TY - JOUR
T1 - Compressible-incompressible two-phase flows with phase transition
T2 - Model problem
AU - Watanabe, Keiichi
N1 - Publisher Copyright:
Copyright © 2017, The Authors. All rights reserved.
Copyright:
Copyright 2020 Elsevier B.V., All rights reserved.
PY - 2017/5/9
Y1 - 2017/5/9
N2 - We study the compressible and incompressible two-phase flows separated by a sharp interface with a phase transition and a surface tension. In particular, we consider the problem in RN, and the Navier-Stokes-Korteweg equations is used in the upper domain and the Navier-Stokes equations is used in the lower domain. We prove the existence of R-bounded solution operator families for a resolvent problem arising from its model problem. According to Shibata [13], the regularity of ρ+ is Wq1 in space, but to solve the kinetic equation: uΓ · nt = [[ρu]] · nt/[[ρ]] on Γt we need Wq2−1/q regularity of ρ+ on Γt, which means the regularity loss. Since the regularity of ρ+ dominated by the Navier-Stokes-Korteweg equations is Wq3 in space, we eliminate the problem by using the Navier-Stokes-Korteweg equations instead of the compressible Navier-Stokes equations.MSC Codes 35Q30 (Primary), 76T10 (Secondary)
AB - We study the compressible and incompressible two-phase flows separated by a sharp interface with a phase transition and a surface tension. In particular, we consider the problem in RN, and the Navier-Stokes-Korteweg equations is used in the upper domain and the Navier-Stokes equations is used in the lower domain. We prove the existence of R-bounded solution operator families for a resolvent problem arising from its model problem. According to Shibata [13], the regularity of ρ+ is Wq1 in space, but to solve the kinetic equation: uΓ · nt = [[ρu]] · nt/[[ρ]] on Γt we need Wq2−1/q regularity of ρ+ on Γt, which means the regularity loss. Since the regularity of ρ+ dominated by the Navier-Stokes-Korteweg equations is Wq3 in space, we eliminate the problem by using the Navier-Stokes-Korteweg equations instead of the compressible Navier-Stokes equations.MSC Codes 35Q30 (Primary), 76T10 (Secondary)
KW - Compressible and incompressible viscous flow
KW - Maximal Lp-Lq regularity
KW - Navier-Stokes-Korteweg equation
KW - Phase transition
KW - R-bounded solution operator
KW - Surface tension
KW - Two-phase flows
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M3 - Article
AN - SCOPUS:85093640238
JO - Nuclear Physics A
JF - Nuclear Physics A
SN - 0375-9474
ER -