Inertial Reference Frames- circular?

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Discussion Overview

The discussion revolves around the concept of inertial reference frames in physics, particularly questioning the circularity of their definition and the relativity of acceleration. Participants explore the implications of defining inertial frames, the relationship between forces and acceleration, and the nature of acceleration itself, touching on theoretical and philosophical aspects of physics.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested
  • Philosophy of science

Main Points Raised

  • One participant questions the circularity in the definition of inertial reference frames, suggesting that knowing whether an object has no forces acting on it requires an inertial frame.
  • Another participant introduces the equivalence principle from general relativity, arguing that free-falling reference frames can be considered inertial without empirical verification.
  • Some participants express that understanding acceleration does not necessitate prior knowledge of inertial frames, while others challenge this view, suggesting a conceptual dependency between forces, acceleration, and inertial frames.
  • There is a debate over whether acceleration is a relative concept, with some asserting that it is, while others argue that it is not, citing examples from Newtonian mechanics and relativity.
  • Participants discuss the implications of different observers agreeing on acceleration's direction but potentially disagreeing on its magnitude or whether it represents an increase or decrease in speed.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the definition of inertial reference frames and the relativity of acceleration. The discussion remains unresolved, with no consensus reached on these topics.

Contextual Notes

Participants highlight limitations in understanding the definitions and relationships between concepts like force, acceleration, and inertial frames, indicating that assumptions may not be universally accepted.

  • #31
Hurkyl said:
(I'm going to lapse into the differential geometry terminology I know)

Coordinate charts aren't required to represent the correct curvature.

A frame (at a point) is nothing more than a choice of basis for the tangent space at that point. (which, I suppose, can be intuitively thought of as an "infinitessimal" coordinate chart)

Only the orthonormal frames are inertial.
I fail to see how this is in any way a response to:

MeJennifer said:
There is no such thing as a non inertial frame in GR (except for a very small region).
Do you or do you not agree that there is no such thing as a non inertial frame in GR (except for a very small region that may be considered flat)?

Hurkyl said:
Depending on exactly what you mean by the word "relative", either all three of "position, velocity, acceleration" are relative, or none of the three are. Since you have said earlier that position and velocity are relative, then in order to be internally consistent, you must also have acceleration as a relative quantity.
It seems we can agree to disagree. :smile:
Whille position and velocity are relative acceleration is absolute in GR.

Feel free to explain how the principle of equivalence would hold if acceleration were not absolute. It would follow that a gravitational field would not be absolute as well.
 
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  • #32
MeJennifer said:
Do you or do you not agree that there is no such thing as a non inertial frame in GR (except for a very small region that may be considered flat)?
No. If by "frame" you mean "coordinate system", then by the definition of manifold, you have to have frames that are defined on "large" regions, and they will be non-inertial.

If by "frame" you mean "a choice of basis vector for the tangent space", then again you can construct a frame over a large region -- you can often do it over the entire manifold. These will almost always be non-inertial (though some inertial ones exist)

If by "frame" you mean something else, then you have to say what it is.


Feel free to explain how the principle of equivalence would hold if acceleration were not absolute.
I can't even figure out why you think there's a problem.
 
  • #33
MeJennifer said:
Do you or do you not agree that there is no such thing as a non inertial frame in GR (except for a very small region that may be considered flat)?
Do you think that Schwarzschild coordinates, which are defined on a large region, qualify as "inertial"? By what criteria? Certainly the path of an object which is at rest in these coordinates (in the sense that its position coordinates are not changing with time) is not following a geodesic.
 
  • #34
JesseM said:
Do you think that Schwarzschild coordinates, which are defined on a large region, qualify as "inertial"? By what criteria? Certainly the path of an object which is at rest in these coordinates (in the sense that its position coordinates are not changing with time) is not following a geodesic.
The selection of coordinates have absolutely nothing to do with something being inertial or not.

Something that is resisting the gravitational pull is obviously not traveling on a geodesic. For instance when you stand on the Earth you are not traveling a geodesic, you are actually accelerating away from the enter of gravity.

Do you realize that the Schwarzschild solution is a model from the perspective of a distant observer who is away from the gravitational pull?
 
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  • #35
MeJennifer said:
The selection of coordinates have absolutely nothing to do with something being inertial or not.
Sure, but I thought we were talking about non-inertial vs. inertial frames, not the question of whether a path is inertial (ie a geodesic) or not. Are you using "frame" to mean something different than "coordinate system"?
MeJennifer said:
Something that is resisting the gravitational pull is obviously not traveling on a geodesic. For instance when you stand on the Earth you are not traveling a geodesic, you are actually accelerating away from the enter of gravity.
Of course I know this, wasn't it obvious that this was exactly my point? Things which are at rest in Schwarzschild coordinates are not moving on a geodesic, therefore Schwarzschild coordinates cannot be considered an "inertial coordinate system". This is exactly the same standard you use to judge whether a coordinate system is inertial or non-inertial in SR--an object moving on a geodesic path will be moving in a straight line in coordinate terms (constant dx/dt, dy/dt and dz/dt) in an inertial coordinate system, and that path will still be a geodesic in a non-inertial coordinate system, but the system is called "non-inertial" precisely because the path would no longer appear straight in terms of the coordinates (dx/dt, dy/dt and dz/dt wouldn't be constant), and because objects which are at rest in this coordinate system (constant x, y, and z coordinate) are moving on non-geodesic paths.

If this is not the standard that you use to judge whether a coordinate system in SR is inertial or non-inertial, than what is?
 
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