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Can someone help me prove that given

$$ y'' + \frac{2}{x}y' + \lambda y = 0 $$

and boundary conditions

$$ {\lim_{x \to 0} xy = 0 , \hspace{5mm} y(1) =0 } $$

that

$$ y(x) = \frac{1}{x}\left[ A \sin{(\sqrt{\lambda}x)} + B \cos{(\sqrt\lambda x)} \right] $$

When trying to solve it the usual way I get

$$ m^2 + \frac{2}{x}m + \lambda = 0 $$ $$ m = -\frac{1}{x} \pm j\sqrt{\lambda - \frac{1}{x^2}}$$

which obviously won't me to the solution because I have the $\sqrt{\lambda - \frac{1}{x^2}}$ term instead of a $\sqrt{\lambda x}$ term.

Ron Gordon
  • 141,538
KillaKem
  • 715

2 Answers2

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Set $u(x) = x y(x)$. You may then show that

$$u'' + \lambda u = 0$$

with $u(0)=0$ and $u(1)=0$. Now solve as usual. When you get the solution for $u(x)$, then $y(x)=u(x)/x$.

EDIT

A few more details about where the above equation comes from. Note that

$$ y' = \frac{x u'-u}{x^2} $$

$$ y'' = \frac{x u'' - u'}{x^2} - \frac{x^2 u' - 2 x u}{x^4} $$

Plugging this back into the original equation above results in

$$\frac{u''}{x} + \lambda \frac{u}{x} = 0$$

which results in the derived equation for $u$ above.

Ron Gordon
  • 141,538
0

Here is a related problem. Already, you have given the solution $ y(x) $

$$ y(x) = \frac{1}{x}\left[ A \sin{(\sqrt{\lambda}x)} + B \cos{(\sqrt\lambda x)} \right]. $$

and you need to find the eigenvalues $\lambda$ and the corresponding eigenfunctions. Exploiting the boundary conditions we get the two equations

$$ 0 = B. $$

$$ 0 = A \sin( \sqrt{\lambda} ) + B\cos(\sqrt{\lambda} ). $$

From the above two equations, we have

$$ \sin(\sqrt{\lambda}) = 0 \implies \lambda_n = n^2\pi^2 . $$

Now, you can find the eigenfunctions corresponding to $\lambda_n$.