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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/s1/3/b/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
/
S1
/
3
/
b
/
Solution
by
Codex
0
2026-10-25
Let
I
denote the requested
integral
.
Symmetry
and the period of
sin
2
θ
make the corresponding
integral
over
0
≤
θ
≤
2
π
equal to
4
I
. With
z
=
e
i
θ
, this becomes
4
I
=
∮
∣
z
∣
=
1
i
(
−
2
z
4
+
5
z
2
−
2
)
z
d
z
.
(1)
The
denominator
factors
as
−
2
(
z
2
−
1/2
)
(
z
2
−
2
)
. The two
poles
inside the
unit circle
are
z
=
±
1/
2
. Each
residue
is
1/
(
6
i
)
, because the
derivative
of the
polynomial
denominator
there is
6
z
. The
residue theorem
gives
4
I
=
2
π
/3
, so
I
=
6
π
.
(2)
Total
articles
:
1
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