Spherical cap

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An example of a spherical cap in blue (and another in red.)

In geometry, a spherical cap, spherical dome, or spherical segment of one base 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.

Volume and surface area[edit]

The volume of the spherical cap and the area of the curved surface may be calculated using combinations of

  • The radius of the sphere
  • The radius of the base of the cap
  • The height of the cap
  • The polar angle between the rays from the center of the sphere to the apex of the cap (the pole) and the edge of the disk forming the base of the cap
Using and Using and Using and
Volume [1]
Area [1]

If denotes the latitude in geographic coordinates, then .

The relationship between and is irrelevant as long as . For example, the red section of the illustration is also a spherical cap for which .

The formulas using and can be rewritten to use the radius of the base of the cap instead of , using the Pythagorean theorem:

so that

Substituting this into the formulas gives:

Deriving the surface area intuitively from the spherical sector volume[edit]

Note that aside from the calculus based argument below, the area of the spherical cap may be derived from the volume of the spherical sector, by an intuitive argument,[2] as

The intuitive argument is based upon summing the total sector volume from that of infinitesimal triangular pyramids. Utilizing the pyramid (or cone) volume formula of , where is the infinitesimal area of each pyramidal base (located on the surface of the sphere) and is the height of each pyramid from its base to its apex (at the center of the sphere). Since each , in the limit, is constant and equivalent to the radius of the sphere, the sum of the infinitesimal pyramidal bases would equal the area of the spherical sector, and:

Deriving the volume and surface area using calculus[edit]

Rotating the green area creates a spherical cap with height and sphere radius .

The volume and area formulas may be derived by examining the rotation of the function

for , using the formulas the surface of the rotation for the area and the solid of the revolution for the volume. The area is

The derivative of is

and hence

The formula for the area is therefore

The volume is

Applications[edit]

Volumes of union and intersection of two intersecting spheres[edit]

The volume of the union of two intersecting spheres of radii and is [3]

where

is the sum of the volumes of the two isolated spheres, and

the sum of the volumes of the two spherical caps forming their intersection. If is the distance between the two sphere centers, elimination of the variables and leads to[4][5]

Surface area bounded by parallel disks[edit]

The curved surface area of the spherical segment bounded by two parallel disks is the difference of surface areas of their respective spherical caps. For a sphere of radius , and caps with heights and , the area is

or, using geographic coordinates with latitudes and ,[6]

For example, assuming the Earth is a sphere of radius 6371 km, the surface area of the arctic (north of the Arctic Circle, at latitude 66.56° as of August 2016[7]) is 2π·6371²|sin 90° − sin 66.56°| = 21.04 million km², or 0.5·|sin 90° − sin 66.56°| = 4.125% of the total surface area of the Earth.

This formula can also be used to demonstrate that half the surface area of the Earth lies between latitudes 30° South and 30° North in a spherical zone which encompasses all of the Tropics.

Generalizations[edit]

Sections of other solids[edit]

The spheroidal dome is obtained by sectioning off a portion of a spheroid so that the resulting dome is circularly symmetric (having an axis of rotation), and likewise the ellipsoidal dome is derived from the ellipsoid.

Hyperspherical cap[edit]

Generally, the -dimensional volume of a hyperspherical cap of height and radius in -dimensional Euclidean space is given by [8]

where (the gamma function) is given by .

The formula for can be expressed in terms of the volume of the unit n-ball and the hypergeometric function or the regularized incomplete beta function as

,

and the area formula can be expressed in terms of the area of the unit n-ball as

,

where .

Earlier in [9] (1986, USSR Academ. Press) the following formulas were derived: , where ,

.

For odd

.

Asymptotics[edit]

It is shown in [10] that, if and , then where is the integral of the standard normal distribution.

A more quantitative way of writing this, is in [11] where the bound is is given. For large caps (that is when as ), the bound simplifies to .

See also[edit]

References[edit]

  1. ^ a b Polyanin, Andrei D; Manzhirov, Alexander V. (2006), Handbook of Mathematics for Engineers and Scientists, CRC Press, p. 69, ISBN 9781584885023.
  2. ^ Shekhtman, Zor. "Unizor - Geometry3D - Spherical Sectors". YouTube. Zor Shekhtman. Retrieved 31 Dec 2018.
  3. ^ Connolly, Michael L. (1985). "Computation of molecular volume". J. Am. Chem. Soc. 107 (5): 1118–1124. doi:10.1021/ja00291a006.
  4. ^ Pavani, R.; Ranghino, G. (1982). "A method to compute the volume of a molecule". Computers & Chemistry. 6 (3): 133–135. doi:10.1016/0097-8485(82)80006-5.
  5. ^ Bondi, A. (1964). "Van der Waals volumes and radii". J. Phys. Chem. 68 (3): 441–451. doi:10.1021/j100785a001.
  6. ^ Scott E. Donaldson, Stanley G. Siegel (2001). Successful Software Development. ISBN 9780130868268. Retrieved 29 August 2016.
  7. ^ "Obliquity of the Ecliptic (Eps Mean)". Neoprogrammics.com. Retrieved 2014-05-13.
  8. ^ 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.
  9. ^ Chudnov, Alexander M. (1986). "On minimax signal generation and reception algorithms (rus.)". Problems of Information Transmission. 22 (4): 49–54.
  10. ^ Chudnov, Alexander M (1991). "Game-theoretical problems of synthesis of signal generation and reception algorithms (rus.)". Problems of Information Transmission. 27 (3): 57–65.
  11. ^ Anja Becker, Léo Ducas, Nicolas Gama, and Thijs Laarhoven. 2016. New directions in nearest neighbor searching with applications to lattice sieving. In Proceedings of the twenty-seventh annual ACM-SIAM symposium on Discrete algorithms (SODA '16), Robert Kraughgamer (Ed.). Society for Industrial and Applied Mathematics, Philadelphia, PA, USA, 10-24.

Further reading[edit]

  • Richmond, Timothy J. (1984). "Solvent accessible surface area and excluded volume in proteins: Analytical equation for overlapping spheres and implications for the hydrophobic effect". J. Mol. Biol. 178 (1): 63–89. doi:10.1016/0022-2836(84)90231-6. PMID 6548264.
  • Lustig, Rolf (1986). "Geometry of four hard fused spheres in an arbitrary spatial configuration". Mol. Phys. 59 (2): 195–207. Bibcode:1986MolPh..59..195L. doi:10.1080/00268978600102011.
  • Gibson, K. D.; Scheraga, Harold A. (1987). "Volume of the intersection of three spheres of unequal size: a simplified formula". J. Phys. Chem. 91 (15): 4121–4122. doi:10.1021/j100299a035.
  • Gibson, K. D.; Scheraga, Harold A. (1987). "Exact calculation of the volume and surface area of fused hard-sphere molecules with unequal atomic radii". Mol. Phys. 62 (5): 1247–1265. Bibcode:1987MolPh..62.1247G. doi:10.1080/00268978700102951.
  • Petitjean, Michel (1994). "On the analytical calculation of van der Waals surfaces and volumes: some numerical aspects". Int. J. Quantum Chem. 15 (5): 507–523. doi:10.1002/jcc.540150504.
  • Grant, J. A.; Pickup, B. T. (1995). "A Gaussian description of molecular shape". J. Phys. Chem. 99 (11): 3503–3510. doi:10.1021/j100011a016.
  • Busa, Jan; Dzurina, Jozef; Hayryan, Edik; Hayryan, Shura (2005). "ARVO: A fortran package for computing the solvent accessible surface area and the excluded volume of overlapping spheres via analytic equations". Comput. Phys. Commun. 165 (1): 59–96. Bibcode:2005CoPhC.165...59B. doi:10.1016/j.cpc.2004.08.002.

External links[edit]