This is a problem from Engineering Mathematics book by K. A. Stroud, 7th edition, Exercise 18, Chapter 12 Further problems. It has been given in a physics manner, but it just requires manipulation of Taylor series to get the result, which is what I can’t figure out. It doesn’t require any physics knowledge really to find the answer, that’s why I posted it on M.S.E. It states:
The field strength of a magnet $(H)$ at a point on the axis, distance $x$ from its center, is given by: $$H=\frac{M}{2l}\left(\frac{1}{(x-l)^2}-\frac{1}{(x+l)^2}\right),$$ where $2l =$ length of magnet and $M =$ moment. Show that if $l$ is very small compared with $x$, then $ H \approx \frac{2M}{x^3} $.
As far as I’m concerned, $H$ is a fraction of $x$ there (but I’m not sure, maybe it’s $H(x,l)$?), so this is $H(x)$. And so i have to find the Taylor series representation of $H(x+l)$. What I get is this: $$H(x+l) = \frac{M}{2l}\left(\frac{1}{(x-l)^2}-\frac{1}{(x+l)^2}\right) + M\left(\frac{1}{(x+l)^3}-\frac{1}{(x-l)^3}\right) + \frac{3Ml}{2}\left(\frac{1}{(x-l)^4}-\frac{1}{(x+l)^4}\right)$$ (since it says $l$ is small, I took only terms until the $x^2$ only).
I really don’t know how to prove what is needed in this. I would be very grateful for any help. Thanks in advance!
There is no need to use Taylor series, just algebra and limits: $$H=\frac{M}{2l}\left(\frac{1}{(x-l)^2}-\frac{1}{(x+l)^2} \right) =\frac{M}{2l}\frac{(x+l)^2-(x-l)^2}{(x^2-l^2)^2} =\frac{M}{2l}\frac{4xl}{x^4(1-(l/x)^2)^2} \approx \frac{2M}{x^3} $$