Degrees per hour to Radian per hour

°/h

1 °/h

rad/hr

0.01745329251994318274337231680736 rad/hr

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Quick Reference Table (Degrees per hour to Radian per hour)

Degrees per hour (°/h)Radian per hour (rad/hr)
0.0010.000017453292519906991596002962392
0.010.000174532925199522305302146554112
0.550.009599310885968750508854774244048
60.104719755119659775044247076239448
150.261799387799149324513282161366072
3606.283185307179586050265482457436688
3,60062.831853071795860050265482457436688

About Degrees per hour (°/h)

Degrees per hour (°/h) is used for very slow angular motions, particularly in navigation, geophysics, and astronomy. High-precision gyroscopes are rated by their drift in °/h — a navigation-grade ring-laser gyro may drift less than 0.01°/h, while a consumer MEMS gyro drifts hundreds of degrees per hour. Earth's rotation corresponds to 15°/h (360° ÷ 24 h), which is why the Sun appears to move 15° per hour across the sky. Telescope drive motors use this rate to compensate for Earth's rotation during long exposures.

Earth rotates at exactly 15°/h, so astronomical telescope drives track stars at 15°/h. Navigation-grade laser gyroscopes achieve drift below 0.01°/h. The Moon moves about 0.55°/h against the background stars.

About Radian per hour (rad/hr)

Radian per hour (rad/hr) describes very slow angular rotation, where even rad/min would give small numbers. Celestial mechanics and geophysical rotation rates are natural fits: Earth rotates at 2π rad per 24 hours ≈ 0.2618 rad/hr. Slow-moving antenna dishes, solar tracker mounts, and geological fault creep rates can be expressed in rad/hr. The unit is rarely used in everyday engineering but appears in astronomical and geophysical literature when tracking long-period rotational phenomena.

Earth completes one rotation in ~24 hours, giving ~0.2618 rad/hr. The Moon orbits Earth at about 0.229 rad/hr (one orbit per ~27.3 days). A clock hour hand moves at π/6 rad/hr ≈ 0.524 rad/hr.


Degrees per hour – Frequently Asked Questions

The ISS completes one orbit (360°) in about 92 minutes, giving roughly 235°/hr — almost 16 times faster than Earth's rotation. That is why astronauts see 16 sunrises every 24 hours. At an altitude of ~408 km, the station covers about 7.66 km/s of ground track. If you could watch it from a fixed point in space, it would visibly sweep through the sky at a rate where one degree takes only about 15 seconds.

Because even tiny drift accumulates into serious navigation errors over a flight or voyage. A navigation-grade ring-laser gyroscope drifts less than 0.01°/hr; over a 10-hour flight that is only 0.1° of heading error. A cheap MEMS gyro drifting 10°/hr would accumulate 100° of error in the same time — useless for navigation. Expressing drift in °/hr makes the operational impact immediately obvious to a pilot or engineer.

Equatorial telescope mounts have a motorised right-ascension axis aligned with Earth's rotation axis. By driving that axis at exactly 15°/hr (one sidereal rate), the telescope counter-rotates against Earth's spin, keeping a star fixed in the eyepiece. Without this drive, stars would drift out of view in seconds at high magnification. Astrophotographers rely on it for long exposures without star trails.

The Moon's apparent motion has two components. It shares the sky's overall 15°/hr westward motion due to Earth's rotation. But it also orbits Earth, moving about 0.55°/hr eastward relative to the stars (360° ÷ 27.32 days ÷ 24 hr). The net effect: the Moon moves westward across the sky at roughly 14.5°/hr, which is why moonrise occurs about 50 minutes later each day.

A Foucault pendulum's swing plane rotates relative to the floor at 15° × sin(latitude) per hour. At the North Pole (90°) that is the full 15°/hr; at 45° latitude it is about 10.6°/hr; at the equator it is zero. The pendulum always swings in a fixed plane in inertial space — it is the Earth rotating underneath it. The sine factor comes from the fact that only the vertical component of Earth's angular velocity vector projects into the pendulum's swing plane. Paris (48.9°N) sees about 11.3°/hr, which is why Foucault's original 1851 demonstration took most of a day to complete a visible rotation.

Radian per hour – Frequently Asked Questions

When the object moves so slowly that rad/s and even rad/min produce inconveniently small numbers. Earth's rotation is 0.2618 rad/hr — much friendlier than 7.27 × 10⁻⁵ rad/s. Astronomical telescope tracking, tidal lock studies, and satellite orbital mechanics often involve motions where one rotation takes hours, days, or longer. Rad/hr keeps the numbers readable while preserving the radian basis.

The Moon completes one orbit (2π radians) in about 27.32 days, or roughly 655.7 hours. That gives approximately 0.00958 rad/hr. Compared to Earth's rotation at 0.2618 rad/hr, the Moon's orbital angular speed is about 27 times slower — which is why moonrise drifts about 50 minutes later each day.

Tectonic plates move at a few centimeters per year, but because they sit on a sphere, that linear drift corresponds to a tiny angular rotation about an Euler pole. The fastest plate — the Pacific — rotates at roughly 10⁻⁸ rad/hr (about 0.00000001 rad/hr). That is around a billion times slower than a clock hour hand. Geophysicists describe plate motion this way because angular velocity around an Euler pole neatly captures both the speed and the curved trajectory of every point on the plate.

A geostationary satellite orbits Earth once per sidereal day (~23.934 hours), matching Earth's rotation. Its angular speed is 2π ÷ 23.934 ≈ 0.2625 rad/hr — essentially the same as Earth's surface rotation. That is the whole point: the satellite appears stationary over one spot on the equator because it rotates at the same angular velocity as the ground below it.

Not typically as a primary readout, but it appears in computed outputs from navigation software, satellite tracking systems, and geophysics simulations. Inertial navigation units report gyro drift budgets in °/hr (degrees per hour), and converting to rad/hr is a single multiplication. The unit is more common in calculations and papers than on any physical gauge dial.

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