The integral ∫ 0 ∞ x 4 + 1 lo g 2 ( x ) d x converges to the value d a π b c , where a , b , c and d are positive integers with a and d being coprime positive integers and c , square-free. Calculate a + b + c + d .
Bonus: Calculate ∫ 0 ∞ x 4 + 1 lo g ( x ) d x . Notation: lo g 2 ( x ) = ( lo g ( x ) ) 2 .
Remark: You may want to use that for n ∈ N ≥ 2 , ∫ 0 ∞ x n + 1 d x = sin ( π / n ) π / n .
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Consider the contour C ⊂ C consisting of the upper-half disk of radius R > 1 minus an upper-half disk of radius r < 1 , as shown in the following picture.
(If this can be scaled, please tell me in a comment).
Let f : C → C , z ↦ z 4 + 1 lo g 2 ( z ) , where lo g : C → C , z ↦ lo g ∣ z ∣ + i ⋅ ar g ( z ) , where − 2 π < ar g ( z ) ≤ 2 3 π denotes the argument of z . We observe that ∮ C f ( z ) d z = ∫ r R f ( x ) d x + ∫ C R f ( z ) d z + ∫ − R − r f ( z ) d z + ∫ C r f ( z ) d z , where C R , C r denote the parts of the contour over the circles with radius R , r respectively. We will first show that both ∫ C R f ( z ) d z and ∫ C r f ( z ) d z tend to 0 as R → ∞ , r → 0 . First, observe that by the triangle inequality, ∣ z 4 + 1 ∣ ≥ ∣ ∣ ∣ z 4 ∣ − ∣ 1 ∣ ∣ ∣ . Now it follows that ∣ ∣ ∣ ∣ ∫ C R f ( z ) d z ∣ ∣ ∣ ∣ ≤ π R ⋅ z ∈ C R max ∣ ∣ ∣ ∣ z 4 + 1 lo g 2 ( z ) ∣ ∣ ∣ ∣ ≤ π R ⋅ z ∈ C R max ∣ ∣ ∣ ∣ R 4 − 1 lo g 2 ( z ) ∣ ∣ ∣ ∣ ≤ π R ⋅ z ∈ C R max R 4 − 1 ∣ lo g 2 ∣ R ∣ ∣ + ∣ i ⋅ ar g ( z ) ∣ < R 4 − 1 π R lo g 2 ( R ) + 2 π 2 R R → ∞ 0 . In a similar fashion, it follows that ∣ ∣ ∣ ∫ C r f ( z ) d z ∣ ∣ ∣ r → 0 0 by using l'Hôpital's rule at the end.
Now, we will use the Residue Theorem on the contour integral to observe that
∮
C
f
(
z
)
d
z
=
2
π
i
⋅
[
Res
z
=
e
π
i
/
4
f
(
z
)
+
Res
z
=
e
3
π
i
/
4
f
(
z
)
]
.
By the lemma which will be proven down below, for
a
∈
{
e
π
i
k
/
4
∣
k
∈
{
1
,
3
,
5
,
7
}
}
:
Res
z
=
a
z
4
+
1
lo
g
2
(
z
)
=
4
a
3
lo
g
2
(
a
)
.
Using this lemma, we obtain
∮
C
f
(
z
)
d
z
=
2
π
i
⋅
[
4
e
3
π
i
/
4
(
π
i
/
4
)
2
+
4
e
π
i
/
4
(
3
π
i
/
4
)
2
]
.
After doing some algebraic calculations, we see that
∮
C
f
(
z
)
d
z
=
−
3
2
5
π
3
2
−
i
⋅
8
π
3
2
.
Letting
R
→
∞
,
r
→
0
, we get the equation
∮
C
f
(
z
)
d
z
=
∫
0
∞
f
(
x
)
d
x
+
∫
−
∞
0
f
(
z
)
d
z
.
We will now simplify the latter integral. Note that
∫
−
∞
0
z
4
+
1
lo
g
2
(
z
)
d
z
=
∫
−
∞
0
z
4
+
1
(
lo
g
∣
z
∣
+
π
i
)
2
d
z
=
∫
0
∞
x
4
+
1
lo
g
2
∣
x
∣
+
2
π
i
lo
g
∣
x
∣
−
π
2
d
x
.
By the remark in the problem,
∫
0
∞
x
4
+
1
π
2
d
x
=
4
π
3
2
.
Using all information gathered so far, we obtain that
−
3
2
5
π
3
2
−
i
⋅
8
π
3
2
=
∮
C
f
(
z
)
d
z
=
2
∫
0
∞
x
4
+
1
lo
g
2
(
x
)
d
x
+
2
π
i
⋅
∫
0
∞
x
4
+
1
lo
g
(
x
)
d
x
−
4
π
3
2
.
As the integrands are real-valued, we conclude that
∫
0
∞
x
4
+
1
lo
g
2
(
x
)
d
x
=
6
4
3
π
3
2
a
n
d
∫
0
∞
x
4
+
1
lo
g
(
x
)
d
x
=
−
1
6
π
2
2
.
Lemma:
For
a
∈
{
e
π
i
k
/
4
∣
k
∈
{
1
,
3
,
5
,
7
}
}
,
Res
z
=
a
z
4
+
1
lo
g
2
(
z
)
=
4
a
3
lo
g
2
(
a
)
.
Proof. By definition, Res z = a z 4 + 1 lo g 2 ( z ) = lim z → a z 4 + 1 ( z − a ) lo g 2 ( z ) . By l'Hôpital's rule, Res z = a z 4 + 1 lo g 2 ( z ) = z → a lim 4 z 3 lo g 2 ( z ) + 2 ( z − a ) lo g ( z ) / z = 4 a 3 lo g 2 ( a ) . ■
How is l'Hospital's rule applicable here? The expression doesn't assume an indeterminate form under the said limit.
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It is not necessary. The integral along C R is O ( R − 3 ln 2 R ) as R → ∞ , while the integral along C r is O ( r ln 2 r ) as r → 0 , which is all we need to make both tend to 0 in the relevant limits.
If your question was about the limit in the lemma, z = a has to be a simple pole, which means that z 4 + 1 = def 0 . I have clarified this now in the answer.
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The change of variable u = x 4 gives ∫ 0 ∞ 1 + x 4 ln 2 x d x = 6 4 1 ∫ 0 ∞ 1 + u u − 4 3 ln 2 u d u = 6 4 1 d u 2 d 2 B ( 1 − u , u ) ∣ ∣ ∣ u = 4 1 = 6 4 1 d u 2 d 2 ( π c o s e c π u ) ∣ ∣ ∣ u = 4 1 = 6 4 1 π 3 c o s e c 2 4 1 π ( 2 cot 2 4 1 π + 1 ) = 3 2 3 π 3 2 making the answer 3 + 3 + 2 + 6 4 = 7 2 .
We can obtain the integral with a single logarithm by differentiating the Beta function once instead of twice, obtaining ∫ 0 ∞ 1 + x 4 ln x d x = 1 6 1 d u d ( π c o s e c π u ) ∣ ∣ ∣ u = 4 1 = − 1 6 π 2 2