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Polar wind

(Redirected from Ambipolar electric field)

The polar wind or plasma fountain is a permanent outflow of plasma from the polar regions of Earth's magnetosphere.[2]: 29  Conceptually similar to the solar wind, it is one of several mechanisms for the outflow of ionized particles. Ions accelerated by a polarization electric field known as an ambipolar electric field is believed to be the primary cause of polar wind. Similar processes operate on other planets.[3]

The Earth's plasma fountain, showing oxygen, helium, and hydrogen ions which gush into space from regions near the Earth's poles. The faint yellow area shown above the north pole represents gas lost from Earth into space; the green area is the aurora borealis—or plasma energy pouring back into the atmosphere.[1]

History

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In 1966 Bauer[4] and, separately, Dessler ahd Michel[5] noted that since the Earth's geomagnetic field above the poles forms a long tail away from the Sun out beyond the Moon's orbit, ions should flow from the higher pressure region in the ionosphere out into space.[6] The term "polar wind" was coined[7]: 1937  in 1968 in a pair of articles by Banks and Holzer[8] and by Ian Axford.[9] Since the process by which the ionospheric plasma flows away from the Earth along magnetic field lines, is similar to the flow of solar plasma away from the Sun's corona (the solar wind), Axford suggested the term "polar wind."

The earliest experimental characterization of the polar wind came from the 1966 Explorer 33 and especially the 1974 ISIS-2 satellite projects.[10][11] Additional data from the 1981 Dynamics Explorer led to some uncertainty in the theoretical models about the role of cool O+ ions. This issue was cleared up with the more comprehensive data from 1989 Akebono satellite,[7]: 1955  and the 1996 Polar satellite.[7]: 1966 

The idea for the polar wind originated with the desire to solve the paradox of the terrestrial helium budget. This paradox consists of the fact that helium in the Earth's atmosphere seems to be produced (via radioactive decay of uranium and thorium) faster than it is lost by escaping from the upper atmosphere. The realization that some helium could be ionized, and therefore escape the Earth along open magnetic field lines near the magnetic poles (the 'polar wind'), is one possible solution to the paradox.

Causes

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Conceptual diagram of the two main effects of the ambipolar electric field: inflating the ionosphere and generating the polar wind.The sparkling blue haze surrounding Earth represents the plasma in the ionosphere. The sparkling lines represent polar wind flowing up and out.[12]

After 30 years of research, the "classical" cause of the polar wind has been shown to be ambipolar outflow of thermal plasma: ion acceleration by a polarization electric field in the ionosphere.[2]: 451  The polarization or ambipolar electric field was originally proposed in the 1920s for ionized stellar atmospheres.[11]: 1927  Gravitational charge separation creates a field amounting to   where   is the gravitational field and   is the mean ionic mass, half the difference between the mass of the singly charged ions and the electron. This simple formula is only applicable in a plasma in hydrostatic equilibrium. More complex models applicable to real plasmas show larger field strength. In any case the field is very small but, unlike other forces, it points away from gravity.[11]: 1927  In low density plasma at high altitude it overwhelms gravity for light ions.

In region of the polar wind, the ionospheric plasma expands and the low density allows gravity to pull ions down relative to the electrons in the plasma. The charge separation results in the electric field which then sends some of the ions up and out of the atmosphere.[13]: 147  This mechanism is known as "ambipolar outflow"[14] and the field as "ambipolar electric field" or "polarization electric field". Additional mechanisms include ion acceleration by solar photoelectrons escaping along magnetic field lines.[14]

The outflow of ions due to the ambipolar electric field end up accumulating in the plasmasphere if they follow closed magnetic field lines but ions following open magnetic field lines exit the Earth system.[13]: 167  Ions following open magnetic field lines are push away from the Sun by forces of the solar wind (anti-solar convection).[13]: 149 

Measurements

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Numerous investigations of the polar wind have launched, including ISIS-2, Dynamics Explorer, the Akebono satellite, and the Polar satellite, covering a variety of altitudes, latitudes, and times relative to the solar cycle. Some of the conclusions include:[7]

  • the primary ingredients in the polar wind are electrons, hydrogen (H+), helium (He+), and oxygen (O+) ions,
  • O+ ions dominate at below 4000km,
  • all three ion species reach supersonic velocities above 7000km and velocities increase to over Mach number 2 above 50,000km.[7]: 1976 
  • polar wind velocity increases with altitude, and is higher on the dayside of the Earth,

The polarization or ambipolar electric field was directly measured in 2022 by a sounding rocket launched from Svalbard. This NASA mission was called Endurance.[12] Comparing the electrical potential at altitude of 250 km to that at 768 km gave a difference of +0.55 volt with an uncertainty of 0.09 volt.[15] The voltage is similar to that used in a wristwatch battery but is sufficient to account for the polar wind.[16]

See also

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References

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  1. ^ Plasma fountain Source, press release: Carlowicz, Mike; "Solar Wind Squeezes Some of Earth's Atmosphere into Space", December 1998
  2. ^ a b Schunk, R. W.; Nagy, Andrew (2000). Ionospheres: physics, plasma physics, and chemistry. Cambridge atmospheric and space science series. New York: Cambridge University Press. ISBN 978-0-521-63237-9.
  3. ^ Gronoff, G.; Arras, P.; Baraka, S.; Bell, J. M.; Cessateur, G.; Cohen, O.; Curry, S. M.; Drake, J. J.; Elrod, M.; Erwin, J.; Garcia-Sage, K.; Garraffo, C.; Glocer, A.; Heavens, N. G.; Lovato, K. (August 2020). "Atmospheric Escape Processes and Planetary Atmospheric Evolution". Journal of Geophysical Research: Space Physics. 125 (8). arXiv:2003.03231. Bibcode:2020JGRA..12527639G. doi:10.1029/2019JA027639. ISSN 2169-9380.
  4. ^ Bauer, S.J. (1966). "The structure of the topside ionosphere". In Frihagen, J. (ed.). Electron Density Profiles in Ionosphere and Exosphere. North-Holland.
  5. ^ Dessler, A. J.; Michel, F. C. (1966-03-01). "Plasma in the geomagnetic tail". Journal of Geophysical Research. 71 (5): 1421–1426. doi:10.1029/JZ071i005p01421.
  6. ^ Schunk, R. W.; Sojka, J. J. (June 1997). "Global ionosphere‐polar wind system during changing magnetic activity". Journal of Geophysical Research: Space Physics. 102 (A6): 11625–11651. doi:10.1029/97JA00292. ISSN 0148-0227.
  7. ^ a b c d e Yau, Andrew W.; Abe, Takumi; Peterson, W. K. (2007-11-01). "The polar wind: Recent observations". Journal of Atmospheric and Solar-Terrestrial Physics. Recent Advances in the Polar Wind Theories and Observations. 69 (16): 1936–1983. doi:10.1016/j.jastp.2007.08.010. ISSN 1364-6826.
  8. ^ Banks, Peter M.; Holzer, Thomas E. (1968). "The Polar Wind". Journal of Geophysical Research. 73 (21): 6846–6854. Bibcode:1968JGR....73.6846B. doi:10.1029/JA073i021p06846.
  9. ^ Axford, W. Ian (1968). "The Polar Wind and the Terrestrial Helium Budget". Journal of Geophysical Research. 73 (21): 6855–6859. Bibcode:1968JGR....73.6855A. doi:10.1029/JA073i021p06855.
  10. ^ Hoffman, J. H.; Dodson, W. H.; Lippincott, C. R.; Hammack, H. D. (1974-10-01). "Initial ion composition results from the Isis 2 satellite". Journal of Geophysical Research. 79 (28): 4246–4251. doi:10.1029/JA079i028p04246.
  11. ^ a b c Lemaire, J. F.; Peterson, W. K.; Chang, T.; Schunk, R. W.; Barakat, A. R.; Demars, H. G.; Khazanov, G. V. (2007-11-01). "History of kinetic polar wind models and early observations". Journal of Atmospheric and Solar-Terrestrial Physics. Recent Advances in the Polar Wind Theories and Observations. 69 (16): 1901–1935. doi:10.1016/j.jastp.2007.08.011. ISSN 1364-6826.
  12. ^ a b Lacey Young (28 August 2024), Discovering Earth’s Third Global Energy Field, NASA
  13. ^ a b c Welling, Daniel T.; André, Mats; Dandouras, Iannis; Delcourt, Dominique; Fazakerley, Andrew; Fontaine, Dominique; Foster, John; Ilie, Raluca; Kistler, Lynn; Lee, Justin H.; Liemohn, Michael W.; Slavin, James A.; Wang, Chih-Ping; Wiltberger, Michael; Yau, Andrew (2015). "The Earth: Plasma Sources, Losses, and Transport Processes". Space Science Reviews. 192 (1–4): 145–208. Bibcode:2015SSRv..192..145W. doi:10.1007/s11214-015-0187-2. ISSN 0038-6308.
  14. ^ a b Schunk, R. W. (2007-11-01). "Time-dependent simulations of the global polar wind". Journal of Atmospheric and Solar-Terrestrial Physics. Recent Advances in the Polar Wind Theories and Observations. 69 (16): 2028–2047. Bibcode:2007JASTP..69.2028S. doi:10.1016/j.jastp.2007.08.009. ISSN 1364-6826.
  15. ^ Collinson, Glyn A.; et al. (29 August 2024). "Earth's ambipolar electrostatic field and its role in ion escape to space". Nature. 632 (8027): 1021–1025. doi:10.1038/s41586-024-07480-3. Retrieved 26 September 2024.
  16. ^ "Discovering Earth's Third Energy Field". svs.gsfc.nasa.gov. Retrieved 2024-09-12.
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