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Show that taylor expansion


Troublesome functional derivative: second term of Euler-Lagrange equationTaylor Series of the Complex Log and Contour IntegrationTaylor theorem for f(x+h)Why is n-th Fréchet derivative symmetric?How do I show that this function is not smooth?$nabla^2 u = 0 $ and integral $u$ around $partial B_rho$Find the Taylor series for $sqrtx$ centered at 16Precisely, what is the polar coordinate system?Change of Variables in Surface Integralfirst order Taylor expansion term of a function multiplied by a dot product of gradients.













2












$begingroup$


Let $M$ be a spherically symmetric $C^2$ manifold. Consider the open ball $B_R$, centered in $xin M$.
Let $yin B_R$, then we define by $rho$ the geodesic distance, beetwen $x$ and $y$.



I don't see the term $-frac12h_p$. Sorry if this is very imprecise, but my point is that I do not understand the indexes of the derivatives of $(*)$, but for me it is not correct that in the derivative the same argument of the function appears and even more multiplying (for instance $h_p(p,theta)p$). Thanks!!!!










share|cite|improve this question











$endgroup$
















    2












    $begingroup$


    Let $M$ be a spherically symmetric $C^2$ manifold. Consider the open ball $B_R$, centered in $xin M$.
    Let $yin B_R$, then we define by $rho$ the geodesic distance, beetwen $x$ and $y$.



    I don't see the term $-frac12h_p$. Sorry if this is very imprecise, but my point is that I do not understand the indexes of the derivatives of $(*)$, but for me it is not correct that in the derivative the same argument of the function appears and even more multiplying (for instance $h_p(p,theta)p$). Thanks!!!!










    share|cite|improve this question











    $endgroup$














      2












      2








      2





      $begingroup$


      Let $M$ be a spherically symmetric $C^2$ manifold. Consider the open ball $B_R$, centered in $xin M$.
      Let $yin B_R$, then we define by $rho$ the geodesic distance, beetwen $x$ and $y$.



      I don't see the term $-frac12h_p$. Sorry if this is very imprecise, but my point is that I do not understand the indexes of the derivatives of $(*)$, but for me it is not correct that in the derivative the same argument of the function appears and even more multiplying (for instance $h_p(p,theta)p$). Thanks!!!!










      share|cite|improve this question











      $endgroup$




      Let $M$ be a spherically symmetric $C^2$ manifold. Consider the open ball $B_R$, centered in $xin M$.
      Let $yin B_R$, then we define by $rho$ the geodesic distance, beetwen $x$ and $y$.



      I don't see the term $-frac12h_p$. Sorry if this is very imprecise, but my point is that I do not understand the indexes of the derivatives of $(*)$, but for me it is not correct that in the derivative the same argument of the function appears and even more multiplying (for instance $h_p(p,theta)p$). Thanks!!!!







      multivariable-calculus taylor-expansion






      share|cite|improve this question















      share|cite|improve this question













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      edited Mar 15 at 20:09







      Pablo_

















      asked Feb 7 at 6:08









      Pablo_Pablo_

      1647




      1647




















          1 Answer
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          $begingroup$

          A full 3-dimensional power series, centered at $x$... that's not something you want to put into spherical coordinates (centered at $x$). The angle variables are singular there. The radius increases in every direction from there. The fundamental premise of the series requires an independent system of coordinates, and you can't have that when the series is centered at the polar origin.



          So, what are we really doing here? We're treating this as a single-variable problem. That $h_rho$ isn't the derivative with respect to radius, it's a directional derivative in the (fixed) $rho$ direction. The series is based entirely on the values of the function along that line, and is used only to calculate values on that line. It is not a Taylor series for the full three-dimensional function.






          share|cite|improve this answer









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            $begingroup$

            A full 3-dimensional power series, centered at $x$... that's not something you want to put into spherical coordinates (centered at $x$). The angle variables are singular there. The radius increases in every direction from there. The fundamental premise of the series requires an independent system of coordinates, and you can't have that when the series is centered at the polar origin.



            So, what are we really doing here? We're treating this as a single-variable problem. That $h_rho$ isn't the derivative with respect to radius, it's a directional derivative in the (fixed) $rho$ direction. The series is based entirely on the values of the function along that line, and is used only to calculate values on that line. It is not a Taylor series for the full three-dimensional function.






            share|cite|improve this answer









            $endgroup$

















              1












              $begingroup$

              A full 3-dimensional power series, centered at $x$... that's not something you want to put into spherical coordinates (centered at $x$). The angle variables are singular there. The radius increases in every direction from there. The fundamental premise of the series requires an independent system of coordinates, and you can't have that when the series is centered at the polar origin.



              So, what are we really doing here? We're treating this as a single-variable problem. That $h_rho$ isn't the derivative with respect to radius, it's a directional derivative in the (fixed) $rho$ direction. The series is based entirely on the values of the function along that line, and is used only to calculate values on that line. It is not a Taylor series for the full three-dimensional function.






              share|cite|improve this answer









              $endgroup$















                1












                1








                1





                $begingroup$

                A full 3-dimensional power series, centered at $x$... that's not something you want to put into spherical coordinates (centered at $x$). The angle variables are singular there. The radius increases in every direction from there. The fundamental premise of the series requires an independent system of coordinates, and you can't have that when the series is centered at the polar origin.



                So, what are we really doing here? We're treating this as a single-variable problem. That $h_rho$ isn't the derivative with respect to radius, it's a directional derivative in the (fixed) $rho$ direction. The series is based entirely on the values of the function along that line, and is used only to calculate values on that line. It is not a Taylor series for the full three-dimensional function.






                share|cite|improve this answer









                $endgroup$



                A full 3-dimensional power series, centered at $x$... that's not something you want to put into spherical coordinates (centered at $x$). The angle variables are singular there. The radius increases in every direction from there. The fundamental premise of the series requires an independent system of coordinates, and you can't have that when the series is centered at the polar origin.



                So, what are we really doing here? We're treating this as a single-variable problem. That $h_rho$ isn't the derivative with respect to radius, it's a directional derivative in the (fixed) $rho$ direction. The series is based entirely on the values of the function along that line, and is used only to calculate values on that line. It is not a Taylor series for the full three-dimensional function.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Feb 11 at 4:22









                jmerryjmerry

                15.3k1632




                15.3k1632



























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