Orbital eccentricity
The orbital eccentricity of an astronomical object is a parameter that determines the amount by which its orbit around another body deviates from a perfect circle. A value of 0 is a circular orbit, values between 0 and 1 form an elliptical orbit, 1 is a parabolic escape orbit, and greater than 1 is a hyperbola. The term derives its name from the parameters of conic sections, as every Kepler orbit is a conic section. It is normally used for the isolated twobody problem, but extensions exist for objects following a rosette orbit through the galaxy.
Definition
In a twobody problem with inversesquarelaw force, every orbit is a Kepler orbit. The eccentricity of this Kepler orbit is a nonnegative number that defines its shape.
The eccentricity may take the following values:
 circular orbit: e = 0
 elliptic orbit: 0 < e < 1 (see ellipse)
 parabolic trajectory: e = 1 (see parabola)
 hyperbolic trajectory: e > 1 (see hyperbola)
The eccentricity e is given by
where E is the total orbital energy, L is the angular momentum, m_{red} is the reduced mass, and α the coefficient of the inversesquare law central force such as gravity or electrostatics in classical physics:

 (α is negative for an attractive force, positive for a repulsive one; see also Kepler problem)
or in the case of a gravitational force:
where ε is the specific orbital energy (total energy divided by the reduced mass), μ the standard gravitational parameter based on the total mass, and h the specific relative angular momentum (angular momentum divided by the reduced mass).
For values of e from 0 to 1 the orbit's shape is an increasingly elongated (or flatter) ellipse; for values of e from 1 to infinity the orbit is a hyperbola branch making a total turn of 2 arccsc e, decreasing from 180 to 0 degrees. The limit case between an ellipse and a hyperbola, when e equals 1, is parabola.
Radial trajectories are classified as elliptic, parabolic, or hyperbolic based on the energy of the orbit, not the eccentricity. Radial orbits have zero angular momentum and hence eccentricity equal to one. Keeping the energy constant and reducing the angular momentum, elliptic, parabolic, and hyperbolic orbits each tend to the corresponding type of radial trajectory while e tends to 1 (or in the parabolic case, remains 1).
For a repulsive force only the hyperbolic trajectory, including the radial version, is applicable.
For elliptical orbits, a simple proof shows that arcsin() yields the projection angle of a perfect circle to an ellipse of eccentricity e. For example, to view the eccentricity of the planet Mercury (e = 0.2056), one must simply calculate the inverse sine to find the projection angle of 11.86 degrees. Next, tilt any circular object (such as a coffee mug viewed from the top) by that angle and the apparent ellipse projected to your eye will be of that same eccentricity.
Etymology
From Medieval Latin eccentricus, derived from Greek ἔκκεντρος ekkentros "out of the center", from ἐκ ek, "out of" + κέντρον kentron "center". Eccentric first appeared in English in 1551, with the definition "a circle in which the earth, sun. etc. deviates from its center." Five years later, in 1556, an adjective form of the word was added.
Calculation
The eccentricity of an orbit can be calculated from the orbital state vectors as the magnitude of the eccentricity vector:
where:
 e is the eccentricity vector.
For elliptical orbits it can also be calculated from the periapsis and apoapsis since r_{p} = a(1 − e) and r_{a} = a(1 + e), where a is the semimajor axis.
where:
 r_{a} is the radius at apoapsis (i.e., the farthest distance of the orbit to the center of mass of the system, which is a focus of the ellipse).
 r_{p} is the radius at periapsis (the closest distance).
The eccentricity of an elliptical orbit can also be used to obtain the ratio of the periapsis to the apoapsis:
Examples
Object  eccentricity 

Triton  0.00002 
Venus  0.0068 
Neptune  0.0086 
Earth  0.0167 
Titan  0.0288 
Uranus  0.0472 
Jupiter  0.0484 
Saturn  0.0541 
Moon  0.0549 
1 Ceres  0.0758 
4 Vesta  0.0887 
Mars  0.0934 
10 Hygiea  0.1146 
Makemake  0.1559 
Haumea  0.1887 
Mercury  0.2056 
2 Pallas  0.2313 
Pluto  0.2488 
3 Juno  0.2555 
324 Bamberga  0.3400 
Eris  0.4407 
Nereid  0.7507 
Sedna  0.8549 
Halley's Comet  0.9671 
Comet HaleBopp  0.9951 
Comet IkeyaSeki  0.9999 
The eccentricity of the Earth's orbit is currently about 0.0167; the Earth's orbit is nearly circular. Venus and Neptune have even lower eccentricity. Over hundreds of thousands of years, the eccentricity of the Earth's orbit varies from nearly 0.0034 to almost 0.058 as a result of gravitational attractions among the planets (see graph).^{[1]}
The table lists the values for all planets and dwarf planets, and selected asteroid, comets and moons. Mercury has the greatest orbital eccentricity of any planet in the Solar System (e = 0.2056). Such eccentricity is sufficient for Mercury to receive twice as much solar irradiation at perihelion compared to aphelion. Before its demotion from planet status in 2006, Pluto was considered to be the planet with the most eccentric orbit (e = 0.248). Other TransNeptunian objects have significant eccentricity, notably the dwarf planet Eris (0.44). Even further out, Sedna, has an extremely high eccentricity of due to its estimated aphelion of 937 0.855 AU and perihelion of about 76 AU.
Most of the Solar System's asteroids have orbital eccentricities between 0 and 0.35 with an average value of 0.17.^{[2]} Their comparatively high eccentricities are probably due to the influence of Jupiter and to past collisions.
The Moon's value is 0.0549, the most eccentric of the large moons of the Solar System. The four Galilean moons have eccentricity < 0.01. Neptune's largest moon Triton has an eccentricity of ×10^{−5} ( 1.6016),^{[3]} the smallest eccentricity of any known body in the Solar System; its orbit is as close to a perfect circle as can be currently measured. However, smaller moons, particularly 0.000irregular moons, can have significant eccentricity, such as Neptune's third largest moon Nereid (0.75).
Comets have very different values of eccentricity. Periodic comets have eccentricities mostly between 0.2 and 0.7,^{[4]} but some of them have highly eccentric elliptical orbits with eccentricities just below 1, for example, Halley's Comet has a value of 0.967. Nonperiodic comets follow nearparabolic orbits and thus have eccentricities even closer to 1. Examples include Comet Hale–Bopp with a value of 0.995^{[5]} and comet C/2006 P1 (McNaught) with a value of 019.^{[6]} As Hale–Bopp's value is less than 1, its orbit is elliptical and it will in fact return.^{[5]} Comet McNaught has a 1.000hyperbolic orbit while within the influence of the planets, but is still bound to the Sun with an orbital period of about 10^{5} years.^{[7]} As of a 2010 Epoch, Comet C/1980 E1 has the largest eccentricity of any known hyperbolic comet with an eccentricity of 1.057,^{[8]} and will leave the Solar System indefinitely.
Mean eccentricity
The mean eccentricity of an object is the average eccentricity as a result of perturbations over a given time period. Neptune currently has an instant (current Epoch) eccentricity of 0.0113,^{[9]} but from 1800 to 2050 has a mean eccentricity of 59.^{[10]} 0.008
Climatic effect
Orbital mechanics require that the duration of the seasons be proportional to the area of the Earth's orbit swept between the solstices and equinoxes, so when the orbital eccentricity is extreme, the seasons that occur on the far side of the orbit (aphelion) can be substantially longer in duration. Today, northern hemisphere fall and winter occur at closest approach (perihelion), when the earth is moving at its maximum velocity—while the opposite occurs in the southern hemisphere. As a result, in the northern hemisphere, fall and winter are slightly shorter than spring and summer—but in global terms this is balanced with them being longer below the equator. In 2006, the northern hemisphere summer was 4.66 days longer than winter, and spring was 2.9 days longer than fall due to the Milankovitch cycles.^{[11]}^{[12]}
Apsidal precession also slowly changes the place in the Earth's orbit where the solstices and equinoxes occur. Note that this is a slow change in the orbit of the Earth, not the axis of rotation, which is referred to as axial precession (see Precession § Astronomy). Over the next 10,000 years, the northern hemisphere winters will become gradually longer and summers will become shorter. However, any cooling effect in one hemisphere is balanced by warming in the other, and any overall change will be counteracted by the fact that the eccentricity of Earth's orbit will be almost halved.^{[13]} This will reduce the mean orbital radius and raise temperatures in both hemispheres closer to the midinterglacial peak.
Exoplanets
Of the many exoplanets discovered, most exoplanets have a higher orbital eccentricity than our solar system. Exoplanets found with low orbital eccentricity, near circular orbits, are very close to its star and are tidal locked to the star, like planet Mercury. All eight planets in the Solar System have nearcircular orbits. The exoplanets discovered show that the solar system, with its unusually low eccentricity, is rare and unique.^{[14]} One theory attributes this low eccentricity to the high number of planets in the Solar System; another suggests it arose because of its unique asteroid belts. A few other multiplanetary systems have been found, but none resemble the solar system. The solar system has unique planetesimal systems, which led the planets to have nearcircular orbits. Solar planetesimal systems include the asteroid belt, Hilda family, Kuiper belt, Hills cloud, and the Oort cloud. The exoplanet solar systems discovered have either no planetesimal systems or one very large planetesimal system. Low eccentricity is needed for habitability, especially advanced life. High multiplicity planet systems are much more likely to have habitable exoplanets.^{[15]}^{[16]} The Grand tack hypothesis of the solar system also helps understand the nearcircular orbits of the solar system and the other unique features of the solar system.^{[17]}^{[18]}^{[19]}^{[20]}^{[21]}^{[22]}^{[23]} ^{[24]} ^{[25]}
See also
References
 ↑ A. Berger & M.F. Loutre (1991). "Graph of the eccentricity of the Earth's orbit". Illinois State Museum (Insolation values for the climate of the last 10 million years). Retrieved 20091217.
 ↑ Asteroids
 ↑ David R. Williams (22 January 2008). "Neptunian Satellite Fact Sheet". NASA. Retrieved 20091217.
 ↑ Lewis, John (2 December 2012). Physics and Chemistry of the Solar System. Academic Press. Retrieved 20150329.
 1 2 "JPL SmallBody Database Browser: C/1995 O1 (HaleBopp)" (20071022 last obs). Retrieved 20081205.
 ↑ "JPL SmallBody Database Browser: C/2006 P1 (McNaught)" (20070711 last obs). Retrieved 20091217.
 ↑ "Comet C/2006 P1 (McNaught)  facts and figures". Perth Observatory in Australia. 20070122. Retrieved 20110201.
 ↑ "JPL SmallBody Database Browser: C/1980 E1 (Bowell)" (19861202 last obs). Retrieved 20100322.
 ↑ Williams, David R. (20071129). "Neptune Fact Sheet". NASA. Retrieved 20091217.
 ↑ "Keplerian elements for 1800 A.D. to 2050 A.D.". JPL Solar System Dynamics. Retrieved 20091217. External link in
publisher=
(help)  ↑ Data from United States Naval Observatory
 ↑ Berger A.; Loutre M.F.; Mélice J.L. (2006). "Equatorial insolation: from precession harmonics to eccentricity frequencies" (PDF). Clim. Past Discuss. 2 (4): 519–533. doi:10.5194/cpd25192006.
 ↑ Arizona U., Long Term Climate
 ↑ exoplanets.org, ORBITAL ECCENTRICITES, by G.Marcy, P.Butler, D.Fischer, S.Vogt, 20 Sept 2003
 ↑ National Academy of Sciences of the United States of America, Astronomy, Exoplanet orbital eccentricity: Multiplicity relation and the Solar System, by Mary Anne Limbacha and Edwin L. Turnera, 2014 Dec 15
 ↑ Steward Observatory, University of Arizona, Tucson, Planetesimals in Debris Disks, by Andrew N. Youdin an dGeorge H. Rieke, 2015
 ↑ Zubritsky, Elizabeth. "Jupiter's Youthful Travels Redefined Solar System". NASA. Retrieved 4 November 2015.
 ↑ Sanders, Ray. "How Did Jupiter Shape Our Solar System?". Universe Today. Retrieved 4 November 2015.
 ↑ Choi, Charles Q. "Jupiter's 'Smashing' Migration May Explain Our Oddball Solar System". Space.com. Retrieved 4 November 2015.
 ↑ Davidsson, Dr. Björn J. R. "Mysteries of the asteroid belt". The History of the Solar System. Retrieved 7 November 2015.
 ↑ Raymond, Sean. "The Grand Tack". PlanetPlanet. Retrieved 7 November 2015.
 ↑ O'Brien, David P.; Walsh, Kevin J.; Morbidelli, Alessandro; Raymond, Sean N.; Mandell, Avi M. (2014). "Water delivery and giant impacts in the 'Grand Tack' scenario". Icarus. 239: 74–84. arXiv:1407.3290. Bibcode:2014Icar..239...74O. doi:10.1016/j.icarus.2014.05.009.
 ↑ Relative Likelihood for Life as a Function of Cosmic Time, Journal of Cosmology and Astroparticle Physics, by Abraham Loeb, Rafael Batista, and David Sloan, August 2016, doi:10.1088/14757516/2016/08/040
 ↑ HarvardSmithsonian Center for Astrophysics, "Is Earthly Life Premature from a Cosmic Perspective?", August 1, 2016
 ↑ Relative Likelihood, by Loeb, Batista, and Sloan
 Prussing, John E., and Bruce A. Conway. Orbital Mechanics. New York: Oxford University Press, 1993.
External links
 World of Physics: Eccentricity
 The NOAA page on Climate Forcing Data includes (calculated) data from Berger (1978), Berger and Loutre (1991). Laskar et al. (2004) on Earth orbital variations, Includes eccentricity over the last 50 million years and for the coming 20 million years.
 The orbital simulations by Varadi, Ghil and Runnegar (2003) provides series for Earth orbital eccentricity and orbital inclination.
 Kepler's Second law's simulation