2005
DOI: 10.3934/cpaa.2005.4.613
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New dissipated energies for the thin fluid film equation

Abstract: Abstract. The thin fluid film evolution ht = −(h n hxxx)x is known to conserve the fluid volume h dx and to dissipate the "energies" h 1.5−n dx and h 2 x dx. We extend this last result by showing the energy h p h 2 x dx is dissipated for some values of p < 0, when 1 2 < n < 3. For example when n = 1, the Hele-Shaw equation ht = −(hhxxx)x dissipates h −1/2 h 2 x dx.

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Cited by 20 publications
(39 citation statements)
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(31 reference statements)
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“…The same result holds for periodic boundary conditions [11]. This bound turns out to be sharp, at least in the one-dimensional case [17]. Moreover, the entropy production Q α in (1.4) can be made explicit: a valid choice is Q α [U ] = Ω |(U (α+β)/2 ) xx | 2 dx with a suitable c > 0 if 3/2 < α + β < 3; see [11].…”
Section: Introductionsupporting
confidence: 58%
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“…The same result holds for periodic boundary conditions [11]. This bound turns out to be sharp, at least in the one-dimensional case [17]. Moreover, the entropy production Q α in (1.4) can be made explicit: a valid choice is Q α [U ] = Ω |(U (α+β)/2 ) xx | 2 dx with a suitable c > 0 if 3/2 < α + β < 3; see [11].…”
Section: Introductionsupporting
confidence: 58%
“…This correspondence -which is summarized in Lemma 2.1 below -constitutes an extension of the ideas previously developed for entropy estimates in one spatial dimension by the last two authors [11]; see also [17] for an alternative approach. The proof of the main theorems are then obtained by solution of the associated algebraic problems.…”
Section: Decision Problem and Shift Polynomialsmentioning
confidence: 98%
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