Earth's rotation

Earth's rotation is the rotation of planet Earth around its own axis. Earth rotates eastward, in prograde motion. As viewed from the north pole star Polaris, Earth turns counterclockwise.

For the duration of daylight and night, see Daytime and Night.

An animation of Earth's rotation around the planet's axis
This long-exposure photo of the northern night sky above the Nepali Himalayas shows the apparent paths of the stars as Earth rotates.
Earth's rotation imaged by DSCOVR EPIC on 29 May 2016, a few weeks before the solstice.

The North Pole, also known as the Geographic North Pole or Terrestrial North Pole, is the point in the Northern Hemisphere where Earth's axis of rotation meets its surface. This point is distinct from Earth's North Magnetic Pole. The South Pole is the other point where Earth's axis of rotation intersects its surface, in Antarctica.

Earth rotates once in about 24 hours with respect to the Sun, but once every 23 hours, 56 minutes, and 4 seconds with respect to other, distant, stars (see below). Earth's rotation is slowing slightly with time; thus, a day was shorter in the past. This is due to the tidal effects the Moon has on Earth's rotation. Atomic clocks show that a modern-day is longer by about 1.7 milliseconds than a century ago,[1] slowly increasing the rate at which UTC is adjusted by leap seconds. Analysis of historical astronomical records shows a slowing trend; the length of a day increased about 2.3 milliseconds per century since the 8th century BCE.[2]It was noted by scientists in 2020 that earth has started spinning faster compared to previous many decades.[3]

History

Among the ancient Greeks, several of the Pythagorean school believed in the rotation of Earth rather than the apparent diurnal rotation of the heavens. Perhaps the first was Philolaus (470–385 BCE), though his system was complicated, including a counter-earth rotating daily about a central fire.[4]

A more conventional picture was that supported by Hicetas, Heraclides and Ecphantus in the fourth century BCE who assumed that Earth rotated but did not suggest that Earth revolved about the Sun. In the third century BCE, Aristarchus of Samos suggested the Sun's central place.

However, Aristotle in the fourth century BCE criticized the ideas of Philolaus as being based on theory rather than observation. He established the idea of a sphere of fixed stars that rotated about Earth.[5] This was accepted by most of those who came after, in particular Claudius Ptolemy (2nd century CE), who thought Earth would be devastated by gales if it rotated.[6]

In 499 CE, the Indian astronomer Aryabhata wrote that the spherical Earth rotates about its axis daily, and that the apparent movement of the stars is a relative motion caused by the rotation of Earth. He provided the following analogy: "Just as a man in a boat going in one direction sees the stationary things on the bank as moving in the opposite direction, in the same way to a man at Lanka the fixed stars appear to be going westward."[7][8]

In the 10th century, some Muslim astronomers accepted that Earth rotates around its axis.[9] According to al-Biruni, Abu Sa'id al-Sijzi (d. circa 1020) invented an astrolabe called al-zūraqī based on the idea believed by some of his contemporaries "that the motion we see is due to the Earth's movement and not to that of the sky."[10][11] The prevalence of this view is further confirmed by a reference from the 13th century which states: "According to the geometers [or engineers] (muhandisīn), the Earth is in constant circular motion, and what appears to be the motion of the heavens is actually due to the motion of the Earth and not the stars."[10] Treatises were written to discuss its possibility, either as refutations or expressing doubts about Ptolemy's arguments against it.[12] At the Maragha and Samarkand observatories, Earth's rotation was discussed by Tusi (b. 1201) and Qushji (b. 1403); the arguments and evidence they used resemble those used by Copernicus.[13]

In medieval Europe, Thomas Aquinas accepted Aristotle's view[14] and so, reluctantly, did John Buridan[15] and Nicole Oresme[16] in the fourteenth century. Not until Nicolaus Copernicus in 1543 adopted a heliocentric world system did the contemporary understanding of Earth's rotation begin to be established. Copernicus pointed out that if the movement of Earth is violent, then the movement of the stars must be very much more so. He acknowledged the contribution of the Pythagoreans and pointed to examples of relative motion. For Copernicus this was the first step in establishing the simpler pattern of planets circling a central Sun.[17]

Tycho Brahe, who produced accurate observations on which Kepler based his laws of planetary motion, used Copernicus's work as the basis of a system assuming a stationary Earth. In 1600, William Gilbert strongly supported Earth's rotation in his treatise on Earth's magnetism[18] and thereby influenced many of his contemporaries.[19] Those like Gilbert who did not openly support or reject the motion of Earth about the Sun are called "semi-Copernicans".[20] A century after Copernicus, Riccioli disputed the model of a rotating Earth due to the lack of then-observable eastward deflections in falling bodies;[21] such deflections would later be called the Coriolis effect. However, the contributions of Kepler, Galileo and Newton gathered support for the theory of the rotation of Earth.

Empirical tests

Earth's rotation implies that the Equator bulges and the geographical poles are flattened. In his Principia, Newton predicted this flattening would occur in the ratio of 1:230, and pointed to the pendulum measurements taken by Richer in 1673 as corroboration of the change in gravity,[22] but initial measurements of meridian lengths by Picard and Cassini at the end of the 17th century suggested the opposite. However, measurements by Maupertuis and the French Geodesic Mission in the 1730s established the oblateness of Earth, thus confirming the positions of both Newton and Copernicus.[23]

In Earth's rotating frame of reference, a freely moving body follows an apparent path that deviates from the one it would follow in a fixed frame of reference. Because of the Coriolis effect, falling bodies veer slightly eastward from the vertical plumb line below their point of release, and projectiles veer right in the Northern Hemisphere (and left in the Southern) from the direction in which they are shot. The Coriolis effect is mainly observable at a meteorological scale, where it is responsible for the opposite directions of cyclone rotation in the Northern and Southern hemispheres (anticlockwise and clockwise, respectively).

Hooke, following a suggestion from Newton in 1679, tried unsuccessfully to verify the predicted eastward deviation of a body dropped from a height of 8.2 meters, but definitive results were obtained later, in the late 18th and early 19th century, by Giovanni Battista Guglielmini in Bologna, Johann Friedrich Benzenberg in Hamburg and Ferdinand Reich in Freiberg, using taller towers and carefully released weights.[n 1] A ball dropped from a height of 158.5 m departed by 27.4 mm from the vertical compared with a calculated value of 28.1 mm.

The most celebrated test of Earth's rotation is the Foucault pendulum first built by physicist Léon Foucault in 1851, which consisted of a lead-filled brass sphere suspended 67 m from the top of the Panthéon in Paris. Because of Earth's rotation under the swinging pendulum, the pendulum's plane of oscillation appears to rotate at a rate depending on latitude. At the latitude of Paris the predicted and observed shift was about 11 degrees clockwise per hour. Foucault pendulums now swing in museums around the world.

Periods
Starry circles arc around the south celestial pole, seen overhead at ESO's La Silla Observatory.[24]

True solar day
Main article: Solar time

Earth's rotation period relative to the Sun (solar noon to solar noon) is its true solar day or apparent solar day. It depends on Earth's orbital motion and is thus affected by changes in the eccentricity and inclination of Earth's orbit. Both vary over thousands of years, so the annual variation of the true solar day also varies. Generally, it is longer than the mean solar day during two periods of the year and shorter during another two.[n 2] The true solar day tends to be longer near perihelion when the Sun apparently moves along the ecliptic through a greater angle than usual, taking about 10 seconds longer to do so. Conversely, it is about 10 seconds shorter near aphelion. It is about 20 seconds longer near a solstice when the projection of the Sun's apparent motion along the ecliptic onto the celestial equator causes the Sun to move through a greater angle than usual. Conversely, near an equinox the projection onto the equator is shorter by about 20 seconds. Currently, the perihelion and solstice effects combine to lengthen the true solar day near 22 December by 30 mean solar seconds, but the solstice effect is partially cancelled by the aphelion effect near 19 June when it is only 13 seconds longer. The effects of the equinoxes shorten it near 26 March and 16 September by 18 seconds and 21 seconds, respectively.[25][26]

Mean solar day
Main article: Solar time § Mean solar time

The average of the true solar day during the course of an entire year is the mean solar day, which contains 86400 mean solar seconds. Currently, each of these seconds is slightly longer than an SI second because Earth's mean solar day is now slightly longer than it was during the 19th century due to tidal friction. The average length of the mean solar day since the introduction of the leap second in 1972 has been about 0 to 2 ms longer than 86400 SI seconds.[27][28][29] Random fluctuations due to core-mantle coupling have an amplitude of about 5 ms.[30][31] The mean solar second between 1750 and 1892 was chosen in 1895 by Simon Newcomb as the independent unit of time in his Tables of the Sun. These tables were used to calculate the world's ephemerides between 1900 and 1983, so this second became known as the ephemeris second. In 1967 the SI second was made equal to the ephemeris second.[32]

The apparent solar time is a measure of Earth's rotation and the difference between it and the mean solar time is known as the equation of time.

Stellar and sidereal day
On a prograde planet like Earth, the stellar day is shorter than the solar day. At time 1, the Sun and a certain distant star are both overhead. At time 2, the planet has rotated 360° and the distant star is overhead again but the Sun is not (1→2 = one stellar day). It is not until a little later, at time 3, that the Sun is overhead again (1→3 = one solar day).

Earth's rotation period relative to the International Celestial Reference Frame, called its stellar day by the International Earth Rotation and Reference Systems Service (IERS), is 86 164.098 903 691 seconds of mean solar time (UT1) (23h 56m 4.098903691s, 0.99726966323716 mean solar days).[33][n 3] Earth's rotation period relative to the precessing mean vernal equinox, named sidereal day, is 86164.09053083288 seconds of mean solar time (UT1) (23h 56m 4.09053083288s, 0.99726956632908 mean solar days).[33] Thus, the sidereal day is shorter than the stellar day by about 8.4 ms.[35]

Both the stellar day and the sidereal day are shorter than the mean solar day by about 3 minutes 56 seconds. This is a result of the Earth turning 1 additional rotation, relative to the celestial reference frame, as it orbits the Sun (so 366.25 rotations/y). The mean solar day in SI seconds is available from the IERS for the periods 1623–2005[36] and 1962–2005.[37]

Recently (1999–2010) the average annual length of the mean solar day in excess of 86400 SI seconds has varied between 0.25 ms and 1 ms, which must be added to both the stellar and sidereal days given in mean solar time above to obtain their lengths in SI seconds (see Fluctuations in the length of day).

Angular speed
Plot of latitude vs tangential speed. The dashed line shows the Kennedy Space Center example. The dot-dash line denotes typical airliner cruise speed.

The angular speed of Earth's rotation in inertial space is (7.2921150 ± 0.0000001)×10^−5 radians per SI second.[33][n 4] Multiplying by (180°/π radians) × (86,400 seconds/day) yields 360.985 6°/day, indicating that Earth rotates more than 360° relative to the fixed stars in one solar day. Earth's movement along its nearly circular orbit while it is rotating once around its axis requires that Earth rotate slightly more than once relative to the fixed stars before the mean Sun can pass overhead again, even though it rotates only once (360°) relative to the mean Sun.[n 5] Multiplying the value in rad/s by Earth's equatorial radius of 6,378,137 m (WGS84 ellipsoid) (factors of 2π radians needed by both cancel) yields an equatorial speed of 465.10 metres per second (1,674.4 km/h).[38] Some sources state that Earth's equatorial speed is slightly less, or 1,669.8 km/h.[39] This is obtained by dividing Earth's equatorial circumference by 24 hours. However, the use of the solar day is incorrect; it must be the sidereal day, so the corresponding time unit must be a sidereal hour. This is confirmed by multiplying by the number of sidereal days in one mean solar day, 1.002 737 909 350 795,[33] which yields the equatorial speed in mean solar hours given above of 1,674.4 km/h or 1040.0mph.

The tangential speed of Earth's rotation at a point on Earth can be approximated by multiplying the speed at the equator by the cosine of the latitude.[40] For example, the Kennedy Space Center is located at latitude 28.59° N, which yields a speed of: cos(28.59°) × 1674.4 km/h = 1470.2 km/h. Latitude is a placement consideration for spaceports.

Changes
Earth's axial tilt is about 23.4°. It oscillates between 22.1° and 24.5° on a 41000-year cycle and is currently decreasing.

In rotational axis
Main article: Earth's rotation axis

Earth's rotation axis moves with respect to the fixed stars (inertial space); the components of this motion are precession and nutation. It also moves with respect to Earth's crust; this is called polar motion.

Precession is a rotation of Earth's rotation axis, caused primarily by external torques from the gravity of the Sun, Moon and other bodies. The polar motion is primarily due to free core nutation and the Chandler wobble.

In rotational speed
Main articles: Day length fluctuations and ΔT (timekeeping)

Tidal interactions

Over millions of years, Earth's rotation has been slowed significantly by tidal acceleration through gravitational interactions with the Moon. Thus angular momentum is slowly transferred to the Moon at a rate proportional to , where is the orbital radius of the Moon. This process has gradually increased the length of the day to its current value, and resulted in the Moon being tidally locked with Earth.

This gradual rotational deceleration is empirically documented by estimates of day lengths obtained from observations of tidal rhythmites and stromatolites; a compilation of these measurements[41] found that the length of the day has increased steadily from about 21 hours at 600 Myr ago[42] to the current 24-hour value. By counting the microscopic lamina that form at higher tides, tidal frequencies (and thus day lengths) can be estimated, much like counting tree rings, though these estimates can be increasingly unreliable at older ages.[43]

Resonant stabilization
A simulated history of Earth's day length, depicting a resonant-stabilizing event throughout the Precambrian era.[44]

The current rate of tidal deceleration is anomalously high, implying Earth's rotational velocity must have decreased more slowly in the past. Empirical data[41] tentatively shows a sharp increase in rotational deceleration about 600 Myr ago. Some models suggest that Earth maintained a constant day length of 21 hours throughout much of the Precambrian.[42] This day length corresponds to the semidiurnal resonant period of the thermally-driven atmospheric tide; at this day length, the decelerative lunar torque could have been canceled by an accelerative torque from the atmospheric tide, resulting in no net torque and a constant rotational period. This stabilizing effect could have been broken by a sudden change in global temperature. Recent computational simulations support this hypothesis and suggest the Marinoan or Sturtian glaciations broke this stable configuration about 600 Myr ago; the simulated results agree quite closely with existing paleorotational data.[44]

Global events
Deviation of day length from SI-based day

Some recent large-scale events, such as the 2004 Indian Ocean earthquake, have caused the length of a day to shorten by 3 microseconds by reducing Earth's moment of inertia.[45] Post-glacial rebound, ongoing since the last Ice age, is also changing the distribution of Earth's mass, thus affecting the moment of inertia of Earth and, by the conservation of angular momentum, Earth's rotation period.[46]

The length of the day can also be influenced by manmade structures. For example, NASA scientists calculated that the water stored in the Three Gorges Dam has increased the length of Earth's day by 0.06 microseconds due to the shift in mass.[47]

Measurement

The primary monitoring of Earth's rotation is performed by very-long-baseline interferometry coordinated with the Global Positioning System, satellite laser ranging, and other satellite techniques. This provides an absolute reference for the determination of universal time, precession, and nutation.[48] The absolute value of Earth rotation including UT1 and nutation can be determined using space geodetic observations, such as Very Long Baseline Interferometry and Lunar laser ranging, whereas their derivatives, denoted as Length-of-day excess and nutation rates can be derived from satellite observations, such as GPS, GLONASS, Galileo[49] and Satellite laser ranging to geodetic satellites.[50]

Ancient observations

There are recorded observations of solar and lunar eclipses by Babylonian and Chinese astronomers beginning in the 8th century BCE, as well as from the medieval Islamic world and elsewhere. These observations can be used to determine changes in Earth's rotation over the last 27 centuries, since the length of the day is a critical parameter in the calculation of the place and time of eclipses. A change in day length of milliseconds per century shows up as a change of hours and thousands of kilometers in eclipse observations. The ancient data are consistent with a shorter day, meaning Earth was turning faster throughout the past.[51][52]

Cyclic variability

Around every 25–30 years Earth's rotation slows temporarily by a few milliseconds per day, usually lasting around 5 years. 2017 was the fourth consecutive year that Earth's rotation has slowed. The cause of this variability has not yet been determined.[53]

Origin
An artist's rendering of the protoplanetary disk.

Earth's original rotation was a vestige of the original angular momentum of the cloud of dust, rocks, and gas that coalesced to form the Solar System. This primordial cloud was composed of hydrogen and helium produced in the Big Bang, as well as heavier elements ejected by supernovas. As this interstellar dust is heterogeneous, any asymmetry during gravitational accretion resulted in the angular momentum of the eventual planet.[54]

However, if the giant-impact hypothesis for the origin of the Moon is correct, this primordial rotation rate would have been reset by the Theia impact 4.5 billion years ago. Regardless of the speed and tilt of Earth's rotation before the impact, it would have experienced a day some five hours long after the impact.[55] Tidal effects would then have slowed this rate to its modern value.

See also

Notes
  1. See Fallexperimente zum Nachweis der Erdrotation (German Wikipedia article).
  2. When Earth's eccentricity exceeds 0.047 and perihelion is at an appropriate equinox or solstice, only one period with one peak balances another period that has two peaks.[25]
  3. Aoki, the ultimate source of these figures, uses the term "seconds of UT1" instead of "seconds of mean solar time".[34]
  4. It can be established that SI seconds apply to this value by following the citation in "USEFUL CONSTANTS" to E. Groten "Parameters of Common Relevance of Astronomy, Geodesy, and Geodynamics" which states units are SI units, except for an instance not relevant to this value.
  5. In astronomy, unlike geometry, 360° means returning to the same point in some cyclical time scale, either one mean solar day or one sidereal day for rotation on Earth's axis, or one sidereal year or one mean tropical year or even one mean Julian year containing exactly 365.25 days for revolution around the Sun.

References
  1. Dennis D. McCarthy; Kenneth P. Seidelmann (18 September 2009). Time: From Earth Rotation to Atomic Physics. John Wiley & Sons. p. 232. ISBN 978-3-527-62795-0.
  2. Stephenson, F. Richard (2003). "Historical eclipses and Earth's rotation". Astronomy & Geophysics. 44 (2): 2.22–2.27. Bibcode:2003A&G....44b..22S. doi:10.1046/j.1468-4004.2003.44222.x.
  3. Rice, Doyle. "Scientists say Earth is spinning faster than it has in decades". USA TODAY. Retrieved 31 January 2021.
  4. Burch, George Bosworth (1954). "The Counter-Earth". Osiris. 11: 267–294. doi:10.1086/368583. JSTOR 301675. S2CID 144330867.
  5. Aristotle. Of the Heavens. Book II, Ch 13. 1.
  6. Ptolemy. Almagest Book I, Chapter 8.
  7. "Archived copy" (PDF). Archived from the original (PDF) on 13 December 2013. Retrieved 8 December 2013.CS1 maint: archived copy as title (link)
  8. Kim Plofker (2009). Mathematics in India. Princeton University Press. p. 71. ISBN 978-0-691-12067-6.
  9. Alessandro Bausani (1973). "Cosmology and Religion in Islam". Scientia/Rivista di Scienza. 108 (67): 762.
  10. Young, M. J. L., ed. (2 November 2006). Religion, Learning and Science in the 'Abbasid Period. Cambridge University Press. p. 413. ISBN 9780521028875.
  11. Nasr, Seyyed Hossein (1 January 1993). An Introduction to Islamic Cosmological Doctrines. SUNY Press. p. 135. ISBN 9781438414195.
  12. Ragep, Sally P. (2007). "Ibn Sīnā: Abū ʿAlī al‐Ḥusayn ibn ʿAbdallāh ibn Sīnā". In Thomas Hockey; et al. (eds.). The Biographical Encyclopedia of Astronomers. New York: Springer. pp. 570–2. ISBN 978-0-387-31022-0. (PDF version)
  13. Ragep, F. Jamil (2001a), "Tusi and Copernicus: The Earth's Motion in Context", Science in Context, 14 (1–2): 145–163, doi:10.1017/s0269889701000060
  14. Aquinas, Thomas. Commentaria in libros Aristotelis De caelo et Mundo. Lib II, cap XIV. trans in Grant, Edward, ed. (1974). A Source Book in Medieval Science. Harvard University Press. pages 496–500
  15. Buridan, John (1942). Quaestiones super libris quattuo De Caelo et mundo. pp. 226–232. in Grant 1974, pp. 500–503
  16. Oresme, Nicole. Le livre du ciel et du monde. pp. 519–539. in Grant 1974, pp. 503–510
  17. Copernicus, Nicolas. On the Revolutions of the Heavenly Spheres. Book I, Chap 5–8.
  18. Gilbert, William (1893). De Magnete, On the Magnet and Magnetic Bodies, and on the Great Magnet the Earth. New York, J. Wiley & sons. pp. 313–347.
  19. Russell, John L (1972). "Copernican System in Great Britain". In J. Dobrzycki (ed.). The Reception of Copernicus' Heliocentric Theory. p. 208. ISBN 9789027703118.
  20. J. Dobrzycki 1972, p. 221
  21. Almagestum novum, chapter nine, cited in Graney, Christopher M. (2012). "126 arguments concerning the motion of the earth. GIOVANNI BATTISTA RICCIOLI in his 1651 ALMAGESTUM NOVUM". Journal for the History of Astronomy. volume 43, pages 215–226. arXiv:1103.2057.
  22. Newton, Isaac (1846). Newton's Principia. Translated by A. Motte. New-York : Published by Daniel Adee. p. 412.
  23. Shank, J. B. (2008). The Newton Wars and the Beginning of the French Enlightenment. University of Chicago Press. pp. 324, 355. ISBN 9780226749471.
  24. "Starry Spin-up". Retrieved 24 August 2015.
  25. Jean Meeus; J. M. A. Danby (January 1997). Mathematical Astronomy Morsels. Willmann-Bell. pp. 345–346. ISBN 978-0-943396-51-4.
  26. Ricci, Pierpaolo. "www.pierpaoloricci.it/dati/giorno solare vero VERSIONE EN". Pierpaoloricci.it. Retrieved 22 September 2018.
  27. "INTERNATIONAL EARTH ROTATION AND REFERENCE SYSTEMS SERVICE : EARTH ORIENTATION PARAMETERS : EOP (IERS) 05 C04". Hpiers.obspm.fr. Retrieved 22 September 2018.
  28. "Physical basis of leap seconds" (PDF). Iopscience.iop.org. Retrieved 22 September 2018.
  29. Leap seconds Archived 12 March 2015 at the Wayback Machine
  30. "Prediction of Universal Time and LOD Variations" (PDF). Ien.it. Retrieved 22 September 2018.
  31. R. Hide et al., "Topographic core-mantle coupling and fluctuations in the Earth's rotation" 1993.
  32. Leap seconds by USNO Archived 12 March 2015 at the Wayback Machine
  33. "USEFUL CONSTANTS". Hpiers.obspm.fr. Retrieved 22 September 2018.
  34. Aoki, et al., "The new definition of Universal Time", Astronomy and Astrophysics 105 (1982) 359–361.
  35. P. Kenneth Seidelmann, ed. (1992). Explanatory Supplement to the Astronomical Almanac. Mill Valley, California: University Science Books. p. 48. ISBN 978-0-935702-68-2.
  36. IERS Excess of the duration of the day to 86,400s … since 1623 Archived 3 October 2008 at the Wayback Machine Graph at end.
  37. "Excess to 86400s of the duration day, 1995–1997". 13 August 2007. Archived from the original on 13 August 2007. Retrieved 22 September 2018.
  38. Arthur N. Cox, ed., Allen's Astrophysical Quantities p.244.
  39. Michael E. Bakich, The Cambridge planetary handbook, p.50.
  40. Butterworth & Palmer. "Speed of the turning of the Earth". Ask an Astrophysicist. NASA Goddard Spaceflight Center.
  41. Williams, George E. (1 February 2000). "Geological constraints on the Precambrian history of Earth's rotation and the Moon's orbit". Reviews of Geophysics. 38 (1): 37–59. Bibcode:2000RvGeo..38...37W. doi:10.1029/1999RG900016. ISSN 1944-9208.
  42. Zahnle, K.; Walker, J. C. (1 January 1987). "A constant daylength during the Precambrian era?". Precambrian Research. 37 (2): 95–105. Bibcode:1987PreR...37...95Z. CiteSeerX 10.1.1.1020.8947. doi:10.1016/0301-9268(87)90073-8. ISSN 0301-9268. PMID 11542096.
  43. Scrutton, C. T. (1 January 1978). "Periodic Growth Features in Fossil Organisms and the Length of the Day and Month". In Brosche, Professor Dr Peter; Sündermann, Professor Dr Jürgen (eds.). Tidal Friction and the Earth's Rotation. Springer Berlin Heidelberg. pp. 154–196. doi:10.1007/978-3-642-67097-8_12. ISBN 9783540090465.
  44. Bartlett, Benjamin C.; Stevenson, David J. (1 January 2016). "Analysis of a Precambrian resonance-stabilized day length". Geophysical Research Letters. 43 (11): 5716–5724. arXiv:1502.01421. Bibcode:2016GeoRL..43.5716B. doi:10.1002/2016GL068912. ISSN 1944-8007. S2CID 36308735.
  45. Sumatran earthquake sped up Earth's rotation, Nature, 30 December 2004.
  46. Wu, P.; W.R.Peltier (1984). "Pleistocene deglaciation and the earth's rotation: a new analysis". Geophysical Journal of the Royal Astronomical Society. 76 (3): 753–792. Bibcode:1984GeoJ...76..753W. doi:10.1111/j.1365-246X.1984.tb01920.x.
  47. "NASA Details Earthquake Effects on the Earth". NASA/JPL. Retrieved 22 March 2019.
  48. "Permanent monitoring". Hpiers.obspm.fr. Retrieved 22 September 2018.
  49. Zajdel, Radosław; Sośnica, Krzysztof; Bury, Grzegorz; Dach, Rolf; Prange, Lars (July 2020). "System-specific systematic errors in earth rotation parameters derived from GPS, GLONASS, and Galileo". GPS Solutions. 24 (3): 74. doi:10.1007/s10291-020-00989-w.
  50. Sośnica, K.; Bury, G.; Zajdel, R. (16 March 2018). "Contribution of Multi‐GNSS Constellation to SLR‐Derived Terrestrial Reference Frame". Geophysical Research Letters. 45 (5): 2339–2348. Bibcode:2018GeoRL..45.2339S. doi:10.1002/2017GL076850.
  51. Sid Perkins (6 December 2016). "Ancient eclipses show Earth's rotation is slowing". Science. doi:10.1126/science.aal0469.
  52. FR Stephenson; LV Morrison; CY Hohonkerk (7 December 2016). "Measurement of the Earth's rotation: 720 BC to AD 2015". Proceedings of the Royal Society A. 472 (2196): 20160404. Bibcode:2016RSPSA.47260404S. doi:10.1098/rspa.2016.0404. PMC 5247521. PMID 28119545.
  53. Nace, Trevor. "Earth's Rotation Is Mysteriously Slowing Down: Experts Predict Uptick In 2018 Earthquakes". Forbes. Retrieved 18 October 2019.
  54. "Why do planets rotate?". Ask an Astronomer.
  55. Stevenson, D. J. (1987). "Origin of the moon–The collision hypothesis". Annual Review of Earth and Planetary Sciences. 15 (1): 271–315. Bibcode:1987AREPS..15..271S. doi:10.1146/annurev.ea.15.050187.001415.
This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.