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Area Of A Sector Derivation

Intersection of a sphere and cone emanating from its center

A spherical sector (blueish)

In geometry, a spherical sector,[1] too known as a spherical cone,[ii] is a portion of a sphere or of a brawl defined by a conical purlieus with apex at the center of the sphere. It can be described as the union of a spherical cap and the cone formed by the center of the sphere and the base of operations of the cap. It is the 3-dimensional analogue of the sector of a circumvolve.

Volume [edit]

If the radius of the sphere is denoted by r and the superlative of the cap by h, the volume of the spherical sector is

V = ii π r 2 h 3 . {\displaystyle V={\frac {2\pi r^{ii}h}{3}}\,.}

This may also be written as

V = 2 π r 3 three ( 1 cos φ ) , {\displaystyle V={\frac {2\pi r^{3}}{iii}}(1-\cos \varphi )\,,}

where φ is one-half the cone bending, i.e., φ is the angle between the rim of the cap and the direction to the middle of the cap as seen from the sphere center.

The volume V of the sector is related to the area A of the cap by:

V = r A three . {\displaystyle 5={\frac {rA}{3}}\,.}

Area [edit]

The curved surface area of the spherical sector (on the surface of the sphere, excluding the cone surface) is

A = 2 π r h . {\displaystyle A=2\pi rh\,.}

Information technology is besides

A = Ω r ii {\displaystyle A=\Omega r^{two}}

where Ω is the solid angle of the spherical sector in steradians, the SI unit of solid bending. One steradian is defined equally the solid bending subtended past a cap area of A = r 2.

Derivation [edit]

The volume can exist calculated by integrating the differential volume chemical element

d V = ρ ii sin ϕ d ρ d ϕ d θ {\displaystyle dV=\rho ^{2}\sin \phi d\rho d\phi d\theta }

over the volume of the spherical sector,

V = 0 two π 0 φ 0 r ρ 2 sin ϕ d ρ d ϕ d θ = 0 2 π d θ 0 φ sin ϕ d ϕ 0 r ρ 2 d ρ = two π r 3 3 ( i cos φ ) , {\displaystyle V=\int _{0}^{2\pi }\int _{0}^{\varphi }\int _{0}^{r}\rho ^{ii}\sin \phi \,d\rho d\phi d\theta =\int _{0}^{2\pi }d\theta \int _{0}^{\varphi }\sin \phi d\phi \int _{0}^{r}\rho ^{2}d\rho ={\frac {two\pi r^{three}}{3}}(1-\cos \varphi )\,,}

where the integrals have been separated, because the integrand can be separated into a production of functions each with one dummy variable.

The area can be similarly calculated by integrating the differential spherical area element

d A = r 2 sin ϕ d ϕ d θ {\displaystyle dA=r^{ii}\sin \phi d\phi d\theta }

over the spherical sector, giving

A = 0 two π 0 φ r 2 sin ϕ d ϕ d θ = r 2 0 2 π d θ 0 φ sin ϕ d ϕ = two π r 2 ( ane cos φ ) , {\displaystyle A=\int _{0}^{two\pi }\int _{0}^{\varphi }r^{2}\sin \phi d\phi d\theta =r^{2}\int _{0}^{2\pi }d\theta \int _{0}^{\varphi }\sin \phi d\phi =two\pi r^{two}(one-\cos \varphi )\,,}

where φ is inclination (or summit) and θ is azimuth (right). Find r is a constant. Again, the integrals tin can be separated.

Run into likewise [edit]

  • Circular sector — the analogous 2D figure.
  • Spherical cap
  • Spherical segment
  • Spherical wedge

References [edit]

  1. ^ Weisstein, Eric Due west. "Spherical sector". MathWorld.
  2. ^ Weisstein, Eric W. "Spherical cone". MathWorld.

Area Of A Sector Derivation,

Source: https://en.wikipedia.org/wiki/Spherical_sector

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