The Chandrasekhar Limit: The Threshold That Makes Life Possible (2024)

There is a thin line between a bang and a whimper.

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For stars, this line is called the Chandrasekhar Limit, and it is the difference between dying in a blaze of glory and going out in a slow fade to black. For our universe, this line means much more: Only by exceeding it can stars sow the seeds of life throughout the cosmos.

The Chandrasekhar Limit is named for Subrahmanyan Chandrasekhar, one of the great child prodigies. Chandrasekhar graduated with a degree in physics before reaching his twentieth birthday. He was awarded a Government of India scholarship to study at Cambridge, and in the fall of 1930 boarded a ship to travel to England. While aboard the ship—still before reaching his twentieth birthday—he did the bulk of the work for which he would later be awarded a Nobel Prize.

By the 1920s—a decade before Chandrasekhar began his journey to England—astronomers had realized that Sirius B, the white dwarf companion to the bright star Sirius, had an astoundingly high density—more than a million times the density of the sun. An object of this density could only exist if the atoms comprising the star were so tightly compressed that they were no longer individual atoms. Gravitational pressure would compress atoms so much that the star would consist of positively-charged ions surrounded by a sea of electrons.

Prior to the discovery of quantum mechanics, physicists knew of no force capable of supporting any star against such gravitational pressure. Quantum mechanics, though, suggested a new way for a star to hold itself up against the force of gravity. According to the rules of quantum mechanics, no two electrons can be in the exact same state. Inside an extremely dense star like Sirius B, this means that some electrons are forced out of low energy states into higher ones, generating a pressure called electron degeneracy pressure that resists the gravitational force. This makes it possible for a star like Sirius B to achieve such extreme density without collapsing in on itself.

This discovery was made by Ralph Fowler, who would later become Chandrasekhar’s graduate supervisor. But Chandrasekhar realized what Fowler had missed: The high-energy electrons inside the white dwarf would have to be traveling at velocities near the speed of light, invoking a set of bizarre relativistic effects. When Chandrasekhar took these relativistic effects into account, something spectacular happened. He found a firm upper limit for the mass of any body which could be supported by electron degeneracy pressure. Once this limit—the Chandraskehar limit—was exceeded, the object could no longer resist the force of gravity, and it would begin to collapse.

When Chandrasekhar published these results in 1931, he set off a battle with one of the greatest astrophysicists of the era, Sir Arthur Eddington, who believed that the white dwarf state was the eventual fate of every star. At a conference in 1935, Eddington told his audience that Chandrasehkar’s work “was almost a reduction ad absurdum of the relativistic degeneracy formula. Various accidents may intervene to save a star, but I want more protection than that. I think there should be a law of Nature to prevent a star from behaving in this absurd way!”

Chandrasekhar was deeply hurt by Eddington’s reaction, but colleagues can disagree profoundly and still remain friends. Chandrasekhar and Eddington remained friends, went to the Wimbledon tennis tournament together and went for bicycle rides in the English countryside. When Eddington passed away in 1944, Chandrasekhar spoke at his funeral, saying “I believe that anyone who has known Eddington will agree that he was a man of the highest integrity and character. I do not believe, for example, that he ever thought harshly of anyone. That was why it was so easy to disagree with him on scientific matters. You can always be certain he would never misjudge you or think ill of you on that account.”

Vindication would eventually come to Chandrasekhar when he was awarded the Nobel Prize in 1983 for his work. The Chandrasekhar Limit is now accepted to be approximately 1.4 times the mass of the sun; any white dwarf with less than this mass will stay a white dwarf forever, while a star that exceeds this mass is destined to end its life in that most violent of explosions: a supernova. In so doing, the star itself dies but furthers the growth process of the universe—it both generates and distributes the elements on which life depends.

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The life of a star is characterized by thermonuclear fusion; hydrogen fuses to helium, helium to carbon, and so on, creating heavier and heavier elements. However, thermonuclear fusion cannot create elements heavier than iron. Only a supernova explosion can create copper, silver, gold, and the “trace elements” that are important for the processes of life.

Lighter elements like carbon, oxygen, and nitrogen are also essential to life, but without supernova explosions, they would remain forever locked up in stars. Being heavier than the hydrogen and helium that comprise most of the initial mass of the stars, they sink to form the central core of the star—just as most of the iron on Earth is locked up in its core. If stars are, as Eddington believed, destined to become white dwarfs, those elements would remain confined to the stellar interior, or at best be delivered in relatively minute quantities to the universe as a whole via stellar winds. Life as we know it requires rocky planets to form, and there simply is no way to get enough rocky material out into the universe unless stars can deliver that material in wholesale quantities. And supernovae do just that.

The Chandrasekhar Limit is therefore not just as upper limit to the maximum mass of an ideal white dwarf, but also a threshold. A star surpassing this threshold no longer hoards its precious cargo of heavy elements. Instead, it delivers them to the universe at large in a supernova that marks its own death but makes it possible for living beings to exist.

Go Deeper
Editor’s picks for further reading

BBC: Test Tubes and Tantrums: Arthur Stanley Eddington and Subrahmanyan Chandrasekhar
In this radio program, discover the history of one of the nastiest disagreements in astrophysics.

FQXi: Exploding the Supernova Paradigm
In this blog post, Zeeya Merali investigates gaps in our understanding of supernova explosions.

Nobelprize.org: Subramanyan Chandrasekhar – Autobiobraphy

The Chandrasekhar Limit: The Threshold That Makes Life Possible (2024)

FAQs

The Chandrasekhar Limit: The Threshold That Makes Life Possible? ›

The Chandrasekhar Limit is now accepted to be approximately 1.4 times the mass of the sun

mass of the sun
standard unit of mass in astronomy which is equal to 1.98892 × 10³⁰ kg. Solar mass is a unit of measurement of mass. It is equal to the mass of the Sun, about 332,950 times the mass of the Earth, or 1,048 times the mass of Jupiter. Masses of other stars and groups of stars are listed in terms of solar masses.
https://simple.wikipedia.org › wiki › Solar_mass
; any white dwarf with less than this mass will stay a white dwarf forever, while a star that exceeds this mass is destined to end its life in that most violent of explosions: a supernova.

What is the equation for the Chandrasekhar limit? ›

For a fully relativistic treatment, the equation of state used interpolates between the equations P = K1ρ5/3 for small ρ and P = K2ρ4/3 for large ρ. When this is done, the model radius still decreases with mass, but becomes zero at Mlimit. This is the Chandrasekhar limit.

What was the theory of Chandrasekhar? ›

Using Albert Einstein's special theory of relativity and the principles of quantum physics, Chandrasekhar showed that it is impossible for a white dwarf star, which is supported solely by a degenerate gas of electrons, to be stable if its mass is greater than 1.44 times the mass of the Sun.

What happens if the Chandrasekhar limit is exceeded? ›

If a white dwarf exceeds the Chandrasekhar limit, they, under gravitational collapse, evolve as a stellar remnant similar to a neutron star or a black hole.

What happens if the iron core of a star exceeds the Chandrasekhar limit? ›

Once the Chandrasekhar Limit is reached, the electron degeneracy pressure of the atoms within the core is no longer able to stop the further collapse of the star; radiation pressure is no longer able to support the core against gravity and the iron core collapses.

What is the Chandrasekhar limit states that the mass of a white dwarf Cannot exceed ________ solar masses? ›

Chandrasekhar found that the limiting mass of a white dwarf is about 1.4 solar masses: beyond that electron degeneracy simply cannot resist gravity (and the object has shrunk too far).

What is the mass threshold for a black hole? ›

In general, stars with final masses in the range 2 to 3 solar masses are believed to ultimately collapse to a black hole.

How powerful is a black hole? ›

A black hole is so dense that gravity just beneath its surface, the event horizon, is strong enough that nothing – not even light – can escape. The event horizon isn't a surface like Earth's or even the Sun's.

Why is Chandrasekhar important? ›

Beginning in the 1930s, Subramanyan Chandrasekhar formulated theories for the development that stars subsequently undergo. He showed that when the hydrogen fuel of stars of a certain size begins to run out, it collapses into a compact, brilliant star known as a white dwarf.

What is the limit of a black hole? ›

Supermassive black holes in any quasar or active galactic nucleus (AGN) appear to have a theoretical upper limit of physically around 50 billion M for typical parameters, as anything above this slows growth down to a crawl (the slowdown tends to start around 10 billion M ) and causes the unstable accretion disk ...

How does a black hole form? ›

How Do Black Holes Form? Primordial black holes are thought to have formed in the early universe, soon after the big bang. Stellar black holes form when the center of a very massive star collapses in upon itself. This collapse also causes a supernova, or an exploding star, that blasts part of the star into space.

How big is a white dwarf? ›

A low or medium mass star (with mass less than about 8 times the mass of our Sun) will become a white dwarf. A typical white dwarf is about as massive as the Sun, yet only slightly bigger than the Earth. This makes white dwarfs one of the densest forms of matter, surpassed only by neutron stars and black holes.

What would happen to the Earth if the sun were suddenly changed to a black hole without changing its mass? ›

Contrary to popular belief, the Solar System would not be sucked in: a solar-mass black hole would exert no more gravitational pull than our Sun. As this computer simulation shows, the planets would actually continue on in their orbits as if nothing had happened.

What element kills stars? ›

Explanation: Large stars over 8 solar masses fuse progressively heavier elements over their life. When the fusion process produces nickel and iron the star will come to the end of its life in a matter of days.

How close would a core collapse supernova have to be to destroy half the Earth's ozone layer? ›

It is estimated that a Type II supernova closer than eight parsecs (26 light-years) would destroy more than half of the Earth's ozone layer.

Why can't massive stars burn iron? ›

Iron is the End-Point of Nuclear Reactions

Under normal circ*mstances iron doesn't fuse in a star. The strong nuclear force which binds nuclei together is a short range force, so there is a limit to how large a nucleus can be. Iron is the most stable element.

What is the Chandrasekhar limit in Quizlet? ›

The maximum mass that a star can have and still become a white dwarf is 1.4 times the mass of the Sun. This limiting mass is known as has the Chandrasekhar limit.

What is the Chandrasekhar and Oppenheimer Volkoff limit? ›

The maximum mass a neutron star can have before it undergoes gravitational collapse to a black hole. It is more difficult to estimate this limit than the analogous Chandrasekhar limit for white dwarf stars. It is thought that the Oppenheimer–Volkoff limit is between two and three times the mass of the sun.

How does a 1.2 solar mass white dwarf compare to a 1.0 solar mass white dwarf? ›

1. Radius: The radius of a white dwarf is inversely proportional to its mass. This means that a higher mass white dwarf will have a smaller radius, and a lower mass white dwarf will have a larger radius. Therefore, the 1.2 solar mass white dwarf will have a smaller radius than the 1.0 solar mass white dwarf.

What is the contribution of S Chandrasekhar to physics? ›

Chandrasekhar's most notable work is on the astrophysical Chandrasekhar limit. The limit gives the maximum mass of a white dwarf star, ~1.44 solar masses, or equivalently, the minimum mass that must be exceeded for a star to collapse into a neutron star or black hole (following a supernova).

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