Spherical cap

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The spherical cap is the purple section.

In geometry, a spherical cap is a portion of a sphere cut off by a plane. If the plane passes through the center of the sphere, so that the height of the cap is equal to the radius of the sphere, the spherical cap is called a hemisphere.

If the radius of the sphere is r, the radius of the base of the cap is a, and the height of the cap is h, then the volume of the spherical cap is

V = \frac{\pi h}{6} (3a^2 + h^2),

and the curved surface area of the spherical cap is

A = 2 \pi r h.

The parameters a, h and r are not independent:

r^2 = (r-h)^2 + a^2 = r^2 +h^2 -2rh +a^2,
r = \frac {a^2 + h^2}{2h}.

Substituting this into the area formula gives:

A = 2 \pi \frac{(a^2 + h^2)}{2h} h = \pi (a^2 + h^2).

Note also that in the upper hemisphere of the diagram, \scriptstyle h = r - \sqrt{r^2 - a^2}, and in the lower hemisphere \scriptstyle h = r + \sqrt{r^2 - a^2}; hence in either hemisphere \scriptstyle a = \sqrt{h(2r-h)} and so an alternative expression for the volume is

V = \frac {\pi h^2}{3} (3r-h).

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[edit] Application

The volume of all points which are in at least one of two intersecting spheres of radii r1 and r2 is [1]

 V = V^{(1)}-V^{(2)},

where

V^{(1)} = \frac{4\pi}{3}r_1^3 +\frac{4\pi}{3}r_2^3

is the total of the two isolated spheres, and

V^{(2)} = \frac{\pi h_1^2}{3}(3r_1-h_1)+\frac{\pi h_2^2}{3}(3r_2-h_2)

the sum of the two spherical caps of the intersection. If d <r1+r2 is the distance between the two sphere centers, elimination of the variables h1 and h2 leads to[2] [3]

V^{(2)} = \frac{\pi}{12d}(r_1+r_2-d)^2[d^2+2d(r_1+r_2)-3(r_1-r_2)^2].

[edit] Hyperspherical cap

Generally, the n-dimensional volume of a hyperspherical cap of height h and radius r in n-dimensional Euclidean space is given by

V = \frac{\pi ^ {\frac{n-1}{2}}\, r^{n}}{\,\Gamma \left ( \frac{n+1}{2} \right )} \int\limits_{0}^{\cos^{-1}\left(\frac{r-h}{r}\right)}\sin^n (t) \,\mathrm{d}t

where \Gamma (the gamma function) is given by  \Gamma(z) = \int_0^\infty  t^{z-1} \mathrm{e}^{-t}\,\mathrm{d}t .

The formula for V can be expressed in terms of the volume of the unit n-ball C_{n}={\scriptstyle \pi^{n/2}/\Gamma[1+\frac{n}{2}]} and the hypergeometric function {}_{2}F_{1} or the regularized incomplete beta function I_x(a,b)as

V = C_{n} \, r^{n} \left( \frac{1}{2}\, - \,\frac{r-h}{r}  \,\frac{\Gamma[1+\frac{n}{2}]}{\sqrt{\pi}\,\Gamma[\frac{n+1}{2}]}
{\,\,}_{2}F_{1}\left(\tfrac{1}{2},\tfrac{1-n}{2};\tfrac{3}{2};\left(\tfrac{r-h}{r}\right)^{2}\right)\right)
=\frac{1}{2}C_{n} \, r^n I_{(2rh-h^2)/r^2} \left(\frac{n+1}{2}, \frac{1}{2} \right) ,

and the area formula A can be expressed in terms of the area of the unit n-ball A_{n}={\scriptstyle 2\pi^{n/2}/\Gamma[\frac{n}{2}]} as

A =\frac{1}{2}A_{n} \, r^{n-1} I_{(2rh-h^2)/r^2} \left(\frac{n-1}{2}, \frac{1}{2} \right) ,

where \scriptstyle 0\le h\le r .

[edit] See also

[edit] References

  1. ^ Connolly, Michael L. (1985). "Computation of molecular volume". J. Am. Chem. Soc: 1118-1124. doi:10.1021/ja00291a006. 
  2. ^ Pavani, R.; Ranghino, G. (1982). "A method to compute the volume of a molecule". Comput. Chem.. doi:10.1016/0097-8485(82)80006-5. 
  3. ^ Bondi, A. (1964). "van der Waals volumes and radii". J. Phys. Chem. (68): 441-451. doi:10.1021/j100785a001. 
  • Li, S. (2011). "Concise Formulas for the Area and Volume of a Hyperspherical Cap". Asian J. Math. Stat. 4 (1): 66–70. doi:10.3923/ajms.2011.66.70. .

[edit] External links

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