I am trying to obtain an approximate expression for the behaviour of the following function for large $x$
$$F(x)=x\frac{ \text{erf}(x)^2}{\text{erf}(2 x)}$$
I know that the $\lim_{x\rightarrow\infty}\frac{1}{x}F(x)=1$ and $\lim_{x\rightarrow\infty}F(x)-x=0$ so that basically one can say that for large $x$, $F(x)\approx x$.
I would like to obtain this result from Series
, but invoking Series[F, {x,∞,1}]
I obtain
$$\frac{e^{2 x^2} \left(e^{2 x^2} \left(x+O\left(\left(\frac{1}{x}\right)^2\right)\right)+e^{x^2} \left(-\frac{2}{\sqrt{\pi }}+O\left(\left(\frac{1}{x}\right)^1\right)\right)+\left(\frac{1}{\pi x}+O\left(\left(\frac{1}{x}\right)^2\right)\right)\right)}{\left(-\frac{1}{2 \sqrt{\pi } x}+O\left(\left(\frac{1}{x}\right)^2\right)\right)+e^{4 x^2}}$$
Why do I get a fraction? How can I get an expansion at infinity which reflects the linear behaviour of the function plus higher order corrections?
F
doesn't yield the "obvious" answer. TheSeries
expansion is only valid "near"x0 = Infinity
, ie, for largex
. Your result (and expansions to any order) gives a singularity betweenx = 0
andx = 1
. Doing the expansion aroundx0 = 0
would give you sensible behaviour for smallx
, but wouldn't mean much for larger values, and vice-versa for expansion aroundx0 = Infinity
. $\endgroup$