Physics
Scientific paper
Dec 2004
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2004agufmsm41a1118f&link_type=abstract
American Geophysical Union, Fall Meeting 2004, abstract #SM41A-1118
Physics
2149 Mhd Waves And Turbulence, 2471 Plasma Waves And Instabilities, 2483 Wave/Particle Interactions
Scientific paper
The radial diffusion coefficient of particles in a symmetric magnetic field perturbed by fluctuating electric fields is well known to depend on the power spectral density of the electric field at frequencies ω = m ω d (where m is the azimuthal mode number, ω d is the particle drift frequency) with an L6 factor. In this work we have derived a radial diffusion coefficient for particles in an asymmetric magnetic field. The asymmetric diffusion coefficient depends on electric field power at resonance frequencies ω = (m ± 1) ω d with L12 dependence multiplying the power spectral density. Numerical diffusion rates obtained using test-particle simulations in model fields agree well with the analytical diffusion coefficients. Solutions of the radial diffusion equation for the September 1998 storm event are compared to an MHD-particle simulation. Earlier calculations used only electric-field diffusion coefficients, which had to be increased by a factor of 2 to 3 to get the best match with the MHD-particle results. New results will be presented of a radial diffusion calculation with compressional ULF waves added.
Chan Anthony A.
Elkington Scot R.
Fei Yingwei
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