Place to discuss the Theory of Relativity

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Discussion Overview

The discussion centers on the Theory of Relativity, particularly focusing on the implications of accelerating objects in space and the concept of speed relative to the speed of light. Participants explore the nuances of special relativity, including time dilation and the behavior of objects as they approach light speed.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes a scenario where an object accelerates to 2/5 the speed of light multiple times, questioning the validity of traveling faster than light and seeking to identify flaws in their reasoning.
  • Another participant explains that in special relativity, speeds do not add linearly as in classical mechanics, introducing the concept of time dilation as one approaches the speed of light.
  • A different participant contrasts the Newtonian perspective of speed accumulation with the relativistic view, emphasizing that as an object's speed increases, its relativistic mass increases, requiring infinite energy to reach the speed of light.
  • One participant challenges the notion of absolute motion, highlighting that all motion is relative and providing an analogy involving a car's speed relative to different reference points.
  • Another participant elaborates on the implications of acceleration from the perspective of both the observer and the accelerating object, noting that while the observer sees diminishing returns on speed increases, the object experiences consistent acceleration.
  • A participant introduces a mathematical perspective on relative speeds, referencing the Newtonian view of adding velocities and contrasting it with Einstein's framework.

Areas of Agreement / Disagreement

Participants express various interpretations of the implications of special relativity, with no consensus reached on the specific scenarios discussed. Multiple competing views remain regarding the nature of speed, acceleration, and the concept of absolute motion.

Contextual Notes

The discussion includes assumptions about reference frames and the nature of speed that may not be universally agreed upon. The mathematical steps involved in relativistic calculations are not fully resolved, leaving room for interpretation.

  • #91
EnumaElish said:
Don't your teachers deserve any credit for the fact that you can smart out almost anybody in this forum?
Being able to out smart anyone on these forums is quite a leap considering I've participated in only a handful of discussions.

As for physics in HS, I did have a very good teacher though I don't recall relativity being covered, perhaps it was briefly.
 
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  • #92
And relativistic mass was never included in your curricula? Or was it?
 
  • #93
EnumaElish said:
And relativistic mass was never included in your curricula? Or was it?
Luckily I still have many of my physics notes. Most of my knowledge of special relativity is self learned though. I never took a class in college devoted solely to special relativity, but my physics classes at least covered the topic. (I have an engineering degree, not a physics degree). One of the best professors I had in college was one of my physics professors and here are his equations:

p = \gamma m v

E = m c^{2} + K = \gamma m c^{2}

E^{2} = (p c)^{2} + (m c^{2})^{2}

As you can see, there is no mention of "relativistic mass" as that equation would be:
E = m_r c^{2}
where m_r is relativistic mass. Also I checked the index of my physics book which contains no reference to relativistic mass.

Edit: Can someone (I am talking to you management, put a link to latex reference on the main page? OR if it is there, please make it more noticable)
 
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  • #94
Aer said:
One of the best professors I had in college was one of my physics professors and here are his equations:

p = \gamma m v

E = m c^{2} + K = \gamma m c^{2}

E^{2} = (p c)^{2} + (m c^{2})^{2}

As you can see, there is no mention of "relativistic mass" as that equation would be:
E = m_r c^{2}
where m_r is relativistic mass.
What is K? And what is \gamma? What I am wondering is whether mr is not part of these equations implicitly, or whether it can be derived from them, e.g. mr = m/b, for a suitably defined b.
 
  • #95
EnumaElish said:
What is K? And what is \gamma? What I am wondering is whether mr is not part of these equations implicitly, or whether it can be derived from them, e.g. mr = m/b, for a suitably defined b.
K is kinetic energy and \gamma is the relativity gamma factor (i.e. {1}/{\sqrt{1-({v}/{c})^{2}}})
 
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  • #96
If m_r is defined as = \gamma m, then E = \gamma m c^2= m_r c^2, so relativistic mass is implicitly in your notes.
 
  • #97
EnumaElish said:
If m_r is defined as = \gamma m, then E = \gamma m c^2= m_r c^2, so relativistic mass is implicitly in your notes.
I made m_r up, it is not in my notes. As I said, that is just a definition and a meaningless definition at that. I could also define a "relativistic velocity" as v_r = \gamma v, does this velocity have any physical meaning? No it doesn't, athough the two terms \gamma v come up in some equations, it doesn't make any sense to think of it as a "relativisitic velocity" to explain anything.
 
  • #98
From now on, whenever I use the expression "relativistic mass" (or the notation mr) I will remember that it was not mentioned in your notes. Or that it is difficult to interpret as a physical entity (because it mixes the two frames, so to speak).
 
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  • #99
George Jones said:
Try the excellent General Relativity from A to B by Robert Geroch, which details different views spacetime from Aristotle to Galileo to Einstein.

Regards,
George

This book has finally arrived. Let's see how I get on :rolleyes:
 

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