Hello Harry,

You asked --
"So, the measuring instrument itself will produce energy, if it is used
to precisely measure the energy of a particle?"

Probably not.
But maybe there are subtleties that obey the 2nd Law of Thermodynamics,
but allow for some counterintuitive effects.  For example, refer to --

"Concentrating Energy by Measurement"
http://arxiv.org/abs/1012.5868

-- LP

Harry Veeder wrote:
> On Fri, Aug 17, 2012 at 8:57 PM,  <[email protected]> wrote:
>> In reply to  [email protected]'s message of Fri, 17 Aug 2012
>> 13:11:31
>> -0400 (EDT):
>> Hi,
>> [snip]
>>>Pardon for this very late postscript, time is hard to find.
>>>
>>>I believe you assume a wave function totally confined in all
>>> 3-dimensions.
>>> This is probably not what was intended.  It is easy to find papers
>>>describing crystal/lattice channel conduction of much higher energy
>>>particles (electrons, protons, ...). These are extended states - only
>>>confined in one or two dimensions.  High energy particles do not
>>>necessarily break the lattice structure.
>>>
>>>-- LP
>>
>> What I meant to do was calculate the momentum (assuming a kinetic energy
>> of
>> 0.782 MeV for the proton), and divide it into h-bar/2. However it
>> appears I got
>> something slightly wrong the first time around. The value I get now is
>> 2.57 fm
>> for a proton, and 0.93 fm for the deuteron.
>>
>> However I don't really stand behind the entire concept. I don't think
>> the energy
>> of particles magically increases when they are confined. I do think the
>> measurement uncertainty increases, but that's not the same thing as
>> their actual
>> energy. Instead, I see it as a limitation on our ability to measure, not
>> a
>> change in the actual properties of the particle itself.
>> IOW the restriction applies to us, not to the particles.
>> Regards,
>>
>> Robin van Spaandonk
>>
>> http://rvanspaa.freehostia.com/project.html
>>
>
> So, the measuring instrument itself will produce energy, if it is used
> to precisely measure the energy of a particle?
>
>
> Harry
>
>
>


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