1986
DOI: 10.1093/mnras/223.2.353
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On the stability of shocks modified by particle acceleration

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Cited by 182 publications
(151 citation statements)
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“…Two-fluid model. The two-fluid model uses the diffusiveconvection equation, coupled with the gas dynamic equations, to simulate the CR's acceleration as a gas component and an accelerated particle component (Drury & Falle 1986;Dorfi 1990;Jones & Kang 1992). Since the CR energy density is solved A&A 530, A92 (2011) instead of the particle's distribution function in this model, the simulation results are based on some assumptions, such as the CR's adiabatic index, averaged diffusive coefficient, and injection rate.…”
Section: Introductionmentioning
confidence: 99%
“…Two-fluid model. The two-fluid model uses the diffusiveconvection equation, coupled with the gas dynamic equations, to simulate the CR's acceleration as a gas component and an accelerated particle component (Drury & Falle 1986;Dorfi 1990;Jones & Kang 1992). Since the CR energy density is solved A&A 530, A92 (2011) instead of the particle's distribution function in this model, the simulation results are based on some assumptions, such as the CR's adiabatic index, averaged diffusive coefficient, and injection rate.…”
Section: Introductionmentioning
confidence: 99%
“…The acoustic instability of Drury and Falle (1986) driven by the CR-pressure gradient is also anisotropic. The strong anisotropy of the magnetic turbulence is observed in the solar wind where the outward flux significantly exceeds the ingoing one.…”
Section: Collisionless Heating Of Ions and Electrons By Magnetic Turbmentioning
confidence: 99%
“…Drury & Falle 1986). x is the spatial coordinate, u is the mean speed of thermal particles, γ c is an adiabatic constant equal to 4/3 for ultrarelativistic cosmic rays, χ is a spatial diffusion coefficient, and P c is the cosmic ray pressure.…”
Section: A One Dimensional Two-fluid Descriptionmentioning
confidence: 99%