2021
DOI: 10.1007/s11565-021-00381-7
|View full text |Cite
|
Sign up to set email alerts
|

Continuous dependence and convergence for a Kelvin–Voigt fluid of order one

Abstract: It is shown that the solution to the boundary - initial value problem for a Kelvin–Voigt fluid of order one depends continuously upon the Kelvin–Voigt parameters, the viscosity, and the viscoelastic coefficients. Convergence of a solution is also shown.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
3
0

Year Published

2022
2022
2024
2024

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 17 publications
(4 citation statements)
references
References 50 publications
0
3
0
Order By: Relevance
“…An interesting class of them can be found in [12]. Linear and nonlinear versions have been studied [8, 9, 16]. For some of them, the study we have developed can be used.…”
Section: Applications To Some Special Problemsmentioning
confidence: 99%
“…An interesting class of them can be found in [12]. Linear and nonlinear versions have been studied [8, 9, 16]. For some of them, the study we have developed can be used.…”
Section: Applications To Some Special Problemsmentioning
confidence: 99%
“…In an elegant analysis of stationary and oscillatory convection in a Brinkman-Darcy-Kelvin-Voigt fluid, Straughan [1] (see also [2][3][4][5]) considered a system of evolution laws including-beyond a regularized balance of momentum-Payne-Song's equation [6] in Eulerian representation, that is an energy balance given by…”
Section: Introductionmentioning
confidence: 99%
“…In an elegant analysis of stationary and oscillatory convection in a Brinkman–Darcy–Kelvin–Voigt fluid, Straughan [1] (see also [25]) considered a system of evolution laws including—beyond a regularized balance of momentum—Payne–Song’s equation [6] in Eulerian representation, that is an energy balance given by T˙=κnormalΔTdivq,where the superposed dot indicates from now on total derivative with respect to time; T is the absolute temperature, κ the conductivity, taken to be constant, and q the heat flux, which satisfies, per se , a version of Guyer–Krumhansl’s equation [7,8], given by DqDt=qκnormal∇T+ς^1normalΔq+ς^2normal∇divq,with a time delay and scriptD/scriptDt a generic objective derivative, which he considers in the analysis to be the Lie derivative with respect to the macroscopic fluid velocity.…”
Section: Introductionmentioning
confidence: 99%
“…β is the cooling coefficient. For more papers of the type, one can refer to [5][6][7][8][9][10][11][12][13][14][15][16][17][18]. However, these results above only considered the case of the bounded region.…”
Section: Introductionmentioning
confidence: 99%