Why do we fall, according to GR?

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Discussion Overview

The discussion centers on understanding how General Relativity (GR) explains the phenomenon of falling objects, particularly in the context of curved spacetime. Participants explore the implications of geodesics, the role of time and space curvature, and the nature of gravitational effects as described by GR.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants suggest that objects fall by following geodesics that lead back to the Earth, influenced by the curvature of spacetime.
  • One participant emphasizes that the curvature of spacetime, rather than just space, is crucial in understanding gravity.
  • Another viewpoint posits that in GR, objects do not fall due to a force but rather move along their natural paths while the Earth accelerates towards them.
  • A participant proposes a scenario where two people walking north on a curved Earth would eventually collide, illustrating how curvature can create the appearance of a force drawing them together.
  • There is a discussion about how time curvature is more significant for slow-moving massive objects compared to space curvature.
  • One participant raises a question about why an object at rest near a massive body begins to fall, seeking clarity on the mechanics of GR.
  • Another participant suggests that the concept of gravity in GR can be viewed similarly to Newtonian mechanics, where gravity acts as a fictitious force that still results in acceleration.

Areas of Agreement / Disagreement

Participants express a range of views on the nature of falling in GR, with no clear consensus on how to interpret the effects of curvature in spacetime. Some agree on the role of geodesics, while others emphasize different aspects of time and space curvature, leading to ongoing debate.

Contextual Notes

Participants note the complexity of visualizing time curvature and its implications for understanding gravitational effects. There are also references to the challenges of reconciling GR with intuitive notions of force and motion.

  • #31
TrickyDicky said:
This is a nice way to see it and certainly describes why we fall, but actually if one considers B (that is in flat spacetime), it begs the question why curvature is needed at all for GR and gravitation; B would only need a mechanism of acceleration. So once we assume gravitation comes from spacetime curvature, C is not adding anything to the question why we fall.
Spacetime curvature is needed only to explain tidal effects of gravity. You are correct that bulk "falling" has little to do with curvature.
 
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  • #32
@Trickydick I'm sorry. I really don't mean to be pedantic. I should be in bed and the "why curvature is needed at all for GR" kind of threw me off.

DaleSpam said:
Spacetime curvature is needed only to explain tidal effects of gravity. You are correct that bulk "falling" has little to do with curvature.
Damn, just when I think something makes sense...
 
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  • #33
On the other hand it is difficult to represent graphically these things, and unfortunately the time dimension in the graph has to be represented as a spatial dimension and we are actually looking at a 2D space instead of a 2D spacetime, so that in C the curvature of the graph that should represent a spacetime curvature, is in fact a purely spatial one and thus it may lead to some confusion for the not well acquainted.
 
  • #34
I see. I figured it couldn't be that simple. :P
 
  • #35
TrickyDicky said:
On the other hand it is difficult to represent graphically these things, and unfortunately the time dimension in the graph has to be represented as a spatial dimension and we are actually looking at a 2D space instead of a 2D spacetime, so that in C the curvature of the graph that should represent a spacetime curvature, is in fact a purely spatial one and thus it may lead to some confusion for the not well acquainted.
I dunno, I think people are pretty familiar with seeing time plotted on a graph. It's not showing time as a spatial dimension; it's simply representing time as an axis on the graph.
 
  • #36
DaveC426913 said:
It's not showing time as a spatial dimension; it's simply representing time as an axis on the graph.

I'm making a (maybe too subtle) distinction between what it represents and what the literal picture shows in the context of the nuances of space vs. spacetime.
We all agree that this axis represents the time coordinate, but the graph cannot easily show the difference between a time coordinate and a space coordinate and so it depicts them in the same way, and we see a 2D SPATIAL surface that represents a 2D Lorentzian Spacetime that is basically a 1D space in time.

This might verge on the pedantic, but it could be a source of confusion for some (precisely those that are very familiar with seeing time plotted in graphs but not so much with Lorentzian manifolds and relativity) , and that is why I mention it.
 
  • #37
DaveC426913 said:
Why would the Earth accelerate upwards?
What you're asking here is pretty much the same as "Why is GR a good theory?". You're focusing on a specific aspect of it, but I think the only good way to answer your question is to explain why the predictions of GR are accurate, and the only thing that can do that is a better theory of gravity.

kweba said:
Is it true spacetime push as back to Earth?
No, Earth is pushing you away from the part of space you'd have to be into do geodesic (i.e. non-accelerating) motion.
 
  • #38
andrewkirk said:
kweba I think it would help if you familiarised yourself with the concept of a 'four-velocity'. When you understand that concept you will see that there is no such thing as being 'at rest'. Every object has a nonzero four-velocity. Hence it has a unique geodesic that it follows - if it is free from non-gravitational forces. That geodesic is defined by its position and the direction in spacetime of its four-velocity.

ETA: looks like somebody has just explained this above, with diagrams too. Nice!

Yes, thank you. I admit I am not familiar with the concept (I never heard of it.) I guess this is what I'm missing all along. Thanks, I will read/study about it.

But I never realized, until now, that we are in a constant motion (velocity) through spacetime, that even though we may be at rest in space, we are still in motion through time.

It said that our four-velocity, with everything in the universe, is at the constant speed of light, but it just goes to the time direction. Is this true?

Yes I tried studying the graphs, but pardon me as I'm having a hard time getting it.
 
  • #39
kweba said:
Yes, thank you. I admit I am not familiar with the concept (I never heard of it.) I guess this is what I'm missing all along. Thanks, I will read/study about it.

But I never realized, until now, that we are in a constant motion (velocity) through spacetime, that even though we may be at rest in space, we are still in motion through time.

It said that our four-velocity, with everything in the universe, is at the constant speed of light, but it just goes to the time direction. Is this true?
It's useful to understand four-velocity, but I don't think it will help you answer the question in the thread title. What you need to understand is that SR and GR both involve a mathematical thing called "spacetime", and that motion of particles is represented by curves in spacetime, called "world lines". There's a class of curves that really distinguish themselves from all the rest, in a way that doesn't depend on a choice of coordinate system. These curves are called geodesics.

Since they are the only world lines that are "special" in a coordinate-independent way, it's natural to define the proper acceleration of a world line in a way that ensures that the proper acceleration of a world line, at an event E on it, is a measure of much the curve "curves away" from a geodesic through E that's tangent to the world line. The force acting on the object can then be defined by F=ma. To find the geodesics near a spherical distribution of mass (like a planet), we must solve Einstein's equation for that distribution. When we do, we find that the curve representing the motion of an object on the surface isn't a geodesic, so the a (acceleration) of the object is non-zero. Since F=ma by definition, this means that there's a force acting on it. Since the surface of the Earth is preventing the object from doing geodesic motion, we say that the surface of the Earth is pushing it with force ma.

(What I wrote as F=ma is actually a four-vector equation. I'm trying to keep things simple, so I won't say anything more about that).

The four-velocity of a world line is defined as the normalized tangent vector of the world line. This makes the statement that everything moves through spacetime at speed c trivial and not interesting in my opinion.
 
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