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 |