Napkin ring problem

Napkin ring problem
If a hole of height h is drilled straight through the center of a sphere, the volume of the remaining band does not depend on the size of the sphere. For a larger sphere, the band will be thinner but longer.

In geometry, it is somewhat surprising that the volume of a band of specified height around a sphere—the part that remains after a hole in the shape of a circular cylinder is drilled through the sphere—does not depend on the sphere's radius.

Specifically, suppose the axis of a right circular cylinder passes through the center of the sphere and the height (defined as distance in a direction parallel to the axis) of the part of the boundary of the cylinder that is inside the sphere is h, and the radius of the sphere is R. The "band" is the part of the sphere that is outside the cylinder.

The result is that the volume of the band depends on h but not on R.

As the radius R of the sphere shrinks, the diameter of the cylinder must also shrink in order that h can remain the same. The band gets thicker, and that would increase its volume. But it also gets shorter in circumference, and that would decrease its volume. The two effects exactly cancel each other out. The most extreme case, involving the smallest possible sphere, is that in which the diameter of the sphere is the same as the height h. In that case the volume of the band is the volume of the whole sphere:

 \frac{\pi h^3}{6}.

An early study of this problem was written by 17th-century Japanese mathematician Seki Kōwa. According to Smith & Mikami (1914), Seki called this solid an arc-ring, or in Japanese kokan or kokwan.

"Napkin Ring Problem" is called so because after removing cylinder from sphere the remaining band resembles shape of napkin ring.

Proof

Suppose the radius of the sphere is R, the radius of the cylinder (or drill-bit) is y, and length of the cylinder (or the tunnel) is h.

By the Pythagorean theorem, the radius of the cylinder is

Finding the measurements of the ring that is the horizontal cross-section.
 \sqrt{R^2 - \left(\frac{h}{2}\right)^2},\qquad\qquad(1)

and the radius of the horizontal cross-section of the sphere at height y above the "equator" is

 \sqrt{R^2 - y^2}.\qquad\qquad(2) \,

The cross-section of the band with the plane at height y is the region inside the larger circle of radius given by (2) and outside the smaller circle of radius given by (1). The cross-section's area is therefore the area of the larger circle minus the area of the smaller circle:


\begin{align}
& {}\quad \pi(\text{larger radius})^2 - \pi(\text{smaller radius})^2 \\
& = \pi\left(\sqrt{R^2 - y^2}\right)^2 - \pi\left(\sqrt{R^2 - \left(\frac{h}{2}\right)^2\,{}}\,\right)^2 = \pi\left(\left(\frac{h}{2}\right)^2 - y^2\right).
\end{align}

The radius R does not appear in the last quantity. Therefore the area of the horizontal cross-section at height y does not depend on R. The volume of the band is

 \int_{-h/2}^{h/2} (\text{area of cross-section at height }y) \, dy,

and that does not depend on R.

This is an application of Cavalieri's principle: volumes with equal-sized corresponding cross-sections are equal. Indeed, the area of the cross-section is the same as that of the corresponding cross-section of a sphere of radius h/2, which has volume

\frac{4}{3}\pi\left(\frac{h}{2}\right)^3 = \frac{\pi h^3}{6}.

References

External links


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