Series Solution for 2nd-Order Homogeneous ODE

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SUMMARY

The discussion focuses on the series solution for a second-order homogeneous ordinary differential equation (ODE) and its relationship with the characteristic polynomial. The series solution, represented by the components a_0 and a_1, is derived from the recurrence relation a_n = (a_1 - a_0)n + a_0/n!. The two bases discussed are {e^x, xe^x} and {e^x, e^x - xe^x}, which correspond to different solution methods. The conclusion emphasizes that while different methods may yield different bases, they should provide the same solution for given initial or boundary conditions.

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  • Understanding of second-order homogeneous ordinary differential equations (ODEs)
  • Familiarity with series solutions and recurrence relations
  • Knowledge of characteristic polynomials in differential equations
  • Basic linear algebra concepts related to vector representation
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rghurst
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TL;DR
Can someone please explain why the solution provided by the characteristic equation does not entirely match the series solution? Thanks.
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Why do you think it doesn't?

Your solution with a_0 = 1 and a_1 = 0 is a solution with y(0) = 1 and y'(0) = 0. e^x doesn't satisfy that, but e^x - xe^x = 1 + \sum_{n=1}^\infty \left(\frac1{n!} - \frac{1}{(n-1)!}\right)x^n = 1 + \sum_{n=1}^\infty \frac{1 -n}{n!}x^n does. Is that series familiar?

Alternatively, if you solve the recurrence relation for a_n you find that <br /> a_n = \frac{(a_1 - a_0)n + a_0}{n!}, and then it is easy to see that <br /> \sum_{n=0}^\infty a_nx^n = (a_1 - a_0)xe^x + a_0e^x.
 
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Thanks. This makes better sense to me. I am still admittedly having a difficult
time seeing why the series solution would not match exactly that provided by the characteristic polynomial.
 
You are representing a vector, y, with respect to two different bases. The first basis - the obvious one obtained from the characteristic polynomial - is \{e^x, xe^x\} and the components are c_1 and c_2. The second basis, obtained from the series solution - is \{e^x, e^x - xe^x\} and the components are a_0 and a_1. These components are related by <br /> \begin{pmatrix} c_1 \\ c_2 \end{pmatrix} = <br /> \begin{pmatrix} 1 &amp; 0 \\ -1 &amp; 1 \end{pmatrix}<br /> \begin{pmatrix} a_0 \\ a_1\end{pmatrix}. You should not expect different solution methods to give you exactly the same basis. However, for given initial or boundary conditions you should expect them to give the same solution.
 
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pasmith said:
You are representing a vector, y, with respect to two different bases. The first basis - the obvious one obtained from the characteristic polynomial - is \{e^x, xe^x\} and the components are c_1 and c_2. The second basis, obtained from the series solution - is \{e^x, e^x - xe^x\} and the components are a_0 and a_1. These components are related by <br /> \begin{pmatrix} c_1 \\ c_2 \end{pmatrix} =<br /> \begin{pmatrix} 1 &amp; 0 \\ -1 &amp; 1 \end{pmatrix}<br /> \begin{pmatrix} a_0 \\ a_1\end{pmatrix}. You should not expect different solution methods to give you exactly the same basis. However, for given initial or boundary conditions you should expect them to give the same solution.
pasmith said:
You are representing a vector, y, with respect to two different bases. The first basis - the obvious one obtained from the characteristic polynomial - is \{e^x, xe^x\} and the components are c_1 and c_2. The second basis, obtained from the series solution - is \{e^x, e^x - xe^x\} and the components are a_0 and a_1. These components are related by <br /> \begin{pmatrix} c_1 \\ c_2 \end{pmatrix} =<br /> \begin{pmatrix} 1 &amp; 0 \\ -1 &amp; 1 \end{pmatrix}<br /> \begin{pmatrix} a_0 \\ a_1\end{pmatrix}. You should not expect different solution methods to give you exactly the same basis. However, for given initial or boundary conditions you should expect them to give the same solution.
This makes full sense to me now. Thanks.
 

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