a question related to calculus of variations












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Consider a particle with coordinates $(x(t),y(t))$ on a smooth curve $phi(x,y)=0$. If the particle moves from $(x(0),y(0))$ to $(x(tau),y(tau))$ for $tau >0$ such that its kinetic energy is minimized, then



$(a)$ $frac{ddot{x}}{phi_x}=frac{ddot{y}}{phi_y}$.



$(b)$ $dot{x}^2(0)+dot{y}^2(0)=dot{x}^2(tau)+dot{y}^2(tau)$.



$(c)$ $dot{x}phi_x+dot{y}phi_y=0$.



$(d)$ $dot{x}^2(0)=dot{x}^2(tau)$.



Now, if we consider this problem as minimizing a functional $J[x(t),y(t)]=int_0^tau F(x,dot{x},y,dot{y},t)dt$ in two dependent variables representing coordinates and one independent variable representing time, then Euler-Lagrange equation will give a family of extremals from which we can conclude the answer. But I am unable to find a way to relate the K.E. as a functional as written above, and include the curve $phi(x,y)=0$ in the same. So is there another method for this problem or am I on the right track? Any help will be appreciated.










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    $begingroup$


    Consider a particle with coordinates $(x(t),y(t))$ on a smooth curve $phi(x,y)=0$. If the particle moves from $(x(0),y(0))$ to $(x(tau),y(tau))$ for $tau >0$ such that its kinetic energy is minimized, then



    $(a)$ $frac{ddot{x}}{phi_x}=frac{ddot{y}}{phi_y}$.



    $(b)$ $dot{x}^2(0)+dot{y}^2(0)=dot{x}^2(tau)+dot{y}^2(tau)$.



    $(c)$ $dot{x}phi_x+dot{y}phi_y=0$.



    $(d)$ $dot{x}^2(0)=dot{x}^2(tau)$.



    Now, if we consider this problem as minimizing a functional $J[x(t),y(t)]=int_0^tau F(x,dot{x},y,dot{y},t)dt$ in two dependent variables representing coordinates and one independent variable representing time, then Euler-Lagrange equation will give a family of extremals from which we can conclude the answer. But I am unable to find a way to relate the K.E. as a functional as written above, and include the curve $phi(x,y)=0$ in the same. So is there another method for this problem or am I on the right track? Any help will be appreciated.










    share|cite|improve this question









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      Consider a particle with coordinates $(x(t),y(t))$ on a smooth curve $phi(x,y)=0$. If the particle moves from $(x(0),y(0))$ to $(x(tau),y(tau))$ for $tau >0$ such that its kinetic energy is minimized, then



      $(a)$ $frac{ddot{x}}{phi_x}=frac{ddot{y}}{phi_y}$.



      $(b)$ $dot{x}^2(0)+dot{y}^2(0)=dot{x}^2(tau)+dot{y}^2(tau)$.



      $(c)$ $dot{x}phi_x+dot{y}phi_y=0$.



      $(d)$ $dot{x}^2(0)=dot{x}^2(tau)$.



      Now, if we consider this problem as minimizing a functional $J[x(t),y(t)]=int_0^tau F(x,dot{x},y,dot{y},t)dt$ in two dependent variables representing coordinates and one independent variable representing time, then Euler-Lagrange equation will give a family of extremals from which we can conclude the answer. But I am unable to find a way to relate the K.E. as a functional as written above, and include the curve $phi(x,y)=0$ in the same. So is there another method for this problem or am I on the right track? Any help will be appreciated.










      share|cite|improve this question









      $endgroup$




      Consider a particle with coordinates $(x(t),y(t))$ on a smooth curve $phi(x,y)=0$. If the particle moves from $(x(0),y(0))$ to $(x(tau),y(tau))$ for $tau >0$ such that its kinetic energy is minimized, then



      $(a)$ $frac{ddot{x}}{phi_x}=frac{ddot{y}}{phi_y}$.



      $(b)$ $dot{x}^2(0)+dot{y}^2(0)=dot{x}^2(tau)+dot{y}^2(tau)$.



      $(c)$ $dot{x}phi_x+dot{y}phi_y=0$.



      $(d)$ $dot{x}^2(0)=dot{x}^2(tau)$.



      Now, if we consider this problem as minimizing a functional $J[x(t),y(t)]=int_0^tau F(x,dot{x},y,dot{y},t)dt$ in two dependent variables representing coordinates and one independent variable representing time, then Euler-Lagrange equation will give a family of extremals from which we can conclude the answer. But I am unable to find a way to relate the K.E. as a functional as written above, and include the curve $phi(x,y)=0$ in the same. So is there another method for this problem or am I on the right track? Any help will be appreciated.







      calculus-of-variations






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      asked Dec 13 '18 at 18:11









      am_11235...am_11235...

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          $begingroup$

          Hint.



          Defining the Lagrangian with $X = (x(t),y(t))$



          $$
          L(X,dot X,lambda) = frac m2left(dot x(t)^2+dot y(t)^2right)+lambda phi(x(t),y(t))
          $$



          we have the Euler-Lagrange movement equations



          $$
          L_X-frac{d}{dt}left(L_{X'}right) = left{begin{array}{rcl}m ddot x(t)-lambdaphi_x(x(t),y(t)) & = & 0\ m ddot y(t)-lambdaphi_y(x(t),y(t)) & = & 0end{array}right.
          $$






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            1 Answer
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            active

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            0












            $begingroup$

            Hint.



            Defining the Lagrangian with $X = (x(t),y(t))$



            $$
            L(X,dot X,lambda) = frac m2left(dot x(t)^2+dot y(t)^2right)+lambda phi(x(t),y(t))
            $$



            we have the Euler-Lagrange movement equations



            $$
            L_X-frac{d}{dt}left(L_{X'}right) = left{begin{array}{rcl}m ddot x(t)-lambdaphi_x(x(t),y(t)) & = & 0\ m ddot y(t)-lambdaphi_y(x(t),y(t)) & = & 0end{array}right.
            $$






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            $endgroup$


















              0












              $begingroup$

              Hint.



              Defining the Lagrangian with $X = (x(t),y(t))$



              $$
              L(X,dot X,lambda) = frac m2left(dot x(t)^2+dot y(t)^2right)+lambda phi(x(t),y(t))
              $$



              we have the Euler-Lagrange movement equations



              $$
              L_X-frac{d}{dt}left(L_{X'}right) = left{begin{array}{rcl}m ddot x(t)-lambdaphi_x(x(t),y(t)) & = & 0\ m ddot y(t)-lambdaphi_y(x(t),y(t)) & = & 0end{array}right.
              $$






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                0












                0








                0





                $begingroup$

                Hint.



                Defining the Lagrangian with $X = (x(t),y(t))$



                $$
                L(X,dot X,lambda) = frac m2left(dot x(t)^2+dot y(t)^2right)+lambda phi(x(t),y(t))
                $$



                we have the Euler-Lagrange movement equations



                $$
                L_X-frac{d}{dt}left(L_{X'}right) = left{begin{array}{rcl}m ddot x(t)-lambdaphi_x(x(t),y(t)) & = & 0\ m ddot y(t)-lambdaphi_y(x(t),y(t)) & = & 0end{array}right.
                $$






                share|cite|improve this answer











                $endgroup$



                Hint.



                Defining the Lagrangian with $X = (x(t),y(t))$



                $$
                L(X,dot X,lambda) = frac m2left(dot x(t)^2+dot y(t)^2right)+lambda phi(x(t),y(t))
                $$



                we have the Euler-Lagrange movement equations



                $$
                L_X-frac{d}{dt}left(L_{X'}right) = left{begin{array}{rcl}m ddot x(t)-lambdaphi_x(x(t),y(t)) & = & 0\ m ddot y(t)-lambdaphi_y(x(t),y(t)) & = & 0end{array}right.
                $$







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                share|cite|improve this answer



                share|cite|improve this answer








                edited Dec 13 '18 at 22:08

























                answered Dec 13 '18 at 18:43









                CesareoCesareo

                8,7193516




                8,7193516






























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