Evaluate $limlimits_xtoinftyfrac1xint_0^xmaxsin t,sin(tsqrt2)dt$

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I want to evaluate
$$L=lim_xtoinftyfrac1xint_0^xmaxsin t,sin(tsqrt2)dt$$
My attempt
$$L=lim_xtoinftyfrac12xint_0^xBig(sin t+sin(tsqrt2)+big|sin t-sin(tsqrt2)big|Big)dt\
=lim_xtoinftyfrac12xint_0^xbig|sin t-sin(tsqrt2)big|dt\
=lim_xtoinftyfrac1xint_0^xbigg|cosfracsqrt2+12tcdotsinfracsqrt2-12tbigg|dt$$
Denote $s_n$ the $n$th zero point of $cosfracsqrt2+12tcdotsinfracsqrt2-12t (tge0)$. Since $1$, $sqrt2$ and $pi$ are linear independent in $mathbb Q$, the order of the zero points should be $1$. According to the squeeze theorem, we have
$$L=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kint_s_k^s_k+1big(sin t-sin(tsqrt2)big)dt\
=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kbigg(cos s_k-cos s_k+1+fraccossqrt2s_k-cossqrt2s_k+1sqrt2bigg)dt$$
I can't go further. I think the zero points of that function is the key point.







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  • I'm a bit puzzled by the first row in your attempt. Why is this true? And I suppose in the second row you split into three integrals and dumped zeros?
    – dEmigOd
    Jul 22 at 10:15










  • @dEmigOd I guess the integral of first two terms are bounded and would vanish in the limit.
    – Szeto
    Jul 22 at 10:18






  • 1




    @dEmigOd I used the identity $maxa,b=(a+b+|a-b|)/2$. The first and the second integral I splitted divided by $x$ is $0$ as $xtoinfty$.
    – LittleCuteKemono
    Jul 22 at 10:19










  • Does the function $|sin t-sin(tsqrt2)|$ have a period?
    – Szeto
    Jul 22 at 10:35






  • 1




    @Szeto: of course not, $sqrt2$ is irrational.
    – Yves Daoust
    Jul 22 at 10:36















up vote
19
down vote

favorite
7












I want to evaluate
$$L=lim_xtoinftyfrac1xint_0^xmaxsin t,sin(tsqrt2)dt$$
My attempt
$$L=lim_xtoinftyfrac12xint_0^xBig(sin t+sin(tsqrt2)+big|sin t-sin(tsqrt2)big|Big)dt\
=lim_xtoinftyfrac12xint_0^xbig|sin t-sin(tsqrt2)big|dt\
=lim_xtoinftyfrac1xint_0^xbigg|cosfracsqrt2+12tcdotsinfracsqrt2-12tbigg|dt$$
Denote $s_n$ the $n$th zero point of $cosfracsqrt2+12tcdotsinfracsqrt2-12t (tge0)$. Since $1$, $sqrt2$ and $pi$ are linear independent in $mathbb Q$, the order of the zero points should be $1$. According to the squeeze theorem, we have
$$L=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kint_s_k^s_k+1big(sin t-sin(tsqrt2)big)dt\
=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kbigg(cos s_k-cos s_k+1+fraccossqrt2s_k-cossqrt2s_k+1sqrt2bigg)dt$$
I can't go further. I think the zero points of that function is the key point.







share|cite|improve this question





















  • I'm a bit puzzled by the first row in your attempt. Why is this true? And I suppose in the second row you split into three integrals and dumped zeros?
    – dEmigOd
    Jul 22 at 10:15










  • @dEmigOd I guess the integral of first two terms are bounded and would vanish in the limit.
    – Szeto
    Jul 22 at 10:18






  • 1




    @dEmigOd I used the identity $maxa,b=(a+b+|a-b|)/2$. The first and the second integral I splitted divided by $x$ is $0$ as $xtoinfty$.
    – LittleCuteKemono
    Jul 22 at 10:19










  • Does the function $|sin t-sin(tsqrt2)|$ have a period?
    – Szeto
    Jul 22 at 10:35






  • 1




    @Szeto: of course not, $sqrt2$ is irrational.
    – Yves Daoust
    Jul 22 at 10:36













up vote
19
down vote

favorite
7









up vote
19
down vote

favorite
7






7





I want to evaluate
$$L=lim_xtoinftyfrac1xint_0^xmaxsin t,sin(tsqrt2)dt$$
My attempt
$$L=lim_xtoinftyfrac12xint_0^xBig(sin t+sin(tsqrt2)+big|sin t-sin(tsqrt2)big|Big)dt\
=lim_xtoinftyfrac12xint_0^xbig|sin t-sin(tsqrt2)big|dt\
=lim_xtoinftyfrac1xint_0^xbigg|cosfracsqrt2+12tcdotsinfracsqrt2-12tbigg|dt$$
Denote $s_n$ the $n$th zero point of $cosfracsqrt2+12tcdotsinfracsqrt2-12t (tge0)$. Since $1$, $sqrt2$ and $pi$ are linear independent in $mathbb Q$, the order of the zero points should be $1$. According to the squeeze theorem, we have
$$L=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kint_s_k^s_k+1big(sin t-sin(tsqrt2)big)dt\
=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kbigg(cos s_k-cos s_k+1+fraccossqrt2s_k-cossqrt2s_k+1sqrt2bigg)dt$$
I can't go further. I think the zero points of that function is the key point.







share|cite|improve this question













I want to evaluate
$$L=lim_xtoinftyfrac1xint_0^xmaxsin t,sin(tsqrt2)dt$$
My attempt
$$L=lim_xtoinftyfrac12xint_0^xBig(sin t+sin(tsqrt2)+big|sin t-sin(tsqrt2)big|Big)dt\
=lim_xtoinftyfrac12xint_0^xbig|sin t-sin(tsqrt2)big|dt\
=lim_xtoinftyfrac1xint_0^xbigg|cosfracsqrt2+12tcdotsinfracsqrt2-12tbigg|dt$$
Denote $s_n$ the $n$th zero point of $cosfracsqrt2+12tcdotsinfracsqrt2-12t (tge0)$. Since $1$, $sqrt2$ and $pi$ are linear independent in $mathbb Q$, the order of the zero points should be $1$. According to the squeeze theorem, we have
$$L=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kint_s_k^s_k+1big(sin t-sin(tsqrt2)big)dt\
=lim_ntoinftyfrac1s_n+1sum_k=0^n(-1)^kbigg(cos s_k-cos s_k+1+fraccossqrt2s_k-cossqrt2s_k+1sqrt2bigg)dt$$
I can't go further. I think the zero points of that function is the key point.









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edited Jul 22 at 10:26
























asked Jul 22 at 9:12









LittleCuteKemono

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46812











  • I'm a bit puzzled by the first row in your attempt. Why is this true? And I suppose in the second row you split into three integrals and dumped zeros?
    – dEmigOd
    Jul 22 at 10:15










  • @dEmigOd I guess the integral of first two terms are bounded and would vanish in the limit.
    – Szeto
    Jul 22 at 10:18






  • 1




    @dEmigOd I used the identity $maxa,b=(a+b+|a-b|)/2$. The first and the second integral I splitted divided by $x$ is $0$ as $xtoinfty$.
    – LittleCuteKemono
    Jul 22 at 10:19










  • Does the function $|sin t-sin(tsqrt2)|$ have a period?
    – Szeto
    Jul 22 at 10:35






  • 1




    @Szeto: of course not, $sqrt2$ is irrational.
    – Yves Daoust
    Jul 22 at 10:36

















  • I'm a bit puzzled by the first row in your attempt. Why is this true? And I suppose in the second row you split into three integrals and dumped zeros?
    – dEmigOd
    Jul 22 at 10:15










  • @dEmigOd I guess the integral of first two terms are bounded and would vanish in the limit.
    – Szeto
    Jul 22 at 10:18






  • 1




    @dEmigOd I used the identity $maxa,b=(a+b+|a-b|)/2$. The first and the second integral I splitted divided by $x$ is $0$ as $xtoinfty$.
    – LittleCuteKemono
    Jul 22 at 10:19










  • Does the function $|sin t-sin(tsqrt2)|$ have a period?
    – Szeto
    Jul 22 at 10:35






  • 1




    @Szeto: of course not, $sqrt2$ is irrational.
    – Yves Daoust
    Jul 22 at 10:36
















I'm a bit puzzled by the first row in your attempt. Why is this true? And I suppose in the second row you split into three integrals and dumped zeros?
– dEmigOd
Jul 22 at 10:15




I'm a bit puzzled by the first row in your attempt. Why is this true? And I suppose in the second row you split into three integrals and dumped zeros?
– dEmigOd
Jul 22 at 10:15












@dEmigOd I guess the integral of first two terms are bounded and would vanish in the limit.
– Szeto
Jul 22 at 10:18




@dEmigOd I guess the integral of first two terms are bounded and would vanish in the limit.
– Szeto
Jul 22 at 10:18




1




1




@dEmigOd I used the identity $maxa,b=(a+b+|a-b|)/2$. The first and the second integral I splitted divided by $x$ is $0$ as $xtoinfty$.
– LittleCuteKemono
Jul 22 at 10:19




@dEmigOd I used the identity $maxa,b=(a+b+|a-b|)/2$. The first and the second integral I splitted divided by $x$ is $0$ as $xtoinfty$.
– LittleCuteKemono
Jul 22 at 10:19












Does the function $|sin t-sin(tsqrt2)|$ have a period?
– Szeto
Jul 22 at 10:35




Does the function $|sin t-sin(tsqrt2)|$ have a period?
– Szeto
Jul 22 at 10:35




1




1




@Szeto: of course not, $sqrt2$ is irrational.
– Yves Daoust
Jul 22 at 10:36





@Szeto: of course not, $sqrt2$ is irrational.
– Yves Daoust
Jul 22 at 10:36











3 Answers
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up vote
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accepted










As pointed out by OP, we can use $maxa,b = fraca+b2 + frac2$ to discover that



$$ L = lim_xtoinfty frac1x int_0^x left|cosleft(fracsqrt2+12tright)sinleft(fracsqrt2-12tright)right| , dt. $$



Applying the substitution $fracsqrt2+12t = pi u$ and writing $alpha=(sqrt2-1)^2$ followed by the substitution $y = fracsqrt2+12pix$, we see that



beginalign*
L
&= lim_ytoinfty frac1y int_0^y left| cos(pi u)sin(pi alpha u) right| , du \
&= lim_Ntoinfty frac1N int_0^N left| cos(pi u)sin(pi alpha u) right| , du \
&= lim_Ntoinfty int_0^1 left| cos(pi u) right| left( frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| right) , du
endalign*



Since $alpha$ is irrational, the equidistribution theorem applied to $v mapsto left| sin(pi v + pi alpha u) right|$ for each fixed $u$ tells that



$$ forall uinmathbbR : lim_Ntoinfty frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| = int_0^1 left| sin(pi v) right| , dv. $$



Therefore by the dominated convergence theorem,



$$ L = left( int_0^1 left| cos(pi u) right| , du right)left( int_0^1 left| sin(pi v) right| , dv right) = frac4pi^2. $$






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  • I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
    – LittleCuteKemono
    Jul 23 at 5:43










  • @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
    – Sangchul Lee
    Jul 23 at 10:48

















up vote
7
down vote













I strongly conjecture that the limit is $4overpi^2=0.405285$. Integrating numerically over the interval $[0,1000]$ Mathematica obtained $0.406966$, but warned that the error might be larger than Mathematica's standard.



Consider the torus $T:=bigl(mathbb R/(2pimathbb Z)bigr)^2$and on $T$ the function
$$f(x,y):=maxsin x,sin y .$$
Draw a figure of the fundamental domain $[-pi,pi]^2$ in order to identify the parts of $T$ where $sin x$, resp. $sin y$, is larger. Then compute the required double integrals and obtain
$$int_T f(x,y)>rm d(x,y)=16 .$$
This means that the "space average" $E$ of $f$ is given by
$$E(f)=16over rm area(T)=4overpi^2 .$$
Now the orbit $$tmapsto bigl(x(t),y(t)bigr):=(t,>sqrt2,t)$$
projects to a line with irrational slope on $T$. In such a situation an "ergodic principle" is at work. According to this principle the "time average" of $f$ coincides with the "space average" $E(f)$. Theoretical basis for this to happen is the fact that the multiples $k/sqrt2$ $(kinmathbb N)$ are uniformly distributed mod $1$.






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    For simplicity I'll notate $alpha = fracsqrt2+12$ and $beta = fracsqrt2-12$. Now note that the integral basically only depends on the asymptotic behaviour of the integrand, meaning that for all $y$:



    $$
    beginalign
    L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
    &= lim_xtoinfty frac1x int_y^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt\
    &= lim_xtoinfty frac1x+y int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt\
    &= lim_xtoinfty frac1x int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt
    endalign
    $$



    Letting $y = frac2pi nalpha$ for $n in mathbbN$ this implies:



    $$
    L = lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt
    $$



    now since $alpha$ and $beta$ are irrational we get (using the ergodic theorem):



    $$
    lim_Ntoinfty frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| = frac12piint_0^2pi bigg| sin(s) bigg| ,mathrmds = frac2pi
    $$



    for almost all $t$. With this we can now solve the original integral as follows:



    $$
    beginalign
    L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
    &= lim_Ntoinfty frac1N sum_n=0^N lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
    &= lim_Ntoinfty lim_xtoinfty frac1x frac1N sum_n=0^Nint_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
    &= lim_Ntoinfty lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
    &= lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac2pi ,mathrmdt\
    &= frac4pi^2
    endalign
    $$



    this second to last step still requires some justification however. This can be done by noting that ergodic theorem guarantees that $frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg|$ converges in the $L^2$ sense on $[0, 2pi / beta]$ to the constant function $frac2pi$. This is enough since, if we have $g$ bounded and $f_n$ periodic with period $2pi / beta$ and $f_n to f$ in the $L^2$ sense over that period then:



    $$
    beginalign
    lim_Ntoinfty left| lim_xtoinfty frac1x int_0^x g cdot f_n ,mathrmdt - lim_xtoinfty frac1x int_0^x g cdot f ,mathrmdt right|
    &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x | g cdot f_n - g cdot f |^2 ,mathrmdt\
    &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x C | f_n - f |^2 ,mathrmdt\
    &le lim_Ntoinfty lim_xtoinfty fracCx leftlceilfracx2pi / betarightrceil | f_n - f |_2^2\
    &le lim_Ntoinfty fracC2pi / beta | f_n - f |_2^2 to 0
    endalign
    $$



    It's possible there's a less fiddly proof to show convergence, but combining asymptotic density and ergodic theory does make things a bit tricky.






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      3 Answers
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      3 Answers
      3






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      active

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      active

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      up vote
      9
      down vote



      accepted










      As pointed out by OP, we can use $maxa,b = fraca+b2 + frac2$ to discover that



      $$ L = lim_xtoinfty frac1x int_0^x left|cosleft(fracsqrt2+12tright)sinleft(fracsqrt2-12tright)right| , dt. $$



      Applying the substitution $fracsqrt2+12t = pi u$ and writing $alpha=(sqrt2-1)^2$ followed by the substitution $y = fracsqrt2+12pix$, we see that



      beginalign*
      L
      &= lim_ytoinfty frac1y int_0^y left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty frac1N int_0^N left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty int_0^1 left| cos(pi u) right| left( frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| right) , du
      endalign*



      Since $alpha$ is irrational, the equidistribution theorem applied to $v mapsto left| sin(pi v + pi alpha u) right|$ for each fixed $u$ tells that



      $$ forall uinmathbbR : lim_Ntoinfty frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| = int_0^1 left| sin(pi v) right| , dv. $$



      Therefore by the dominated convergence theorem,



      $$ L = left( int_0^1 left| cos(pi u) right| , du right)left( int_0^1 left| sin(pi v) right| , dv right) = frac4pi^2. $$






      share|cite|improve this answer























      • I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
        – LittleCuteKemono
        Jul 23 at 5:43










      • @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
        – Sangchul Lee
        Jul 23 at 10:48














      up vote
      9
      down vote



      accepted










      As pointed out by OP, we can use $maxa,b = fraca+b2 + frac2$ to discover that



      $$ L = lim_xtoinfty frac1x int_0^x left|cosleft(fracsqrt2+12tright)sinleft(fracsqrt2-12tright)right| , dt. $$



      Applying the substitution $fracsqrt2+12t = pi u$ and writing $alpha=(sqrt2-1)^2$ followed by the substitution $y = fracsqrt2+12pix$, we see that



      beginalign*
      L
      &= lim_ytoinfty frac1y int_0^y left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty frac1N int_0^N left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty int_0^1 left| cos(pi u) right| left( frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| right) , du
      endalign*



      Since $alpha$ is irrational, the equidistribution theorem applied to $v mapsto left| sin(pi v + pi alpha u) right|$ for each fixed $u$ tells that



      $$ forall uinmathbbR : lim_Ntoinfty frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| = int_0^1 left| sin(pi v) right| , dv. $$



      Therefore by the dominated convergence theorem,



      $$ L = left( int_0^1 left| cos(pi u) right| , du right)left( int_0^1 left| sin(pi v) right| , dv right) = frac4pi^2. $$






      share|cite|improve this answer























      • I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
        – LittleCuteKemono
        Jul 23 at 5:43










      • @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
        – Sangchul Lee
        Jul 23 at 10:48












      up vote
      9
      down vote



      accepted







      up vote
      9
      down vote



      accepted






      As pointed out by OP, we can use $maxa,b = fraca+b2 + frac2$ to discover that



      $$ L = lim_xtoinfty frac1x int_0^x left|cosleft(fracsqrt2+12tright)sinleft(fracsqrt2-12tright)right| , dt. $$



      Applying the substitution $fracsqrt2+12t = pi u$ and writing $alpha=(sqrt2-1)^2$ followed by the substitution $y = fracsqrt2+12pix$, we see that



      beginalign*
      L
      &= lim_ytoinfty frac1y int_0^y left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty frac1N int_0^N left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty int_0^1 left| cos(pi u) right| left( frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| right) , du
      endalign*



      Since $alpha$ is irrational, the equidistribution theorem applied to $v mapsto left| sin(pi v + pi alpha u) right|$ for each fixed $u$ tells that



      $$ forall uinmathbbR : lim_Ntoinfty frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| = int_0^1 left| sin(pi v) right| , dv. $$



      Therefore by the dominated convergence theorem,



      $$ L = left( int_0^1 left| cos(pi u) right| , du right)left( int_0^1 left| sin(pi v) right| , dv right) = frac4pi^2. $$






      share|cite|improve this answer















      As pointed out by OP, we can use $maxa,b = fraca+b2 + frac2$ to discover that



      $$ L = lim_xtoinfty frac1x int_0^x left|cosleft(fracsqrt2+12tright)sinleft(fracsqrt2-12tright)right| , dt. $$



      Applying the substitution $fracsqrt2+12t = pi u$ and writing $alpha=(sqrt2-1)^2$ followed by the substitution $y = fracsqrt2+12pix$, we see that



      beginalign*
      L
      &= lim_ytoinfty frac1y int_0^y left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty frac1N int_0^N left| cos(pi u)sin(pi alpha u) right| , du \
      &= lim_Ntoinfty int_0^1 left| cos(pi u) right| left( frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| right) , du
      endalign*



      Since $alpha$ is irrational, the equidistribution theorem applied to $v mapsto left| sin(pi v + pi alpha u) right|$ for each fixed $u$ tells that



      $$ forall uinmathbbR : lim_Ntoinfty frac1N sum_n=0^N-1 left| sin(pi alpha k + pi alpha u) right| = int_0^1 left| sin(pi v) right| , dv. $$



      Therefore by the dominated convergence theorem,



      $$ L = left( int_0^1 left| cos(pi u) right| , du right)left( int_0^1 left| sin(pi v) right| , dv right) = frac4pi^2. $$







      share|cite|improve this answer















      share|cite|improve this answer



      share|cite|improve this answer








      edited Jul 23 at 10:47


























      answered Jul 22 at 13:12









      Sangchul Lee

      85.5k12155253




      85.5k12155253











      • I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
        – LittleCuteKemono
        Jul 23 at 5:43










      • @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
        – Sangchul Lee
        Jul 23 at 10:48
















      • I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
        – LittleCuteKemono
        Jul 23 at 5:43










      • @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
        – Sangchul Lee
        Jul 23 at 10:48















      I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
      – LittleCuteKemono
      Jul 23 at 5:43




      I think you have a typo: $maxa,b=fraca+b2+|fraca-b2|$.
      – LittleCuteKemono
      Jul 23 at 5:43












      @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
      – Sangchul Lee
      Jul 23 at 10:48




      @LittleCuteKemono, Thank you for pointing out the typo. It is now fixed :)
      – Sangchul Lee
      Jul 23 at 10:48










      up vote
      7
      down vote













      I strongly conjecture that the limit is $4overpi^2=0.405285$. Integrating numerically over the interval $[0,1000]$ Mathematica obtained $0.406966$, but warned that the error might be larger than Mathematica's standard.



      Consider the torus $T:=bigl(mathbb R/(2pimathbb Z)bigr)^2$and on $T$ the function
      $$f(x,y):=maxsin x,sin y .$$
      Draw a figure of the fundamental domain $[-pi,pi]^2$ in order to identify the parts of $T$ where $sin x$, resp. $sin y$, is larger. Then compute the required double integrals and obtain
      $$int_T f(x,y)>rm d(x,y)=16 .$$
      This means that the "space average" $E$ of $f$ is given by
      $$E(f)=16over rm area(T)=4overpi^2 .$$
      Now the orbit $$tmapsto bigl(x(t),y(t)bigr):=(t,>sqrt2,t)$$
      projects to a line with irrational slope on $T$. In such a situation an "ergodic principle" is at work. According to this principle the "time average" of $f$ coincides with the "space average" $E(f)$. Theoretical basis for this to happen is the fact that the multiples $k/sqrt2$ $(kinmathbb N)$ are uniformly distributed mod $1$.






      share|cite|improve this answer

























        up vote
        7
        down vote













        I strongly conjecture that the limit is $4overpi^2=0.405285$. Integrating numerically over the interval $[0,1000]$ Mathematica obtained $0.406966$, but warned that the error might be larger than Mathematica's standard.



        Consider the torus $T:=bigl(mathbb R/(2pimathbb Z)bigr)^2$and on $T$ the function
        $$f(x,y):=maxsin x,sin y .$$
        Draw a figure of the fundamental domain $[-pi,pi]^2$ in order to identify the parts of $T$ where $sin x$, resp. $sin y$, is larger. Then compute the required double integrals and obtain
        $$int_T f(x,y)>rm d(x,y)=16 .$$
        This means that the "space average" $E$ of $f$ is given by
        $$E(f)=16over rm area(T)=4overpi^2 .$$
        Now the orbit $$tmapsto bigl(x(t),y(t)bigr):=(t,>sqrt2,t)$$
        projects to a line with irrational slope on $T$. In such a situation an "ergodic principle" is at work. According to this principle the "time average" of $f$ coincides with the "space average" $E(f)$. Theoretical basis for this to happen is the fact that the multiples $k/sqrt2$ $(kinmathbb N)$ are uniformly distributed mod $1$.






        share|cite|improve this answer























          up vote
          7
          down vote










          up vote
          7
          down vote









          I strongly conjecture that the limit is $4overpi^2=0.405285$. Integrating numerically over the interval $[0,1000]$ Mathematica obtained $0.406966$, but warned that the error might be larger than Mathematica's standard.



          Consider the torus $T:=bigl(mathbb R/(2pimathbb Z)bigr)^2$and on $T$ the function
          $$f(x,y):=maxsin x,sin y .$$
          Draw a figure of the fundamental domain $[-pi,pi]^2$ in order to identify the parts of $T$ where $sin x$, resp. $sin y$, is larger. Then compute the required double integrals and obtain
          $$int_T f(x,y)>rm d(x,y)=16 .$$
          This means that the "space average" $E$ of $f$ is given by
          $$E(f)=16over rm area(T)=4overpi^2 .$$
          Now the orbit $$tmapsto bigl(x(t),y(t)bigr):=(t,>sqrt2,t)$$
          projects to a line with irrational slope on $T$. In such a situation an "ergodic principle" is at work. According to this principle the "time average" of $f$ coincides with the "space average" $E(f)$. Theoretical basis for this to happen is the fact that the multiples $k/sqrt2$ $(kinmathbb N)$ are uniformly distributed mod $1$.






          share|cite|improve this answer













          I strongly conjecture that the limit is $4overpi^2=0.405285$. Integrating numerically over the interval $[0,1000]$ Mathematica obtained $0.406966$, but warned that the error might be larger than Mathematica's standard.



          Consider the torus $T:=bigl(mathbb R/(2pimathbb Z)bigr)^2$and on $T$ the function
          $$f(x,y):=maxsin x,sin y .$$
          Draw a figure of the fundamental domain $[-pi,pi]^2$ in order to identify the parts of $T$ where $sin x$, resp. $sin y$, is larger. Then compute the required double integrals and obtain
          $$int_T f(x,y)>rm d(x,y)=16 .$$
          This means that the "space average" $E$ of $f$ is given by
          $$E(f)=16over rm area(T)=4overpi^2 .$$
          Now the orbit $$tmapsto bigl(x(t),y(t)bigr):=(t,>sqrt2,t)$$
          projects to a line with irrational slope on $T$. In such a situation an "ergodic principle" is at work. According to this principle the "time average" of $f$ coincides with the "space average" $E(f)$. Theoretical basis for this to happen is the fact that the multiples $k/sqrt2$ $(kinmathbb N)$ are uniformly distributed mod $1$.







          share|cite|improve this answer













          share|cite|improve this answer



          share|cite|improve this answer











          answered Jul 22 at 12:39









          Christian Blatter

          163k7107306




          163k7107306




















              up vote
              3
              down vote













              For simplicity I'll notate $alpha = fracsqrt2+12$ and $beta = fracsqrt2-12$. Now note that the integral basically only depends on the asymptotic behaviour of the integrand, meaning that for all $y$:



              $$
              beginalign
              L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
              &= lim_xtoinfty frac1x int_y^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt\
              &= lim_xtoinfty frac1x+y int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt\
              &= lim_xtoinfty frac1x int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt
              endalign
              $$



              Letting $y = frac2pi nalpha$ for $n in mathbbN$ this implies:



              $$
              L = lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt
              $$



              now since $alpha$ and $beta$ are irrational we get (using the ergodic theorem):



              $$
              lim_Ntoinfty frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| = frac12piint_0^2pi bigg| sin(s) bigg| ,mathrmds = frac2pi
              $$



              for almost all $t$. With this we can now solve the original integral as follows:



              $$
              beginalign
              L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
              &= lim_Ntoinfty frac1N sum_n=0^N lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
              &= lim_Ntoinfty lim_xtoinfty frac1x frac1N sum_n=0^Nint_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
              &= lim_Ntoinfty lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
              &= lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac2pi ,mathrmdt\
              &= frac4pi^2
              endalign
              $$



              this second to last step still requires some justification however. This can be done by noting that ergodic theorem guarantees that $frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg|$ converges in the $L^2$ sense on $[0, 2pi / beta]$ to the constant function $frac2pi$. This is enough since, if we have $g$ bounded and $f_n$ periodic with period $2pi / beta$ and $f_n to f$ in the $L^2$ sense over that period then:



              $$
              beginalign
              lim_Ntoinfty left| lim_xtoinfty frac1x int_0^x g cdot f_n ,mathrmdt - lim_xtoinfty frac1x int_0^x g cdot f ,mathrmdt right|
              &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x | g cdot f_n - g cdot f |^2 ,mathrmdt\
              &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x C | f_n - f |^2 ,mathrmdt\
              &le lim_Ntoinfty lim_xtoinfty fracCx leftlceilfracx2pi / betarightrceil | f_n - f |_2^2\
              &le lim_Ntoinfty fracC2pi / beta | f_n - f |_2^2 to 0
              endalign
              $$



              It's possible there's a less fiddly proof to show convergence, but combining asymptotic density and ergodic theory does make things a bit tricky.






              share|cite|improve this answer



























                up vote
                3
                down vote













                For simplicity I'll notate $alpha = fracsqrt2+12$ and $beta = fracsqrt2-12$. Now note that the integral basically only depends on the asymptotic behaviour of the integrand, meaning that for all $y$:



                $$
                beginalign
                L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
                &= lim_xtoinfty frac1x int_y^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt\
                &= lim_xtoinfty frac1x+y int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt\
                &= lim_xtoinfty frac1x int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt
                endalign
                $$



                Letting $y = frac2pi nalpha$ for $n in mathbbN$ this implies:



                $$
                L = lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt
                $$



                now since $alpha$ and $beta$ are irrational we get (using the ergodic theorem):



                $$
                lim_Ntoinfty frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| = frac12piint_0^2pi bigg| sin(s) bigg| ,mathrmds = frac2pi
                $$



                for almost all $t$. With this we can now solve the original integral as follows:



                $$
                beginalign
                L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
                &= lim_Ntoinfty frac1N sum_n=0^N lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                &= lim_Ntoinfty lim_xtoinfty frac1x frac1N sum_n=0^Nint_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                &= lim_Ntoinfty lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                &= lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac2pi ,mathrmdt\
                &= frac4pi^2
                endalign
                $$



                this second to last step still requires some justification however. This can be done by noting that ergodic theorem guarantees that $frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg|$ converges in the $L^2$ sense on $[0, 2pi / beta]$ to the constant function $frac2pi$. This is enough since, if we have $g$ bounded and $f_n$ periodic with period $2pi / beta$ and $f_n to f$ in the $L^2$ sense over that period then:



                $$
                beginalign
                lim_Ntoinfty left| lim_xtoinfty frac1x int_0^x g cdot f_n ,mathrmdt - lim_xtoinfty frac1x int_0^x g cdot f ,mathrmdt right|
                &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x | g cdot f_n - g cdot f |^2 ,mathrmdt\
                &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x C | f_n - f |^2 ,mathrmdt\
                &le lim_Ntoinfty lim_xtoinfty fracCx leftlceilfracx2pi / betarightrceil | f_n - f |_2^2\
                &le lim_Ntoinfty fracC2pi / beta | f_n - f |_2^2 to 0
                endalign
                $$



                It's possible there's a less fiddly proof to show convergence, but combining asymptotic density and ergodic theory does make things a bit tricky.






                share|cite|improve this answer

























                  up vote
                  3
                  down vote










                  up vote
                  3
                  down vote









                  For simplicity I'll notate $alpha = fracsqrt2+12$ and $beta = fracsqrt2-12$. Now note that the integral basically only depends on the asymptotic behaviour of the integrand, meaning that for all $y$:



                  $$
                  beginalign
                  L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
                  &= lim_xtoinfty frac1x int_y^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt\
                  &= lim_xtoinfty frac1x+y int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt\
                  &= lim_xtoinfty frac1x int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt
                  endalign
                  $$



                  Letting $y = frac2pi nalpha$ for $n in mathbbN$ this implies:



                  $$
                  L = lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt
                  $$



                  now since $alpha$ and $beta$ are irrational we get (using the ergodic theorem):



                  $$
                  lim_Ntoinfty frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| = frac12piint_0^2pi bigg| sin(s) bigg| ,mathrmds = frac2pi
                  $$



                  for almost all $t$. With this we can now solve the original integral as follows:



                  $$
                  beginalign
                  L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
                  &= lim_Ntoinfty frac1N sum_n=0^N lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                  &= lim_Ntoinfty lim_xtoinfty frac1x frac1N sum_n=0^Nint_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                  &= lim_Ntoinfty lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                  &= lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac2pi ,mathrmdt\
                  &= frac4pi^2
                  endalign
                  $$



                  this second to last step still requires some justification however. This can be done by noting that ergodic theorem guarantees that $frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg|$ converges in the $L^2$ sense on $[0, 2pi / beta]$ to the constant function $frac2pi$. This is enough since, if we have $g$ bounded and $f_n$ periodic with period $2pi / beta$ and $f_n to f$ in the $L^2$ sense over that period then:



                  $$
                  beginalign
                  lim_Ntoinfty left| lim_xtoinfty frac1x int_0^x g cdot f_n ,mathrmdt - lim_xtoinfty frac1x int_0^x g cdot f ,mathrmdt right|
                  &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x | g cdot f_n - g cdot f |^2 ,mathrmdt\
                  &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x C | f_n - f |^2 ,mathrmdt\
                  &le lim_Ntoinfty lim_xtoinfty fracCx leftlceilfracx2pi / betarightrceil | f_n - f |_2^2\
                  &le lim_Ntoinfty fracC2pi / beta | f_n - f |_2^2 to 0
                  endalign
                  $$



                  It's possible there's a less fiddly proof to show convergence, but combining asymptotic density and ergodic theory does make things a bit tricky.






                  share|cite|improve this answer















                  For simplicity I'll notate $alpha = fracsqrt2+12$ and $beta = fracsqrt2-12$. Now note that the integral basically only depends on the asymptotic behaviour of the integrand, meaning that for all $y$:



                  $$
                  beginalign
                  L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
                  &= lim_xtoinfty frac1x int_y^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt\
                  &= lim_xtoinfty frac1x+y int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt\
                  &= lim_xtoinfty frac1x int_0^x bigg| cos alpha (t+y) cdot sin beta (t+y)bigg| ,mathrmdt
                  endalign
                  $$



                  Letting $y = frac2pi nalpha$ for $n in mathbbN$ this implies:



                  $$
                  L = lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt
                  $$



                  now since $alpha$ and $beta$ are irrational we get (using the ergodic theorem):



                  $$
                  lim_Ntoinfty frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| = frac12piint_0^2pi bigg| sin(s) bigg| ,mathrmds = frac2pi
                  $$



                  for almost all $t$. With this we can now solve the original integral as follows:



                  $$
                  beginalign
                  L =lim_xtoinfty frac1x int_0^x bigg| cos alpha t cdot sin beta tbigg| ,mathrmdt
                  &= lim_Ntoinfty frac1N sum_n=0^N lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                  &= lim_Ntoinfty lim_xtoinfty frac1x frac1N sum_n=0^Nint_0^x bigg| cos alpha t bigg| cdotbigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                  &= lim_Ntoinfty lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg| ,mathrmdt\
                  &= lim_xtoinfty frac1x int_0^x bigg| cos alpha t bigg| cdot frac2pi ,mathrmdt\
                  &= frac4pi^2
                  endalign
                  $$



                  this second to last step still requires some justification however. This can be done by noting that ergodic theorem guarantees that $frac1N sum_n=0^N bigg| sin beta Bigl(t+frac2pi nalphaBigr)bigg|$ converges in the $L^2$ sense on $[0, 2pi / beta]$ to the constant function $frac2pi$. This is enough since, if we have $g$ bounded and $f_n$ periodic with period $2pi / beta$ and $f_n to f$ in the $L^2$ sense over that period then:



                  $$
                  beginalign
                  lim_Ntoinfty left| lim_xtoinfty frac1x int_0^x g cdot f_n ,mathrmdt - lim_xtoinfty frac1x int_0^x g cdot f ,mathrmdt right|
                  &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x | g cdot f_n - g cdot f |^2 ,mathrmdt\
                  &le lim_Ntoinfty lim_xtoinfty frac1x int_0^x C | f_n - f |^2 ,mathrmdt\
                  &le lim_Ntoinfty lim_xtoinfty fracCx leftlceilfracx2pi / betarightrceil | f_n - f |_2^2\
                  &le lim_Ntoinfty fracC2pi / beta | f_n - f |_2^2 to 0
                  endalign
                  $$



                  It's possible there's a less fiddly proof to show convergence, but combining asymptotic density and ergodic theory does make things a bit tricky.







                  share|cite|improve this answer















                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited Jul 22 at 13:48


























                  answered Jul 22 at 13:34









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