Kinetic Energy & Speed in Inertial Frames: Chris, Bob & Angelica

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Discussion Overview

The discussion revolves around the kinetic energy of objects moving at relativistic speeds as viewed from different inertial frames. Participants explore the relationships between speed, kinetic energy, and the effects of special relativity, with a focus on the calculations and expectations of kinetic energy from various perspectives.

Discussion Character

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

Main Points Raised

  • Chris presents calculations of relative speeds and kinetic energies for Bob and Angelica from his perspective, expecting Bob's kinetic energy to be half of Angelica's.
  • Some participants question the validity of Chris's expectation, arguing that in both non-relativistic and relativistic contexts, the kinetic energy does not behave as he anticipates.
  • One participant explains that the kinetic energy observed from an inertial frame is not directly proportional to the velocities of the objects involved, referencing the non-linear relationship between kinetic energy and velocity.
  • Another participant illustrates that the change in kinetic energy for an object moving at higher speeds is greater than for one moving at lower speeds, emphasizing the non-linear nature of the kinetic energy versus velocity graph.
  • Participants discuss the implications of these relationships and how they lead to different kinetic energy values when viewed from different frames of reference.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the expectations regarding kinetic energy calculations. There are competing views on how kinetic energy should be interpreted in the context of special relativity, and the discussion remains unresolved regarding the initial assumptions made by Chris.

Contextual Notes

Limitations include potential misunderstandings of relativistic effects, the dependence on the definitions of kinetic energy, and the assumptions made about the velocities involved. Some calculations presented may lack clarity or completeness.

Wout Veltman
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From Chris' perspective Bob is traveling with 1.5*108 m/s in direction a. Angelica is also traveling with 2.4*108 m/s in direction a.

From Bob's perspective Chris is traveling with 1.5*108 m/s in direction b (The opposite of x). Angelica is traveling with 1.5*108 m/s in direction a.

They all have a mass of 1

I am pretty sure these numbers are right. I used w = (u+v)/(1+(u*v)/(c2)) To calculate the relative speeds.
I used the calculation in the picture to calculate the Ek of Bob. I also calculated the Ek of Angelica, all from chris' perspective. Now the outcome that I was expecting was that Bob's Ek would be half of Angelica's Ek when looking from Chris' perspective. Because Angelica is also traveling with 1.5*108 m/s when measured from Bob's perspective. Why does this not count up?

I am sorry if a skipped a few vital steps. All of my special relativity knowledge comes from self-studying. We don't get this in school.

Thank you in advance.
 
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Wout Veltman said:
Now the outcome that I was expecting was that Bob's Ek would be half of Angelica's Ek when looking from Chris' perspective
Why would that be true? Even in the non relativistic domain, it makes no sense.
Suppose you have an observer ##C## at the origin. An object ##B## moves with velocity ##v## in a particular direction. In the same direction, another object ##A## moves with velocity ##v## as seen by ##B##. The velocity of ##A## as seen by ##C## will be ##2v## ( since this is non relativistic, they simply add). The kinetic energy ( as observed by ##C##), of ##A## is not twice that of ##B##, rather it's four times .
Likewise, in the relativistic domain, there is no reason for the results you expected.
 
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I see I made a few unnecessary mistakes there, also in the picture I posted with it. But my confusion is still there, let me try to explain it in another way.

You have an observer ##C## at the origin. An object ##B## is moving with 1.5*108 m/s in a particular direction. Object ##B## has his buddy ##A## moving next to him, with the same velocity and direction as ##B##. Now object ##A## accelerates till he reaches a speed of 1.5*108 m/s, when looking from ##B##'s point of view, and a speed of 2.4*108 m/s viewed from the observers point of view.

The Ek of ##B## viewed from ##C##'s point of view = 1,392*1016 J.
The Ek of ##A## viewed from ##C##'s point of view = 6,00*1016 J.
The Ek of ##A## viewed from ##B##'s point of view = 1,392*1016 J.

Now from ##C##'s point of view, ##A## gained 4,606*1016 J.
And from ##B## point of view, ##A## only gained 1,392*1016 J.

Now my question is, how do you explain this?I used 3*108 m/s as the speed of light to make things easier.
0ef9f8c42e.jpg
 
Is your doubt something like this : The change in velocity for both A and B is the same, yet the change in their kinetic energies are different. How?
If so, the answer is simple. The slope of the curve in ##K## vs ##v## graph is not a straight line. It keeps on increasing (the curve has an asymptote at ##v=c##). It means that as the value of ##v## increases, so does the slope. It means for a given ##\Delta v## , ##\Delta K## is greater for larger values of ##v##.
 
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The same thing is seen in non relativistic domain also. The change in kinetic energy of a body going from ##100 m/s## to ##101 m/s## is greater than the change in ##K## for a body going from ##0 m/s## to ##1m/s##.
The reason is same here. The slope ##(\Delta K)/(\Delta v)## is not a straight line.
 
Aniruddha@94 said:
Is your doubt something like this : The change in velocity for both A and B is the same, yet the change in their kinetic energies are different. How?
If so, the answer is simple. The slope of the curve in ##K## vs ##v## graph is not a straight line. It keeps on increasing (the curve has an asymptote at ##v=c##). It means that as the value of ##v## increases, so does the slope. It means for a given ##\Delta v## , ##\Delta K## is greater for larger values of ##v##.

That does come very close to what I ment, yes, thank you very much.
 

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