Example 1
Reference example: one full turn takes 8 s. An angular velocity of 0.785 rad/s is 45° per second.
ω = 0.785 rad/s
Enter the period T, the time of one full turn, in seconds. The calculator divides the full angle 2π by that time with ω = 2π/T and reports angular velocity in radians per second plus frequency, revolutions per minute, degrees per second, and the linear speed of a point 1 m from the axis. For T = 8 s the result is 0.785 rad/s, or 45° per second. The model is uniform rotation; it does not return ω = v/r as the primary result.
Enter the period of one turn. The angular velocity, frequency, revolutions per minute, and the ω(T) chart will appear here.
For linear speed from angular speed, use the v = ω·r calculator; for angular momentum, L = I·ω; and for rotational energy, E = ½Iω².
Angular velocity says what angle a rotating body sweeps out per unit time. If one full turn — an angle of 2π radians — takes time T, then in uniform motion ω = 2π/T. The unit is the radian per second; because the radian is dimensionless, formally it is 1/s. The same quantity is the angular frequency of harmonic oscillations and the basis for describing circular motion in every mechanics course (Halliday, Resnick, Walker; Young, Freedman).
The calculator works with a single number: the period T in seconds. It divides 2π = 6.2832 by it. For T = 8 s you get ω = 0.7854 rad/s. For the second hand of a clock T = 60 s and ω = 0.1047 rad/s, that is 6° per second. For a turntable platter at 33⅓ rpm the period is 1.8 s and the angular velocity 3.49 rad/s. If you know the revolutions per minute n, the period is T = 60/n.
What the result panel shows. Besides ω in rad/s, the calculator reports the frequency f = 1/T in hertz (0.125 Hz in the example), revolutions per minute (7.5 rpm), degrees per second (45°/s), the linear speed of a point 1 m from the axis (v = ω·r, here 0.785 m/s or 2.58 ft/s), the entered period in a convenient unit, and the angular velocity at half the period — twice as large, because ω is inversely proportional to T. The chart draws the hyperbola ω(T) from ½T to 4T.
Limits of the model. The formula describes uniform rotation; for a rotation that speeds up the result is the average angular velocity over one turn, and the instantaneous value is the time derivative of the angle, ω = dθ/dt. The calculator does not compute the linear speed for an arbitrary radius (that is the v = ω·r calculator), the centripetal acceleration, or the angular momentum. Nor does it distinguish the sense of rotation — it reports the magnitude of the vector ω.
The unit switch in the header does not change radians or seconds, because they are shared by both systems; the linear speed in the panel is additionally shown in ft/s. The values in the text stay in SI units as a reference. The period must be greater than zero: a body that does not complete a turn has no angular velocity defined by this formula.
Examples on this page: T = 8 s → 0.785 rad/s; the second hand → 0.105 rad/s; the hour hand (T = 12 h) → 1.45·10⁻⁴ rad/s; the Earth’s sidereal day → 7.29·10⁻⁵ rad/s; a turntable at 33⅓ rpm → 3.49 rad/s; a hard drive at 7,200 rpm → 754 rad/s. The “Fill this example” button enters the same number into the field and refreshes the result panel and the chart.
ω = 2π / T
[ω] = rad / s = 1/s; f = 1/T, ω = 2πf, n = 60/T rpm, 1 rad/s = 57.296 °/s, v = ω·r
Model: angular velocity of uniform circular motion (rotational kinematics; the radian as an angle measure from R. Cotes, 1714, named by J. Thomson, 1873). The rearrangements T = 2π/ω and f = ω/2π follow from the same formula, but this calculator solves only for ω. Order of computation: 2π/T in seconds, then f = 1/T, 60/T, 360/T, and v = ω·1 m.
Angular velocity ω is the rate of change of the rotation angle with time: ω = dθ/dt. In uniform circular motion the angle grows linearly, and a full turn of 2π radians takes the period T, so ω = 2π/T. The unit is the radian per second; the radian is the ratio of arc length to radius, hence dimensionless, and ω formally has the dimension 1/s — the same as frequency, from which it differs by the factor 2π.
Angular velocity is a vector along the axis of rotation, following the right-hand rule; the calculator reports its magnitude. The other quantities of circular motion follow from ω: linear speed v = ω·r, centripetal acceleration a = ω²·r, angular momentum L = I·ω, and rotational kinetic energy E = ½Iω². The same letter denotes the angular frequency of harmonic oscillations, because the projection of circular motion onto a diameter is a harmonic oscillation with the same ω.
The concept of the arc measure of an angle — the ratio of arc length to radius — was introduced by Roger Cotes in 1714, who noticed it is the natural measure for calculus. The name “radian” was proposed by James Thomson, brother of Lord Kelvin, in Belfast in 1873. Leonhard Euler, in works from 1750–1765, described the rotation of a rigid body by an angular velocity vector and showed that every instantaneous motion of a body about a point is a rotation about some axis.
The distinction between angular velocity ω in radians per second and frequency f in hertz settled in the 19th century with the theory of oscillations and alternating currents. In electrical engineering ω = 2πf is called the angular frequency of the supply: 376.99 rad/s for the 60 Hz US grid, 314.16 rad/s for 50 Hz. The SI treats the radian as a derived unit of dimension 1 (resolution of the 8th CGPM in 1960 and the SI Brochure), so rad/s and 1/s are formally equivalent, although for clarity one always writes rad/s.
Step 1. In uniform circular motion the angle θ swept out since the start grows in proportion to time: θ(t) = ω·t. Step 2. After one full turn the angle is 2π radians (360°) and the time one period T. Substituting: 2π = ω·T, hence ω = 2π/T. Step 3. Frequency is the number of turns per second, f = 1/T, so equivalently ω = 2πf; revolutions per minute are n = 60·f = 60/T.
Step 4. For T = 8 s: ω = 6.2832/8 = 0.7854 rad/s, f = 0.125 Hz, n = 7.5 rpm, and in degrees 360°/8 s = 45°/s. Step 5. A point at distance r from the axis covers the circumference 2πr in one period, so its linear speed is v = 2πr/T = ω·r; for r = 1 m it is numerically equal to ω, that is 0.785 m/s. For a carousel seat at a radius of 4 m with the same period, 3.14 m/s.
The formula ω = 2π/T is exact for uniform rotation, in which every equal interval of time corresponds to the same angle. For a rotation that speeds up or slows down — a rotor spinning up, a braking wheel — the result is the average angular velocity over one full turn, and the instantaneous ω(t) must be found from the time derivative of the angle or from a measurement over a short interval.
The calculator also assumes that the period is the time of exactly one turn. When timing with a stopwatch it is better to measure several or several dozen turns and divide by their number, which reduces the reaction-time error. For astronomical objects one must distinguish the sidereal period (relative to the stars) from the synodic one (relative to the Sun): the Earth turns about its axis in 23 h 56 min 4 s, not in 24 h — hence 7.292·10⁻⁵ rad/s rather than 7.272·10⁻⁵ rad/s.
Three measures of the same motion are linked by simple factors: ω [rad/s] = 2π·f [Hz] = 2π·n/60 [rpm] ≈ 0.10472·n. Conversely n = 9.5493·ω. In degrees per second, ω·57.296. An engine at 3,000 rpm has ω = 314 rad/s, a hard drive at 7,200 rpm 754 rad/s, a wind turbine at 12 rpm 1.26 rad/s, the second hand of a clock 0.105 rad/s, that is 6° per second, and the hour hand 0.5° per minute.
Physics and engineering use ω instead of f wherever trigonometric functions and derivatives appear: x(t) = A·cos(ωt), v = ω·r, a = ω²·r, L = I·ω, E = ½Iω². The factor 2π then hides in a single letter and the formulas are simpler. Frequency in hertz and revolutions per minute are in turn more convenient in measurements and in describing machines — which is why the result panel shows all three quantities side by side.
The range of angular velocities found in nature and technology spans more than twenty orders of magnitude. The Sun orbits the center of the Galaxy once every 230 million years or so, giving ω ≈ 8.7·10⁻¹⁶ rad/s. The Earth orbits the Sun at ω = 1.99·10⁻⁷ rad/s and turns about its own axis at 7.29·10⁻⁵ rad/s. A clock’s hour hand has 1.45·10⁻⁴ rad/s, the minute hand 1.75·10⁻³ rad/s, the second hand 0.105 rad/s. A carousel about 0.5 rad/s, a turntable 3.5 rad/s, a ceiling fan 20 rad/s.
On the high side: a car engine at idle 84 rad/s, a washing-machine drum 126 rad/s, a hard drive 754 rad/s, a jet engine turbine about 1,500 rad/s, a laboratory centrifuge up to 10⁴ rad/s, a turbocharger up to 2·10⁴ rad/s. The pulsar in the Crab Nebula spins at ω ≈ 190 rad/s, and the fastest known millisecond pulsar at about 4,500 rad/s, despite a mass greater than the Sun’s. The same formula ω = 2π/T describes them all.
The definition, derivation, and historical note come from mechanics textbooks and metrology sources: D. Halliday, R. Resnick, J. Walker, Fundamentals of Physics, chapters on circular motion and rotation; H. D. Young, R. A. Freedman, University Physics, chapters “Motion in Two or Three Dimensions” (uniform circular motion) and “Rotation of Rigid Bodies” (angular velocity); R. P. Feynman, R. B. Leighton, M. Sands, The Feynman Lectures on Physics, vol. I, chapters 18 and 21 (rotation, the harmonic oscillator); L. Euler, Theoria motus corporum solidorum seu rigidorum, 1765; R. Cotes, Harmonia mensurarum, 1722 (arc measure); BIPM, The International System of Units (SI), 9th edition (radian, hertz); IAU, rotation and orbital periods of Solar System bodies. This page is for educational purposes.
ω is the angular velocity, T the period of rotation, f the frequency. For T = 8 s the result is 0.785 rad/s.
Reference example: one full turn takes 8 s. An angular velocity of 0.785 rad/s is 45° per second.
ω = 0.785 rad/s
The second hand of a clock: a full turn in 60 s. That is six degrees per second.
ω = 0.105 rad/s
The minute hand: one turn per hour, T = 3,600 s.
ω = 1.75·10⁻³ rad/s
The hour hand: two turns per day, T = 12 h = 43,200 s. That is half a degree per minute.
ω = 1.45·10⁻⁴ rad/s
The Earth about its own axis: the sidereal day T = 23 h 56 min 4 s = 86,164 s. This value enters the Earth’s angular momentum.
ω = 7.29·10⁻⁵ rad/s
The Earth around the Sun: one year T = 365.25 days = 31,557,600 s. That is just under one degree per day.
ω = 1.99·10⁻⁷ rad/s
A turntable platter at 33⅓ rpm: T = 60/33.33 = 1.8 s.
ω = 3.49 rad/s
A washing-machine drum in a 1,200 rpm spin cycle: T = 60/1,200 = 0.05 s. That is twenty turns per second.
ω = 125.7 rad/s
A car engine at idle, 800 rpm: T = 0.075 s.
ω = 83.8 rad/s
A ceiling fan at 200 rpm: T = 0.3 s. A blade tip at a radius of 0.6 m moves at 12.6 m/s.
ω = 20.9 rad/s
A hard-drive platter at 7,200 rpm: T = 1/120 s = 0.008333 s.
ω = 754 rad/s
The London Eye observation wheel: one turn in about 30 min = 1,800 s. A capsule at a radius of 60 m moves at 0.21 m/s.
ω = 3.49·10⁻³ rad/s
The calculator finds the angular velocity of uniform rotation from ω = 2π/T: it divides the full angle of 2π radians by the period of one turn. For T = 8 s the result is 0.785 rad/s, that is 0.125 Hz, 7.5 rpm, and 45° per second.
Seconds. Multiply minutes by 60 and hours by 3,600. If you know the revolutions per minute n, the period is T = 60/n: 1,200 rpm gives 0.05 s. The unit switch in the header does not change seconds or radians, because they are shared by both systems.
Both describe the same rotation but in different angle units: frequency f counts full turns per second (Hz), while angular velocity ω counts radians per second. The relation is ω = 2πf. The result panel shows both values as well as revolutions per minute.
Multiply by 2π/60 ≈ 0.10472: 3,000 rpm is 314 rad/s. Conversely, multiply rad/s by 9.549 to get rpm. The calculator does this through the period T = 60/n.
A radian is the angle at which the arc length equals the radius; a full turn is 2π ≈ 6.2832 rad, and 1 rad ≈ 57.3°. In radians the formulas are simplest: v = ω·r, a = ω²·r, θ = ω·t — without the extra factors that would appear with degrees.
The speed of a point one meter from the axis of rotation, v = ω·r for r = 1 m — numerically equal to ω. For another radius multiply ω by r: a carousel seat at a radius of 4 m with ω = 0.785 rad/s moves at 3.14 m/s. A separate v = ω·r calculator does this for any r.
Because the same angle 2π is swept out in less time: ω is inversely proportional to T. Half the period doubles ω — the panel shows that value separately, and the chart draws the hyperbola ω(T).
The formula ω = 2π/T assumes uniform rotation. For a rotor spinning up the result is the average angular velocity over one turn; the instantaneous angular velocity comes from the time derivative of the angle or from a measurement over a short interval.
Time several or several dozen full turns and divide by their number — this reduces the reaction-time error. For fast rotors a stroboscope or a tachometer is used, which gives revolutions per minute directly; then T = 60/n.
Because a full turn relative to the stars (the sidereal day) takes 23 h 56 min 4 s; the 24 h solar day is almost 4 minutes longer because the Earth moves along its orbit in the meantime and must turn slightly more than 360° for the Sun to return to the meridian. The sidereal day is used for the Earth’s ω.
Yes. The vector ω lies along the axis of rotation, with its sense given by the right-hand rule: fingers in the direction of rotation, thumb pointing along ω. The calculator reports the magnitude of that vector; the sense of rotation does not affect the result.
Division by zero is undefined, and a zero period would mean an infinitely fast rotation. The calculator requires T > 0, and until then it displays a message instead of a result.
Use ω = 2π/T. At T = 8 s you get 2π/8 ≈ 0.785 rad/s. The panel also shows f = 1/T = 0.125 Hz and 7.5 rpm.
About 314 rad/s. First T = 60/3000 = 0.02 s, then ω = 2π/T ≈ 314.16 rad/s — same as 50 Hz mains.
f counts full turns per second (Hz); ω counts radians per second. The link is ω = 2πf. Same rotation, different angle units.
Not as the primary result. Here ω = 2π/T from the period. Linear speed at a known r has its own v = ω·r calculator; the panel only shows v at r = 1 m.
Multiply by 60. A 0.5 min period is T = 30 s. Entering minutes without converting overstates ω sixtyfold.
The definition, unit, history, and derivation below come from recognized physics and metrology sources.
Page updated November 3, 2026.