Author(s)

Joseph E. Borovsky^1,2

¹Space Science Institute, Boulder, CO, USA.
²CSSE, University of Michigan, Ann Arbor, MI, USA.

The motional electric field of the solar wind as seen by the Earth is examined theoretically and with spacecraft measurements. As it flows outward from the sun, the solar-wind plasma carries a spatially structured magnetic field with it. To calculate the motional electric field of the solar wind the spatially structured magnetic field is Lorentz transformed; for a full physical understanding, it is also necessary to Lorentz transform the current densities and charge densities in the solar wind. Referring to Maxwell’s equations, two related questions are asked: 1) Is the source of the solar-wind motional electric field charge density in the solar wind, time derivatives of current densities in the solar wind, or both? 2) Is the solar-wind motional electric field at Earth an electrostatic field, an induction field, or a superposition of the two? A Helmholtz decomposition of the motional electric field of the solar wind is made into a divergence-origin (electrostatic) and a curl-origin (induction) electric field. The global electric field associated with the outward advection of the global Parker-spiral magnetic field is found to be electrostatic with its origin being a distributed charge density in the solar-wind plasma. The electrostatic versus induction nature of the time-varying electric field associated with the advection of mesoscale magnetic structure varies with time as differently shaped magnetic structures in the solar-wind plasma pass the Earth; the mesoscale structure of the solar-wind plasma contains sheets of space charge and sheets wherein the current density has nonzero time derivatives.

Lorentz Transformation, Electric Field, Induction, Helmholtz Decomposition, Solar Wind, Magnetic Structure, Heliosphere, Plasma

Borovsky, J. (2016) Relativity and the Solar Wind: The Maxwell-Equation Origins of the Solar-Wind Motional Electric Field. Journal of Electromagnetic Analysis and Applications, 8, 133-151. doi: 10.4236/jemaa.2016.88014.