Juan,
Thanks for your comments. I have a few replies.
First, regarding Robinson, I certainly am no fan of his and I did not cite him in such a way as to say I supported his conclusion. I simply cited him in order to point out that someone had attempted to "vindicate" Newton and Leibniz in recent decades.
I agree that time is a complicated and funky problem (and I'm looking forward to the FQXi conference in August when we'll be discussing the nature of time in greater detail).
Here is what I mean about the uncertainty relations when applied to a radar gun. A radar gun relies on a measurable change in the wavelength of the light it emits and then reabsorbs. Since the wavelength is directly related to the energy, as Delta t goes to zero, Delta E must go to infinity by the uncertainty relation. But Delta E *can't* be infinite if the radar gun is to work (it *must* be finite). Therefore, Delta t must have a non-zero lower bound.
One of my points is that if we tried to truly measure quantities exactly and in a truly continuous manner, we need to have more and more accurate measurements. But as we make more and more accurate measurements, we eventually leave the classical realm and end up in the quantum realm and the quantum realm is constrained by the uncertainty relations. This limits our knowledge to discrete "chunks." So our knowledge of the universe is limited to discrete "chunks."
As for the old chemists, they certainly may have believed in the discrete nature of matter, but did they necessarily think that the universe itself was necessarily discrete? I seriously doubt that. The atomic hypothesis applies to matter. I am unaware of it having been applied to the universe as a whole by anyone between the Ancient Greeks and the twentieth (maybe late nineteenth?) century.
Regarding the non-geometric interpretation of gravity, while there certainly are non-geometric interpretations of gravity, they are by no means mainstream. The geometric interpretation of gravity has been the paradigm since Einstein. Nevertheless, I certainly was not defending that interpretation. In fact, that was my point. I don't like that interpretation because it is difficult to reconcile with quantization (despite what the field theorists think).
I am familiar with how quantum field theory handles quantization and localization. In fact there is a rich history of foundational discussions surrounding this but, alas, I was limited to 25000 characters and I know how Dirac viewed it. But it is still a fact that QFT is built on top of QM and thus includes its postulates and thus its limitations, i.e., as different as they may be, they do *not* contradict one another.
You say, "I think that this is a reflect of the traditional epistemological approach to physical reality, where science is perceived as a sequence of approximations to one supposed fundamental true." I don't know if I agree that what I'm saying is necessarily a reflection of this. In fact, assuming that classical physics is just an approximation and that the world is really quantum only seems to allow for *multiple* truths, in my opinion. After all, the quantum world is a strange place.
The reason I say classical physics is a "myth" is because as soon as you start to make classical measurements more and more accurate (to more and more decimal places) you will eventually bump into the quantum realm. In other words, you can't have perfectly accurate measuring apparatuses without getting into quantum mechanics. Just think about how we "define" the meter now. It used to be a rod in Paris, but then copying it introduced small defects. The only way anyone could see to it that the meter was the same everywhere was to redefine it in such a way that it can only be measured in ways that involve quantum mechanics! (The current definition is based on the speed of light, which is classical, but all laboratory measurements of the speed of light run up against quantum uncertainties and quantum photon counting statistics.)
Ian