Julian year The Julian year, as used in astronomy and other sciences, is a time unit now defined as exactly 365.25 days of
SI seconds each ("
ephemeris days"). This is one meaning of the unit "year" used in various scientific contexts. The Julian century of ephemeris days and the Julian millennium of ephemeris days are used in astronomical calculations. Fundamentally, expressing a time interval in Julian years is a way to precisely specify an amount of time (not how many "real" years), for long time intervals where stating the number of ephemeris days would be unwieldy and unintuitive. By convention, the Julian year is used in the computation of the distance covered by a
light-year. In the
Unified Code for Units of Measure (but not according to the
International Union of Pure and Applied Physics or the
International Union of Geological Sciences, see below), the symbol 'a' (without subscript) always refers to the Julian year, 'aj', of exactly
seconds. : 365.25 d × = 1 a = 1 aj =
Ms The
SI multiplier prefixes may be applied to it to form "ka", "Ma", etc. Today the mean tropical year is defined as the period of time for the mean
ecliptic longitude of the Sun to increase by 360 degrees. Since the Sun's ecliptic longitude is measured with respect to the equinox, the tropical year comprises a complete cycle of the seasons and is the basis of
solar calendars such as the internationally used
Gregorian calendar. The modern definition of mean tropical year differs from the actual time between passages of, e.g., the northward equinox, by a minute or two, for several reasons explained below. Because of the Earth's
axial precession, this year is about 20 minutes shorter than the sidereal year. The mean tropical year is approximately 365 days, 5 hours, 48 minutes, 45 seconds, using the modern definition (= × = ). The length of the tropical year varies a bit over thousands of years because the rate of axial precession is not constant. The anomalistic year is the time taken for the Earth to complete one revolution with respect to its
apsides. The orbit of the Earth is elliptical; the extreme points, called apsides, are the
perihelion, where the Earth is closest to the Sun, and the
aphelion, where the Earth is farthest from the Sun. The anomalistic year is usually defined as the time between perihelion passages. Its average duration is 365.259636 days (365 d 6 h 13 min 52.6 s) (at the epoch J2011.0).
Draconic year The draconic year, draconitic year, eclipse year, or ecliptic year is the time taken for the Sun (as seen from the Earth) to complete one revolution with respect to the same
lunar node (a point where the Moon's orbit intersects the ecliptic). The year is associated with
eclipses: these occur only when both the Sun and the Moon are near these nodes; so eclipses occur within about a month of every half eclipse year. Hence there are two
eclipse seasons every eclipse year. The average duration of the eclipse year is : days (346 d 14 h 52 min 54 s) (at the epoch J2000.0). This term is sometimes erroneously used for the draconic or nodal period of
lunar precession, that is the period of a complete revolution of the Moon's ascending node around the ecliptic: Julian years ( days; at the epoch J2000.0).
Full moon cycle The
full moon cycle is the time for the Sun (as seen from the Earth) to complete one revolution with respect to the
perigee of the Moon's orbit. This period is associated with the apparent size of the
full moon, and also with the varying duration of the
synodic month. The duration of one full moon cycle is: : days (411 days 18 hours 49 minutes 35 seconds) (at the epoch J2000.0).
Lunar year The
lunar year comprises twelve full cycles of the phases of the Moon, as seen from Earth. It has a duration of approximately 354.37 days.
Muslims use this for religious purposes, including calculating the date of the
Hajj and the fasting month of
Ramadan, and thus also the
Eids. The
Jewish calendar is also mainly lunar, but with the addition of an intercalary lunar month once every two or three years, designed to keep the calendar broadly synchronous with the solar cycle. Thus, a lunar year on the Jewish (Hebrew) calendar consists of either twelve or thirteen lunar months.
Vague year The vague year, from or wandering year, is an integral approximation to the year equaling 365 days, which wanders in relation to more exact years. Typically the vague year is divided into 12
schematic months of 30 days each plus 5
epagomenal days. The vague year was used in the calendars of
Ethiopia,
Ancient Egypt,
Iran,
Armenia and in
Mesoamerica among the
Aztecs and
Maya. It is still used by many Zoroastrian communities.
Heliacal year A heliacal year is the interval between the
heliacal risings of a star. It differs from the
sidereal year for stars away from the
ecliptic due mainly to the
precession of the equinoxes.
Sothic year The
Sothic year is the heliacal year, the interval between heliacal risings, of the star
Sirius. It is currently less than the
sidereal year and its duration is very close to the Julian year of 365.25 days.
Gaussian year The
Gaussian year is the sidereal year for a planet of negligible mass (relative to the Sun) and unperturbed by other planets that is governed by the
Gaussian gravitational constant. Such a planet would be slightly closer to the Sun than Earth's mean distance. Its length is: : days (365 d 6 h 9 min 56 s).
Besselian year The
Besselian year is a tropical year that starts when the (fictitious) mean Sun reaches an ecliptic longitude of 280°. This is currently on or close to January 1. It is named after the 19th-century German astronomer and mathematician
Friedrich Bessel. The following equation can be used to compute the current Besselian epoch (in years): : B = 1900.0 + (Julian dateTT − ) / The TT subscript indicates that for this formula, the Julian date should use the
Terrestrial Time scale, or its predecessor,
ephemeris time.
Variation in the length of the year and the day The exact length of an astronomical year changes over time. • The positions of the equinox and solstice points with respect to the apsides of Earth's orbit change: the equinoxes and solstices move westward relative to the stars because of
precession, and the apsides move in the other direction because of the long-term effects of gravitational pull by the other planets. Since the speed of the Earth varies according to its position in its orbit as measured from its perihelion, Earth's speed when in a solstice or equinox point changes over time: if such a point moves toward perihelion, the interval between two passages decreases a little from year to year; if the point moves towards aphelion, that period increases a little from year to year. So a "tropical year" measured from one passage of the northward ("vernal") equinox to the next, differs from the one measured between passages of the southward ("autumnal") equinox. The average over the full orbit does not change because of this, so the length of the average tropical year does not change because of this second-order effect. • Each planet's movement is perturbed by the gravity of every other planet. This leads to short-term fluctuations in its speed, and therefore its period from year to year. Moreover, it causes long-term changes in its orbit, and therefore also long-term changes in these periods. •
Tidal drag between the Earth and the Moon and Sun increases the length of the day and of the month (by transferring angular momentum from the rotation of the Earth to the revolution of the Moon); since the apparent mean solar day is the unit with which we measure the length of the year in civil life, the length of the year appears to decrease. The rotation rate of the Earth is also changed by factors such as
post-glacial rebound and
sea level rise. Numerical value of year variation Mean year lengths in this section are calculated for 2000, and differences in year lengths, compared to 2000, are given for past and future years. In the tables a day is SI seconds long.
Summary Some of the year lengths in this table are in average
solar days, which are slowly getting longer (at a rate that cannot be exactly predicted in advance) and are now around
SI seconds. An average Gregorian year may be said to be 365.2425
days (52.1775
weeks, and if an hour is defined as one twenty-fourth of a day,
hours,
minutes or
seconds). Note however that in absolute time the average Gregorian year is not adequately defined unless the period of the averaging (start and end dates) is stated, because each period of 400 years is longer (by more than 1000 seconds) than the preceding one as the rotation of the Earth slows. In this calendar, a common year is 365 days ( hours, minutes or seconds), and a leap year is 366 days ( hours, minutes or seconds). The 400-year civil cycle of the Gregorian calendar has days and hence exactly weeks. == Greater astronomical years ==