time solutions to the
Navier–Stokes equations In physics, the Navier–Stokes equations ( ) are partial differential equations which describe the motion of viscous fluid substances, named after French engineer and physicist Claude-Louis Navier and Anglo-Irish physicist and mathematician Geo ...
in two spatial dimensions (for smooth enough initial data). There is an analogous inequality for functions of three real variables, but the exponents are slightly different; much of the difficulty in establishing existence and uniqueness of solutions to the three-dimensional Navier–Stokes equations stems from these different exponents. Ladyzhenskaya's inequality is one member of a broad class of inequalities known as interpolation inequalities. Let \Omega be a
Lipschitz domain In mathematics, a Lipschitz domain (or domain with Lipschitz boundary) is a domain in Euclidean space whose boundary is "sufficiently regular" in the sense that it can be thought of as locally being the graph of a Lipschitz continuous function. T ...
in \mathbb R^ for n = 2 \text 3 and let u: \Omega \rightarrow \mathbb R be a weakly differentiable function that vanishes on the boundary of \Omega in the sense of
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(that is, u is a limit in the
Sobolev space In mathematics, a Sobolev space is a vector space of functions equipped with a norm that is a combination of ''Lp''-norms of the function together with its derivatives up to a given order. The derivatives are understood in a suitable weak sense ...
H^1(\Omega) of a sequence of smooth functions that are
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in \Omega). Then there exists a constant C depending only on \Omega such that, in the case n = 2: : \, u \, _ \leq C \, u \, _^ \, \nabla u \, _^ and in the case n = 3: : \, u \, _ \leq C \, u \, _^ \, \nabla u \, _^


Generalizations

* Both the two- and three-dimensional versions of Ladyzhenskaya's inequality are special cases of the Gagliardo–Nirenberg interpolation inequality :: \, u \, _ \leq C \, u \, _^\alpha \, u \, _^, :which holds whenever :: p > q \geq 1, s > n ( \tfrac - \tfrac ), \text \tfrac = \tfrac + (1 - \alpha) ( \tfrac - \tfrac ). :Ladyzhenskaya's inequalities are the special cases p = 4, q = 2, s = 1 \alpha = \tfrac when n = 2 and \alpha = \tfrac when n = 3. * A simple modification of the argument used by Ladyzhenskaya in her 1958 paper (see e.g. Constantin & Seregin 2010) yields the following inequality for u: \mathbb R^ \rightarrow \mathbb R, valid for all r \ge 2: :: \, u \, _ \leq C r \, u \, _^ \, \nabla u \, _^. * The usual Ladyzhenskaya inequality on \mathbb R^, n = 2 \text 3, can be generalized (see McCormick & al. 2013) to use the weak L^ "norm" of u in place of the usual L^ norm: :: \, u \, _ \leq \begin C \, u \, _^ \, \nabla u \, _^, & n = 2, \\ C \, u \, _^ \, \nabla u \, _^, & n = 3. \end


See also

* Agmon's inequality


References

* * [] * {{cite journal , last1 = McCormick , first1 = D. S. , last2 = Robinson , first2 = J. C. , last3 = Rodrigo , first3 = J. L. , title = Generalised Gagliardo–Nirenberg inequalities using weak Lebesgue spaces and BMO , journal = Milan J. Math. , volume = 81 , issue = 2 , pages = 265–289 , year = 2013 , doi = 10.1007/s00032-013-0202-6 , arxiv = 1303.6351 , citeseerx = 10.1.1.758.7957 , s2cid = 44022084 Inequalities Fluid dynamics Sobolev spaces