^ watch less youtube channels with names like "storm clouds gathering". cant wait until i can get a mr. fusion though
Muncey wrote:Not sure if this comparison has been made before, it probably has, but I recently heard (not for the first time) Feynmans quote about QM: "If you think you understand quantum mechanics, you don't understand quantum mechanics."
On hearing it this time, it reminded me of Wittgenstein's lion.. he said if a lion could speak English we couldn't understand him because we have hugely different points of reference, inputs and processing those inputs. We essentially experience the world entirely differently and therefore could never understand a lion speaking English. As we live in the sort of middle ground between the extremely big and the extremely small, possibly quantum mechanics could never fully be an understandable concept for the exact same reason why we couldn't understand a lion. We use computers to test theories and draw conclusions but our interpretations and understandings of these aren't adequate, maybe because of the same reason?
Maybe we're doomed to never understand quantum mechanics fully? Or the extremely small/large?
Does this go some way to support the Copenhagen interpretation?
I'm sure someone with better knowledge of physics could shed some light on this.
not sure if this is the answer you're looking for but here's my thoughts (probably overdid it lol):
i'm optimistic, but it is a very real possibility that we'll never manage to progress beyond our current understanding of quantum mechanics. for all we know, maybe there just isnt a way to mathematically describe it. 
i would say that does fit with the copenhagen interpretation. the copenhagen interpretation essentially takes what we don't know about it, and shoves it into a mysterious black box that it labels "wave function collapse". we have a quantum system at the beginning, then wave function collapse mysteriously does its work on the system, and then we end up with classical qualities. what gives? like you say, scale might play a role. right now at the LHC we're probing around 10^-18m, while the smallest possible scale is 10^-35 (around which quantum gravity becomes strong). obviously we've still got a long way to go. maybe we'll get more hints to go off of as we start to approach the smallest scales and highest energies.
my optimism comes from the belief that we're facing a similar dilemma to the one that physics was facing at the late 19th / early 20th century, before the classical to quantum revolution. classical mechanics obviously worked, but it couldn't account for a lot of things. quantum mechanics is also relatively successful in its own right, and in the form of quantum field theory (where it's combined with special relativity), it's given us the standard model. but there's obvious gaps, just like with classical mechanics. there's the unexplained mysteries of quantum mechanics, and when it comes to QFT, there's a whole other set of issues (hierarchy problem, neutrino masses, quantum gravity, the fact that we have to experimentally determine particle masses and plug them in rather than being able to derive them from the model itself, etc). 
i think i've probably mentioned this before in the thread, but there's a physicist called Nima Arkani-Hamed who has a lot of interesting talks where he covers this. he mentions how, looking back now, a big hint towards the existence of quantum mechanics, way before it was actually discovered, was that you could reformulate classical mechanics using the principle of least action, which is non-deterministic (unlike the strictly deterministic classical mechanics). 
right now he's spearheading work where they've been able to calculate scattering amplitudes (which when squared give you probabilities) of particle interactions using an entirely new method, one that isn't based off of quantum field theory. and similarly to the way that quantum mechanics abandoned determinism, his method abandons what are called locality and unitary (
which means that the particle interactions are point-like and sum of the probabilities in scattering experiments must be equal to one). in my opinion it's by far the most interesting thing going on in theoretical physics today, and is one of the few areas that really shows a lot of promise (unlike string theory which seems hopeless 

 )