What makes me chuckle is Smith's (E)^2 = (pc)^2 + (mc^2)^2 that he calls "correct". If we take E= mc^2 as a given and equal to the rest mass, (let me know if you want a proof of this) and give the mass a push so that it has some kinetic energy 1/2 mv^2, Then this simulates a particle in an accelerator, and the total is E = mc^2 + 1/2 mv^2 [ Note to reader: Relativistic energy is defined as E = mc^2/sqrt(1-v^2/c^2) ] Squaring, E^2 = (mc^2 + 1/2 mv^2)^2 = (mc^2 + 1/2 mv^2)(mc^2 + 1/2 mv^2) = m^2c^4 + m^2c^2 v^2 + 1/4 m^2v^4 Defining p = mv , [ Note to reader: Relativistic momentum is defined as p = mv/sqrt(1-v^2/c^2) ] E^2 = (mc^2)^2 + (pc)^2 + (1/2mv^2)^2 Smith conveniently drops off the 1/4 m^2v^4, which, if v almost equals c, would be quite a lot of energy. The reason for doing this is to include gamma so that they can make for the missing energy in any real experiment involving a particle. And of the course the actual speed, v, cannot be directly measured and is calculated from the equations, thus "proving" SR. [ Note to reader: With the given definitions it can easily be shown that (E)^2 = (pc)^2 + (mc^2)^2 ] |
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Fumble Index | Original post & context: t0RWc.232$nC1.2470968@news-text.cableinet.net |