Lineintegral $int_{gamma}|z|^2dz$ over ellipse











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Let $a,binmathbb{R}_{>0}$ and $gamma: [0,2pi]rightarrowmathbb{C},tmapsto acos(t)+ibsin(t)$



calculate the line integral



$int_{gamma}|z|^2dz$



My calculation turns out to be really ugly. Is there maybe a "nice" way to calculate this integral?










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    up vote
    1
    down vote

    favorite












    Let $a,binmathbb{R}_{>0}$ and $gamma: [0,2pi]rightarrowmathbb{C},tmapsto acos(t)+ibsin(t)$



    calculate the line integral



    $int_{gamma}|z|^2dz$



    My calculation turns out to be really ugly. Is there maybe a "nice" way to calculate this integral?










    share|cite|improve this question
























      up vote
      1
      down vote

      favorite









      up vote
      1
      down vote

      favorite











      Let $a,binmathbb{R}_{>0}$ and $gamma: [0,2pi]rightarrowmathbb{C},tmapsto acos(t)+ibsin(t)$



      calculate the line integral



      $int_{gamma}|z|^2dz$



      My calculation turns out to be really ugly. Is there maybe a "nice" way to calculate this integral?










      share|cite|improve this question













      Let $a,binmathbb{R}_{>0}$ and $gamma: [0,2pi]rightarrowmathbb{C},tmapsto acos(t)+ibsin(t)$



      calculate the line integral



      $int_{gamma}|z|^2dz$



      My calculation turns out to be really ugly. Is there maybe a "nice" way to calculate this integral?







      integration complex-analysis complex-integration line-integrals






      share|cite|improve this question













      share|cite|improve this question











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      asked Nov 20 at 15:49









      Christian Singer

      341113




      341113






















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          The integrals are not ugly at all. You obtain
          $$int_gamma|z|^2>dz=int_{omega-pi}^{omega+pi}bigl(acos^2 t+b^2sin^2 tbigr)(-asin t+ibcos t)>dt ,$$
          whereby $omega$ can be chosen at will, due to periodicity. Choose $omega:=0$ for the real part, then $omega:={piover2}$ for the imaginary part, and note that the respective integrands are odd with respect to these points.






          share|cite|improve this answer





















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            1 Answer
            1






            active

            oldest

            votes








            1 Answer
            1






            active

            oldest

            votes









            active

            oldest

            votes






            active

            oldest

            votes








            up vote
            3
            down vote



            accepted










            The integrals are not ugly at all. You obtain
            $$int_gamma|z|^2>dz=int_{omega-pi}^{omega+pi}bigl(acos^2 t+b^2sin^2 tbigr)(-asin t+ibcos t)>dt ,$$
            whereby $omega$ can be chosen at will, due to periodicity. Choose $omega:=0$ for the real part, then $omega:={piover2}$ for the imaginary part, and note that the respective integrands are odd with respect to these points.






            share|cite|improve this answer

























              up vote
              3
              down vote



              accepted










              The integrals are not ugly at all. You obtain
              $$int_gamma|z|^2>dz=int_{omega-pi}^{omega+pi}bigl(acos^2 t+b^2sin^2 tbigr)(-asin t+ibcos t)>dt ,$$
              whereby $omega$ can be chosen at will, due to periodicity. Choose $omega:=0$ for the real part, then $omega:={piover2}$ for the imaginary part, and note that the respective integrands are odd with respect to these points.






              share|cite|improve this answer























                up vote
                3
                down vote



                accepted







                up vote
                3
                down vote



                accepted






                The integrals are not ugly at all. You obtain
                $$int_gamma|z|^2>dz=int_{omega-pi}^{omega+pi}bigl(acos^2 t+b^2sin^2 tbigr)(-asin t+ibcos t)>dt ,$$
                whereby $omega$ can be chosen at will, due to periodicity. Choose $omega:=0$ for the real part, then $omega:={piover2}$ for the imaginary part, and note that the respective integrands are odd with respect to these points.






                share|cite|improve this answer












                The integrals are not ugly at all. You obtain
                $$int_gamma|z|^2>dz=int_{omega-pi}^{omega+pi}bigl(acos^2 t+b^2sin^2 tbigr)(-asin t+ibcos t)>dt ,$$
                whereby $omega$ can be chosen at will, due to periodicity. Choose $omega:=0$ for the real part, then $omega:={piover2}$ for the imaginary part, and note that the respective integrands are odd with respect to these points.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Nov 20 at 16:22









                Christian Blatter

                171k7111325




                171k7111325






























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