Investigate uniqueness of the following differential equation

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This is Problem 1.13 from Teschl's book (ODEs and Dynamical Systems). The equation is as follows:



$$
x' =
begincases
-tsqrt, &text if x ge 0\
tsqrt, &text if x le 0.
endcases
$$



It asks to show that the initial value problem $x(0) = x_0$ has unique global solution for every $x_0 in mathbbR$. There is a hint saying that if $x(t)$ is a solution so is $-x(t)$ and $x(-t)$, so it suffices to consider $x_0 ge 0$ and $t ge 0$. For $x_0 > 0$, I managed to find the solution



$$
x(t) =
begincases
(sqrtx_0 - frac14t^2)^2, &text if |t| le 2x_0^1/4\
0, &text otherwise.
endcases
$$



It is easy to see that this is a solution by using the Mean Value Theorem when calculating $x'(t)$ for $t = pm 2x_0^1/4$, because $x$ is continuous at these points and $x'(theta) to 0$ as $theta to t$. For $x_0 = 0$ the obvious solution is $x(t) = 0$ for all $t$. The problem is that I do not know how to show these solutions are unique.



If $x$ is a is solution and $x_0 > 0$, then by continuity there is an open interval $(t_1, t_2)$ containing $0$ where $x(t)$ is positive, and so it makes sense to write



$$
-s = fracx'(s)sqrtx(s),
$$



for $s in (t_1, t_2)$, and to integrate both sides



beginalign
-frac12t^2 = int_0^t -s ds = int_0^t fracx'(s)sqrtx(s) ds = 2(sqrtx(t) - sqrtx(0)).
endalign



This yields $x(t) = (sqrtx_0 - frac14t^2)^2$ for $t in (t_1, t_2)$. Assuming that $(t_1, t_2)$ is a maximal interval where $x(t)$ is positive, and since $(t_1, t_2) subseteq (-2x_0^1/4, 2x_0^1/4)$, we see by continuity of $x$ that $x(t_1) = x(t_2) = 0$ and thus $(t_1, t_2) = (-2x_0^1/4, 2x_0^1/4)$. How do I show that $x(t) = 0$ when $t$ is not in this interval? I suspect the same technique in this last step can be used to show that $x(t) = 0$ when $x_0 = 0$.







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    This is Problem 1.13 from Teschl's book (ODEs and Dynamical Systems). The equation is as follows:



    $$
    x' =
    begincases
    -tsqrt, &text if x ge 0\
    tsqrt, &text if x le 0.
    endcases
    $$



    It asks to show that the initial value problem $x(0) = x_0$ has unique global solution for every $x_0 in mathbbR$. There is a hint saying that if $x(t)$ is a solution so is $-x(t)$ and $x(-t)$, so it suffices to consider $x_0 ge 0$ and $t ge 0$. For $x_0 > 0$, I managed to find the solution



    $$
    x(t) =
    begincases
    (sqrtx_0 - frac14t^2)^2, &text if |t| le 2x_0^1/4\
    0, &text otherwise.
    endcases
    $$



    It is easy to see that this is a solution by using the Mean Value Theorem when calculating $x'(t)$ for $t = pm 2x_0^1/4$, because $x$ is continuous at these points and $x'(theta) to 0$ as $theta to t$. For $x_0 = 0$ the obvious solution is $x(t) = 0$ for all $t$. The problem is that I do not know how to show these solutions are unique.



    If $x$ is a is solution and $x_0 > 0$, then by continuity there is an open interval $(t_1, t_2)$ containing $0$ where $x(t)$ is positive, and so it makes sense to write



    $$
    -s = fracx'(s)sqrtx(s),
    $$



    for $s in (t_1, t_2)$, and to integrate both sides



    beginalign
    -frac12t^2 = int_0^t -s ds = int_0^t fracx'(s)sqrtx(s) ds = 2(sqrtx(t) - sqrtx(0)).
    endalign



    This yields $x(t) = (sqrtx_0 - frac14t^2)^2$ for $t in (t_1, t_2)$. Assuming that $(t_1, t_2)$ is a maximal interval where $x(t)$ is positive, and since $(t_1, t_2) subseteq (-2x_0^1/4, 2x_0^1/4)$, we see by continuity of $x$ that $x(t_1) = x(t_2) = 0$ and thus $(t_1, t_2) = (-2x_0^1/4, 2x_0^1/4)$. How do I show that $x(t) = 0$ when $t$ is not in this interval? I suspect the same technique in this last step can be used to show that $x(t) = 0$ when $x_0 = 0$.







    share|cite|improve this question























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      This is Problem 1.13 from Teschl's book (ODEs and Dynamical Systems). The equation is as follows:



      $$
      x' =
      begincases
      -tsqrt, &text if x ge 0\
      tsqrt, &text if x le 0.
      endcases
      $$



      It asks to show that the initial value problem $x(0) = x_0$ has unique global solution for every $x_0 in mathbbR$. There is a hint saying that if $x(t)$ is a solution so is $-x(t)$ and $x(-t)$, so it suffices to consider $x_0 ge 0$ and $t ge 0$. For $x_0 > 0$, I managed to find the solution



      $$
      x(t) =
      begincases
      (sqrtx_0 - frac14t^2)^2, &text if |t| le 2x_0^1/4\
      0, &text otherwise.
      endcases
      $$



      It is easy to see that this is a solution by using the Mean Value Theorem when calculating $x'(t)$ for $t = pm 2x_0^1/4$, because $x$ is continuous at these points and $x'(theta) to 0$ as $theta to t$. For $x_0 = 0$ the obvious solution is $x(t) = 0$ for all $t$. The problem is that I do not know how to show these solutions are unique.



      If $x$ is a is solution and $x_0 > 0$, then by continuity there is an open interval $(t_1, t_2)$ containing $0$ where $x(t)$ is positive, and so it makes sense to write



      $$
      -s = fracx'(s)sqrtx(s),
      $$



      for $s in (t_1, t_2)$, and to integrate both sides



      beginalign
      -frac12t^2 = int_0^t -s ds = int_0^t fracx'(s)sqrtx(s) ds = 2(sqrtx(t) - sqrtx(0)).
      endalign



      This yields $x(t) = (sqrtx_0 - frac14t^2)^2$ for $t in (t_1, t_2)$. Assuming that $(t_1, t_2)$ is a maximal interval where $x(t)$ is positive, and since $(t_1, t_2) subseteq (-2x_0^1/4, 2x_0^1/4)$, we see by continuity of $x$ that $x(t_1) = x(t_2) = 0$ and thus $(t_1, t_2) = (-2x_0^1/4, 2x_0^1/4)$. How do I show that $x(t) = 0$ when $t$ is not in this interval? I suspect the same technique in this last step can be used to show that $x(t) = 0$ when $x_0 = 0$.







      share|cite|improve this question













      This is Problem 1.13 from Teschl's book (ODEs and Dynamical Systems). The equation is as follows:



      $$
      x' =
      begincases
      -tsqrt, &text if x ge 0\
      tsqrt, &text if x le 0.
      endcases
      $$



      It asks to show that the initial value problem $x(0) = x_0$ has unique global solution for every $x_0 in mathbbR$. There is a hint saying that if $x(t)$ is a solution so is $-x(t)$ and $x(-t)$, so it suffices to consider $x_0 ge 0$ and $t ge 0$. For $x_0 > 0$, I managed to find the solution



      $$
      x(t) =
      begincases
      (sqrtx_0 - frac14t^2)^2, &text if |t| le 2x_0^1/4\
      0, &text otherwise.
      endcases
      $$



      It is easy to see that this is a solution by using the Mean Value Theorem when calculating $x'(t)$ for $t = pm 2x_0^1/4$, because $x$ is continuous at these points and $x'(theta) to 0$ as $theta to t$. For $x_0 = 0$ the obvious solution is $x(t) = 0$ for all $t$. The problem is that I do not know how to show these solutions are unique.



      If $x$ is a is solution and $x_0 > 0$, then by continuity there is an open interval $(t_1, t_2)$ containing $0$ where $x(t)$ is positive, and so it makes sense to write



      $$
      -s = fracx'(s)sqrtx(s),
      $$



      for $s in (t_1, t_2)$, and to integrate both sides



      beginalign
      -frac12t^2 = int_0^t -s ds = int_0^t fracx'(s)sqrtx(s) ds = 2(sqrtx(t) - sqrtx(0)).
      endalign



      This yields $x(t) = (sqrtx_0 - frac14t^2)^2$ for $t in (t_1, t_2)$. Assuming that $(t_1, t_2)$ is a maximal interval where $x(t)$ is positive, and since $(t_1, t_2) subseteq (-2x_0^1/4, 2x_0^1/4)$, we see by continuity of $x$ that $x(t_1) = x(t_2) = 0$ and thus $(t_1, t_2) = (-2x_0^1/4, 2x_0^1/4)$. How do I show that $x(t) = 0$ when $t$ is not in this interval? I suspect the same technique in this last step can be used to show that $x(t) = 0$ when $x_0 = 0$.









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      edited Jul 15 at 12:50
























      asked Jul 14 at 23:20









      Doughnut Pump

      439312




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          Alright, I've done it. Suppose first $x_0 = 0$ and let $x(t)$ be a solution. Assume by contradiction that $x(t) > 0$ for some $t > 0$ and set
          $$
          d = infa < t: x(s) > 0 text for every s in (a, t) .
          $$
          By continuity $d$ is well defined, $0 le d < t$ and $x(d) = 0$. By the Mean Value Theorem, we see that
          $$
          x(t) = x(t) - x(d) = x'(theta)(t - d),
          $$
          for some $theta in (d, t)$, so
          $$
          x(t) = -thetasqrt(t - d) le 0
          $$
          which is a contradiction. If $x(t) < 0$ the proof should be analogous and we can do the same thing to finish what I wrote above for the case $x_0 > 0$.






          share|cite|improve this answer





















          • Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
            – user539887
            Jul 15 at 7:34











          • @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
            – Doughnut Pump
            Jul 15 at 9:28










          • You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
            – user539887
            Jul 15 at 10:52


















          up vote
          0
          down vote













          To prove uniqueness, let's assume two solutions $x(t)$ and $y(t)$, $x(0)=y(0)=x_0>0$. Let $u=x-y$ with $u(0)=u_0=0$. We subtract the equations for $x$ and $y$ and obtain
          $$
          u'(t)=-tfracusqrtx+sqrty,
          $$
          which yields
          $$
          u(t)=u_0 expleft(-int_0^t fracssqrtx(s)+sqrty(s)dsright).
          $$
          Since $u_0=0$, then $uequiv0$.






          share|cite|improve this answer





















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            2 Answers
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            2 Answers
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            active

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            active

            oldest

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            active

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            up vote
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            down vote













            Alright, I've done it. Suppose first $x_0 = 0$ and let $x(t)$ be a solution. Assume by contradiction that $x(t) > 0$ for some $t > 0$ and set
            $$
            d = infa < t: x(s) > 0 text for every s in (a, t) .
            $$
            By continuity $d$ is well defined, $0 le d < t$ and $x(d) = 0$. By the Mean Value Theorem, we see that
            $$
            x(t) = x(t) - x(d) = x'(theta)(t - d),
            $$
            for some $theta in (d, t)$, so
            $$
            x(t) = -thetasqrt(t - d) le 0
            $$
            which is a contradiction. If $x(t) < 0$ the proof should be analogous and we can do the same thing to finish what I wrote above for the case $x_0 > 0$.






            share|cite|improve this answer





















            • Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
              – user539887
              Jul 15 at 7:34











            • @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
              – Doughnut Pump
              Jul 15 at 9:28










            • You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
              – user539887
              Jul 15 at 10:52















            up vote
            0
            down vote













            Alright, I've done it. Suppose first $x_0 = 0$ and let $x(t)$ be a solution. Assume by contradiction that $x(t) > 0$ for some $t > 0$ and set
            $$
            d = infa < t: x(s) > 0 text for every s in (a, t) .
            $$
            By continuity $d$ is well defined, $0 le d < t$ and $x(d) = 0$. By the Mean Value Theorem, we see that
            $$
            x(t) = x(t) - x(d) = x'(theta)(t - d),
            $$
            for some $theta in (d, t)$, so
            $$
            x(t) = -thetasqrt(t - d) le 0
            $$
            which is a contradiction. If $x(t) < 0$ the proof should be analogous and we can do the same thing to finish what I wrote above for the case $x_0 > 0$.






            share|cite|improve this answer





















            • Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
              – user539887
              Jul 15 at 7:34











            • @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
              – Doughnut Pump
              Jul 15 at 9:28










            • You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
              – user539887
              Jul 15 at 10:52













            up vote
            0
            down vote










            up vote
            0
            down vote









            Alright, I've done it. Suppose first $x_0 = 0$ and let $x(t)$ be a solution. Assume by contradiction that $x(t) > 0$ for some $t > 0$ and set
            $$
            d = infa < t: x(s) > 0 text for every s in (a, t) .
            $$
            By continuity $d$ is well defined, $0 le d < t$ and $x(d) = 0$. By the Mean Value Theorem, we see that
            $$
            x(t) = x(t) - x(d) = x'(theta)(t - d),
            $$
            for some $theta in (d, t)$, so
            $$
            x(t) = -thetasqrt(t - d) le 0
            $$
            which is a contradiction. If $x(t) < 0$ the proof should be analogous and we can do the same thing to finish what I wrote above for the case $x_0 > 0$.






            share|cite|improve this answer













            Alright, I've done it. Suppose first $x_0 = 0$ and let $x(t)$ be a solution. Assume by contradiction that $x(t) > 0$ for some $t > 0$ and set
            $$
            d = infa < t: x(s) > 0 text for every s in (a, t) .
            $$
            By continuity $d$ is well defined, $0 le d < t$ and $x(d) = 0$. By the Mean Value Theorem, we see that
            $$
            x(t) = x(t) - x(d) = x'(theta)(t - d),
            $$
            for some $theta in (d, t)$, so
            $$
            x(t) = -thetasqrt(t - d) le 0
            $$
            which is a contradiction. If $x(t) < 0$ the proof should be analogous and we can do the same thing to finish what I wrote above for the case $x_0 > 0$.







            share|cite|improve this answer













            share|cite|improve this answer



            share|cite|improve this answer











            answered Jul 15 at 0:14









            Doughnut Pump

            439312




            439312











            • Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
              – user539887
              Jul 15 at 7:34











            • @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
              – Doughnut Pump
              Jul 15 at 9:28










            • You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
              – user539887
              Jul 15 at 10:52

















            • Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
              – user539887
              Jul 15 at 7:34











            • @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
              – Doughnut Pump
              Jul 15 at 9:28










            • You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
              – user539887
              Jul 15 at 10:52
















            Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
            – user539887
            Jul 15 at 7:34





            Yes, this part is O.K. I would only define $d$ as the supremum of the set of those $a<t$ such that $x(a)=0$ (easier to show it is nonempty). Remember that you should also show that we have uniqueness at each point where the value of the solution is nonzero, and that any solution is global. Can you do that?
            – user539887
            Jul 15 at 7:34













            @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
            – Doughnut Pump
            Jul 15 at 9:28




            @user539887 What do you mean by "uniqueness at each point where the value of the solution is nonzero"? I have shown it is unique for every choice of $x_0$, isn't that all there is to it?
            – Doughnut Pump
            Jul 15 at 9:28












            You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
            – user539887
            Jul 15 at 10:52





            You showed only that the solution cannot branch at a point where its value is $0$. At other points it cannot branch, either, but here one needs to use, for example, the local Lipschitz continuity at such a point. Or, alternatively, you can argue that your arguments in the last paragraph of your question show that the obtained formula is the only possible.
            – user539887
            Jul 15 at 10:52











            up vote
            0
            down vote













            To prove uniqueness, let's assume two solutions $x(t)$ and $y(t)$, $x(0)=y(0)=x_0>0$. Let $u=x-y$ with $u(0)=u_0=0$. We subtract the equations for $x$ and $y$ and obtain
            $$
            u'(t)=-tfracusqrtx+sqrty,
            $$
            which yields
            $$
            u(t)=u_0 expleft(-int_0^t fracssqrtx(s)+sqrty(s)dsright).
            $$
            Since $u_0=0$, then $uequiv0$.






            share|cite|improve this answer

























              up vote
              0
              down vote













              To prove uniqueness, let's assume two solutions $x(t)$ and $y(t)$, $x(0)=y(0)=x_0>0$. Let $u=x-y$ with $u(0)=u_0=0$. We subtract the equations for $x$ and $y$ and obtain
              $$
              u'(t)=-tfracusqrtx+sqrty,
              $$
              which yields
              $$
              u(t)=u_0 expleft(-int_0^t fracssqrtx(s)+sqrty(s)dsright).
              $$
              Since $u_0=0$, then $uequiv0$.






              share|cite|improve this answer























                up vote
                0
                down vote










                up vote
                0
                down vote









                To prove uniqueness, let's assume two solutions $x(t)$ and $y(t)$, $x(0)=y(0)=x_0>0$. Let $u=x-y$ with $u(0)=u_0=0$. We subtract the equations for $x$ and $y$ and obtain
                $$
                u'(t)=-tfracusqrtx+sqrty,
                $$
                which yields
                $$
                u(t)=u_0 expleft(-int_0^t fracssqrtx(s)+sqrty(s)dsright).
                $$
                Since $u_0=0$, then $uequiv0$.






                share|cite|improve this answer













                To prove uniqueness, let's assume two solutions $x(t)$ and $y(t)$, $x(0)=y(0)=x_0>0$. Let $u=x-y$ with $u(0)=u_0=0$. We subtract the equations for $x$ and $y$ and obtain
                $$
                u'(t)=-tfracusqrtx+sqrty,
                $$
                which yields
                $$
                u(t)=u_0 expleft(-int_0^t fracssqrtx(s)+sqrty(s)dsright).
                $$
                Since $u_0=0$, then $uequiv0$.







                share|cite|improve this answer













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                answered Jul 16 at 4:34









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