Kinetic energy in frames of reference

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SUMMARY

The discussion centers on the differences in kinetic energy (KE) gain when one object accelerates from velocity v to 2v, while another remains at velocity v. It is established that the work done is not constant across different frames of reference due to variations in distance traveled under constant acceleration. In the stationary frame, the work done is three times larger than in the moving frame, correlating with the change in kinetic energy. This highlights the importance of understanding frame-dependent calculations in classical mechanics.

PREREQUISITES
  • Understanding of classical mechanics principles, particularly kinetic energy and work.
  • Familiarity with the concept of frames of reference in physics.
  • Knowledge of calculus, specifically integration as it applies to motion.
  • Ability to apply Newton's laws of motion in different contexts.
NEXT STEPS
  • Study the relationship between work and kinetic energy in different frames of reference.
  • Learn about the implications of constant acceleration on distance and velocity calculations.
  • Explore the mathematical derivation of kinetic energy formulas in various frames.
  • Investigate the effects of relativistic speeds on kinetic energy and work done.
USEFUL FOR

Students of physics, educators teaching classical mechanics, and anyone interested in the nuances of kinetic energy and work in different frames of reference.

daveed
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i was just reading, and i saw this question, and i don't know how to explain it...

how can you describe why when two things go at a velocity v, and one of them accelerates to 2v, the KE gain w/ respect to the Earth and the other object are different, but the work done is constant?

i just don't know how to explain this... it should not be so difficult, no?
 
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daveed said:
how can you describe why when two things go at a velocity v, and one of them accelerates to 2v, the KE gain w/ respect to the Earth and the other object are different, but the work done is constant?

The work, Fx (assuming constant acceleration), isn't constant. The force is the same in both frames, but the distance isn't.

[tex]x=\int v~dt[/tex]

Moving frame:

[tex]v=\int a~dt=at[/tex]
[tex]x=\frac{1}{2}at^2[/tex]

Stationary frame:

[tex]v=v_0+\int a~dt=v_0+at[/tex]
[tex]x=v_0t+\frac{1}{2}at^2[/tex]

In your example, this leads to work that's three times larger in the stationary frame, just like the change of kinetic energy.
 

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