Are Geometric Points Affected By Forces?

In summary, the conversation revolved around the distinction between Tier 1 and Tier 2 arguments of relativity. Tier 2 argued that acceleration is observer dependent, while Tier 1 promoted the idea of using an inertial coordinate system to determine acceleration. However, neither of these accurately reflect the role of acceleration in relativity. Proper acceleration is an invariant and can be measured with an accelerometer, while coordinate acceleration is a coordinate-dependent quantity without physical meaning. The conversation also touched on the use of non-inertial coordinate systems in solving problems, but the existence of inertial frames is not a topic of dispute in relativity theory. Without a valid reference, the discussion could not continue.
  • #1
JDoolin
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Could there be two different "camps" of relativity? Could we call these "A priorists" who say costationary geometric points are definable independent of the motion of matter, and "Observists", who say costationary geometric points can only exist if matter is embedded witin those points?
Yesterday I found a playlist of videos by a youtuber "Dialect" who made a distinction between what he called Tier 1 and Tier 2 arguments of Relativity.

Tier 2 promoted a view that acceleration was an observer dependent phenomena. In particular he was discussing the Twin Paradox, and he said that in situations where observer A accelerates toward observer B, that one had an equal right to say that observer B is accelerating toward observer A.

Tier 1 promotes a view that acceleration is determined from an a priori inertial coordinate system. He said that Tier 1 advocates must accept "An inertial frame is not being acted on by any known force-producing sources". However, I do not find that this is a fair characterization. I would say An inertial frame (being constructed only of massless conceptual points) cannot be acted on by any known or unknown force-producing sources.

It seems to me, Newton's Second Law and the Impulse Momentum Theorem are designed to work in a non-accelerated reference frame. The acceleration of Newton's Second Law is intended to only include accelerations against an inertial frame (or at least approximately inertial on the time scales involved in the problem), and the net force is intended to include only real forces... Not fictitious forces such as the force that pushes you back in an accelerating bus, or the force that pushes you outward on a turning merry-go-round.

I have not studied General Relativity in sufficient detail to know how to solve, for instance, the Mercury Orbit problem. It seems to me that one could find a simplification to that problem by invoking a spinning coordinate system, much as one might invokes a spinning coordinate system to calculate the Roche Limit, or to explain the Dzhanibekov effect.

But in regards to the Dzhanibekov effect and Roche limit, one never actually makes the claim that the original inertial coordinate system does not exist. Rather, they invoke a rotating reference frame that coexists.

But in the pedagogy of General Relativity, is it generally taught that new noninertial coordinate systems are being introduced because this makes various problems easier to solve, or is it generally taught that the reason for not using inertial coordinate systems (Minkowski/Cartesian) is because such coordinate systems do not exist because they are unobservable?

Or are there simply two philosophical "camps" in Relativity theory... One camp believing that inertial frames do exist as definable entities, even though we cannot physically construct them, and another camp believing that inertial frames are undefinable, because we cannot construct them from masses and clocks?
 
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  • #2
JDoolin said:
Yesterday I found a playlist of videos by a youtuber
This is not a valid reference. If you want to claim that there is any such distinction made by physicists, you are going to need to find valid references (textbooks or peer-reviewed papers) that say so.
 
  • #3
JDoolin said:
Tier 2 promoted a view that acceleration was an observer dependent phenomena. In particular he was discussing the Twin Paradox, and he said that in situations where observer A accelerates toward observer B, that one had an equal right to say that observer B is accelerating toward observer A.

Tier 1 promotes a view that acceleration is determined from an a priori inertial coordinate system.
Neither of these are a correct description of the role acceleration plays in relativity. In relativity, proper acceleration is an invariant; it is a direct observable (you can measure it with an accelerometer). There is also coordinate acceleration, but that, as its name implies, is a coordinate-dependent quantity that does not have any physical meaning.
 
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  • #4
Thread closed due to lack of a valid reference as a basis for further discussion.
 

1. How do forces affect geometric points?

Forces can affect geometric points by changing their position, orientation, and shape. This can be seen in the bending or stretching of objects, as well as the rotation or translation of points in a coordinate system.

2. Can forces change the shape of a geometric point?

Yes, forces can change the shape of a geometric point. This is known as deformation and is a common occurrence in materials science and engineering. Forces can cause a point to stretch, compress, or bend depending on the type and magnitude of the force.

3. Are geometric points affected by both external and internal forces?

Yes, geometric points can be affected by both external and internal forces. External forces, such as gravity or applied forces, act on the entire object and can affect the position and shape of points within the object. Internal forces, such as tension or compression, act within the object and can also affect the shape of points.

4. Do different types of forces affect geometric points differently?

Yes, different types of forces can affect geometric points differently. For example, a point may experience a different amount of deformation when subjected to a compressive force compared to a tensile force. Additionally, different types of forces may result in different types of motion, such as rotation or translation of points.

5. Is it possible for a geometric point to be unaffected by forces?

No, it is not possible for a geometric point to be completely unaffected by forces. Even if a point appears to be stationary, there are likely forces acting on it that are balancing out and keeping it in place. In physics, it is often said that every action has an equal and opposite reaction, so even if a point is not visibly moving, forces are still acting on it in some way.

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