EGU25-9622, updated on 14 Mar 2025
https://doi.org/10.5194/egusphere-egu25-9622
EGU General Assembly 2025
© Author(s) 2025. This work is distributed under
the Creative Commons Attribution 4.0 License.
Oral | Monday, 28 Apr, 09:15–09:35 (CEST)
 
Room 1.34
Decay of magnetohydrodynamic turbulence in the expanding solar wind: WIND observations
Andrea Verdini1,2, Petr Hellinger4,5, Simone Landi1,2, Roland Grappin7,8, Victor Montagud-Camps6, and Emanuele Papini3
Andrea Verdini et al.
  • 1Università di Firenze, Dipartimento di Fisica e Astronomia, Sesto Fiorentino, Italy (andrea.verdini@unifi.it)
  • 2Inaf, Osservatorio Astrofisico di Arcetri, Firenze, Italy
  • 3INAF–Istituto di Astrofisica e Planetologia Spaziali, Roma, Italy
  • 4Astronomical Institute of the Czech Academy of Sciences, Prague, Czech Republic
  • 5Institute of Atmospheric Physics of the Czech Academy of Sciences, Prague, Czech Republic
  • 6Department of Electromagnetism and Electronics, University of Murcia, Murcia, Spain
  • 7Laboratoire de Physique des Plasmas (LPP), École Polytechnique, Rte de Saclay, 91120 Palaiseau, France
  • 8CNRS, Observatoire de Paris, Sorbonne Université, Université Paris Saclay, Ecole Polytechnique, Institut Polytechnique de Paris, F-91120 Palaiseau, France

We have studied the decay of turbulence in the solar wind. Fluctuations carried by the expanding wind are naturally damped because of flux conservation, slowing down the development of a turbulent cascade. The latter also damps fluctuations but results in plasma heating. We analyzed time series of the velocity and magnetic field (v and B, respectively) obtained by the WIND spacecraft at 1 au. Fluctuations were recast in terms of the Elsasser variables, z± = v ± B/√4πρ, with ρ being the average density, and their second- and third-order structure functions were used to evaluate the Politano-Pouquet relation, modified to account for the effect of expansion.

We find that expansion plays a major role in the Alfvénic stream, those for which z+ ≫ z‑. In such a stream, expansion damping and turbulence damping act, respectively, on large and small scales for z+, and also balance each other. Instead, z‑ is only subject to a weak turbulent damping because expansion is a negligible loss at large scales and a weak source at inertial range scales.

These properties are in qualitative agreement with the observed evolution of energy spectra that is described by a double power law separated by a break that sweeps toward lower frequencies for increasing heliocentric distances. However, the data at 1 au indicate that injection by sweeping is not enough to sustain the turbulent cascade. We derived approximate decay laws of energy with distance that suggest possible solutions for the inconsistency: in our analysis, we either overestimated the cascade of z± or missed an additional injection mechanism; for example, velocity shear among streams.

How to cite: Verdini, A., Hellinger, P., Landi, S., Grappin, R., Montagud-Camps, V., and Papini, E.: Decay of magnetohydrodynamic turbulence in the expanding solar wind: WIND observations, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-9622, https://doi.org/10.5194/egusphere-egu25-9622, 2025.