Let
a=h/2 and place the hole axis along
z. At the rim,
r02=R2−a2.
A horizontal slice at
∣z∣≤a is an annulus of
area π[(R2−z2)−r02]=π(a2−z2). Thus the
napkin ring problem gives
V=π∫−aa(a2−z2)dz=34πa3=6πh3.
Each slice depends only on
a and
z, explaining the independence from the original
sphere radius, rather than obtaining it merely by cancellation after integration.