Compute No > N the number of Bose-Einstein particles in the ground state from the formula 3 No 1- Tc where No is the number of Bose-Einstein particles in the He ground state, N is the number of particles at temperature T, and and T=3.1K for liquid He in the ground state (а) Т %3 3Т-/4, (b)T = Tc/2, (с) Т %3 Тc/4, (d) T = Tc/8 %3D to show that the Bose-Einstein ground state of He can contain a large number of states in distinction to Fermi-Dirac where the ground state because of the Pauli exclusion principle can only have two states (spin up and spin down)
Compute No > N the number of Bose-Einstein particles in the ground state from the formula 3 No 1- Tc where No is the number of Bose-Einstein particles in the He ground state, N is the number of particles at temperature T, and and T=3.1K for liquid He in the ground state (а) Т %3 3Т-/4, (b)T = Tc/2, (с) Т %3 Тc/4, (d) T = Tc/8 %3D to show that the Bose-Einstein ground state of He can contain a large number of states in distinction to Fermi-Dirac where the ground state because of the Pauli exclusion principle can only have two states (spin up and spin down)
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Transcribed Image Text:Compute No > N the number of Bose-Einstein particles in the ground state
from the formula
3
No
1 -
Tc
N
where No is the number of Bose-Einstein particles in the "He ground state, N
is the number of particles at temperature T, and and T.=3.1K for liquid He
in the ground state
(а) Т %3D 37./4,
(b)Т — Т./2,
(c) Т %3 Тc/4,
(d) Т — Тc/8
to show that the Bose-Einstein ground state of He can contain a large
number of states in distinction to Fermi-Dirac where the ground state
because of the Pauli exclusion principle can only have two states (spin up
and spin down)
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