Geosynchronous orbit

Over the course of a day, the object's position in the sky may remain still or trace out a path, typically in a figure-8 form, whose precise characteristics depend on the orbit's inclination and eccentricity.British science fiction author Arthur C. Clarke popularised and expanded the concept in a 1945 paper entitled Extra-Terrestrial Relays – Can Rocket Stations Give Worldwide Radio Coverage?, published in Wireless World magazine.[15] Although these projects had difficulties with signal strength and tracking that could be solved through geosynchronous satellites, the concept was seen as impractical, so Hughes often withheld funds and support.Although its inclined orbit still required moving antennas, it was able to relay TV transmissions, and allowed for US President John F. Kennedy to phone Nigerian prime minister Abubakar Tafawa Balewa from a ship on August 23, 1963.[26] Each satellite dwells over Japan, allowing signals to reach receivers in urban canyons then passes quickly over Australia.[28][30] Once in a viable geostationary orbit, spacecraft can change their longitudinal position by adjusting their semi-major axis such that the new period is shorter or longer than a sidereal day, in order to effect an apparent "drift" Eastward or Westward, respectively.[34] Geosynchronous satellites require some station-keeping in order to remain in position, and once they run out of thruster fuel and are no longer useful they are moved into a higher graveyard orbit.It is not feasible to deorbit geosynchronous satellites, for to do so would take far more fuel than would be used by slightly elevating the orbit; and atmospheric drag is negligible, giving GSOs lifetimes of thousands of years.[35] The retirement process is becoming increasingly regulated and satellites must have a 90% chance of moving over 200 km above the geostationary belt at end of life.Satellites commonly have an inclination of zero, ensuring that the orbit remains over the equator at all times, making it stationary with respect to latitude from the point of view of a ground observer (and in the ECEF reference frame).In the general case of a geosynchronous orbit with a non-zero inclination or eccentricity, the ground track is a more or less distorted figure-eight, returning to the same places once per sidereal day.
Animation (not to scale) showing geosynchronous satellite orbiting the Earth
The geosynchronous orbit was popularised by the science fiction author Arthur C. Clarke , and is thus sometimes called the Clarke Orbit.
Syncom 2 : The first functional geosynchronous satellite
The geostationary satellite (green) always remains above the same marked spot on the equator (brown).
A quasi- zenith satellite orbit
Earth from space, surrounded by small white dots
A computer-generated image of space debris. Two debris fields are shown: around geosynchronous space and low Earth orbit.
The orbit of a geosynchronous satellite at an inclination, from the perspective of an off-Earth observer ( ECI ) and of an observer rotating around the Earth at its spin rate ( ECEF ).
orbital periodEarth's rotationsidereal dayinclinationeccentricitygeostationary orbitequatorial planeCommunications satellitessatellite antennasArthur C. ClarkeHerman Potočnikspace stationsVenus EquilateralGeorge O. Smithscience fictionWireless Worldequatorial orbitHarold RosenHughes AircraftSputnik 1high frequencyundersea cablerocketmediumEcho balloon satellitesTelstar 1spin stabilisedinclined orbitJohn F. KennedyAbubakar Tafawa Balewaremote sensingmicrowavefiber-opticdiurnal motiontelecommunications satellitessolar windradiation pressuregravitationalstation-keepingzenithanalemmaground stationsTundra orbitfrozen orbitstationkeepingSirius XM Satellite RadioQuasi-Zenith Satellite Systemurban canyonsGeostationary transfer orbitEchoStar XVIIinclination changelaunch vehiclesgeosynchronous transfer orbitapogeeperigeestatitesolar sailspace elevatorgraveyard orbiteccentric orbitsEuropean Space AgencyOlympus-1meteoroidExpress-AM11Telkom-1standard gravitational parameterargument of perigeeground trackequatorGeosynchronous satelliteHigh Earth orbitList of orbitsList of satellites in geosynchronous orbitLow Earth orbitMedium Earth orbitMolniya orbitSubsynchronous orbitSupersynchronous orbitSynchronous orbitSmith, George O.Ballantine BooksClarke, Arthur C.Los Angeles TimesBibcodeInternational Telecommunication UnionEUMETSATNASA Institute for Advanced ConceptsorbitsCaptureCircularEllipticalHighly ellipticalEscapeHorseshoeHyperbolic trajectoryInclinedNon-inclinedKeplerLagrange pointOsculatingParabolic trajectoryParkingPrograde / RetrogradeSynchronousTransfer orbitGeocentricGeostationaryGeostationary transferGraveyardHigh EarthLow EarthMedium EarthMolniyaNear-equatorialOrbit of the MoonSun-synchronousTransatmosphericTundraVery low EarthAreocentricAreosynchronousAreostationaryDistant retrogradeLissajousLibrationHeliocentricEarth's orbitMars cyclerHeliosynchronousLunar cyclerParametersSemi-major axisSemi-minor axisApsidesLongitude of the ascending nodeArgument of periapsisLongitude of the periapsisMean anomalyTrue anomalyEccentric anomalyMean longitudeTrue longitudeMean motionOrbital speedManeuversBi-elliptic transferCollision avoidance (spacecraft)Delta-vDelta-v budgetGravity assistGravity turnHohmann transferLow-energy transferOberth effectPhasingRocket equationRendezvousTrans-lunar injectionTransposition, docking, and extractionOrbitalmechanicsAstronomical coordinate systemsCharacteristic energyEscape velocityEphemerisEquatorial coordinate systemHill sphereInterplanetary Transport NetworkKepler's laws of planetary motionKozai mechanismLagrangian pointn-body problemOrbit equationOrbital state vectorsPerturbationRetrograde and prograde motionSpecific orbital energySpecific angular momentumTwo-line elementsRing systemsPlanetsRings of JupiterRings of SaturnRings of UranusRings of NeptuneRings of Earthspace debrisMinor planetsRings of CharikloRing of HaumeaRings of RheaAccretion discGas torusCircumstellar discCircumplanetary discSpaceflightAstrodynamicsHistoryTimelineSpace RaceRecordsAccidents and incidentsSpace launchSpace policyEuropean UnionNorth KoreaSouth KoreaRussiaSoviet UnionUnited StatesSpace lawOuter Space TreatyRescue AgreementSpace Liability ConventionRegistration ConventionMoon TreatySpace warfareSpace commandSpace forceMilitarisation of spacePrivate spaceflightBillionaire space raceApplicationsAstronomyEarth observationArchaeologyImagery and mappingReconnaissanceWeather and environment monitoringCommunications satelliteInternetTelephoneTelevisionSatellite navigationCommercial use of spaceSpace launch market competitionSpace architectureSpace explorationSpace researchSpace technologySpace weatherHuman spaceflightAstronautcommercialLife-support systemAnimals in spaceBioastronauticsSpace suitExtravehicular activityOverview effectWeightlessnessSpace toiletSpace tourismSpace colonizationSpace divingVostokMercuryVoskhodGeminiApolloSkylabApollo–SoyuzSpace ShuttleShuttle–MirInternational Space StationShenzhouTiangongNew ShepardArtemisEffect of spaceflight on the human bodySpace adaptation syndromeHealth threat from cosmic raysSpace psychologyPsychological and sociological effectsSpace and survivalSpace medicineSpace nursingSpace sexologySpacecraftLaunch vehicleSpace capsuleOrbital moduleReentry capsuleService moduleSpaceplaneRobotic spacecraftSatelliteSpace probeLanderSelf-replicating spacecraftSpace telescopeSpacecraft propulsionRocket engineElectric propulsionSub-orbitalOrbitalInterplanetaryInterstellarIntergalacticDirect ascentExpendablereusable launch systemsLaunch padNon-rocket spacelaunchSpaceportGround segmentFlight controllerGround stationMission control center