Information about Crab Nebula
M1, the Crab Nebula. Courtesy of NASA/ESA | |
| Observation data: J2000.0 epoch | |
|---|---|
| Type: | Supernova Remnant |
| Right ascension: | 05h 34m 31.97s[1] |
| Declination: | +22° 00′ 52.1″<ref name="simbad" /> |
| Distance: | 6,300 ly |
| Apparent magnitude (V): | +8.4 |
| Apparent dimensions (V): | 6 × 4 arcmin |
| Constellation: | Taurus |
| Physical characteristics | |
| Radius: | 3 ly |
| Absolute magnitude (V): | −3 |
| Notable features: | Optical pulsar |
| Other designations: | M 1,<ref name="simbad" /> NGC 1952<ref name="simbad" /> |
| See also: Diffuse nebula, | |
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
Recent analyses of historical records have found that the supernova that created the Crab Nebula probably occurred 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.[5] 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.[4]
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 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.[8] 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.[9]
The Crab Nebula is currently expanding outwards at about 1,500 km/s.[10] Images taken several years apart reveal the slow expansion of the nebula, and by comparing this angular expansion with its spectroscopically determined expansion velocity, the nebula's distance can be estimated. Modern observations give a distance to the nebula of about 6,300 ly,[11] meaning that it is about 11 ly in length.
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.[12] 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.[13]
Estimates of the total mass of the nebula are important for estimating the mass of the supernova's progenitor star. Estimates of the amount of matter contained in the filaments of the Crab Nebula range from about 1–5 solar masses;[14] although other estimates based on the investigation of the Crab Pulsar yield different numbers.
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.
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.[19] 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;[20] it emits pulses of radiation every 33 milliseconds.[21] 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.[22]
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.[23] 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 star that exploded as a supernova is referred to as the supernova's progenitor star. Two types of star 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 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 8 and 12 solar masses. 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.[24]
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.[25] 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.<ref name="Davidson" /> 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.[26]
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.
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.[27] When X-rays were first observed from the Crab, a lunar occultation was used to determine the exact location of their source.<ref name="Bowyer" />
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.[28]
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.[29] The transit of Saturn itself could not be observed, because Chandra was passing through the Van Allen belts at the time.
In fiction
- See Crab Nebula in fiction.
References
1. ^ SIMBAD Astronomical Database. Results for NGC 1952. Retrieved on 2006-12-25.
2. ^ Glyn Jones K. (1976), The Search for the Nebulae, Journal of the History of Astronomy, v. 7, p.67
3. ^ 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
4. ^ Mayall N.U. (1939), The Crab Nebula, a Probable Supernova'', Astronomical Society of the Pacific Leaflets, v. 3, p.145
5. ^ Collins G.W., Claspy W.P., Martin J.C. (1999), Reinterpretation of Historical References to the Supernova of A.D. 1054, Publications of the Astronomical Society of the Pacific, v. 111, p. 871
6. ^ Mayall N.U. (1939), The Crab Nebula, a Probable Supernova, Astronomical Society of the Pacific Leaflets, v. 3, p.145
7. ^ Fesen R.A., Kirshner R.P. (1982), The Crab Nebula. I - Spectrophotometry of the filaments, Astrophysical Journal, v. 258, p. 1–10
8. ^ Shklovskii, Iosif (1953). "On the Nature of the Crab Nebula’s Optical Emission". Doklady Akademii Nauk SSSR 90: 983.
9. ^ 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)
10. ^ Bietenholz M.F., Kronberg P.P., Hogg D.E., Wilson A.S. (1991), The expansion of the Crab Nebula, Astrophysical Journal Letters, vol. 373, p. L59-L62
11. ^ Trimble, V. (1973), The Distance to the Crab Nebula and NP 0532, Publications of the Astronomical Society of the Pacific, v. 85, p. 579
12. ^ Trimble V. (1968), Motions and Structure of the Filamentary Envelope of the Crab Nebula, Astronomical Journal, v. 73, p. 535
13. ^ Bejger M., Haensel P. (2003), Accelerated expansion of the Crab Nebula and evaluation of its neutron-star parameters, Astronomy and Astrophysics, v.405, p.747–751
14. ^ Fesen R.A., Shull J.M., Hurford A.P. (1997), An Optical Study of the Circumstellar Environment Around the Crab Nebula, Astronomical Journal v.113, p. 354-363
15. ^ Minkowski R. (1942), The Crab Nebula, Astrophysical Journal, v. 96, p.199
16. ^ 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
17. ^ Bowyer S., Byram E.T., Chubb T.A., Friedman H. (1964), Lunar Occulation of X-ray Emission from the Crab Nebula, Science, v. 146, pp. 912–917
18. ^ 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
19. ^ Del Puerto C. (2005), Pulsars In The Headlines, EAS Publications Series, v. 16, pp.115–119
20. ^ M. Bejger and P. Haensel (2002), Moments of inertia for neutron and strange stars: Limits derived for the Crab pulsar, Astronomy and Astrophysics , v. 396, p. 917–921
21. ^ Harnden F.R., Seward F.D. (1984), Einstein observations of the Crab nebula pulsar, Astrophysical Journal, v. 283, p. 279–285
22. ^ Kaufmann W.J. (1996), Universe 4th edition, Freeman press, p. 428
23. ^ 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
24. ^ Davidson K., Fesen R.A. (1985), Recent developments concerning the Crab Nebula, Annual Review of Astronomy and Astrophysics, v. 23, p. 119–146
25. ^ Fesen R.A., Shull J.M., Hurford A.P. (1997), An Optical Study of the Circumstellar Environment Around the Crab Nebula, Astronomical Journal v.113, p. 354–363
26. ^ 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
27. ^ 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
28. ^ Erickson W.C. (1964), The Radio-Wave Scattering Properties of the Solar Corona, Astrophysical Journal, v. 139, p.1290
29. ^ 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.
2. ^ Glyn Jones K. (1976), The Search for the Nebulae, Journal of the History of Astronomy, v. 7, p.67
3. ^ 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
4. ^ Mayall N.U. (1939), The Crab Nebula, a Probable Supernova'', Astronomical Society of the Pacific Leaflets, v. 3, p.145
5. ^ Collins G.W., Claspy W.P., Martin J.C. (1999), Reinterpretation of Historical References to the Supernova of A.D. 1054, Publications of the Astronomical Society of the Pacific, v. 111, p. 871
6. ^ Mayall N.U. (1939), The Crab Nebula, a Probable Supernova, Astronomical Society of the Pacific Leaflets, v. 3, p.145
7. ^ Fesen R.A., Kirshner R.P. (1982), The Crab Nebula. I - Spectrophotometry of the filaments, Astrophysical Journal, v. 258, p. 1–10
8. ^ Shklovskii, Iosif (1953). "On the Nature of the Crab Nebula’s Optical Emission". Doklady Akademii Nauk SSSR 90: 983.
9. ^ 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)
10. ^ Bietenholz M.F., Kronberg P.P., Hogg D.E., Wilson A.S. (1991), The expansion of the Crab Nebula, Astrophysical Journal Letters, vol. 373, p. L59-L62
11. ^ Trimble, V. (1973), The Distance to the Crab Nebula and NP 0532, Publications of the Astronomical Society of the Pacific, v. 85, p. 579
12. ^ Trimble V. (1968), Motions and Structure of the Filamentary Envelope of the Crab Nebula, Astronomical Journal, v. 73, p. 535
13. ^ Bejger M., Haensel P. (2003), Accelerated expansion of the Crab Nebula and evaluation of its neutron-star parameters, Astronomy and Astrophysics, v.405, p.747–751
14. ^ Fesen R.A., Shull J.M., Hurford A.P. (1997), An Optical Study of the Circumstellar Environment Around the Crab Nebula, Astronomical Journal v.113, p. 354-363
15. ^ Minkowski R. (1942), The Crab Nebula, Astrophysical Journal, v. 96, p.199
16. ^ 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
17. ^ Bowyer S., Byram E.T., Chubb T.A., Friedman H. (1964), Lunar Occulation of X-ray Emission from the Crab Nebula, Science, v. 146, pp. 912–917
18. ^ 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
19. ^ Del Puerto C. (2005), Pulsars In The Headlines, EAS Publications Series, v. 16, pp.115–119
20. ^ M. Bejger and P. Haensel (2002), Moments of inertia for neutron and strange stars: Limits derived for the Crab pulsar, Astronomy and Astrophysics , v. 396, p. 917–921
21. ^ Harnden F.R., Seward F.D. (1984), Einstein observations of the Crab nebula pulsar, Astrophysical Journal, v. 283, p. 279–285
22. ^ Kaufmann W.J. (1996), Universe 4th edition, Freeman press, p. 428
23. ^ 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
24. ^ Davidson K., Fesen R.A. (1985), Recent developments concerning the Crab Nebula, Annual Review of Astronomy and Astrophysics, v. 23, p. 119–146
25. ^ Fesen R.A., Shull J.M., Hurford A.P. (1997), An Optical Study of the Circumstellar Environment Around the Crab Nebula, Astronomical Journal v.113, p. 354–363
26. ^ 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
27. ^ 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
28. ^ Erickson W.C. (1964), The Radio-Wave Scattering Properties of the Solar Corona, Astrophysical Journal, v. 139, p.1290
29. ^ 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.
External links
- Crab Nebula at ESA/Hubble
- Messier 1, SEDS Messier pages
- Images of the Crab from the Chandra X-ray Observatory
- Chandra page about the nebula
- Images of the Crab from the Hubble Space Telescope
- Lord Rosse's drawings of M1, the Crab Nebula from SEDS
- NightSkyInfo.com - M1, the Crab Nebula
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Agency overview
Formed 29 July 1958
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European Space Agency (ESA), established in 1974, is an inter-governmental organisation dedicated to the exploration of space, currently with 17 member states. Its headquarters are in Paris.
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Right ascension (abbrev. RA; symbol α) is the astronomical term for one of the two coordinates of a point on the celestial sphere when using the equatorial coordinate system. The other coordinate is the declination.
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In astronomy, declination (abbrev. dec or δ) is one of the two coordinates of the equatorial coordinate system, the other being either right ascension or hour angle.
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1 light-year =
SI units
01015 m 01012 km
Astronomical units
0103 AU 0 pc
US customary / Imperial units
01015 ft 01012 mi
A light-year or lightyear (symbol: SI units
01015 m 01012 km
Astronomical units
0103 AU 0 pc
US customary / Imperial units
01015 ft 01012 mi
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The apparent magnitude (m) of a celestial body is a measure of its brightness as seen by an observer on Earth, normalized to the value it would have in the absence of the atmosphere.
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A minute of arc, arcminute, or MOA is a unit of angular measurement, equal to one sixtieth (1/60) of one degree. [1] Since one degree is defined as one three hundred sixtieth (1/360) of a circle, 1 MOA is 1/21600 of the amount of arc in a closed circle, or
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constellation of Orion is the area outlined in the dashed yellow line. Orion contains a striking and well-known star pattern that has the form of a hunter.]] A constellation is any one of the 88 areas into which the sky — or the celestial sphere — is divided.
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Taurus
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List of stars in Taurus
Abbreviation: Tau
Genitive: Tauri
Symbology: the Bull
Right ascension: 4 h
Declination: +15
Area: 797 sq. deg.
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Click for larger image
List of stars in Taurus
Abbreviation: Tau
Genitive: Tauri
Symbology: the Bull
Right ascension: 4 h
Declination: +15
Area: 797 sq. deg.
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In classical geometry, a radius (plural: radii) of a circle or sphere is any line segment from its center to its perimeter. By extension, the radius of a circle or sphere is the length of any such segment. The radius is half the diameter.
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In astronomy, absolute magnitude is the apparent magnitude, m, an object would have if it were at a standard luminosity distance away from us, in the absence of interstellar extinction. It allows the overall brightnesses of objects to be compared without regard to distance.
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Pulsars are highly magnetized rotating neutron stars which emit a beam of detectable electromagnetic radiation in the form of radio waves. Their periods range from 1.5 ms to 8.5 s[1].
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diffuse nebulae is the general term for illuminated nebulae. The three types of diffuse nebulae are reflection nebulae, emission nebulae and supernova remnants. They are diffuse as opposed to the non-diffuse dark nebulae, i.e. the particles have spread out.
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Messier objects are a set of astronomical objects catalogued by French astronomer Charles Messier in his catalogue of Nebulae and Star Clusters first published in 1774.
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New General Catalogue (NGC)
Spiral Galaxy NGC 3982 displays numerous spiral arms filled with bright stars, blue star clusters, and dark dust lanes. It spans about 30,000 light years, lies about 68 million light years from Earth and can be seen with a small telescope
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Spiral Galaxy NGC 3982 displays numerous spiral arms filled with bright stars, blue star clusters, and dark dust lanes. It spans about 30,000 light years, lies about 68 million light years from Earth and can be seen with a small telescope
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supernova remnant (SNR) is the structure resulting from the gigantic explosion of a star in a supernova. The supernova remnant is bounded by an expanding shock wave, and consists of ejected material expanding from the explosion, and the interstellar material it sweeps up and
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pulsar wind nebula (also known as "plerion", derived from Ancient Greek "pleres" meaning "full" - a term coined by Weiler & Panagia (1978)) is a synchrotron nebula powered by the relativistic wind of an energetic pulsar.
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constellation of Orion is the area outlined in the dashed yellow line. Orion contains a striking and well-known star pattern that has the form of a hunter.]] A constellation is any one of the 88 areas into which the sky — or the celestial sphere — is divided.
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Taurus
Click for larger image
List of stars in Taurus
Abbreviation: Tau
Genitive: Tauri
Symbology: the Bull
Right ascension: 4 h
Declination: +15
Area: 797 sq. deg.
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Click for larger image
List of stars in Taurus
Abbreviation: Tau
Genitive: Tauri
Symbology: the Bull
Right ascension: 4 h
Declination: +15
Area: 797 sq. deg.
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nebula (from Latin: "mist" [1] ; pl. nebulae or nebulæ, with ligature) is an interstellar cloud of dust, hydrogen gas and plasma. It is the first stage of a star's cycle.
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John Bevis (October 311693 or November 101695 – November 6, 1771) was an English doctor and astronomer. He is best known for discovering the Crab Nebula in 1731.
Bevis was born in Old Sarum, Wiltshire.
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Bevis was born in Old Sarum, Wiltshire.
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Astronomy in China has a very long history.
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Islamic astronomy or Arabic astronomy refers to the astronomical developments made by the Islamic civilization between the 8th and 17th centuries and written in Arabic.
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Supernova SN 1054
The Crab Nebula, remnant of SN 1054. Credit: NASA/ESA.
Observation data
(Epoch ?)
Supernova type Type II
Remnant type Nebula
Host Galaxy Milky Way
Constellation Taurus
Right ascension 5h 34.
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The Crab Nebula, remnant of SN 1054. Credit: NASA/ESA.
Observation data
(Epoch ?)
Supernova type Type II
Remnant type Nebula
Host Galaxy Milky Way
Constellation Taurus
Right ascension 5h 34.
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1 light-year =
SI units
01015 m 01012 km
Astronomical units
0103 AU 0 pc
US customary / Imperial units
01015 ft 01012 mi
A light-year or lightyear (symbol: SI units
01015 m 01012 km
Astronomical units
0103 AU 0 pc
US customary / Imperial units
01015 ft 01012 mi
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parsec (symbol pc) is a unit of length used in astronomy. The length of the parsec is based on the method of trigonometric parallax, one of the oldest methods for measuring the distances to stars.
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EARTH was a short-lived Japanese vocal trio which released 6 singles and 1 album between 2000 and 2001. Their greatest hit, their debut single "time after time", peaked at #13 in the Oricon singles chart.
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nebula (from Latin: "mist" [1] ; pl. nebulae or nebulæ, with ligature) is an interstellar cloud of dust, hydrogen gas and plasma. It is the first stage of a star's cycle.
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1 kilometre =
SI units
0 m 0106 mm
US customary / Imperial units
0 ft 0 mi
A kilometre (American spelling: kilometer, symbol kmSI units
0 m 0106 mm
US customary / Imperial units
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