Equation of Time (Fourier Series Approximation)

Also known as equation of time · sundial correction · apparent solar time minus mean solar time · sundial fast or slow · solar noon correction · NOAA equation of time · eqtime · Spencer equation of time · Fourier series equation of time · analemma time offset · why solar noon is not at twelve · true solar time correction · fractional year gamma

E=229.18(0.000075+0.001868cos⁡γ−0.032077sin⁡γ−0.014615cos⁡2γ−0.040849sin⁡2γ),γ=2πY(n−1+h−1224)E = 229.18\left(0.000075 + 0.001868\cos\gamma - 0.032077\sin\gamma - 0.014615\cos 2\gamma - 0.040849\sin 2\gamma\right), \quad \gamma = \frac{2\pi}{Y}\left(n - 1 + \frac{h - 12}{24}\right)
sig figs

Worked example: Wikipedia's extremes: 3 November (day 307), noon → +16 min 25 s = 16.417 min, within 0.75 min. Press Try an example to run it live, then adjust anything.

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See also

Longitude to Solar Time Difference: The other correction between solar time and clock time: 4 minutes for each degree of longitude from the zone's middle meridian.Solar Azimuth Angle (Compass Bearing of the Sun): Needs the hour angle, which is solar time less noon, so it is where this correction ends up.Solar Elevation Angle (Height of the Sun above the Horizon): The height of the Sun at a given solar time, which this correction turns into clock time.Day Length from Latitude and Solar Declination (Sunrise Equation): Gives the half-day length, which this page shifts by E to place sunrise and sunset on a clock.Solar Declination Angle (Cooper's Equation): The other quantity that swings through the year with the Sun's position, from the same fractional year.
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Equation of Time (Fourier Series Approximation) explained

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A sundial and a clock do not keep the same time. The equation of time EE is the difference between the time a sundial reads (apparent solar time) and the time a clock keeps (mean solar time). It is positive when the Sun is ahead of the clock, about +16 minutes in early November, and negative when it is behind, about -14 minutes in mid February. Two effects add up to it: Earth's orbit is an ellipse, so the Sun's apparent speed through the year changes, and the Sun travels along the ecliptic, which is tilted against the celestial equator.

This page does not compute those effects one by one. It uses the Fourier series in the fractional year that NOAA's Global Monitoring Laboratory prints in its General Solar Position Calculations note. The fractional year γ\gamma, in radians, is 2π/Y2\pi/Y times n−1+(h−12)/24n - 1 + (h-12)/24, where YY is the days in the year (365, or 366 in a leap year), nn the day of the year and hh the hour of the day. Then EE, in minutes, is 229.18 times a sum of five terms in cos⁡γ\cos\gamma, sin⁡γ\sin\gamma, cos⁡2γ\cos 2\gamma and sin⁡2γ\sin 2\gamma. The 229.18 is 1440/(2π)1440/(2\pi), the minutes in a day per radian, rounded as NOAA prints it. The hour moves the answer by at most about 30 seconds a day, so any clock will do for it.

This is a Fourier approximation, not a physical law and not an almanac. Measured here against an independent solar position calculation across 2003 and 2004, it stays within about 0.7 minute (about 40 seconds), and no worse than 0.75 minute in the 366-day year. At the instant of the worked example in NREL's Solar Position Algorithm report (17 October 2003, day 290, 19:30:30 universal time), it gives 14.88 minutes against the report's 14.6415, which is 14 seconds high. That is good enough to correct a sundial or to place solar noon to the minute, and not good enough for celestial navigation.

Two quick checks. At noon on 3 November (day 307) the series gives 16.37 minutes, against 16 min 25 s (16.417 minutes) in a rough published table of the extremes; at noon on 11 February (day 42) it gives -14.20 against -14 min 15 s. Both are well inside 0.75 minute. Solar noon on a mean-time clock at the middle meridian of a time zone falls at 12:00 less EE; at other longitudes the longitude page adds 4 minutes for each degree.

Equation of Time (Fourier Series Approximation)

E=229.18(0.000075+0.001868cos⁡γ−0.032077sin⁡γ−0.014615cos⁡2γ−0.040849sin⁡2γ),γ=2πY(n−1+h−1224)E = 229.18\left(0.000075 + 0.001868\cos\gamma - 0.032077\sin\gamma - 0.014615\cos 2\gamma - 0.040849\sin 2\gamma\right), \quad \gamma = \frac{2\pi}{Y}\left(n - 1 + \frac{h - 12}{24}\right)
Where
  • EE= Equation of time (min)
  • nn= Day of the year
  • hh= Hour of the day (h)
  • YY= Days in the year
Where this comes from
  • NOAA Global Monitoring Laboratory, "General Solar Position Calculations" (the Solar Calculator's equations note, a US federal work in the public domain): the fractional year gamma, the equation of time and declination as Fourier series in gamma, the true solar time, the hour angle ha = tst / 4 - 180, and the azimuth (degrees clockwise from north) by cos(180 - theta) = -[sin(lat) cos(zenith) - sin(decl)] / [cos(lat) sin(zenith)]. Read it
  • Reda, I., and Andreas, A. (2008). Solar Position Algorithm for Solar Radiation Applications, NREL/TP-560-34302 (revised January 2008), National Renewable Energy Laboratory, a US Department of Energy laboratory report available at no cost. Section 3.13 (topocentric local hour angle, equation 40), section 3.15 (equation 45, the astronomers' azimuth Gamma = atan2(sin H', cos H' sin phi - tan delta' cos phi), measured westward from south; equation 46, Phi = Gamma + 180, measured eastward from north), Appendix A.1 (equation of time, equation A1) and Appendix A.5 Table A5.1 (the worked example: 17 October 2003, 12:30:30 local standard time, time zone -7, latitude 39.742476, longitude -105.1786). Read it
Revised 31 October 2026
Cite this page

formula.expert. (2026, October 31). Equation of Time (Fourier Series Approximation) Calculator. https://formula.expert/solvers/equation-of-time-fourier-series