Special Relativity: 3 Objects, Momentum & Time Dilation

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SUMMARY

This discussion centers on the application of special relativity to analyze the motion of three observers in a coordinate plane. Observer 1 is stationary at (0,0), while Observer 2 moves at 5 m/s in the x-direction from Observer 1, and Observer 3 moves at 0.5C in the y-direction as seen by Observer 2. The key conclusion is that both Observers 2 and 3 share the same x-component of velocity as measured by Observer 1, despite differing y-components. The discussion clarifies that relativistic mass is no longer a relevant concept, emphasizing the importance of momentum conservation across different reference frames.

PREREQUISITES
  • Understanding of special relativity concepts, including reference frames and velocity transformations.
  • Familiarity with the Lorentz factor (γ) and its application in relativistic equations.
  • Knowledge of momentum conservation principles in physics.
  • Basic mathematical skills to manipulate equations involving velocity and relativistic effects.
NEXT STEPS
  • Study the Lorentz transformation equations in detail to understand their implications in different reference frames.
  • Explore the concept of relativistic momentum and its differences from classical momentum.
  • Learn about the implications of time dilation and how it affects moving observers in special relativity.
  • Investigate the historical context and evolution of the concept of relativistic mass in physics.
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This discussion is beneficial for physics students, educators, and anyone interested in the principles of special relativity, particularly those studying motion and reference frames in relativistic contexts.

learning
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Let us have an observer at rest at (0,0) in a coordinate plane. Another at (1,0) moving away from the first observer at 5 m/s in the x direction as seen by observer 1 and another object at (1,1) moving away from observer 2 at 0.5C in the y direction as seen by observer 2. Should observer 1 see observer 2 moving in the x direction faster than observer 3.
Let us have an observer at rest at (0,0) in a coordinate plane. Another at (1,0) moving away from the first observer at 5 m/s in the x direction as seen by observer 1 and another object at (1,1) moving away from observer 2 at 0.5C in the y direction as seen by observer 2. Should observer 1 see observer 2 moving in the x direction faster than observer 3?

The confusion I have is because if an object has more mass at higher velocities would it slow down in directions where it is not moving relativistically because of conservation of momentum or time dilation or something?
 
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learning said:
Summary:: Let us have an observer at rest at (0,0) in a coordinate plane. Another at (1,0) moving away from the first observer at 5 m/s in the x direction as seen by observer 1 and another object at (1,1) moving away from observer 2 at 0.5C in the y direction as seen by observer 2. Should observer 1 see observer 2 moving in the x direction faster than observer 3.

Let us have an observer at rest at (0,0) in a coordinate plane. Another at (1,0) moving away from the first observer at 5 m/s in the x direction as seen by observer 1 and another object at (1,1) moving away from observer 2 at 0.5C in the y direction as seen by observer 2. Should observer 1 see observer 2 moving in the x direction faster than observer 3?
They will have the same x-component of velocity, but different y-components. You can use the velocity transformation rule. Here we have the second frame moving to the right at some speed ##v##. And in that frame, the velocity of the third object is ##u'_x = 0, u'_y = 0.5c##.

When we transform the velocity of this object to the first frame we get: $$u_x = \frac{u'_x + v}{1 + vu'_x/c^2} = v$$ And both objects 2 and 3 have ##v## as the x-component of their velocity, as measured in the first frame.

learning said:
The confusion I have is because if an object has more mass at higher velocities would it slow down in directions where it is not moving relativistically because of conservation of momentum or time dilation or something?
This makes no sense. Generally, relativistic mass is a red herring and not used any more.

Conservation of momentum means "the same momentum over time". Momentum varies between reference frames, as it must: you can be at rest in one frame but not in another.
 
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PS The y-component of the velocity transforms according to: $$u_y = \frac{u'_y}{\gamma(1 + vu'_x/c^2)} = \frac{u'_y}{\gamma} < u'_y$$
 
@learning positions you said as (0,0)or (1,1) does not matter.
May I interpret your question as :

No. 2 observes No.1 is moving x direction with v1, you say -5 m/s.
No. 1 observes No. 2 is moving x direction with -v1, you say 5m/s.
No. 2 observes No.3 is moving y direction with v3, you say 0.5 c =1.5E8 m/s.
No. 3 observes No.2 is moving y direction with -v3, you say -0.5 c =-1.5E8 m/s.
Question: How fast does No.1 observe No.3 moves ?
 
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PeroK said:
They will have the same x-component of velocity, but different y-components. You can use the velocity transformation rule. Here we have the second frame moving to the right at some speed ##v##. And in that frame, the velocity of the third object is ##u'_x = 0, u'_y = 0.5c##.

When we transform the velocity of this object to the first frame we get: $$u_x = \frac{u'_x + v}{1 + vu'_x/c^2} = v$$ And both objects 2 and 3 have ##v## as the x-component of their velocity, as measured in the first frame.This makes no sense. Generally, relativistic mass is a red herring and not used any more.

Conservation of momentum means "the same momentum over time". Momentum varies between reference frames, as it must: you can be at rest in one frame but not in another.
Thank you this clears things up.
 

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