Magnetospheric ULF wave coupling in the dipole model: The impulsive excitation

The coupling of compressional and transverse hydromagnetic waves is studied in the cold and inhomogeneous outer magnetosphere. A general computer program has been developed for a dipole model. This model allows a realistic spatial variation of Alfven speed and includes dipole geometric effects. The propagation and the structure of each mode are analyzed on a two-dimensional map of a meridian plane. The properties of coupling are also investigated through time histories and wave frequency spectra. The highly spatially structured form of transverse and compressional waves is shown on the meridian plane. The theory of global compressional mode damping is compared with the numerical results. We have found a set of global modes whose spatial structure is complicated due to the inhomogeneity of the dipole geometry. These global modes are strongly coupled to field line resonances when the global mode frequency is harmonically matched to the toroidal resonant frequency. The coupling of the two modes results in relatively large-amplitude oscillations along the resonant field lines.

[1]  G. Rostoker,et al.  Latitude‐dependent characteristics of long‐period geomagnetic micropulsations , 1971 .

[2]  J. Samson,et al.  Latitude‐dependent characteristics of high‐latitude Pc 4 and Pc 5 micropulsations , 1972 .

[3]  E. Nielsen,et al.  The hydromagnetic oscillation of individual shells of the geomagnetic field , 1982 .

[4]  R. McPherron,et al.  Multispacecraft observations of the harmonic structure of Pc 3–4 magnetic pulsations , 1984 .

[5]  E. M. Poulter,et al.  Impulse-excited hydromagnetic cavity and field-line resonances in the magnetosphere , 1986 .

[6]  W. Allan,et al.  Magnetospheric coupling of hydromagnetic waves ‐ Initial results , 1985 .

[7]  Mike Warner,et al.  Time of flight calculations for high latitude geomagnetic pulsations , 1979 .

[8]  K. Glassmeier,et al.  Ionospheric Joule dissipation as a damping mechanism for high latitude ULF pulsations: Observational evidence , 1984 .

[9]  R. McPherron,et al.  Harmonic structure of Pc 3–4 pulsations , 1982 .

[10]  A. Hasegawa,et al.  A theory of long period magnetic pulsations, 3. Local field line oscillations , 1983 .

[11]  W. Hughes,et al.  Damping of geomagnetic pulsations by the ionosphere , 1978 .

[12]  A. Hasegawa,et al.  A theory of long period magnetic pulsations 1 , 1974 .

[13]  D. Southwood Some features of field line resonances in the magnetosphere , 1974 .

[14]  G. Crowley,et al.  Observational evidence of cavity modes in the Earth's magnetosphere , 1987 .

[15]  M. Kivelson,et al.  Alfven wave resonances in a realistic magnetospheric magnetic field geometry , 1981 .

[16]  H. Radoski A theory of latitude dependent geomagnetic micropulsations: The asymptotic fields , 1974 .

[17]  J. Olson,et al.  Longitudinal phase variations of Pc 4‐5 micropulsations , 1978 .

[18]  M. Kivelson,et al.  Coupling of global magnetospheric MHD eigenmodes to field line resonances , 1986 .

[19]  B. Inhester Numerical modeling of hydromagnetic wave coupling in the magnetosphere , 1987 .

[20]  R. McPherron,et al.  Geomagnetic pulsations observed simultaneously on three geostationary satellites , 1978 .

[21]  David J. Southwood,et al.  Resonant ULF waves: A new interpretation , 1985 .

[22]  H. Gough,et al.  Observations of forced oscillations of the magnetosphere by a geostationary satellite and an extensive ground magnetometer array , 1986 .

[23]  M. Kivelson,et al.  The effect of parallel inhomogeneity on magnetospheric hydromagnetic wave coupling , 1986 .

[24]  W. Allan,et al.  A dipole field model for axisymmetric alfvén waves with finite ionosphere conductivities , 1979 .

[25]  M. Kivelson,et al.  Analytic formulation and quantitative solutions of the coupled ULf wave problem , 1988 .

[26]  W. Hughes,et al.  Theory of hydromagnetic waves in the magnetosphere , 1983 .