Integral curves and flows of bounded vector fields











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Let $X=(X_1,dots, X_n)in L^infty$ be a smooth (non Lipschitz) vector field such that



begin{equation}tag{1}
X_n ge c|(X_1, dots, X_{n-1})|,.
end{equation}



Does the cone condition (1) imply that the flow $Phi(t,x)$ is globally defined? I would say so, as it seems that forces integral curves to be confined.



Is this true?



Take $bar x$ and given the maximal interval $(0, t_{bar x})$, I argue by contradiction that $t_{bar x}$ is finite. Take a sequence of times $t_n$ converging to $t_{bar x}$ and let $x_n$ be the points corresponding to the flow $Phi(t_n,bar x)$. If I am able to prove that the sequence $x_n$ is bounded, then it must converge and thus I would be able to extend the flow at $t_{bar x}$ by setting it equal to $lim_n x_n$.



How do I prove that these $x_n$ stay bounded, given (1)?










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    up vote
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    Let $X=(X_1,dots, X_n)in L^infty$ be a smooth (non Lipschitz) vector field such that



    begin{equation}tag{1}
    X_n ge c|(X_1, dots, X_{n-1})|,.
    end{equation}



    Does the cone condition (1) imply that the flow $Phi(t,x)$ is globally defined? I would say so, as it seems that forces integral curves to be confined.



    Is this true?



    Take $bar x$ and given the maximal interval $(0, t_{bar x})$, I argue by contradiction that $t_{bar x}$ is finite. Take a sequence of times $t_n$ converging to $t_{bar x}$ and let $x_n$ be the points corresponding to the flow $Phi(t_n,bar x)$. If I am able to prove that the sequence $x_n$ is bounded, then it must converge and thus I would be able to extend the flow at $t_{bar x}$ by setting it equal to $lim_n x_n$.



    How do I prove that these $x_n$ stay bounded, given (1)?










    share|cite|improve this question


























      up vote
      2
      down vote

      favorite









      up vote
      2
      down vote

      favorite











      Let $X=(X_1,dots, X_n)in L^infty$ be a smooth (non Lipschitz) vector field such that



      begin{equation}tag{1}
      X_n ge c|(X_1, dots, X_{n-1})|,.
      end{equation}



      Does the cone condition (1) imply that the flow $Phi(t,x)$ is globally defined? I would say so, as it seems that forces integral curves to be confined.



      Is this true?



      Take $bar x$ and given the maximal interval $(0, t_{bar x})$, I argue by contradiction that $t_{bar x}$ is finite. Take a sequence of times $t_n$ converging to $t_{bar x}$ and let $x_n$ be the points corresponding to the flow $Phi(t_n,bar x)$. If I am able to prove that the sequence $x_n$ is bounded, then it must converge and thus I would be able to extend the flow at $t_{bar x}$ by setting it equal to $lim_n x_n$.



      How do I prove that these $x_n$ stay bounded, given (1)?










      share|cite|improve this question















      Let $X=(X_1,dots, X_n)in L^infty$ be a smooth (non Lipschitz) vector field such that



      begin{equation}tag{1}
      X_n ge c|(X_1, dots, X_{n-1})|,.
      end{equation}



      Does the cone condition (1) imply that the flow $Phi(t,x)$ is globally defined? I would say so, as it seems that forces integral curves to be confined.



      Is this true?



      Take $bar x$ and given the maximal interval $(0, t_{bar x})$, I argue by contradiction that $t_{bar x}$ is finite. Take a sequence of times $t_n$ converging to $t_{bar x}$ and let $x_n$ be the points corresponding to the flow $Phi(t_n,bar x)$. If I am able to prove that the sequence $x_n$ is bounded, then it must converge and thus I would be able to extend the flow at $t_{bar x}$ by setting it equal to $lim_n x_n$.



      How do I prove that these $x_n$ stay bounded, given (1)?







      vector-fields






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      edited Nov 23 at 15:57

























      asked Nov 16 at 15:06









      Paolo Intuito

      988218




      988218






















          1 Answer
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          You don't even need the assumption $(1)$.



          Local existence and uniqueness is ensured because $X$ is locally Lipschitz.
          You have that
          $$
          |Phi(t,x)-x| = left|int_0^t X(Phi(s,x))dsright| leq int_0^t |X(Phi(s,x))|ds
          leq |X|_infty t.
          $$

          This means that solutions stay in a compact set in finite time, which implies that they can be extended to $[0,infty)$.






          share|cite|improve this answer





















          • Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
            – Paolo Intuito
            Nov 26 at 9:17






          • 1




            Nope: try $Xequiv 0$.
            – Federico
            Nov 26 at 17:16










          • Besides the trivial case, i.e. if $|X|_infty>0$?
            – Paolo Intuito
            Nov 27 at 11:10






          • 1




            For that you would $X_n>0$.
            – Federico
            Nov 27 at 13:36






          • 1




            Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
            – Federico
            Nov 28 at 16:13











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          1 Answer
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          active

          oldest

          votes








          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes








          up vote
          1
          down vote



          accepted
          +50










          You don't even need the assumption $(1)$.



          Local existence and uniqueness is ensured because $X$ is locally Lipschitz.
          You have that
          $$
          |Phi(t,x)-x| = left|int_0^t X(Phi(s,x))dsright| leq int_0^t |X(Phi(s,x))|ds
          leq |X|_infty t.
          $$

          This means that solutions stay in a compact set in finite time, which implies that they can be extended to $[0,infty)$.






          share|cite|improve this answer





















          • Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
            – Paolo Intuito
            Nov 26 at 9:17






          • 1




            Nope: try $Xequiv 0$.
            – Federico
            Nov 26 at 17:16










          • Besides the trivial case, i.e. if $|X|_infty>0$?
            – Paolo Intuito
            Nov 27 at 11:10






          • 1




            For that you would $X_n>0$.
            – Federico
            Nov 27 at 13:36






          • 1




            Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
            – Federico
            Nov 28 at 16:13















          up vote
          1
          down vote



          accepted
          +50










          You don't even need the assumption $(1)$.



          Local existence and uniqueness is ensured because $X$ is locally Lipschitz.
          You have that
          $$
          |Phi(t,x)-x| = left|int_0^t X(Phi(s,x))dsright| leq int_0^t |X(Phi(s,x))|ds
          leq |X|_infty t.
          $$

          This means that solutions stay in a compact set in finite time, which implies that they can be extended to $[0,infty)$.






          share|cite|improve this answer





















          • Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
            – Paolo Intuito
            Nov 26 at 9:17






          • 1




            Nope: try $Xequiv 0$.
            – Federico
            Nov 26 at 17:16










          • Besides the trivial case, i.e. if $|X|_infty>0$?
            – Paolo Intuito
            Nov 27 at 11:10






          • 1




            For that you would $X_n>0$.
            – Federico
            Nov 27 at 13:36






          • 1




            Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
            – Federico
            Nov 28 at 16:13













          up vote
          1
          down vote



          accepted
          +50







          up vote
          1
          down vote



          accepted
          +50




          +50




          You don't even need the assumption $(1)$.



          Local existence and uniqueness is ensured because $X$ is locally Lipschitz.
          You have that
          $$
          |Phi(t,x)-x| = left|int_0^t X(Phi(s,x))dsright| leq int_0^t |X(Phi(s,x))|ds
          leq |X|_infty t.
          $$

          This means that solutions stay in a compact set in finite time, which implies that they can be extended to $[0,infty)$.






          share|cite|improve this answer












          You don't even need the assumption $(1)$.



          Local existence and uniqueness is ensured because $X$ is locally Lipschitz.
          You have that
          $$
          |Phi(t,x)-x| = left|int_0^t X(Phi(s,x))dsright| leq int_0^t |X(Phi(s,x))|ds
          leq |X|_infty t.
          $$

          This means that solutions stay in a compact set in finite time, which implies that they can be extended to $[0,infty)$.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Nov 23 at 17:25









          Federico

          2,556510




          2,556510












          • Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
            – Paolo Intuito
            Nov 26 at 9:17






          • 1




            Nope: try $Xequiv 0$.
            – Federico
            Nov 26 at 17:16










          • Besides the trivial case, i.e. if $|X|_infty>0$?
            – Paolo Intuito
            Nov 27 at 11:10






          • 1




            For that you would $X_n>0$.
            – Federico
            Nov 27 at 13:36






          • 1




            Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
            – Federico
            Nov 28 at 16:13


















          • Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
            – Paolo Intuito
            Nov 26 at 9:17






          • 1




            Nope: try $Xequiv 0$.
            – Federico
            Nov 26 at 17:16










          • Besides the trivial case, i.e. if $|X|_infty>0$?
            – Paolo Intuito
            Nov 27 at 11:10






          • 1




            For that you would $X_n>0$.
            – Federico
            Nov 27 at 13:36






          • 1




            Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
            – Federico
            Nov 28 at 16:13
















          Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
          – Paolo Intuito
          Nov 26 at 9:17




          Great thanks. I somehow got distracted by the assumtpion (1) which apparently was not needed. Maybe I can infer something more from it, such that the integral curves will pass through every hyperplane of fixed $n$-th coordinate, $H_h:={x_n = h}$?
          – Paolo Intuito
          Nov 26 at 9:17




          1




          1




          Nope: try $Xequiv 0$.
          – Federico
          Nov 26 at 17:16




          Nope: try $Xequiv 0$.
          – Federico
          Nov 26 at 17:16












          Besides the trivial case, i.e. if $|X|_infty>0$?
          – Paolo Intuito
          Nov 27 at 11:10




          Besides the trivial case, i.e. if $|X|_infty>0$?
          – Paolo Intuito
          Nov 27 at 11:10




          1




          1




          For that you would $X_n>0$.
          – Federico
          Nov 27 at 13:36




          For that you would $X_n>0$.
          – Federico
          Nov 27 at 13:36




          1




          1




          Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
          – Federico
          Nov 28 at 16:13




          Just consider a trajectory $x(t)$. Assume $M=sup_t x_n(t)=lim_{ttoinfty} x_n(t)<infty$. Then by $(1)$ you get that $x^*=lim_{ttoinfty} x(t)$ exists. But then $x^*$ needs to be a stationary point, giving $X_n(x^*)=0$, contradiction.
          – Federico
          Nov 28 at 16:13


















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