Crosson said:
My point is that many derived equations of relativity (such as Hamiltons equations, relativistic momentum, schwarschild radius) reduce to classical (and more importnat, sensible) expressions in the limit c goes to infinity. It is standard to see this sort of thing done in textbooks.
OK, I agree with this, and I pointed out that it's related to the way that the Lorentz transforms reduce to the Gallilean transforms when c->infinity, so there is a formal basis for saying that relativity reduces to classical mechanics when c-> infinity.
Why ignore a very important case in which the limit does not lead to an expected result? I think special relativity implies that 'rest mass' (whatever that is) could not exist in a universe with infinite speed limit.
I guess I don' follow your question. To put it very simplistically, my view is that the limit of 1/c as c-> infinty exists, but the limit of c as c-> infinity doesn't exist. (One might say informally that it's infinite, but mathematically there is no limit). So one does not expect everything to have a well defined limit as c-> infinity.
To expand on this further, the Lorentz interval x^2+y^2+z^2 - c t^2 only makes sense mathematically if c is finite. When c is infinte, there isn't any corresponding interpretation of this quantity. Thus, classical mechanics doesn't have any corresponding concept of the Lorentz interval. Space and time are totally separate entities in classical mechanics, they never mix.
The length of the Lorentz interval gives proper time when the 4 vector is space-time (x,y,z,t), and it gives the invariant mass when the 4-vector is the energy-momentum 4-vector (dx/dtau, dy/dtau, dz/dtau, dt/dtau). This yields the very basic equation that's the root of your question.
Since the former concept doesn't exist in classical mechanics (there is no Lorentz interval in classical mechanics), the later concept doesn't exist either (there is nothing equivalent to the invariant mass of the energy-momentum 4-vector).
Sorry if this sounds too basic.