Is Absolute Position Necessary to Understand Relativity?

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Discussion Overview

The discussion revolves around the necessity of absolute position in understanding the principles of relativity, particularly in the context of force and velocity as objects approach the speed of light. Participants explore the implications of frame-dependence in measuring speed and force, and how these concepts relate to Newtonian mechanics.

Discussion Character

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

Main Points Raised

  • One participant suggests that understanding relativity requires the existence of absolute position, questioning how force and velocity can be defined without it.
  • Another participant counters that speed and force are frame-dependent, asserting that there is no absolute inertial frame.
  • It is noted that the force required to accelerate an object varies depending on the observer's frame of reference, with different observers measuring different forces for the same scenario.
  • One participant clarifies that the statement about force should specify that it is measured in the frame where the object approaches the speed of light.
  • A follow-up question raises confusion about whether it is possible to reach the speed of light relative to Earth by pushing an object while traveling alongside it, highlighting the differences in time measurement between frames.
  • Another participant explains that while an object can be accelerated to a certain speed in one frame, it will be measured differently in another frame, emphasizing the relativistic effects on time and speed measurements.

Areas of Agreement / Disagreement

Participants generally agree that speed and force are frame-dependent, but there remains disagreement on the necessity of absolute position in understanding relativity. The discussion includes multiple competing views and does not reach a consensus.

Contextual Notes

Participants express uncertainty regarding the implications of frame-dependence on force and velocity, as well as the conditions under which Newtonian mechanics applies in relativistic contexts. The discussion does not resolve these complexities.

joshk
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I am guessing this is an easy one to grasp, but I think I am missing something in my understanding of relativity.
Relativity suggests that as an object moves toward the speed of light, a greater amount of force is required to increase its velocity.
For this to be true, wouldn't it require the existence of absolute position?
For instance, when we say an object is approaching the speed of light, shouldn't this be relative to another inertial frame, such as an absolute inertial frame?
An apple is moving through space near the speed of light relative to the earth. If relativity is saying that a larger force (than predicted by Newtonian mechanics) is required to increase the velocity of the apple, then why wouldn't it be also be the case for a pear on Earth (who is also moving relative to the apple near the speed of light)?
 
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joshk said:
For this to be true, wouldn't it require the existence of absolute position?

No, because speed and force are frame-dependent.

joshk said:
when we say an object is approaching the speed of light, shouldn't this be relative to another inertial frame

It's relative to some inertial frame, yes. But there will always be some other inertial frame in which the object is at rest. Speed is frame-dependent.

joshk said:
such as an absolute inertial frame?

There is no such thing.

joshk said:
An apple is moving through space near the speed of light relative to the earth. If relativity is saying that a larger force (than predicted by Newtonian mechanics) is required to increase the velocity of the apple, then why wouldn't it be also be the case for a pear on Earth (who is also moving relative to the apple near the speed of light)?

The force an observer on Earth would have to exert on the apple would be larger. But the force someone moving along with the apple would have to exert would not. And conversely, an observer on Earth would not have to exert more force on the pear, but an observer moving along with the apple would. Speed and force are frame-dependent.
 
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joshk said:
For instance, when we say an object is approaching the speed of light, shouldn't this be relative to another inertial frame
Yes it should. Also "a greater amount of force is required to increase its velocity" should read "a greater amount of force as measured in the frame in which the object is approaching the speed of light is required to increase its velocity".
joshk said:
If relativity is saying that a larger force (than predicted by Newtonian mechanics) is required to increase the velocity of the apple, then why wouldn't it be also be the case for a pear on Earth (who is also moving relative to the apple near the speed of light)?
Force is frame dependent. According to the pear's frame it requires more force to achieve the same coordinate acceleration of the apple as for the pear. According to the apple's frame, vice versa.
 
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thanks peter and ibix that clears up a lot!
I did suspect that would be the explanation for the last question. So if I could follow up, I get confused in that...
If the force to increase the speed of the apple as you move along with the apple is Newtonian, then wouldn't it be possible to actually get the velocity of the apple relative to Earth to the speed of light as long as someone (or something like a rocket) is traveling along with and pushing the apple?
 
joshk said:
thanks peter and ibix that clears up a lot!
I did suspect that would be the explanation for the last question. So if I could follow up, I get confused in that...
If the force to increase the speed of the apple as you move along with the apple is Newtonian, then wouldn't it be possible to actually get the velocity of the apple relative to Earth to the speed of light as long as someone (or something like a rocket) is traveling along with and pushing the apple?
The problem is that someone in the spaceship measures time differently than someone on the Earth. So for example, if the ship is moving at 0.9c, it is perfectly possible for something in the rocket to be accelerated to 0.1c relative the the rocket as measured by someone in the rocket. However, someone on the Earth would only measure the object as being accelerated to 0.91743...c relative to the Earth.( and the object would only measure its velocity as being 0.91743...c relative to the Earth.)
 
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Janus said:
The problem is that someone in the spaceship measures time differently than someone on the Earth. So for example, if the ship is moving at 0.9c, it is perfectly possible for something in the rocket to be accelerated to 0.1c relative the the rocket as measured by someone in the rocket. However, someone on the Earth would only measure the object as being accelerated to 0.91743...c relative to the Earth.( and the object would only measure its velocity as being 0.91743...c relative to the Earth.)

thanks that makes perfect sense!
 

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