The electron velocity distribution in the high-speed solar wind: Modeling the effects of protons

The evolution of the electron velocity distribution function (VDF) in high- speed solar wind streams is modeled taking the expanding geometry, the pola rization electric field, and Coulomb collisions into account. The VDF we fi nd at the orbit of Mercury is composed of an isotropic, collision-dominated core, a trapped, anisotropic population called "halo" in this study, and a narrow, high-energy "strahl" that escapes along the magnetic field. The di stribution function is very similar to the electron VDF observed in the low -density, high-speed solar wind by Pilipp et al. [1987] and Phillips et al. [1989]. The main features of the VDF can be obtained by considering only e lectron self-collisions; the effect of proton collisions is to make the dis tribution function more isotropic. At low energies, collisions with protons dominate the angular scattering, but electron self-collisions alone are fr equent enough to keep the core of the distribution function quite isotropic . The expanding geometry produces an anisotropic halo and a narrow strahl. The angular scattering by protons reduces the anisotropy of the trapped hal o particles and broadens the lower-energy part of the strahl. Along the mag netic field the resulting electron velocity distribution is composed of a r elatively cold core and a halo-strahl spectrum that is "flatter" than the c oronal spectrum. The two-temperature electron distribution function often o bserved in the solar wind may therefore be produced by Coulomb collisions a nd should not be taken as a "proof" of a non-Maxwellian (two-temperature) d istribution function in the corona,