Superluminal Frame Adjustments?

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Discussion Overview

The discussion revolves around the implications of switching between inertial reference frames (IRFs) in the context of special relativity, particularly focusing on the potential for superluminal speeds when transitioning from one frame to another. Participants explore the theoretical constructs of IRFs, length contraction, and the perception of motion during acceleration.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant suggests that when switching from IRF K to K’, distant parts of K’ may appear to move outward at speeds faster than c, raising questions about the violation of the speed of light limit.
  • Another participant counters that the relative velocity between the two frames does not necessitate superluminal speeds, as points in K remain at rest relative to K, and thus no violation occurs.
  • A different viewpoint emphasizes that the perception of superluminal motion arises during acceleration between IRFs, and that one cannot conclude that the universe is moving while feeling the effects of acceleration.
  • It is noted that special relativity does not prohibit travel faster than light but restricts communication at such speeds, challenging the notion that one can disprove special relativity through perceived superluminal motion.
  • A later reply questions whether it is correct to assert that an observer transitioning between IRFs while only experiencing linear acceleration remains within a series of comoving inertial frames, each moving at less than c relative to the original frame.

Areas of Agreement / Disagreement

Participants express differing views on the implications of switching IRFs and the nature of perceived motion during acceleration. No consensus is reached regarding the resolution of potential superluminal speeds or the interpretation of special relativity in this context.

Contextual Notes

Participants highlight the complexity of transitioning between IRFs, particularly under acceleration, and the potential for misinterpretation of motion. The discussion remains open to various interpretations and does not resolve the mathematical or conceptual nuances involved.

GRDixon
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In theory the set of Inertial Reference Frames could consist of an infinite set of rectangular grids and distributed clocks, overlaid and sliding through one another without interference. Let us say we are initially at rest at the Origin of IRF K. Relative to K, the grid of moving frame K’ will be length contracted, etc.

If we switch our rest frame to K’, then it will be the grid of K that is length contracted, etc. At great enough distances from the Origin of K, this would seem to require parts of the K’ grid to move outward, away from the Origins, at speeds faster than c. (And similarly, from the Origin of K’ it would seem distant parts of the K grid must move closer to the Origins at speeds greater than c.)

How can this violation of the rule, that c is the maximum speed of material objects, be resolved?
 
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GRDixon said:
In theory the set of Inertial Reference Frames could consist of an infinite set of rectangular grids and distributed clocks, overlaid and sliding through one another without interference. Let us say we are initially at rest at the Origin of IRF K. Relative to K, the grid of moving frame K’ will be length contracted, etc.

If we switch our rest frame to K’, then it will be the grid of K that is length contracted, etc. At great enough distances from the Origin of K, this would seem to require parts of the K’ grid to move outward, away from the Origins, at speeds faster than c. (And similarly, from the Origin of K’ it would seem distant parts of the K grid must move closer to the Origins at speeds greater than c.)

How can this violation of the rule, that c is the maximum speed of material objects, be resolved?

Let the relative velocity of the two frames be v. Every point of the grid at rest in K remains at rest in K and so a constant distance from the origin of the grid in K. Every point of the grid in K' moves at velocity v with respect to the origin of the grid at rest in K. And vice versa. No superluminal speeds required.

Matheinste.
 
GRDixon said:
In theory the set of Inertial Reference Frames could consist of an infinite set of rectangular grids and distributed clocks, overlaid and sliding through one another without interference. Let us say we are initially at rest at the Origin of IRF K. Relative to K, the grid of moving frame K’ will be length contracted, etc.

If we switch our rest frame to K’, then it will be the grid of K that is length contracted, etc. At great enough distances from the Origin of K, this would seem to require parts of the K’ grid to move outward, away from the Origins, at speeds faster than c. (And similarly, from the Origin of K’ it would seem distant parts of the K grid must move closer to the Origins at speeds greater than c.)

How can this violation of the rule, that c is the maximum speed of material objects, be resolved?

This is actually a valid (but somewhat silly, once you realize what's going on) question. What you are thinking of is acceleration from one IRF to another. When we are accelerating, especially if we are accelerating rapidly, we percieve distant parts of the Universe moving around, as if to violate the speed of light limit. But what you are missing is that since we are the one feeling the acceleration, we can't possibly conclude that we are at rest and the Universe is moving. The same thing happens with rotation: Sit down. Look up at the night sky and rotate your head. Sure, you could pretend that your head is stationary and that the cosmos are rotating rapidly around you, but that is obviously false and silly.

In fact, the shift of objects as we accelerate is a kind of rotation. It's called the Penrose rotation.

At any rate, SR does not forbid travel faster than light - it only forbids communication faster than light. So don't try too hard to come up with arguments like 'hey, I just proved that something can travel faster than light, so I disproved SR!' It doesn't work that way.
 
IttyBittyBit said:
This is actually a valid (but somewhat silly, once you realize what's going on) question. What you are thinking of is acceleration from one IRF to another. When we are accelerating, especially if we are accelerating rapidly, we percieve distant parts of the Universe moving around, as if to violate the speed of light limit. But what you are missing is that since we are the one feeling the acceleration, we can't possibly conclude that we are at rest and the Universe is moving. The same thing happens with rotation: Sit down. Look up at the night sky and rotate your head. Sure, you could pretend that your head is stationary and that the cosmos are rotating rapidly around you, but that is obviously false and silly.

In fact, the shift of objects as we accelerate is a kind of rotation. It's called the Penrose rotation.

At any rate, SR does not forbid travel faster than light - it only forbids communication faster than light. So don't try too hard to come up with arguments like 'hey, I just proved that something can travel faster than light, so I disproved SR!' It doesn't work that way.

Would it be corrrect to say that if only linear acceleration is involved while moving from being at rest in K to being at rest in K' the accelerating observer will be at rest in a series of comoving inertial frames each of whose velocities relative to the observer's original rest frame is less than c, and so all objects at rest in this series of frames are traveling at less than c relative to the non accelerating observer's rest frame at every stage?

Matheinste.
 

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