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]