Fourier Analysis - Functions on a Circle












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In general, if a continuous function $g(x)$ is defined on the interval $[-pi,pi]$, can I say it is definitely possible to extend this function to be a $2pi$-period function? I think we need to make sure the endpoints match? Functions are $2pi$-period on the real line are also called functions on a circle in Fourier analysis. But what about $$g(x) = x \on [-pi,pi]$$



This is clearly continuous, but $g(-pi) ne g(pi)$. How can I still extend this function to a continuous $2pi$-period function? Or do I have some conceptual misunderstandings?



Thanks so much for your help.










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    0












    $begingroup$


    In general, if a continuous function $g(x)$ is defined on the interval $[-pi,pi]$, can I say it is definitely possible to extend this function to be a $2pi$-period function? I think we need to make sure the endpoints match? Functions are $2pi$-period on the real line are also called functions on a circle in Fourier analysis. But what about $$g(x) = x \on [-pi,pi]$$



    This is clearly continuous, but $g(-pi) ne g(pi)$. How can I still extend this function to a continuous $2pi$-period function? Or do I have some conceptual misunderstandings?



    Thanks so much for your help.










    share|cite|improve this question









    $endgroup$















      0












      0








      0





      $begingroup$


      In general, if a continuous function $g(x)$ is defined on the interval $[-pi,pi]$, can I say it is definitely possible to extend this function to be a $2pi$-period function? I think we need to make sure the endpoints match? Functions are $2pi$-period on the real line are also called functions on a circle in Fourier analysis. But what about $$g(x) = x \on [-pi,pi]$$



      This is clearly continuous, but $g(-pi) ne g(pi)$. How can I still extend this function to a continuous $2pi$-period function? Or do I have some conceptual misunderstandings?



      Thanks so much for your help.










      share|cite|improve this question









      $endgroup$




      In general, if a continuous function $g(x)$ is defined on the interval $[-pi,pi]$, can I say it is definitely possible to extend this function to be a $2pi$-period function? I think we need to make sure the endpoints match? Functions are $2pi$-period on the real line are also called functions on a circle in Fourier analysis. But what about $$g(x) = x \on [-pi,pi]$$



      This is clearly continuous, but $g(-pi) ne g(pi)$. How can I still extend this function to a continuous $2pi$-period function? Or do I have some conceptual misunderstandings?



      Thanks so much for your help.







      fourier-analysis fourier-series periodic-functions






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      asked Feb 2 at 21:39









      xf16xf16

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          2 Answers
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          $begingroup$

          If the values at the endpoints don't match, you can't extend to a continuous function. But you can perform Fourier analysis even with functions admitting some discontinuities. Pretty much any periodic function which is not completely insane admits a Fourier expansion (of course the type and rate of convergence depends on regularity of the function; if you insist on some particular type of convergence, e.g. uniform convergence, then my statement is strictly speaking false).






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
            $endgroup$
            – xf16
            Feb 2 at 21:58












          • $begingroup$
            Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
            $endgroup$
            – Blazej
            Feb 2 at 22:20










          • $begingroup$
            Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
            $endgroup$
            – xf16
            Feb 2 at 22:25










          • $begingroup$
            This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
            $endgroup$
            – Blazej
            Feb 2 at 23:10



















          0












          $begingroup$

          If $g(-pi) ne g(pi)$, then you cannot extend to a $2pi$ periodic function because a $2pi$ periodic function $h$ on $mathbb{R}$ is required to satisfy $h(x)=h(x+2pi)$ for all $x$, and your $g$ does not satisfy that for $x=-pi$. You can extend any function defined on $[-pi,pi)$ or on $(-pi,pi]$ to a $2pi$ periodic function on $mathbb{R}$, but not if it is defined on $[-pi,pi]$ with $h(-pi)ne h(pi)$.






          share|cite|improve this answer









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            2 Answers
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            2 Answers
            2






            active

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            active

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            votes






            active

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            2












            $begingroup$

            If the values at the endpoints don't match, you can't extend to a continuous function. But you can perform Fourier analysis even with functions admitting some discontinuities. Pretty much any periodic function which is not completely insane admits a Fourier expansion (of course the type and rate of convergence depends on regularity of the function; if you insist on some particular type of convergence, e.g. uniform convergence, then my statement is strictly speaking false).






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
              $endgroup$
              – xf16
              Feb 2 at 21:58












            • $begingroup$
              Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
              $endgroup$
              – Blazej
              Feb 2 at 22:20










            • $begingroup$
              Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
              $endgroup$
              – xf16
              Feb 2 at 22:25










            • $begingroup$
              This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
              $endgroup$
              – Blazej
              Feb 2 at 23:10
















            2












            $begingroup$

            If the values at the endpoints don't match, you can't extend to a continuous function. But you can perform Fourier analysis even with functions admitting some discontinuities. Pretty much any periodic function which is not completely insane admits a Fourier expansion (of course the type and rate of convergence depends on regularity of the function; if you insist on some particular type of convergence, e.g. uniform convergence, then my statement is strictly speaking false).






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
              $endgroup$
              – xf16
              Feb 2 at 21:58












            • $begingroup$
              Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
              $endgroup$
              – Blazej
              Feb 2 at 22:20










            • $begingroup$
              Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
              $endgroup$
              – xf16
              Feb 2 at 22:25










            • $begingroup$
              This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
              $endgroup$
              – Blazej
              Feb 2 at 23:10














            2












            2








            2





            $begingroup$

            If the values at the endpoints don't match, you can't extend to a continuous function. But you can perform Fourier analysis even with functions admitting some discontinuities. Pretty much any periodic function which is not completely insane admits a Fourier expansion (of course the type and rate of convergence depends on regularity of the function; if you insist on some particular type of convergence, e.g. uniform convergence, then my statement is strictly speaking false).






            share|cite|improve this answer









            $endgroup$



            If the values at the endpoints don't match, you can't extend to a continuous function. But you can perform Fourier analysis even with functions admitting some discontinuities. Pretty much any periodic function which is not completely insane admits a Fourier expansion (of course the type and rate of convergence depends on regularity of the function; if you insist on some particular type of convergence, e.g. uniform convergence, then my statement is strictly speaking false).







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered Feb 2 at 21:46









            BlazejBlazej

            1,632620




            1,632620












            • $begingroup$
              Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
              $endgroup$
              – xf16
              Feb 2 at 21:58












            • $begingroup$
              Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
              $endgroup$
              – Blazej
              Feb 2 at 22:20










            • $begingroup$
              Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
              $endgroup$
              – xf16
              Feb 2 at 22:25










            • $begingroup$
              This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
              $endgroup$
              – Blazej
              Feb 2 at 23:10


















            • $begingroup$
              Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
              $endgroup$
              – xf16
              Feb 2 at 21:58












            • $begingroup$
              Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
              $endgroup$
              – Blazej
              Feb 2 at 22:20










            • $begingroup$
              Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
              $endgroup$
              – xf16
              Feb 2 at 22:25










            • $begingroup$
              This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
              $endgroup$
              – Blazej
              Feb 2 at 23:10
















            $begingroup$
            Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
            $endgroup$
            – xf16
            Feb 2 at 21:58






            $begingroup$
            Hi Blazej, is that possible we can use change of variables to change the domain from $[-pi, pi]$ to $[-pi/2, pi/2]$ and then say we can extend this function to a new function $F(x)$ such that in $[-pi/2, pi/2]$ $F(x)$ is just equal to the same values and we require $F(x)$ to be continuous and $F(pi) = F(-pi)$. Then from there, we extend $F(x)$ to be $2pi$-periodic?
            $endgroup$
            – xf16
            Feb 2 at 21:58














            $begingroup$
            Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
            $endgroup$
            – Blazej
            Feb 2 at 22:20




            $begingroup$
            Dear xf16, why do you want to insist on continuity?Given your input on $[-pi,pi]$ and assumption of periodicity you can define your function ambigously everywhere, except for $pi, 3 pi$ etc. Whatever value you choose at this point, Fourier series will be unchanged. Actually the natural choice would be the arithmetic average of the two values, which is $0$ in your case. Then Fourier series converges pointwise.
            $endgroup$
            – Blazej
            Feb 2 at 22:20












            $begingroup$
            Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
            $endgroup$
            – xf16
            Feb 2 at 22:25




            $begingroup$
            Hi Blazej, the reason I hope for continuity is that I kind of want to extend to a function which is continuous on the circle so that I can use Fejer's theorem on this function to say that there exists a trigonometric polynomial to uniformly approximate this function.
            $endgroup$
            – xf16
            Feb 2 at 22:25












            $begingroup$
            This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
            $endgroup$
            – Blazej
            Feb 2 at 23:10




            $begingroup$
            This is impossible if you want to approximate the function on the whole domain. If you extend to a discontinuous function you will get a uniform approximation on compact subsets not including the points of discontinuity. At the point of discontinuity Fourier series converges to the arithmetic average of the two values. Moreover this convergence is only pointwise, not uniform. Look up Gibbs phenomenon.
            $endgroup$
            – Blazej
            Feb 2 at 23:10











            0












            $begingroup$

            If $g(-pi) ne g(pi)$, then you cannot extend to a $2pi$ periodic function because a $2pi$ periodic function $h$ on $mathbb{R}$ is required to satisfy $h(x)=h(x+2pi)$ for all $x$, and your $g$ does not satisfy that for $x=-pi$. You can extend any function defined on $[-pi,pi)$ or on $(-pi,pi]$ to a $2pi$ periodic function on $mathbb{R}$, but not if it is defined on $[-pi,pi]$ with $h(-pi)ne h(pi)$.






            share|cite|improve this answer









            $endgroup$


















              0












              $begingroup$

              If $g(-pi) ne g(pi)$, then you cannot extend to a $2pi$ periodic function because a $2pi$ periodic function $h$ on $mathbb{R}$ is required to satisfy $h(x)=h(x+2pi)$ for all $x$, and your $g$ does not satisfy that for $x=-pi$. You can extend any function defined on $[-pi,pi)$ or on $(-pi,pi]$ to a $2pi$ periodic function on $mathbb{R}$, but not if it is defined on $[-pi,pi]$ with $h(-pi)ne h(pi)$.






              share|cite|improve this answer









              $endgroup$
















                0












                0








                0





                $begingroup$

                If $g(-pi) ne g(pi)$, then you cannot extend to a $2pi$ periodic function because a $2pi$ periodic function $h$ on $mathbb{R}$ is required to satisfy $h(x)=h(x+2pi)$ for all $x$, and your $g$ does not satisfy that for $x=-pi$. You can extend any function defined on $[-pi,pi)$ or on $(-pi,pi]$ to a $2pi$ periodic function on $mathbb{R}$, but not if it is defined on $[-pi,pi]$ with $h(-pi)ne h(pi)$.






                share|cite|improve this answer









                $endgroup$



                If $g(-pi) ne g(pi)$, then you cannot extend to a $2pi$ periodic function because a $2pi$ periodic function $h$ on $mathbb{R}$ is required to satisfy $h(x)=h(x+2pi)$ for all $x$, and your $g$ does not satisfy that for $x=-pi$. You can extend any function defined on $[-pi,pi)$ or on $(-pi,pi]$ to a $2pi$ periodic function on $mathbb{R}$, but not if it is defined on $[-pi,pi]$ with $h(-pi)ne h(pi)$.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Feb 3 at 4:15









                DisintegratingByPartsDisintegratingByParts

                60.4k42681




                60.4k42681






























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