Is force/mass ratio an invariant quantity in GR?

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Discussion Overview

The discussion centers on the invariance of force and mass within the framework of General Relativity (GR), specifically examining whether the ratio of force to mass, known as proper acceleration, is invariant. Participants explore the implications of these concepts in both theoretical and practical contexts.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants assert that proper acceleration is defined as applied force divided by mass, noting that gravity is not considered a force in GR.
  • It is proposed that 4-force is a 4-vector and mass is a Lorentz scalar, leading to the conclusion that the ratio of 4-force to mass is also a 4-vector.
  • Participants discuss that the magnitude of the proper acceleration 4-vector is invariant, being equal to the magnitude of the 4-force vector divided by mass.
  • Some express a preference for discussing proper acceleration due to its intuitive geometric meaning related to the curvature of an object's worldline.
  • There is a suggestion that proper acceleration is frequently referenced because it is useful in calculating an object's worldline through spacetime.
  • One participant questions whether the description of path curvature could be rephrased in terms of deviation from a geodesic, to which another participant agrees.
  • Concerns are raised about the intuitive nature of these concepts, particularly for those less comfortable with mathematical formulations.

Areas of Agreement / Disagreement

Participants express varying opinions on the intuitiveness and utility of proper acceleration, with some favoring its geometric interpretation while others acknowledge the complexity of the underlying mathematics. The discussion does not reach a consensus on the invariance of force and mass or the implications of their ratio.

Contextual Notes

Participants note that the discussion involves complex concepts from GR, including the transformation properties of 4-vectors and scalars, and the relationship between proper acceleration and the geometry of spacetime. There are unresolved aspects regarding the broader implications of these definitions and their applications.

JohnNemo
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[Mentors' note - this thread was split off from https://www.physicsforums.com/threads/invariance-of-force-and-mass.939025/]
PeterDonis said:
@JohnNemo Proper acceleration is not the rate of change of velocity. It is best thought of as applied force (and as you say, gravity is not a force in GR so it doesn't count here) divided by the object's mass. So when you move your phone around and the accelerometer number changes, it's not telling you how the phone's speed changes; it's telling you how much force you are applying to move the phone (and of course this is in addition to the force of the Earth pushing you up and transmitted through you to the phone).

Are force and mass both invariant, or is it just the force divided by mass value which is invariant?
 
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JohnNemo said:
Are force and mass both invariant, or is it just the force divided by mass value which is invariant?

4-force is a 4-vector. Mass is a Lorentz scalar (i.e., a number which is invariant). So 4-force divided by mass is also a 4-vector. The magnitude of a 4-vector is an invariant, but its individual components are not: they are covariant--they transform according to the appropriate coordinate transformation.

When I said proper acceleration was an invariant, strictly speaking what I should have said was that the magnitude of the proper acceleration 4-vector is an invariant, and is equal to the magnitude of the 4-force vector divided by the mass. (And the mass itself is the magnitude of the 4-momentum vector, which is why it is an invariant.)
 
PeterDonis said:
4-force is a 4-vector. Mass is a Lorentz scalar (i.e., a number which is invariant). So 4-force divided by mass is also a 4-vector. The magnitude of a 4-vector is an invariant, but its individual components are not: they are covariant--they transform according to the appropriate coordinate transformation.

When I said proper acceleration was an invariant, strictly speaking what I should have said was that the magnitude of the proper acceleration 4-vector is an invariant, and is equal to the magnitude of the 4-force vector divided by the mass. (And the mass itself is the magnitude of the 4-momentum vector, which is why it is an invariant.)

If proper acceleration and mass are both invariant, if there a particular reason why the quotient value, proper acceleration, is mentioned a lot? Does it crop up in a lot of formulas?
 
JohnNemo said:
if there a particular reason why the quotient value, proper acceleration, is mentioned a lot?

I couldn't say in general. I prefer it because it seems more intuitive to me, since it's the path curvature of the object's worldline, so it has an immediate geometric meaning. But not everyone prefers the geometric viewpoint.
 
JohnNemo said:
If proper acceleration and mass are both invariant, if there a particular reason why the quotient value, proper acceleration, is mentioned a lot? Does it crop up in a lot of formulas?
Yes; it's a very useful quantity when you are calculating an object's worldline through spacetime. It has an intuitive geometric meaning that is not apparent from either the rest mass or the four-force when considered in isolation.

You will also have noticed that the ordinary boring classical Newtonian acceleration is mentioned a lot in classical physics, even though it is also just the quotient value of two other invariant (under the Galilean transforms of Newtonian mechanics) quantities. The reason is similar; an intuitive meaning not apparent in the two quantities from which it is derived.
 
PeterDonis said:
I couldn't say in general. I prefer it because it seems more intuitive to me, since it's the path curvature of the object's worldline, so it has an immediate geometric meaning. But not everyone prefers the geometric viewpoint.

When you say 'the path curvature of the object's worldline' would another way to express that be 'the extent of a object's worldline's deviation from a geodesic'?
 
JohnNemo said:
When you say 'the path curvature of the object's worldline' would another way to express that be 'the extent of a object's worldline's deviation from a geodesic'?

Yes.
 
Nugatory said:
Yes; it's a very useful quantity when you are calculating an object's worldline through spacetime. It has an intuitive geometric meaning that is not apparent from either the rest mass or the four-force when considered in isolation.

You will also have noticed that the ordinary boring classical Newtonian acceleration is mentioned a lot in classical physics, even though it is also just the quotient value of two other invariant (under the Galilean transforms of Newtonian mechanics) quantities. The reason is similar; an intuitive meaning not apparent in the two quantities from which it is derived.
I'm all for things which are intuitive. Maths is not my strong suit!
 

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