Expansion of function in polar coordinates












3












$begingroup$


I'd like to expand a function in polar coordinates to something that splits radius and angle



$f(r,theta)=sum_i A_i(r)B_i(theta)$



I've found some hints on the internet by the name of polar Fourier transform, but I didn't find a Wikipedia page or a good explanation. What is the name for such a decomposition and how to find a basic description?



Is using Bessel function the only way to find such a factor decomposition?



Is it possible (or useful) to write this operation in complex number representation for the 2D coordinates?










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  • $begingroup$
    I like how this is explained in the book on harmonic analysis by Stein and Weiss, chapter on spherical harmonics.
    $endgroup$
    – Giuseppe Negro
    Oct 30 '18 at 10:02
















3












$begingroup$


I'd like to expand a function in polar coordinates to something that splits radius and angle



$f(r,theta)=sum_i A_i(r)B_i(theta)$



I've found some hints on the internet by the name of polar Fourier transform, but I didn't find a Wikipedia page or a good explanation. What is the name for such a decomposition and how to find a basic description?



Is using Bessel function the only way to find such a factor decomposition?



Is it possible (or useful) to write this operation in complex number representation for the 2D coordinates?










share|cite|improve this question











$endgroup$












  • $begingroup$
    I like how this is explained in the book on harmonic analysis by Stein and Weiss, chapter on spherical harmonics.
    $endgroup$
    – Giuseppe Negro
    Oct 30 '18 at 10:02














3












3








3


3



$begingroup$


I'd like to expand a function in polar coordinates to something that splits radius and angle



$f(r,theta)=sum_i A_i(r)B_i(theta)$



I've found some hints on the internet by the name of polar Fourier transform, but I didn't find a Wikipedia page or a good explanation. What is the name for such a decomposition and how to find a basic description?



Is using Bessel function the only way to find such a factor decomposition?



Is it possible (or useful) to write this operation in complex number representation for the 2D coordinates?










share|cite|improve this question











$endgroup$




I'd like to expand a function in polar coordinates to something that splits radius and angle



$f(r,theta)=sum_i A_i(r)B_i(theta)$



I've found some hints on the internet by the name of polar Fourier transform, but I didn't find a Wikipedia page or a good explanation. What is the name for such a decomposition and how to find a basic description?



Is using Bessel function the only way to find such a factor decomposition?



Is it possible (or useful) to write this operation in complex number representation for the 2D coordinates?







fourier-series






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edited Jan 27 '15 at 14:59









Arjang

5,63062363




5,63062363










asked Jan 27 '15 at 14:43









GerenukGerenuk

1,0532920




1,0532920












  • $begingroup$
    I like how this is explained in the book on harmonic analysis by Stein and Weiss, chapter on spherical harmonics.
    $endgroup$
    – Giuseppe Negro
    Oct 30 '18 at 10:02


















  • $begingroup$
    I like how this is explained in the book on harmonic analysis by Stein and Weiss, chapter on spherical harmonics.
    $endgroup$
    – Giuseppe Negro
    Oct 30 '18 at 10:02
















$begingroup$
I like how this is explained in the book on harmonic analysis by Stein and Weiss, chapter on spherical harmonics.
$endgroup$
– Giuseppe Negro
Oct 30 '18 at 10:02




$begingroup$
I like how this is explained in the book on harmonic analysis by Stein and Weiss, chapter on spherical harmonics.
$endgroup$
– Giuseppe Negro
Oct 30 '18 at 10:02










1 Answer
1






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oldest

votes


















1












$begingroup$

Consider the 2D Fourier transform in rectangular coordinates,



$$
F(u,v) = int_{-infty}^{infty} left[ int_{-infty}^{infty} f(x,y)e^{2ipi ux}dx right]e^{2ipi vy}dy
$$
One can take 1D FT in X direction then in Y direction. But for Polar coordinates the expression changes,
Let , $ux+vy = rho r cos (phi-theta)$, then
$$
F(u,v) = int_{0}^{2pi} int_{0}^{infty} f(r,theta)e^{2ipirho r cos(phi- theta)}rdr dtheta
$$
Now the function $f(r,theta) $ has seperability in polar coordinates if it can be written in the form ,
$$f(r,theta)= f_r(r)f_{theta}(theta)$$
Then the function $f(r,theta)$ is a circularly symmetric with $f_{theta}(theta)=1$ , examples include like that of a cylinder etc. Read more about Hankel transform, 2D Polar Fourier transform and functions of this type.






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    protected by user26857 Nov 4 '15 at 22:03



    Thank you for your interest in this question.
    Because it has attracted low-quality or spam answers that had to be removed, posting an answer now requires 10 reputation on this site (the association bonus does not count).



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    1 Answer
    1






    active

    oldest

    votes








    1 Answer
    1






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes









    1












    $begingroup$

    Consider the 2D Fourier transform in rectangular coordinates,



    $$
    F(u,v) = int_{-infty}^{infty} left[ int_{-infty}^{infty} f(x,y)e^{2ipi ux}dx right]e^{2ipi vy}dy
    $$
    One can take 1D FT in X direction then in Y direction. But for Polar coordinates the expression changes,
    Let , $ux+vy = rho r cos (phi-theta)$, then
    $$
    F(u,v) = int_{0}^{2pi} int_{0}^{infty} f(r,theta)e^{2ipirho r cos(phi- theta)}rdr dtheta
    $$
    Now the function $f(r,theta) $ has seperability in polar coordinates if it can be written in the form ,
    $$f(r,theta)= f_r(r)f_{theta}(theta)$$
    Then the function $f(r,theta)$ is a circularly symmetric with $f_{theta}(theta)=1$ , examples include like that of a cylinder etc. Read more about Hankel transform, 2D Polar Fourier transform and functions of this type.






    share|cite|improve this answer











    $endgroup$


















      1












      $begingroup$

      Consider the 2D Fourier transform in rectangular coordinates,



      $$
      F(u,v) = int_{-infty}^{infty} left[ int_{-infty}^{infty} f(x,y)e^{2ipi ux}dx right]e^{2ipi vy}dy
      $$
      One can take 1D FT in X direction then in Y direction. But for Polar coordinates the expression changes,
      Let , $ux+vy = rho r cos (phi-theta)$, then
      $$
      F(u,v) = int_{0}^{2pi} int_{0}^{infty} f(r,theta)e^{2ipirho r cos(phi- theta)}rdr dtheta
      $$
      Now the function $f(r,theta) $ has seperability in polar coordinates if it can be written in the form ,
      $$f(r,theta)= f_r(r)f_{theta}(theta)$$
      Then the function $f(r,theta)$ is a circularly symmetric with $f_{theta}(theta)=1$ , examples include like that of a cylinder etc. Read more about Hankel transform, 2D Polar Fourier transform and functions of this type.






      share|cite|improve this answer











      $endgroup$
















        1












        1








        1





        $begingroup$

        Consider the 2D Fourier transform in rectangular coordinates,



        $$
        F(u,v) = int_{-infty}^{infty} left[ int_{-infty}^{infty} f(x,y)e^{2ipi ux}dx right]e^{2ipi vy}dy
        $$
        One can take 1D FT in X direction then in Y direction. But for Polar coordinates the expression changes,
        Let , $ux+vy = rho r cos (phi-theta)$, then
        $$
        F(u,v) = int_{0}^{2pi} int_{0}^{infty} f(r,theta)e^{2ipirho r cos(phi- theta)}rdr dtheta
        $$
        Now the function $f(r,theta) $ has seperability in polar coordinates if it can be written in the form ,
        $$f(r,theta)= f_r(r)f_{theta}(theta)$$
        Then the function $f(r,theta)$ is a circularly symmetric with $f_{theta}(theta)=1$ , examples include like that of a cylinder etc. Read more about Hankel transform, 2D Polar Fourier transform and functions of this type.






        share|cite|improve this answer











        $endgroup$



        Consider the 2D Fourier transform in rectangular coordinates,



        $$
        F(u,v) = int_{-infty}^{infty} left[ int_{-infty}^{infty} f(x,y)e^{2ipi ux}dx right]e^{2ipi vy}dy
        $$
        One can take 1D FT in X direction then in Y direction. But for Polar coordinates the expression changes,
        Let , $ux+vy = rho r cos (phi-theta)$, then
        $$
        F(u,v) = int_{0}^{2pi} int_{0}^{infty} f(r,theta)e^{2ipirho r cos(phi- theta)}rdr dtheta
        $$
        Now the function $f(r,theta) $ has seperability in polar coordinates if it can be written in the form ,
        $$f(r,theta)= f_r(r)f_{theta}(theta)$$
        Then the function $f(r,theta)$ is a circularly symmetric with $f_{theta}(theta)=1$ , examples include like that of a cylinder etc. Read more about Hankel transform, 2D Polar Fourier transform and functions of this type.







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Nov 6 '17 at 9:36









        Faraad Armwood

        7,5442719




        7,5442719










        answered Aug 2 '15 at 18:37









        Syed Alam AbbasSyed Alam Abbas

        335411




        335411

















            protected by user26857 Nov 4 '15 at 22:03



            Thank you for your interest in this question.
            Because it has attracted low-quality or spam answers that had to be removed, posting an answer now requires 10 reputation on this site (the association bonus does not count).



            Would you like to answer one of these unanswered questions instead?



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