(i) Marall. Boltzmann No Configuration 1 2. 3 4 S 6 7 8 9 1 2 3 + 5 6 2 () Fermi-Dirac & () Boson Bose- Ginstein: Nader Canligation No Configuration AG A A B 8 E AA A A E 28 A AB B A A 8 AA A A સુદ In distinguishable 28 22 AR A B A B A JE AA A A A Energy system A SAFFAR 28 Indstinguishable We know fermion follow exclusion principle.. 38 Energy 48 32 48 28 4E SE SE Energy system 22 48 62 38 48 SE 38 48 SE Calculate the average energy of the system as a temperature function for the three statistics above.
(i) Marall. Boltzmann No Configuration 1 2. 3 4 S 6 7 8 9 1 2 3 + 5 6 2 () Fermi-Dirac & () Boson Bose- Ginstein: Nader Canligation No Configuration AG A A B 8 E AA A A E 28 A AB B A A 8 AA A A સુદ In distinguishable 28 22 AR A B A B A JE AA A A A Energy system A SAFFAR 28 Indstinguishable We know fermion follow exclusion principle.. 38 Energy 48 32 48 28 4E SE SE Energy system 22 48 62 38 48 SE 38 48 SE Calculate the average energy of the system as a temperature function for the three statistics above.
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Transcribed Image Text:View a system of two particles that do not interact with each other, where each particle
can occupy three possible states, each with energy &, 2ɛ, 3E
(i) Marwell-Boltzmann:
Na. Configuration
1
2
3
4
S
6
7
2
9
Nader Conligation
1
2
2
+
1
2
5
6
(1) Fermi-Dirac
3
No. Configuration
E
AG
A
A
B
B
AA
A
A
Distinguishable
28
E
AB
(6) Boson: Base- Ginstein: Indistinguishable
င်
A
A
B
A
A
8
28
AA
A
A
38
A
2
A
AB
B
A
CO
B
A
JE
AA
A
A
Energy system
A
A
wwwww
Indistinguishable
We know formion follow exclusion principle.
28
38
Smarty tem
28
32
38
4E
SE
SE
Energy system
22
48
68
38
48
SE
38
4€
SE
Calculate the average energy of the system as a temperature function for the three
statistics above.
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