Solar prominence

Last updated

Solar prominence seen in true color during totality of a Solar eclipse. Prominence ESA423294.jpg
Solar prominence seen in true color during totality of a Solar eclipse.

In solar physics, a prominence, sometimes referred to as a filament, [lower-alpha 1] is a large, shiny, reddish plasma and magnetic field structure extending outward from the Sun's surface, often in a loop shape. Prominences are anchored to the Sun's surface in the much brighter photosphere, and extend outwards into the solar corona. While the corona consists of extremely hot plasma, prominences contain much cooler plasma, similar in composition to that of the chromosphere.

Contents

Prominences form over timescales of about a day and may persist in the corona for several weeks or months, looping hundreds of thousands of kilometers into space. Some prominences may give rise to coronal mass ejections. Exact mechanism of prominence generation is an ongoing target of scientific research.

A typical prominence extends over many thousands of kilometers; the largest on record was estimated at over 800,000 km (500,000 mi) long, [2] roughly of solar radius.

History

The first detailed description of a solar prominence was in 14th-century Laurentian Codex, describing the solar eclipse of May 1, 1185. They were described as "flame-like tongues of live embers". [3] [4] [5]

Prominences were first photographed during the solar eclipse of July 18, 1860, by Angelo Secchi. From these photographs, altitude, emissivity, and many other important parameters were able to be derived for the first time. [6]

During the solar eclipse of August 18, 1868, spectroscopes were for the first time able to detect the presence of emission lines from prominences. The detection of a hydrogen line confirmed that prominences were gaseous in nature. Pierre Janssen was also able to detect an emission line corresponding to an at the time unknown element now known as helium. The following day, Janssen confirmed his measurements by recording the emission lines from the now unobstructed Sun, a task that had never been done before. Using his new techniques, astronomers were able to study prominences daily. [7]

Classification

Grayscale H-alpha image of the Solar disk showing quiescent filaments (QF), intermediate filaments (IF), and active region filaments (ARF). BBSO H-alpha solar disk 2002-07-24 labeled.png
Grayscale H-alpha image of the Solar disk showing quiescent filaments (QF), intermediate filaments (IF), and active region filaments (ARF).

Historically, any feature that was visible extending above the surface of the sun, including solar spicules, coronal loops, and some coronal mass ejections, was considered a solar prominence. Today, due to a better understanding of the diversity of these phenomena, most of these are classified separately, and the word "prominence" is primarily used to refer to larger and cooler features. [8]

There are a number of different prominence classification schemes in use today. One of the most widely used and basic schemes classifies prominences based on the magnetic environment in which they had formed. There are three classes:

Active region and quiescent prominences can also be differentiated by their emitted spectra. The spectra of active region prominences is identical to that of the upper chromosphere having strong He II lines but very weak ionized metal lines. On the other hand, the spectra of quiescent prominences is identical to the spectra measured at 1,500 km (930 mi) in the chromosphere with strong H, He I, and ionized metal lines, but weak He II lines. [13]

Morphology

Filament channels

Prominences form in magnetic structures known as filament channels where they are thermally shielded from the surrounding corona and supported against gravity. These channels are found in the chromosphere and lower corona above divisions between regions of opposite photospheric magnetic polarity known as polarity inversion lines (PIL). [lower-alpha 2] The presence of a filament channel is a necessary condition for the formation of a prominence, but a filament channel can exist without containing a prominence. Multiple prominences may form and erupt from within one filament channel over the channel's lifetime. The magnetic field making up the filament channel is predominantly horizontal, pointing in the same direction on both sides of the PIL (see § Chirality). [14] [15] [16]

Prominence material does not occupy the entire width of the filament channel; a tunnel-like region less dense than the corona, known as a coronal cavity, occupies the volume between the prominence and the overlying magnetic arcade. [7]

Spines and barbs

Typical prominences have a narrow structure oriented along the filament channel known as a spine. The spine defines the upper main body of a prominence and is generally in the form of a vertical sheet that diverges towards the photosphere at both ends. Many prominences also have smaller structures referred to as barbs that similarly diverge from the spine towards the chromosphere and photosphere. Spines and barbs are both composed of thin threads that trace the magnetic field similar to chromospheric fibrils. [15]

The cool prominence material that makes up spines and barbs—the prominence core—is surrounded by a prominence-corona transition region (PCTR) where there is a steep temperature gradient. The PCTR is responsible for most of the optical emission of prominences. [7]

H-alpha DOT image of a solar filament colored.jpg
H-alpha image of an active region filament showing a spine, two barbs, and chromospheric fibrils oriented parallel to the PIL [14]

Overlying structures

Above filament channels lie overarching magnetic arcades which can extend from 50,000 to 70,000 km (31,000 to 43,000 mi) into the corona. Above these arcades, the closed coronal magnetic field may extend radially outward, forming what is known as a helmet streamer. [17] These streamers may reach a solar radius or more above the Sun's surface. [7]

Chirality

Filament channels and their prominence, if present, exhibit chirality. When observed from the side of the filament channel with positive magnetic polarity, the channel is said to be dextral if the horizontal magnetic field is oriented rightward and sinistral if it is oriented leftward. Dextral channels have been found more frequently in the Sun's northern hemisphere and sinistral channels more frequently in the southern hemisphere.

The horizontally oriented magnetic field causes chromospheric fibrils along the filament channel to lie nearly parallel to the PIL and anti-parallel to one another on opposite sides of the PIL. The directions that these fibrils are oriented depend on the chirality of the channel. On the side of the PIL with positive magnetic polarity, dextral channels have fibrils which stream to the right and barbs which bear to the right, whereas sinistral channels have fibrils which stream to the left and barbs which bear to the left. Additionally, the overlying magnetic arcades of dextral channels are left-skewed, and those of sinistral channels are right-skewed. [7]

Formation

The exact mechanism which leads to the formation of solar prominences is not currently known. Models must be able to explain the formation of the filament channel and its hemisphere-dependent chirality, as well as the origin of the dense plasma that makes up the prominence core. [7]

Eruption

A solar prominence erupting. False color ultraviolet image.

Some prominences are ejected from the Sun in what is known as a prominence eruption. These eruptions can have speeds ranging from 600 km/s to more than 1000 km/s. [1] At least 70% of prominence eruptions are associated with an ejection of coronal material into the solar wind known as a coronal mass ejection. [18]

See also

Explanatory notes

  1. When viewed against the background of space (off-limb), they are referred to as prominences; when viewed against the Sun's surface (on-disk), they are referred to as filaments. [1]
  2. Divisions between regions of opposite photospheric magnetic polarity are variously referred to as polarity inversion lines (PIL), polarity reversal boundaries (PRB), or neutral lines.

Related Research Articles

<span class="mw-page-title-main">Stellar corona</span> Outermost layer of a stars atmosphere

A corona is the outermost layer of a star's atmosphere. It is a hot but relatively dim region of plasma populated by intermittent coronal structures known as solar prominences or filaments.

<span class="mw-page-title-main">Solar flare</span> Eruption of electromagnetic radiation

A solar flare is a relatively intense, localized emission of electromagnetic radiation in the Sun's atmosphere. Flares occur in active regions and are often, but not always, accompanied by coronal mass ejections, solar particle events, and other eruptive solar phenomena. The occurrence of solar flares varies with the 11-year solar cycle.

<span class="mw-page-title-main">Chromosphere</span> Layer of a stars atmosphere

A chromosphere is the second layer of a star's atmosphere, located above the photosphere and below the solar transition region and corona. The term usually refers to the Sun's chromosphere, but not exclusively.

<span class="mw-page-title-main">Coronal mass ejection</span> Ejecta from the Suns corona

A coronal mass ejection (CME) is a significant ejection of magnetic field and accompanying plasma mass from the Sun's corona into the heliosphere. CMEs are often associated with solar flares and other forms of solar activity, but a broadly accepted theoretical understanding of these relationships has not been established.

A solar storm is a disturbance on the Sun, which can emanate outward across the heliosphere, affecting the entire Solar System, including Earth and its magnetosphere, and is the cause of space weather in the short-term with long-term patterns comprising space climate.

<span class="mw-page-title-main">Alfvén wave</span> Low-frequency plasma wave

In plasma physics, an Alfvén wave, named after Hannes Alfvén, is a type of plasma wave in which ions oscillate in response to a restoring force provided by an effective tension on the magnetic field lines.

The Evershed effect, named after the British astronomer John Evershed, is the radial flow of gas across the photospheric surface of the penumbra of sunspots from the inner border with the umbra towards the outer edge.

<span class="mw-page-title-main">Coronal hole</span> Cool, tenuous region of the Suns corona

A coronal hole is a temporary region of relatively cool, less dense plasma in the solar corona where the Sun's magnetic field extends into interplanetary space as an open field. Compared to the corona's usual closed magnetic field that arches between regions of opposite magnetic polarity, the open magnetic field of a coronal hole allows solar wind to escape into space at a much quicker rate. This results in decreased temperature and density of the plasma at the site of a coronal hole, as well as an increased speed in the average solar wind measured in interplanetary space. If streams of high-speed solar wind from coronal holes encounter the Earth, they can cause major displays of aurorae. Near solar minimum, when activity such as coronal mass ejections is less frequent, such streams are the main cause of geomagnetic storms and associated aurorae.

<span class="mw-page-title-main">Coronal loop</span> Arch-like structure in the Suns corona

In solar physics, a coronal loop is a well-defined arch-like structure in the Sun's atmosphere made up of relatively dense plasma confined and isolated from the surrounding medium by magnetic flux tubes. Coronal loops begin and end at two footpoints on the photosphere and project into the transition region and lower corona. They typically form and dissipate over periods of seconds to days and may span anywhere from 1 to 1,000 megametres in length.

Coronal seismology is a technique of studying the plasma of the Sun's corona with the use of magnetohydrodynamic (MHD) waves and oscillations. Magnetohydrodynamics studies the dynamics of electrically conducting fluids - in this case the fluid is the coronal plasma. Observed properties of the waves (e.g. period, wavelength, amplitude, temporal and spatial signatures, characteristic scenarios of the wave evolution, combined with a theoretical modelling of the wave phenomena, may reflect physical parameters of the corona which are not accessible in situ, such as the coronal magnetic field strength and Alfvén velocity and coronal dissipative coefficients. Originally, the method of MHD coronal seismology was suggested by Y. Uchida in 1970 for propagating waves, and B. Roberts et al. in 1984 for standing waves, but was not practically applied until the late 90s due to a lack of necessary observational resolution. Philosophically, coronal seismology is similar to the Earth's seismology, helioseismology, and MHD spectroscopy of laboratory plasma devices. In all these approaches, waves of various kind are used to probe a medium.

<span class="mw-page-title-main">Helmet streamer</span> Structure in the Suns corona

Helmet streamers, also known as coronal streamers, are elongated cusp-like structures in the Sun's corona which are often visible in white-light coronagraphs and during solar eclipses. They are closed magnetic loops which lie above divisions between regions of opposite magnetic polarity on the Sun's surface. The solar wind elongates these loops to pointed tips which can extend a solar radius or more into the corona.

<span class="mw-page-title-main">Interface Region Imaging Spectrograph</span> NASA satellite of the Explorer program

Interface Region Imaging Spectrograph (IRIS), also called Explorer 94 and SMEX-12, is a NASA solar observation satellite. The mission was funded through the Small Explorer program to investigate the physical conditions of the solar limb, particularly the interface region made up of the chromosphere and transition region. The spacecraft consists of a satellite bus and spectrometer built by the Lockheed Martin Solar and Astrophysics Laboratory (LMSAL), and a telescope provided by the Smithsonian Astrophysical Observatory (SAO). IRIS is operated by LMSAL and NASA's Ames Research Center.

<span class="mw-page-title-main">Nanoflare</span> Type of episodic heating event

A nanoflare is a very small episodic heating event which happens in the corona, the external atmosphere of the Sun.

<span class="mw-page-title-main">Coronal radiative losses</span>

In astronomy and in astrophysics, for radiative losses of the solar corona, it is meant the energy flux radiated from the external atmosphere of the Sun, and, in particular, the processes of production of the radiation coming from the solar corona and transition region, where the plasma is optically-thin. On the contrary, in the chromosphere, where the temperature decreases from the photospheric value of 6000 K to the minimum of 4400 K, the optical depth is about 1, and the radiation is thermal.

<span class="mw-page-title-main">Solar phenomena</span> Natural phenomena within the Suns atmosphere

Solar phenomena are natural phenomena which occur within the atmosphere of the Sun. They take many forms, including solar wind, radio wave flux, solar flares, coronal mass ejections, coronal heating and sunspots.

<span class="mw-page-title-main">Hyder flare</span> Slow, large-scale brightening that occurs in the solar chromosphere

A Hyder flare is slow, large-scale brightening that occurs in the solar chromosphere. It resembles a large but feeble solar flare and is identifiable as the signature of the sudden disappearance of a solar prominence. These events occur in the quiet Sun, away from active regions or sunspot groups, and typically in the polar crown filament zone near the Sun's poles. Hyder flares have a two-ribbon morphology and can be faintly observed in chromospheric emission lines such as Hα or as enhanced absorption in He I 1083 nm line.

<span class="mw-page-title-main">Sarah E. Gibson</span> American solar physicist

Sarah E. Gibson is an American solar physicist. She is a Senior Scientist and past Interim Director of the High Altitude Observatory in Boulder, Colorado. As of 2019, Dr. Gibson is the Project Scientist for the PUNCH Small Explorer mission being built for NASA.

Solar radio emission refers to radio waves that are naturally produced by the Sun, primarily from the lower and upper layers of the atmosphere called the chromosphere and corona, respectively. The Sun produces radio emissions through four known mechanisms, each of which operates primarily by converting the energy of moving electrons into electromagnetic radiation. The four emission mechanisms are thermal bremsstrahlung (braking) emission, gyromagnetic emission, plasma emission, and electron-cyclotron maser emission. The first two are incoherent mechanisms, which means that they are the summation of radiation generated independently by many individual particles. These mechanisms are primarily responsible for the persistent "background" emissions that slowly vary as structures in the atmosphere evolve. The latter two processes are coherent mechanisms, which refers to special cases where radiation is efficiently produced at a particular set of frequencies. Coherent mechanisms can produce much larger brightness temperatures (intensities) and are primarily responsible for the intense spikes of radiation called solar radio bursts, which are byproducts of the same processes that lead to other forms of solar activity like solar flares and coronal mass ejections.

<span class="mw-page-title-main">Transequatorial loop</span>

In solar physics, a transequatorial loop is a structure present in the solar corona that connects two different regions of opposite magnetic polarity in opposite hemispheres of the Sun. These connected regions are not limited to active regions, but are most commonly found during the times of maximum solar activity, the solar maximum.

<span class="mw-page-title-main">Gordon Dean Holman</span> American astrophysicist, NASA scientist

Gordon Dean Holman is an emeritus research astrophysicist at the National Aeronautics and Space Administration's (NASA’s) Goddard Space Flight Center in Greenbelt, Maryland. His research mostly focused on obtaining an understanding of high-energy radiation from astronomical objects. This radiation cannot be observed from Earth's surface, but is observed with instruments on satellites launched to orbits above Earth's atmosphere. It is primarily emitted by high-energy electrons interacting with ions. These electrons also emit radiation at radio frequencies which is observed from Earth's surface. Consequently, these observations from space and radio telescopes provide a view of hot gas and energetic particles in the Universe that could not otherwise be obtained. Holman has specialized in the interpretation of these observed emissions to determine the origin and evolution of this hot gas and energetic particles. He has been described as "not just a theorist, he also looks at the data".

References

  1. 1 2 "About Filaments and Prominences". solar.physics.montana.edu. Retrieved January 2, 2010.
  2. Atkinson, Nancy (August 6, 2012). "Huge Solar Filament Stretches Across the Sun". Universe Today . Retrieved August 11, 2012.
  3. "1185: The first description of solar prominences". Solar Physics Historical Timeline (0–1599). High Altitude Observatory. 2008.
  4. "1185: The first description of solar prominences" (PDF). Great Moments in the History of Solar Physics. Université de Montréal. 2008. Archived from the original on April 2, 2015. Retrieved March 30, 2015.
  5. Poitevin, Patrick; Edmonds, Joanne (2003). "Solar Eclipse Newsletter" (PDF). Retrieved March 30, 2015.
  6. Secchi, Angelo (1870). Le Soleil, Part 1. Paris: Gauthier-Villars. p. 378.
  7. 1 2 3 4 5 6 Vial, Jean-Claude; Engvold, Oddbjørn (2015). Solar Prominences. Springer. ISBN   978-3-319-10415-7.
  8. Vial, Jean-Claude; Engvold, Oddbjørn (2015). Solar prominences. Cham Heielberg New York Dordrecht London: Springer. p. 33–37. ISBN   978-3-319-10416-4.
  9. 1 2 Mackay, D. H.; Karpen, J. T.; Ballester, J. L.; Schmieder, B.; Aulanier, G. (April 2010). "Physics of Solar Prominences: II – Magnetic Structure and Dynamics". Space Science Reviews. 151 (4): 333–399. arXiv: 1001.1635 . Bibcode:2010SSRv..151..333M. doi:10.1007/s11214-010-9628-0. S2CID   118391089.
  10. 1 2 Menzel, Donald H.; Jones, F. Shirley (December 1962). "Solar Prominence Activity, 1944–1954". Journal of the Royal Astronomical Society of Canada. 56: 193. Bibcode:1962JRASC..56..193M. Archived from the original on June 2, 2021.
  11. 1 2 Minarovjech, M.; Rybanský, M.; Rušin, V. (1998). "Time-Latitude Prominence and the Green Corona Distribution over the Solar Activity Cycle". International Astronomical Union Colloquium. 167: 484–487. doi: 10.1017/S0252921100048132 .
  12. Engvold, Oddbjørn (1998). "Observations of Filament Structure and Dynamics". International Astronomical Union Colloquium. 167: 22–31. doi: 10.1017/S0252921100047229 .
  13. Zirin, Harold; Tandberg-Hanssen, Einar (1960). "Physical Conditions in Limb Flares and Active Prominences. IV. Comparison of Active and Quiescent Prominences". The Astrophysical Journal. 131: 717–724. Bibcode:1960ApJ...131..717Z. doi: 10.1086/146884 .
  14. 1 2 Parenti, Susanna (2014). "Solar Prominences: Observations" (PDF). Living Reviews in Solar Physics. 11 (1): 1. Bibcode:2014LRSP...11....1P. doi:10.12942/lrsp-2014-1. S2CID   122831380 . Retrieved January 29, 2022.
  15. 1 2 Gibson, Sarah E. (December 2018). "Solar prominences: theory and models: Fleshing out the magnetic skeleton" (PDF). Living Reviews in Solar Physics. 15 (1): 7. Bibcode:2018LRSP...15....7G. doi:10.1007/s41116-018-0016-2. PMC   6390890 . PMID   30872983 . Retrieved January 29, 2022.
  16. Gaizauskas, V. (1998). "Filament Channels: Essential Ingredients for Filament Formation". International Astronomical Union Colloquium. 167: 257–264. doi: 10.1017/S0252921100047709 . ISSN   0252-9211. S2CID   124424544.
  17. Guo, W. P.; Wu, S. T. (February 10, 1998). "A Magnetohydrodynamic Description of Coronal Helmet Streamers Containing a Cavity". The Astrophysical Journal. 494 (1): 419–429. Bibcode:1998ApJ...494..419G. doi: 10.1086/305196 . S2CID   120452722.
  18. Gopalswamy, N.; Shimojo, M.; Lu, W.; Yashiro, S.; Shibasaki, K.; Howard, R. A. (March 20, 2003). "Prominence Eruptions and Coronal Mass Ejection: A Statistical Study Using Microwave Observations". The Astrophysical Journal. 586 (1): 562–578. Bibcode:2003ApJ...586..562G. doi: 10.1086/367614 . S2CID   119654267.

Further reading