2013
DOI: 10.1016/s0252-9602(13)60046-6
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Energy dissipation for weak solutions of incompressible MHD equations

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Cited by 14 publications
(12 citation statements)
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“…From (3.5), we can easily prove another conclusion about the total energy balance. Referring to Gao et al, 11 the total energy E(t) is Proof. To prove our corollary, we need to prove for arbitrary (t) ∈ C ∞ 0 (0, T), there is…”
Section: Then the System Satisfies The Following Local Energy Equatimentioning
confidence: 95%
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“…From (3.5), we can easily prove another conclusion about the total energy balance. Referring to Gao et al, 11 the total energy E(t) is Proof. To prove our corollary, we need to prove for arbitrary (t) ∈ C ∞ 0 (0, T), there is…”
Section: Then the System Satisfies The Following Local Energy Equatimentioning
confidence: 95%
“…From (), we can easily prove another conclusion about the total energy balance. Referring to Gao et al, 11 the total energy E ( t ) is E(t)=12𝕋3ρ|u|2dx+𝕋3P(ρ)dx+12μ𝕋3|B|2dx+1μ2σ0t𝕋3|B|2dx. …”
Section: Energy Conservation For Compressible Isentropic Mhd Equationsmentioning
confidence: 99%
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“…Whether the energy equality holds for weak solutions or is connected to the fundamental problem is an open problem. There are also extensions, [10], of the results of Duchon and Robert [7] to MHD flows. These yield existence of a non negative operator (in effect) filling in possible gaps between the energy equality and inequality.…”
Section: The Ensemble Averaged Mhd Systemmentioning
confidence: 99%
“…Remark 3.1 Just as for non-conducting fluids, the energy equality is known to hold for strong solutions and for slightly more regular weak solutions [5], [10]. Whether the energy equality holds for weak solutions or is connected to the fundamental problem is an open problem.…”
Section: The Ensemble Averaged Mhd Systemmentioning
confidence: 99%