zefram_c
- 252
- 0
I think I know why it would be said that \mu_o and \epsilon_0 are not physically measurable. They depend on the way we define quantities like one metre, one second, one unit of current, etc. For example, in SI one Ampere is that current that enters the Biot-Savart law so that \mu_o is *exactly* as shown. These dimensionful quantities can always be redefined. I have not done the math, but I think we could say that light travels exactly one meter per second, then adjust all other fundamental quantities to recover the same physics. There is a principle that says physics must be independent of the choice of units. On the other hand, no amount of tinkering can let us redefine the value of the fine structure constant, as that is a dimensionless parameter and must be preserved if we redefine our choice of units. That is truly a fundamental parameter of the observed universe.marcus said:Goodness!
It says here that the value of mu_0 is exactly
4\pi \times 10^{-7}
how can something like 4pi be measurable?
surely this can't be an actual physical property of empty space
what kind of intrument can you picture using to measure it?
An excellent point; I prefer to refer to such things as the "twin scenario" or the "twin experiment" to emphasize that there is no unsolved paradox threatening relativity there.russ_waters said:Not sure who I would address this to (Einstein's editor?), but names like "train paradox" and "twins paradox" are somewhat misleading. They are only paradoxes when using incorrect physics, ie applying Galilean relativity to situations where it doesn't apply. People read "twins paradox" regarding Relativity and assume its a paradox in Einstein's theory. It isn't. How about "apparent train paradox"? I guess when Einstein was doing his work though, they were still unresolved paradoxes.