Proving Relativistic Kinetic Energy: (1/2)*(gamma)mv^2

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SUMMARY

The discussion centers on the proof that the kinetic energy of a particle moving at relativistic speeds is given by the equation E_{kin}=m_{0}c^{2}(\gamma-1), which differs from the classical kinetic energy formula (1/2)*(gamma)mv^2. Participants clarify that mass does not change with speed, emphasizing the distinction between invariant mass and relativistic mass, with the latter increasing according to m_r = \gamma m_0. The conversation highlights the preference for invariant mass in modern physics and critiques the concept of relativistic mass.

PREREQUISITES
  • Understanding of special relativity concepts, including gamma factor (γ)
  • Familiarity with invariant mass versus relativistic mass
  • Knowledge of kinetic energy formulas in classical and relativistic contexts
  • Basic grasp of the work-energy theorem
NEXT STEPS
  • Study the derivation of the relativistic kinetic energy formula E_{K} = (\gamma - 1)m_{0}c^{2}
  • Explore the implications of invariant mass in modern physics
  • Learn about the gamma factor (γ) and its role in relativistic equations
  • Review the work-energy theorem and its applications in relativistic scenarios
USEFUL FOR

Students of physics, educators teaching special relativity, and anyone interested in the nuances of relativistic mechanics and energy calculations.

asdf1
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How do you prove that (1/2)*(gamma)mv^2 doen't equal the kinetic energy of a particle moving at relativistic speeds?
 
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Simply because

E_{kin}=m_{0}c^{2}\left(\gamma-1\right)

,which is different from your \frac{1}{2} \gamma m_{0}v^{2}...?

Daniel.
 
asdf1 said:
How do you prove that (1/2)*(gamma)mv^2 doen't equal the kinetic energy of a particle moving at relativistic speeds?
... yet another example why relativistic mass was a bad idea.

Mass doesn't change with speed.
E_{K} = (\gamma -1)mc^{2}
 
How so mass does not change with speed? I thought that as a particle approaches the speed of light then it must lose mass. What is it i got wrong here?
 
There are two sorts of mass. One of them, called invariant mass, stays constant regardless of velocity and is a property of the particle itself (it doesn't depend on the particles state of motion).

This is preferred by many, probably even most, people, but there are a few vocal people who prefer the other sort of mass, relativistic mass.

Relativistic mass _increases_ with velocity according to the formula

m_r = \gamma m_0

where m_r is the relativistic mass, m_0 is the invariant mass, and \gamma = \frac{1}{\sqrt{1-(v/c)^2}} depends on the velocity of the particle.

For some more information, see for instance the sci.physics.faq "Does mass change with velocity".

http://math.ucr.edu/home/baez/physics/Relativity/SR/mass.html
 
Last edited:
Trilairian said:
... yet another example why relativistic mass was a bad idea.

Mass doesn't change with speed.
E_{K} = (\gamma -1)mc^{2}
This question has absolutely nothing to do with the great idea of relativistic mass.

asdf1 - Its a matter of calculation. Simply calculate the kinetic energy and you'll obtain

K = (\gamma - 1)m_0 c^2

I worked out the calculation based on the work-energy theorem and placed them online at - http://www.geocities.com/physics_world/sr/work_energy.htm

Pete
 
wow! thank you very much! :)
 

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