∫ 0 1 { 1 x } n d x = ∑ k = 1 ∞ ζ ( k + 1 ) − 1 ( n + k k ) \large \displaystyle\int _{ 0 }^{ 1 }{ \left \{ \dfrac { 1 }{ x } \right\} ^{ n } } \, dx=\sum _{ k=1 }^{ \infty }{ \frac { \zeta (k+1)-1 }{ \binom{n+k}{k} } } ∫ 0 1 { x 1 } n d x = k = 1 ∑ ∞ ( k n + k ) ζ ( k + 1 ) − 1
Prove the equation above for positive integers n n n .
This is actually a result from a more generalized form ∫ 0 1 { 1 x } k x n d x = k ! ( n + 1 ) ! ∑ i = 1 ∞ ( n + i ) ! ( k + i ) ! ( ζ ( n + i + 1 ) − 1 ) . \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \frac { 1 }{ x } \right\} ^{ k }{ x }^{ n }dx } =\frac { k! }{ (n+1)! } \sum _{ i=1 }^{ \infty }{ \frac { (n+i)! }{ (k+i)! } \big(\zeta (n+i+1)-1\big). } ∫ 0 1 { x 1 } k x n d x = ( n + 1 )! k ! i = 1 ∑ ∞ ( k + i )! ( n + i )! ( ζ ( n + i + 1 ) − 1 ) .
Let's denote the above as
∫ 0 1 { 1 x } k x n d x = f ( k , n ) = ∫ 1 ∞ { t } k t n + 2 d t . \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \frac { 1 }{ x } \right\} ^{ k }{ x }^{ n }\, dx } =f(k,n)=\displaystyle\int _{ 1 }^{ \infty }{ \frac { \{ t\} ^{ k } }{ { t }^{ n+2 } } dt }. ∫ 0 1 { x 1 } k x n d x = f ( k , n ) = ∫ 1 ∞ t n + 2 { t } k d t .
Converting this to a sum of integrals, we have
∑ i = 1 ∞ ∫ i i + 1 { t } k t n + 2 d t = ∑ i = 1 ∞ ( t − i ) k t n + 2 . \displaystyle\sum _{ i=1 }^{ \infty }{ \displaystyle\int _{ i }^{ i+1 }{ \frac { \{ t\} ^{ k } }{ { t }^{ n+2 } } }\, dt } =\displaystyle\sum _{ i=1 }^{ \infty }{ \frac { (t-i)^{ k } }{ { t }^{ n+2 } } }. i = 1 ∑ ∞ ∫ i i + 1 t n + 2 { t } k d t = i = 1 ∑ ∞ t n + 2 ( t − i ) k .
U U U -substituting by letting u = t − i , u=t-i, u = t − i , we get
∑ i = 1 ∞ ∫ 0 1 u k ( i + u ) n + 2 d u = ∫ 0 1 u k ( ∑ i = 1 ∞ 1 ( i + u ) n + 2 ) d y . ( 1 ) \sum _{ i=1 }^{ \infty }{ \displaystyle\int _{ 0 }^{ 1 }{ \frac { { u }^{ k } }{ (i+u)^{ n+2 } } } }\, du=\int _{ 0 }^{ 1 }{ { u }^{ k }\left( \sum _{ i=1 }^{ \infty }{ \frac { 1 }{ (i+u)^{ n+2 } } } \right) dy }. \qquad (1) i = 1 ∑ ∞ ∫ 0 1 ( i + u ) n + 2 u k d u = ∫ 0 1 u k ( i = 1 ∑ ∞ ( i + u ) n + 2 1 ) d y . ( 1 )
Then since 1 ( i + u ) n + 2 = 1 ( n + 1 ) ! ∫ 0 ∞ e − ( i + u ) u y n + 1 d y , \frac { 1 }{ (i+u)^{ n+2 } } =\frac { 1 }{ (n+1)! } \displaystyle\int _{ 0 }^{ \infty }{ { e }^{ -(i+u)u }{ y }^{ n+1 } } dy, ( i + u ) n + 2 1 = ( n + 1 )! 1 ∫ 0 ∞ e − ( i + u ) u y n + 1 d y , putting this in gives
∑ i = 1 ∞ 1 ( i + u ) n + 2 = 1 ( n + 1 ) ! ∑ i = 1 ∞ ∫ 0 ∞ e − ( i + u ) y y n + 1 d y = 1 ( n + 1 ) ! ∫ 0 ∞ y n + 1 e − u y ( ∑ i = 1 ∞ e − i y ) d y = 1 ( n + 1 ) ! ∫ 0 ∞ y n + 1 e − u y e y − 1 d y . ( 2 ) \begin{aligned}
\sum _{ i=1 }^{ \infty }{ \frac { 1 }{ (i+u)^{ n+2 } } }
&=\frac { 1 }{ (n+1)! } \sum _{ i=1 }^{ \infty }{ \int _{ 0 }^{ \infty }{ { e }^{ -(i+u)y }{ y }^{ n+1 }\, dy } } \\
&=\frac { 1 }{ (n+1)! } \int _{ 0 }^{ \infty }{ { y }^{ n+1 } } { e }^{ -uy }\left(\sum _{ i=1 }^{ \infty }{ { e }^{ -iy } } \right)\, dy\\
&=\frac { 1 }{ (n+1)! } \int _{ 0 }^{ \infty }{ \frac { { y }^{ n+1 }{ e }^{ -uy } }{ { e }^{ y }-1 } dy }.\qquad (2)
\end{aligned} i = 1 ∑ ∞ ( i + u ) n + 2 1 = ( n + 1 )! 1 i = 1 ∑ ∞ ∫ 0 ∞ e − ( i + u ) y y n + 1 d y = ( n + 1 )! 1 ∫ 0 ∞ y n + 1 e − u y ( i = 1 ∑ ∞ e − i y ) d y = ( n + 1 )! 1 ∫ 0 ∞ e y − 1 y n + 1 e − u y d y . ( 2 )
Combining (1) and (2), we get
1 ( n + 1 ) ! ∫ 0 1 u k ( ∫ 0 ∞ y n + 1 e − u y e y − 1 d y ) d u = 1 ( n + 1 ) ! ∫ 0 ∞ y n + 1 e y − 1 ( ∫ 0 1 u k e − u y d u ) d y . \frac { 1 }{ (n+1)! } \int _{ 0 }^{ 1 }{ { u }^{ k }\left( \int _{ 0 }^{ \infty }{ \frac { { y }^{ n+1 }{ e }^{ -uy } }{ { e }^{ y }-1 } dy } \right) \, du } =\frac { 1 }{ (n+1)! } \int _{ 0 }^{ \infty }{ \frac { { y }^{ n+1 } }{ { e }^{ y }-1 } } \left( \int _{ 0 }^{ 1 }{ { u }^{ k }{ e }^{ -uy }\, du } \right)\, dy. ( n + 1 )! 1 ∫ 0 1 u k ( ∫ 0 ∞ e y − 1 y n + 1 e − u y d y ) d u = ( n + 1 )! 1 ∫ 0 ∞ e y − 1 y n + 1 ( ∫ 0 1 u k e − u y d u ) d y .
By IBP we can evaluate the inner integral as k ! e − y ∑ i = 1 ∞ y i − 1 ( k + i ) ! , k!{ e }^{ -y }\displaystyle\sum _{ i=1 }^{ \infty }{ \frac { { y }^{ i-1 } }{ (k+i)! } }, k ! e − y i = 1 ∑ ∞ ( k + i )! y i − 1 , so this simplifies to
1 ( n + 1 ) ! ∑ i = 1 ∞ k ! ( k + i ) ! ∫ 0 ∞ y n + i e − y e y − 1 d y . \frac { 1 }{ (n+1)! } \displaystyle\sum _{ i=1 }^{ \infty }{ \frac { k! }{ (k+i)! } } \displaystyle\int _{ 0 }^{ \infty }{ \frac { { y }^{ n+i }{ e }^{ -y } }{ { e }^{ y }-1 } dy }. ( n + 1 )! 1 i = 1 ∑ ∞ ( k + i )! k ! ∫ 0 ∞ e y − 1 y n + i e − y d y .
Evaluating that integral, we have
1 ( n + 1 ) ! ∑ i = 1 ∞ k ! ( k + i ) ! ∫ 0 ∞ y n + i e − y e y − 1 d y = ∫ 0 ∞ y n + i e − 2 y ∑ j = 0 ∞ e − j y d y = ∑ j = 0 ∞ ∫ 0 ∞ y n + i e − ( 2 + j ) y d y = ∑ j = 0 ∞ Γ ( n + i + 1 ) ( 2 + j ) n + i + 1 = ( n + i ) ! ( ζ ( n + i + 1 ) − 1 ) . \begin{aligned}
\frac { 1 }{ (n+1)! } \sum _{ i=1 }^{ \infty }{ \frac { k! }{ (k+i)! } } \int _{ 0 }^{ \infty }{ \frac { { y }^{ n+i }{ e }^{ -y } }{ { e }^{ y }-1 } \, dy }
&= \int _{ 0 }^{ \infty }{ { y }^{ n+i }{ e }^{ -2y }\sum _{ j=0 }^{ \infty }{ { e }^{ -jy } } dy } \\
&=\sum _{ j=0 }^{ \infty }{ \int _{ 0 }^{ \infty }{ { y }^{ n+i }{ e }^{ -(2+j)y }\, dy }} \\
&=\sum _{ j=0 }^{ \infty }{ \frac { \Gamma (n+i+1) }{ (2+j)^{ n+i+1 } } } =(n+i)! \big( \zeta (n+i+1)-1 \big).
\end{aligned} ( n + 1 )! 1 i = 1 ∑ ∞ ( k + i )! k ! ∫ 0 ∞ e y − 1 y n + i e − y d y = ∫ 0 ∞ y n + i e − 2 y j = 0 ∑ ∞ e − j y d y = j = 0 ∑ ∞ ∫ 0 ∞ y n + i e − ( 2 + j ) y d y = j = 0 ∑ ∞ ( 2 + j ) n + i + 1 Γ ( n + i + 1 ) = ( n + i )! ( ζ ( n + i + 1 ) − 1 ) .
Hence,
∫ 0 1 { 1 x } k x n d x = k ! ( n + 1 ) ! ∑ i = 1 ∞ ( n + i ) ! ( k + i ) ! ( ζ ( n + i + 1 ) − 1 ) , \int _{ 0 }^{ 1 }{ \left\{ \frac { 1 }{ x } \right\} ^{ k }{ x }^{ n }dx } =\frac { k! }{ (n+1)! } \displaystyle\sum _{ i=1 }^{ \infty }{ \frac { (n+i)! }{ (k+i)! } (\zeta (n+i+1)-1) }, ∫ 0 1 { x 1 } k x n d x = ( n + 1 )! k ! i = 1 ∑ ∞ ( k + i )! ( n + i )! ( ζ ( n + i + 1 ) − 1 ) ,
and the result follows. □ _\square □
∫ 0 1 ∫ 0 1 { x y } k y a x b d x d y = 1 a − b + 2 ( 1 k − b + 1 + k ! ( a + 1 ) ! ∑ n = 1 ∞ ( a + n ) ! ( k + n ) ! ( ζ ( a + n + 1 ) − 1 ) ) \int _{ 0 }^{ 1 }{ \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \dfrac { x }{ y } \right\} ^{ k }\dfrac { { y }^{ a } }{ { x }^{ b } } \, dx \; dy } } =\dfrac { 1 }{ a-b+2 } \left( \dfrac { 1 }{ k-b+1 } +\dfrac { k! }{ (a+1)! } \sum _{ n=1 }^{ \infty }{ \frac { (a+n)! }{ (k+n)! } \Big( \zeta (a+n+1)-1 \Big) } \right) ∫ 0 1 ∫ 0 1 { y x } k x b y a d x d y = a − b + 2 1 ( k − b + 1 1 + ( a + 1 )! k ! n = 1 ∑ ∞ ( k + n )! ( a + n )! ( ζ ( a + n + 1 ) − 1 ) )
Prove the equation above with k k k being a real number ≥ 1 \ge1 ≥ 1 and a , b a,b a , b nonnegative integers such that a − b > − 2 a-b>-2 a − b > − 2 and k − b > − 1 k-b>-1 k − b > − 1 .
Rearranging the integral we get
∫ 0 1 1 x b ∫ 0 1 { x y } k y a d x d y . \int _{ 0 }^{ 1 }{ \frac { 1 }{ { x }^{ b } } \int _{ 0 }^{ 1 }{ \left\{ \frac { x }{ y } \right\} ^{ k }{ y }^{ a }\, dx\, dy } }. ∫ 0 1 x b 1 ∫ 0 1 { y x } k y a d x d y .
Then we let x y = u \frac { x }{ y } =u y x = u and the integral converts into
∫ 0 1 x a + 1 − b ( ∫ x ∞ { u } k u a + 2 d u ) d x . \int _{ 0 }^{ 1 }{ { x }^{ a+1-b } } \left( \int _{ x }^{ \infty }{ \frac { \{ u\} ^{ k } }{ { u }^{ a+2 } } du } \right) dx. ∫ 0 1 x a + 1 − b ( ∫ x ∞ u a + 2 { u } k d u ) d x .
Now we integrate by parts to get
∫ 0 1 x a + 1 − b ( ∫ x ∞ { u } k u a + 2 d u ) d x = ( x a + 2 − b a + 2 − b ∫ x ∞ { u } k u a + 2 d u ) ∣ x = 0 x = 1 + 1 a + 2 − b ∫ 0 1 x k − b d x = 1 a + 2 − b ∫ 1 ∞ { u } k u a + 2 d u + 1 ( a + 2 − b ) ( k − b + 1 ) . \begin{aligned}
\displaystyle\int _{ 0 }^{ 1 }{ { x }^{ a+1-b } } \left( \displaystyle\int _{ x }^{ \infty }{ \frac { \{ u\} ^{ k } }{ { u }^{ a+2 } } du } \right) dx
&=\left. \left( \frac { { x }^{ a+2-b } }{ a+2-b } \displaystyle\int _{ x }^{ \infty }{ \frac { \{ u\} ^{ k } }{ { u }^{ a+2 } } du } \right)\right|_{x=0}^{x=1} +\frac { 1 }{ a+2-b } \displaystyle\int _{ 0 }^{ 1 }{ { x }^{ k-b }dx } \\
&=\frac { 1 }{ a+2-b } \displaystyle\int _{ 1 }^{ \infty }{ \frac { \{ u\} ^{ k } }{ { u }^{ a+2 } } du } +\frac { 1 }{ (a+2-b)(k-b+1) }.
\end{aligned} ∫ 0 1 x a + 1 − b ( ∫ x ∞ u a + 2 { u } k d u ) d x = ( a + 2 − b x a + 2 − b ∫ x ∞ u a + 2 { u } k d u ) x = 0 x = 1 + a + 2 − b 1 ∫ 0 1 x k − b d x = a + 2 − b 1 ∫ 1 ∞ u a + 2 { u } k d u + ( a + 2 − b ) ( k − b + 1 ) 1 .
We evaluated that integral in the previous example.
Putting that in, we get
∫ 0 1 ∫ 0 1 { x y } k y a x b d x d y = 1 a − b + 2 ( 1 k − b + 1 + k ! ( a + 1 ) ! ∑ n = 1 ∞ ( a + n ) ! ( k + n ) ! ( ζ ( a + n + 1 ) − 1 ) ) . □ \int _{ 0 }^{ 1 }{ \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \frac { x }{ y } \right\} ^{ k }\frac { { y }^{ a } }{ x^{ b } } \, dx\, dy } } =\frac { 1 }{ a-b+2 } \left( \frac { 1 }{ k-b+1 } +\frac { k! }{ (a+1)! } \displaystyle\sum _{ n=1 }^{ \infty }{ \frac { (a+n)! }{ (k+n)! } \Big( \zeta (a+n+1)-1 \Big) } \right).\ _\square ∫ 0 1 ∫ 0 1 { y x } k x b y a d x d y = a − b + 2 1 ( k − b + 1 1 + ( a + 1 )! k ! n = 1 ∑ ∞ ( k + n )! ( a + n )! ( ζ ( a + n + 1 ) − 1 ) ) . □
Reveal the answer
∫ 0 1 { ( − 1 ) ⌊ 1 x ⌋ x } d x = A + B ln ( C π ) \large \int_0^1 \left \{ \dfrac{(-1)^{\big\lfloor \frac1x\big\rfloor }}{x}\right \} \, dx = A + B \ln \left( \dfrac C{\pi} \right) ∫ 0 1 ⎩ ⎨ ⎧ x ( − 1 ) ⌊ x 1 ⌋ ⎭ ⎬ ⎫ d x = A + B ln ( π C )
The equation above holds true for positive integers A , B , A,B, A , B , and C C C . Find A + B + C A+B+C A + B + C .
Notation : { ⋅ } \{ \cdot \} { ⋅ } denotes the fractional part function .
This is a part of "Who's up to the challenge?"
The correct answer is: 4
Reveal the answer
∫ 0 1 ∫ 0 1 { x y } 3 { y x } 3 d x d y = A − π B C − π B + 2 D − ζ ( E ) \large \int_0^1 \int _{ 0 }^{ 1 }{ { \left\{ \dfrac { x }{ y } \right\} }^{ 3 }{ \left\{ \dfrac { y }{ x } \right\} }^{ 3 } \, dx \; dy } =A-\dfrac { { \pi }^{ B } }{ C } -\dfrac { { \pi }^{ B+2 } }{ D } -\zeta \left( E \right) ∫ 0 1 ∫ 0 1 { y x } 3 { x y } 3 d x d y = A − C π B − D π B + 2 − ζ ( E )
The equation above holds true for positive integers A , B , C , D A,B,C,D A , B , C , D and E E E . Find A + B + C + D + E A+B+C+D+E A + B + C + D + E .
Notations :
The correct answer is: 390
Reveal the answer
∫ 0 1 { 1 x } x 1 − x d x = A γ + B \large \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \dfrac { 1 }{ x } \right\} \dfrac { x }{ 1-x } \, dx=A\gamma } +B ∫ 0 1 { x 1 } 1 − x x d x = A γ + B
The equation above holds true for integers A A A and B B B . Find A + B A+B A + B .
Notations :
The correct answer is: 1
Reveal the answer
∫ 0 1 ∫ 0 1 x { 1 1 − x y } d x d y = A − ζ ( B ) C \large \displaystyle\int _{ 0 }^{ 1 }{ \displaystyle\int _{ 0 }^{ 1 }{ x\left\{ \dfrac { 1 }{ 1-xy } \right\} \, dx\; dy } } =A-\dfrac { \zeta (B) }{ C } ∫ 0 1 ∫ 0 1 x { 1 − x y 1 } d x d y = A − C ζ ( B )
If the equation above holds true for positive integers A , B A,B A , B and C C C , find A × B × C A\times B \times C A × B × C .
Notations :
This is a part of "Who's up to the challenge?"
The correct answer is: 4
Reveal the answer
∫ 0 1 { 1 x 1729 − 1 ( 1 − x ) 1729 } x 6 ( 1 − x ) 6 d x = a b \large \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \dfrac { 1 }{ { x }^{ 1729 } } -\dfrac { 1 }{ (1-x)^{ 1729 } } \right\} { x }^{ 6 }(1-x)^{ 6 } \, dx } =\dfrac { a}{ b } ∫ 0 1 { x 1729 1 − ( 1 − x ) 1729 1 } x 6 ( 1 − x ) 6 d x = b a
The equation above holds true for coprime positive integers a a a and b b b . Find a + b a+b a + b .
Bonus : Generalize it.
Notation : { ⋅ } \{ \cdot \} { ⋅ } denotes the fractional part function .
This problem is a part of "Who's up to the challenge?"
The correct answer is: 24025
Reveal the answer
∫ 0 1 { 1 x } 3 d x = − H U − M γ + M 1 U 1 ln ( S π ) − B ln A \int _{ 0 }^{ 1 }{ \left\{ \frac { 1 }{ x } \right\} ^{ 3 } } dx=-\frac { H }{ U } -Mγ+\frac { { M }_{ 1 } }{ U_1 } \ln { (Sπ) } -B\ln { A } ∫ 0 1 { x 1 } 3 d x = − U H − M γ + U 1 M 1 ln ( S π ) − B ln A
In the equation above, A A A is the Glaisher–Kinkelin constant, all other variables are positive integers, and all the fractions mentioned are coprime.
Find H + U + M + M 1 + U 1 + S + B . H+U+M+{ M }_{ 1 }+{ U }_{ 1 }+S+B. H + U + M + M 1 + U 1 + S + B .
Note : { x } \{x\} { x } denotes the fractional part of x . x. x .
This is a part of "Who's up to the challenge?"
The correct answer is: 17
Evaluate ∫ 0 1 { n x n } d x \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \frac { n }{ \sqrt [ n ]{ x } } \right\}\, dx } ∫ 0 1 { n x n } d x for n ≥ 2. n\ge2. n ≥ 2.
We make the substitution x = n n y n , x=\dfrac { { n }^{ n } }{ { y }^{ n } }, x = y n n n , which will convert the integral to
n n + 1 ∫ n ∞ { y } y n + 1 d y = n n + 1 ∑ k = n ∞ ∫ k k + 1 y − k y n + 1 d y = n n + 1 n − 1 ∑ k = n ∞ ( 1 k n − 1 − 1 ( k + 1 ) n − 1 ) + n n ∑ k = n ∞ k ( 1 ( k + 1 ) n − 1 k n ) = n 2 n − 1 + n n ∑ k = n ∞ ( 1 ( k + 1 ) n − 1 − 1 k n − 1 − 1 ( k + 1 ) n ) = n n − 1 − n n ( ζ ( n ) − ∑ k = 1 n 1 k n ) . □ \begin{aligned}
{ n }^{ n+1 }\displaystyle\int _{ n }^{ \infty }{ \frac { \{ y\} }{ { y }^{ n+1 } } dy }
&={ n }^{ n+1 }\displaystyle\sum _{ k=n }^{ \infty }{ \displaystyle\int _{ k }^{ k+1 }{ \frac { y-k }{ { y }^{ n+1 } } dy } } \\
&=\frac { { n }^{ n+1 } }{ n-1 } \displaystyle\sum _{ k=n }^{ \infty }{ \left( \frac { 1 }{ { k }^{ n-1 } } -\frac { 1 }{ (k+1)^{ n-1 } } \right) } +{ n }^{ n }\displaystyle\sum _{ k=n }^{ \infty }{ k\left( \frac { 1 }{ (k+1)^{ n } } -\frac { 1 }{ { k }^{ n } } \right) } \\
&=\frac { { n }^{ 2 } }{ n-1 } +{ n }^{ n} \displaystyle\sum _{ k=n }^{ \infty }{ \left( \frac { 1 }{ (k+1)^{ n-1 } } -\frac { 1 }{ { k }^{ n-1 } } -\frac { 1 }{ (k+1)^{ n } } \right) } \\
&=\frac { n }{ n-1 } -{ n }^{ n }\left( \zeta (n)-\displaystyle\sum _{ k=1 }^{ n }{ \frac { 1 }{ { k }^{ n } } } \right).\ _\square
\end{aligned} n n + 1 ∫ n ∞ y n + 1 { y } d y = n n + 1 k = n ∑ ∞ ∫ k k + 1 y n + 1 y − k d y = n − 1 n n + 1 k = n ∑ ∞ ( k n − 1 1 − ( k + 1 ) n − 1 1 ) + n n k = n ∑ ∞ k ( ( k + 1 ) n 1 − k n 1 ) = n − 1 n 2 + n n k = n ∑ ∞ ( ( k + 1 ) n − 1 1 − k n − 1 1 − ( k + 1 ) n 1 ) = n − 1 n − n n ( ζ ( n ) − k = 1 ∑ n k n 1 ) . □
Prove that ∫ 0 1 { 1 n x n } d x = 1 n − 1 − ζ ( n ) n n . \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \frac { 1 }{ n\sqrt [ n ]{ x } } \right\} dx } =\frac { 1 }{ n-1 } -\frac { \zeta (n) }{ { n }^{ n } } . ∫ 0 1 { n n x 1 } d x = n − 1 1 − n n ζ ( n ) .
First we let x = 1 n n y n , x=\frac { 1 }{ { n }^{ n }{ y }^{ n } }, x = n n y n 1 , then the integral converts to
1 n n − 1 ∫ 1 n ∞ { y } y n + 1 = 1 n n − 1 ( ∫ 1 n 1 d y y n + ∫ 1 ∞ { y } y n + 1 d y ) . \frac { 1 }{ { n }^{ n-1 } } \displaystyle\int _{ \frac1n }^{ \infty }{ \frac { \{ y\} }{ { y }^{ n+1 } } } =\frac { 1 }{ { n }^{ n-1 } } \left( \displaystyle\int _{ \frac1n }^{ 1 }{ \frac { dy }{ { y }^{ n } } } +\displaystyle\int _{ 1 }^{ \infty }{ \frac { \{ y\} }{ { y }^{ n+1 } } dy } \right). n n − 1 1 ∫ n 1 ∞ y n + 1 { y } = n n − 1 1 ( ∫ n 1 1 y n d y + ∫ 1 ∞ y n + 1 { y } d y ) .
The first integral is easy to evaluate and we evaluated the second here (see my solution--Hummus A).
So with a bit of simplification, we obtain the result
∫ 0 1 { 1 n x n } d x = 1 n − 1 − ζ ( n ) n n . □ \displaystyle\int _{ 0 }^{ 1 }{ \left\{ \frac { 1 }{ n\sqrt [ n ]{ x } } \right\} dx } =\frac { 1 }{ n-1 } -\frac { \zeta (n) }{ { n }^{ n } }.\ _\square ∫ 0 1 { n n x 1 } d x = n − 1 1 − n n ζ ( n ) . □
Reveal the answer
∫ 0 1 { 1 x } 1 − { 1 x } 3 d x 1 − x \int_0^1 \sqrt[3]{\frac{\big\{\frac1x\big\}}{1-\big\{\frac1x\big\}}}\frac{dx}{1-x} ∫ 0 1 3 1 − { x 1 } { x 1 } 1 − x d x
If the closed form of the value of the integral above can be expressed as a π k c d , \dfrac{a\pi^k}{c\sqrt{d}}, c d a π k , where a a a and c c c are coprime and d d d is square-free, find a + k + c + d a+k+c+d a + k + c + d .
Also, is it possible to find the following in a closed form?
∫ 0 1 { 1 x } 1 − { 1 x } n d x 1 − x \int_0^1 \sqrt[n]{\frac{\big\{\frac1x\big\}}{1-\big\{\frac1x\big\}}}\frac{dx}{1-x} ∫ 0 1 n 1 − { x 1 } { x 1 } 1 − x d x
The correct answer is: 7