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When supernovae explode, these elements (as well as the ones the star made during more stable times) are ejected into the existing gas between the stars and mixed with it. Thus, supernovae play a crucial role in enriching their galaxy with heavier elements, allowing, among other things, the chemical elements that make up earthlike planets and the building blocks of life to become more common as time goes on ( [link] ).

Kepler supernova remant.

Multi-wavelength Image of the Kepler Supernova Remant. In this image labeled at top as: “Kepler’s Supernova Remnant - SN 1604”, the upper panel shows the final combined image of this diffuse, spherical shell of gas. Inset at bottom are the individual images at different wavelengths. From left to right: “X-ray (Chandra X-ray Observatory)” in blue, “X-ray (Chandra X-ray Observatory)” in green, “Visible (Hubble Space Telescope)” in yellow, and “Infrared (Spitzer Space Telescope)” in red. The credit at bottom reads: “NASA, ESA, R. Sankrit and W. Blair (Johns Hopkins University) STScI-PRC04-29a”.
This image shows the expanding remains of a supernova explosion, which was first seen about 400 years ago by sky watchers, including the famous astronomer Johannes Kepler. The bubble-shaped shroud of gas and dust is now 14 light-years wide and is expanding at 2,000 kilometers per second (4 million miles per hour). The remnant emits energy at wavelengths from X-rays (shown in blue and green) to visible light (yellow) and into the infrared (red). The expanding shell is rich in iron, which was produced in the star that exploded. The main image combines the individual single-color images seen at the bottom into one multi-wavelength picture. (credit: modification of work by NASA, ESA, R. Sankrit and W. Blair (Johns Hopkins University))

Supernovae are also thought to be the source of many of the high-energy cosmic ray particles discussed in Cosmic Rays . Trapped by the magnetic field of the Galaxy, the particles from exploded stars continue to circulate around the vast spiral of the Milky Way. Scientists speculate that high-speed cosmic rays    hitting the genetic material of Earth organisms over billions of years may have contributed to the steady mutations —subtle changes in the genetic code—that drive the evolution of life on our planet. In all the ways we have mentioned, supernovae have played a part in the development of new generations of stars, planets, and life.

But supernovae also have a dark side. Suppose a life form has the misfortune to develop around a star that happens to lie near a massive star destined to become a supernova. Such life forms may find themselves snuffed out when the harsh radiation and high-energy particles from the neighboring star’s explosion reach their world. If, as some astronomers speculate, life can develop on many planets around long-lived (lower-mass) stars, then the suitability of that life’s own star and planet may not be all that matters for its long-term evolution and survival. Life may well have formed around a number of pleasantly stable stars only to be wiped out because a massive nearby star suddenly went supernova. Just as children born in a war zone may find themselves the unjust victims of their violent neighborhood, life too close to a star that goes supernova may fall prey to having been born in the wrong place at the wrong time.

What is a safe distance to be from a supernova explosion? A lot depends on the violence of the particular explosion, what type of supernova it is (see The Evolution of Binary Star Systems ), and what level of destruction we are willing to accept. Calculations suggest that a supernova less than 50 light-years away from us would certainly end all life on Earth, and that even one 100 light-years away would have drastic consequences for the radiation levels here. One minor extinction of sea creatures about 2 million years ago on Earth may actually have been caused by a supernova at a distance of about 120 light-years.

The good news is that there are at present no massive stars that promise to become supernovae within 50 light-years of the Sun. (This is in part because the kinds of massive stars that become supernovae are overall quite rare.) The massive star closest to us, Spica (in the constellation of Virgo), is about 260 light-years away, probably a safe distance, even if it were to explode as a supernova in the near future.

Extreme gravity

In this section, you were introduced to some very dense objects. How would those objects’ gravity affect you? Recall that the force of gravity, F , between two bodies is calculated as

F = G M 1 M 2 R 2

where G is the gravitational constant, 6.67 × 10 –11 Nm 2 /kg 2 , M 1 and M 2 are the masses of the two bodies, and R is their separation. Also, from Newton’s second law,

F = M × a

where a is the acceleration of a body with mass M .

So let’s consider the situation of a mass—say, you—standing on a body, such as Earth or a white dwarf (where we assume you will be wearing a heat-proof space suit). You are M 1 and the body you are standing on is M 2 . The distance between you and the center of gravity of the body on which you stand is its radius, R . The force exerted on you is

F = M 1 × a = GM 1 M 2 / R 2

Solving for a , the acceleration of gravity on that world, we get

g = ( G × M ) R 2

Note that we have replaced the general symbol for acceleration, a , with the symbol scientists use for the acceleration of gravity, g .

Say that a particular white dwarf has the mass of the Sun (2 × 10 30 kg) but the radius of Earth (6.4 × 10 6 m). What is the acceleration of gravity at the surface of the white dwarf?

Solution

The acceleration of gravity at the surface of the white dwarf is

g ( white dwarf ) = ( G × M Sun ) R Earth 2 = ( 6.67 × 10 −11 m 2 /kg s 2 × 2 × 10 30 kg ) ( 6.4 × 10 6 m ) 2 = 3.26 × 10 6 m/s 2

Compare this to g on the surface of Earth, which is 9.8 m/s 2 .

Check your learning

What is the acceleration of gravity at the surface if the white dwarf has the twice the mass of the Sun and is only half the radius of Earth?

Answer:

g ( white dwarf ) = ( G × 2 M Sun ) ( 0.5 R Earth ) 2 = ( 6.67 × 10 −11 m 2 /kg s 2 × 4 × 10 30 kg ) ( 3.2 × 10 6 ) 2 = 2.61 × 10 7 m/s 2

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Key concepts and summary

In a massive star, hydrogen fusion in the core is followed by several other fusion reactions involving heavier elements. Just before it exhausts all sources of energy, a massive star has an iron core surrounded by shells of silicon, sulfur, oxygen, neon, carbon, helium, and hydrogen. The fusion of iron requires energy (rather than releasing it). If the mass of a star’s iron core exceeds the Chandrasekhar limit (but is less than 3 M Sun ), the core collapses until its density exceeds that of an atomic nucleus, forming a neutron star with a typical diameter of 20 kilometers. The core rebounds and transfers energy outward, blowing off the outer layers of the star in a type II supernova explosion.

Practice Key Terms 2

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Source:  OpenStax, Astronomy. OpenStax CNX. Apr 12, 2017 Download for free at http://cnx.org/content/col11992/1.13
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