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	<title>Synchronous orbit - Revision history</title>
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		<title>imported&gt;CloverV: /* Examples */</title>
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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;Examples&lt;/span&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Orbit of an astronomical body equal to that body&amp;#039;s average rotational period}}&lt;br /&gt;
A &amp;#039;&amp;#039;&amp;#039;synchronous orbit&amp;#039;&amp;#039;&amp;#039; is an [[orbit]] in which an orbiting body (usually a [[satellite]]) has a period equal to the average rotational period of the body being orbited (usually a planet), and in the same direction of rotation as that body.&amp;lt;ref&amp;gt;{{Cite web|url=http://earthobservatory.nasa.gov/Features/OrbitsCatalog/|title=Catalog of Earth Satellite Orbits : Feature Articles|last=Holli|first=Riebeek|date=2009-09-04|website=earthobservatory.nasa.gov|language=en|access-date=2016-05-08}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Simplified meaning ==&lt;br /&gt;
A [[synchronous]] orbit is an [[orbit]] in which the orbiting object (for example, an artificial satellite or a moon) takes the same amount of time to complete an orbit as it takes the object it is orbiting to rotate once.&lt;br /&gt;
&lt;br /&gt;
== Properties ==&lt;br /&gt;
A satellite in a synchronous orbit that is both [[equator]]ial and [[circle|circular]] will appear to be suspended motionless above a point on the orbited planet&amp;#039;s equator. For synchronous satellites orbiting [[Earth]], this is also known as a [[geostationary orbit]]. However, a synchronous orbit need not be equatorial; nor circular. A body in a non-equatorial synchronous orbit will appear to oscillate north and south above a point on the planet&amp;#039;s equator, whereas a body in an [[ellipse|elliptical]] orbit will appear to oscillate eastward and westward. As seen from the orbited body the combination of these two motions produces a figure-8 pattern called an [[analemma]].&lt;br /&gt;
&lt;br /&gt;
== Nomenclature ==&lt;br /&gt;
There are many specialized terms for synchronous orbits depending on the body orbited. The following are some of the more common ones. A synchronous orbit around [[Earth]] that is circular and lies in the equatorial plane is called a [[geostationary orbit]]. The more general case, when the orbit is inclined to Earth&amp;#039;s equator or is non-circular is called a [[geosynchronous orbit]]. The corresponding terms for synchronous orbits around [[Mars]] are [[Areostationary orbit|areostationary]] and [[Areosynchronous orbit|areosynchronous]] orbits.&amp;lt;ref&amp;gt;{{cite web |title=A Proposed Communication and Navigation Infrastructure at Mars |url=http://marsnet.jpl.nasa.gov/what-is-it/what-is-it.html |website=Mars Network |publisher=NASA JPL |archive-url=https://web.archive.org/web/20070621171137/http://marsnet.jpl.nasa.gov/what-is-it/what-is-it.html |archive-date=2007-06-21 |date=1999-11-24 |url-status=dead}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Formula ==&lt;br /&gt;
&lt;br /&gt;
For a stationary synchronous orbit:&amp;lt;ref&amp;gt;{{Cite news|url=https://www.askwillonline.com/2012/12/calculating-radius-of-geostationary.html|title=Calculating the Radius of a Geostationary Orbit - Ask Will Online|date=2012-12-27|work=Ask Will Online|access-date=2017-11-21|language=en-GB}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;R_{syn} = \sqrt[3]{{G(m_2)T^2\over 4 \pi^2}}&amp;lt;/math&amp;gt;&lt;br /&gt;
where:&lt;br /&gt;
{{block indent |left=1.5 |text={{plainlist}}&lt;br /&gt;
* &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;G&amp;lt;/math&amp;gt; is the [[gravitational constant]]&lt;br /&gt;
* &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;m_2&amp;lt;/math&amp;gt; is the mass of the celestial body&lt;br /&gt;
* &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;T&amp;lt;/math&amp;gt; is the [[Sidereal time|sidereal]] rotational period of the body&lt;br /&gt;
* &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;R_{syn}&amp;lt;/math&amp;gt; is the radius of orbit&lt;br /&gt;
{{endplainlist}}}}&lt;br /&gt;
&lt;br /&gt;
By this formula, one can find the synchronous orbital radius of a body, given its mass and sidereal rotational period. &lt;br /&gt;
&lt;br /&gt;
Orbital speed (how fast a satellite is moving through space) is calculated by multiplying the angular speed of the satellite by the orbital radius.&amp;lt;ref&amp;gt;see [[Circular motion#Formulas]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Due to obscure quirks of [[orbital mechanics]], no [[Tidal locking|tidally locked]] body in a 1:1 spin-orbit resonance (i.e. a moon locked to a planet or a planet locked to a star) can have a stable satellite in a synchronous orbit, as the synchronous orbital radius lies outside the body&amp;#039;s [[Hill sphere]].&amp;lt;ref&amp;gt;{{Cite web |title=Is it possible to achieve a stable &amp;quot;selenostationary&amp;quot; orbit around the Moon? |url=https://astronomy.stackexchange.com/questions/20499/is-it-possible-to-achieve-a-stable-selenostationary-orbit-around-the-moon/55436#55436 |access-date=2025-05-29 |website=Astronomy Stack Exchange |language=en}}&amp;lt;/ref&amp;gt; This is universal and irrespective of the masses and distances involved.&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
An astronomical example is [[Pluto]]&amp;#039;s largest moon [[Charon (moon)|Charon]].&amp;lt;ref&amp;gt;{{cite journal |title = The Pluto-Charon system |author = S.A. Stern |year = 1992 |journal = Annual Review of Astronomy and Astrophysics |volume = 30 |page = 190 |quote=Charon&amp;#039;s orbit is (a) synchronous with Pluto&amp;#039;s rotation and (b) highly inclined to the plane of the ecliptic. |bibcode=1992ARA&amp;amp;A..30..185S|doi = 10.1146/annurev.aa.30.090192.001153 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
Much more commonly, synchronous orbits are employed by artificial satellites used for communication, such as [[geostationary satellites]].&lt;br /&gt;
&lt;br /&gt;
For natural satellites, which can attain a synchronous orbit only by [[tidal locking|tidally locking]] their parent body, it always goes in hand with [[synchronous rotation]] of the satellite. This is because the smaller body becomes tidally locked faster, and by the time a synchronous orbit is achieved, it has had a locked synchronous rotation for a long time already.&amp;lt;ref&amp;gt;{{Cite web |date=2023-06-06 |title=Tidal Locking - NASA Science |url=https://science.nasa.gov/moon/tidal-locking/ |access-date=2026-03-09 |language=en-US}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The following table lists select [[List of Solar System objects by size|Solar System bodies]]&amp;#039; masses, sidereal rotational periods, and the semi-major axises and altitudes of their synchronous orbital radii (calculated by the formula in the above section):&amp;lt;!--Could someone change the last column from &amp;quot;yes&amp;quot; and &amp;quot;no&amp;quot;s to instead be checks and x&amp;#039;s? I wanted to do that using emojis but it might no render for everyone, and I don&amp;#039;t know how to input the Wikipedia checkmarks and x&amp;#039;s.--&amp;gt; &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable sortable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Body !! Body&amp;#039;s Mass (kg) !! Sidereal Rotation period !! Semi-major axis of synchronous orbit (km) !! Altitude of synchronous orbit (km) &lt;br /&gt;
!Synchronous orbit within [[Hill sphere]]?&lt;br /&gt;
|-&lt;br /&gt;
| [[Mercury (planet)|Mercury]]&amp;lt;ref&amp;gt;{{Cite web |title=Mercury Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/mercuryfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;|| 0.33010×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt; || 1407.6 h || 242,895 km||240,454 km&lt;br /&gt;
|No&lt;br /&gt;
|-&lt;br /&gt;
| [[Venus]]&amp;lt;ref&amp;gt;{{Cite web |title=Venus Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/venusfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;|| 4.8673×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt; || 5832.6 h|| 1,536,578 km||1,530,526 km&lt;br /&gt;
|No&lt;br /&gt;
|-&lt;br /&gt;
| [[Earth]]&amp;lt;ref&amp;gt;{{Cite web |title=Earth Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/earthfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;|| 5.9722×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;|| 23.9345 h|| 42,164 km||35,786 km&lt;br /&gt;
|Yes &lt;br /&gt;
|-&lt;br /&gt;
| [[Moon]]&amp;lt;ref&amp;gt;{{Cite web |title=Moon Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/moonfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;|| 0.07346×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;|| 655.72 h|| 88,453 km||86,715 km&lt;br /&gt;
|No&lt;br /&gt;
|-&lt;br /&gt;
|[[Mars]]&amp;lt;ref&amp;gt;{{Cite web |title=Mars Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/marsfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|0.64169×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;&lt;br /&gt;
|24.6229 h&lt;br /&gt;
|20,428 km&lt;br /&gt;
|17,031 km&lt;br /&gt;
|Yes &lt;br /&gt;
|-&lt;br /&gt;
|[[Ceres (dwarf planet)|Ceres]]&amp;lt;ref&amp;gt;{{Cite web |title=Asteroid Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/asteroidfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|0.09393×10&amp;lt;sup&amp;gt;22&amp;lt;/sup&amp;gt;&lt;br /&gt;
|9.074 h&lt;br /&gt;
|1,192 km&lt;br /&gt;
|723 km&lt;br /&gt;
|Yes&lt;br /&gt;
|-&lt;br /&gt;
|[[Jupiter]]&amp;lt;ref&amp;gt;{{Cite web |title=Jupiter Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/jupiterfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|1898.13×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;&lt;br /&gt;
|9.925 h&lt;br /&gt;
|169,010 km&lt;br /&gt;
|88,518 km&lt;br /&gt;
|Yes&lt;br /&gt;
|-&lt;br /&gt;
|[[Saturn]]&amp;lt;ref&amp;gt;{{Cite web |title=Saturn Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/saturnfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|568.32×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;&lt;br /&gt;
|10.656 h&lt;br /&gt;
|112,239 km&lt;br /&gt;
|51,971 km&lt;br /&gt;
|Yes&lt;br /&gt;
|-&lt;br /&gt;
|[[Uranus]]&amp;lt;ref&amp;gt;{{Cite web |title=Uranus Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/uranusfact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|86.811×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;&lt;br /&gt;
|17.24 h&lt;br /&gt;
|82,686 km&lt;br /&gt;
|57,127 km&lt;br /&gt;
|Yes&lt;br /&gt;
|-&lt;br /&gt;
|[[Neptune]]&amp;lt;ref&amp;gt;{{Cite web |title=Neptune Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/neptunefact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|102.409×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;&lt;br /&gt;
|16.11 h&lt;br /&gt;
|83,508 km&lt;br /&gt;
|58,744 km&lt;br /&gt;
|Yes&lt;br /&gt;
|-&lt;br /&gt;
|[[Pluto]]&amp;lt;ref&amp;gt;{{Cite web |title=Pluto Fact Sheet |url=https://nssdc.gsfc.nasa.gov/planetary/factsheet/plutofact.html |access-date=2025-05-30 |website=nssdc.gsfc.nasa.gov}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
|0.01303×10&amp;lt;sup&amp;gt;24&amp;lt;/sup&amp;gt;&lt;br /&gt;
|153.2928 h&lt;br /&gt;
|18,860 km&lt;br /&gt;
|17,672 km&lt;br /&gt;
|Yes&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Subsynchronous orbit]]&lt;br /&gt;
* [[Supersynchronous orbit]] &lt;br /&gt;
* [[Graveyard orbit]]&lt;br /&gt;
* [[Tidal locking]] (synchronous rotation)&lt;br /&gt;
* [[Sun-synchronous orbit]]&lt;br /&gt;
* [[List of orbits]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
* {{FS1037C}}&lt;br /&gt;
&lt;br /&gt;
{{orbits|state=expanded}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Astrodynamics]]&lt;br /&gt;
[[Category:Orbits]]&lt;/div&gt;</summary>
		<author><name>imported&gt;CloverV</name></author>
	</entry>
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