Maxwell models for viscoelastic flows are famous for their potential to unify elastic motions of solids with viscous motions of liquids in the continuum mechanics perspective. But the usual Maxwell models allow one to define well motions mostly for one-dimensional flows only. To define unequivocal multi-dimensional viscoelastic flows (as solutions to well-posed initial-value problems) we advocated in [ESAIM:M2AN 55 (2021), p. 807-831] an upper-convected Maxwell model for compressible flows with a symmetric-hyperbolic formulation. Here, that model is derived again, with new details.
@article{CRMECA_2023__351_S1_A4_0, author = {S\'ebastien Boyaval}, title = {A viscoelastic flow model of {Maxwell-type} with a symmetric-hyperbolic formulation}, journal = {Comptes Rendus. M\'ecanique}, publisher = {Acad\'emie des sciences, Paris}, year = {2023}, doi = {10.5802/crmeca.165}, language = {en}, note = {Online first}, }
Sébastien Boyaval. A viscoelastic flow model of Maxwell-type with a symmetric-hyperbolic formulation. Comptes Rendus. Mécanique, Online first (2023), pp. 1-9. doi : 10.5802/crmeca.165.
[1] Mathematical Foundations of Elasticity, Dover Civil and Mechanical Engineering, Dover Publications, New York, 2012
[2] Hyperbolic Conservation Laws in Continuum Physics, Springer-Verlag, Berlin, 2016 | DOI
[3] Viscoelastic flows of Maxwell fluids with conservation laws, ESAIM Math. Model. Numer. Anal., Volume 55 (2021) no. 3, pp. 807-831 | DOI | Zbl
[4] Symmetric-hyperbolic equations of motion for a hyperelastic material, J. Hyperbolic Differ. Equ., Volume 6 (2009) no. 3, pp. 615-630 | DOI | Zbl
[5] The Physics of Rubber Elasticity, Oxford University Press, USA, 2005
[6] Lagrangian gas dynamics in two dimensions and lagrangian systems, Arch. Rat. Mech. Anal., Volume 178 (2005) no. 3, pp. 327-372 | DOI | Zbl
[7] The Boltzmann equation and its hydrodynamic limits, Evolutionary Equations (Handbook of Differential Equations), Volume II, Elsevier/North-Holland, Amsterdam, 2005 | Zbl
[8] The thermodynamics of elastic materials with heat conduction and viscosity, Arch. Rat. Mech. Anal., Volume 13 (1963) no. 1, pp. 167-178 | DOI | Zbl
[9] IV. On double refraction in a viscous fluid in motion, Proc. R. Soc. Lond., Volume 22 (1874) no. 148-155, pp. 46-47
[10] Computational Rheology, Imperial College Press/World Scientific, Singapore, 2002 | DOI
[11] Stokes’ first problem for viscoelastic fluids, J. Non-Newton. Fluid Mech., Volume 25 (1987) no. 3, pp. 239-259 | DOI | Zbl
[12] Convergence of the equations for a Maxwell fluid, Stud. Appl. Math., Volume 103 (1999) no. 3, pp. 267-278 | DOI | Zbl
[13] About the structural stability of Maxwell fluids: convergence toward elastodynamics (2022) (hal-03899611) (Technical report)
[14] On the mathematical modelling of a compressible viscoelastic fluid, Arch. Rat. Mech. Anal., Volume 205 (2012) no. 1, pp. 1-26 | DOI | Zbl
[15] Non-convex entropies for conservation laws with involutions, Philos. Trans. R. Soc. Lond. Ser. A, Volume 371 (2013) no. 2005, 20120344 | Zbl
[16] Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math., Volume 11 (1973), pp. 267-288 | DOI | Zbl
[17] Non-isothermal viscoelastic flows with conservation laws and relaxation, J. Hyperbolic Differ. Equ., Volume 19 (2022) no. 2, pp. 337-364 | DOI | Zbl
Cited by Sources:
Risk-averse estimates of effective properties in heterogeneous elasticity
Jeremy Bleyer
C. R. Méca (2023)
Evolution of CFD numerical methods and physical models towards a full discrete approach
Jean-Paul Caltagirone
C. R. Méca (2022)