Nodal precession is the precession of the orbital plane of a satellite around the rotational axis of an astronomical body such as Earth. This precession is due to the non-spherical nature of a rotating body, which creates a non-uniform gravitational field. The following discussion relates to low Earth orbit of artificial satellites, which have no measurable effect on the motion of Earth. The nodal precession of more massive, natural satellites like the Moon is more complex.
Around a spherical body, an orbital plane would remain fixed in space around the gravitational primary body. However, most bodies rotate, which causes an equatorial bulge. This bulge creates a gravitational effect that causes orbits to precess around the rotational axis of the primary body.
The direction of precession is opposite the direction of revolution. For a typical prograde orbit around Earth (that is, in the direction of primary body's rotation), the longitude of the ascending node decreases, that is the node precesses westward. If the orbit is retrograde, this increases the longitude of the ascending node, that is the node precesses eastward. This nodal progression enables heliosynchronous orbits to maintain a nearly constant angle relative to the Sun.
A non-rotating body of planetary scale or larger would be pulled by gravity into a spherical shape. Virtually all bodies rotate, however. The centrifugal force deforms the body so that it has an equatorial bulge. Because of the bulge of the central body, the gravitational force on a satellite is not directed toward the center of the central body, but is offset toward its equator. Whichever hemisphere of the central body the satellite lies over, it is preferentially pulled slightly toward the equator of the central body. This creates a torque on the satellite. This torque does not reduce the inclination; rather, it causes a torque-induced gyroscopic precession, which causes the orbital nodes to drift with time.
The rate of precession depends on the inclination of the orbital plane to the equatorial plane, as well as the orbital eccentricity.
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vignette|droite|200px|Animation de la Lune avec ses différentes phases, vue depuis l'hémisphère Nord. Le flottement apparent de la Lune est connu sous le vocable de libration. Un mois lunaire est une unité de temps correspondant à la durée entre deux occurrences d'une position relative de la Lune et de la Terre. Comme pour la définition de l'année, il n'existe pas de définition unique du mois lunaire, un ensemble de définitions conduisant à des durées proches selon le phénomène utilisé comme repère.
A lunar standstill or lunistice is when the moon reaches its furthest north or furthest south point during the course of a month (specifically a draconic month of about 27.2 days). The declination (a celestial coordinate measured as the angle from the celestial equator, analogous to latitude) at lunar standstill varies in a cycle 18.6 years long between 18.134° (north or south) and 28.725° (north or south), due to lunar precession. These extremes are called the minor and major lunar standstills.
vignette|redresse=1.62|Schéma du système Terre - Lune. Echelle de distance non respectée. L’orbite de la Lune autour de la Terre est effectuée en environ . La Lune la décrit à environ du centre de la Terre en moyenne, à la vitesse moyenne de . Elle diffère de la plupart des satellites naturels des autres planètes par son orbite plus proche du plan de l'écliptique que de l'équateur terrestre. Bien que globalement elliptique, l'orbite de la Lune présente de nombreuses irrégularités (connues sous le nom de perturbations), dont l'étude possède une très longue histoire.
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Institute of Electrical and Electronics Engineers2014