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Steradian

From Wikipedia, the free encyclopedia
(Redirected fromSteradians)
SI derived unit of solid angle
steradian
A graphical representation of two different steradians.
The sphere has radiusr, and in this case the areaA of the highlightedspherical cap isr2. The solid angleΩ equals[A/r2] sr which is1 sr in this example. The entire sphere has a solid angle of4π sr.
General information
Unit systemSI
Unit ofsolid angle
Symbolsr
Conversions
1 srin ...... is equal to ...
   SI base units   1 m2/m2
   square degrees   1802/π2 deg2
3282.8 deg2

Thesteradian (symbol:sr) orsquare radian[1][2] is the unit ofsolid angle in theInternational System of Units (SI). It is used inthree dimensional geometry, and is analogous to theradian, which quantifiesplanar angles. A solid angle in the form of aright circular cone can be projected onto a sphere, defining aspherical cap where the cone intersects the sphere. The magnitude of the solid angle expressed in steradians is defined as the quotient of the surface area of the spherical cap and the square of the sphere's radius. This is analogous to the way a plane angle projected onto a circle defines acircular arc on the circumference, whose length is proportional to the angle. Steradians can be used to measure a solid angle of any shape. The solid angle subtended is the same as that of a cone with the same projected area. A solid angle of one steradian subtends acone aperture of approximately 1.144 radians or 65.54 degrees.

In the SI, solid angle is considered to be adimensionless quantity, the ratio of the area projected onto a surrounding sphere and the square of the sphere's radius. This is the number of square radians in the solid angle. This means that the SI steradian is the number of square radians in a solid angle equal to one square radian, which of course is the number one. It is useful to distinguish between dimensionless quantities of a differentkind, such as the radian (in the SI, a ratio of quantities of dimension length), so the symbol sr is used. For example,radiant intensity can be measured in watts per steradian (W⋅sr−1). The steradian was formerly anSI supplementary unit, but this category was abolished in 1995 and the steradian is now considered anSI derived unit.

The namesteradian is derived from theGreekστερεόςstereos 'solid' + radian.

Solid angle of countries and other entities relative to the centre of Earth.

Definition

[edit]

A steradian can be defined as the solid anglesubtended at the centre of aunit sphere by a unitarea (of any shape) on its surface. For a general sphere ofradiusr, any portion of its surface with areaA =r2 subtends one steradian at its centre.[3]

A solid angle in the form of a circular cone is related to the area it cuts out of a sphere:

Ω=Ar2 sr=2πhr sr,{\displaystyle \Omega ={\frac {A}{r^{2}}}\ {\text{sr}}\,={\frac {2\pi h}{r}}\ {\text{sr}},}

where

Because the surface areaA of a sphere is4πr2, the definition implies that a sphere subtends4π steradians (≈ 12.56637 sr) at its centre, or that a steradian subtends1/4π ≈ 0.07958 of a sphere. By the same argument, the maximum solid angle that can be subtended at any point is4π sr.

Other properties

[edit]
Section of cone (1) and spherical cap (2) that subtend a solid angle of one steradian inside a sphere

The area of aspherical cap isA = 2πrh, whereh is the "height" of the cap. IfA =r2, thenhr=12π{\displaystyle {\tfrac {h}{r}}={\tfrac {1}{2\pi }}}. From this, one can compute thecone aperture (a plane angle)2θ of the cross-section of a simplespherical cone whose solid angle equals one steradian:

θ=arccos(rhr)=arccos(1hr)=arccos(112π),{\displaystyle \theta =\arccos \left({\frac {r-h}{r}}\right)=\arccos \left(1-{\frac {h}{r}}\right)=\arccos \left(1-{\frac {1}{2\pi }}\right),}

givingθ 0.572 rad = 32.77° and aperture2θ 1.144 rad = 65.54°.

The solid angle of a spherical cone whose cross-section subtends the angle2θ is:

Ω=2π(1cosθ) sr=4πsin2(θ2) sr.{\displaystyle \Omega =2\pi (1-\cos \theta ){\text{ sr}}=4\pi \sin ^{2}\left({\frac {\theta }{2}}\right){\text{ sr}}.}

A steradian is also equal to14π{\displaystyle {\tfrac {1}{4\pi }}} of a completesphere (spat), to(3602π)2{\displaystyle \left({\tfrac {360^{\circ }}{2\pi }}\right)^{2}} 3282.80635 square degrees, and to the spherical area of apolygon having anangle excess of 1 radian.[clarification needed]

SI multiples

[edit]

Millisteradians (msr) and microsteradians (μsr) are occasionally used to describelight andparticle beams.[4][5] Other multiples are rarely used.

See also

[edit]

References

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  1. ^Stutzman, Warren L; Thiele, Gary A (2012-05-22).Antenna Theory and Design. John Wiley & Sons.ISBN 978-0-470-57664-9.
  2. ^Woolard, Edgar (2012-12-02).Spherical Astronomy. Elsevier.ISBN 978-0-323-14912-9.
  3. ^"Steradian",McGraw-Hill Dictionary of Scientific and Technical Terms, fifth edition, Sybil P. Parker, editor in chief. McGraw-Hill, 1997.ISBN 0-07-052433-5.
  4. ^Stephen M. Shafroth, James Christopher Austin,Accelerator-based Atomic Physics: Techniques and Applications, 1997,ISBN 1563964848, p. 333
  5. ^R. Bracewell, Govind Swarup, "The Stanford microwave spectroheliograph antenna, a microsteradian pencil beam interferometer"IRE Transactions on Antennas and Propagation9:1:22-30 (1961)

External links

[edit]
Look upsteradian in Wiktionary, the free dictionary.
  • Media related toSteradian at Wikimedia Commons
Base units
Derived units
with special names
Other accepted units
See also
Linear/translational quantitiesAngular/rotational quantities
Dimensions1LL2Dimensions1θθ2
Ttime:t
s
absement:A
m s
Ttime:t
s
1distance:d,position:r,s,x,displacement
m
area:A
m2
1angle:θ,angular displacement:θ
rad
solid angle:Ω
rad2, sr
T−1frequency:f
s−1,Hz
speed:v,velocity:v
m s−1
kinematic viscosity:ν,
specific angular momentumh
m2 s−1
T−1frequency:f,rotational speed:n,rotational velocity:n
s−1,Hz
angular speed:ω,angular velocity:ω
rad s−1
T−2acceleration:a
m s−2
T−2rotational acceleration
s−2
angular acceleration:α
rad s−2
T−3jerk:j
m s−3
T−3angular jerk:ζ
rad s−3
Mmass:m
kg
weighted position:Mx⟩ = ∑mxmoment of inertiaI
kg m2
ML
MT−1Mass flow rate:m˙{\displaystyle {\dot {m}}}
kg s−1
momentum:p,impulse:J
kg m s−1,N s
action:𝒮,actergy:
kg m2 s−1,J s
MLT−1angular momentum:L,angular impulse:ΔL
kg m rad s−1
MT−2force:F,weight:Fg
kg m s−2,N
energy:E,work:W,Lagrangian:L
kg m2 s−2,J
MLT−2torque:τ,moment:M
kg m rad s−2,N m
MT−3yank:Y
kg m s−3, N s−1
power:P
kg m2 s−3W
MLT−3rotatum:P
kg m rad s−3, N m s−1
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