Solution to a second-order nonlinear ordinary differential equation












1












$begingroup$


I am given three functions $z'(t), y'(t), x'(t)$ and I have reduced these functions to the equation:
begin{equation}
z''=x_{0}beta z'e^{-frac{beta}{gamma}z} - gamma z
end{equation}

where $beta, gamma ,x_{0}$ are constants.
Next we introduce a new function:
begin{equation}
u(t)=e^{-frac{beta}{gamma}z}
end{equation}

Substitution yields
begin{equation}
ufrac{d^{2}u}{dt^{2}}- bigg(frac{du}{dt}bigg)^{2}+(gamma - x_{0}beta u)ufrac{du}{dt} = 0
end{equation}

Next a new function is introduced:
begin{equation}
phi = frac{dt}{du}
end{equation}

Now the equation can be rearranged to:
begin{equation}
frac{dphi}{du}+frac{1}{u} phi = (gamma-x_{0}beta u )phi^{2}
end{equation}

The solution to this equation is:
begin{equation}
phi = frac{1}{u(C_{1}-gamma ln u +x_{0}beta u)}
end{equation}

So what would be the solution to the original equation in terms of $u$?










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$endgroup$












  • $begingroup$
    The ordinary differential equation (ODE) that you write down for $u$ is equivalent to $z'' = x_0 beta z' e^{-frac{beta}{gamma} z} - gamma z'$. So there is either a mistake in the original ODE for $z$ or in the ODE for $u$. Please check.
    $endgroup$
    – Christoph
    Jan 16 at 2:31


















1












$begingroup$


I am given three functions $z'(t), y'(t), x'(t)$ and I have reduced these functions to the equation:
begin{equation}
z''=x_{0}beta z'e^{-frac{beta}{gamma}z} - gamma z
end{equation}

where $beta, gamma ,x_{0}$ are constants.
Next we introduce a new function:
begin{equation}
u(t)=e^{-frac{beta}{gamma}z}
end{equation}

Substitution yields
begin{equation}
ufrac{d^{2}u}{dt^{2}}- bigg(frac{du}{dt}bigg)^{2}+(gamma - x_{0}beta u)ufrac{du}{dt} = 0
end{equation}

Next a new function is introduced:
begin{equation}
phi = frac{dt}{du}
end{equation}

Now the equation can be rearranged to:
begin{equation}
frac{dphi}{du}+frac{1}{u} phi = (gamma-x_{0}beta u )phi^{2}
end{equation}

The solution to this equation is:
begin{equation}
phi = frac{1}{u(C_{1}-gamma ln u +x_{0}beta u)}
end{equation}

So what would be the solution to the original equation in terms of $u$?










share|cite|improve this question









$endgroup$












  • $begingroup$
    The ordinary differential equation (ODE) that you write down for $u$ is equivalent to $z'' = x_0 beta z' e^{-frac{beta}{gamma} z} - gamma z'$. So there is either a mistake in the original ODE for $z$ or in the ODE for $u$. Please check.
    $endgroup$
    – Christoph
    Jan 16 at 2:31
















1












1








1





$begingroup$


I am given three functions $z'(t), y'(t), x'(t)$ and I have reduced these functions to the equation:
begin{equation}
z''=x_{0}beta z'e^{-frac{beta}{gamma}z} - gamma z
end{equation}

where $beta, gamma ,x_{0}$ are constants.
Next we introduce a new function:
begin{equation}
u(t)=e^{-frac{beta}{gamma}z}
end{equation}

Substitution yields
begin{equation}
ufrac{d^{2}u}{dt^{2}}- bigg(frac{du}{dt}bigg)^{2}+(gamma - x_{0}beta u)ufrac{du}{dt} = 0
end{equation}

Next a new function is introduced:
begin{equation}
phi = frac{dt}{du}
end{equation}

Now the equation can be rearranged to:
begin{equation}
frac{dphi}{du}+frac{1}{u} phi = (gamma-x_{0}beta u )phi^{2}
end{equation}

The solution to this equation is:
begin{equation}
phi = frac{1}{u(C_{1}-gamma ln u +x_{0}beta u)}
end{equation}

So what would be the solution to the original equation in terms of $u$?










share|cite|improve this question









$endgroup$




I am given three functions $z'(t), y'(t), x'(t)$ and I have reduced these functions to the equation:
begin{equation}
z''=x_{0}beta z'e^{-frac{beta}{gamma}z} - gamma z
end{equation}

where $beta, gamma ,x_{0}$ are constants.
Next we introduce a new function:
begin{equation}
u(t)=e^{-frac{beta}{gamma}z}
end{equation}

Substitution yields
begin{equation}
ufrac{d^{2}u}{dt^{2}}- bigg(frac{du}{dt}bigg)^{2}+(gamma - x_{0}beta u)ufrac{du}{dt} = 0
end{equation}

Next a new function is introduced:
begin{equation}
phi = frac{dt}{du}
end{equation}

Now the equation can be rearranged to:
begin{equation}
frac{dphi}{du}+frac{1}{u} phi = (gamma-x_{0}beta u )phi^{2}
end{equation}

The solution to this equation is:
begin{equation}
phi = frac{1}{u(C_{1}-gamma ln u +x_{0}beta u)}
end{equation}

So what would be the solution to the original equation in terms of $u$?







real-analysis calculus ordinary-differential-equations






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asked Jan 15 at 17:10









wittgensteinsrulerwittgensteinsruler

243




243












  • $begingroup$
    The ordinary differential equation (ODE) that you write down for $u$ is equivalent to $z'' = x_0 beta z' e^{-frac{beta}{gamma} z} - gamma z'$. So there is either a mistake in the original ODE for $z$ or in the ODE for $u$. Please check.
    $endgroup$
    – Christoph
    Jan 16 at 2:31




















  • $begingroup$
    The ordinary differential equation (ODE) that you write down for $u$ is equivalent to $z'' = x_0 beta z' e^{-frac{beta}{gamma} z} - gamma z'$. So there is either a mistake in the original ODE for $z$ or in the ODE for $u$. Please check.
    $endgroup$
    – Christoph
    Jan 16 at 2:31


















$begingroup$
The ordinary differential equation (ODE) that you write down for $u$ is equivalent to $z'' = x_0 beta z' e^{-frac{beta}{gamma} z} - gamma z'$. So there is either a mistake in the original ODE for $z$ or in the ODE for $u$. Please check.
$endgroup$
– Christoph
Jan 16 at 2:31






$begingroup$
The ordinary differential equation (ODE) that you write down for $u$ is equivalent to $z'' = x_0 beta z' e^{-frac{beta}{gamma} z} - gamma z'$. So there is either a mistake in the original ODE for $z$ or in the ODE for $u$. Please check.
$endgroup$
– Christoph
Jan 16 at 2:31












1 Answer
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$begingroup$

The last equation od
$$
frac{dt}{du}=frac{1}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
$$

Integrating
$$
t=intfrac{du}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
$$

I do not think that there is a closed formula for the integral.






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    $begingroup$

    The last equation od
    $$
    frac{dt}{du}=frac{1}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
    $$

    Integrating
    $$
    t=intfrac{du}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
    $$

    I do not think that there is a closed formula for the integral.






    share|cite|improve this answer









    $endgroup$


















      0












      $begingroup$

      The last equation od
      $$
      frac{dt}{du}=frac{1}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
      $$

      Integrating
      $$
      t=intfrac{du}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
      $$

      I do not think that there is a closed formula for the integral.






      share|cite|improve this answer









      $endgroup$
















        0












        0








        0





        $begingroup$

        The last equation od
        $$
        frac{dt}{du}=frac{1}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
        $$

        Integrating
        $$
        t=intfrac{du}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
        $$

        I do not think that there is a closed formula for the integral.






        share|cite|improve this answer









        $endgroup$



        The last equation od
        $$
        frac{dt}{du}=frac{1}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
        $$

        Integrating
        $$
        t=intfrac{du}{u(C_{1}-gamma ln u +x_{0}beta, u)}.
        $$

        I do not think that there is a closed formula for the integral.







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Jan 15 at 22:52









        Julián AguirreJulián Aguirre

        69.5k24297




        69.5k24297






























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