“…However, the only different term between our system and that in [2] is the Hall term. On the other hand, we will only use the formulation of M ptq, which is same as that in [2] in our estimates. For example, we mainly use sup…”
mentioning
confidence: 82%
“…The novelty of our paper lies in that the system has the Hall term with strong nonlinearity and therefore the difference between our paper and the references [2,7,19,20] is that we will bound some new terms I i pi " 1,¨¨¨, 6q coming from the Hall term.…”
mentioning
confidence: 99%
“…When the Hall effect term rot´r ot bˆb ρ¯i s neglected, the system (1)-(5) reduces to the well-known full compressible MHD system, which has received many studies [2,8,13,14,16,17,19]. The local strong solution was obtained by Fan-Yu [13].…”
mentioning
confidence: 99%
“…The global weak solutions was obtained by Fan-Yu [14], Ducomet-Feireisl [8] and Hu-Wang [16] respectively. The low Mach number limit problem was studied by Jiang-Ju-Li [18] in T 3 for well-prepared initial data, Jiang-Ju-Li-Xin [19] in R 3 for ill-prepared initial data, and Cui-Ou-Ren [2] in a bounded domain for well-prepared initial data.…”
In this paper we study the low Mach number limit of the full compressible Hall-magnetohydrodynamic (Hall-MHD) system in T 3. We prove that, as the Mach number tends to zero, the strong solution of the full compressible Hall-MHD system converges to that of the incompressible Hall-MHD system.
“…However, the only different term between our system and that in [2] is the Hall term. On the other hand, we will only use the formulation of M ptq, which is same as that in [2] in our estimates. For example, we mainly use sup…”
mentioning
confidence: 82%
“…The novelty of our paper lies in that the system has the Hall term with strong nonlinearity and therefore the difference between our paper and the references [2,7,19,20] is that we will bound some new terms I i pi " 1,¨¨¨, 6q coming from the Hall term.…”
mentioning
confidence: 99%
“…When the Hall effect term rot´r ot bˆb ρ¯i s neglected, the system (1)-(5) reduces to the well-known full compressible MHD system, which has received many studies [2,8,13,14,16,17,19]. The local strong solution was obtained by Fan-Yu [13].…”
mentioning
confidence: 99%
“…The global weak solutions was obtained by Fan-Yu [14], Ducomet-Feireisl [8] and Hu-Wang [16] respectively. The low Mach number limit problem was studied by Jiang-Ju-Li [18] in T 3 for well-prepared initial data, Jiang-Ju-Li-Xin [19] in R 3 for ill-prepared initial data, and Cui-Ou-Ren [2] in a bounded domain for well-prepared initial data.…”
In this paper we study the low Mach number limit of the full compressible Hall-magnetohydrodynamic (Hall-MHD) system in T 3. We prove that, as the Mach number tends to zero, the strong solution of the full compressible Hall-MHD system converges to that of the incompressible Hall-MHD system.
“…It follows from that []: and thus the proof of existence is complete by taking and the standard compactness principle. The uniqueness part can be shown by the very similar calculations as that in [], and thus we omit the details here.…”
In this paper we prove the local well‐posedness and a blow‐up criterion of strong solutions for a compressible Navier‐Stokes‐P1 approximate model arising in radiation hydrodynamics, provided the initial data satisfy a natural compatibility condition. We do not assume the positivity of initial density, it may vanish in an open subset (vacuum) of Ω:=double-struckT3.
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