
Switchbacks in the Solar Magnetic Field: Their Evolution, Their Content, and Their Effects on the Plasma
Author(s) -
F. S. Mozer,
Oleksiy Agapitov,
S. D. Bale,
J. W. Bonnell,
A. W. Case,
C. C. Chaston,
D. W. Curtis,
T. Dudok de Wit,
K. Goetz,
K. Goodrich,
P. Harvey,
J. C. Kasper,
K. E. Korreck,
V. Krasnoselskikh,
D. E. Larson,
R. Livi,
R. J. MacDowall,
D. Malaspina,
M. Pulupa,
Michael L. Stevens,
P. L. Whittlesey,
J. R. Wygant
Publication year - 2020
Publication title -
the astrophysical journal. supplement series/astrophysical journal. supplement series
Language(s) - English
Resource type - Journals
eISSN - 1538-4365
pISSN - 0067-0049
DOI - 10.3847/1538-4365/ab7196
Subject(s) - poynting vector , physics , plasma , solar wind , magnetic field , flux (metallurgy) , magnetohydrodynamic drive , magnetohydrodynamics , amplitude , mechanics , computational physics , optics , materials science , quantum mechanics , metallurgy
Switchbacks (rotations of the magnetic field) are observed on the Parker Solar Probe . Their evolution, content, and plasma effects are studied in this paper. The solar wind does not receive a net acceleration from switchbacks that it encountered upstream of the observation point. The typical switchback rotation angle increased with radial distance. Significant Poynting fluxes existed inside, but not outside, switchbacks, and the dependence of the Poynting flux amplitude on the switchback radial location and rotation angle is explained quantitatively as being proportional to ( B sin( θ )) 2 . The solar wind flow inside switchbacks was faster than that outside due to the frozen-in ions moving with the magnetic structure at the Alfvén speed. This energy gain results from the divergence of the Poynting flux from outside to inside the switchback, which produces a loss of electromagnetic energy on switchback entry and recovery of that energy on exit, with the lost energy appearing in the plasma flow. Switchbacks contain 0.3–10 Hz waves that may result from currents and the Kelvin–Helmholtz instability that occurs at the switchback boundaries. These waves may combine with lower frequency magnetohydrodynamic waves to heat the plasma.