In the approximation A « 1, Fermi-Dirac and Bose-Einstein statistics both tend to Maxwell-Boltzmann statistics: 1 • eu/kT .e=. -e/kT (6 - u) exp kT

icon
Related questions
Question
100%

Explain the following solution to the problem

womos
Jn clarical mechawics
So the probakectity of
farticles is nglig ible and thus
heated as distingusishab le .
a cell untaining tuo r mane
ngligible
(oceu potime 1)
1 ) The pautily
camot be heated as diting wihable ,we theu une
when
vcu
Index
quantiur stati,ties.
at hower energies
FD
-3
- 2
MB
e
So BE and FD will an tend to Me.
when
Hightemperature and las
ぐ。
Condition.
when
TくY
strongly adogerarate
TくY
di «1
Transcribed Image Text:womos Jn clarical mechawics So the probakectity of farticles is nglig ible and thus heated as distingusishab le . a cell untaining tuo r mane ngligible (oceu potime 1) 1 ) The pautily camot be heated as diting wihable ,we theu une when vcu Index quantiur stati,ties. at hower energies FD -3 - 2 MB e So BE and FD will an tend to Me. when Hightemperature and las ぐ。 Condition. when TくY strongly adogerarate TくY di «1
In the approximation A < 1, Fermi-Dirac and Bose-Einstein statistics
both tend to Maxwell-Boltzmann statistics:
1
+ e4/kT . e-e/kT.
(€ — м)
exp
土1
kT
Transcribed Image Text:In the approximation A < 1, Fermi-Dirac and Bose-Einstein statistics both tend to Maxwell-Boltzmann statistics: 1 + e4/kT . e-e/kT. (€ — м) exp 土1 kT
Expert Solution
steps

Step by step

Solved in 2 steps with 1 images

Blurred answer