Schwartzchild Radius Adjustment: Susskind's Online Lecture Series

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In summary, the Schwarzschild solution is the unique spherically symmetric solution to Einstein's equations in vacuum, but it is stationary (static) if it is used outside of a spherically symmetric star.
  • #1
pnmeadowcroft
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What if Schwatzchild has made the same mistake as Newton?

( 1 - 2MG / c2 r ) dt

can be view as a binomial expansion to first order of

1 / ( 1 + 4MG / C2 r )1/2 dt

then would the event horizon be at the singularity?

I've been reviewing Susskind's online lecture series, and would like to explore the derivation of the Schwatzchild in more detail. Links to any relevant papers appreciated.
 
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  • #2
Historically, Schwarzschild did indeed make a mistake about the event horizon, and was not able to distinguish the coordinate singularity seen in some coordinate systems as the event horizon is approached, from the true singularity. A good way to see that the event horizon is real is to use a coordinate system which smoothly covers the event horizon. One example are Kruskal–Szekeres coordinates

http://preposterousuniverse.com/grnotes/grnotes-seven.pdf
http://www.blau.itp.unibe.ch/newlecturesGR.pdf (Section 26.6)
 
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  • #3
The Schwarzschild spacetime is an exact solution to the Einstein field equations of general relativity. It's also (provably) the only solution to these equations for a spherically symmetric stationary mass distribution. Thus, the only way that it could need additional correction terms would be if the field equations themselves were wrong - which is certainly possible - but so far no one has found any theory that works better than general relativity.
 
  • #4
Thanks

Both posts are a great help.

The spherically symmetric stationary mass distribution assumption seems quite reasonable, I'm happy with the explanations of that. In atty referrence 1, Sean Carrol sites the proof that the Schwartzchild solution is the only solution, as Birkhoff's Theorem. I'll study that in more detail as well as the constraints imposed by the field equations themselves.
 
  • #5
It's in Carroll's notes that "the Schwarzschild solution is the unique spherically symmetric solution to Einstein’s equations in vacuum", but I just wanted to highlight that the uniqueness for the Schwarzschild solution is under the assumption of a vacuum solution, so there is no matter in the Schwarzschild solution. Also, the uniqueness does not depend on the solution being stationary.

Because the Schwarzschild solution represents vacuum, it can be used outside a spherically symmetric star, being joined to something else that describes matter in the star. The solution with the event horizon is a fully vacuum solution, and if people want to be clear they say something like the "maximally extended vacuum Schwarzschild solution".
 
  • #6
atyy said:
the uniqueness does not depend on the solution being stationary.

More precisely, the fact that the solution is stationary (in fact, static) is a *result* of the solution, not an assumption that needs to be made at the start in order to find the solution. (Even more precisely, the solution has a 4th Killing vector field in addition to the three associated with spherical symmetry; but the solution does not require that that KVF is timelike everywhere, so the term "stationary", strictly speaking, does not necessarily apply everywhere.)
 

1. What is the Schwartzchild radius and why is it important in physics?

The Schwartzchild radius is a measure of the size of the event horizon of a black hole. It is derived from the theory of general relativity and is important because it determines the point at which the gravitational pull of a black hole becomes strong enough to prevent even light from escaping.

2. How does the Schwartzchild radius affect the behavior of light around a black hole?

The Schwartzchild radius is directly related to the curvature of space-time around a black hole. As light approaches the Schwartzchild radius, it is bent more and more by the strong gravitational pull. At the Schwartzchild radius, light is bent so much that it is unable to escape, creating the event horizon of the black hole.

3. Can the Schwartzchild radius of a black hole be changed or adjusted?

No, the Schwartzchild radius is a fundamental property of a black hole and cannot be changed or adjusted. It is determined by the mass of the black hole, with larger masses resulting in larger Schwartzchild radii.

4. How does the concept of Schwartzchild radius relate to the theories of Stephen Hawking and Leonard Susskind?

Both Hawking and Susskind have made significant contributions to our understanding of black holes and the concept of Schwartzchild radius. Hawking's work on black hole thermodynamics and the emission of Hawking radiation has helped to explain the behavior of black holes near their Schwartzchild radius. Susskind's contributions include the idea that the information of an object that falls into a black hole is not lost, but rather stored on the event horizon.

5. What are some real-world applications of understanding the Schwartzchild radius?

Understanding the Schwartzchild radius is crucial in astrophysics and the study of black holes. It allows scientists to make predictions about the behavior of light and matter around black holes, as well as the potential effects of black holes on their surrounding environments. It also has implications for our understanding of gravity and the nature of space-time.

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