Calculation of elapsed time by the apparent position of the sun
On aprograde planet like theEarth, thesidereal day is shorter than thesolar day. At time 1, theSun and a certain distantstar are both overhead. At time 2, the planet has rotated 360° and the distant star is overhead again (1→2 = one sidereal day). But it is not until a little later, at time 3, that the Sun is overhead again (1→3 = one solar day). More simply, 1→2 is a completerotation of the Earth, but because the revolution around the Sun affects theangle at which the Sun is seen from the Earth, 1→3 is how long it takesnoon to return. [Note that in this diagram, the relative motion, and corresponding angles, are highly exaggerated for illustrative purposes.]
The Earth's orbit around the Sun, showing its eccentricity
A tall pole vertically fixed in the ground casts a shadow on any sunny day. At one moment during the day, the shadow will point exactly north or south (or disappear when and if the Sun moves directly overhead). That instant is calledlocal apparent noon, or 12:00 local apparent time. About 24 hours later the shadow will again point north–south, the Sun seeming to have covered a 360-degree arc around Earth's axis. When the Sun has covered exactly 15 degrees (1/24 of a circle, both angles being measured in a plane perpendicular to Earth's axis), local apparent time is 13:00 exactly; after 15 more degrees it will be 14:00 exactly.
The problem is that in September the Sun takes less time (as measured by an accurate clock) to make an apparent revolution than it does in December; 24 "hours" of solar time can be 21 seconds less or 29 seconds more than 24 hours of clock time. This change is quantified by theequation of time, and is due to theeccentricity of Earth's orbit (as in, Earth's orbit is not perfectly circular, meaning that the Earth–Sun distance varies throughout the year), and the fact that Earth's axis is not perpendicular to the plane of its orbit (the so-calledobliquity of the ecliptic).
The effect of this is that a clock running at a constant rate – e.g. completing the same number of pendulum swings in each hour – cannot follow the actual Sun; instead it follows an imaginary "mean Sun" that moves along the celestial equator at a constant rate that matches the real Sun's average rate over the year.[2] This is "mean solar time", which is still not perfectly constant from one century to the next but is close enough for most purposes. As of 2008[update], a mean solar day is about 86,400.002SI seconds, i.e., about 24.0000006 hours.[3]
Theapparent sun is the true sun as seen by an observer on Earth.[4]Apparent solar time ortrue solar time[a] is based on the apparent motion of the actualSun. It is based on theapparent solar day, the interval between two successive returns of the Sun to the localmeridian.[5][6] Apparent solar time can be crudely measured by asundial.[b]
The length of a solar day varies through the year, and the accumulated effect produces seasonal deviations of up to 16 minutes from the mean. The effect has two main causes. First, due to the eccentricity ofEarth's orbit, Earth moves faster when it is nearest the Sun (perihelion) and slower when it is farthest from the Sun (aphelion) (seeKepler's laws of planetary motion). Second, due to Earth'saxial tilt (known as theobliquity of theecliptic), the Sun's annual motion is along agreat circle (theecliptic) that is tilted to Earth'scelestial equator. When the Sun crosses the equator at bothequinoxes, the Sun's daily shift (relative to the background stars) is at an angle to the equator, so the projection of this shift onto the equator is less than itsaverage for the year; when the Sun is farthest from the equator at bothsolstices, the Sun's shift in position from one day to the next is parallel to the equator, so the projection onto the equator of this shift is larger than the average for the year (seetropical year). In June and December when the sun is farthest from the celestial equator, a given shift along the ecliptic corresponds to a large shift at the equator. Therefore, apparent solar days are shorter in March and September than in June or December.
The equation of time—above the x-axis a sundial will appearfast relative to a clock showing local mean time, and below the axis a sundial will appearslow.
Mean solar time is thehour angle of themean position of the Sun, plus 12 hours. This 12 hour offset comes from the decision to make each day start at midnight for civil purposes, whereas the hour angle or the mean sun is measured from the local meridian.[10] As of 2009[update], this is realized with theUT1 time scale, constructed mathematically fromvery-long-baseline interferometry observations of thediurnal motions of radio sources located in other galaxies, and other observations.[11]: 68, 326 [12] The duration of daylight varies during the year but the length of amean solar day is nearly constant, unlike that of an apparent solar day.[13] An apparent solar day can be 20 seconds shorter or 30 seconds longer than a mean solar day.[9][14] Long or short days occur in succession, so the difference builds up until mean time is ahead of apparent time by about 14 minutes near February 6, and behind apparent time by about 16 minutes near November 3. Theequation of time is this difference, which is cyclical and does not accumulate from year to year.
Mean time follows the mean sun.Jean Meeus describes the mean sun as follows:
Consider a first fictitious Sun travelling along theecliptic with a constant speed and coinciding with the true sun at the perigee and apogee (when the Earth is in perihelion and aphelion, respectively). Then consider a second fictitious Sun travelling along thecelestial equator at a constant speed and coinciding with the first fictitious Sun at the equinoxes. This second fictitious sun is themean Sun.[15]
The length of the mean solar day is slowly increasing due to thetidal acceleration of the Moon by Earth and the corresponding slowing of Earth's rotation by the Moon.
The sun has always been visible in the sky, and its position forms the basis of apparent solar time, the timekeeping method used in antiquity. An Egyptianobelisk constructed c. 3500 BC,[16] agnomon in China dated 2300 BC,[17] and an Egyptiansundial dated 1500 BC[18] are some of the earliest methods for measuring the sun's position.
Babylonian astronomers knew that the hours of daylight varied throughout the year. A tablet from 649 BC shows that they used a 2:1 ratio for the longest day to the shortest day, and estimated the variation using a linear zigzag function.[19] It is not clear if they knew of the variation in the length of the solar day and the correspondingequation of time.Ptolemy clearly distinguishes the mean solar day and apparent solar day in hisAlmagest (2nd century), and he tabulated the equation of time in hisHandy Tables.[20]
Apparent solar time grew less useful as commerce increased and mechanical clocks improved. Mean solar time was introduced in almanacs in England in 1834 and in France in 1835. Because the sun was difficult to observe directly due to its large size in the sky, mean solar time was determined as a fixed ratio of time as observed by the stars, which used point-like observations. A specific standard for measuring "mean solar time" from midnight came to be called Universal Time.[11]: 9–11
ConceptuallyUniversal Time is the rotation of the Earth with respect to the sun and hence is mean solar time. However, UT1, the version in common use since 1955, uses a slightly different definition of rotation that corrects for the motion of Earth's poles as it rotates. The difference between this corrected mean solar time andCoordinated Universal Time (UTC) determines whether aleap second is needed. (Since 1972 the UTC time scale has run onSI seconds, and the SI second, when adopted, was already a little shorter than the current value of the second of mean solar time.[21][11]: 227–231 )
^'apparent' is commonly used in English-language sources, but 'true' is used in French astronomical literature and has become nearly as common in English sources. See:
^Yallop, B. D.; Hohenker, C. Y. (August 1989)."Astronomical Information Sheet No. 58"(PDF).HM Nautical Almanac Office. Solar Location Diagram. Archived fromthe original(PDF) on December 23, 2022. RetrievedJune 17, 2022.
^Hilton, James L;McCarthy, Dennis D. (2013). "Precession, Nutation, Polar Motion, and Earth Rotation". In Urban, Sean E.; Seidelmann, P. Kenneth (eds.).Explanatory Supplement to the Astronomical Almanac (3rd ed.). Mill Valley, CA: University Science Books.ISBN978-1-891389-85-6.
^Neugebauer, Otto (1975),A History of Ancient Mathematical Astronomy, New York / Heidelberg / Berlin: Springer-Verlag, pp. 984–986,ISBN978-0-387-06995-1
^:(1) In "The Physical Basis of the Leap Second", by D D McCarthy, C Hackman and R A Nelson, in Astronomical Journal, vol.136 (2008), pages 1906-1908, it is stated (page 1908), that "the SI second is equivalent to an older measure of the second of UT1, which was too small to start with and further, as the duration of the UT1 second increases, the discrepancy widens." :(2) In the late 1950s, the cesium standard was used to measure both the current mean length of the second of mean solar time (UT2) (result: 9192631830 cycles) and also the second of ephemeris time (ET) (result:9192631770 ± 20 cycles), see"Time Scales", by L. EssenArchived October 19, 2008, at theWayback Machine, in Metrologia, vol.4 (1968), pp.161-165, on p.162. As is well known, the 9192631770 figure was chosen for theSI second. L Essen in the same 1968 article (p.162) stated that this "seemed reasonable in view of the variations in UT2".