A system of partial differential equations models the magneto-hydrodynamics of an ideal fluid in a bounded time-space domain Q =(0, \tau) × B_R[O] endowed with Euclidean metric and having M=3 space dimensions. The equations describe conservation of mass, conservation of momentum and magnetic induction. The {mass, momentum} equations correspond to the {time, space} divergence (Div[·]) of a 4 × 4 tensor denoted A_{Euler}, which is real valued, symmetric and positive definite, provided the terms depending on the magnetic field, \vec H, are moved to the right side. By assuming the existence of a solution to some initial-boundary value problem, a property known as the “higher integrability” of det[A_{Euler}] is investigated. Articles by D. SERRE from 2018 onwards [Divergence-free positive symmetric tensors and fluid dynamics. Ann. I. H. Poincaré - Analyse Non-lineaire. 2018; AN 35:1209-1234] motivated this work. Letting Φ := p + ρ_f φ, with p pressure, ρ_f density and φ (>0) the potential of external forces, one has det[A_{Euler}] = Φ^M ρ_f . If the entries of A_{Euler} are in L^1(Q), then higher integrability consists of ρ_f^{1/M}Φ ∈ L^1(Q) and holds provided Div[A_{Euler}] has finite total mass in Q. Higher integrability thus affects p and ρ_f , leaving out velocity, \vec u and \vec H. If a solution {ρ_f , p, \vec u, \vec H } were known to exist and comply with a number of requirements, then higher integrability would mean continuous dependence of ρ_f^{1/M}Φ on \vec H. In the absence of information about existence, the L^1(Q)-estimate is a qualitative result about the dynamical system: a property of the solution is inferred from that of det[A_{Euler}]. Many problems are still open, some of which are stated.
Crosta, G. (2021). Higher integrability of a determinant related to a system of magneto-hydrodynamic equations [Working paper].
Higher integrability of a determinant related to a system of magneto-hydrodynamic equations
Crosta, GFF
2021
Abstract
A system of partial differential equations models the magneto-hydrodynamics of an ideal fluid in a bounded time-space domain Q =(0, \tau) × B_R[O] endowed with Euclidean metric and having M=3 space dimensions. The equations describe conservation of mass, conservation of momentum and magnetic induction. The {mass, momentum} equations correspond to the {time, space} divergence (Div[·]) of a 4 × 4 tensor denoted A_{Euler}, which is real valued, symmetric and positive definite, provided the terms depending on the magnetic field, \vec H, are moved to the right side. By assuming the existence of a solution to some initial-boundary value problem, a property known as the “higher integrability” of det[A_{Euler}] is investigated. Articles by D. SERRE from 2018 onwards [Divergence-free positive symmetric tensors and fluid dynamics. Ann. I. H. Poincaré - Analyse Non-lineaire. 2018; AN 35:1209-1234] motivated this work. Letting Φ := p + ρ_f φ, with p pressure, ρ_f density and φ (>0) the potential of external forces, one has det[A_{Euler}] = Φ^M ρ_f . If the entries of A_{Euler} are in L^1(Q), then higher integrability consists of ρ_f^{1/M}Φ ∈ L^1(Q) and holds provided Div[A_{Euler}] has finite total mass in Q. Higher integrability thus affects p and ρ_f , leaving out velocity, \vec u and \vec H. If a solution {ρ_f , p, \vec u, \vec H } were known to exist and comply with a number of requirements, then higher integrability would mean continuous dependence of ρ_f^{1/M}Φ on \vec H. In the absence of information about existence, the L^1(Q)-estimate is a qualitative result about the dynamical system: a property of the solution is inferred from that of det[A_{Euler}]. Many problems are still open, some of which are stated.File | Dimensione | Formato | |
---|---|---|---|
Integrabili04.pdf
Solo gestori archivio
Descrizione: Dattiloscritto accettato per la pubblicazione ma non ancora pubblicato
Tipologia di allegato:
Submitted Version (Pre-print)
Licenza:
Tutti i diritti riservati
Dimensione
212.89 kB
Formato
Adobe PDF
|
212.89 kB | Adobe PDF | Visualizza/Apri Richiedi una copia |
I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.