A two-dimensional Alfvén wave-driven solar wind model with proton temperature anisotropy

Details A two-dimensional Alfvén wave-driven solar wind model with proton temperature anisotropy A two-dimensional Alfvén wave-driven solar wind model with proton temperature anisotropy

Jul 2004

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2004jgra..10907103l&link_type=abstract

Journal of Geophysical Research, Volume 109, Issue A7, CiteID A07103

Physics

Plasma Physics

6

Interplanetary Physics: Sources Of The Solar Wind, Space Plasma Physics: Numerical Simulation Studies, Interplanetary Physics: Solar Wind Plasma, Interplanetary Physics: Plasma Waves And Turbulence

Scientific paper

We present the first two-dimensional (2-D) Alfvén wave turbulence-driven solar wind model which takes the proton temperature anisotropy into account. While the modeled proton temperature anisotropy in the fast solar wind is established in the inner corona and yields Tp$\parallel$/Tp$\perp$ = 0.57 at 1 AU, which is comparable to measured values, Tp$\parallel$ and Tp$\perp$ are only about half the observed values. In the slow wind, on the other hand, the modeled values for Tp$\parallel$ and Tp$\perp$ as well as their ratio are close to those measured in interplanetary space. Curiously, the dip in the velocity that develops near the cusp at the top of the helmet streamer reduces the effect of transverse expansion and leads to a realistic electron temperature in the slow wind at 1 AU, although no explicit external heating is applied to electrons. Comparison with models with and without proton temperature anisotropy shows that by allowing the proton temperature anisotropy to develop, the average proton temperature is lower than the isotropic case primarily because of the cooling in the direction parallel to the magnetic field. These results imply that ion cyclotron resonance models with isotropic proton temperature are somewhat optimistic in assessing the role of Alfvén wave turbulence in driving the fast solar wind. Inclusion of the temperature anisotropy of protons and proton thermal conduction are necessary for any physically realistic model.

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