The J-S model versus a non-ideal MHD theory

DOI10.1016/J.PHYSLETA.2015.03.026zbMath1349.76890OpenAlexW2013819247MaRDI QIDQ341030

Roberta Nibbi, Barbara Lazzari, Franca Franchi

Publication date: 15 November 2016

Published in: Physics Letters. A (Search for Journal in Brave)

Full work available at URL: https://doi.org/10.1016/j.physleta.2015.03.026

zbMATH Keywords

magnetic reconnectionAlfvén dispersive and hyperbolic wavesJ-S type viscoelasticitynon-ideal Ohm's law

Mathematics Subject Classification ID

Viscoelastic fluids (76A10) Magnetohydrodynamics and electrohydrodynamics (76W05)

Related Items (5)

Instability thresholds for thermal convection in a Kelvin-Voigt fluid of variable order ⋮ Viscoelastic type magnetic effects and self-gravity on the propagation of MHD waves ⋮ Continuous dependence and convergence for a Kelvin-Voigt fluid of order one ⋮ Thermosolutal convection with a Navier-Stokes-Voigt fluid ⋮ Competitive double diffusive convection in a Kelvin-Voigt fluid of order one

Cites Work

• Frame indifferent formulation of Maxwell's elastic-fluid model and the rational continuum mechanics of the electromagnetic field
• Acoustic waves in a Cattaneo-Christov gas
• Uniqueness and stability results for non-linear Johnson-Segalman viscoelasticity and related models
• A viscoelastic model of blood capillary extension and regression: derivation, analysis, and simulation
• Mathematical models for the non-isothermal Johnson-Segalman viscoelasticity in porous media: stability and wave propagation
• Continuous Dependence on the Heat Source in Resonant Porous Penetrative Convection
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