Find a two term asymptotic expansion of the following problem Announcing the arrival of Valued Associate #679: Cesar Manara Planned maintenance scheduled April 17/18, 2019 at 00:00UTC (8:00pm US/Eastern)Matched asymptotic expansion with interior layer (corner layer?)Asymptotic expansion of $sinleft(pi + exp(-1/epsilon)right)$Asymptotic Inner and Outer Expansion for a FunctionFind the first two terms in the perturbation expansion of the solutionTwo-term asymptotic approximation for roots of an equationUsing the iterative method find terms in the asymptotic expansion of the roots of this polynomialFind a two-term expansion for the root of 1+sqrt(x^2+epsilon)=e^x.Asymptotic expansion for roots of singular cubic equationAsymptotic Expansion of PolynomialFind a two term expansion of the following equation

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Find a two term asymptotic expansion of the following problem



Announcing the arrival of Valued Associate #679: Cesar Manara
Planned maintenance scheduled April 17/18, 2019 at 00:00UTC (8:00pm US/Eastern)Matched asymptotic expansion with interior layer (corner layer?)Asymptotic expansion of $sinleft(pi + exp(-1/epsilon)right)$Asymptotic Inner and Outer Expansion for a FunctionFind the first two terms in the perturbation expansion of the solutionTwo-term asymptotic approximation for roots of an equationUsing the iterative method find terms in the asymptotic expansion of the roots of this polynomialFind a two-term expansion for the root of 1+sqrt(x^2+epsilon)=e^x.Asymptotic expansion for roots of singular cubic equationAsymptotic Expansion of PolynomialFind a two term expansion of the following equation










1












$begingroup$


I want to find a two term asymptotic expansion, for small $epsilon$, of the solution of the following problem:
$$
y'' - epsilon y' - y = 1tag1, , y(0) = 0, ,y(1) = 1
$$

My approach: I assume that the solution has an asymptotic expansion that looks like this:
$$
ysim y_0 + epsilon^alpha y_1 + epsilon^beta y_2 + ldots tag2
$$

with $0<alpha <beta<ldots$.
If I substitute $(2)$ into $(1)$ I get the following equation:
$$
(y_0 + epsilon y_1 + ldots)'' - epsilon(y_0 + epsilon y_1 + ldots)' - (y_0 + epsilon y_1 + ldots) = 1
$$

I will now try to find $y_0, y_1$ by inspecting different order terms:



$mathcalO(1):$ In order to have balance in the equation, $y_0$ must satisfy
$$
y_0'' - y_0 = 1
$$

Solving this equation for $y_0$ gives
$$y_0 = c_1exp((frac12 + sqrt5/2)t) + c_2exp((frac12
) - sqrt5/2)t)$$

This solution needs to satisfy $y(0) = 0$. Substituting $t = 0$ and setting $y_0(0) = 0$ leads to the solution:
$$
y_0 = -dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t)
$$

Furthermore, to have balance we need $alpha = 1$.



$mathcalO(epsilon):$ In order to have balance in the equation $y_1$ must satisfy
$$
y_1'' - y_1 = -y_0'
$$

Or
$$
y_1'' - y_1 = dfracddt(-dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t))
$$

While I could plug this into wolfram to find a solution for $y_1$, I'm not sure whether this is the correct way to find a two term asymptotic expansion for the initial problem.



Question: Am I on the right track? It feels like there must be an easier way to do this. Could someone point me in the right direction?










share|cite|improve this question











$endgroup$
















    1












    $begingroup$


    I want to find a two term asymptotic expansion, for small $epsilon$, of the solution of the following problem:
    $$
    y'' - epsilon y' - y = 1tag1, , y(0) = 0, ,y(1) = 1
    $$

    My approach: I assume that the solution has an asymptotic expansion that looks like this:
    $$
    ysim y_0 + epsilon^alpha y_1 + epsilon^beta y_2 + ldots tag2
    $$

    with $0<alpha <beta<ldots$.
    If I substitute $(2)$ into $(1)$ I get the following equation:
    $$
    (y_0 + epsilon y_1 + ldots)'' - epsilon(y_0 + epsilon y_1 + ldots)' - (y_0 + epsilon y_1 + ldots) = 1
    $$

    I will now try to find $y_0, y_1$ by inspecting different order terms:



    $mathcalO(1):$ In order to have balance in the equation, $y_0$ must satisfy
    $$
    y_0'' - y_0 = 1
    $$

    Solving this equation for $y_0$ gives
    $$y_0 = c_1exp((frac12 + sqrt5/2)t) + c_2exp((frac12
    ) - sqrt5/2)t)$$

    This solution needs to satisfy $y(0) = 0$. Substituting $t = 0$ and setting $y_0(0) = 0$ leads to the solution:
    $$
    y_0 = -dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t)
    $$

    Furthermore, to have balance we need $alpha = 1$.



    $mathcalO(epsilon):$ In order to have balance in the equation $y_1$ must satisfy
    $$
    y_1'' - y_1 = -y_0'
    $$

    Or
    $$
    y_1'' - y_1 = dfracddt(-dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t))
    $$

    While I could plug this into wolfram to find a solution for $y_1$, I'm not sure whether this is the correct way to find a two term asymptotic expansion for the initial problem.



    Question: Am I on the right track? It feels like there must be an easier way to do this. Could someone point me in the right direction?










    share|cite|improve this question











    $endgroup$














      1












      1








      1





      $begingroup$


      I want to find a two term asymptotic expansion, for small $epsilon$, of the solution of the following problem:
      $$
      y'' - epsilon y' - y = 1tag1, , y(0) = 0, ,y(1) = 1
      $$

      My approach: I assume that the solution has an asymptotic expansion that looks like this:
      $$
      ysim y_0 + epsilon^alpha y_1 + epsilon^beta y_2 + ldots tag2
      $$

      with $0<alpha <beta<ldots$.
      If I substitute $(2)$ into $(1)$ I get the following equation:
      $$
      (y_0 + epsilon y_1 + ldots)'' - epsilon(y_0 + epsilon y_1 + ldots)' - (y_0 + epsilon y_1 + ldots) = 1
      $$

      I will now try to find $y_0, y_1$ by inspecting different order terms:



      $mathcalO(1):$ In order to have balance in the equation, $y_0$ must satisfy
      $$
      y_0'' - y_0 = 1
      $$

      Solving this equation for $y_0$ gives
      $$y_0 = c_1exp((frac12 + sqrt5/2)t) + c_2exp((frac12
      ) - sqrt5/2)t)$$

      This solution needs to satisfy $y(0) = 0$. Substituting $t = 0$ and setting $y_0(0) = 0$ leads to the solution:
      $$
      y_0 = -dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t)
      $$

      Furthermore, to have balance we need $alpha = 1$.



      $mathcalO(epsilon):$ In order to have balance in the equation $y_1$ must satisfy
      $$
      y_1'' - y_1 = -y_0'
      $$

      Or
      $$
      y_1'' - y_1 = dfracddt(-dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t))
      $$

      While I could plug this into wolfram to find a solution for $y_1$, I'm not sure whether this is the correct way to find a two term asymptotic expansion for the initial problem.



      Question: Am I on the right track? It feels like there must be an easier way to do this. Could someone point me in the right direction?










      share|cite|improve this question











      $endgroup$




      I want to find a two term asymptotic expansion, for small $epsilon$, of the solution of the following problem:
      $$
      y'' - epsilon y' - y = 1tag1, , y(0) = 0, ,y(1) = 1
      $$

      My approach: I assume that the solution has an asymptotic expansion that looks like this:
      $$
      ysim y_0 + epsilon^alpha y_1 + epsilon^beta y_2 + ldots tag2
      $$

      with $0<alpha <beta<ldots$.
      If I substitute $(2)$ into $(1)$ I get the following equation:
      $$
      (y_0 + epsilon y_1 + ldots)'' - epsilon(y_0 + epsilon y_1 + ldots)' - (y_0 + epsilon y_1 + ldots) = 1
      $$

      I will now try to find $y_0, y_1$ by inspecting different order terms:



      $mathcalO(1):$ In order to have balance in the equation, $y_0$ must satisfy
      $$
      y_0'' - y_0 = 1
      $$

      Solving this equation for $y_0$ gives
      $$y_0 = c_1exp((frac12 + sqrt5/2)t) + c_2exp((frac12
      ) - sqrt5/2)t)$$

      This solution needs to satisfy $y(0) = 0$. Substituting $t = 0$ and setting $y_0(0) = 0$ leads to the solution:
      $$
      y_0 = -dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t)
      $$

      Furthermore, to have balance we need $alpha = 1$.



      $mathcalO(epsilon):$ In order to have balance in the equation $y_1$ must satisfy
      $$
      y_1'' - y_1 = -y_0'
      $$

      Or
      $$
      y_1'' - y_1 = dfracddt(-dfrac1e^1/2 - sqrt5/2exp((1/2 + sqrt5/2)t) + dfrac1e^1/2 - sqrt5/2exp((1/2 - sqrt5/2)t))
      $$

      While I could plug this into wolfram to find a solution for $y_1$, I'm not sure whether this is the correct way to find a two term asymptotic expansion for the initial problem.



      Question: Am I on the right track? It feels like there must be an easier way to do this. Could someone point me in the right direction?







      calculus asymptotics perturbation-theory






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




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      edited yesterday









      Martin Sleziak

      45k10123277




      45k10123277










      asked Mar 26 at 10:17









      TitusTitus

      1145




      1145




















          1 Answer
          1






          active

          oldest

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          0












          $begingroup$

          My calculation is different from yours. Let
          $$
          y=y_0 + epsilon y_1 +O(epsilon^2)
          $$

          in the equation to get
          $$ (y''_0 + epsilon y''_1 +O(epsilon^2))-epsilon(y'_0 + epsilon y'_1 +O(epsilon^2))-(y_0 + epsilon y_1 +O(epsilon^2))=1. tag1 $$
          Then the boundary conditions $y(0)=0,y(1)=1$ become
          $$ y_0(0)=y_1(0)=0, y_0(1)=1,y_1(0)=0.$$
          $O(1)$:
          $$ y''_0-y_0=1, y_0(0)=0,y_0(1)=1 $$
          which has the solution
          $$ y_0= frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1. $$
          $O(epsilon)$:
          $$ y''_1-y_1=y_0', y_1(0)=0,y_1(1)=0 $$
          which has the solution
          begineqnarray* y_1&=& frac12 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*

          Thus
          begineqnarray*
          y&=&y_0+epsilon y_1+O(epsilon^2)\
          &=&frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1\
          && +fracepsilon2 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
            $endgroup$
            – Maxim
            Apr 1 at 14:03











          Your Answer








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          1 Answer
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          active

          oldest

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          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes









          0












          $begingroup$

          My calculation is different from yours. Let
          $$
          y=y_0 + epsilon y_1 +O(epsilon^2)
          $$

          in the equation to get
          $$ (y''_0 + epsilon y''_1 +O(epsilon^2))-epsilon(y'_0 + epsilon y'_1 +O(epsilon^2))-(y_0 + epsilon y_1 +O(epsilon^2))=1. tag1 $$
          Then the boundary conditions $y(0)=0,y(1)=1$ become
          $$ y_0(0)=y_1(0)=0, y_0(1)=1,y_1(0)=0.$$
          $O(1)$:
          $$ y''_0-y_0=1, y_0(0)=0,y_0(1)=1 $$
          which has the solution
          $$ y_0= frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1. $$
          $O(epsilon)$:
          $$ y''_1-y_1=y_0', y_1(0)=0,y_1(1)=0 $$
          which has the solution
          begineqnarray* y_1&=& frac12 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*

          Thus
          begineqnarray*
          y&=&y_0+epsilon y_1+O(epsilon^2)\
          &=&frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1\
          && +fracepsilon2 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
            $endgroup$
            – Maxim
            Apr 1 at 14:03















          0












          $begingroup$

          My calculation is different from yours. Let
          $$
          y=y_0 + epsilon y_1 +O(epsilon^2)
          $$

          in the equation to get
          $$ (y''_0 + epsilon y''_1 +O(epsilon^2))-epsilon(y'_0 + epsilon y'_1 +O(epsilon^2))-(y_0 + epsilon y_1 +O(epsilon^2))=1. tag1 $$
          Then the boundary conditions $y(0)=0,y(1)=1$ become
          $$ y_0(0)=y_1(0)=0, y_0(1)=1,y_1(0)=0.$$
          $O(1)$:
          $$ y''_0-y_0=1, y_0(0)=0,y_0(1)=1 $$
          which has the solution
          $$ y_0= frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1. $$
          $O(epsilon)$:
          $$ y''_1-y_1=y_0', y_1(0)=0,y_1(1)=0 $$
          which has the solution
          begineqnarray* y_1&=& frac12 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*

          Thus
          begineqnarray*
          y&=&y_0+epsilon y_1+O(epsilon^2)\
          &=&frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1\
          && +fracepsilon2 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
            $endgroup$
            – Maxim
            Apr 1 at 14:03













          0












          0








          0





          $begingroup$

          My calculation is different from yours. Let
          $$
          y=y_0 + epsilon y_1 +O(epsilon^2)
          $$

          in the equation to get
          $$ (y''_0 + epsilon y''_1 +O(epsilon^2))-epsilon(y'_0 + epsilon y'_1 +O(epsilon^2))-(y_0 + epsilon y_1 +O(epsilon^2))=1. tag1 $$
          Then the boundary conditions $y(0)=0,y(1)=1$ become
          $$ y_0(0)=y_1(0)=0, y_0(1)=1,y_1(0)=0.$$
          $O(1)$:
          $$ y''_0-y_0=1, y_0(0)=0,y_0(1)=1 $$
          which has the solution
          $$ y_0= frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1. $$
          $O(epsilon)$:
          $$ y''_1-y_1=y_0', y_1(0)=0,y_1(1)=0 $$
          which has the solution
          begineqnarray* y_1&=& frac12 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*

          Thus
          begineqnarray*
          y&=&y_0+epsilon y_1+O(epsilon^2)\
          &=&frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1\
          && +fracepsilon2 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*






          share|cite|improve this answer











          $endgroup$



          My calculation is different from yours. Let
          $$
          y=y_0 + epsilon y_1 +O(epsilon^2)
          $$

          in the equation to get
          $$ (y''_0 + epsilon y''_1 +O(epsilon^2))-epsilon(y'_0 + epsilon y'_1 +O(epsilon^2))-(y_0 + epsilon y_1 +O(epsilon^2))=1. tag1 $$
          Then the boundary conditions $y(0)=0,y(1)=1$ become
          $$ y_0(0)=y_1(0)=0, y_0(1)=1,y_1(0)=0.$$
          $O(1)$:
          $$ y''_0-y_0=1, y_0(0)=0,y_0(1)=1 $$
          which has the solution
          $$ y_0= frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1. $$
          $O(epsilon)$:
          $$ y''_1-y_1=y_0', y_1(0)=0,y_1(1)=0 $$
          which has the solution
          begineqnarray* y_1&=& frac12 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*

          Thus
          begineqnarray*
          y&=&y_0+epsilon y_1+O(epsilon^2)\
          &=&frace^-x left(e^x-e^2 x-e^x+2+2 e^2 x+1-2 e+e^2right)e^2-1\
          && +fracepsilon2 left(e^2-1right)^2bigg[e^-x (-e^2 x+2 (x-4)+2 e^x-4 e^x+2+2 e^x+4+e^2 x (x-2)+2 e^2 x+3 (x-2)\
          &&-2 e^2 x+1 x+e^2 x-2 e x-e^4 (x+2)+2 e^3 (x+2))bigg].
          endeqnarray*







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Mar 28 at 13:52

























          answered Mar 27 at 15:09









          xpaulxpaul

          23.5k24655




          23.5k24655











          • $begingroup$
            The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
            $endgroup$
            – Maxim
            Apr 1 at 14:03
















          • $begingroup$
            The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
            $endgroup$
            – Maxim
            Apr 1 at 14:03















          $begingroup$
          The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
          $endgroup$
          – Maxim
          Apr 1 at 14:03




          $begingroup$
          The solution for the ODE for $y_1$is $$y_1(x) = frac e^-x (2 (x - 1) e^2 x + 1 - x e^2 x + e (e - 2) x + 2 e) 2 (e^2 - 1).$$
          $endgroup$
          – Maxim
          Apr 1 at 14:03

















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