G
George Herold
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On Apr 7, 3:04 pm, RichD <r_delaney2...@yahoo.com> wrote:
particle that is participating in the event. As an electron goes from
one atomic orbital to another what is the energy of the electron? You
don't know, because you don't know which state it's in.
Now an electron can't just go BANG from one orbital to another. If it
did that there would have to be all sorts of high frequency stuff in
the light that came from it. But when you look at the light you see
only one frequency.... well not quite one there a bit of spread... and
that's the time uncertainty.
why they have the value they do.
George H.
The energy of the event is the uncertainty in the energy of theOn Apr 5, 1:43 pm, PD <thedraperfam...@gmail.com> wrote:> >the time-energy uncertainty principle,
which seems more obscure
than posiition-momentum. The books refer
almost entirely to the electron orbital energy
>>levels in the atom. That is, the emitted wavelength
dispersion, as the electron drops to a lower
energy, is inversely related to the time emitted,
in a probabilistic manner; the narrower the
spectrum, the wider (more unpredictable) the
time dispersion
But does the formula hold for every energy
measurement? For example, circuit voltage -
as on a capacitor - is a measure of energy.
Does this uncertainty principle apply there?
Does it place a limit on our time (frequency)
resolution in every circumstance?
It's not clear to me what it means, in these
classical situations.
It applies everywhere.
An interesting application is this:
You can reconstruct a decaying particle's rest
mass by measuring the momenta and identification
of all the daughter particles, and then combining
them in the usual fashion:
m^2 = (sum:E)^2 - (sum)^2.
What you will find, even in a detector with
exquisite momentum resolution, that the
reconstructed mass distribution has a natural
width. That natural width turns out to be related
to the half-life of the decaying particle, in exactly
the way you'd expect from the uncertainty principle.
Sure, but that's typical of all textbook discussions -
a matter of PREDICTION. We cannot predict the
duration of an event, except statistically. That's
time uncertainty.
I'm talking about measurement. The
common misunderstanding is "you can
measure the energy of an event, but you
can't know exactly when it happened!" Well,
why not? Why can't I observe the energy,
and look at my watch? None of the books address
this.
particle that is participating in the event. As an electron goes from
one atomic orbital to another what is the energy of the electron? You
don't know, because you don't know which state it's in.
Now an electron can't just go BANG from one orbital to another. If it
did that there would have to be all sorts of high frequency stuff in
the light that came from it. But when you look at the light you see
only one frequency.... well not quite one there a bit of spread... and
that's the time uncertainty.
At some point it's more fun to measure e and h, rather than discussI'm thinking of electric circuit A/D conversion,
in particular. I want to arbitrarily crank up both
the # of bits (energy resolution), and the
sample rate (time resolution). Does QM set a
limit? I have not seen any such proof.
Another problem is the definition of time uncertainty. Usually it's
fuzzy, heuristic, dumbed down for the introductory level.
But strictly, it's defined in terms of the energy
operator's statistics. It is abstruse. The only
place I have seen a rigorous derivation is Albert
Messiah's book. You could stare at it all day, and
not suss it. Obviously it is crucial to this question.
For more plebian examples, a transmission signal
chopped to a finite length sample will have a
frequency (e.g. energy) spectrum whose
minimum width is determined by the uncertainty
principle.
But that's just a mathematical corollary
of time-frequency duality, not really physics.
Time-energy uncertainty depends on h /= 0,
in QM. Consider: if h = 0, we get classical
mechanics, with no such uncertainty formula,
yet the Fourier uncertainty would still hold.
So that is not the answer, though it probably
bears on the answer.
--
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why they have the value they do.
George H.