The speeds of coronal mass ejection events

The outward speeds of mass ejection events observed with the white light coronagraph experiment on Skylab varied over a range extending from less than 100 km s−1 to greater than 1200 km s−1. For all events the average speed within the field of view of the experiment (1.75 to 6 solar radii) was 470 km s−1. Typically, flare associated events (Importance 1 or greater) traveled faster (775 km s−1) than events associated with eruptive prominences (330 km s−1); no flare associated event had a speed less than 360 km s−1, and only one eruptive prominence associated event had a speed greater than 600 km s−1. Speeds versus height profiles for a limited number of events indicate that the leading edges of the ejecta move outward with constant or increasing speeds.Metric wavelength type II and IV radio bursts are associated only with events moving faster than about 400 km s−1; all but two events moving faster than 500 km −1 produced either a type II or IV radio burst or both. This suggests that the characteristic speed with which MHD signals propagate in the lower (1.1 to 3 solar radii) corona, where metric wavelength bursts are generated, is about 400 to 500 km s−1. The fact that the fastest mass ejection events are almost always associated with flares and with metric wavelength type II and IV radio bursts explains why major shock wave disturbances in the solar wind at 1 AU are most often associated with these forms of solar activity rather than with eruptive prominences.

[1]  S. Smerd,et al.  80 MHz Radioheliograph Evidence on Moving Type IV Bursts and Coronal Magnetic Fields , 1971 .

[2]  D. Smith PLASMA RADIATION FROM COLLISIONLESS MHD SHOCK WAVES. III. TYPE II SOLAR RADIO BURSTS. , 1972 .

[3]  J. Warwick Flare-Connected Prominences. , 1957 .

[4]  Observations of coronal disturbances from 1 to 9 solar radii. I - First event of 1973 January 11 , 1974 .

[5]  R. Stewart,et al.  Observation of a Coronal Disturbance from 1 to 9 R , 1974 .

[6]  R. Howard,et al.  The coronal transient of 16 June 1972 , 1974 .

[7]  J. D. Bohlin,et al.  The sources of material comprising a mass ejection coronal transient , 1975 .

[8]  R. Robinson,et al.  Coronal disturbances , 1973 .

[9]  R. MacQueen,et al.  Mass ejections from the Sun: A view from Skylab , 1974 .

[10]  A. Hundhausen,et al.  Coronal Expansion and Solar Wind , 1972 .

[11]  R. E. Marshak,et al.  Interplanetary Dynamical Processes , 1963 .

[12]  J. Chao,et al.  A correlative study of ssc's, interplanetary shocks, and solar activity , 1974 .

[13]  A. Poland,et al.  Direct observations of a flare related coronal and solar wind disturbance , 1975 .

[14]  A. Hundhausen,et al.  Numerical simulation of flare‐generated disturbances in the solar wind , 1969 .

[15]  R. Hansen,et al.  ABRUPT DEPLETIONS OF THE INNER CORONA , 1974 .

[16]  E. Hildner,et al.  The outer solar corona as observed from Skylab - Preliminary results , 1974 .

[17]  R. MacQueen,et al.  The large coronal transient of 10 June 1973 , 1975 .