Consider a circle with radius $R$ centered in the origin of plane $xy$. Then, consider all the inscribed circles with radius $x$ (or $y$). The length of each of the inner circles is $2\pi x$.
If I want to calculate the area of the external circle, then I can "sum" all the lengths of the inner circles as follows:
$$A = \int_{0}^R 2\pi x dx = \pi R^2.$$
In my opinion, this is a rather intuitive way to explain how integral works when we have a radial symmetry.
Another approach is the following. Cut vertically the circle and sum up twice all the lengths of the segments you obtain in this process (the segments are parallel to axis $y$ and intersect the circle in two points). Each segment has length equal to $2\sqrt{R^2-x^2}$. Then, the area is:
$$A = 2\int_0^R 2\sqrt{R^2-x^2} dx = \pi R^2.$$
Similarly, consider a sphere of radius $R$ centered in the origin of the space $xyz$. I can also consider all the inscribed spheres with radius $x$ (or $y$ or $z$), which surfaces are equal to $4\pi x^2.$
The volume of the outer sphere is given by the sum of all the surfaces of internal spheres, namely:
$$V = \int_{0}^R 4\pi x^2 dx = \frac{4}{3}\pi R^3.$$
I can find the same results by summing up twice all the areas of all the slices I can obtain from the sphere cutting along all the planes which are parallel to $yz$. In this case, the radii of the slices are equal to $\sqrt{R^2-x^2}$, and their areas are equal to $\pi (R^2-x^2)$. Then:
$$V = 2 \int_0^R \pi(R^2-x^2)dx = \frac{4}{3}\pi R^3.$$
Anyway, when I want to use a similar approach in order to find the surface of sphere, I fail. Here the intuition says me that I must sum up twice all the length of all the slices as before. These lengths are equal to $2\pi \sqrt{R^2-x^2}$, and the integral to solve is:
$$S = 2\int_0^R 2\pi \sqrt{R^2-x^2} dx = \pi^2 R^2 \neq 4 \pi R^2.$$
Why does my intuition fail here?
