2020
DOI: 10.1016/j.aml.2019.106143
|View full text |Cite
|
Sign up to set email alerts
|

Weak-strong uniqueness for the Navier–Stokes–Poisson equations

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
4
0

Year Published

2021
2021
2022
2022

Publication Types

Select...
2
1

Relationship

1
2

Authors

Journals

citations
Cited by 3 publications
(4 citation statements)
references
References 19 publications
0
4
0
Order By: Relevance
“…In this section, we will establish the relative entropy inequality (18) to the system (1)-( 5) and extend the admissible class of test function.…”
Section: Relative Entropy Inequalitymentioning
confidence: 99%
See 2 more Smart Citations
“…In this section, we will establish the relative entropy inequality (18) to the system (1)-( 5) and extend the admissible class of test function.…”
Section: Relative Entropy Inequalitymentioning
confidence: 99%
“…Extending the Admissible Class of Test Function. Making use of density argument, we can extend the class of test function ðr, U, Ψ, HÞ appeared in the relative entropy inequality (18), (20).…”
Section: Advances In Mathematical Physicsmentioning
confidence: 99%
See 1 more Smart Citation
“…Indeed, the convexity of the pressure potential P = P (̺) guarantees the non-negativity of E = E(t) for any time t ∈ [0, T ]. Moreover, if ̺, ̺ > 0, proving the weak-strong uniqueness principle is equivalent to showing that E(t) ≡ 0 for any time t ∈ [0, T ]; this is the strategy pursued by He and Tan [8] to prove the weak-strong uniqueness principle on a bounded domain Ω. For σ = −1, however, the problem gets more complicated.…”
Section: Introductionmentioning
confidence: 99%