Finding $limlimits_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4,mathrm dx$Evaluating $lim limits_nto infty,,, n!! intlimits_0^pi/2!! left(1-sqrt [n]sin x right),mathrm dx$Evaluate $int_0^1 frac1 x^2+2x+3,mathrm dx$Show how $fracpartialpartial x left[int_0^x (x-t)g(t),mathrmdtright] = int_0^x g(t),mathrmdt$Evaluate $large int_0^1left(frac1ln x + frac11-xright)^2 mathrm dx $ using elementary, high school techniquesFind the limit $lim_limitsxto 0^+left( e^frac1sin x-e^frac1xright)$L'Hopital rule to solve $ limlimits_xto 0 left(fracsin xxright)^frac1x^2 $Compute the limit $lim_ntoinfty nleft [int_0^frac pi4tan^n left ( fracxn right )mathrm dxright]^frac1n$How to find $limlimits_xto 0^+ frac1x int_0^x sin(frac1t),mathrm dt$$n^2 int_0^1 (1-x)^n sin(pi x) mathrmdx$If $I_n=int_0^1 fracx^nx^2+2019,mathrm dx$, evaluate $limlimits_nto infty nI_n$

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Finding $limlimits_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4,mathrm dx$


Evaluating $lim limits_nto infty,,, n!! intlimits_0^pi/2!! left(1-sqrt [n]sin x right),mathrm dx$Evaluate $int_0^1 frac1 x^2+2x+3,mathrm dx$Show how $fracpartialpartial x left[int_0^x (x-t)g(t),mathrmdtright] = int_0^x g(t),mathrmdt$Evaluate $large int_0^1left(frac1ln x + frac11-xright)^2 mathrm dx $ using elementary, high school techniquesFind the limit $lim_limitsxto 0^+left( e^frac1sin x-e^frac1xright)$L'Hopital rule to solve $ limlimits_xto 0 left(fracsin xxright)^frac1x^2 $Compute the limit $lim_ntoinfty nleft [int_0^frac pi4tan^n left ( fracxn right )mathrm dxright]^frac1n$How to find $limlimits_xto 0^+ frac1x int_0^x sin(frac1t),mathrm dt$$n^2 int_0^1 (1-x)^n sin(pi x) mathrmdx$If $I_n=int_0^1 fracx^nx^2+2019,mathrm dx$, evaluate $limlimits_nto infty nI_n$













5












$begingroup$


$$lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4,mathrm dx$$I don't know how to solve this limit problem. I'm roughly clear about using the pinch theorem, but I haven't done it yet. Could somebody please tell me? Thanks!










share|cite|improve this question











$endgroup$











  • $begingroup$
    (pinch theorem)
    $endgroup$
    – mathworker21
    22 hours ago










  • $begingroup$
    there's some formula like $sum_ le N e(ntheta) = fracsin(Ntheta)sin(theta)$. Something like that. I think that should be useful
    $endgroup$
    – mathworker21
    21 hours ago










  • $begingroup$
    I checked through W|A for values of $n$ as high as $nsim 20000$ and it seems that the limit does exist and is equal to $ln 2$. But at present I don't have a rigorous proof for the same.
    $endgroup$
    – Darkrai
    21 hours ago










  • $begingroup$
    After a lengthy semi-heuristic study I suspect the simple result $lim = log(2) simeq 0.6931471805599453..$
    $endgroup$
    – Dr. Wolfgang Hintze
    21 hours ago







  • 1




    $begingroup$
    Another way to reach the integral in Tianlalu's answer is as follows: Substituting $nx = u$ and writing $operatornamesinc(x) = fracsin xx$, we have $$ frac1n^2 int_0^fracpi2 x fracsin^4(nx)sin^4 x , mathrmdx = int_0^fracn pi2 fracsin^4 uu^3 operatornamesinc^4(u/n) , mathrmd u xrightarrow[ntoinfty]textDCT int_0^infty fracsin^4 uu^3 , mathrmd u, $$ where the convergence follows from the dominated convergence together with the integrable dominating function $Cu^-3sin^4 u$ for some constant $C > 0$.
    $endgroup$
    – Sangchul Lee
    17 hours ago















5












$begingroup$


$$lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4,mathrm dx$$I don't know how to solve this limit problem. I'm roughly clear about using the pinch theorem, but I haven't done it yet. Could somebody please tell me? Thanks!










share|cite|improve this question











$endgroup$











  • $begingroup$
    (pinch theorem)
    $endgroup$
    – mathworker21
    22 hours ago










  • $begingroup$
    there's some formula like $sum_ le N e(ntheta) = fracsin(Ntheta)sin(theta)$. Something like that. I think that should be useful
    $endgroup$
    – mathworker21
    21 hours ago










  • $begingroup$
    I checked through W|A for values of $n$ as high as $nsim 20000$ and it seems that the limit does exist and is equal to $ln 2$. But at present I don't have a rigorous proof for the same.
    $endgroup$
    – Darkrai
    21 hours ago










  • $begingroup$
    After a lengthy semi-heuristic study I suspect the simple result $lim = log(2) simeq 0.6931471805599453..$
    $endgroup$
    – Dr. Wolfgang Hintze
    21 hours ago







  • 1




    $begingroup$
    Another way to reach the integral in Tianlalu's answer is as follows: Substituting $nx = u$ and writing $operatornamesinc(x) = fracsin xx$, we have $$ frac1n^2 int_0^fracpi2 x fracsin^4(nx)sin^4 x , mathrmdx = int_0^fracn pi2 fracsin^4 uu^3 operatornamesinc^4(u/n) , mathrmd u xrightarrow[ntoinfty]textDCT int_0^infty fracsin^4 uu^3 , mathrmd u, $$ where the convergence follows from the dominated convergence together with the integrable dominating function $Cu^-3sin^4 u$ for some constant $C > 0$.
    $endgroup$
    – Sangchul Lee
    17 hours ago













5












5








5


4



$begingroup$


$$lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4,mathrm dx$$I don't know how to solve this limit problem. I'm roughly clear about using the pinch theorem, but I haven't done it yet. Could somebody please tell me? Thanks!










share|cite|improve this question











$endgroup$




$$lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4,mathrm dx$$I don't know how to solve this limit problem. I'm roughly clear about using the pinch theorem, but I haven't done it yet. Could somebody please tell me? Thanks!







calculus integration limits






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited 18 hours ago









rash

550115




550115










asked 22 hours ago









赵家艺赵家艺

362




362











  • $begingroup$
    (pinch theorem)
    $endgroup$
    – mathworker21
    22 hours ago










  • $begingroup$
    there's some formula like $sum_ le N e(ntheta) = fracsin(Ntheta)sin(theta)$. Something like that. I think that should be useful
    $endgroup$
    – mathworker21
    21 hours ago










  • $begingroup$
    I checked through W|A for values of $n$ as high as $nsim 20000$ and it seems that the limit does exist and is equal to $ln 2$. But at present I don't have a rigorous proof for the same.
    $endgroup$
    – Darkrai
    21 hours ago










  • $begingroup$
    After a lengthy semi-heuristic study I suspect the simple result $lim = log(2) simeq 0.6931471805599453..$
    $endgroup$
    – Dr. Wolfgang Hintze
    21 hours ago







  • 1




    $begingroup$
    Another way to reach the integral in Tianlalu's answer is as follows: Substituting $nx = u$ and writing $operatornamesinc(x) = fracsin xx$, we have $$ frac1n^2 int_0^fracpi2 x fracsin^4(nx)sin^4 x , mathrmdx = int_0^fracn pi2 fracsin^4 uu^3 operatornamesinc^4(u/n) , mathrmd u xrightarrow[ntoinfty]textDCT int_0^infty fracsin^4 uu^3 , mathrmd u, $$ where the convergence follows from the dominated convergence together with the integrable dominating function $Cu^-3sin^4 u$ for some constant $C > 0$.
    $endgroup$
    – Sangchul Lee
    17 hours ago
















  • $begingroup$
    (pinch theorem)
    $endgroup$
    – mathworker21
    22 hours ago










  • $begingroup$
    there's some formula like $sum_ le N e(ntheta) = fracsin(Ntheta)sin(theta)$. Something like that. I think that should be useful
    $endgroup$
    – mathworker21
    21 hours ago










  • $begingroup$
    I checked through W|A for values of $n$ as high as $nsim 20000$ and it seems that the limit does exist and is equal to $ln 2$. But at present I don't have a rigorous proof for the same.
    $endgroup$
    – Darkrai
    21 hours ago










  • $begingroup$
    After a lengthy semi-heuristic study I suspect the simple result $lim = log(2) simeq 0.6931471805599453..$
    $endgroup$
    – Dr. Wolfgang Hintze
    21 hours ago







  • 1




    $begingroup$
    Another way to reach the integral in Tianlalu's answer is as follows: Substituting $nx = u$ and writing $operatornamesinc(x) = fracsin xx$, we have $$ frac1n^2 int_0^fracpi2 x fracsin^4(nx)sin^4 x , mathrmdx = int_0^fracn pi2 fracsin^4 uu^3 operatornamesinc^4(u/n) , mathrmd u xrightarrow[ntoinfty]textDCT int_0^infty fracsin^4 uu^3 , mathrmd u, $$ where the convergence follows from the dominated convergence together with the integrable dominating function $Cu^-3sin^4 u$ for some constant $C > 0$.
    $endgroup$
    – Sangchul Lee
    17 hours ago















$begingroup$
(pinch theorem)
$endgroup$
– mathworker21
22 hours ago




$begingroup$
(pinch theorem)
$endgroup$
– mathworker21
22 hours ago












$begingroup$
there's some formula like $sum_ le N e(ntheta) = fracsin(Ntheta)sin(theta)$. Something like that. I think that should be useful
$endgroup$
– mathworker21
21 hours ago




$begingroup$
there's some formula like $sum_ le N e(ntheta) = fracsin(Ntheta)sin(theta)$. Something like that. I think that should be useful
$endgroup$
– mathworker21
21 hours ago












$begingroup$
I checked through W|A for values of $n$ as high as $nsim 20000$ and it seems that the limit does exist and is equal to $ln 2$. But at present I don't have a rigorous proof for the same.
$endgroup$
– Darkrai
21 hours ago




$begingroup$
I checked through W|A for values of $n$ as high as $nsim 20000$ and it seems that the limit does exist and is equal to $ln 2$. But at present I don't have a rigorous proof for the same.
$endgroup$
– Darkrai
21 hours ago












$begingroup$
After a lengthy semi-heuristic study I suspect the simple result $lim = log(2) simeq 0.6931471805599453..$
$endgroup$
– Dr. Wolfgang Hintze
21 hours ago





$begingroup$
After a lengthy semi-heuristic study I suspect the simple result $lim = log(2) simeq 0.6931471805599453..$
$endgroup$
– Dr. Wolfgang Hintze
21 hours ago





1




1




$begingroup$
Another way to reach the integral in Tianlalu's answer is as follows: Substituting $nx = u$ and writing $operatornamesinc(x) = fracsin xx$, we have $$ frac1n^2 int_0^fracpi2 x fracsin^4(nx)sin^4 x , mathrmdx = int_0^fracn pi2 fracsin^4 uu^3 operatornamesinc^4(u/n) , mathrmd u xrightarrow[ntoinfty]textDCT int_0^infty fracsin^4 uu^3 , mathrmd u, $$ where the convergence follows from the dominated convergence together with the integrable dominating function $Cu^-3sin^4 u$ for some constant $C > 0$.
$endgroup$
– Sangchul Lee
17 hours ago




$begingroup$
Another way to reach the integral in Tianlalu's answer is as follows: Substituting $nx = u$ and writing $operatornamesinc(x) = fracsin xx$, we have $$ frac1n^2 int_0^fracpi2 x fracsin^4(nx)sin^4 x , mathrmdx = int_0^fracn pi2 fracsin^4 uu^3 operatornamesinc^4(u/n) , mathrmd u xrightarrow[ntoinfty]textDCT int_0^infty fracsin^4 uu^3 , mathrmd u, $$ where the convergence follows from the dominated convergence together with the integrable dominating function $Cu^-3sin^4 u$ for some constant $C > 0$.
$endgroup$
– Sangchul Lee
17 hours ago










2 Answers
2






active

oldest

votes


















8












$begingroup$

From
$$lim_xto 0x^2left(frac1sin^4 x-frac1x^4right)=frac23,$$
for $xin(0,fracpi 2)$, there is $C$ such that
$$left|fracxsin^4 nxsin^4 x-fracsin^4 nxx^3right|le fracCsin^4 nxxle Cn.$$



Thus,
beginalign*
lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4, mathrm dx&=lim_ntoinftyfrac1n^2int_0^fracpi2fracsin^4 nxx^3, mathrm dx\
&= lim_ntoinftyint_0^fracnpi2fracsin^4 xx^3, mathrm dx\
&= int_0^inftyfracsin^4 xx^3, mathrm dx\
text(IBP)quad &= int_0^inftyfrac2sin^3 xcos xx^2, mathrm dx\
text(IBP)quad &= int_0^inftyfrac6sin^2 xcos^2 x-2sin^4 xx, mathrm dx\
&= int_0^inftyfraccos 2x-cos 4xx, mathrm dx\
text(Frullani)quad &=ln 2.
endalign*






share|cite|improve this answer









$endgroup$




















    4












    $begingroup$

    Result



    Let



    $$f(n) = int_0^fracpi 2 x left(fracsin (n x)sin (x)right)^4 , dx$$



    then



    $$lim_nto infty , fracf(n)n^2=log (2)simeq 0.6931471805599453 ...$$



    This result is in good agreement with the numerical estimate of the integral.



    Derivation



    This is more heuristic and not really strict. Maybe others can fill in the gaps.



    We split the integral into equally spaced intervals, and observe $sin(pi x/n) simeq pi x/n$ for $nto infty$ and get



    $$lim_nto infty f(n)/n^2 =lim_nto infty sum_k=1^infty a(k)tag1$$



    where



    $$a(k) = int_k-1^k pi ^2 s left(fracsin (pi s)pi sright)^4 , ds$$



    The first two values are



    $$a(1) = textCi(2 pi )-textCi(4 pi )+log (2)$$
    $$a(2) = -textCi(-8 pi )+textCi(-4 pi )-textCi(2 pi )+textCi(4 pi )$$



    and for $k ge 3$



    $$a(k) = -textCi(2 (k-1) pi )+textCi(4 (k-1) pi )-textCi(-4 k pi )+textCi(-2 k pi )$$



    Here $textCi(z) = -int_-infty ^z fraccos (t)t , dt$ is the cosine integral.



    The sum in $(1)$ telescopes and we are left with the announced result.



    Discussion



    My statement "the sum telescopes" is fairly bold.



    In fact, the cancellation is like this



    $$textCi(-4 pi )-textCi(4 pi )=i pi$$
    $$textCi(8 pi )-textCi(-8 pi )=-i pi$$



    see symmetry relations in http://people.math.sfu.ca/~cbm/aands/abramowitz_and_stegun.pdf, 5.2.20, and the sum of these two lines is $0$.






    share|cite|improve this answer











    $endgroup$












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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes









      8












      $begingroup$

      From
      $$lim_xto 0x^2left(frac1sin^4 x-frac1x^4right)=frac23,$$
      for $xin(0,fracpi 2)$, there is $C$ such that
      $$left|fracxsin^4 nxsin^4 x-fracsin^4 nxx^3right|le fracCsin^4 nxxle Cn.$$



      Thus,
      beginalign*
      lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4, mathrm dx&=lim_ntoinftyfrac1n^2int_0^fracpi2fracsin^4 nxx^3, mathrm dx\
      &= lim_ntoinftyint_0^fracnpi2fracsin^4 xx^3, mathrm dx\
      &= int_0^inftyfracsin^4 xx^3, mathrm dx\
      text(IBP)quad &= int_0^inftyfrac2sin^3 xcos xx^2, mathrm dx\
      text(IBP)quad &= int_0^inftyfrac6sin^2 xcos^2 x-2sin^4 xx, mathrm dx\
      &= int_0^inftyfraccos 2x-cos 4xx, mathrm dx\
      text(Frullani)quad &=ln 2.
      endalign*






      share|cite|improve this answer









      $endgroup$

















        8












        $begingroup$

        From
        $$lim_xto 0x^2left(frac1sin^4 x-frac1x^4right)=frac23,$$
        for $xin(0,fracpi 2)$, there is $C$ such that
        $$left|fracxsin^4 nxsin^4 x-fracsin^4 nxx^3right|le fracCsin^4 nxxle Cn.$$



        Thus,
        beginalign*
        lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4, mathrm dx&=lim_ntoinftyfrac1n^2int_0^fracpi2fracsin^4 nxx^3, mathrm dx\
        &= lim_ntoinftyint_0^fracnpi2fracsin^4 xx^3, mathrm dx\
        &= int_0^inftyfracsin^4 xx^3, mathrm dx\
        text(IBP)quad &= int_0^inftyfrac2sin^3 xcos xx^2, mathrm dx\
        text(IBP)quad &= int_0^inftyfrac6sin^2 xcos^2 x-2sin^4 xx, mathrm dx\
        &= int_0^inftyfraccos 2x-cos 4xx, mathrm dx\
        text(Frullani)quad &=ln 2.
        endalign*






        share|cite|improve this answer









        $endgroup$















          8












          8








          8





          $begingroup$

          From
          $$lim_xto 0x^2left(frac1sin^4 x-frac1x^4right)=frac23,$$
          for $xin(0,fracpi 2)$, there is $C$ such that
          $$left|fracxsin^4 nxsin^4 x-fracsin^4 nxx^3right|le fracCsin^4 nxxle Cn.$$



          Thus,
          beginalign*
          lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4, mathrm dx&=lim_ntoinftyfrac1n^2int_0^fracpi2fracsin^4 nxx^3, mathrm dx\
          &= lim_ntoinftyint_0^fracnpi2fracsin^4 xx^3, mathrm dx\
          &= int_0^inftyfracsin^4 xx^3, mathrm dx\
          text(IBP)quad &= int_0^inftyfrac2sin^3 xcos xx^2, mathrm dx\
          text(IBP)quad &= int_0^inftyfrac6sin^2 xcos^2 x-2sin^4 xx, mathrm dx\
          &= int_0^inftyfraccos 2x-cos 4xx, mathrm dx\
          text(Frullani)quad &=ln 2.
          endalign*






          share|cite|improve this answer









          $endgroup$



          From
          $$lim_xto 0x^2left(frac1sin^4 x-frac1x^4right)=frac23,$$
          for $xin(0,fracpi 2)$, there is $C$ such that
          $$left|fracxsin^4 nxsin^4 x-fracsin^4 nxx^3right|le fracCsin^4 nxxle Cn.$$



          Thus,
          beginalign*
          lim_ntoinftyfrac1n^2int_0^fracpi2xleft(fracsin nxsin xright)^4, mathrm dx&=lim_ntoinftyfrac1n^2int_0^fracpi2fracsin^4 nxx^3, mathrm dx\
          &= lim_ntoinftyint_0^fracnpi2fracsin^4 xx^3, mathrm dx\
          &= int_0^inftyfracsin^4 xx^3, mathrm dx\
          text(IBP)quad &= int_0^inftyfrac2sin^3 xcos xx^2, mathrm dx\
          text(IBP)quad &= int_0^inftyfrac6sin^2 xcos^2 x-2sin^4 xx, mathrm dx\
          &= int_0^inftyfraccos 2x-cos 4xx, mathrm dx\
          text(Frullani)quad &=ln 2.
          endalign*







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered 19 hours ago









          TianlaluTianlalu

          3,16721138




          3,16721138





















              4












              $begingroup$

              Result



              Let



              $$f(n) = int_0^fracpi 2 x left(fracsin (n x)sin (x)right)^4 , dx$$



              then



              $$lim_nto infty , fracf(n)n^2=log (2)simeq 0.6931471805599453 ...$$



              This result is in good agreement with the numerical estimate of the integral.



              Derivation



              This is more heuristic and not really strict. Maybe others can fill in the gaps.



              We split the integral into equally spaced intervals, and observe $sin(pi x/n) simeq pi x/n$ for $nto infty$ and get



              $$lim_nto infty f(n)/n^2 =lim_nto infty sum_k=1^infty a(k)tag1$$



              where



              $$a(k) = int_k-1^k pi ^2 s left(fracsin (pi s)pi sright)^4 , ds$$



              The first two values are



              $$a(1) = textCi(2 pi )-textCi(4 pi )+log (2)$$
              $$a(2) = -textCi(-8 pi )+textCi(-4 pi )-textCi(2 pi )+textCi(4 pi )$$



              and for $k ge 3$



              $$a(k) = -textCi(2 (k-1) pi )+textCi(4 (k-1) pi )-textCi(-4 k pi )+textCi(-2 k pi )$$



              Here $textCi(z) = -int_-infty ^z fraccos (t)t , dt$ is the cosine integral.



              The sum in $(1)$ telescopes and we are left with the announced result.



              Discussion



              My statement "the sum telescopes" is fairly bold.



              In fact, the cancellation is like this



              $$textCi(-4 pi )-textCi(4 pi )=i pi$$
              $$textCi(8 pi )-textCi(-8 pi )=-i pi$$



              see symmetry relations in http://people.math.sfu.ca/~cbm/aands/abramowitz_and_stegun.pdf, 5.2.20, and the sum of these two lines is $0$.






              share|cite|improve this answer











              $endgroup$

















                4












                $begingroup$

                Result



                Let



                $$f(n) = int_0^fracpi 2 x left(fracsin (n x)sin (x)right)^4 , dx$$



                then



                $$lim_nto infty , fracf(n)n^2=log (2)simeq 0.6931471805599453 ...$$



                This result is in good agreement with the numerical estimate of the integral.



                Derivation



                This is more heuristic and not really strict. Maybe others can fill in the gaps.



                We split the integral into equally spaced intervals, and observe $sin(pi x/n) simeq pi x/n$ for $nto infty$ and get



                $$lim_nto infty f(n)/n^2 =lim_nto infty sum_k=1^infty a(k)tag1$$



                where



                $$a(k) = int_k-1^k pi ^2 s left(fracsin (pi s)pi sright)^4 , ds$$



                The first two values are



                $$a(1) = textCi(2 pi )-textCi(4 pi )+log (2)$$
                $$a(2) = -textCi(-8 pi )+textCi(-4 pi )-textCi(2 pi )+textCi(4 pi )$$



                and for $k ge 3$



                $$a(k) = -textCi(2 (k-1) pi )+textCi(4 (k-1) pi )-textCi(-4 k pi )+textCi(-2 k pi )$$



                Here $textCi(z) = -int_-infty ^z fraccos (t)t , dt$ is the cosine integral.



                The sum in $(1)$ telescopes and we are left with the announced result.



                Discussion



                My statement "the sum telescopes" is fairly bold.



                In fact, the cancellation is like this



                $$textCi(-4 pi )-textCi(4 pi )=i pi$$
                $$textCi(8 pi )-textCi(-8 pi )=-i pi$$



                see symmetry relations in http://people.math.sfu.ca/~cbm/aands/abramowitz_and_stegun.pdf, 5.2.20, and the sum of these two lines is $0$.






                share|cite|improve this answer











                $endgroup$















                  4












                  4








                  4





                  $begingroup$

                  Result



                  Let



                  $$f(n) = int_0^fracpi 2 x left(fracsin (n x)sin (x)right)^4 , dx$$



                  then



                  $$lim_nto infty , fracf(n)n^2=log (2)simeq 0.6931471805599453 ...$$



                  This result is in good agreement with the numerical estimate of the integral.



                  Derivation



                  This is more heuristic and not really strict. Maybe others can fill in the gaps.



                  We split the integral into equally spaced intervals, and observe $sin(pi x/n) simeq pi x/n$ for $nto infty$ and get



                  $$lim_nto infty f(n)/n^2 =lim_nto infty sum_k=1^infty a(k)tag1$$



                  where



                  $$a(k) = int_k-1^k pi ^2 s left(fracsin (pi s)pi sright)^4 , ds$$



                  The first two values are



                  $$a(1) = textCi(2 pi )-textCi(4 pi )+log (2)$$
                  $$a(2) = -textCi(-8 pi )+textCi(-4 pi )-textCi(2 pi )+textCi(4 pi )$$



                  and for $k ge 3$



                  $$a(k) = -textCi(2 (k-1) pi )+textCi(4 (k-1) pi )-textCi(-4 k pi )+textCi(-2 k pi )$$



                  Here $textCi(z) = -int_-infty ^z fraccos (t)t , dt$ is the cosine integral.



                  The sum in $(1)$ telescopes and we are left with the announced result.



                  Discussion



                  My statement "the sum telescopes" is fairly bold.



                  In fact, the cancellation is like this



                  $$textCi(-4 pi )-textCi(4 pi )=i pi$$
                  $$textCi(8 pi )-textCi(-8 pi )=-i pi$$



                  see symmetry relations in http://people.math.sfu.ca/~cbm/aands/abramowitz_and_stegun.pdf, 5.2.20, and the sum of these two lines is $0$.






                  share|cite|improve this answer











                  $endgroup$



                  Result



                  Let



                  $$f(n) = int_0^fracpi 2 x left(fracsin (n x)sin (x)right)^4 , dx$$



                  then



                  $$lim_nto infty , fracf(n)n^2=log (2)simeq 0.6931471805599453 ...$$



                  This result is in good agreement with the numerical estimate of the integral.



                  Derivation



                  This is more heuristic and not really strict. Maybe others can fill in the gaps.



                  We split the integral into equally spaced intervals, and observe $sin(pi x/n) simeq pi x/n$ for $nto infty$ and get



                  $$lim_nto infty f(n)/n^2 =lim_nto infty sum_k=1^infty a(k)tag1$$



                  where



                  $$a(k) = int_k-1^k pi ^2 s left(fracsin (pi s)pi sright)^4 , ds$$



                  The first two values are



                  $$a(1) = textCi(2 pi )-textCi(4 pi )+log (2)$$
                  $$a(2) = -textCi(-8 pi )+textCi(-4 pi )-textCi(2 pi )+textCi(4 pi )$$



                  and for $k ge 3$



                  $$a(k) = -textCi(2 (k-1) pi )+textCi(4 (k-1) pi )-textCi(-4 k pi )+textCi(-2 k pi )$$



                  Here $textCi(z) = -int_-infty ^z fraccos (t)t , dt$ is the cosine integral.



                  The sum in $(1)$ telescopes and we are left with the announced result.



                  Discussion



                  My statement "the sum telescopes" is fairly bold.



                  In fact, the cancellation is like this



                  $$textCi(-4 pi )-textCi(4 pi )=i pi$$
                  $$textCi(8 pi )-textCi(-8 pi )=-i pi$$



                  see symmetry relations in http://people.math.sfu.ca/~cbm/aands/abramowitz_and_stegun.pdf, 5.2.20, and the sum of these two lines is $0$.







                  share|cite|improve this answer














                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited 18 hours ago

























                  answered 20 hours ago









                  Dr. Wolfgang HintzeDr. Wolfgang Hintze

                  3,825620




                  3,825620



























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