If one expands a function $phi(x,v(theta),t)$ to complex Fourier: $sum_{k=-infty}^{infty} phi_k(x,t)...












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If one expands a function $phi(x,v(theta),t)$ to complex Fourier series marked like: $$phi(x,v(theta),t)=sum_{k=-infty}^{infty} phi_k(x,t) e^{iktheta}$$



then why/how does argument $v$ "disappear"?



Intuitively,



$$phi_k(x,t)=frac{1}{2pi} int_{-pi}^{pi} e^{-int} phi(x,v(theta),t) dsomething$$



Would the notation used perhaps suggest that $dsomething=dv$?



And that by "going backwards" one "recovers" $v$ to $phi(x,v,t)$, when one computes the complex Fourier series?










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    $begingroup$


    If one expands a function $phi(x,v(theta),t)$ to complex Fourier series marked like: $$phi(x,v(theta),t)=sum_{k=-infty}^{infty} phi_k(x,t) e^{iktheta}$$



    then why/how does argument $v$ "disappear"?



    Intuitively,



    $$phi_k(x,t)=frac{1}{2pi} int_{-pi}^{pi} e^{-int} phi(x,v(theta),t) dsomething$$



    Would the notation used perhaps suggest that $dsomething=dv$?



    And that by "going backwards" one "recovers" $v$ to $phi(x,v,t)$, when one computes the complex Fourier series?










    share|cite|improve this question











    $endgroup$















      1












      1








      1





      $begingroup$


      If one expands a function $phi(x,v(theta),t)$ to complex Fourier series marked like: $$phi(x,v(theta),t)=sum_{k=-infty}^{infty} phi_k(x,t) e^{iktheta}$$



      then why/how does argument $v$ "disappear"?



      Intuitively,



      $$phi_k(x,t)=frac{1}{2pi} int_{-pi}^{pi} e^{-int} phi(x,v(theta),t) dsomething$$



      Would the notation used perhaps suggest that $dsomething=dv$?



      And that by "going backwards" one "recovers" $v$ to $phi(x,v,t)$, when one computes the complex Fourier series?










      share|cite|improve this question











      $endgroup$




      If one expands a function $phi(x,v(theta),t)$ to complex Fourier series marked like: $$phi(x,v(theta),t)=sum_{k=-infty}^{infty} phi_k(x,t) e^{iktheta}$$



      then why/how does argument $v$ "disappear"?



      Intuitively,



      $$phi_k(x,t)=frac{1}{2pi} int_{-pi}^{pi} e^{-int} phi(x,v(theta),t) dsomething$$



      Would the notation used perhaps suggest that $dsomething=dv$?



      And that by "going backwards" one "recovers" $v$ to $phi(x,v,t)$, when one computes the complex Fourier series?







      fourier-series






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      edited Dec 23 '18 at 19:04







      mavavilj

















      asked Dec 23 '18 at 17:52









      mavaviljmavavilj

      2,81911137




      2,81911137






















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          $begingroup$

          As given there are added variables and missing variables.



          If given a function of three variables one may expand a function about one of the variables, as in:
          $$phi(x,t,theta) = sum_{n=0}^{infty} phi_{n}(x,t) , e^{i n theta}.$$



          In an integral case a variable can be removed, or evaluated, as in:
          $$int_{a}^{b} phi(x,t,theta) , dtheta = sigma(x,t),$$
          where $sigma$ is the function of two variables after integration.






          share|cite|improve this answer









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            $begingroup$

            As given there are added variables and missing variables.



            If given a function of three variables one may expand a function about one of the variables, as in:
            $$phi(x,t,theta) = sum_{n=0}^{infty} phi_{n}(x,t) , e^{i n theta}.$$



            In an integral case a variable can be removed, or evaluated, as in:
            $$int_{a}^{b} phi(x,t,theta) , dtheta = sigma(x,t),$$
            where $sigma$ is the function of two variables after integration.






            share|cite|improve this answer









            $endgroup$


















              0












              $begingroup$

              As given there are added variables and missing variables.



              If given a function of three variables one may expand a function about one of the variables, as in:
              $$phi(x,t,theta) = sum_{n=0}^{infty} phi_{n}(x,t) , e^{i n theta}.$$



              In an integral case a variable can be removed, or evaluated, as in:
              $$int_{a}^{b} phi(x,t,theta) , dtheta = sigma(x,t),$$
              where $sigma$ is the function of two variables after integration.






              share|cite|improve this answer









              $endgroup$
















                0












                0








                0





                $begingroup$

                As given there are added variables and missing variables.



                If given a function of three variables one may expand a function about one of the variables, as in:
                $$phi(x,t,theta) = sum_{n=0}^{infty} phi_{n}(x,t) , e^{i n theta}.$$



                In an integral case a variable can be removed, or evaluated, as in:
                $$int_{a}^{b} phi(x,t,theta) , dtheta = sigma(x,t),$$
                where $sigma$ is the function of two variables after integration.






                share|cite|improve this answer









                $endgroup$



                As given there are added variables and missing variables.



                If given a function of three variables one may expand a function about one of the variables, as in:
                $$phi(x,t,theta) = sum_{n=0}^{infty} phi_{n}(x,t) , e^{i n theta}.$$



                In an integral case a variable can be removed, or evaluated, as in:
                $$int_{a}^{b} phi(x,t,theta) , dtheta = sigma(x,t),$$
                where $sigma$ is the function of two variables after integration.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Dec 23 '18 at 18:44









                LeucippusLeucippus

                19.6k102871




                19.6k102871






























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