Cassiopeia A
The brightest extrasolar radio source below 1 GHz, a supernova remnant in Cassiopeia.
Cassiopeia A (Cas A) is a supernova remnant (SNR) in the constellation Cassiopeia and the brightest extrasolar radio source in the sky at frequencies below 1 GHz. The supernova occurred approximately 11000 ly away within the Milky Way; given the width of the Orion Arm, it lies in the next-nearest arm outwards, the Perseus Arm, about 30 degrees from the Galactic anticenter. The expanding cloud of material left over from the supernova now appears approximately 10 ly across from Earth's perspective.
- type
- Supernova remnant
- constellation
- Cassiopeia
- distance
- Approximately 11,000 light-years (3.4 kpc)
- discovery_year
- 1948 (radio); 1951 (optical)
- discoverers
- Martin Ryle and Francis Graham-Smith
- known_for
- Brightest extrasolar radio source below 1 GHz; first discrete radio source found
Quick Facts
- Epoch
- J2000
- Snrtype
- Shell
- Host
- Milky Way
- Ra
- 23 · 23 · 26.0
- Dec
- +58 · 48 · 41
- Gal
- 111.734745°, −02.129570°
- Discovery
- 1947 by Martin Ryle and Francis Graham-Smith)
- Distance
- 11,000 ly
- Mag V
- 6
- Notes
- Strongest radio source beyond the Solar System
- Predecessor
- SN 1604
- Successor
- G1.9+0.3 (unobserved, c. 1868), SN 1885A (next observed)
Facts from the source article.
Lore & Background
It is estimated that light from the supernova itself first reached Earth near 1680 (±30 years), although there are no definitively corresponding records from then. Cas A is circumpolar at and above mid-Northern latitudes which had extensive records and basic telescopes. Its likely omission in records is probably due to interstellar dust absorbing optical wavelength radiation before it reached Earth, although it is possible that it was recorded as a sixth magnitude star 3 Cassiopeiae by John Flamsteed in 1680. Possible explanations lean toward the idea that the source star was unusually massive and had previously ejected much of its outer layers. These outer layers would have cloaked the star and absorbed much of the visible-light emission as the inner star collapsed. Cas A was among the first discrete astronomical radio sources found. Its discovery was reported in 1948 by Martin Ryle and Francis Graham-Smith, astronomers at Cambridge, based on observations with the Long Michelson Interferometer. The optical component was first identified in 1951.
Reader's Guide
The expansion shell has a temperature of around 30 million K, and is expanding at 4,000−6,000 km/s. Observations of the exploded star through the Hubble Space Telescope have shown that, despite the original belief that the remnants were expanding in a uniform manner, there are high velocity outlying eject knots moving with transverse velocities of 5,500−14,500 km/s with the highest speeds occurring in two nearly opposing jets. When the view of the expanding star uses colors to differentiate materials of different chemical compositions, it shows that similar materials often remain gathered together in the remnants of the explosion. Cas A had a flux density of at 1 GHz in 1980. Because the supernova remnant is cooling, its flux density is decreasing. At 1 GHz, its flux density is decreasing at a rate of per year. This decrease means that, at frequencies below 1 GHz, Cas A is now less intense than Cygnus A. Cas A is still the brightest extrasolar radio source in the sky at frequencies above 1 GHz. In 1999, the Chandra X-Ray Observatory found CXOU J232327.8+584842, a central compact object that is the neutron star remnant left by the explosion.
Did You Know?
- In 2005 an infrared echo of the Cassiopeia A explosion was observed on nearby gas clouds using Spitzer Space Telescope. The infrared echo was also seen by IRAS and studied with the Infrared Spectrograph on Spitzer.
- The recorded spectrum of the optical light echo proved the supernova was of Type IIb, meaning it resulted from the internal collapse and violent explosion of a massive star, most probably a red supergiant with a helium c
- In 2013, astronomers detected phosphorus in Cassiopeia A, which confirmed that this element is produced in supernovae through supernova nucleosynthesis. The phosphorus-to-iron ratio in material from the supernova remnant
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