Solutions of certain differential equations in two variablesProve theorem of Existence and Uniqueness of solutions of a $n$-th order differential equation using Picard-Lindelöf theoremDisplacement of differential equationfinding a solution of an autonomous differential equation with two variablesnecessary and sufficient conditions for the existence of solutions.Is it the Picard-Lindelöf Theorem?Is there a harder way to prove that if an integral curve's derivative vanishes then the curve is constant?Boundedness of solutions to a certain system of “weakly-coupled” linear differential equationsEquivalence of two definitions for submanifoldsProperty of solutions of differential equationSmooth map with null differential at each point are constant on the connected component of the domain

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Solutions of certain differential equations in two variables


Prove theorem of Existence and Uniqueness of solutions of a $n$-th order differential equation using Picard-Lindelöf theoremDisplacement of differential equationfinding a solution of an autonomous differential equation with two variablesnecessary and sufficient conditions for the existence of solutions.Is it the Picard-Lindelöf Theorem?Is there a harder way to prove that if an integral curve's derivative vanishes then the curve is constant?Boundedness of solutions to a certain system of “weakly-coupled” linear differential equationsEquivalence of two definitions for submanifoldsProperty of solutions of differential equationSmooth map with null differential at each point are constant on the connected component of the domain













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Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.



How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
$$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$



I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.










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$endgroup$
















    0












    $begingroup$


    Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.



    How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
    $$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$



    I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.










    share|cite|improve this question









    $endgroup$














      0












      0








      0





      $begingroup$


      Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.



      How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
      $$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$



      I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.










      share|cite|improve this question









      $endgroup$




      Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.



      How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
      $$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$



      I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.







      ordinary-differential-equations differential-geometry






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      share|cite|improve this question











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      asked Mar 17 at 13:04









      inequalitynoob2inequalitynoob2

      1447




      1447




















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          $begingroup$

          This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.



          In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.



          With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
          $$
          psi(s,t) = f(t) + sphi(t).
          $$






          share|cite|improve this answer









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            $begingroup$

            This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.



            In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.



            With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
            $$
            psi(s,t) = f(t) + sphi(t).
            $$






            share|cite|improve this answer









            $endgroup$

















              0












              $begingroup$

              This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.



              In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.



              With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
              $$
              psi(s,t) = f(t) + sphi(t).
              $$






              share|cite|improve this answer









              $endgroup$















                0












                0








                0





                $begingroup$

                This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.



                In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.



                With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
                $$
                psi(s,t) = f(t) + sphi(t).
                $$






                share|cite|improve this answer









                $endgroup$



                This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.



                In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.



                With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
                $$
                psi(s,t) = f(t) + sphi(t).
                $$







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Mar 17 at 17:44









                Jack LeeJack Lee

                27.7k54868




                27.7k54868



























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