limn→∞∏r=0n(2r+1)∏r=1n+12r\large\lim_{n \to\infty} \dfrac{\displaystyle\prod_{r=0}^n{(2r+1)}}{\displaystyle\prod_{r=1}^{n+1}{2r}} n→∞limr=1∏n+12rr=0∏n(2r+1)
I am unable to compute this limit mathematically, but my guess is that it is 000. Please post your solution to this.
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use sandwich theorem , it greatly helps here
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Thanks very much for the suggestion, but I don't know how to apply sandwich theorem in problems, I have only studied it in theory, can you give me a hint? :)
The infinite product representation of sinx\sin xsinx is sinxx=∏r=1∞(1−x2r2π2)\displaystyle \frac{\sin x}{x} = \prod_{r=1}^{\infty} (1-\frac{x^2}{r^2 \pi^2} ) xsinx=r=1∏∞(1−r2π2x2)
Put x=π2\displaystyle x=\frac{\pi}{2}x=2π to check that , 2π=1.3.3.5.5.7.7⋯2.2.4.4.6.6⋯=(1.3.5⋯2.4.6⋯)2\displaystyle \frac{2}{\pi}=\frac{1.3.3.5.5.7.7\cdots}{2.2.4.4.6.6\cdots} = (\frac{1.3.5\cdots}{2.4.6\cdots})^2 π2=2.2.4.4.6.6⋯1.3.3.5.5.7.7⋯=(2.4.6⋯1.3.5⋯)2
So your limit is : ∏n=1∞2n−12n=2π\displaystyle \prod_{n=1}^{\infty} \frac{2n-1}{2n} = \sqrt{\frac{2}{\pi}}n=1∏∞2n2n−1=π2
Okay, but my question is different from your expression in the last step, you have solved for ∏n=1∞2n−12n\displaystyle\prod_{n=1}^{\infty}{\frac{2n-1}{2n}}n=1∏∞2n2n−1 ,whereas I asked for limn→∞∏r=0n(2r+1)∏r=1n+12r\displaystyle\lim_{n \rightarrow \infty} \frac{\displaystyle\prod_{r=0}^n{(2r+1)}}{\displaystyle\prod_{r=1}^{n+1}{2r}} n→∞limr=1∏n+12rr=0∏n(2r+1)
Observe that ∏r=0n(2r+1)=∏r=1n(2(r−1)+1)=∏r=1n(2r−1)\prod_{r=0}^{n} (2r+1)=\prod_{r=1}^{n}(2(r-1)+1)=\prod_{r=1}^{n}(2r-1)∏r=0n(2r+1)=∏r=1n(2(r−1)+1)=∏r=1n(2r−1) , Put limit to obtain limn→∞∏r=0n(2r+1)=∏r=1∞(2n−1)\displaystyle \lim_{n\to\infty}\prod_{r=0}^{n}(2r+1)=\prod_{r=1}^{\infty}(2n-1)n→∞limr=0∏n(2r+1)=r=1∏∞(2n−1)
Similarly , limn→∞∏r=1n+12r=∏r=1∞2r\displaystyle \lim_{n\to\infty}\prod_{r=1}^{n+1}2r=\prod_{r=1}^{\infty}2rn→∞limr=1∏n+12r=r=1∏∞2r
@Aditya Narayan Sharma – I think the answer is 000 because, limn→∞∏r=0n(2r+1)∏r=1n+12r=limn→∞1⋅3⋅5⋯(2n+1)2⋅4⋅6⋯(2(n+1))\displaystyle\lim _{ n\rightarrow \infty } \dfrac {\displaystyle \prod _{ r=0 }^{ n }{ (2r+1) } }{ \displaystyle\prod _{ r=1 }^{ n+1 }{ 2r } } =\displaystyle\lim _{ n\rightarrow \infty } \dfrac { 1\cdot 3\cdot 5\cdots (2n+1) }{ 2\cdot 4\cdot 6\cdots (2(n+1)) } n→∞limr=1∏n+12rr=0∏n(2r+1)=n→∞lim2⋅4⋅6⋯(2(n+1))1⋅3⋅5⋯(2n+1) Multiplying both sides by π/2\pi/2π/2, and using Walli's formula, we get: limn→∞π2⋅1⋅3⋅5⋯(2n+1)2⋅4⋅6⋯(2(n+1))=limn→∞∫0π/2sin2n+2x.dx=limn→∞Γ(32+n)π⋅Γ(2+n)=0⇒limn→∞∏r=0n(2r+1)∏r=1n+12r=2π×(limn→∞π⋅Γ(32+n)2⋅Γ(2+n))=2π×0=0\displaystyle\lim _{ n\rightarrow \infty } \dfrac\pi2\cdot\dfrac { 1\cdot 3\cdot 5\cdots (2n+1) }{ 2\cdot 4\cdot 6\cdots (2(n+1)) }=\displaystyle\lim _{ n\rightarrow \infty } \displaystyle \int_{0}^{{\pi}/{2}} {\sin ^{ 2n+2 }{ x }.dx }=\displaystyle\lim _{ n\rightarrow \infty }\dfrac{\Gamma \left({\dfrac32+n}\right)}{\sqrt π\cdot \Gamma{\left(2+n\right) }} =\boxed0 \\ \Rightarrow \displaystyle\lim _{ n\rightarrow \infty } \dfrac {\displaystyle \prod _{ r=0 }^{ n }{ (2r+1) } }{ \displaystyle\prod _{ r=1 }^{ n+1 }{ 2r } }=\dfrac2\pi \times\left(\displaystyle\lim _{ n\rightarrow \infty }\dfrac{\sqrt π \cdot \Gamma \left({\dfrac32+n}\right)}{2\cdot \Gamma{\left(2+n\right) }}\right)=\dfrac2\pi \times 0 =\boxed0 n→∞lim2π⋅2⋅4⋅6⋯(2(n+1))1⋅3⋅5⋯(2n+1)=n→∞lim∫0π/2sin2n+2x.dx=n→∞limπ⋅Γ(2+n)Γ(23+n)=0⇒n→∞limr=1∏n+12rr=0∏n(2r+1)=π2×⎝⎜⎜⎛n→∞lim2⋅Γ(2+n)π⋅Γ(23+n)⎠⎟⎟⎞=π2×0=0
I used wolfram alpha for computing the second last step, because I don't know how to compute limits in gamma functions.
The given function can also be written as
limn→∞(2n+2)!(2n+1⋅(n+1)!)2=limn→∞(2n+2n+1)(2n+1)2=0\displaystyle\lim_{n \rightarrow \infty}\dfrac{(2n+2)!}{\left(2^{n+1}\cdot(n+1)!\right)^{2}}=\displaystyle\lim_{n \rightarrow \infty}\dfrac {\dbinom{2n+2}{n+1} } { (2^{ n+1 })^{ 2 } }=0 n→∞lim(2n+1⋅(n+1)!)2(2n+2)!=n→∞lim(2n+1)2(n+12n+2)=0 because(2n+2n+1)(2n+1)2\dfrac {\dbinom{2n+2}{n+1} }{ (2^{ n+1 })^{ 2 } }(2n+1)2(n+12n+2) is a decreasing function.
@Swagat Panda – Yes, this is correct. The limit is 0. However, instead of using W|A for calculating the limit, you could use Legendre's duplication formula to get 22n+2Γ(n+32)Γ(n+2)=π⋅Γ(2n+3)2^{2n+2}\Gamma(n+\frac 32)\Gamma(n+2)=\sqrt{\pi}\cdot\Gamma(2n+3)22n+2Γ(n+23)Γ(n+2)=π⋅Γ(2n+3) and using this along with Γ(2n+3)(Γ(n+2))2=(2n+2)!((n+1)!)2=(2n+2n+1)\dfrac{\Gamma(2n+3)}{\left(\Gamma(n+2)\right)^2}=\dfrac{(2n+2)!}{\left((n+1)!\right)^2}=\dbinom{2n+2}{n+1}(Γ(n+2))2Γ(2n+3)=((n+1)!)2(2n+2)!=(n+12n+2), you could rewrite the limit as,
L=limn→∞Γ(n+3/2)π⋅Γ(n+2)=limn→∞Γ(2n+3)22n+2⋅(Γ(n+2))2=limn→∞(2n+2n+1)(2n+1)2L=\lim_{n\to\infty}\frac{\Gamma(n+3/2)}{\sqrt\pi\cdot\Gamma(n+2)}=\lim_{n\to\infty}\frac{\Gamma(2n+3)}{2^{2n+2}\cdot\left(\Gamma(n+2)\right)^2}=\lim_{n\to\infty}\frac{\binom{2n+2}{n+1}}{(2^{n+1})^2}L=n→∞limπ⋅Γ(n+2)Γ(n+3/2)=n→∞lim22n+2⋅(Γ(n+2))2Γ(2n+3)=n→∞lim(2n+1)2(n+12n+2)
Note that this is the second limit you mentioned in your comment. Rather than concluding that the limit is 0 using a handwavy argument that the binomial coefficient is a decreasing function (I can't see an easy way to verify it), I think a formal way would be to use a corollary of Stirling's result that (2nn)∼4nπn\dbinom{2n}n\sim\dfrac{4^n}{\sqrt{\pi n}}(n2n)∼πn4n as n→∞n\to\inftyn→∞, so the limit becomes,
L=limn→∞4n+1π(n+1)(2n+1)2=1πlimn→∞1n+1=0L=\lim_{n\to\infty}\frac{4^{n+1}}{\sqrt{\pi(n+1)}(2^{n+1})^2}=\frac 1{\sqrt\pi}\lim_{n\to\infty}\frac{1}{\sqrt{n+1}}=0L=n→∞limπ(n+1)(2n+1)24n+1=π1n→∞limn+11=0
where the penultimate limit is easily evaluated noting that n+1→∞\sqrt{n+1}\to\inftyn+1→∞ as n→∞n\to\inftyn→∞, hence 1n+1→0\frac{1}{\sqrt{n+1}}\to 0n+11→0 as n→∞n\to\inftyn→∞.
@Prasun Biswas – I asked for help because I couldn't find a way to interpret this limit formally using methods mentioned in the JEE syllabus and I was relatively new to Stirling's approximation then, which is why I gave the reason of decreasing function. Thanks for helping me out.
Also you don't need to go to Legendre's formula to get to the function I mentioned. Just multiply the numerator and denominator with the denominator(i.e. product of even numbers) again to get that.
This is incorrect. Putting x=π/2x=\pi/2x=π/2 gives 2π=∏n=1∞(2n)2−1(2n)2\dfrac 2\pi=\prod\limits_{n=1}^\infty\dfrac{(2n)^2-1}{(2n)^2}π2=n=1∏∞(2n)2(2n)2−1. So, we have 2π=∏n=1∞(2n)2−12n\sqrt{\dfrac 2\pi}=\prod\limits_{n=1}^\infty\dfrac{\sqrt{(2n)^2-1}}{2n}π2=n=1∏∞2n(2n)2−1 which is obviously not the same as the one you wrote.
I guess you mistook the numerator (2n)2−1(2n)^2-1(2n)2−1 as (2n−1)2(2n-1)^2(2n−1)2.
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use sandwich theorem , it greatly helps here
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Thanks very much for the suggestion, but I don't know how to apply sandwich theorem in problems, I have only studied it in theory, can you give me a hint? :)
The infinite product representation of sinx is xsinx=r=1∏∞(1−r2π2x2)
Put x=2π to check that , π2=2.2.4.4.6.6⋯1.3.3.5.5.7.7⋯=(2.4.6⋯1.3.5⋯)2
So your limit is : n=1∏∞2n2n−1=π2
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Okay, but my question is different from your expression in the last step, you have solved for n=1∏∞2n2n−1 ,whereas I asked for n→∞limr=1∏n+12rr=0∏n(2r+1)
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Observe that ∏r=0n(2r+1)=∏r=1n(2(r−1)+1)=∏r=1n(2r−1) , Put limit to obtain n→∞limr=0∏n(2r+1)=r=1∏∞(2n−1)
Similarly , n→∞limr=1∏n+12r=r=1∏∞2r
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0 because, n→∞limr=1∏n+12rr=0∏n(2r+1)=n→∞lim2⋅4⋅6⋯(2(n+1))1⋅3⋅5⋯(2n+1) Multiplying both sides by π/2, and using Walli's formula, we get: n→∞lim2π⋅2⋅4⋅6⋯(2(n+1))1⋅3⋅5⋯(2n+1)=n→∞lim∫0π/2sin2n+2x.dx=n→∞limπ⋅Γ(2+n)Γ(23+n)=0⇒n→∞limr=1∏n+12rr=0∏n(2r+1)=π2×⎝⎜⎜⎛n→∞lim2⋅Γ(2+n)π⋅Γ(23+n)⎠⎟⎟⎞=π2×0=0
I think the answer isI used wolfram alpha for computing the second last step, because I don't know how to compute limits in gamma functions.
The given function can also be written as
n→∞lim(2n+1⋅(n+1)!)2(2n+2)!=n→∞lim(2n+1)2(n+12n+2)=0 because(2n+1)2(n+12n+2) is a decreasing function.
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Legendre's duplication formula to get 22n+2Γ(n+23)Γ(n+2)=π⋅Γ(2n+3) and using this along with (Γ(n+2))2Γ(2n+3)=((n+1)!)2(2n+2)!=(n+12n+2), you could rewrite the limit as,
Yes, this is correct. The limit is 0. However, instead of using W|A for calculating the limit, you could useL=n→∞limπ⋅Γ(n+2)Γ(n+3/2)=n→∞lim22n+2⋅(Γ(n+2))2Γ(2n+3)=n→∞lim(2n+1)2(n+12n+2)
Note that this is the second limit you mentioned in your comment. Rather than concluding that the limit is 0 using a handwavy argument that the binomial coefficient is a decreasing function (I can't see an easy way to verify it), I think a formal way would be to use a corollary of Stirling's result that (n2n)∼πn4n as n→∞, so the limit becomes,
L=n→∞limπ(n+1)(2n+1)24n+1=π1n→∞limn+11=0
where the penultimate limit is easily evaluated noting that n+1→∞ as n→∞, hence n+11→0 as n→∞.
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Also you don't need to go to Legendre's formula to get to the function I mentioned. Just multiply the numerator and denominator with the denominator(i.e. product of even numbers) again to get that.
This is incorrect. Putting x=π/2 gives π2=n=1∏∞(2n)2(2n)2−1. So, we have π2=n=1∏∞2n(2n)2−1 which is obviously not the same as the one you wrote.
I guess you mistook the numerator (2n)2−1 as (2n−1)2.