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This discussion board is a place to discuss our Daily Challenges and the math and science related to those challenges. Explanations are more than just a solution — they should explain the steps and thinking strategies that you used to obtain the solution. Comments should further the discussion of math and science.
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2^{34}
a_{i-1}
\frac{2}{3}
\sqrt{2}
\sum_{i=1}^3
\sin \theta
\boxed{123}
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We will proceed to generalize the above integral into
∫01{x1}kxndx
Denote
f(k,n)=∫01{x1}kxndx
After the substitution t1=x we obtain:
f(k,n)=∫1∞tn+2{t}kdt
This is simply a sum of consecutive integrals:
f(k,n)=i=1∑∞∫ii+1tn+2{t}kdt=i=1∑∞∫ii+1tn+2(t−i)k
By the u-substitution u=t−i we obtain: f(k,n)=i=1∑∞∫01(i+u)n+2ukdu =∫01uk(i=1∑∞(i+u)n+21)dy (1)
Given that ∫0∞e−kxxn dx=k−n−1n! We can see that (i+u)n+21=(n+1)!1∫0∞e−(i+u)yyn+1dy Proceeding to substitute the above expression we obtain:
i=1∑∞(i+u)n+21=(n+1)!1i=1∑∞∫0∞e−(i+u)yyn+1dy
=(n+1)!1∫0∞yn+1e−uy(i=1∑∞e−iy)dy
=(n+1)!1∫0∞ey−1yn+1e−uydy (2)
Substituting (2) into (1) : f(k,n)=(n+1)!1∫01uk(∫0∞ey−1yn+1e−uydy)du =(n+1)!1∫0∞ey−1yn+1(∫01uke−uydu)dy
It is easy to show through integration by parts that the inner integral is k!e−yi=1∑∞(k+i)!yi−1 . Therefore,
f(k,n)=(n+1)!1i=1∑∞(k+i)!k!∫0∞ey−1yn+ie−ydy
After evaluating that integral in the expression we obtain:
(n+1)!1i=1∑∞(k+i)!k!∫0∞ey−1yn+ie−ydy
=(n+1)!1i=1∑∞(k+i)!k!∫0∞yn+ie−2yj=0∑∞e−jydy
=(n+1)!1i=1∑∞(k+i)!k!j=0∑∞∫0∞yn+ie−(2+j)ydy
=(n+1)!1i=1∑∞(k+i)!k!j=0∑∞(2+j)n+i+1Γ(n+i+1)
=(n+1)!1i=1∑∞(k+i)!k!(n+i)!(ζ(n+i+1)−1)
Hence,
∫01{x1}kxndx=(n+1)!k!i=1∑∞(k+i)!(n+i)!(ζ(n+i+1)−1)
Plugging in n=0 gives us our original integral ∫01{x1}ndx=k=1∑∞(kn+k)ζ(k+1)−1
QED
Note:this is the longest LATEX document i've ever done,so it may contain errors
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How long did you take to prove this identity? It's just awesome!
I, bow to you.
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i just happen to really like calculus :)