2022
DOI: 10.1002/zamm.202100240
|View full text |Cite
|
Sign up to set email alerts
|

Relative energy and weak–strong uniqueness of a two‐phase viscoelastic phase separation model

Abstract: The aim of this paper is to analyze a viscoelastic phase separation model. We derive a suitable notion of the relative energy taking into account the nonconvex nature of the energy law for the viscoelastic phase separation. This allows us to prove the weak–strong uniqueness principle. We will provide the estimates for the full model in two space dimensions. For a reduced model, we present the estimates in three space dimensions and derive conditional relative energy estimates.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
7
0

Year Published

2022
2022
2023
2023

Publication Types

Select...
1
1

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(7 citation statements)
references
References 35 publications
0
7
0
Order By: Relevance
“…A related model is the Navier-Stokes-Korteweg system, the corresponding results can be found in [16]. The relative energy and the corresponding weak-strong uniqueness results for the viscoelastic phase separation model are given in our recent work [3]. The proof is valid in two space dimensions and conditionally valid in three space dimensions by requiring the existence of a suitable weak solution.…”
Section: Introductionmentioning
confidence: 91%
See 4 more Smart Citations
“…A related model is the Navier-Stokes-Korteweg system, the corresponding results can be found in [16]. The relative energy and the corresponding weak-strong uniqueness results for the viscoelastic phase separation model are given in our recent work [3]. The proof is valid in two space dimensions and conditionally valid in three space dimensions by requiring the existence of a suitable weak solution.…”
Section: Introductionmentioning
confidence: 91%
“…For the standard Lebesgue spaces, L p (Ω) the norm is denoted by • p . We use the standard notation for the Sobolev spaces and introduce the notation V := H 1 0,div (Ω) 3 , H := L 2 div (Ω) 3 . As usual these space are obtained as closure with respect to the L 2 , H 1 norm of the space of C 0,∞ ( Ω) function with zero divergence, respectively.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
See 3 more Smart Citations