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Solution
ID: past-exam-of-the-short-options-paper-shared-by-prelims-and-parts-a-and-b-of-the-physics-course-of-the-university-of-oxford/2015/s16/3/4/solution
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Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
/
2015
/
S16
/
3
/
4
/
Solution
by
Codex
0
2026-10-25
The supplied
confinement
criterion alone fixes
a
product, not
a
unique current or
machine
size
. Choose
a
representative
ion
density
n
i
=
1
0
20
m
−
3
. Then
τ
≳
n
i
1
0
20
s
≃
1
s
.
(1)
For
n
i
=
1
0
19
to
1
0
21
m
−
3
, the same criterion gives
τ
≳
10
to
0.1
s
. These are illustrative
density
choices
, not additional source
data
.
For
a
current estimate, assume
a
large-
aspect-ratio
circular
tokamak
with major
radius
R
0
=
3
m
, minor
radius
a
=
1
m
, toroidal
field
B
ϕ
=
5
T
and edge
tokamak safety factor
q
s
≃
3
. The geometrical winding relation and
Ampère's law
give
q
s
≃
R
0
B
θ
a
B
ϕ
,
B
θ
(
a
)
≃
2
πa
μ
0
I
p
,
I
p
≃
μ
0
R
0
q
s
2
π
a
2
B
ϕ
.
(2)
For the stated assumptions,
I
p
≃
2.8
×
1
0
6
A
,
(3)
so toroidal plasma currents of order megaamperes are
a
natural scale.
As
a
consistency
check at
T
∼
1
0
8
K
, quasineutral singly charged heavy
hydrogen
has total
thermal pressure
p
≃
2
n
i
k
B
T
≃
2.8
×
1
0
5
Pa
. With
5
T
,
2
μ
0
p
/
B
2
≃
0.028
, so the assumed
magnetic pressure
exceeds the
thermal pressure
. The particular current depends on
geometry
and
field
-line
pitch
; it cannot be inferred from the
confinement
product alone.
Total
articles
:
1
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