Skip to end of metadata
Go to start of metadata

Compressional Pc 5

Compressional Pc 5 pulsations (plasma waves), found on the nightside close to the flanks of the Earth's magnetosphere, are the dominant pulsations occurring beyond L=8. The compressional (along magnetic field) perturbation of the wave is often accompanied by a comparable radial perturbation, amplitude of the oscillations being large with periods of 5 to 10 minutes. These waves are, most likely, locally generated drift mirror waves driven by positive plasma pressure anisotropy. Accordingly, the events are strongly associated with high beta plasma clouds and are much more likely to be observed near the equator than >10° off the equator (see, e.g., Anderson, 1993). The azimuthal wavelength of the waves is short, m = 50-100, and the particle signatures associated with the waves show anti-phase correlation between the ion and magnetic field pressures.

The dusk and dawn compressional Pc 5 occur under quite different geophysical conditions. While the evening side events occur during enhanced ring current, high AE index, and strongly southward IMF ("storm time Pc 5" related to the substorm particle injection), the dawnside events occur during small negative Dst (weak ring current), low AE, and northward IMF. The dusk side waves propagate westward with the speeds comparable to energetic (10-30 keV) proton drift speed, while the dawn side events propagate eastward because of the general drift direction: in plasma frame they propagate westward (see, e.g., Anderson, 1994).

Toroidal Pc 5

Azimuthally polarized toroidal Pc 5 pulsations are thought to be fundamental mode toroidal field line resonances (FLR) with magnetic node at the equator. They are considered to be a separate phenomena from the multi-harmonics (discussed in the Pc 3 section) because of the difference in occurrence distribution: toroidal Pc 5 are found close to the flanks of the magnetosphere either both at dawn and dusk (as derived from some ground based studies), or only at dawn side (as derived from satellite measurements). The reason for this discrepancy is still not known, but it can be that the toroidal waves present at dusk are just more difficult to separate (by satellite measurements) from other waves occuring there. (To make things even more complicated, electric field measurements of the waves have shown a broad dayside distribution!) However, because the occurrence rate increases monotonically with L, the energy source of the waves is though to be near the magnetopause boundary. Some measurements support the idea that some form of wave structure commonly propagates anti-sunward at the flanks producing undulating motions of the magnetopause boundary. The present theories for the wave generations are:

  • Kelvin-Helmholtz instability (KHI)
    • KHI at the magnetopause can generate boundary surface waves when the magnetosheath plasma flow velocity exceeds a threshold velocity (e.g., Cahill and Winckler, 1992)
  • Pressure variations
    • Pressure variations in the magnetosheath plasma flow can create magnetopause surface waves. For example, solar wind pressure pulses can produce compressional (fast mode) Alfven waves, which can couple and mode convert into shear Alfven waves at the point where the compressional wave frequency matches the shear mode eigenfrequency of the field line; see MHD waves. See, e.g., Warnecke (1990), Lysak and Lee (1992).
  • Local magnetic anomalies
    • For example, flux-transfer events (FTE) or other intermittent reconnection (or plasma penetration) processes may be associated with magnetopause boundary waves (e.g., Cahill and Winckler, 1992).

Also the nightside injections of electrons seem to have an effect on these Pc 5 waves (e.g., Saka et al., 1992).

The only found relation between toroidal Pc 5 and the solar wind/IMF conditions is that stronger events occur during higher average solar wind velocity. This may, however, be only a magnetospheric compression effect (the source of the waves comes closer to the measurement point). Besides, increasing power with solar wind velocity and density is found for all other pulsations as well, even those driven by local ion instabilities, so this correlation does not tell much about the source mechanism for the waves. See, e.g., Anderson (1994).

When measured from the ground, the toroidal Pc 5 pulsations show a 90 degrees counter clockwise rotation of the magnetic field variation due to modifications in the ionosphere (Hughes, 1974). For a recent study of ground based Pc 5 pulsations measurements, see Chisman and Orr (1997).

Transients

Nightside transient toroidal waves at Pc 3-5 frequency range have been observed (Takahashi et al., 1996).

Aurora related

Various ground-based measurements have shown that some auroral features correlate with non-FLR wave activity at Pc 5 frequncy range (Elphinstone, ICS-3).

References

  • Anderson, B. J., Statistical studies of Pc 3-5 pulsations and their relevance for possible source mechanisms of ULF waves, Ann. Geophysicae, 11, 128-143, 1993.
  • Anderson, B. J., An overview of spacecraft observations of 10 s to 600 s period magnetic pulsations in the Earth's magnetosphere, in Solar Wind Sources of Magnetospheric Ultra-Low-Frequency Waves, eds. M. J. Engebretson, K. Takahashi, and M. Scholer, AGU Geophysical Monograph 81, 25-43, 1994.
  • Cahill, L. J. Jr. and J. R. Winckler, Periodic magnetopause oscillations observed with the GOES satellites on March 24, 1991, J. Geophys. Res., 97, 8239-8243, 1992.
  • Chisham, G., and D. Orr, A statistical study of the local time asymmetry of Pc 5 ULF wave characteristics observed at midlatitudes by SAMNET, J. Geophys. Res., 102, 24339-24350, 1997.
  • Hughes, W. J., The effect of the atmosphere and ionosphere on long period magnetospheric micropulsations, Planet. Space Sci., 22, 1157-1172, 1974.
  • Lysak, R. L. and D. Lee, Response of the dipole magnetosphere to pressure pulses, Geophys. Res. Lett., 19, 937-940, 1992.
  • Potemra, T. A., and L. G. Blomberg, A survey of Pc 5 pulsations in the dayside high-latitude regions observed by Viking, J. Geophys. Res., 101, 24801-24813, 1996.
  • Saka, O., T. Iijima, H. Yamagishi, N. Sato, and D. N. Baker, Excitation of Pc 5 pulsations in the morning sector by a local injection of particles in the magnetosphere, J. Geophys. Res., 97, 10693-10701, 1992.
  • Takahashi, K., B. J. Anderson, and S. Ohtani, Multisatellite study of nightside transient toroidal waves, J. Geophys. Res., 101, 24815-24825, 1996.
  • Warnecke, J., H. Lühr, and K. Takahashi, Observational features of field line resonances excited by solar wind pressure variations on 4 September 1984, Planet. Space Sci., 38, 1517-1531, 1990.
  • No labels