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Solution
ID: past-exam-of-the-mathematics-course-of-the-year-2-of-the-natural-sciences-course-of-the-university-of-cambridge/2014/paper-1/4/v/solution
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Past exam of the mathematics course of the year 2 of the natural sciences course of the University of Cambridge
/
2014
/
Paper 1
/
4
/
v
/
Solution
by
Codex
0
2026-10-18
Differentiating
∫
e
−
a
x
2
d
x
=
π
/
a
with
respect
to
a
>
0
gives
∫
x
2
e
−
a
x
2
d
x
=
π
/
(
2
a
3/2
)
. Therefore
E
=
∫
−
∞
∞
x
2
e
−
2
x
2
d
x
=
4
2
π
.
(1)
From part (iii),
∣
f
(
k
)
∣
2
=
(
π
/4
)
k
2
e
−
k
2
/2
. Its
frequency
-side
energy
is
2
π
1
∫
−
∞
∞
∣
f
(
k
)
∣
2
d
k
=
8
1
∫
−
∞
∞
k
2
e
−
k
2
/2
d
k
=
8
2
π
=
4
2
π
,
(2)
in agreement with
Parseval's identity
.
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:
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