Integro-differential equation including a convolution of the first derivative.












2












$begingroup$


I am having difficulty finding the right approach to solving the following differential equation,
$$
y''(t)+int_t^Tg(s-t)y'(s),ds=f(t),
$$

with the boundary conditions,
$$y(0)=y_0,,quad y(T)=0.$$
I considered representing $y(t)$ using a Fourier series, but term-wise differentiation is not guaranteed because the periodic extension of $y(t)$ isn't
differentiable at the boundaries $t=0,T$.



What approach is the smartest to solve this equation? Any help will be appreciated.










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$endgroup$












  • $begingroup$
    Just a thought, but can you subtract off the boundary by writing $y(t) = u(t) + frac{y_0}{T}(T-t)$? Then due to linearity, $u(t)$ would satisfy a very similar equation
    $endgroup$
    – Dylan
    Jan 9 at 18:42










  • $begingroup$
    @Dylan I considered that too. In that case, the first derivative of the Fourier series would indeed converge to $y'(t)$, but $y'(0) = y'(T)$ is not guaranteed so the second derivative of the Fourier series would NOT converge to $y''(t)$.
    $endgroup$
    – honey.mustard
    Jan 10 at 1:21
















2












$begingroup$


I am having difficulty finding the right approach to solving the following differential equation,
$$
y''(t)+int_t^Tg(s-t)y'(s),ds=f(t),
$$

with the boundary conditions,
$$y(0)=y_0,,quad y(T)=0.$$
I considered representing $y(t)$ using a Fourier series, but term-wise differentiation is not guaranteed because the periodic extension of $y(t)$ isn't
differentiable at the boundaries $t=0,T$.



What approach is the smartest to solve this equation? Any help will be appreciated.










share|cite|improve this question











$endgroup$












  • $begingroup$
    Just a thought, but can you subtract off the boundary by writing $y(t) = u(t) + frac{y_0}{T}(T-t)$? Then due to linearity, $u(t)$ would satisfy a very similar equation
    $endgroup$
    – Dylan
    Jan 9 at 18:42










  • $begingroup$
    @Dylan I considered that too. In that case, the first derivative of the Fourier series would indeed converge to $y'(t)$, but $y'(0) = y'(T)$ is not guaranteed so the second derivative of the Fourier series would NOT converge to $y''(t)$.
    $endgroup$
    – honey.mustard
    Jan 10 at 1:21














2












2








2


1



$begingroup$


I am having difficulty finding the right approach to solving the following differential equation,
$$
y''(t)+int_t^Tg(s-t)y'(s),ds=f(t),
$$

with the boundary conditions,
$$y(0)=y_0,,quad y(T)=0.$$
I considered representing $y(t)$ using a Fourier series, but term-wise differentiation is not guaranteed because the periodic extension of $y(t)$ isn't
differentiable at the boundaries $t=0,T$.



What approach is the smartest to solve this equation? Any help will be appreciated.










share|cite|improve this question











$endgroup$




I am having difficulty finding the right approach to solving the following differential equation,
$$
y''(t)+int_t^Tg(s-t)y'(s),ds=f(t),
$$

with the boundary conditions,
$$y(0)=y_0,,quad y(T)=0.$$
I considered representing $y(t)$ using a Fourier series, but term-wise differentiation is not guaranteed because the periodic extension of $y(t)$ isn't
differentiable at the boundaries $t=0,T$.



What approach is the smartest to solve this equation? Any help will be appreciated.







ordinary-differential-equations convolution boundary-value-problem integro-differential-equations






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edited Jan 9 at 15:36









Adrian Keister

5,26571933




5,26571933










asked Jan 9 at 15:22









honey.mustardhoney.mustard

8619




8619












  • $begingroup$
    Just a thought, but can you subtract off the boundary by writing $y(t) = u(t) + frac{y_0}{T}(T-t)$? Then due to linearity, $u(t)$ would satisfy a very similar equation
    $endgroup$
    – Dylan
    Jan 9 at 18:42










  • $begingroup$
    @Dylan I considered that too. In that case, the first derivative of the Fourier series would indeed converge to $y'(t)$, but $y'(0) = y'(T)$ is not guaranteed so the second derivative of the Fourier series would NOT converge to $y''(t)$.
    $endgroup$
    – honey.mustard
    Jan 10 at 1:21


















  • $begingroup$
    Just a thought, but can you subtract off the boundary by writing $y(t) = u(t) + frac{y_0}{T}(T-t)$? Then due to linearity, $u(t)$ would satisfy a very similar equation
    $endgroup$
    – Dylan
    Jan 9 at 18:42










  • $begingroup$
    @Dylan I considered that too. In that case, the first derivative of the Fourier series would indeed converge to $y'(t)$, but $y'(0) = y'(T)$ is not guaranteed so the second derivative of the Fourier series would NOT converge to $y''(t)$.
    $endgroup$
    – honey.mustard
    Jan 10 at 1:21
















$begingroup$
Just a thought, but can you subtract off the boundary by writing $y(t) = u(t) + frac{y_0}{T}(T-t)$? Then due to linearity, $u(t)$ would satisfy a very similar equation
$endgroup$
– Dylan
Jan 9 at 18:42




$begingroup$
Just a thought, but can you subtract off the boundary by writing $y(t) = u(t) + frac{y_0}{T}(T-t)$? Then due to linearity, $u(t)$ would satisfy a very similar equation
$endgroup$
– Dylan
Jan 9 at 18:42












$begingroup$
@Dylan I considered that too. In that case, the first derivative of the Fourier series would indeed converge to $y'(t)$, but $y'(0) = y'(T)$ is not guaranteed so the second derivative of the Fourier series would NOT converge to $y''(t)$.
$endgroup$
– honey.mustard
Jan 10 at 1:21




$begingroup$
@Dylan I considered that too. In that case, the first derivative of the Fourier series would indeed converge to $y'(t)$, but $y'(0) = y'(T)$ is not guaranteed so the second derivative of the Fourier series would NOT converge to $y''(t)$.
$endgroup$
– honey.mustard
Jan 10 at 1:21










1 Answer
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$begingroup$

Set $v(t) = y'(t)$. Thus $y(t) = - int_t^T v(s) , ds$.



Now solve the first order integrodifferential equation
$$
v'(t)+int_t^Tg(s-t)v(s),ds=f(t), ; v(T) = alpha
$$

for general $alpha in mathbb{R}$. The solution may be expressed in the form
$$
v(t) = alpha r(t) + int_t^T r(s-t)f(s), ds = alpha r(t) + tilde f(t)
$$


where $r$ is known as differential resolvent (see monographs on integral equations, e.g. Gripenberg - Londen - Staffans, CUP 1990, Theorem 3.1). Therefore
$$
y(t) = - int_t^T v(s) ds = - alpha int_t^T r(s) ds - int_t^T tilde f(s) , ds
$$

Set $t = 0$ to find the right value of $alpha$. This gives a unique solution if $int_0^T r(t) , dt ne 0$. If $int_0^T r(t) , dt = 0$, there either are infinitely many solutions or there is no solution, depending on whether $int_0^T tilde f(s) + y_0 = 0$ or not.






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    active

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    1












    $begingroup$

    Set $v(t) = y'(t)$. Thus $y(t) = - int_t^T v(s) , ds$.



    Now solve the first order integrodifferential equation
    $$
    v'(t)+int_t^Tg(s-t)v(s),ds=f(t), ; v(T) = alpha
    $$

    for general $alpha in mathbb{R}$. The solution may be expressed in the form
    $$
    v(t) = alpha r(t) + int_t^T r(s-t)f(s), ds = alpha r(t) + tilde f(t)
    $$


    where $r$ is known as differential resolvent (see monographs on integral equations, e.g. Gripenberg - Londen - Staffans, CUP 1990, Theorem 3.1). Therefore
    $$
    y(t) = - int_t^T v(s) ds = - alpha int_t^T r(s) ds - int_t^T tilde f(s) , ds
    $$

    Set $t = 0$ to find the right value of $alpha$. This gives a unique solution if $int_0^T r(t) , dt ne 0$. If $int_0^T r(t) , dt = 0$, there either are infinitely many solutions or there is no solution, depending on whether $int_0^T tilde f(s) + y_0 = 0$ or not.






    share|cite|improve this answer









    $endgroup$


















      1












      $begingroup$

      Set $v(t) = y'(t)$. Thus $y(t) = - int_t^T v(s) , ds$.



      Now solve the first order integrodifferential equation
      $$
      v'(t)+int_t^Tg(s-t)v(s),ds=f(t), ; v(T) = alpha
      $$

      for general $alpha in mathbb{R}$. The solution may be expressed in the form
      $$
      v(t) = alpha r(t) + int_t^T r(s-t)f(s), ds = alpha r(t) + tilde f(t)
      $$


      where $r$ is known as differential resolvent (see monographs on integral equations, e.g. Gripenberg - Londen - Staffans, CUP 1990, Theorem 3.1). Therefore
      $$
      y(t) = - int_t^T v(s) ds = - alpha int_t^T r(s) ds - int_t^T tilde f(s) , ds
      $$

      Set $t = 0$ to find the right value of $alpha$. This gives a unique solution if $int_0^T r(t) , dt ne 0$. If $int_0^T r(t) , dt = 0$, there either are infinitely many solutions or there is no solution, depending on whether $int_0^T tilde f(s) + y_0 = 0$ or not.






      share|cite|improve this answer









      $endgroup$
















        1












        1








        1





        $begingroup$

        Set $v(t) = y'(t)$. Thus $y(t) = - int_t^T v(s) , ds$.



        Now solve the first order integrodifferential equation
        $$
        v'(t)+int_t^Tg(s-t)v(s),ds=f(t), ; v(T) = alpha
        $$

        for general $alpha in mathbb{R}$. The solution may be expressed in the form
        $$
        v(t) = alpha r(t) + int_t^T r(s-t)f(s), ds = alpha r(t) + tilde f(t)
        $$


        where $r$ is known as differential resolvent (see monographs on integral equations, e.g. Gripenberg - Londen - Staffans, CUP 1990, Theorem 3.1). Therefore
        $$
        y(t) = - int_t^T v(s) ds = - alpha int_t^T r(s) ds - int_t^T tilde f(s) , ds
        $$

        Set $t = 0$ to find the right value of $alpha$. This gives a unique solution if $int_0^T r(t) , dt ne 0$. If $int_0^T r(t) , dt = 0$, there either are infinitely many solutions or there is no solution, depending on whether $int_0^T tilde f(s) + y_0 = 0$ or not.






        share|cite|improve this answer









        $endgroup$



        Set $v(t) = y'(t)$. Thus $y(t) = - int_t^T v(s) , ds$.



        Now solve the first order integrodifferential equation
        $$
        v'(t)+int_t^Tg(s-t)v(s),ds=f(t), ; v(T) = alpha
        $$

        for general $alpha in mathbb{R}$. The solution may be expressed in the form
        $$
        v(t) = alpha r(t) + int_t^T r(s-t)f(s), ds = alpha r(t) + tilde f(t)
        $$


        where $r$ is known as differential resolvent (see monographs on integral equations, e.g. Gripenberg - Londen - Staffans, CUP 1990, Theorem 3.1). Therefore
        $$
        y(t) = - int_t^T v(s) ds = - alpha int_t^T r(s) ds - int_t^T tilde f(s) , ds
        $$

        Set $t = 0$ to find the right value of $alpha$. This gives a unique solution if $int_0^T r(t) , dt ne 0$. If $int_0^T r(t) , dt = 0$, there either are infinitely many solutions or there is no solution, depending on whether $int_0^T tilde f(s) + y_0 = 0$ or not.







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Jan 10 at 3:11









        Hans EnglerHans Engler

        10.5k11836




        10.5k11836






























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