Standing waves at low Mach number laminar bow shocks. [earth-solar wind interaction

Explorer 43 data have been used to study 34 bow shock crossings observed from 5 to 16 RE upstream from the average bow shock location. These shocks have magnetosonic Mach numbers between 1.2 and 2.0, and they display particularly simple laminar structures. In 17 of these cases waves are detected adjacent to and upstream of the shock with amplitudes ranging up to ΔB/B ≃ 1 and period ranging from 6 to 130 s. A variance analysis of the magnetic field data reveals that the vectors of these waves are oriented along the shock normals. The wave polarization relative to the average field direction is right-handed when the crossing is from the interplanetary medium to the magnetosheath but is left-handed when the crossing is made in the opposite direction. On the basis of these observations the waves are identified as the standing whistler waves that have been predicted by the theory of low Mach number oblique shocks. The observed amplitude and the occasional lack of waves are in general agreement with theory, which predicts that decreasing amplitudes should correspond to larger field-shock normal angles and lower plasma betas. Variations in the observed frequencies can be explained by changes in the wavelength of the standing wave as upstream parameters change. Shock velocities calculated from theoretical wavelengths typically range from 10 to 30 km/s, but in one instance the velocity was 150 km/s.

[1]  C. Russell,et al.  Structure of the quasi-perpendicular laminar bow shock. [earth-solar wind interaction , 1975 .

[2]  D. Fairfield Whistler waves observed upstream from collisionless shocks , 1974 .

[3]  D. Biskamp Collisionless shock waves in plasmas , 1973 .

[4]  J. Scudder,et al.  Electron observations in the solar wind and magnetosheath , 1973 .

[5]  V. Formisano,et al.  Solar wind interaction with the Earth's magnetic field: 3. On the Earth's bow shock structure , 1973 .

[6]  W. Feldman,et al.  Double ion streams in the solar wind , 1973 .

[7]  C. Russell,et al.  Study of waves in the earth's bow shock. , 1972 .

[8]  C. Russell,et al.  Large-scale coherence and high velocities of the earth's bow shock on February 12, 1969. , 1972 .

[9]  J. Marburger,et al.  Ogo 5 magnetic‐field data near the Earth's bow shock: A correlation with theory , 1972 .

[10]  V. Formisano,et al.  Observations of Earth's bow shock for low mach numbers , 1971 .

[11]  D. H. Fairfield,et al.  Average and unusual locations of the Earth's magnetopause and bow shock , 1971 .

[12]  V. Formisano,et al.  Solar wind and location of shock front and magnetopause at the 1969 solar maximum , 1970 .

[13]  T. Northrop,et al.  STATIONARY WAVES PRODUCED BY THE EARTH'S BOW SHOCK. , 1970 .

[14]  A. E. Robson,et al.  OBLIQUE HYDROMAGNETIC SHOCK WAVES. , 1969 .

[15]  H. E. Taylor Sudden commencement associated discontinuities in the interplanetary magnetic field observed by IMP 3 , 1969 .

[16]  I. M. Green,et al.  Earth's Bow Shock: Elapsed-Time Observations by Two Closely Spaced Satellites , 1968, Science.

[17]  T. Skillman,et al.  OGO-A magnetic field observations , 1967 .

[18]  R. Kaufmann Shock observations with the Explorer 12 magnetometer , 1967 .

[19]  D. Colburn,et al.  Discontinuities in the solar wind , 1966 .

[20]  E. Smith,et al.  Preliminary results from the Ogo 1 Search Coil Magnetometer: Boundary positions and magnetic noise spectra , 1966 .

[21]  Heinrich J. Völk,et al.  Motions of the bow shock induced by interplanetary disturbances , 1974 .

[22]  A. E. Robson,et al.  INSTABILITY OF THE WHISTLER STRUCTURE OF OBLIQUE HYDROMAGNETIC SHOCKS. , 1972 .

[23]  M. L. Sloan Instability of Whistler‐Dominated Laminar Shocks , 1971 .

[24]  A. Summers,et al.  External aerodynamics of the magnetosphere , 1968 .