The Solar Wind and Its Interaction with the Interstellar Medium

The solar wind is a magnetized plasma of ions and electrons which flows outward from the Sun. This chapter begins with a brief history of the discovery of the solar wind. Solar wind properties at 1 AU are discussed as well as how these properties change over a solar cycle. The solar wind evolves as it moves outward through the solar system and interacts with the interstellar neutrals which slow and heat the wind. The solar wind runs into a variety of obstacles as it moves outward, the non-conducting Moon and asteroids, comets and unmagnetized planets where the atmosphere forms a conducting barrier, and magnetized planets with large magnetospheres. Finally the solar wind reaches the interstellar medium, going through the termination shock and then diverting down the tail of the heliosphere.

[1]  S. Krimigis,et al.  Mediation of the solar wind termination shock by non-thermal ions , 2008, Nature.

[2]  J. Belcher,et al.  The heliospheric boundary response to large‐scale solar wind fluctuations: A gasdynamic model with pickup ions , 1999 .

[3]  J. Richardson,et al.  Solar wind oscillations with a 1.3 year period , 1994 .

[4]  W. Matthaeus,et al.  Turbulent Heating of the Distant Solar Wind by Interstellar Pickup Protons , 2003 .

[5]  K. Ogilvie,et al.  The solar cycle variation of the solar wind helium abundance , 1974 .

[6]  Alan J. Lazarus,et al.  The solar wind helium abundance: Variation with wind speed and the solar cycle , 2001 .

[7]  N. Pogorelov,et al.  The Direction of the Neutral Hydrogen Velocity in the Inner Heliosphere as a Possible Interstellar Magnetic Field Compass , 2006 .

[8]  William M. Farrell,et al.  Observations of the lunar plasma wake from the WIND spacecraft on December 27, 1994 , 1996 .

[9]  J. Brackbill,et al.  Motion of the termination shock in response to an 11 Year variation in the solar wind , 1995 .

[10]  Philip L. Roe,et al.  Heliosphere in the magnetized local interstellar medium' Results of a three-dimensional MHD , 1998 .

[11]  M. Vinokur,et al.  EFFECT OF VARYING STRENGTH AND ORIENTATION OF LOCAL INTERSTELLAR MAGNETIC FIELD ON CONFIGURATION OF EXTERIOR HELIOSPHERE : 3D MHD SIMULATIONS , 1998 .

[12]  W. Webber,et al.  An asymmetric solar wind termination shock , 2008, Nature.

[13]  John W. Belcher,et al.  Cool heliosheath plasma and deceleration of the upstream solar wind at the termination shock , 2008, Nature.

[14]  W. Feldman,et al.  Long-term variations of selected solar wind properties - IMP 6, 7, and 8 results , 1978 .

[15]  R. C. Carrington Description of a Singular Appearance seen in the Sun on September 1, 1859 , 1859 .

[16]  The dynamical heliosphere , 2001 .

[17]  M. Neugebauer,et al.  Solar Plasma Experiment , 1962, Science.

[18]  E. Parker Dynamics of the Interplanetary Gas and Magnetic Fields , 1958 .

[19]  J. Richardson,et al.  Magnetic fields at the solar wind termination shock , 2008, Nature.

[20]  D. C. Hamilton,et al.  Voyager 1 in the Foreshock, Termination Shock, and Heliosheath , 2005, Science.

[21]  J. Richardson,et al.  Turbulent Heating of the Solar Wind by Newborn Interstellar Pickup Protons , 2006 .

[22]  R. McNutt,et al.  Plasma Observations in the Distant Heliosphere: A View from Voyager , 1990 .

[23]  J. Richardson,et al.  Determining the LIC H density from the solar wind slowdown , 2008 .

[24]  P. Gazis,et al.  Physics of the outer heliosphere , 1991 .

[25]  L. Lanzerotti,et al.  Acceleration of solar wind and pickup ions by shocks , 2005 .

[26]  T. Gombosi,et al.  The Orientation of the Local Interstellar Magnetic Field , 2007, Science.

[27]  Iver H. Cairns,et al.  Interstellar pickup ions and quasi‐perpendicular shocks: Implications for the termination shock and interplanetary shocks , 1996 .

[28]  John W. Belcher,et al.  Evidence for a solar wind slowdown in the outer heliosphere , 1995 .

[29]  E. C. Stone,et al.  Voyager 1 Explores the Termination Shock Region and the Heliosheath Beyond , 2005, Science.

[30]  David J. McComas,et al.  The three‐dimensional solar wind around solar maximum , 2003 .

[31]  S. Chapman,et al.  A New Theory of Magnetic Storms. , 1930, Nature.

[32]  S. Silverman SECULAR VARIATION OF THE AURORA FOR THE PAST 500 YEARS , 1992 .

[33]  Thompson,et al.  Dynamic variations at the base of the solar convection zone , 2000, Science.

[34]  R. P. Lepping,et al.  Crossing the Termination Shock into the Heliosheath: Magnetic Fields , 2005, Science.

[35]  J. Giacalone,et al.  Radial Streaming Anisotropies of Charged Particles Accelerated at the Solar Wind Termination Shock , 2004 .

[36]  N. Pogorelov,et al.  Three-dimensional Features of the Outer Heliosphere Due to Coupling between the Interstellar and Interplanetary Magnetic Fields. I. Magnetohydrodynamic Model: Interstellar Perspective , 2004 .

[37]  P. Gazis Limits on Deceleration and Asymmetry of Solar Wind Speed , 1995 .

[38]  Paulett C. Liewer,et al.  The Effects of a Local Interstellar Magnetic Field on Voyager 1 and 2 Observations , 2006, astro-ph/0603318.

[39]  S. Krimigis,et al.  Low‐energy ions near the termination shock , 2006 .

[40]  K. Gringauz Some Results of Experiments in Interplanetary Space by Means of Charged Particle Traps on Soviet Space Probes , 1961 .