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Re: [Csnd] OT: uncertainty question

Date2012-09-28 02:18
Frompj@pjb.com.au
SubjectRe: [Csnd] OT: uncertainty question
Peiman wrote: 
> Also, does this in anyway relate to the uncertainty principle?

Yes, because (until they've been Observed) particles move in Waves
(described by Schroedinger's wave-equation); think of them as
probability-waves.

For example, if you want to know the Momentum of a particle, 
that's done by measuring the wavelength of its quantum-wave,
and to get an accurate answer you need to look at a packet many
wavelengths long, so that its fourier-analysis contains only
a very narrow band of wavelengths; but that means you don't
have a precise measure of the particle's Position, it's spread
out over that whole long distance.  Conversely, if you want
an accurate answer for its position, then you only look at a
short snippet of its wave, which means the fourier analysis of
that short snippet contains a broad band of wavelengths so
your measurement of the momentum will be very uncertain.

The maths of fourier-transforms means that there's a very simple
equation relating the uncertainty in the momentum to the uncertainty
in the position; it's called Heisenberg's Uncertainty Principle.

That's between position and momentum; they're called "complimetary
variables".  There are other pairs of complimetary measurements, like
Energy and Time, and they manifest the same uncertainty principle,
because of the same simple feature of the maths of fourier-transforms,
and the fact that particles move in probability-waves...

It's exactly the same maths as when you play a 1-millisec snippet
out of a bass-guitar note; the ear hears a click at a precise
time, but can't make out what the note was.

Regards,  Peter Billam

(P.S. hope I didn't make too many mistakes :-))

http://www.pjb.com.au      pj@pjb.com.au     (03) 6278 9410
"Follow the charge, not the particle."  --  Richard Feynman
 from The Theory of Positrons, Physical Review, 1949


Date2012-09-28 10:17
Frompeiman khosravi
SubjectRe: [Csnd] OT: uncertainty question
Thanks very much for this explanation. 

Best,
Peiman

On 28 September 2012 02:18, <pj@pjb.com.au> wrote:
Peiman wrote:
> Also, does this in anyway relate to the uncertainty principle?

Yes, because (until they've been Observed) particles move in Waves
(described by Schroedinger's wave-equation); think of them as
probability-waves.

For example, if you want to know the Momentum of a particle,
that's done by measuring the wavelength of its quantum-wave,
and to get an accurate answer you need to look at a packet many
wavelengths long, so that its fourier-analysis contains only
a very narrow band of wavelengths; but that means you don't
have a precise measure of the particle's Position, it's spread
out over that whole long distance.  Conversely, if you want
an accurate answer for its position, then you only look at a
short snippet of its wave, which means the fourier analysis of
that short snippet contains a broad band of wavelengths so
your measurement of the momentum will be very uncertain.

The maths of fourier-transforms means that there's a very simple
equation relating the uncertainty in the momentum to the uncertainty
in the position; it's called Heisenberg's Uncertainty Principle.

That's between position and momentum; they're called "complimetary
variables".  There are other pairs of complimetary measurements, like
Energy and Time, and they manifest the same uncertainty principle,
because of the same simple feature of the maths of fourier-transforms,
and the fact that particles move in probability-waves...

It's exactly the same maths as when you play a 1-millisec snippet
out of a bass-guitar note; the ear hears a click at a precise
time, but can't make out what the note was.

Regards,  Peter Billam

(P.S. hope I didn't make too many mistakes :-))

http://www.pjb.com.au      pj@pjb.com.au     (03) 6278 9410
"Follow the charge, not the particle."  --  Richard Feynman
 from The Theory of Positrons, Physical Review, 1949



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