Heliospheric tomography using interplanetary scintillation observations: 2. Latitude and heliocentric distance dependence of solar wind structure at 0.1–1 AU

Interplanetary scintillation is a useful means to measure the solar wind in regions inaccessible to in situ observation. However, interplanetary scintillation measurements involve a line-of-sight integration, which relates contributions from all locations along the line of sight to the actual observation. We have developed a computer assisted tomography (CAT) program to reduce the adverse effects of the line-of-sight integration. The program uses solar rotation and solar wind motion to provide three-dimensional perspective views of each point in space accessible to the interplanetary scintillation observations and optimizes a three-dimensional solar wind speed distribution to fit the observations. We analyzed IPS speeds observed at the Solar-Terrestrial Environment Laboratory and confirmed that (1) the solar wind during the solar minimum phase has a dominant polar high-speed solar wind region with speeds of about 800 km s−1 and within 30° of the solar equator speeds decrease to 400 km s−1 as observed by Ulysses, and (2) high-speed winds get their final speed of 750–900 km s−1 within 0.1 AU, and consequently, that acceleration of the solar wind is small above 0.1 AU.

[1]  Hiroaki Misawa,et al.  Multi-Station System for Solar Wind Observations Using the Interplanetary Scintillation Method , 1995 .

[2]  M. Kojima,et al.  Solar cycle evolution of solar wind speed structure between 1973 and 1985 observed with the interplanetary scintillation method , 1987 .

[3]  G. Woan,et al.  Synoptic IPS and Yohkoh soft X‐ray observations , 1995 .

[4]  P. J. Williams,et al.  Rapid acceleration of the polar solar wind , 1996, Nature.

[5]  B. Rickett,et al.  Evolution of the solar wind structure over a solar cycle: Interplanetary scintillation velocity measurements compared with coronal observations , 1991 .

[6]  S. Suess,et al.  Ulysses solar wind plasma observations from pole to pole , 1995 .

[7]  P. K. Manoharan,et al.  3. Correlation between speed and electron density fluctuations in the solar wind , 1998 .

[8]  J. R. Jokipii,et al.  On the relation between the pattern and wind velocities in interplanetary scintillations. , 1973 .

[9]  J. Harmon,et al.  Propagation observations of the solar wind near the sun , 1989 .

[10]  M. Kojima,et al.  Solar cycle dependence of global distribution of solar wind speed , 1990 .

[11]  P. K. Manoharan Three-dimensional structure of the solar wind: Variation of density with the solar cycle , 1993 .

[12]  J. King,et al.  Solar radio burst and in situ determination of interplanetary electron density , 1983 .

[13]  B. Jackson,et al.  Heliospheric tomography using interplanetary scintillation observations. 1. Combined Nagoya and Cambridge data , 1998 .

[14]  A. T. Young INTERPRETATION OF INTERPLANETARY SCINTILLATIONS. , 1971 .

[15]  J. D. Sullivan,et al.  Comparison of 74‐MHZ interplanetary scintillation and Imp 7 observations of the solar wind during 1973 , 1978 .

[16]  J. Harmon,et al.  The solar wind density spectrum near the Sun: Results from Voyager radio measurements , 1991 .

[17]  W. A. Coles,et al.  Solar wind velocity estimation from multi-station IPS , 1978 .

[18]  S. L. Scott,et al.  Solar cycle changes in the polar solar wind , 1980, Nature.

[19]  B. Jackson,et al.  Heliospheric tomography using interplanetary scintillation observations , 1997 .

[20]  W. Coles,et al.  Microturbulence in solar wind streams , 1980 .

[21]  H. Rosenbauer,et al.  Two states of the solar wind at the time of solar activity minimum - II. Radial gradients of plasma parameters in fast and slow streams , 1981 .