Chapter 2 Corollary 2.7 of Colding and Minicozzi's minimal surfaces book












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I have a question about the last step in the proof of corollary 2.7 in the chapter 2 of Colding and Minicozzi's book A Course in Minimal Surfaces.



Corollary 2.7 If $Sigma^2subsetmathbb{R}^3$ is immersed and minimal, $B_{r_0}^{Sigma}subset Sigma^2$ is an intrinsic disk of radius $r_0$, and $B_{r_0}^{Sigma}cappartialSigma=emptyset$, then
$$something=2(Area(B_{r_0}^{Sigma})-pi r_0^2)le Length(partial B_{r_0}^{Sigma})-2pi r_0^2.$$



The proof of this last inequality is first to notice that $$frac{d^2}{dt^2}Length(partial B_t^{Sigma})ge 0$$ by a previous lemma, therefore
$$tfrac{d}{dt}Length(partial B_t^{Sigma})ge Length(partial B_t^{Sigma})$$



therefore



$$frac{d}{dt}(Length(partial B_t^{Sigma})/t)ge 0.$$



The authors say that the inequality that we want now follows easily. However, I cannot see why. Intuitively the length of $partial B_t^{Sigma}$ should be $c(t)pi t$ and we now know $c(t)$ is increasing.



I guess then we should use the coarea formula somehow to finish it, but I just cannot write it out explicitly. Any help will be appreciated. Thanks in advance!










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    1














    I have a question about the last step in the proof of corollary 2.7 in the chapter 2 of Colding and Minicozzi's book A Course in Minimal Surfaces.



    Corollary 2.7 If $Sigma^2subsetmathbb{R}^3$ is immersed and minimal, $B_{r_0}^{Sigma}subset Sigma^2$ is an intrinsic disk of radius $r_0$, and $B_{r_0}^{Sigma}cappartialSigma=emptyset$, then
    $$something=2(Area(B_{r_0}^{Sigma})-pi r_0^2)le Length(partial B_{r_0}^{Sigma})-2pi r_0^2.$$



    The proof of this last inequality is first to notice that $$frac{d^2}{dt^2}Length(partial B_t^{Sigma})ge 0$$ by a previous lemma, therefore
    $$tfrac{d}{dt}Length(partial B_t^{Sigma})ge Length(partial B_t^{Sigma})$$



    therefore



    $$frac{d}{dt}(Length(partial B_t^{Sigma})/t)ge 0.$$



    The authors say that the inequality that we want now follows easily. However, I cannot see why. Intuitively the length of $partial B_t^{Sigma}$ should be $c(t)pi t$ and we now know $c(t)$ is increasing.



    I guess then we should use the coarea formula somehow to finish it, but I just cannot write it out explicitly. Any help will be appreciated. Thanks in advance!










    share|cite|improve this question

























      1












      1








      1







      I have a question about the last step in the proof of corollary 2.7 in the chapter 2 of Colding and Minicozzi's book A Course in Minimal Surfaces.



      Corollary 2.7 If $Sigma^2subsetmathbb{R}^3$ is immersed and minimal, $B_{r_0}^{Sigma}subset Sigma^2$ is an intrinsic disk of radius $r_0$, and $B_{r_0}^{Sigma}cappartialSigma=emptyset$, then
      $$something=2(Area(B_{r_0}^{Sigma})-pi r_0^2)le Length(partial B_{r_0}^{Sigma})-2pi r_0^2.$$



      The proof of this last inequality is first to notice that $$frac{d^2}{dt^2}Length(partial B_t^{Sigma})ge 0$$ by a previous lemma, therefore
      $$tfrac{d}{dt}Length(partial B_t^{Sigma})ge Length(partial B_t^{Sigma})$$



      therefore



      $$frac{d}{dt}(Length(partial B_t^{Sigma})/t)ge 0.$$



      The authors say that the inequality that we want now follows easily. However, I cannot see why. Intuitively the length of $partial B_t^{Sigma}$ should be $c(t)pi t$ and we now know $c(t)$ is increasing.



      I guess then we should use the coarea formula somehow to finish it, but I just cannot write it out explicitly. Any help will be appreciated. Thanks in advance!










      share|cite|improve this question













      I have a question about the last step in the proof of corollary 2.7 in the chapter 2 of Colding and Minicozzi's book A Course in Minimal Surfaces.



      Corollary 2.7 If $Sigma^2subsetmathbb{R}^3$ is immersed and minimal, $B_{r_0}^{Sigma}subset Sigma^2$ is an intrinsic disk of radius $r_0$, and $B_{r_0}^{Sigma}cappartialSigma=emptyset$, then
      $$something=2(Area(B_{r_0}^{Sigma})-pi r_0^2)le Length(partial B_{r_0}^{Sigma})-2pi r_0^2.$$



      The proof of this last inequality is first to notice that $$frac{d^2}{dt^2}Length(partial B_t^{Sigma})ge 0$$ by a previous lemma, therefore
      $$tfrac{d}{dt}Length(partial B_t^{Sigma})ge Length(partial B_t^{Sigma})$$



      therefore



      $$frac{d}{dt}(Length(partial B_t^{Sigma})/t)ge 0.$$



      The authors say that the inequality that we want now follows easily. However, I cannot see why. Intuitively the length of $partial B_t^{Sigma}$ should be $c(t)pi t$ and we now know $c(t)$ is increasing.



      I guess then we should use the coarea formula somehow to finish it, but I just cannot write it out explicitly. Any help will be appreciated. Thanks in advance!







      differential-geometry minimal-surfaces






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      asked Mar 21 '18 at 10:24









      user392347

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          I integrated the equation:



          $int_0^{r_0} tfrac{d}{dt}Length(partial B_t^Sigma)geq int_0^{r_0}Length(partial B_t^Sigma)$



          Observed that right hand side is equal to $Area(B_{r_0}^Sigma)$



          By integrating by parts left hand side we get:



          $r_0Length(partial B_t^Sigma)- Area(B_{r_0}^Sigma)geq Area(B_{r_0}^Sigma)$



          and hence we conclude by subtracting from both equations $2pi r_0^2$






          share|cite|improve this answer























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            I integrated the equation:



            $int_0^{r_0} tfrac{d}{dt}Length(partial B_t^Sigma)geq int_0^{r_0}Length(partial B_t^Sigma)$



            Observed that right hand side is equal to $Area(B_{r_0}^Sigma)$



            By integrating by parts left hand side we get:



            $r_0Length(partial B_t^Sigma)- Area(B_{r_0}^Sigma)geq Area(B_{r_0}^Sigma)$



            and hence we conclude by subtracting from both equations $2pi r_0^2$






            share|cite|improve this answer




























              0














              I integrated the equation:



              $int_0^{r_0} tfrac{d}{dt}Length(partial B_t^Sigma)geq int_0^{r_0}Length(partial B_t^Sigma)$



              Observed that right hand side is equal to $Area(B_{r_0}^Sigma)$



              By integrating by parts left hand side we get:



              $r_0Length(partial B_t^Sigma)- Area(B_{r_0}^Sigma)geq Area(B_{r_0}^Sigma)$



              and hence we conclude by subtracting from both equations $2pi r_0^2$






              share|cite|improve this answer


























                0












                0








                0






                I integrated the equation:



                $int_0^{r_0} tfrac{d}{dt}Length(partial B_t^Sigma)geq int_0^{r_0}Length(partial B_t^Sigma)$



                Observed that right hand side is equal to $Area(B_{r_0}^Sigma)$



                By integrating by parts left hand side we get:



                $r_0Length(partial B_t^Sigma)- Area(B_{r_0}^Sigma)geq Area(B_{r_0}^Sigma)$



                and hence we conclude by subtracting from both equations $2pi r_0^2$






                share|cite|improve this answer














                I integrated the equation:



                $int_0^{r_0} tfrac{d}{dt}Length(partial B_t^Sigma)geq int_0^{r_0}Length(partial B_t^Sigma)$



                Observed that right hand side is equal to $Area(B_{r_0}^Sigma)$



                By integrating by parts left hand side we get:



                $r_0Length(partial B_t^Sigma)- Area(B_{r_0}^Sigma)geq Area(B_{r_0}^Sigma)$



                and hence we conclude by subtracting from both equations $2pi r_0^2$







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Nov 21 '18 at 8:46

























                answered Oct 24 '18 at 15:27









                F.T.

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