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Angular frequency

From Wikipedia, the free encyclopedia
(Redirected fromAngular speed)
Rate of change of angle
Angular frequency
Angular speedω is greater than rotational frequencyν by a factor of 2π.
Other names
angular speed, angular rate
Common symbols
ω
SI unitradian per second (rad/s)
Other units
degrees per second (°/s)
InSI base unitss−1
Derivations from
other quantities
ω = 2πrad⋅ν,ω = dθ/dt
DimensionT1{\displaystyle {\mathsf {T}}^{-1}}
A sphere rotating around an axis. Points farther from the axis move faster, satisfyingω =v /r.

Inphysics,angular frequency (symbolω), also calledangular speed andangular rate, is ascalar measure of theanglerate (the angle per unit time) or thetemporal rate of change of thephaseargument of asinusoidal waveform orsine function (for example, in oscillations and waves).Angular frequency (or angular speed) is the magnitude of thepseudovector quantityangular velocity.[1]

Angular frequency can be obtained by multiplyingrotational frequency,ν (or ordinaryfrequency,f) by a fullturn (2πradians):ω = 2π rad⋅ν.It can also be formulated asω = dθ/dt, theinstantaneous rate of change of theangular displacement,θ, with respect to time, t.[2][3]

Unit

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InSIunits, angular frequency is normally presented in the unitradian persecond. The unithertz (Hz) is dimensionally equivalent, but by convention it is only used for frequency f, never for angular frequency ω. This convention is used to help avoid the confusion[4] that arises when dealing with quantities such as frequency and angular quantities because the units of measure (such as cycle or radian) are considered to be one and hence may be omitted when expressing quantities in terms of SI units.[5][6]

Indigital signal processing, the frequency may be normalized by thesampling rate, yielding thenormalized frequency.

Examples

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Circular motion

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Main article:Circular motion

In a rotating or orbiting object, there is a relation between distance from the axis,r{\displaystyle r},tangential speed,v{\displaystyle v}, and the angular frequency of the rotation. During one period,T{\displaystyle T}, a body in circular motion travels a distancevT{\displaystyle vT}. This distance is also equal to the circumference of the path traced out by the body,2πr{\displaystyle 2\pi r}. Setting these two quantities equal, and recalling the link between period and angular frequency we obtain:ω=v/r.{\displaystyle \omega =v/r.} Circular motion on the unit circle is given byω=2πT=2πf,{\displaystyle \omega ={\frac {2\pi }{T}}={2\pi f},}where:

Oscillations of a spring

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Part of a series on
Classical mechanics
F=dpdt{\displaystyle {\textbf {F}}={\frac {d\mathbf {p} }{dt}}}

An object attached to a spring canoscillate. If the spring is assumed to be ideal and massless with no damping, then the motion issimple and harmonic with an angular frequency given by[7]ω=km,{\displaystyle \omega ={\sqrt {\frac {k}{m}}},}where

ω is referred to as the natural angular frequency (sometimes be denoted asω0).

As the object oscillates, its acceleration can be calculated bya=ω2x,{\displaystyle a=-\omega ^{2}x,}wherex is displacement from an equilibrium position.

Using standard frequencyf, this equation would bea=(2πf)2x.{\displaystyle a=-(2\pi f)^{2}x.}

LC circuits

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The resonant angular frequency in a seriesLC circuit equals the square root of thereciprocal of the product of thecapacitance (C, with SI unitfarad) and theinductance of the circuit (L, with SI unithenry):[8]ω=1LC.{\displaystyle \omega ={\sqrt {\frac {1}{LC}}}.}

Adding series resistance (for example, due to the resistance of the wire in a coil) does not change the resonant frequency of the series LC circuit. For a parallel tuned circuit, the above equation is often a useful approximation, but the resonant frequency does depend on the losses of parallel elements.

Terminology

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Although angular frequency is often loosely referred to as frequency, it differs from frequency by a factor of 2π, which potentially leads confusion when the distinction is not made clear.

See also

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References and notes

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  1. ^Cummings, Karen; Halliday, David (2007).Understanding physics. New Delhi: John Wiley & Sons, authorized reprint to Wiley – India. pp. 449, 484, 485, 487.ISBN 978-81-265-0882-2.(UP1)
  2. ^"ISO 80000-3:2019 Quantities and units — Part 3: Space and time" (2 ed.).International Organization for Standardization. 2019. Retrieved2019-10-23.[1] (11 pages)
  3. ^Holzner, Steven (2006).Physics for Dummies. Hoboken, New Jersey: Wiley Publishing. pp. 201.ISBN 978-0-7645-5433-9.angular frequency.
  4. ^Lerner, Lawrence S. (1996-01-01).Physics for scientists and engineers. Jones & Bartlett Learning. p. 145.ISBN 978-0-86720-479-7.
  5. ^Mohr, J. C.; Phillips, W. D. (2015). "Dimensionless Units in the SI".Metrologia.52 (1):40–47.arXiv:1409.2794.Bibcode:2015Metro..52...40M.doi:10.1088/0026-1394/52/1/40.S2CID 3328342.
  6. ^"SI units need reform to avoid confusion". Editorial.Nature.548 (7666): 135. 7 August 2011.doi:10.1038/548135b.PMID 28796224.
  7. ^Serway, Raymond A.; Jewett, John W. (2006).Principles of physics (4th ed.). Belmont, CA: Brooks / Cole – Thomson Learning. pp. 375, 376, 385, 397.ISBN 978-0-534-46479-0.
  8. ^Nahvi, Mahmood; Edminister, Joseph (2003).Schaum's outline of theory and problems of electric circuits. McGraw-Hill Companies (McGraw-Hill Professional). pp. 214, 216.ISBN 0-07-139307-2. (LC1)

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