Fundamentally you can't disprove Heisenberg with
Newtonian laws, so
if you think you can, you are likely wrong (to very high degree of
liklihood).
And if you have such an argument and it _is_ right, all you've shown is
that Newtonian mechanics and Heisenberg are incompatible, that they
cannot both be right. Which, if either, _is_ right is a question for
experiment, not theorizing. (My money would be on Heisenberg in such a
case.)
People have already mentioned how acceleration and
smallness can mess
up the measurement, but it's probably more than that. Indirectly
related might be the Bose-Einstein concentrate. Scientists slowed
down subatomic particles to a near stop, so they knew the position
and the speed right? Apparently the particles by theory and by the
experiment just "deres" or become big fuzzballs that have no definite
position.
That's part of it; the Pauli exclusion principle is also related.
The exclusion principle says that particles with non-integer spin
(fermions, such as electrons with their spin ??) cannot be identical:
two such particles must differ in location, or spin, or some such.
This is why atoms have electron shells that can fill up - for example,
the first shell is spatially symmetric, and thus can tolerate only two
electrons, one with spin +? and one with spin -?; the next shells are
lobed, with three such available (one for each spatial dimension),
holding two electrons each. Fermions display Fermi-Dirac statistics, I
think the term is.
Particles with integer spin (bosons, such as photons with their zero
spin) can be as identical as they care to; they are said to display
Bose-Einstein statistics.
As you say, when particles get very cold, their momentum becomes very
small, to a high degree of precision, which means their position
becomes correspondingly _un_certain: they fuzz out, to put it loosely.
But if you try this with fermions, they resist overlapping because of
the exclusion principle[%]; you have to do it with bosons to get
anything really interesting. (This is why helium-4 becomes superfluid
but helium-3 doesn't: that extra neutron makes the difference between
the nuclei being fermions and their being bosons.) With fermions, all
you get is zero-point motion (particles still jiggling around some
regardless of how close to absolute zero you get; they refuse to sit
still because that would give them very precise position _and_
velocity, and fuzzing out into a B-E condensate would make them overlap
with other fermions.)
[%] Actually, "because of" is a very imprecise way of putting it. We
do not know _why_ the world works this way; we do not know even
that there _is_ a "why". All we know is _that_ it does, and the
exclusion principle is just a description of one aspect of the way
the world works. To say that the exclusion principle is _why_
something happens is, strictly speaking, mistaking description for
causality.
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