2014
DOI: 10.3233/asy-141238
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On the ℛ-boundedness of the solution operators in the study of the compressible viscous fluid flow with free boundary conditions

Abstract: In this paper, we consider a generalized resolvent problem for the linearization system of the Navier-Stokes equations describing some free boundary problem of a compressible barotropic viscous fluid flow without taking the surface tension into account. We prove the existence of the R-bounded solution operators, which drives not only the generation of analytic semigroup but also the maximal Lp-Lq regularity by means of Weis' operator valued Fourier multiplier theorem for the corresponding time dependent proble… Show more

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Cited by 16 publications
(18 citation statements)
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“…Substituting (21), ( 22), (23), ( 24) and ( 25) to (7), we obtain the formula of � = � = 〈 � 1 , � 2 , … , � −1 〉 and � in equation system of (5) which completes the proof of Theorem 2…”
Section: =1mentioning
confidence: 57%
See 1 more Smart Citation
“…Substituting (21), ( 22), (23), ( 24) and ( 25) to (7), we obtain the formula of � = � = 〈 � 1 , � 2 , … , � −1 〉 and � in equation system of (5) which completes the proof of Theorem 2…”
Section: =1mentioning
confidence: 57%
“…In this paper, we put the different approach of the general solution of velocity as in [7]. This research focus on considering the solution formula of the compressible Stokes equation system (2) without surface tension by using Fourier transform.…”
Section: Methodsmentioning
confidence: 99%
“…In this section, we shall show the proof of Theorem 2.8. In order to prove Theorem 2.8, we use the following lemmas which is proven by Götz and Shibata [7].…”
Section: 3mentioning
confidence: 99%
“…He proved the existence of R bounded solution operators for the model problem that derives the maximal L p -L q regularity of solutions to the linearized equations automatically with the help of Weis's operator valued Fourier multiplier theorem [35]. According to Shibata [13], the regularity of ρ + is W 1 q in space, but to solve the kinetic equation: u Γ · n t = [[ρu]] · n t /[[ρ]] on Γ t we need W 2−1/q q regularity of ρ + on Γ t , which means the regularity loss. On the other hand, the regularity of ρ + dominated by the Navier-Stokes-Korteweg equations is W 3 q in Ω t+ (cf.…”
Section: Introductionmentioning
confidence: 99%