Behavior of differential equation as argument goes to zero I'm trying to solve a coupled set of ODEs, but before attempting the full numerical solution, I would like to get an idea of what the solution looks like around the origin. 
The equation at hand is:
$$ y''_l - (f'+g')y'_l  + \biggr[ \frac{2-l^2-l}{x^2}e^{2f}  - \frac{2}{x}(f'+g') - \frac{2}{x^2} \biggr]y_l = \frac{4}{x}(f'+g')z_l$$
$y,f,g,z$ are all functions of $x$, which has the domain ($0, X_0$). If I specifically take the $l=2$ case I of course have 
$$ y''_2 - (f'+g')y'_2  + \biggr[ \frac{-4}{x^2}e^{2f}  - \frac{2}{x}(f'+g') - \frac{2}{x^2} \biggr]y_2 = \frac{4}{x}(f'+g')z_2$$
To avoid issues with singularities, I multiply both sides of the equation by $x^2$, to get, lets call it EQ1.
$$ x^2 y''_2 - x^2(f'+g')y'_2  + \biggr[ -4e^{2f}  - x(f'+g') - 2 \biggr]y_2 = 4 x(f'+g')z_2$$
Now if by some magic I know by that as $x \rightarrow 0$, $y_l = x^{l+1}$ so that $y_2 = x^3$. How would I determine what the functions $z_2$ is around the origin? 
Actually I already know the answer: $z_2$ should also go as $x^3$, but I have not been able to show it. 
Any help is much appreciated. 
My attempt at a solution: 
 I have tried to keep things general so I expand $f[x] = 1 + f_1 x + f_2 x^2 +f_3 x^3$, and similarly $g[x] = 1 + g_1 x + g_2 x^2 +g_3 x^3$ where $f_1,f_2,f_3, g_1,g_2,g_3$ are constants. I have kept up to third order because I want to substitute $y_2 = x^3$, so I figured I should take the other functions to that order as well. 
As for the $e^{2f}$ term, I use a truncated Taylor series for the exponential, $1+\frac{x^2}{2!} + \frac{x^3}{3!}$, into which I substitue my expansion of $f[x]$. After expanding everything out and eliminating terms of higher order than $x^3$ from the right hand side of EQ1, I get something like $constant*x^3$, while the left hand side is third order polynomial times $z_2$. 
I really just don't know how to proceed. Should I have left higher order terms in the RHS, so that I could divide by a third order polynomial and still end up with $z_2 \propto x^3$. I don't know how this would work because on the RHS I had terms has high as $x^{12}$. 

My solution is as follows. I essentially tried to reproduce 5PM's work in Maple with some mathematica code. 
First I create the generic expansions of the functions $f$ and $g$ using
f = Sum{ff[k]*x^k, {k,0,5}]
g = Sum{gf[k]*x^k, {k,0,5}]

I had to create the variables "ff", and "gg" so as to avoid recursions limit errors in mathematica. Then I substituted these expansions into equation 1 above and then then divided the right hand side so get $z_2$ by itself. Then I used
Series[z2[r], {r,0,5}]

For which I got the following output. (I have cleaned it up a bit, having only kept terms of order three, and replacing the "ff" and "gg" with just "f" and "g".)
$
z_2= -\frac {(e^{2 f_0} - 1 ) x^2} {f_1 + g_1} + \frac {1} {4} x^3  \biggr \{ \frac {2 (4e^{2 f_0} - 4)(f_2 + g_2))} {(f_1 + g_1)^2} - \frac {8 e^{2 f_0} f_1 + 5 f_1 + 5 g_1} {f_1 + g_1}\biggr \}$ 
I esentially get the same result as 5PM. From this analysis it seems that $z_2$ goes as $x^2$. 
The reason this disagrees with the paper I was reading, is that I forgot that physically speaking $f_0$ is very close to zero, and so the x^2 term does go to zero, and so the physical answer is 
$
z_2=  \frac {1} {4} x^3  \biggr \{\frac {8 e^{2 f_0} f_1 + 5 f_1 + 5 g_1} {f_1 + g_1}\biggr \}$ . 
