Proof of Discrete Fourier Series Integration Property












0












$begingroup$


In my recent studies of the Fourier Series, I came along to proof the properties of the Fourier Series (just to avoid confusion, not the fourier transform but the series itself in discrete time domain).



I also came into the following property:



The question



For any Discrete Fourier Series whose average is zero (condition for convergence), the following property is met:



$$y[n] = sum_{r=-infty}^{n}x[r]$$
$$Longrightarrow Y_k = frac{1}{1-e^{-ifrac{2pi k}{N}}} X_k$$



so that:



$$y[n] = sum_{k=0}^{N-1} Big(frac{1}{1-e^{-ifrac{2pi k}{N}}} X_kBig) e^{ifrac{2pi k}{N} n}$$



Where $Y_k$ and $X_k$ are the respective Fourier Coefficients, and $N$ is the period.



The question is, ¿how can I prove that? or better, ¿what is wrong with what I have approached?



What I have been able to do



The first thing I did, is to define $y[n]$ as:



$$y[n] = sum_{r=0}^{n} x[r]$$



Since the average per period is zero.



Then, using the linearity property and the displacement in time property, I got into:



$$y[n] = sum_{r=0}^{n} sum_{k=0}^{N-1} X_ke^{-ifrac{2pi k}{N} r} e^{ifrac{2pi k}{N} n} = sum_{k=0}^{N-1} X_kBig( sum_{r=0}^{n}e^{-ifrac{2pi k}{N} r} Big) e^{ifrac{2pi k}{N} n}$$



Using the fact that, from hypothesis, $X_0$ is zero (since $X_0$ represents the average of one period), we can use the geometric progression into the second summatory:



$$y[n] = sum_{k=1}^{N-1}X_k frac{1-(e^{-ifrac{2pi k}{N} (n+1)})}{1-e^{-ifrac{2pi k}{N}}} e^{ifrac{2pi k}{N} n}$$



Which is, after splitting the summatory:



$$y[n] = sum_{k=1}^{N-1} underbrace{Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big)}_{text{Yay!}} e^{ifrac{2pi k}{N} n} - sum_{k=1}^{N-1} Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big) e^{-ifrac{2pi k}{N}}$$



The first expression is what I am looking for, but I haven't been able to work with the second expression/summatory, I suppose that there might be a way to prove that it is zero, but I am not very sure about it, so I don't know if either there is something wrong in the procedure or I am missing something.



Thanks for the help in advance.










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    0












    $begingroup$


    In my recent studies of the Fourier Series, I came along to proof the properties of the Fourier Series (just to avoid confusion, not the fourier transform but the series itself in discrete time domain).



    I also came into the following property:



    The question



    For any Discrete Fourier Series whose average is zero (condition for convergence), the following property is met:



    $$y[n] = sum_{r=-infty}^{n}x[r]$$
    $$Longrightarrow Y_k = frac{1}{1-e^{-ifrac{2pi k}{N}}} X_k$$



    so that:



    $$y[n] = sum_{k=0}^{N-1} Big(frac{1}{1-e^{-ifrac{2pi k}{N}}} X_kBig) e^{ifrac{2pi k}{N} n}$$



    Where $Y_k$ and $X_k$ are the respective Fourier Coefficients, and $N$ is the period.



    The question is, ¿how can I prove that? or better, ¿what is wrong with what I have approached?



    What I have been able to do



    The first thing I did, is to define $y[n]$ as:



    $$y[n] = sum_{r=0}^{n} x[r]$$



    Since the average per period is zero.



    Then, using the linearity property and the displacement in time property, I got into:



    $$y[n] = sum_{r=0}^{n} sum_{k=0}^{N-1} X_ke^{-ifrac{2pi k}{N} r} e^{ifrac{2pi k}{N} n} = sum_{k=0}^{N-1} X_kBig( sum_{r=0}^{n}e^{-ifrac{2pi k}{N} r} Big) e^{ifrac{2pi k}{N} n}$$



    Using the fact that, from hypothesis, $X_0$ is zero (since $X_0$ represents the average of one period), we can use the geometric progression into the second summatory:



    $$y[n] = sum_{k=1}^{N-1}X_k frac{1-(e^{-ifrac{2pi k}{N} (n+1)})}{1-e^{-ifrac{2pi k}{N}}} e^{ifrac{2pi k}{N} n}$$



    Which is, after splitting the summatory:



    $$y[n] = sum_{k=1}^{N-1} underbrace{Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big)}_{text{Yay!}} e^{ifrac{2pi k}{N} n} - sum_{k=1}^{N-1} Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big) e^{-ifrac{2pi k}{N}}$$



    The first expression is what I am looking for, but I haven't been able to work with the second expression/summatory, I suppose that there might be a way to prove that it is zero, but I am not very sure about it, so I don't know if either there is something wrong in the procedure or I am missing something.



    Thanks for the help in advance.










    share|cite|improve this question











    $endgroup$















      0












      0








      0





      $begingroup$


      In my recent studies of the Fourier Series, I came along to proof the properties of the Fourier Series (just to avoid confusion, not the fourier transform but the series itself in discrete time domain).



      I also came into the following property:



      The question



      For any Discrete Fourier Series whose average is zero (condition for convergence), the following property is met:



      $$y[n] = sum_{r=-infty}^{n}x[r]$$
      $$Longrightarrow Y_k = frac{1}{1-e^{-ifrac{2pi k}{N}}} X_k$$



      so that:



      $$y[n] = sum_{k=0}^{N-1} Big(frac{1}{1-e^{-ifrac{2pi k}{N}}} X_kBig) e^{ifrac{2pi k}{N} n}$$



      Where $Y_k$ and $X_k$ are the respective Fourier Coefficients, and $N$ is the period.



      The question is, ¿how can I prove that? or better, ¿what is wrong with what I have approached?



      What I have been able to do



      The first thing I did, is to define $y[n]$ as:



      $$y[n] = sum_{r=0}^{n} x[r]$$



      Since the average per period is zero.



      Then, using the linearity property and the displacement in time property, I got into:



      $$y[n] = sum_{r=0}^{n} sum_{k=0}^{N-1} X_ke^{-ifrac{2pi k}{N} r} e^{ifrac{2pi k}{N} n} = sum_{k=0}^{N-1} X_kBig( sum_{r=0}^{n}e^{-ifrac{2pi k}{N} r} Big) e^{ifrac{2pi k}{N} n}$$



      Using the fact that, from hypothesis, $X_0$ is zero (since $X_0$ represents the average of one period), we can use the geometric progression into the second summatory:



      $$y[n] = sum_{k=1}^{N-1}X_k frac{1-(e^{-ifrac{2pi k}{N} (n+1)})}{1-e^{-ifrac{2pi k}{N}}} e^{ifrac{2pi k}{N} n}$$



      Which is, after splitting the summatory:



      $$y[n] = sum_{k=1}^{N-1} underbrace{Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big)}_{text{Yay!}} e^{ifrac{2pi k}{N} n} - sum_{k=1}^{N-1} Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big) e^{-ifrac{2pi k}{N}}$$



      The first expression is what I am looking for, but I haven't been able to work with the second expression/summatory, I suppose that there might be a way to prove that it is zero, but I am not very sure about it, so I don't know if either there is something wrong in the procedure or I am missing something.



      Thanks for the help in advance.










      share|cite|improve this question











      $endgroup$




      In my recent studies of the Fourier Series, I came along to proof the properties of the Fourier Series (just to avoid confusion, not the fourier transform but the series itself in discrete time domain).



      I also came into the following property:



      The question



      For any Discrete Fourier Series whose average is zero (condition for convergence), the following property is met:



      $$y[n] = sum_{r=-infty}^{n}x[r]$$
      $$Longrightarrow Y_k = frac{1}{1-e^{-ifrac{2pi k}{N}}} X_k$$



      so that:



      $$y[n] = sum_{k=0}^{N-1} Big(frac{1}{1-e^{-ifrac{2pi k}{N}}} X_kBig) e^{ifrac{2pi k}{N} n}$$



      Where $Y_k$ and $X_k$ are the respective Fourier Coefficients, and $N$ is the period.



      The question is, ¿how can I prove that? or better, ¿what is wrong with what I have approached?



      What I have been able to do



      The first thing I did, is to define $y[n]$ as:



      $$y[n] = sum_{r=0}^{n} x[r]$$



      Since the average per period is zero.



      Then, using the linearity property and the displacement in time property, I got into:



      $$y[n] = sum_{r=0}^{n} sum_{k=0}^{N-1} X_ke^{-ifrac{2pi k}{N} r} e^{ifrac{2pi k}{N} n} = sum_{k=0}^{N-1} X_kBig( sum_{r=0}^{n}e^{-ifrac{2pi k}{N} r} Big) e^{ifrac{2pi k}{N} n}$$



      Using the fact that, from hypothesis, $X_0$ is zero (since $X_0$ represents the average of one period), we can use the geometric progression into the second summatory:



      $$y[n] = sum_{k=1}^{N-1}X_k frac{1-(e^{-ifrac{2pi k}{N} (n+1)})}{1-e^{-ifrac{2pi k}{N}}} e^{ifrac{2pi k}{N} n}$$



      Which is, after splitting the summatory:



      $$y[n] = sum_{k=1}^{N-1} underbrace{Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big)}_{text{Yay!}} e^{ifrac{2pi k}{N} n} - sum_{k=1}^{N-1} Big(frac{1}{1-e^{-frac{2pi k}{N}}}X_k Big) e^{-ifrac{2pi k}{N}}$$



      The first expression is what I am looking for, but I haven't been able to work with the second expression/summatory, I suppose that there might be a way to prove that it is zero, but I am not very sure about it, so I don't know if either there is something wrong in the procedure or I am missing something.



      Thanks for the help in advance.







      discrete-mathematics proof-explanation fourier-series






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      edited Jan 26 at 19:55







      Zumbock

















      asked Jan 26 at 19:08









      ZumbockZumbock

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      135






















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          $begingroup$

          Let $alpha=e^{frac{-2pi ik}{N}}$ to ease the notation a little bit. Substituting into the definiton of DTFS yields:



          $$begin{align}Y_k &=sum_{n=0}^{N-1}sum_{r=0}^nx[r]alpha^n=sum_{r=0}^{N-1}x[r]sum_{n=r}^{N-1}alpha^n=-sum_{r=0}^{N-1}x[r]sum_{n=0}^{r-1}alpha^n=sum_{r=0}^{N-1}x[r]frac{alpha^r-1}{1-alpha} \ &=frac{1}{1-alpha}left(sum_{r=0}^{N-1}x[r]alpha^r+sum_{r=0}^{N-1}x[r]right)=frac{X_k}{1-alpha}end{align}$$



          since $sum_{r=0}^{N-1}x[r]=0$, and the other term is the definition of DTFS of $x[n]$.






          share|cite|improve this answer









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          • $begingroup$
            Thanks for the answer. Can't even imagine the answer was this easy.
            $endgroup$
            – Zumbock
            Jan 26 at 20:29











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          $begingroup$

          Let $alpha=e^{frac{-2pi ik}{N}}$ to ease the notation a little bit. Substituting into the definiton of DTFS yields:



          $$begin{align}Y_k &=sum_{n=0}^{N-1}sum_{r=0}^nx[r]alpha^n=sum_{r=0}^{N-1}x[r]sum_{n=r}^{N-1}alpha^n=-sum_{r=0}^{N-1}x[r]sum_{n=0}^{r-1}alpha^n=sum_{r=0}^{N-1}x[r]frac{alpha^r-1}{1-alpha} \ &=frac{1}{1-alpha}left(sum_{r=0}^{N-1}x[r]alpha^r+sum_{r=0}^{N-1}x[r]right)=frac{X_k}{1-alpha}end{align}$$



          since $sum_{r=0}^{N-1}x[r]=0$, and the other term is the definition of DTFS of $x[n]$.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            Thanks for the answer. Can't even imagine the answer was this easy.
            $endgroup$
            – Zumbock
            Jan 26 at 20:29
















          0












          $begingroup$

          Let $alpha=e^{frac{-2pi ik}{N}}$ to ease the notation a little bit. Substituting into the definiton of DTFS yields:



          $$begin{align}Y_k &=sum_{n=0}^{N-1}sum_{r=0}^nx[r]alpha^n=sum_{r=0}^{N-1}x[r]sum_{n=r}^{N-1}alpha^n=-sum_{r=0}^{N-1}x[r]sum_{n=0}^{r-1}alpha^n=sum_{r=0}^{N-1}x[r]frac{alpha^r-1}{1-alpha} \ &=frac{1}{1-alpha}left(sum_{r=0}^{N-1}x[r]alpha^r+sum_{r=0}^{N-1}x[r]right)=frac{X_k}{1-alpha}end{align}$$



          since $sum_{r=0}^{N-1}x[r]=0$, and the other term is the definition of DTFS of $x[n]$.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            Thanks for the answer. Can't even imagine the answer was this easy.
            $endgroup$
            – Zumbock
            Jan 26 at 20:29














          0












          0








          0





          $begingroup$

          Let $alpha=e^{frac{-2pi ik}{N}}$ to ease the notation a little bit. Substituting into the definiton of DTFS yields:



          $$begin{align}Y_k &=sum_{n=0}^{N-1}sum_{r=0}^nx[r]alpha^n=sum_{r=0}^{N-1}x[r]sum_{n=r}^{N-1}alpha^n=-sum_{r=0}^{N-1}x[r]sum_{n=0}^{r-1}alpha^n=sum_{r=0}^{N-1}x[r]frac{alpha^r-1}{1-alpha} \ &=frac{1}{1-alpha}left(sum_{r=0}^{N-1}x[r]alpha^r+sum_{r=0}^{N-1}x[r]right)=frac{X_k}{1-alpha}end{align}$$



          since $sum_{r=0}^{N-1}x[r]=0$, and the other term is the definition of DTFS of $x[n]$.






          share|cite|improve this answer









          $endgroup$



          Let $alpha=e^{frac{-2pi ik}{N}}$ to ease the notation a little bit. Substituting into the definiton of DTFS yields:



          $$begin{align}Y_k &=sum_{n=0}^{N-1}sum_{r=0}^nx[r]alpha^n=sum_{r=0}^{N-1}x[r]sum_{n=r}^{N-1}alpha^n=-sum_{r=0}^{N-1}x[r]sum_{n=0}^{r-1}alpha^n=sum_{r=0}^{N-1}x[r]frac{alpha^r-1}{1-alpha} \ &=frac{1}{1-alpha}left(sum_{r=0}^{N-1}x[r]alpha^r+sum_{r=0}^{N-1}x[r]right)=frac{X_k}{1-alpha}end{align}$$



          since $sum_{r=0}^{N-1}x[r]=0$, and the other term is the definition of DTFS of $x[n]$.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Jan 26 at 20:09









          gunesgunes

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          3747












          • $begingroup$
            Thanks for the answer. Can't even imagine the answer was this easy.
            $endgroup$
            – Zumbock
            Jan 26 at 20:29


















          • $begingroup$
            Thanks for the answer. Can't even imagine the answer was this easy.
            $endgroup$
            – Zumbock
            Jan 26 at 20:29
















          $begingroup$
          Thanks for the answer. Can't even imagine the answer was this easy.
          $endgroup$
          – Zumbock
          Jan 26 at 20:29




          $begingroup$
          Thanks for the answer. Can't even imagine the answer was this easy.
          $endgroup$
          – Zumbock
          Jan 26 at 20:29


















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