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Oppenheimer–Snyder model

Exact solution to the Einstein field equations

  • 7 min read
  • 4 chapters

Related on Lably

Through Black hole, Albert Einstein and Event horizon

During the collapse of a star to a black hole the geometry on the outside of the sphere is the Schwarzschild geometry. However the geometry inside is the same Robertson-Walker geometry as in the rest of the observable universe.

History

Albert Einstein, who had developed his theory of general relativity in 1915, initially denied the possibility of black holes, even though they were a genuine implication of the Schwarzschild metric, obtained by Karl Schwarzschild in 1916, the first known non-trivial exact solution to Einstein's field equations. In 1939, Einstein published "On a Stationary System with Spherical Symmetry Consisting of Many Gravitating Masses" in the Annals of Mathematics, claiming to provide "a clear understanding as to why these 'Schwarzschild singularities' do not exist in physical reality."

Months after the issuing of Einstein's article, J. Robert Oppenheimer and his student Hartland Snyder studied this topic with their paper "On Continued Gravitational Contraction" making the opposite argument as Einstein's. They showed when a sufficiently massive star runs out of thermonuclear fuel, it will undergo continued gravitational contraction and become separated from the rest of the universe by a boundary called the event horizon, which not even light can escape. This paper predicted the existence of what are today known as black holes. The term "black hole" was coined decades later, in the fall of 1967, by John Archibald Wheeler at a conference held by the Goddard Institute for Space Studies in New York City; it appeared for the first time in print the following year. In this paper, Oppenheimer and Snyder used Einstein's own theory of gravity to prove how black holes could develop for the first time in contemporary physics, but without referencing the aforementioned article by Einstein. Oppenheimer and Snyder did, however, refer to an earlier article by Oppenheimer and Robert Serber on neutron stars, improving upon the work of Lev Davidovich Landau, in what was essentially an exercise in nuclear physics and gravitation.

This investigation attracted the attention of Richard Chace Tolman, who had previously obtained an exact solution to the Einstein field equations describing a static ideal fluid sphere. Oppenheimer and George Volkoff subsequently published paper on the stability of neutron stars, the Tolman-Oppenheimer-Volkoff limit. These papers established the foundation for the general-relativistic theory of stellar structure. Actually, the objects Tolman, Oppenheimer, and Volkoff studied were the neutron stars of Fritz Zwicky rather than the "neutron cores" of Lev Landau. But while Zwicky did introduce the notion of neutron stars, much of his work on this topic was later rejected as wrong. By contrast, the paper by Oppenheimer and Volkoff has been accepted as correct. This led Oppenheimer to consider the natural next problem of determining what would happen if a neutron star were so heavy it would collapse due to its own weight.

However, Oppenheimer would not revisit the topic in future publications.

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