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?
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.
PREREQUISITESStudents of physics, educators teaching special relativity, and anyone interested in the nuances of relativistic mechanics and energy calculations.
... yet another example why relativistic mass was a bad idea.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?
This question has absolutely nothing to do with the great idea of relativistic mass.Trilairian said:... yet another example why relativistic mass was a bad idea.
Mass doesn't change with speed.
E_{K} = (\gamma -1)mc^{2}