Quantum Gravity 149.1: The Bose-Einstein, Fermi-Dirac, and Maxwell-Boltzmann Statistics



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Topic: Science > Physics
User: "OsherD"
Date: 01 Jun 2007 06:39:50 PM
Object: Quantum Gravity 149.1: The Bose-Einstein, Fermi-Dirac, and Maxwell-Boltzmann Statistics

From Osher Doctorow

Some people are still under the impression that large areas of physics
escape either exponention functions or Probable Causation/Influence or
ratios of exponential functions. From what we have seen in recent
posts in this thread, only essentially statistically independent
events can generate such "other" scenarios
For examples of the ratio type of exponential functions, look at
Hyperphysics' "The energy distribution function(s)" on the internet,
including "Bose-Einstein" (boson) and "Fermi-Dirac" (fermion)
statistics, while the classical Maxwell-Boltzmann statistics are just
exponential. All involve basically exponential decay or contraction
rather than expansion or growth.
The probability density functions (pdfs), which is roughly speaking
probabilities of various energy levels E, are:
1) f(E) = 1/[A exp(E/kT)] (Maxwell-Boltzmann)
2 f(E) = 1/[A exp(E/kT) - 1] (Bose-Einstein)
3) f(E) = 1/[A exp(E/kT) + 1] (Fermi-Dirac)
where for example the Fermi-Dirac case (3) can be written:
4) f(E) = 1/[exp{(E - E_F)/kT} + 1]
with E_F the Fermi energy.
Osher Doctorow
.

User: "kunzmilan"

Title: Re: Quantum Gravity 149.1: The Bose-Einstein, Fermi-Dirac, and Maxwell-Boltzmann Statistics 02 Jun 2007 04:36:15 AM
On Jun 2, 1:39 am, OsherD <mdocto...@comcast.net> wrote:

From Osher Doctorow


Some people are still under the impression that large areas of physics
escape either exponention functions or Probable Causation/Influence or
ratios of exponential functions. From what we have seen in recent
posts in this thread, only essentially statistically independent
events can generate such "other" scenarios

For examples of the ratio type of exponential functions, look at
Hyperphysics' "The energy distribution function(s)" on the internet,
including "Bose-Einstein" (boson) and "Fermi-Dirac" (fermion)
statistics, while the classical Maxwell-Boltzmann statistics are just
exponential. All involve basically exponential decay or contraction
rather than expansion or growth.

The probability density functions (pdfs), which is roughly speaking
probabilities of various energy levels E, are:

1) f(E) = 1/[A exp(E/kT)] (Maxwell-Boltzmann)
2 f(E) = 1/[A exp(E/kT) - 1] (Bose-Einstein)
3) f(E) = 1/[A exp(E/kT) + 1] (Fermi-Dirac)

where for example the Fermi-Dirac case (3) can be written:

4) f(E) = 1/[exp{(E - E_F)/kT} + 1]

with E_F the Fermi energy.

Osher Doctorow

I showed long ago (Physics Letters A, vol. 135, p. 421-424, 1989) that
all three statistics have one generating function. They depend on
aspects which can be and are observed. Maxwell-Boltzmann statistics is
just the largest orbit, Bose-Einstein statistics is just the
difference according one observed vector going out the black body,
Fermi-Dirac statistics is the difference.
kunzmilan
.


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