Time between two rates in a ODE system

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I am reading the book on virus dynamics by Novak and May, and it describes a system of ODEs to describe the viral load when antivirals are used. The systems is



$dot y = -ay\dot v = ky-uv$



The solutions of this system are



$y(t)= y^*e^-at\v(t) = v^*(ue^-at-ae^-ut)over (u-a)$.



it is assumed that $u>>a$.

Then it is analysed that the virus load ($v(t)$) start to decline at rate $e^-at$ only after a certain shoulder phase of duration given as $Delta t approx 1/u$ (more precisely, $Delta t= (-1/a) ln (1-a/u) $ ).



enter image description hereCan someone please explain how this $Delta t$ is obtained?







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    I am reading the book on virus dynamics by Novak and May, and it describes a system of ODEs to describe the viral load when antivirals are used. The systems is



    $dot y = -ay\dot v = ky-uv$



    The solutions of this system are



    $y(t)= y^*e^-at\v(t) = v^*(ue^-at-ae^-ut)over (u-a)$.



    it is assumed that $u>>a$.

    Then it is analysed that the virus load ($v(t)$) start to decline at rate $e^-at$ only after a certain shoulder phase of duration given as $Delta t approx 1/u$ (more precisely, $Delta t= (-1/a) ln (1-a/u) $ ).



    enter image description hereCan someone please explain how this $Delta t$ is obtained?







    share|cite|improve this question





















      up vote
      0
      down vote

      favorite









      up vote
      0
      down vote

      favorite











      I am reading the book on virus dynamics by Novak and May, and it describes a system of ODEs to describe the viral load when antivirals are used. The systems is



      $dot y = -ay\dot v = ky-uv$



      The solutions of this system are



      $y(t)= y^*e^-at\v(t) = v^*(ue^-at-ae^-ut)over (u-a)$.



      it is assumed that $u>>a$.

      Then it is analysed that the virus load ($v(t)$) start to decline at rate $e^-at$ only after a certain shoulder phase of duration given as $Delta t approx 1/u$ (more precisely, $Delta t= (-1/a) ln (1-a/u) $ ).



      enter image description hereCan someone please explain how this $Delta t$ is obtained?







      share|cite|improve this question











      I am reading the book on virus dynamics by Novak and May, and it describes a system of ODEs to describe the viral load when antivirals are used. The systems is



      $dot y = -ay\dot v = ky-uv$



      The solutions of this system are



      $y(t)= y^*e^-at\v(t) = v^*(ue^-at-ae^-ut)over (u-a)$.



      it is assumed that $u>>a$.

      Then it is analysed that the virus load ($v(t)$) start to decline at rate $e^-at$ only after a certain shoulder phase of duration given as $Delta t approx 1/u$ (more precisely, $Delta t= (-1/a) ln (1-a/u) $ ).



      enter image description hereCan someone please explain how this $Delta t$ is obtained?









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      asked Jul 27 at 11:33









      clarkson

      80411428




      80411428




















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          To see it, first note that since $ugg a>0$ (assuming they are positive constants), the term $ae^-ut$ will go to $0$ more quickly than $ue^-at$. That is why $v(t)$ can be approximated by $ue^-at/(u-a)v_0$ after a certain time. To compute that time, see that on such a logarithmic scale as in your figure, $ue^-at/(u-a)v_0$ and $e^-atv_0$ correspond to parallel lines. Now since we start at $v_0$, i.e. at $e^-atv_0|_t=0$ and converge to $ue^-at/(u-a)v_0$ then the question can be rephrased to finding the translation from line to line, i.e. solving
          beginalign
          e^-a(t-Delta t)v_0 &= fracuu-ae^-atv_0\
          aDelta t &=mathrmln(u)-mathrmln(u-a)\
          Delta t &= -frac1abig(mathrmln(u-a)-mathrmln(u)big)\
          &= -frac1amathrmln((u-a)/u)\
          &= -frac1amathrmln(1-a/u).
          endalign






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            1 Answer
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            1 Answer
            1






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            active

            oldest

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            up vote
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            down vote



            accepted










            To see it, first note that since $ugg a>0$ (assuming they are positive constants), the term $ae^-ut$ will go to $0$ more quickly than $ue^-at$. That is why $v(t)$ can be approximated by $ue^-at/(u-a)v_0$ after a certain time. To compute that time, see that on such a logarithmic scale as in your figure, $ue^-at/(u-a)v_0$ and $e^-atv_0$ correspond to parallel lines. Now since we start at $v_0$, i.e. at $e^-atv_0|_t=0$ and converge to $ue^-at/(u-a)v_0$ then the question can be rephrased to finding the translation from line to line, i.e. solving
            beginalign
            e^-a(t-Delta t)v_0 &= fracuu-ae^-atv_0\
            aDelta t &=mathrmln(u)-mathrmln(u-a)\
            Delta t &= -frac1abig(mathrmln(u-a)-mathrmln(u)big)\
            &= -frac1amathrmln((u-a)/u)\
            &= -frac1amathrmln(1-a/u).
            endalign






            share|cite|improve this answer



























              up vote
              1
              down vote



              accepted










              To see it, first note that since $ugg a>0$ (assuming they are positive constants), the term $ae^-ut$ will go to $0$ more quickly than $ue^-at$. That is why $v(t)$ can be approximated by $ue^-at/(u-a)v_0$ after a certain time. To compute that time, see that on such a logarithmic scale as in your figure, $ue^-at/(u-a)v_0$ and $e^-atv_0$ correspond to parallel lines. Now since we start at $v_0$, i.e. at $e^-atv_0|_t=0$ and converge to $ue^-at/(u-a)v_0$ then the question can be rephrased to finding the translation from line to line, i.e. solving
              beginalign
              e^-a(t-Delta t)v_0 &= fracuu-ae^-atv_0\
              aDelta t &=mathrmln(u)-mathrmln(u-a)\
              Delta t &= -frac1abig(mathrmln(u-a)-mathrmln(u)big)\
              &= -frac1amathrmln((u-a)/u)\
              &= -frac1amathrmln(1-a/u).
              endalign






              share|cite|improve this answer

























                up vote
                1
                down vote



                accepted







                up vote
                1
                down vote



                accepted






                To see it, first note that since $ugg a>0$ (assuming they are positive constants), the term $ae^-ut$ will go to $0$ more quickly than $ue^-at$. That is why $v(t)$ can be approximated by $ue^-at/(u-a)v_0$ after a certain time. To compute that time, see that on such a logarithmic scale as in your figure, $ue^-at/(u-a)v_0$ and $e^-atv_0$ correspond to parallel lines. Now since we start at $v_0$, i.e. at $e^-atv_0|_t=0$ and converge to $ue^-at/(u-a)v_0$ then the question can be rephrased to finding the translation from line to line, i.e. solving
                beginalign
                e^-a(t-Delta t)v_0 &= fracuu-ae^-atv_0\
                aDelta t &=mathrmln(u)-mathrmln(u-a)\
                Delta t &= -frac1abig(mathrmln(u-a)-mathrmln(u)big)\
                &= -frac1amathrmln((u-a)/u)\
                &= -frac1amathrmln(1-a/u).
                endalign






                share|cite|improve this answer















                To see it, first note that since $ugg a>0$ (assuming they are positive constants), the term $ae^-ut$ will go to $0$ more quickly than $ue^-at$. That is why $v(t)$ can be approximated by $ue^-at/(u-a)v_0$ after a certain time. To compute that time, see that on such a logarithmic scale as in your figure, $ue^-at/(u-a)v_0$ and $e^-atv_0$ correspond to parallel lines. Now since we start at $v_0$, i.e. at $e^-atv_0|_t=0$ and converge to $ue^-at/(u-a)v_0$ then the question can be rephrased to finding the translation from line to line, i.e. solving
                beginalign
                e^-a(t-Delta t)v_0 &= fracuu-ae^-atv_0\
                aDelta t &=mathrmln(u)-mathrmln(u-a)\
                Delta t &= -frac1abig(mathrmln(u-a)-mathrmln(u)big)\
                &= -frac1amathrmln((u-a)/u)\
                &= -frac1amathrmln(1-a/u).
                endalign







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                share|cite|improve this answer



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                edited Jul 27 at 14:05


























                answered Jul 27 at 12:14









                WalterJ

                793611




                793611






















                     

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