Understanding the Effects of Relative Curvature and Mass on Space and Observers

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Discussion Overview

The discussion revolves around the effects of mass and relative speed on the curvature of space as perceived by different observers. Participants explore the implications of relativistic mass, energy, and the nature of gravitational fields in relation to observer frames, touching on theoretical aspects of general relativity and spacetime curvature.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant suggests that mass curves space and questions whether an observer traveling near the speed of light would perceive increased curvature around a particle moving relative to them.
  • Another participant clarifies that the term "relativistic mass" is outdated and emphasizes that rest mass remains constant, while energy, which sources gravitational fields, changes with speed.
  • This participant also asserts that the gravitational field, represented by the Riemann tensor, varies with the observer's frame of reference, indicating that curvature is frame-dependent.
  • A later reply questions whether there exists a preferred reference frame where curvature is minimized, suggesting a complexity in understanding curvature across different frames.
  • Another participant reinforces that curvature should not be viewed as a single quantity, noting the multiple independent components of the curvature tensor even in a rest frame.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of mass and curvature, with no consensus on whether a preferred reference frame exists or how curvature is perceived across different frames. The discussion remains unresolved regarding the implications of these concepts.

Contextual Notes

There are limitations in the discussion regarding the definitions of mass and energy, as well as the assumptions about the nature of curvature and its dependence on observer frames. The complexity of the Riemann tensor and its components is acknowledged but not fully resolved.

friend
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Mass curves space. And speed near the the speed of light increases mass. So for someone traveling near c and is passing a partice at rest, the traveling observe feels like he's at rest and the other particle is moving. So if the other particle is moving wrt his rest frame, does he see an increased curvature of space surrounding the particle approaching him? Whereas, a particle traveling along side the approaching particle will experience a different curvature?

Does the curvature of mass depend on the speed of observers since the mass of that object does depend on the speed of the observer? Thank you.
 
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friend, We get this question (or some variation of it) at least a few times a week. Just so you know you're not alone in wondering. :smile: As the professor said, "I use the same questions on the exam every year, but to make it more interesting I change the answers." So I'll try to come up with a different answer!

In the first place, the "mass" you're talking about, that increases with the object's speed, is the "relativistic mass", which no one uses any more. When we say mass nowadays we mean rest mass, which does not change. But what does change is the particle's energy, and that's better to talk about anyway, since the source of the gravitational field is in fact energy, not mass. So - energy.
Does the curvature depend on the speed of observers?
Yes, surely it does! Most quantities in physics are like this - they change when we go from one rest frame to another. Charge becomes current, energy becomes momentum, and so on. The individual quantities we talk about are components of an object, a vector or tensor, that transforms in a known way when going from one frame to another. The frequency of a light ray increases if we move toward it. Similarly, the energy of a particle increases, and its gravitational field does too.

The gravitational field is represented by the curvature of spacetime, which is described by a tensor called the Riemann tensor. In vacuum the Riemann curvature tensor has ten independent components, and sure enough they change when we change to a different rest frame.

That does not, however, mean that the properties of the particle change. It does not, for example, become a black hole! But its gravitational field does look different to us, just from the fact that it's moving.
 
Bill_K said:
The gravitational field is represented by the curvature of spacetime, which is described by a tensor called the Riemann tensor. In vacuum the Riemann curvature tensor has ten independent components, and sure enough they change when we change to a different rest frame.

Does that mean there is a preferred reference frame where the curvature of most things in the universe is minimized?
 
The rest frame of the particle.

Again, it is best not to think of "the" curvature as if it were a single quantity. Even in the rest frame, the curvature tensor has five independent components.
 

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