The reverse implication in the stability theory












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Let us consider the system of differential equation $dot x=Ax+h(t),$ where A is a constant matrix of dimension $ngeq2$ and $h$ is continuous on $[0,infty).$ All eigenvalues of $A$ have a negative real part. It is known, that $h(t)to 0$ for $ttoinfty$ implies that all solutions $x(t)$ of $dot x=Ax+h(t)$ converge to $0$ for $ttoinfty.$
Is the converse implication true too? (All solutions $x(t)to 0$ implies $h(t)to 0$).



Thank you.










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    Let us consider the system of differential equation $dot x=Ax+h(t),$ where A is a constant matrix of dimension $ngeq2$ and $h$ is continuous on $[0,infty).$ All eigenvalues of $A$ have a negative real part. It is known, that $h(t)to 0$ for $ttoinfty$ implies that all solutions $x(t)$ of $dot x=Ax+h(t)$ converge to $0$ for $ttoinfty.$
    Is the converse implication true too? (All solutions $x(t)to 0$ implies $h(t)to 0$).



    Thank you.










    share|cite|improve this question









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      $begingroup$


      Let us consider the system of differential equation $dot x=Ax+h(t),$ where A is a constant matrix of dimension $ngeq2$ and $h$ is continuous on $[0,infty).$ All eigenvalues of $A$ have a negative real part. It is known, that $h(t)to 0$ for $ttoinfty$ implies that all solutions $x(t)$ of $dot x=Ax+h(t)$ converge to $0$ for $ttoinfty.$
      Is the converse implication true too? (All solutions $x(t)to 0$ implies $h(t)to 0$).



      Thank you.










      share|cite|improve this question









      $endgroup$




      Let us consider the system of differential equation $dot x=Ax+h(t),$ where A is a constant matrix of dimension $ngeq2$ and $h$ is continuous on $[0,infty).$ All eigenvalues of $A$ have a negative real part. It is known, that $h(t)to 0$ for $ttoinfty$ implies that all solutions $x(t)$ of $dot x=Ax+h(t)$ converge to $0$ for $ttoinfty.$
      Is the converse implication true too? (All solutions $x(t)to 0$ implies $h(t)to 0$).



      Thank you.







      differential-equations stability-in-odes






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      asked Nov 23 '18 at 18:27









      RobertRobert

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      112






















          2 Answers
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          $begingroup$

          More precisely, the equivalence holds if for some vector norm $leftVertcdotrightVert,$
          begin{equation}
          suplimits_{0leq uleq1}leftVertintlimits_{t}^{t+u}h(s)dsrightVertto 0
          end{equation}

          as $ttoinfty.$



          For the details and (long) proof see Theorem B in:



          Strauss, A.; Yorke, J. A., Perturbing uniform asymptotically stable nonlinear systems, J. Differ. Equations 6, 452-483 (1969). ZBL0182.12103.






          share|cite|improve this answer









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            No. Consider $h$ which is $0$ everywhere except near $n^2$ for $ninmathbb N$ where it has bumps of height $1$ and width $1/n$:
            $$
            h(t) = sum_{ninmathbb N} 1_{[n^2-1/n,n^2+1/n]}(t).
            $$

            Consider now for instance $x'(t)=-x(t)+h(t)$.
            All trajectories become eventually positive. Then it's clear that the effect of $h$ perturbs $x$ by at most $2/n$ when $t$ passes the time $n$:
            $$
            x(n+1/n)-x(n-1/n) leq int_{n^2-1/n}^{n^2+1/n} h(t),dt=2/n.
            $$

            From this you should be able to conclude that $x$ goes to $0$ nonetheless, because in the interval $[n^2,(n+1)^2]$ of length $sim n$ it has plenty of time to become exponentially close to $0$.






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              2 Answers
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              active

              oldest

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              2 Answers
              2






              active

              oldest

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              active

              oldest

              votes






              active

              oldest

              votes









              1












              $begingroup$

              More precisely, the equivalence holds if for some vector norm $leftVertcdotrightVert,$
              begin{equation}
              suplimits_{0leq uleq1}leftVertintlimits_{t}^{t+u}h(s)dsrightVertto 0
              end{equation}

              as $ttoinfty.$



              For the details and (long) proof see Theorem B in:



              Strauss, A.; Yorke, J. A., Perturbing uniform asymptotically stable nonlinear systems, J. Differ. Equations 6, 452-483 (1969). ZBL0182.12103.






              share|cite|improve this answer









              $endgroup$


















                1












                $begingroup$

                More precisely, the equivalence holds if for some vector norm $leftVertcdotrightVert,$
                begin{equation}
                suplimits_{0leq uleq1}leftVertintlimits_{t}^{t+u}h(s)dsrightVertto 0
                end{equation}

                as $ttoinfty.$



                For the details and (long) proof see Theorem B in:



                Strauss, A.; Yorke, J. A., Perturbing uniform asymptotically stable nonlinear systems, J. Differ. Equations 6, 452-483 (1969). ZBL0182.12103.






                share|cite|improve this answer









                $endgroup$
















                  1












                  1








                  1





                  $begingroup$

                  More precisely, the equivalence holds if for some vector norm $leftVertcdotrightVert,$
                  begin{equation}
                  suplimits_{0leq uleq1}leftVertintlimits_{t}^{t+u}h(s)dsrightVertto 0
                  end{equation}

                  as $ttoinfty.$



                  For the details and (long) proof see Theorem B in:



                  Strauss, A.; Yorke, J. A., Perturbing uniform asymptotically stable nonlinear systems, J. Differ. Equations 6, 452-483 (1969). ZBL0182.12103.






                  share|cite|improve this answer









                  $endgroup$



                  More precisely, the equivalence holds if for some vector norm $leftVertcdotrightVert,$
                  begin{equation}
                  suplimits_{0leq uleq1}leftVertintlimits_{t}^{t+u}h(s)dsrightVertto 0
                  end{equation}

                  as $ttoinfty.$



                  For the details and (long) proof see Theorem B in:



                  Strauss, A.; Yorke, J. A., Perturbing uniform asymptotically stable nonlinear systems, J. Differ. Equations 6, 452-483 (1969). ZBL0182.12103.







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Nov 24 '18 at 9:54









                  RobertRobert

                  112




                  112























                      0












                      $begingroup$

                      No. Consider $h$ which is $0$ everywhere except near $n^2$ for $ninmathbb N$ where it has bumps of height $1$ and width $1/n$:
                      $$
                      h(t) = sum_{ninmathbb N} 1_{[n^2-1/n,n^2+1/n]}(t).
                      $$

                      Consider now for instance $x'(t)=-x(t)+h(t)$.
                      All trajectories become eventually positive. Then it's clear that the effect of $h$ perturbs $x$ by at most $2/n$ when $t$ passes the time $n$:
                      $$
                      x(n+1/n)-x(n-1/n) leq int_{n^2-1/n}^{n^2+1/n} h(t),dt=2/n.
                      $$

                      From this you should be able to conclude that $x$ goes to $0$ nonetheless, because in the interval $[n^2,(n+1)^2]$ of length $sim n$ it has plenty of time to become exponentially close to $0$.






                      share|cite|improve this answer









                      $endgroup$


















                        0












                        $begingroup$

                        No. Consider $h$ which is $0$ everywhere except near $n^2$ for $ninmathbb N$ where it has bumps of height $1$ and width $1/n$:
                        $$
                        h(t) = sum_{ninmathbb N} 1_{[n^2-1/n,n^2+1/n]}(t).
                        $$

                        Consider now for instance $x'(t)=-x(t)+h(t)$.
                        All trajectories become eventually positive. Then it's clear that the effect of $h$ perturbs $x$ by at most $2/n$ when $t$ passes the time $n$:
                        $$
                        x(n+1/n)-x(n-1/n) leq int_{n^2-1/n}^{n^2+1/n} h(t),dt=2/n.
                        $$

                        From this you should be able to conclude that $x$ goes to $0$ nonetheless, because in the interval $[n^2,(n+1)^2]$ of length $sim n$ it has plenty of time to become exponentially close to $0$.






                        share|cite|improve this answer









                        $endgroup$
















                          0












                          0








                          0





                          $begingroup$

                          No. Consider $h$ which is $0$ everywhere except near $n^2$ for $ninmathbb N$ where it has bumps of height $1$ and width $1/n$:
                          $$
                          h(t) = sum_{ninmathbb N} 1_{[n^2-1/n,n^2+1/n]}(t).
                          $$

                          Consider now for instance $x'(t)=-x(t)+h(t)$.
                          All trajectories become eventually positive. Then it's clear that the effect of $h$ perturbs $x$ by at most $2/n$ when $t$ passes the time $n$:
                          $$
                          x(n+1/n)-x(n-1/n) leq int_{n^2-1/n}^{n^2+1/n} h(t),dt=2/n.
                          $$

                          From this you should be able to conclude that $x$ goes to $0$ nonetheless, because in the interval $[n^2,(n+1)^2]$ of length $sim n$ it has plenty of time to become exponentially close to $0$.






                          share|cite|improve this answer









                          $endgroup$



                          No. Consider $h$ which is $0$ everywhere except near $n^2$ for $ninmathbb N$ where it has bumps of height $1$ and width $1/n$:
                          $$
                          h(t) = sum_{ninmathbb N} 1_{[n^2-1/n,n^2+1/n]}(t).
                          $$

                          Consider now for instance $x'(t)=-x(t)+h(t)$.
                          All trajectories become eventually positive. Then it's clear that the effect of $h$ perturbs $x$ by at most $2/n$ when $t$ passes the time $n$:
                          $$
                          x(n+1/n)-x(n-1/n) leq int_{n^2-1/n}^{n^2+1/n} h(t),dt=2/n.
                          $$

                          From this you should be able to conclude that $x$ goes to $0$ nonetheless, because in the interval $[n^2,(n+1)^2]$ of length $sim n$ it has plenty of time to become exponentially close to $0$.







                          share|cite|improve this answer












                          share|cite|improve this answer



                          share|cite|improve this answer










                          answered Nov 23 '18 at 18:51









                          FedericoFederico

                          4,869514




                          4,869514






























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