Eigenvalues Sturm-Liouville system

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SUMMARY

The discussion focuses on solving the auxiliary equation derived from the Sturm-Liouville system represented by the differential equation \(y^{''} + 2y^{'} + \alpha^{2}y = 0\) with \(\lambda > 1\) and \(\alpha > 0\). The solution involves completing the square or using the quadratic formula to find the roots, leading to the expression \(m = i \sqrt{\alpha^{2} - 1} - 1\). The general solution for \(y\) is given as \(y = e^{-x}\left( C_{1}\cos(x\sqrt{\alpha^{2} - 1}) + C_{2}\sin(x\sqrt{\alpha^{2} - 1}) \right)\), with boundary conditions determining the constants \(C_{1}\) and \(C_{2}\). Ultimately, the eigenvalues are expressed as \(\alpha^{2} = \frac{n^{2} \pi^{2}}{L^{2}} + 1 = \lambda_{n}\) for \(n \in \mathbb{Z}, n \geq 1\).

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Homework Statement



See figure attached

Homework Equations





The Attempt at a Solution



[tex]\lambda > 1,[/tex]

[tex]y^{''} + 2y^{'} + \alpha^{2}y = 0, \quad \alpha > 0[/tex]

Into auxillary equation,

[tex]m^{2} + 2m + \alpha^{2} = 0[/tex]

I'm stuck as to how to solve this auxillary equation.

Any ideas?

Thanks again!
 

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Either complete the square on m or use the quadratic formula.
 
LCKurtz said:
Either complete the square on m or use the quadratic formula.

Okay so completing the square,

[tex]m^{2} + 2m + 1 = - \alpha^{2} +1[/tex]

[tex](m+1)^{2} = - \alpha^{2} + 1[/tex]

[tex]m= \sqrt{- \alpha^{2} + 1} - 1[/tex]

[tex]\forall \quad \alpha > 0, \quad \sqrt{- \alpha^{2} + 1} \quad \stackrel{\leftrightarrow}{ iff } \quad i \sqrt{\alpha^{2} - 1}[/tex]

So,

[tex]m = i \sqrt{\alpha^{2} - 1} -1[/tex]

Then,

[tex]y = e^{-x}\left( C_{1}cos(x\sqrt{\alpha^{2} - 1}) + C_{2}sin(x\sqrt{\alpha^{2} - 1}) \right)[/tex]

Using the boundary conditions,

[tex]C_{1} = 0,[/tex]

[tex]C_{2}e^{-L}sin(L\sqrt{\alpha^{2} - 1}) = 0, \quad C_{2} \neq 0[/tex]

[tex]\alpha^{2} = \frac{n^{2} \pi^{2}}{L^{2}} + 1 = \lambda_{n}, \quad n \in Z, n \geq 1[/tex]

So,

[tex]y_{n}(x) = e^{-x}sin(\frac{n\pi x}{L})[/tex]
 
Last edited:

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