Skip to main content
. 2018 Jul 20;39(5):817–859. doi: 10.1007/s10712-018-9487-x

Table 3.

Plasma-wave populations in the magnetospheric system

Type Location Properties Typical period (s) or frequency (Hz)
ULF waves Dipolar region Driven by Kelvin–Helmholtz
Driven by solar-wind compressions
Driven by ion plasma sheet
Produce radial diffusion of electron radiation belt
Energize radiation belt
100–600 s
Electromagnetic ion-cyclotron waves (EMIC) Dipolar region inside plasmasphere and plume Driven by ion plasma sheet
Scatter plasma-sheet ions and radiation-belt electrons into atmosphere
0.2–5 s
Whistler-mode chorus waves Dipolar region outside of plasmasphere Driven by substorm-injected electrons
Energize the electron radiation belt
Scatter plasma-sheet and radiation-belt electrons into atmosphere
Produce diffuse aurora
100–5000 Hz
Whistler-mode hiss waves Dipolar region inside plasmasphere and plume Driven by electron plasma sheet?
Scatter radiation-belt electrons into atmosphere
100–5000 Hz
Lightning-generated whistler waves Dipolar region close to Earth Associated with lightning occurrence
Scatter radiation-belt electrons into atmosphere
100–10,000 Hz
Kelvin–Helmholtz
oscillations
Magnetopause Driven by magnetosheath flow
Transport plasma from magnetosheath into magnetosphere
Transport momentum into magnetosphere to produce magnetospheric convection
Produce ULF waves in dipolar region
80–700 s
Magnetosonic waves (equatorial noise) Dipolar region Driven by ion plasma sheet
Energize the electron radiation belt
20–150 Hz
Alfven waves Throughout the magnetosphere Initiate electrical currents that couple the motions of plasmas 60–500 s