- #36
Dale
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I have already given a counterexample. ##G## is dimensionless in geometrized units, and it is not dimensionless in SI units.ohwilleke said:the dimensions to which units may be affixed are defined by physics. Quantities that are dimensionless in one unit system are necessarily dimensionless in others
There are quantities that are dimensionless in all unit systems, like ##\alpha##, but not all dimensionless quantities are like that.
This doesn’t work because the equations are different in different unit systems. In those other systems there aren’t any other parts of the equation to shift them to.ohwilleke said:You can use a different physical constants than Newton's constant defined in a dimensionless way (as quantum theories of gravity often do) and shift the dimensions that are captured by the dimensions in Newton's constant to some other part of the equation, but you can't simply change units and eliminate their dimensionality.
For example in SI units Newton’s 2nd law is ##\Sigma \vec f =m\vec a## but you could make a system of units (Dale units) where force is its own base dimension. In those units Newton’s 2nd law is ##\Sigma \vec f = k m \vec a## where ##k## is a dimensionful universal constant with dimensions of ##F^{1}\ M^{-1}\ L^{-1}\ T^{2}##.
When we convert from Dale units to SI units we set ##k## to be a dimensionless 1. In the SI system force is not a base unit, it is a derived unit. That ##k## factor is not hidden in any of the remaining terms. It is simply gone. It doesn’t exist at all in SI units. Natural units do the same thing for ##c## and ##G##. They are not hidden somewhere in the equations, they are simply gone in those units, and the equations are simpler with nowhere to hide them anyway.
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