Covariant derivative in cylindrical coordinates












2












$begingroup$


I am confused by the Wolfram article on cylindrical coordinates. Specifically, I do not understand how they go from equation (48) to equations (49)-(57).



Equation (48) shows that the covariant derivative is:



$$A_{j;k} = frac{1}{g_{kk}}frac{partial A_j}{partial x_k} - Gamma^i_{jk}A_i$$



The next few equations expand this for the case of cylindrical coordinates, equation (50) is:



$$A_{r;theta} = frac{1}{r}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



The contravariant metric tensor has non-zero elements:



$$g^{11} = 1$$
$$g^{22} = frac{1}{r^2}$$
$$g^{33} = 1$$



And the Christoffel symbols of the second kind have non-zero elements:



$$Gamma^1_{22} = -r$$
$$Gamma^2_{12} = frac{1}{r}$$
$$Gamma^2_{21} = frac{1}{r}$$



If I plug these values back into their definition of the covariant derivative I get for equation (50):



$$A_{r;theta} = frac{1}{r^2}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



Why does this not match up with their results?










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    2












    $begingroup$


    I am confused by the Wolfram article on cylindrical coordinates. Specifically, I do not understand how they go from equation (48) to equations (49)-(57).



    Equation (48) shows that the covariant derivative is:



    $$A_{j;k} = frac{1}{g_{kk}}frac{partial A_j}{partial x_k} - Gamma^i_{jk}A_i$$



    The next few equations expand this for the case of cylindrical coordinates, equation (50) is:



    $$A_{r;theta} = frac{1}{r}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



    The contravariant metric tensor has non-zero elements:



    $$g^{11} = 1$$
    $$g^{22} = frac{1}{r^2}$$
    $$g^{33} = 1$$



    And the Christoffel symbols of the second kind have non-zero elements:



    $$Gamma^1_{22} = -r$$
    $$Gamma^2_{12} = frac{1}{r}$$
    $$Gamma^2_{21} = frac{1}{r}$$



    If I plug these values back into their definition of the covariant derivative I get for equation (50):



    $$A_{r;theta} = frac{1}{r^2}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



    Why does this not match up with their results?










    share|cite|improve this question











    $endgroup$















      2












      2








      2


      2



      $begingroup$


      I am confused by the Wolfram article on cylindrical coordinates. Specifically, I do not understand how they go from equation (48) to equations (49)-(57).



      Equation (48) shows that the covariant derivative is:



      $$A_{j;k} = frac{1}{g_{kk}}frac{partial A_j}{partial x_k} - Gamma^i_{jk}A_i$$



      The next few equations expand this for the case of cylindrical coordinates, equation (50) is:



      $$A_{r;theta} = frac{1}{r}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



      The contravariant metric tensor has non-zero elements:



      $$g^{11} = 1$$
      $$g^{22} = frac{1}{r^2}$$
      $$g^{33} = 1$$



      And the Christoffel symbols of the second kind have non-zero elements:



      $$Gamma^1_{22} = -r$$
      $$Gamma^2_{12} = frac{1}{r}$$
      $$Gamma^2_{21} = frac{1}{r}$$



      If I plug these values back into their definition of the covariant derivative I get for equation (50):



      $$A_{r;theta} = frac{1}{r^2}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



      Why does this not match up with their results?










      share|cite|improve this question











      $endgroup$




      I am confused by the Wolfram article on cylindrical coordinates. Specifically, I do not understand how they go from equation (48) to equations (49)-(57).



      Equation (48) shows that the covariant derivative is:



      $$A_{j;k} = frac{1}{g_{kk}}frac{partial A_j}{partial x_k} - Gamma^i_{jk}A_i$$



      The next few equations expand this for the case of cylindrical coordinates, equation (50) is:



      $$A_{r;theta} = frac{1}{r}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



      The contravariant metric tensor has non-zero elements:



      $$g^{11} = 1$$
      $$g^{22} = frac{1}{r^2}$$
      $$g^{33} = 1$$



      And the Christoffel symbols of the second kind have non-zero elements:



      $$Gamma^1_{22} = -r$$
      $$Gamma^2_{12} = frac{1}{r}$$
      $$Gamma^2_{21} = frac{1}{r}$$



      If I plug these values back into their definition of the covariant derivative I get for equation (50):



      $$A_{r;theta} = frac{1}{r^2}frac{partial A_r}{partial theta} - frac{A_theta}{r}$$



      Why does this not match up with their results?







      differential-geometry






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      edited Jun 16 '14 at 20:11







      OSE

















      asked Jun 13 '14 at 18:44









      OSEOSE

      95110




      95110






















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          $begingroup$

          The thing you forgot is the scale factor $frac{1}{r}$ given in equation (14). See Scale Factor in Mathworld.






          share|cite|improve this answer









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          • $begingroup$
            I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
            $endgroup$
            – OSE
            Jun 13 '14 at 21:05












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          $begingroup$

          The thing you forgot is the scale factor $frac{1}{r}$ given in equation (14). See Scale Factor in Mathworld.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
            $endgroup$
            – OSE
            Jun 13 '14 at 21:05
















          0












          $begingroup$

          The thing you forgot is the scale factor $frac{1}{r}$ given in equation (14). See Scale Factor in Mathworld.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
            $endgroup$
            – OSE
            Jun 13 '14 at 21:05














          0












          0








          0





          $begingroup$

          The thing you forgot is the scale factor $frac{1}{r}$ given in equation (14). See Scale Factor in Mathworld.






          share|cite|improve this answer









          $endgroup$



          The thing you forgot is the scale factor $frac{1}{r}$ given in equation (14). See Scale Factor in Mathworld.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Jun 13 '14 at 20:10









          Mark FischlerMark Fischler

          34k12552




          34k12552












          • $begingroup$
            I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
            $endgroup$
            – OSE
            Jun 13 '14 at 21:05


















          • $begingroup$
            I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
            $endgroup$
            – OSE
            Jun 13 '14 at 21:05
















          $begingroup$
          I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
          $endgroup$
          – OSE
          Jun 13 '14 at 21:05




          $begingroup$
          I don't see how the scale factor is involved with the first term. Could you explain it a little more explicitly? My understanding of this is a little shaky...
          $endgroup$
          – OSE
          Jun 13 '14 at 21:05


















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