In physics there is a formula calculate the variation in the acceleration due to gravity at a height, it is given by:
$$g=g_0\left(1+\frac{h}{R}\right)^{-2}$$
But it is approximated as $$g=g_0\left(1-\frac{2h}{R}\right)$$
Some how the terms in the brackets are almost equal could anyone show why ?

For small $\frac hR$, ignore the terms of $(\frac hR)^2$ below
$$\left(1+\frac{h}{R}\right)^{-2} = \frac1{1+\frac{2h}{R}+( \frac{h}{R})^2} \approx \frac1{1+\frac{2h}{R}} = \frac{1-\frac{2h}{R}}{1-(\frac{2h}{R})^2} \approx 1-\frac{2h}{R} $$