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SamRoss
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Does anyone know of a derivation of the energy-momentum relation that does not make use of relativistic mass? In other words, a derivation that only uses invariant mass.
SamRoss said:Does anyone know of a derivation of the energy-momentum relation that does not make use of relativistic mass?
torquil said:I wish "relativistic mass" had never been defined!
It seems to be a source of confusion for newbies in SR.
The energy-momentum relation is a fundamental equation in physics that describes the relationship between energy and momentum in a system. It states that the energy of a particle is equal to its mass times the speed of light squared (E=mc²), and its momentum is equal to its mass times its velocity (p=mv).
Deriving the energy-momentum relation without using relativistic mass is important because it provides a more accurate and fundamental understanding of the relationship between energy and momentum. Relativistic mass is a concept that is used to simplify calculations in special relativity, but it can be misleading and cause confusion.
The energy-momentum relation can be derived using the principles of special relativity, specifically the Lorentz transformations and the equation for total energy in a system. By combining these equations and making the necessary substitutions, the classic form of the energy-momentum relation (E²=p²c²+m²c⁴) can be derived without the use of relativistic mass.
Deriving the energy-momentum relation without relativistic mass reinforces the idea that mass is a constant property of a particle, and that it does not change with velocity. This can help to clarify misconceptions about relativistic mass and lead to a better understanding of the relationship between energy and momentum.
Yes, the derivation of the energy-momentum relation without relativistic mass is widely accepted and is the standard approach in modern physics. It is based on the principles of special relativity and has been experimentally verified numerous times. However, the concept of relativistic mass is still used in some contexts for convenience and simplicity, but it is not considered a fundamental property of particles.