2001
DOI: 10.1029/2000ja000389
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Relationships of models of the inner magnetosphere to the Rice Convection Model

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Cited by 24 publications
(44 citation statements)
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“…This discrepancy is, in large part, a symptom of the ''pressure balance inconsistency'', i.e., the fact that statistical models indicate that the specific entropy, PV 5/3 (where V = R ds/B is the flux tube volume, and P is the pressure), typically increases strongly and monotonically with distance from Earth [Erickson and Wolf, 1980]. This is inconsistent with adiabatic drift theory, which implies that P s V 5/3 is conserved along a drift path for particles in strong, elastic pitch-angle scattering, if losses are negligible [Heinemann and Wolf, 2001]; here P s is the partial pressure due to particles with isotropic energy invariant l s = W K V 2/3 , and W K = kinetic energy. , convection models therefore compress the plasma to unnaturally high densities and energies during earthward convection.…”
Section: Introductioncontrasting
confidence: 49%
“…This discrepancy is, in large part, a symptom of the ''pressure balance inconsistency'', i.e., the fact that statistical models indicate that the specific entropy, PV 5/3 (where V = R ds/B is the flux tube volume, and P is the pressure), typically increases strongly and monotonically with distance from Earth [Erickson and Wolf, 1980]. This is inconsistent with adiabatic drift theory, which implies that P s V 5/3 is conserved along a drift path for particles in strong, elastic pitch-angle scattering, if losses are negligible [Heinemann and Wolf, 2001]; here P s is the partial pressure due to particles with isotropic energy invariant l s = W K V 2/3 , and W K = kinetic energy. , convection models therefore compress the plasma to unnaturally high densities and energies during earthward convection.…”
Section: Introductioncontrasting
confidence: 49%
“…A slightly more complicated (but more realistic) way to view the same phenomenon is through the use of a bounce‐averaged drift formalism. If one uses this formalism but also assumes that strong, elastic pitch angle scattering keeps the distribution function isotropic, then the distribution function f (λ, , t ) is constant along a drift path, where is the isotropic energy invariant, and E is the particle's kinetic energy [ Wolf , 1983; Heinemann and Wolf , 2001]. The assumption of isotropy is reasonable in the middle plasma sheet, beyond the “isotropy boundary” [e.g., Sergeev et al , 1993], because chaotic motion in the current sheet keeps the distribution roughly isotropic [ Stiles et al , 1978], but it becomes less realistic close to the Earth.…”
Section: Introductionmentioning
confidence: 99%
“…This procedure effectively amounts to a single fluid reduction. In this paper we show that this implied procedure can be written explicitly as an a priori energy transport equation with a nonzero heat flux as suggested by Heinemann and Wolf [2001]. The chief benefit of this theory is that it provides a computationally more efficient way to tackle the convection problem.…”
Section: Introductionmentioning
confidence: 99%