emol1414
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Homework Statement
Let
r_{\pm} = \sqrt{r^2 \mp rdcos\theta + (d/2)^2}
in my book it is said that for a approximation where d << r (we don't want d=0 cause the purpose is to find the potential, and with d=0 there would be no potential) so he does a expansion carried to first order in d. Then its given the following result
r_{\pm} \approx r(1 \mp \frac{d}{2r}cos\theta)
and it follows that
\frac{1}{r_{\pm}} \approx \frac{1}{r}(1 \pm \frac{d}{2r}cos\theta)
2. The attempt at a solution
So... he doesn't mention it, but I guess it is a Taylor expansion, right?
Rewriting the equation... r_{\pm} \approx r\sqrt{1 \mp \frac{dcos\theta}{r} + {\frac{d}{2r}}^2}.
But I'm getting a bit confused about it... i can't figure out how exactly he comes up with that. Cause to me... the expansion, based on the equation given bellow for Taylor Series, would go like... r_{\pm} \approx r\left\{\sqrt{1 \mp \frac{d'cos\theta}{r} + {\frac{d'}{2r}}^2} + \frac{1}{2}*\frac{cos\theta/r + d'/2r^2}{\sqrt{1 \mp \frac{d'cos\theta}{r} + {\frac{d'}{2r}}^2}}\right\}...
It seems so simple, but I can't get what I'm missing. =/ Anyone could please help?
3. Relevant equations
Taylor series
f(a) + \frac{f'(a)}{1!} (x - a) + \frac{f''(a)}{2!}(x - a)^2 + ...