Generals 2005 I 1

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We consider the differential equation:

\frac{d^{2}y}{dx^{2}}+\frac{1}{x^{2}}\frac{dy}{dx}+\frac{1}{x^{2}}y=0


[edit] Part a

For x˜0, the equation is singular, so we guess y˜eS:

\left(S^{\prime\prime}+\left(S^{\prime}\right)^{2}\right)+\frac{S^{\prime}}{x^{2}}+\frac{1}{x^{2}}=0


Balance between \left(S^{\prime}\right)^{2} and S^{\prime}/x^{2} gives S^{\prime}=-x^{-2}, which is dominant. There is an alternate balance between S^{\prime}/x^{2} and x − 2, giving S^{\prime}=-1. Finding the next term g for the first case:

\left(\frac{2}{x^{3}}+g^{\prime\prime}-\frac{2g^{\prime}}{x^{2}}+\left(g^{\prime}\right)^{2}\right)+\frac{g^{\prime}}{x^{2}}+\frac{1}{x^{2}}=0


So balance between 2 / x3 and g^{\prime}/x^{2} gives g^{\prime}=x^{-1}. The other term is already less singular that lnx. The leading asymptotic forms are then:

y\sim xe^{1/x},\quad e^{-x}


[edit] Part b

For x\rightarrow\infty, the equation is again singular, so, guessing $y\sim e^{S}</math>:

\left(S^{\prime\prime}+\left(S^{\prime}\right)^{2}\right)+\frac{S^{\prime}}{x^{2}}+\frac{1}{x^{2}}=0


This time there is balance between S^{\prime\prime}+\left(S^{\prime}\right)^{2}+x^{-2}, giving S\sim\frac{1}{2}\left(-1\pm i\sqrt{3}\right)\ln x. So:

y\sim x^{-\left(1\pm i\sqrt{3}\right)/2}


For x\rightarrow\infty the equation is not singluar, so, writing $y=\sum_{n}a_{n}x^{-n-\alpha}</math>:

\sum_{n}a_{n}\left(n+\alpha\right)\left(n+\alpha+1\right)x^{-n-2-\alpha}-\sum_{n}a_{n}\left(n+\alpha\right)x^{-n-3-\alpha}+\sum_{n}a_{n}x^{-n-2-\alpha}=0


Shifting:

a_{n+1}\left(n+1+\alpha\right)\left(n+2+\alpha\right)-a_{n}\left(n+\alpha\right)+a_{n+1}=0


For n = 0, we want to find α s. t. the coefficient for an + 1 is zero:

\left(1+\alpha\right)\left(2+\alpha\right)+1=0


Or:

3 + 3α + α2 = 0


Which has solution:

\alpha=\frac{-3\pm\sqrt{9-12}}{2}=-\frac{3\pm i\sqrt{3}}{2}


So we must have a0 = 0, but a1 is free. That term gives the leading asymptotic form for two solutions:

y=x^{-\left(1\pm i\sqrt{3}\right)/2}


We know our solutions are real, so we can combine these solutions to be:

y=x^{-1/2}\sin\left(\sqrt{3}\ln x/2\right);\quad x^{-1/2}\cos\left(\sqrt{3}\ln x/2\right)
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