Understanding GR Vacuum Solutions: Explaining the Role of Matter in Curvature

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In summary, the conversation discusses the concept of GR solutions in the absence of matter and the apparent contradiction of using the mass of an object, such as the sun, in the solutions. The speakers mention the concept of vacuum solutions in both GR and EM, where a specific region of vacuum may have a field or curvature due to matter located elsewhere. They also touch on the difference between tidal curvature and curvature caused by mass within a specific volume of space. Overall, the conversation highlights the complexities of understanding and applying GR solutions.
  • #1
TrickyDicky
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I would like to have a conceptually better understanding of GR solutions in the absence of matter, and a little difficulty I usually run into is that seemingly since in these solutions we have both the Einstein and stress-energy tensors equal to zero (which is what it means to have no matter-energy there) we are ignoring the curvature produced by any mass, however, when applying the solution to the Mercury precession problem or the bending of light by the sun problem, we are actually introducing the mass of the sun to solve them, and this to me seems a bit contradictory with the premise that there is no matter in the manifold under consideration.
Is there a simple way to explain away this false contradiction?
My own way to explain this is that actually in the Schwartzschild metric we have the expresion (1-2m/r) which seems to imply that we are substracting(that is close to ignoring) the curvature produced by the spherical symmetric mass from the total spacetime curvature, but I'm not sure if this is really so or even has any logic, it just helps me understand conceptually the premise of this vacuum solution.
 
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  • #2
The Schwarzschild solution has two patches matching at the Schwarzschild radius. The outer solution is the familiar vacuum solution, whereas there is an inner solution which is NOT a vacuum metric and which therefore differs from the well-known inner vacuum solution used for a black hole. Instead a spherical symmetric, non-rotating, incompressible fluid is used which leads to a regular solution w/o singularity at r=0.
 
  • #3
tom.stoer said:
The Schwarzschild solution has two patches matching at the Schwarzschild radius. The outer solution is the familiar vacuum solution, whereas there is an inner solution which is NOT a vacuum metric and which therefore differs from the well-known inner vacuum solution used for a black hole. Instead a spherical symmetric, non-rotating, incompressible fluid is used which leads to a regular solution w/o singularity at r=0.

Thanks but you answer has nothing to do whatsoever with the point of my question, nothing to do with the inner solution or black hole, I am referring to the outer solution only and the apparent incongruence of using the sun's mass in a solution whose premise is the absence of mass.
 
  • #4
Conceptually this is similar to EM, where charge is the source of the field, but vacuum solutions exist. Specifically, in EM the charge is proportional to the divergence of the E-field, but a specific region of vacuum may have a field due to charge located elsewhere. Similarly, in GR the stress energy tensor is proportional to the Ricci curvature and the curvature scalar, but a specific region of vacuum may have a Riemann curvature due to stress-energy located elsewhere.
 
  • #5
TrickyDicky said:
Thanks but you answer has nothing to do whatsoever with the point of my question, nothing to do with the inner solution or black hole, I am referring to the outer solution only and the apparent incongruence of using the sun's mass in a solution whose premise is the absence of mass.
That's not correct; the outer solution IS a vacuum solution (vacuum outside the sun) generated by a mass confined to the sun's volume (it is not a global vacuum with T=0 everywhere).

Look at classical electrodynamics: the Coulomb potential is a vacuum solution of the Maxwell equation valid outside the charge distribution = "in vacuum".
 
  • #6
tom.stoer said:
The Schwarzschild solution has two patches matching at the Schwarzschild radius. The outer solution is the familiar vacuum solution, whereas there is an inner solution which is NOT a vacuum metric and which therefore differs from the well-known inner vacuum solution used for a black hole. Instead a spherical symmetric, non-rotating, incompressible fluid is used which leads to a regular solution w/o singularity at r=0.

Tom, maybe I'm misunderstanding you, but this seems incorrect to me. It's true that in the case of an object that's not a black hole, you would have to have a separate equation for the interior of the object, and this would be a non-vacuum solution without a singularity. However, the surface where this is glued onto the exterior vacuum spacetime is not at the Schwarzschild radius. In the case you're talking about, the Schwarzschild radius is less than the radius of the object, and nothing physically happens at the Schwarzschild radius. I think your answer would be correct if you just changed "Schwarzschild radius" to "radius of the object." Maybe that was what you intended, but you wrote "Schwarzschild radius" by mistake?

DaleSpam said:
Conceptually this is similar to EM, where charge is the source of the field, but vacuum solutions exist. Specifically, in EM the charge is proportional to the divergence of the E-field, but a specific region of vacuum may have a field due to charge located elsewhere. Similarly, in GR the stress energy tensor is proportional to the Ricci curvature and the curvature scalar, but a specific region of vacuum may have a Riemann curvature due to stress-energy located elsewhere.
To put this in less technical language, I think the issue boils down to distinguishing between two types of curvature. There is tidal curvature, which can be caused by mass outside that volume of space, and there's a different type of curvature (measured by the Einstein tensor) that can only be caused by mass that exists inside that volume of space. TrickyDicky, if you have access to either the Feynman lectures or Penrose's The Road to Reality, both of those have good nontechnical discussions of this distinction. My own explanation is here: http://www.lightandmatter.com/html_books/genrel/ch05/ch05.html#Section5.1

-Ben
 
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  • #7
Ben,

bcrowell said:
Tom, maybe I'm misunderstanding you, but this seems incorrect to me. It's true that in the case of an object that's not a black hole, you would have to have a separate equation for the interior of the object, and this would be a non-vacuum solution without a singularity. However, the surface where this is glued onto the exterior vacuum spacetime is not at the Schwarzschild radius. ... Maybe that was what you intended, but you wrote "Schwarzschild radius" by mistake?

Yes, you are absolutely right. Patching of outer = vacuum and inner = non-vacuum solution obviously is done at the physical radius of the object, not at the Schwarzschild radius, which is irrelevant in that case. Sorry for the confusion!
 

1. What is the role of matter in curvature?

The presence of matter, specifically mass and energy, is crucial in determining the curvature of spacetime according to Einstein's theory of general relativity. Matter causes spacetime to curve, which in turn affects the motion of other matter and objects in the vicinity.

2. How does matter affect the vacuum solutions in general relativity?

Matter plays a significant role in determining the vacuum solutions in general relativity. The type and distribution of matter in a given region of spacetime determine the curvature and geometry of that region, which ultimately affects the vacuum solutions.

3. Can the presence of matter cause variations in the vacuum solutions?

Yes, the presence of matter can cause significant variations in the vacuum solutions in general relativity. This is because the curvature of spacetime is directly influenced by the distribution and concentration of matter, leading to different vacuum solutions in different regions.

4. How does matter contribute to the overall understanding of general relativity?

Matter is a fundamental component in the understanding of general relativity. It is one of the main sources of curvature in spacetime, which is the foundation of the theory. By studying the effects of matter on spacetime, we can gain a deeper understanding of the fundamental principles of general relativity.

5. Are there any real-life applications of understanding the role of matter in curvature?

Yes, understanding the role of matter in curvature has practical applications in various fields, including astronomy, cosmology, and space exploration. By studying the effects of matter on spacetime, we can better understand the behavior of objects in the universe and make accurate predictions about their motion and interactions.

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