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Coronal mass ejection

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Coronal mass ejection

This video shows the particle flow around Earth as solar ejecta associated with a coronal mass ejection strike.

A coronal mass ejection (CME) is a massive burst of gas and magnetic field arising from the solar corona and being released into the solar wind, as observed in a coronagraph.[1]

Coronal mass ejections are often associated with other forms of solar activity, most notably solar flares or filament eruptions, but a broadly accepted theoretical understanding of these relationships has not been established. CMEs most often originate from active regions on the Sun's surface, such as groupings of sunspots associated with frequent flares. Near solar maxima, the Sun produces about three CMEs every day, whereas near solar minima, there is about one CME every five days.[2]


  • Description 1
  • Cause 2
  • Impact on Earth 3
  • Physical properties 4
  • Association with other solar phenomena 5
  • Theoretical models 6
  • Interplanetary CMEs 7
  • Related solar observation missions 8
    • NASA mission Wind 8.1
    • NASA mission STEREO 8.2
  • History 9
    • First traces 9.1
    • First clear detections 9.2
    • Recent events 9.3
  • See also 10
  • References 11
  • Further reading 12
  • External links 13


Arcs rise above an active region on the surface of the Sun.

Coronal mass ejections release huge quantities of matter and electromagnetic radiation into space above the sun's surface, either near the corona (sometimes called a solar prominence), or farther into the planet system, or beyond (interplanetary CME). The ejected material is a plasma consisting primarily of electrons and protons. While solar flares are very fast, CMEs are relatively slow.[3]

Coronal mass ejections are associated with enormous changes and disturbances in the coronal magnetic field. They are usually observed with a white-light coronagraph.


Recent scientific research[4][5] has shown that the phenomenon of magnetic reconnection is closely associated with CMEs and solar flares. Magnetic reconnection is the name given, within magnetohydrodynamic theory, to the rearrangement of magnetic field lines when two oppositely directed magnetic fields are brought together. This rearrangement is accompanied with a sudden release of energy stored in the original stressed magnetic fields.

On the sun, magnetic reconnection may happen on solar arcades—a series of closely occurring loops of magnetic lines of force. These lines of force quickly reconnect into a low arcade of loops, leaving a helix of magnetic field unconnected to the rest of the arcade. The sudden release of energy during this process causes the solar flare and ejects the CME. The helical magnetic field and the material that it contains may violently expand outwards forming a CME.[6] This also explains why CMEs and solar flares typically erupt from what are known as the active regions on the sun where magnetic fields are much stronger on average.

Aurora borealis stretch across Quebec and Ontario early on the morning of 8 October 2012.

Impact on Earth

When the ejection is directed towards Earth and reaches it as an interplanetary CME (ICME), the shock wave of the traveling mass of solar energetic particles causes a geomagnetic storm that may disrupt Earth's magnetosphere, compressing it on the day side and extending the night-side magnetic tail. When the magnetosphere reconnects on the nightside, it releases power on the order of terawatt scale, which is directed back toward Earth's upper atmosphere.

Solar energetic particles can cause particularly strong aurorae in large regions around Earth's magnetic poles. These are also known as the Northern Lights (aurora borealis) in the northern hemisphere, and the Southern Lights (aurora australis) in the southern hemisphere. Coronal mass ejections, along with solar flares of other origin, can disrupt radio transmissions and cause damage to satellites and electrical transmission line facilities, resulting in potentially massive and long-lasting power outages.[7][8]

Humans at high altitudes, as in airplanes or space stations, risk exposure to relatively intense cosmic rays. The energy absorbed by astronauts is not reduced by a typical spacecraft shield design and, if any protection is provided, it would result from changes in the microscopic inhomogeneity of the energy absorption events.[9]

Physical properties

A video of the series of CMEs in August 2010.
This video features two model runs. One looks at a moderate coronal mass ejection (CME) from 2006. The second run examines the consequences of a large coronal mass ejection, such as The Carrington-Class CME of 1859.

A typical coronal mass ejection may have any or all of three distinctive features: a cavity of low electron density, a dense core (the prominence, which appears as a bright region on coronagraph images embedded in this cavity), and a bright leading edge.

Most ejections originate from active regions on the Sun's surface, such as groupings of sunspots associated with frequent flares. These regions have closed magnetic field lines, in which the magnetic field strength is large enough to contain the plasma. These field lines must be broken or weakened for the ejection to escape from the sun. However, CMEs may also be initiated in quiet surface regions, although in many cases the quiet region was recently active. During solar minimum, CMEs form primarily in the coronal streamer belt near the solar magnetic equator. During solar maximum, they originate from active regions whose latitudinal distribution is more homogeneous.

Coronal mass ejections reach velocities between 20 to 3,200 km/s (12 to 1,988 mi/s) with an average speed of 489 km/s (304 mi/s), based on SOHO/LASCO measurements between 1996 and 2003. These speeds correspond to transit times from the sun out to the mean radius of Earth's orbit of about 86 days to 13 hours (extremes) and 3.5 days (average), respectively. The average mass ejected is 1.6×1012 kg (3.5×1012 lb). The mass values are only lower limits, because coronagraph measurements provide only two-dimensional data analysis. The frequency of ejections depends on the phase of the solar cycle: from about one every fifth day near the solar minimum to 3.5 per day near the solar maximum.[10] These values are also lower limits because ejections propagating away from Earth (backside CMEs) can usually not be detected by coronagraphs.

Current knowledge of coronal mass ejection kinematics indicates that the ejection starts with an initial pre-acceleration phase characterized by a slow rising motion, followed by a period of rapid acceleration away from the Sun until a near-constant velocity is reached. Some balloon CMEs, usually the slowest ones, lack this three-stage evolution, instead accelerating slowly and continuously throughout their flight. Even for CMEs with a well-defined acceleration stage, the pre-acceleration stage is often absent, or perhaps unobservable.

Association with other solar phenomena

A video of a solar filament being launched

Coronal mass ejections are often associated with other forms of solar activity, most notably:

  • Solar flares
  • Eruptive prominence and X-ray sigmoids
  • Coronal dimming (long-term brightness decrease on the solar surface)
  • Moreton waves
  • Coronal waves (bright fronts propagating from the location of the eruption)
  • Post-eruptive arcades

The association of a CME with some of those phenomena is common but not fully understood. For example, CMEs and flares are normally closely related, but there was confusion about this point caused by the events originating beyond the limb. For such events no flare could be detected. Most weak flares do not have associated CMEs; most powerful ones do. Some CMEs occur without any flare-like manifestation, but these are the weaker and slower ones.[11] It is now thought that CMEs and associated flares are caused by a common event (the CME peak acceleration and the flare impulsive phase generally coincide). In general, all of these events (including the CME) are thought to be the result of a large-scale restructuring of the magnetic field; the presence or absence of a CME during one of these restructures would reflect the coronal environment of the process (i.e., can the eruption be confined by overlying magnetic structure, or will it simply break through and enter the solar wind).

Theoretical models

It was first postulated that CMEs might be driven by the heat of an explosive flare. However, it soon became apparent that many CMEs were not associated with flares, and that even those that were often started before the flare. Because CMEs are initiated in the solar corona (which is dominated by magnetic energy), their energy source must be magnetic.

Because the energy of CMEs is so high, it is unlikely that their energy could be directly driven by emerging magnetic fields in the photosphere (although this is still a possibility). Therefore, most models of CMEs assume that the energy is stored up in the coronal magnetic field over a long period of time and then suddenly released by some instability or a loss of equilibrium in the field. There is still no consensus on which of these release mechanisms is correct, and observations are not currently able to constrain these models very well. These same considerations apply equally well to solar flares, but the observable signatures of these phenomena differ.[12]

Interplanetary CMEs

Illustration of a coronal mass ejection moving beyond the planets toward the heliopause

CMEs typically reach Earth one to five days after leaving the Sun. During their propagation, CMEs interact with the solar wind and the interplanetary magnetic field (IMF). As a consequence, slow CMEs are accelerated toward the speed of the solar wind and fast CMEs are decelerated toward the speed of the solar wind. CMEs faster than about 500 km/s (310 mi/s) eventually drive a shock wave.[13] This happens when the speed of the CME in the frame of reference moving with the solar wind is faster than the local fast magnetosonic speed. Such shocks have been observed directly by coronagraphs[14] in the corona, and are related to type II radio bursts. They are thought to form sometimes as low as 2 Rs (solar radii). They are also closely linked with the acceleration of solar energetic particles.[15]

Related solar observation missions

NASA mission Wind

On 1 November 1994, NASA launched the WIND spacecraft as a solar wind monitor to orbit Earth's L1 Lagrange point as the interplanetary component of the Global Geospace Science (GGS) Program within the International Solar Terrestrial Physics (ISTP) program. The spacecraft is a spin axis-stabilized satellite that carries eight instruments measuring solar wind particles from thermal to >MeV energies, electromagnetic radiation from DC to 13 MHz radio waves, and gamma-rays. Though the WIND spacecraft is nearly two decades old, it still provides the highest time, angular, and energy resolution of any of the solar wind monitors. It continues to produce relevant research as its data has contributed to over 150 publications since 2008 alone.


On 25 October 2006, NASA launched STEREO, two near-identical spacecraft which from widely separated points in their orbits are able to produce the first stereoscopic images of CMEs and other solar activity measurements. The spacecraft orbit the Sun at distances similar to that of Earth, with one slightly ahead of Earth and the other trailing. Their separation gradually increased so that after four years they were almost diametrically opposite each other in orbit.[16][17]


First traces

The largest recorded geomagnetic perturbation, resulting presumably from a CME, coincided with the first-observed solar flare on 1 September 1859, and is now referred to as the Carrington Event, or the solar storm of 1859. The flare and the associated sunspots were visible to the naked eye (both as the flare itself appearing on a projection of the sun on a screen and as an aggregate brightening of the solar disc), and the flare was independently observed by English astronomers R. C. Carrington and R. Hodgson. The geomagnetic storm was observed with the recording magnetograph at Kew Gardens. The same instrument recorded a crochet, an instantaneous perturbation of Earth's ionosphere by ionizing soft X-rays. This could not easily be understood at the time because it predated the discovery of X-rays by Röntgen and the recognition of the ionosphere by Kennelly and Heaviside. The storm took down parts of the recently created US telegraph network, starting fires and shocking some telegraph operators.[8]

Historical records were collected and new observations recorded in annual summaries by the Astronomical Society of the Pacific between 1953 and 1960.[18]

First clear detections

The first detection of a CME as such was made on 14 December 1971, by R. Tousey (1973) of the Naval Research Laboratory using the seventh Orbiting Solar Observatory (OSO-7).[19] The discovery image (256 × 256 pixels) was collected on a Secondary Electron Conduction (SEC) vidicon tube, transferred to the instrument computer after being digitized to 7 bits. Then it was compressed using a simple run-length encoding scheme and sent down to the ground at 200 bit/s. A full, uncompressed image would take 44 minutes to send down to the ground. The telemetry was sent to ground support equipment (GSE) which built up the image onto Polaroid print. David Roberts, an electronics technician working for NRL who had been responsible for the testing of the SEC-vidicon camera, was in charge of day-to-day operations. He thought that his camera had failed because certain areas of the image were much brighter than normal. But on the next image the bright area had moved away from the Sun and he immediately recognized this as being unusual and took it to his supervisor, Dr. Guenter Brueckner,[20] and then to the solar physics branch head, Dr. Tousey. Earlier observations of coronal transients or even phenomena observed visually during solar eclipses are now understood as essentially the same thing.

Recent events

On 1 August 2010, during solar cycle 24, scientists at the Harvard-Smithsonian Center for Astrophysics (CfA) observed a series of four large CMEs emanating from the Earth-facing hemisphere of the Sun. The initial CME was generated by an eruption on 1 August that was associated with NOAA Active Region 1092, which was large enough to be seen without the aid of a solar telescope. The event produced significant aurorae on Earth three days later.

On 23 July 2012, a massive, and potentially damaging, solar superstorm (solar flare, CME, solar EMP) barely missed Earth, according to NASA.[21][22] There is an estimated 12% chance of a similar event hitting Earth between 2012 and 2022.[21]

On 31 August 2012 a CME connected with Earth's magnetic environment, or magnetosphere, with a glancing blow causing aurora to appear on the night of 3 September.[23][24] Geomagnetic storming reached the G2 (Kp=6) level on NOAA's Space Weather Prediction Center scale of geomagnetic disturbances.[25][26]

See also


  1. ^ Christian, Eric R. (5 March 2012). "Coronal Mass Ejections". Retrieved 9 July 2013. 
  2. ^ Nicky Fox. "Coronal Mass Ejections". Goddard Space Flight Center @ NASA. Retrieved 2011-04-06. 
  3. ^ http://www
  4. ^ "Coronal Mass Ejections: Scientists Unlock the Secrets of Exploding Plasma Clouds On the Sun". Science Daily. 
  5. ^ Gopalswamy, Natchimuthuk (1 March 2001). "Cannibal Coronal Mass Ejections". NASA Science News. Retrieved 20 March 2015. 
  6. ^ "The Mysterious Origins of Solar Flares". Scientific American (Nature Publishing Group) 294 (4). April 2006.  
  7. ^ Baker, Daniel N.; et al. (2008). Severe Space Weather Events – Understanding Societal and Economic Impacts: A Workshop Report.  
  8. ^ a b Morring, Jr., Frank (14 January 2013). "Major Solar Event Could Devastate Power Grid".  
  9. ^ Wilson, John W.; Wood, J. S.; Shinn, Judy L.; Cucinotta, Francis A.; Nealy, John E. (August 1993). "A proposed performance index for galactic cosmic ray shielding materials". NASA.  
  10. ^ Carroll, Bradley W.; Dale A. Ostlie (2007). An Introduction to Modern Astrophysics. San Francisco: Addison-Wesley. p. 390.  
  11. ^ Andrews, M. D. (December 2003). "A Search for CMEs Associated with Big Flares". Solar Physics 218 (1): 261–279.  
  12. ^
  13. ^ Wilkinson, John (2012). New Eyes on the Sun: A Guide to Satellite Images and Amateur Observation. Springer. p. 98.  
  14. ^ Vourlidas, A., Wu, S.T., Wang, A. H., Subramanian, P., Howard, R. A. "Direct Detection of a Coronal Mass Ejection-Associated Shock in Large Angle and Spectrometric Coronagraph Experiment White-Light Images" in the "Astrophysical Journal", 598, 2, 1392–1402, 2003
  15. ^ Manchester, W. B., IV, T. I. Gombosi, D. L. De Zeeuw, I. V. Sokolov, ;, Roussev I., I., K. G. Powell, J. Kóta, G. Tóth, and T. H. Zurbuchen (2005). Coronal Mass Ejection Shock and Sheath Structures Relevant to Particle Acceleration. The Astrophysical Journal, Volume 622, Issue 2, pp. 1225–1239. 622 2: 1225–1239
  16. ^ Spacecraft go to film Sun in 3D BBC news, 2006-10-26
  17. ^ [2] NASA Mission Page, STEREO
  18. ^ Astronomical Society of the Pacific Visual Records
    • Nicholson, Seth B. (1954). "Solar Activity in 1953". Publications of the Astronomical Society of the Pacific 66 (389): 55–57.  
    • Cragg, Thomas A. (1955). "Solar Activity in 1954". Publications of the Astronomical Society of the Pacific 67 (395): 99–101.  
    • Nicholson, Seth B. (1956). "Solar Activity in 1955". Publications of the Astronomical Society of the Pacific 68 (401): 146–148.  
    • Cragg, Thomas A. (1957). "Solar Activity in 1956". Publications of the Astronomical Society of the Pacific 69 (407): 166–168.  
    • Cragg, Thomas A. (1958). "Solar Activity in 1957". Publications of the Astronomical Society of the Pacific 70 (414): 299–302.  
    • Cragg, Thomas A. (1959). "Solar Activity in 1958". Publications of the Astronomical Society of the Pacific 71 (420): 212–215.  
    • Cragg, Thomas A. (1960). "Solar Activity in 1959". Publications of the Astronomical Society of the Pacific 72 (426): 200–203.  
    • Cragg, Thomas A. (1961). "Solar Activity in 1960". Publications of the Astronomical Society of the Pacific 73 (432): 198–201.  
  19. ^ R.A. Howard, A Historical Perspective on Coronal Mass Ejections
  20. ^ Obit with brief bio for Dr. Brueckner
  21. ^ a b Phillips, Dr. Tony (23 July 2014). "Near Miss: The Solar Superstorm of July 2012".  
  22. ^ Staff (28 April 2014). "Video (04:03) - Carrington-class coronal mass ejection narrowly misses Earth".  
  23. ^ "NASA's SDO Sees Massive Filament Erupt on Sun". NASA. 4 September 2012. Retrieved 11 September 2012. 
  24. ^ "August 31, 2012 Magnificent CME". NASA/Goddard Space Flight Center. 31 August 2012. Retrieved 11 September 2012. 
  25. ^ "Space Weather Alerts and Warnings Timeline: September 1–16, 2012 (archive)".  
  26. ^ Chillymanjaro (6 September 2012). "Geomagnetic storming levels back to normal". The Watchers. Retrieved 11 September 2012. 

Further reading

  • Gopalswamy, Natchimuthukonar; Mewaldt, Richard A; Torsti, Jarmo, eds. (2006). Solar Eruptions and Energetic Particles. Geophys. Monograph Series 165. Am. Geophys. Union.  
Internet articles
  • Bell, Trudy E; Phillips, Tony (6 May 2008). "A Super Solar Flare". Science@NASA. 
  • Phillips, Tony (27 May 2008). "Cartwheel Coronal Mass Ejection". Science@NASA. 
  • Odenwald, Sten F; Green, James L (28 July 2008). "Bracing the Satellite Infrastructure for a Solar Superstorm". Scientific American. 
  • Lavraud, Benoit; Masson, Arnaud (21 November 2007). "Cluster captures the impact of CMEs". ESA Science & Technology. 
  • Morring Jr., Frank (14 January 2013). "Major Solar Event Could Devastate Power Grid". Aviation Week & Space Technology. 

External links

  • NOAA/NWS Space Weather Prediction Center
  • Coronal Mass Ejection FAQ
  • STEREO and SOHO observed CME rate versus the Sunspot number (PNG plot) / (text version)
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