Difference between revisions of "Crab Nebula" - New World Encyclopedia

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Tracing back its expansion consistently yields a date for the creation of the nebula several decades after 1054, implying that its outward velocity has accelerated since the supernova explosion.<ref name="Trimble1968">{{ citation
 
Tracing back its expansion consistently yields a date for the creation of the nebula several decades after 1054, implying that its outward velocity has accelerated since the supernova explosion.<ref name="Trimble1968">{{ citation

Revision as of 01:52, 11 December 2008

Crab Nebula
Crab Nebula.jpg

M1, the Crab Nebula. Courtesy of NASA/ESA

Observation data: J2000.0 epoch
TypeSupernova Remnant
Right ascension05h 34m 31.97s[1]
Declination+22° 00′ 52.1″[1]
Distance6.5 ± 1.6 kly (2.0 ± 0.5 kpc)[2]
Apparent magnitude (V)+8.4
Apparent dimensions (V)420″ × 290″[3][4]
ConstellationTaurus
Physical characteristics
Radius6.5 ± 1.5 ly[5]
Absolute magnitude (V)−3.1 ± 0.5[6]
Notable featuresOptical pulsar
Other designationsM1,[1] NGC 1952[1], Sharpless 244
See also: Diffuse nebula, Lists of nebulae

The Crab Nebula (catalogue designations M1, NGC 1952, Taurus A) is a supernova remnant and pulsar wind nebula in the constellation of Taurus. The nebula was first observed in the western world in 1731 by John Bevis, and corresponds to a bright supernova recorded by Chinese and Arab astronomers in 1054. Located at a distance of about 6,500 light-years (2 kpc) from Earth, the nebula has a diameter of 11 ly (3.4 pc) and expands at a rate of about 1,500 kilometers per second.

At the center of the nebula lies the Crab Pulsar, a rotating neutron star, which emits pulses of radiation from gamma rays to radio waves with a spin rate of 30.2 times per second. The nebula was the first astronomical object identified with a historical supernova explosion.

The nebula acts as a source of radiation for studying celestial bodies that occult it. In the 1950s and 1960s, the Sun's corona was mapped from observations of the Crab's radio waves passing through it, and more recently, the thickness of the atmosphere of Saturn's moon Titan was measured as it blocked out X-rays from the nebula.

Origins

First observed in 1731 by John Bevis, the Crab Nebula corresponds to the bright SN 1054 supernova that was recorded by Chinese and Arab astronomers in 1054. The nebula was independently rediscovered in 1758 by Charles Messier as he was observing a bright comet. Messier catalogued it as the first entry in his catalogue of comet-like objects. The Earl of Rosse observed the nebula at Birr Castle in the 1840s, and referred to the object as the Crab Nebula because a drawing he made of it looked like a crab.[7]

In the early 20th century, the analysis of early photographs of the nebula taken several years apart revealed that it was expanding. Tracing the expansion back revealed that the nebula must have become visible on Earth about 900 years ago. Historical records revealed that a new star bright enough to be seen in the daytime had been recorded in the same part of the sky by Chinese and Arab astronomers in 1054[8][9] Given its great distance, the daytime "guest star" observed by the Chinese and Arabs could only have been a supernova—a massive, exploding star, having exhausted its supply of energy from nuclear fusion and collapsed in on itself.

Recent analysis of historical records have found that the supernova that created the Crab Nebula probably appeared in April or early May, rising to its maximum brightness of between apparent magnitude −7 and −4.5 (brighter than everything in the night sky except the Moon) by July. The supernova was visible to the naked eye for about two years after its first observation.[10] Thanks to the recorded observations of Far Eastern and Middle Eastern astronomers of 1054, Crab Nebula became the first astronomical object recognized as being connected to a supernova explosion.[9]

Physical conditions

The Crab Pulsar. This image combines optical data from Hubble (in red) and X-ray images from Chandra X-ray Observatory (in blue).

In visible light, the Crab Nebula consists of a broadly oval-shaped mass of filaments, about 6 arcminutes long and 4 arcminutes wide (by comparison, the full moon is 30 arcminutes across) surrounding a diffuse blue central region. In three dimensions, the nebula is thought to be shaped like a prolate spheroid.[3] The filaments are the remnants of the progenitor star's atmosphere, and consist largely of ionised helium and hydrogen, along with carbon, oxygen, nitrogen, iron, neon and sulfur. The filaments' temperatures are typically between 11,000 and 18,000 K, and their densities are about 1,300 particles per cm³.[11]

In 1953 Iosif Shklovsky proposed that the diffuse blue region is predominantly produced by synchrotron radiation, which is radiation given off by the curving of electrons moving at speeds up to half the speed of light.[12] Three years later the theory was confirmed by observations. In the 1960s it was found that the source of the electron curved paths was the strong magnetic field produced by a neutron star at the center of the nebula.[13]

Distance

Even though the Crab Nebula is the focus of much attention among astronomers, its distance remains an open question due to uncertainties in every method used to estimate its distance. In 2008, the general consensus is that its distance from Earth is 2.0 ± 0.5 kpc (6.5 ± 1.6 kly). The Crab Nebula is currently expanding outwards at about 1,500 km/s.[14] Images taken several years apart reveal the slow expansion of the nebula[15], and by comparing this angular expansion with its spectroscopically determined expansion velocity, the nebula's distance can be estimated. In 1973, an analysis of many different methods used to compute the distance to the nebula reached a conclusion of about 6,300 ly.[3] Along its longest visible dimension, it measures about 13 ± 3 ly across.[5]

Tracing back its expansion consistently yields a date for the creation of the nebula several decades after 1054, implying that its outward velocity has accelerated since the supernova explosion.[16] This acceleration is believed to be caused by energy from the pulsar that feeds into the nebula's magnetic field, which expands and forces the nebula's filaments outwards.[17]

Mass

Estimates of the total mass of the nebula are important for estimating the mass of the supernova's progenitor star. The amount of matter contained in the Crab Nebula's filaments (ejecta mass of ionized and neutral gas; mostly helium[18]) is estimated to be 4.6 ± 1.8 M☉.[19]

Helium-rich torus

One of the many nebular components (or anomalies) of the Crab is a helium-rich torus which is visible as an east-west band crossing the pulsar region. The torus composes about 25% of the visible ejecta and is composed of about 95% helium. As of yet, there has been no plausible explanation put forth for the structure of the torus.[20]

Central star

This sequence of Hubble Space Telescope images shows features in the inner Crab Nebula changing over a period of four months. Credit: NASA/ESA.

At the centre of the Crab Nebula are two faint stars, one of which is the star responsible for existence of the nebula. It was identified as such in 1942, when Rudolf Minkowski found that its optical spectrum was extremely unusual.[21] The region around the star was found to be a strong source of radio waves in 1949[22] and X-rays in 1963,[23] and was identified as one of the brightest objects in the sky in gamma rays in 1967.[24] Then, in 1968, the star was found to be emitting its radiation in rapid pulses, becoming one of the first pulsars to be discovered.

Pulsars are sources of powerful electromagnetic radiation, emitted in short and extremely regular pulses many times a second. They were a great mystery when discovered in 1967, and the team which identified the first one considered the possibility that it could be a signal from an advanced civilization.[25] However, the discovery of a pulsating radio source in the centre of the Crab Nebula was strong evidence that pulsars were formed by supernova explosions. They are now understood to be rapidly rotating neutron stars, whose powerful magnetic field concentrates their radiation emissions into narrow beams.

The Crab Pulsar is believed to be about 28–30 km in diameter;[26] it emits pulses of radiation every 33 milliseconds.[27] Pulses are emitted at wavelengths across the electromagnetic spectrum, from radio waves to X-rays. Like all isolated pulsars, its period is slowing very gradually. Occasionally, its rotational period shows sharp changes, known as 'glitches', which are believed to be caused by a sudden realignment inside the neutron star. The energy released as the pulsar slows down is enormous, and it powers the emission of the synchrotron radiation of the Crab Nebula, which has a total luminosity about 75,000 times greater than that of the Sun.[28]

The pulsar's extreme energy output creates an unusually dynamic region at the centre of the Crab Nebula. While most astronomical objects evolve so slowly that changes are visible only over timescales of many years, the inner parts of the Crab show changes over timescales of only a few days.[29] The most dynamic feature in the inner part of the nebula is the point where the pulsar's equatorial wind slams into the bulk of the nebula, forming a shock front. The shape and position of this feature shifts rapidly, with the equatorial wind appearing as a series of wisp-like features that steepen, brighten, then fade as they move away from the pulsar to well out into the main body of the nebula.

Progenitor star

The Crab Nebula seen in infrared by the Spitzer Space Telescope.

The star that exploded as a supernova is referred to as the supernova's progenitor star. Two types of stars explode as supernovae: white dwarfs and massive stars. In the so-called Type Ia supernovae, gases falling onto a white dwarf raise its mass until it nears a critical level, the Chandrasekhar limit, resulting in an explosion; in Type Ib/c and Type II supernovae, the progenitor star is a massive star which runs out of fuel to power its nuclear fusion reactions and collapses in on itself, reaching such phenomenal temperatures that it explodes. The presence of a pulsar in the Crab means that it must have formed in a core-collapse supernova; Type Ia supernovae do not produce pulsars.

Theoretical models of supernova explosions suggest that the star that exploded to produce the Crab Nebula must have had a mass of between 9 and 11 M☉.[30][20] Stars with masses lower than 8 solar masses are thought to be too small to produce supernova explosions, and end their lives by producing a planetary nebula instead, while a star heavier than 12 solar masses would have produced a nebula with a different chemical composition to that observed in the Crab.[31]

A significant problem in studies of the Crab Nebula is that the combined mass of the nebula and the pulsar add up to considerably less than the predicted mass of the progenitor star, and the question of where the 'missing mass' is remains unresolved.[19] Estimates of the mass of the nebula are made by measuring the total amount of light emitted, and calculating the mass required, given the measured temperature and density of the nebula. Estimates range from about 1–5 solar masses, with 2–3 solar masses being the generally accepted value.[31] The neutron star mass is estimated to be between 1.4 and 2 solar masses.

The predominant theory to account for the missing mass of the Crab is that a substantial proportion of the mass of the progenitor was carried away before the supernova explosion in a fast stellar wind. However, this would have created a shell around the nebula. Although attempts have been made at several different wavelengths to observe a shell, none has yet been found.[32]

Transits by solar system bodies

Hubble Space Telescope image of a small region of the Crab Nebula, showing Rayleigh–Taylor instabilities in its intricate filamentary structure. Credit: NASA/ESA.

The Crab Nebula lies roughly 1½ ° away from the ecliptic—the plane of Earth's orbit around the Sun. This means that the Moon — and occasionally, planets — can transit or occult the nebula. Although the Sun does not transit the nebula, its corona passes in front of it. These transits and occultations can be used to analyse both the nebula and the object passing in front of it, by observing how radiation from the nebula is altered by the transiting body.

Lunar transits have been used to map X-ray emissions from the nebula. Before the launch of X-ray-observing satellites, such as the Chandra X-ray Observatory, X-ray observations generally had quite low angular resolution, but when the Moon passes in front of the nebula, its position is very accurately known, and so the variations in the nebula's brightness can be used to create maps of X-ray emission.[33] When X-rays were first observed from the Crab, a lunar occultation was used to determine the exact location of their source.[23]

The Sun's corona passes in front of the Crab every June. Variations in the radio waves received from the Crab at this time can be used to infer details about the corona's density and structure. Early observations established that the corona extended out to much greater distances than had previously been thought; later observations found that the corona contained substantial density variations.[34]

Very rarely, Saturn transits the Crab Nebula. Its transit in 2003 was the first since 1296; another will not occur until 2267. Observers used the Chandra X-ray Observatory to observe Saturn's moon Titan as it crossed the nebula, and found that Titan's X-ray 'shadow' was larger than its solid surface, due to absorption of X-rays in its atmosphere. These observations showed that the thickness of Titan's atmosphere is 880 km.[35] The transit of Saturn itself could not be observed, because Chandra was passing through the Van Allen belts at the time.

See also

Notes

  1. ↑ 1.0 1.1 1.2 1.3 SIMBAD Astronomical Database. Results for NGC 1952. Retrieved 2006-12-25.
  2. ↑ Kaplan, D. L.; S. Chatterjee & B. M. Gaensler et al. (2008), "A Precise Proper Motion for the Crab Pulsar, and the Difficulty of Testing Spin-Kick Alignment for Young Neutron Stars", Accepted for publication in the Astrophysical Journal 677: 1201, DOI:10.1086/529026 
  3. ↑ 3.0 3.1 3.2 Trimble, Virginia Louise (October 1973), "The Distance to the Crab Nebula and NP 0532", Publications of the Astronomical Society of the Pacific 85 (507): 579, DOI:10.1086/129507 
  4. ↑ van den Bergh, Sidney. 1970. The Astrophysical Journal (letters). 160: L27.
  5. ↑ 5.0 5.1 distance × tan( diameter_angle = 420″ ) = 4.1 ± 1.0 pc diameter = 13 ± 3 ly diameter
  6. ↑ Apparent Magnitude of 8.4 - distance modulus of 11.5 ± 0.5 = −3.1 ± 0.5.
  7. ↑ Glyn Jones K. (1976), The Search for the Nebulae, Journal of the History of Astronomy, v. 7, p.67
  8. ↑ Lundmark K. (1921), Suspected New Stars Recorded in Old Chronicles and Among Recent Meridian Observations'', Publications of the Astronomical Society of the Pacific, v. 33, p.225
  9. ↑ 9.0 9.1 Mayall N.U. (1939), The Crab Nebula, a Probable Supernova, Astronomical Society of the Pacific Leaflets, v. 3, p.145
  10. ↑ Collins, George W., II; William P. Claspy & John C. Martin (July 1999), "A Reinterpretation of Historical References to the Supernova of A.D. 1054", The Publications of the Astronomical Society of the Pacific 111 (761): 871-880 
  11. ↑ Fesen, R. A. & R. P. Kirshner (July 1 1982), "The Crab Nebula. I - Spectrophotometry of the filaments", Astrophysical Journal 258 (1): 1, DOI:10.1086/160043 
  12. ↑ Shklovskii, Iosif (1953). On the Nature of the Crab Nebula’s Optical Emission. Doklady Akademii Nauk SSSR 90: 983.
  13. ↑ Burn B.J. (1973), A synchrotron model for the continuum spectrum of the Crab Nebula, Monthly Notices of the Royal Astronomical Society, v. 165, p. 421 (1973)
  14. ↑ Bietenholz, M. F.; P. P. Kronberg & D. E. Hogg et al. (June 1, 1991), "The expansion of the Crab Nebula", Astrophysical Journal, Part 2 - Letters (ISSN 0004-637X); Research supported by NSERC and University of Toronto 373: L59, DOI:10.1086/186051 
  15. ↑ Animation showing expansion from 1973 to 2001
  16. ↑ Trimble, Virginia Louise (September 1968), "Motions and Structure of the Filamentary Envelope of the Crab Nebula", Astronomical Journal 73: 535, DOI:10.1086/110658 
  17. ↑ Bejger, M. & P. Haensel (July 2003), "Accelerated expansion of the Crab Nebula and evaluation of its neutron-star parameters", Astronomy and Astrophysics 405: 747, DOI:10.1051/0004-6361:20030642 
  18. ↑ Green, D. A.; R. J. Tuffs & C. C. Popescu (December 2004), "Far-infrared and submillimetre observations of the Crab nebula", Monthly Notices of the Royal Astronomical Society 355 (4): 1315, DOI:10.1111/j.1365-2966.2004.08414.x 
  19. ↑ 19.0 19.1 Fesen, Robert A.; J. Michael Shull & Alan P. Hurford (January 1997), "An Optical Study of the Circumstellar Environment Around the Crab Nebula", Astronomical Journal 113: 354, DOI:10.1086/118258 
  20. ↑ 20.0 20.1 MacAlpine, Gordon M.; Tait C. Ecklund & William R. Lester et al. (January 2007), "A Spectroscopic Study of Nuclear Processing and the Production of Anomalously Strong Lines in the Crab Nebula", The Astronomical Journal 133 (1): 81, DOI:10.1086/509504 
  21. ↑ Minkowski R. (1942), The Crab Nebula, Astrophysical Journal, v. 96, p.199
  22. ↑ Bolton J.G., Stanley G.J., Slee O.B. (1949), Positions of three discrete sources of Galactic radio frequency radiation, Nature, v. 164, p. 101
  23. ↑ 23.0 23.1 Bowyer S., Byram E.T., Chubb T.A., Friedman H. (1964), Lunar Occultation of X-ray Emission from the Crab Nebula, Science, v. 146, pp. 912–917
  24. ↑ Haymes R.C., Ellis D.V., Fishman G.J., Kurfess J.D., Tucker, W.H. (1968), Observation of Gamma Radiation from the Crab Nebula, Astrophysical Journal, v. 151, p.L9
  25. ↑ Del Puerto C. (2005), Pulsars In The Headlines, EAS Publications Series, v. 16, pp.115–119
  26. ↑ Bejger, M. & P. Haensel (December 2002), "Moments of inertia for neutron and strange stars: Limits derived for the Crab pulsar", Astronomy and Astrophysics 396: 917, DOI:10.1051/0004-6361:20021241 
  27. ↑ Harnden F.R., Seward F.D. (1984), Einstein observations of the Crab nebula pulsar, Astrophysical Journal, v. 283, p. 279–285
  28. ↑ Kaufmann W.J. (1996), Universe 4th edition, Freeman press, p. 428
  29. ↑ Hester J.J., Scowen P.A., Sankrit R., Michel F.C., Graham J.R., Watson A., Gallagher J.S. (1996), The Extremely Dynamic Structure of the Inner Crab Nebula, Bulletin of the American Astronomical Society, Vol. 28, p.950
  30. ↑ Nomoto, K. (October 11, 1984), "Evolutionary models of the Crab Nebula's progenitor", The Crab Nebula and related supernova remnants; Proceedings of the Workshop, (A86-41101 19-90). Sponsorship: Ministry of Education, Science, and Culture.: 97-113, Fairfax, VA: Cambridge University Press 
  31. ↑ 31.0 31.1 Davidson, K. & R. A. Fesen (1985), "Recent developments concerning the Crab Nebula", Annual review of astronomy and astrophysics. (A86-14507 04-90) 23 (507): 119, Palo Alto, CA: Annual Reviews, Inc., DOI:10.1146/annurev.aa.23.090185.001003 
  32. ↑ Frail D.A., Kassim N.E., Cornwell T.J., Goss W.M. (1995), Does the Crab Have a Shell?, Astrophysical Journal, v. 454, p. L129–L132
  33. ↑ Palmieri T.M., Seward F.D., Toor A., van Flandern T.C. (1975), Spatial distribution of X-rays in the Crab Nebula, Astrophysical Journal, v. 202, p. 494–497
  34. ↑ Erickson W.C. (1964), The Radio-Wave Scattering Properties of the Solar Corona, Astrophysical Journal, v. 139, p.1290
  35. ↑ Mori K., Tsunemi H., Katayama H., Burrows D.N., Garmire G.P., Metzger A.E. (2004), An X-Ray Measurement of Titan's Atmospheric Extent from Its Transit of the Crab Nebula, Astrophysical Journal, v. 607, pp. 1065–1069. Chandra images used by Mori et al can be viewed here.

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