How does the weight of a rock change in relativistic speeds?

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Discussion Overview

The discussion revolves around the effects of relativistic speeds on the perceived weight of a rock held by a person in motion. It explores concepts from special relativity (SR) and general relativity (GR), focusing on how different observers perceive changes in weight and force due to relative motion and time dilation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that from Person A's perspective, the rock's weight remains unchanged, while from Person B's perspective, the rock appears to gain weight due to relativistic effects.
  • Others argue that in special relativity, the rock does not get heavier; it either maintains the same weight or becomes lighter depending on the direction of the force relative to the observer's motion.
  • A participant notes that the weight perceived by Person A does not change because his time is dilated, implying that the relationship between time and force is crucial in this context.
  • Another participant raises a question about how space-time in general relativity might depend on the relative motion of an observer towards a gravitational source, suggesting a potential connection to the discussion.
  • There is a repeated assertion that the weight cannot appear lighter in the frame of the person holding the rock, as this would imply a way to measure absolute velocity.
  • One participant seeks clarification on the concept of force and the time derivative mentioned in relation to the weight held by Person A.

Areas of Agreement / Disagreement

Participants express differing views on how relativistic effects influence the weight of the rock, with no consensus reached on the implications of these effects in special or general relativity.

Contextual Notes

There are unresolved assumptions regarding the definitions of weight and force in relativistic contexts, as well as the implications of time dilation on these concepts. The discussion also touches on the complexities of gravitational effects in general relativity, which are not fully addressed.

The Rev
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I'm pretty new to the ideas of relativity, so maybe this is old ground to cover for some of you. However, I need to know how to resolve an apparent paradox.

Person A is traveling at relativistic speeds holding a stone over his head. The stone weighs just slightly less than the maximum weight that he is able to hold up. Person B is an observer, watching Person A. From Person A's point of view, the rock is unchanged, so he continues to hold it up. From Person B's point of view, however, the rock grows heavier due to relativistic increases in mass, and falls on Person A's head, killing him.

Now, how does Person A, who is alive from his own point of view, communicate to Person B that he really isn't dead?

o:)

The Rev
 
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SR doesn't deal with gravity and unfortunately relativstic descriptions of grabity can never be that simple. Also remember F=Ma isn't generally true in SR anyway.
 
It turns out the rock never gets heavier in SR. It either has the same weight, or it gets lighter! (By "weight" I mean "force").

It's the same weight (force!) if the force points in the same direction as the observer is moving.

It's lighter (a lower force) if the force points at at an angle to the direction of motion.

This comes from the transformation laws, which can be derived from the folowing defintions.

4-force = dp/dtau, where p is energy-momentum 4-vector, and tau is the "proper time".

4-forces transform like any other 4-vector.

3-force = dp/dt - where p is the relativistic momentum (the energy-momentum 4-vector with the energy part omitted), and t is the coordinate time, rather than the proper time.

From the above, it can be seen that the 4-force and the 3-force are related by the time dilation factor, dt/dtau, i.e. (dp/dtau) = (dp/dt) * (dt/dtau)
 
pervect said:
It turns out the rock never gets heavier in SR. It either has the same weight, or it gets lighter! (By "weight" I mean "force").

It's the same weight (force!) if the force points in the same direction as the observer is moving.

It's lighter (a lower force) if the force points at at an angle to the direction of motion.
Just to avoid confusion, the weight cannot get lighter in the frame of the man carrying the boulder, since that would provide the man with a way of measuring his absolute velocity...I guess the resolution would be that even if the force from the boulder pushing down on the man weakens as seen in some other frame, the force upwards from the man pushing on the boulder will also weaken as seen in that frame, so this frame will also predict no change in how high the boulder is held up.
 
Jscd : This is an interesting problem you put forward :

1)in SR, time and space change depend on the relative speed
2)in GR time and space depend on the relative position towards the source of gravitation.

shouldn't in GR space-time depends on the relative motion of the observer towards the source of gravitation too ?
 
For the guy hodling the rock, the weight he must hold doesn't change because his
time is slowing down. A heavier rock in slower time doesn't weigh more because there
is a time derivative in computing the force.
 
For the guy hodling the rock, the weight he must hold doesn't change because his
time is slowing down. A heavier rock in slower time doesn't weigh more because there
is a time derivative in computing the force.


just for the record, what force are you talking about, and in regards to what time derivative?
 

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