On 02/08/2010 01:07 PM, Jones Beene wrote:
> -----Original Message----- From: Stephen A. Lawrence
> 
> Jones Beene wrote:
> 
> 
> 
>> I have lost the citation from a few weeks ago that claimed that
>> below a threshold of about 10 nm, the expected blackbody frequency is
>> upshifted for nanostructures, in general.
> 
>> SAL: If I understand you, and if this is true, then it's a
>> violation of the second law of thermodynamics.
> 
> No, not if other parts of the structure compensate, so that the net 
> energy is unchanged.

Your description makes this sound like a local surface phenomenon.  In
that case, I can coat the whole thing with identical nanoparticles, and
the argument that other parts of the structure will somehow compensate
is nulled out.

I suspect the answer's actually somewhat simpler:  Small particles are
"invisible" to wavelengths which are on the order of the particle size
or longer.  Consequently, nanostructures don't just cease to radiate at
long wavelengths -- they also become transparent to those wavelengths.

And that's all that's needed to avoid a second law violation.


> 
> IOW sub-radiance compensates for super-radiance so that net energy
> is conserved. This what Brian Ahern calls energy "localization". It
> is usually a surface effect, and that is due to nanostructure.
> 
> This all goes back to simulations done by Fermi, Pasta and Ulam on
> one of the first supercomputers at LANL. According to Brian, they
> simulated a one-dimensional array of masses connected by ideal
> springs obeying Hooke's Law. They gave the system x-amount of
> vibrational energy and then followed oscillators over time. The
> simulation showed that all of the masses got the same amount of
> vibrational energy. This was important as it verified one of the most
> basic tenets of statistical Thermodynamics. However, this is NOT the
> end of story, and they quickly found exceptions to the rule.

I'm not going to pretend I can follow the reasoning here.  Sorry...


> Ulam changed the equation from F = -k1X  to F = -k1x + k2X*2.  He
> kept the constant k2 small so that he was adding only a small
> nonlinear component.  Surprisingly, even a small amount of
> nonlinearity caused the energy to become highly localized. A small
> number of the masses went into permanent large amplitude oscillations
> and the remaining masses became 'vibrationally cold'. Note: there is
> no violation of CoE – at least not until abnormally large vibrations
> are able to cause another reaction – such as LENR (possibly).
> 
> Later all of this was picked up in the context of LENR by Preperata
> and has been called DPSR = Dicke-Preparata Super-radiance. Robert
> Dicke is the original genius behind it all, prior to LENR. Here is an
> earlier posting on vortex (which you commented on, so don't say you
> never heard of it :)
> 
> _http://www.mail-archive.com/[email protected]/msg22621.html_
> 
> There's another argument (from Brian): 

The text you quote here is very slightly paraphrased version of what I
said in the post to which you're responding, up to and including the
placement of the parentheses.  Since I typed that in off the top of my
head, as a paraphrase of something I'd said previously on one of my web
pages (which was also off the top of my head, quoting nobody else) I
find it surprising to read that the following text originated with Brian
Ahern.  Seems like a remarkable coincidence.

> When two objects with
> different surface characteristics are placed next to each other in a
> uniformly hot oven and a dichroic filter is placed between them, if
> one radiates more strongly at the filter's peak reflection frequency
> than the other, their relative temperatures will change.  (The one
> which radiates more strongly at the mirror's reflection frequency
> will "see" more radiation coming in than the other object, and so
> will get warmer.)

Now the next sentence, which seems to have been appended to my words, is
not from me, and in fact I don't understand it.

> You can analogize that to a single layered material
> with a surface that has greater vibrational mobility.


> But alas, I still have not found the paper in question, but am still 
> looking. Here is one that is close:
> 
> _http://www.iop.org/EJ/abstract/0953-8984/15/7/308_
> 
> Jones
> 

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