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Canonical partition function for an ultrarelativistic gas in a power-law trap
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Past exam of the mathematics course of the University of Cambridge
/
2024
/
ii
/
Paper 1
/
36B
/
c
/
i
/
Solution
Created
2026-09-24
Updated
2026-09-25
View more
With
r
=
∣
x
∣
,
set
r
=
V
1/3
(
k
B
T
)
1/
(
2
n
)
u
.
(1)
Then
∫
e
−
β
U
(
x
)
d
3
x
=
4
πV
(
k
B
T
)
3/
(
2
n
)
I
n
.
(2)
Part (
b
) gives
Z
1
=
π
(
ℏ
c
)
3
4
V
(
k
B
T
)
3
+
3/
(
2
n
)
I
n
.
(3)
For
N
identical classical non-interacting particles,
Z
N
=
N
!
Z
1
N
.
(4)
Using
lo
g
N
!
=
N
lo
g
N
−
N
+
o
(
N
)
,
F
=
−
N
k
B
T
[
lo
g
V
+
A
lo
g
(
k
B
T
)
+
lo
g
I
n
+
B
]
+
o
(
N
)
,
(5)
where
A
=
3
+
2
n
3
,
B
=
1
+
lo
g
(
π
N
(
ℏ
c
)
3
4
)
.
(6)
This is the
canonical partition function for an ultrarelativistic gas in a power-law trap
.
Total
articles
:
1