In Purcell's, Electricity and Magnetism, 61, is stated that the following limit : $$\lim_{V_{i} \to 0}\frac{\int_{S_{i}} \overrightarrow{F}.\overrightarrow{ds}}{V_{i}}$$
[ Where $\overrightarrow{F}$ is a vector field, $S_{i}$ a small closed surface containing the point $i$ and $V_{i}$ the volume inside $S_{i}\,$] , which is the definition of $\,\mathrm{div}F\,$, is independent of the shape of $S_{i}$. Why is it this true? Why do these two shapes:
have the same limit defined above?
P.S. the second shape is essentially the first one completed
