Euler-Lagrange equation for the Brachistochrone problem with friction












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The WolframMathworld website has a page containing the derivation for the brachistochrone with and without friction.



I am able to follow the derivation for the with-friction case up to the point of writing out the Euler-Lagrange equation from the functional derived from the physics of the situation. This is done in step (29) of the demonstration in the linked website.



I am asking for an algebraic demonstration of how applying the Euler-Lagrange equation to the integrand in step (28) results in the expression in step (29).










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    0












    $begingroup$


    The WolframMathworld website has a page containing the derivation for the brachistochrone with and without friction.



    I am able to follow the derivation for the with-friction case up to the point of writing out the Euler-Lagrange equation from the functional derived from the physics of the situation. This is done in step (29) of the demonstration in the linked website.



    I am asking for an algebraic demonstration of how applying the Euler-Lagrange equation to the integrand in step (28) results in the expression in step (29).










    share|cite|improve this question









    $endgroup$















      0












      0








      0


      1



      $begingroup$


      The WolframMathworld website has a page containing the derivation for the brachistochrone with and without friction.



      I am able to follow the derivation for the with-friction case up to the point of writing out the Euler-Lagrange equation from the functional derived from the physics of the situation. This is done in step (29) of the demonstration in the linked website.



      I am asking for an algebraic demonstration of how applying the Euler-Lagrange equation to the integrand in step (28) results in the expression in step (29).










      share|cite|improve this question









      $endgroup$




      The WolframMathworld website has a page containing the derivation for the brachistochrone with and without friction.



      I am able to follow the derivation for the with-friction case up to the point of writing out the Euler-Lagrange equation from the functional derived from the physics of the situation. This is done in step (29) of the demonstration in the linked website.



      I am asking for an algebraic demonstration of how applying the Euler-Lagrange equation to the integrand in step (28) results in the expression in step (29).







      calculus-of-variations euler-lagrange-equation






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      asked Jan 10 at 5:57









      AkaashAkaash

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      285






















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          Let $f(x,y,xi) := sqrt{frac{1 + xi^2}{2g(y - mu x)}}$. Then $$t = int f(x,y,y'),dx$$ and the Euler-Lagrange equation is given by $$frac{partial f}{partial y} - frac{d}{dx}frac{partial f}{partial xi} = 0.$$
          We now compute these derivatives $$frac{partial f}{partial y} = -sqrt{frac{1 + xi^2}{2g}}frac{1}{2(y - mu x)^{3/2}},$$ $$frac{partial f}{partial xi} = frac{xi}{sqrt{(1 + xi^2)2g(y - mu x)}},$$
          and evaluate them at $(x,y(x),y'(x))$.
          The Euler-Lagrange equation can then be rewritten as $$frac{d}{dx}left(frac{y'(x)}{sqrt{(1 + y'(x)^2)2g(y(x) - mu x)}}right) = sqrt{frac{1 + y'(x)^2}{2g}}frac{1}{2(y(x) - mu x)^{3/2}}.$$
          Equation (29) follows upon expanding the derivative on the left hand side in the previous equation. The computations are a little lengthy, but I'm sure you can fill in the details.






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            $begingroup$

            Let $f(x,y,xi) := sqrt{frac{1 + xi^2}{2g(y - mu x)}}$. Then $$t = int f(x,y,y'),dx$$ and the Euler-Lagrange equation is given by $$frac{partial f}{partial y} - frac{d}{dx}frac{partial f}{partial xi} = 0.$$
            We now compute these derivatives $$frac{partial f}{partial y} = -sqrt{frac{1 + xi^2}{2g}}frac{1}{2(y - mu x)^{3/2}},$$ $$frac{partial f}{partial xi} = frac{xi}{sqrt{(1 + xi^2)2g(y - mu x)}},$$
            and evaluate them at $(x,y(x),y'(x))$.
            The Euler-Lagrange equation can then be rewritten as $$frac{d}{dx}left(frac{y'(x)}{sqrt{(1 + y'(x)^2)2g(y(x) - mu x)}}right) = sqrt{frac{1 + y'(x)^2}{2g}}frac{1}{2(y(x) - mu x)^{3/2}}.$$
            Equation (29) follows upon expanding the derivative on the left hand side in the previous equation. The computations are a little lengthy, but I'm sure you can fill in the details.






            share|cite|improve this answer









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              $begingroup$

              Let $f(x,y,xi) := sqrt{frac{1 + xi^2}{2g(y - mu x)}}$. Then $$t = int f(x,y,y'),dx$$ and the Euler-Lagrange equation is given by $$frac{partial f}{partial y} - frac{d}{dx}frac{partial f}{partial xi} = 0.$$
              We now compute these derivatives $$frac{partial f}{partial y} = -sqrt{frac{1 + xi^2}{2g}}frac{1}{2(y - mu x)^{3/2}},$$ $$frac{partial f}{partial xi} = frac{xi}{sqrt{(1 + xi^2)2g(y - mu x)}},$$
              and evaluate them at $(x,y(x),y'(x))$.
              The Euler-Lagrange equation can then be rewritten as $$frac{d}{dx}left(frac{y'(x)}{sqrt{(1 + y'(x)^2)2g(y(x) - mu x)}}right) = sqrt{frac{1 + y'(x)^2}{2g}}frac{1}{2(y(x) - mu x)^{3/2}}.$$
              Equation (29) follows upon expanding the derivative on the left hand side in the previous equation. The computations are a little lengthy, but I'm sure you can fill in the details.






              share|cite|improve this answer









              $endgroup$
















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                $begingroup$

                Let $f(x,y,xi) := sqrt{frac{1 + xi^2}{2g(y - mu x)}}$. Then $$t = int f(x,y,y'),dx$$ and the Euler-Lagrange equation is given by $$frac{partial f}{partial y} - frac{d}{dx}frac{partial f}{partial xi} = 0.$$
                We now compute these derivatives $$frac{partial f}{partial y} = -sqrt{frac{1 + xi^2}{2g}}frac{1}{2(y - mu x)^{3/2}},$$ $$frac{partial f}{partial xi} = frac{xi}{sqrt{(1 + xi^2)2g(y - mu x)}},$$
                and evaluate them at $(x,y(x),y'(x))$.
                The Euler-Lagrange equation can then be rewritten as $$frac{d}{dx}left(frac{y'(x)}{sqrt{(1 + y'(x)^2)2g(y(x) - mu x)}}right) = sqrt{frac{1 + y'(x)^2}{2g}}frac{1}{2(y(x) - mu x)^{3/2}}.$$
                Equation (29) follows upon expanding the derivative on the left hand side in the previous equation. The computations are a little lengthy, but I'm sure you can fill in the details.






                share|cite|improve this answer









                $endgroup$



                Let $f(x,y,xi) := sqrt{frac{1 + xi^2}{2g(y - mu x)}}$. Then $$t = int f(x,y,y'),dx$$ and the Euler-Lagrange equation is given by $$frac{partial f}{partial y} - frac{d}{dx}frac{partial f}{partial xi} = 0.$$
                We now compute these derivatives $$frac{partial f}{partial y} = -sqrt{frac{1 + xi^2}{2g}}frac{1}{2(y - mu x)^{3/2}},$$ $$frac{partial f}{partial xi} = frac{xi}{sqrt{(1 + xi^2)2g(y - mu x)}},$$
                and evaluate them at $(x,y(x),y'(x))$.
                The Euler-Lagrange equation can then be rewritten as $$frac{d}{dx}left(frac{y'(x)}{sqrt{(1 + y'(x)^2)2g(y(x) - mu x)}}right) = sqrt{frac{1 + y'(x)^2}{2g}}frac{1}{2(y(x) - mu x)^{3/2}}.$$
                Equation (29) follows upon expanding the derivative on the left hand side in the previous equation. The computations are a little lengthy, but I'm sure you can fill in the details.







                share|cite|improve this answer












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                share|cite|improve this answer










                answered Jan 10 at 7:11









                GiovanniGiovanni

                5,25351326




                5,25351326






























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