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A Day Is Not Exactly 24 Hours

Exact Day Length* — sam 4 avr 2026

Today's prediction: 24 hours, 0 minutes, 0,0004458 seconds (0,4458 milliseconds)

Yesterday: 24 hours, 0 minutes, 0,0006971 seconds (0,6971 milliseconds)

At the start of today, UT1 was 0.0485894 seconds ahead of UTC.

* Based on mean solar day. Numbers provided by the International Earth Rotation and Reference System Service (IERS).

Star trails over an observatory.

The Earth's rotation slows down over time.

©iStockphoto.com/nukleerkedi

Earth's Rotation Defines Length of Day

Modern timekeeping defines a day as the sum of 24 hours—but that is not entirely correct. The Earth's rotation is not constant, so in terms of solar time, most days are a little longer or shorter than that.

The Moon is—very gradually—slowing the Earth's rotation because of friction produced by tides. Over the course of a century, the length of a day increases by a couple of milliseconds (where 1 millisecond equals 0.001 seconds).

Within this general trend, however, there is fluctuation: sometimes the Earth spins a bit faster, sometimes a bit slower. Recently, our planet has been speeding up a little, making for slightly shorter days.

How Long Is Today?

Today is predicted to be 0,4458 ms (milliseconds) or 0,0004458 seconds longer than 24 hours. This is the time it takes Earth to rotate 20,73 cm (8,16 in), as measured at the equator.

This means that today lasts:

  • 24,0000001238 hours or
  • 24 hours and 0,45 ms

On average, a mean solar day in the last 365 days was -0,03 ms under 24 hours, so today's day length is above average. Over this period, 83 days have been longer than today, while 283 have been shorter than today.

If every day were as long as today, a leap second would have to be added every 2243,16 days.

Today's Day Length* in Context
 Day lengthDate
Yesterday24 hours +0,70 msven 3 avr 2026
Today24 hours +0,45 mssam 4 avr 2026
Tomorrow24 hours +0,28 msdim 5 avr 2026
Shortest 202624 hours -0,61 mssam 17 jan 2026
Longest 202624 hours +1,19 msjeu 19 mar 2026
Last Year Average24 hours -0,08 msYear 2025
* The figures for today and tomorrow are predictions. The shortest and longest day lengths are for the year so far (up to and including today).

Average Day Lengths & Leap Seconds

Overall, the Earth is a good timekeeper: the length of a day is consistently within a few milliseconds of 86,400 seconds, which is equivalent to 24 hours. However, over the course of months and years, these small differences can add up and put our clocks out of sync with the Earth's spin. When this happens, a leap second is used to bring them back into alignment.

Leap seconds can be positive or negative. A positive leap second adds a second to our clocks, while a negative leap second subtracts a second.

The system of leap seconds was introduced in 1972. So far, there have been 27 leap seconds, and they have all been positive. The table below shows the yearly average day lengths since 1973.

Average Solar Day Length*
YearAverage dayTotal yearly differenceShortest dayLongest dayLeap second added
2026+0,27 ms+25,64 ms17 jan -0,61 ms19 mar +1,19 ms-
2025-0,08 ms-27,93 ms10 juil -1,37 ms30 nov +1,14 ms-
2024-0,10 ms-37,25 ms5 juil -1,66 ms11 mar +1,28 ms-
2023-0,08 ms-28,61 ms16 juil -1,31 ms15 mai +1,32 ms-
2022-0,25 ms-90,78 ms30 juin -1,59 ms5 nov +1,02 ms-
2021-0,18 ms-65,17 ms9 juil -1,47 ms26 avr +0,99 ms-
2020-0,00 ms-1,28 ms19 juil -1,47 ms8 avr +1,62 ms-
2019+0,39 ms+141,25 ms16 juil -0,95 ms22 mar +1,68 ms-
2018+0,69 ms+252,47 ms30 juin -0,64 ms4 fév +1,69 ms-
2017+1,03 ms+375,01 ms4 aoû +0,06 ms25 avr +2,20 ms-
2016+1,34 ms+490,76 ms18 juil -0,03 ms10 mar +2,49 ms31 déc
2015+1,25 ms+458,03 ms17 juin +0,19 ms26 oct +2,31 ms30 juin
2014+0,99 ms+362,96 ms24 juil +0,02 ms26 avr +2,02 ms-
2013+1,02 ms+373,99 ms6 juil -0,35 ms28 mar +1,97 ms-
2012+0,83 ms+304,11 ms16 juil -0,35 ms5 avr +1,87 ms30 juin
2011+0,76 ms+277,94 ms27 juil -0,34 ms14 mai +1,85 ms-
2010+0,70 ms+254,74 ms23 juil -0,76 ms1 mar +2,09 ms-
2009+0,80 ms+293,37 ms6 juil -0,43 ms22 avr +1,81 ms-
2008+0,87 ms+319,49 ms16 juil -0,41 ms5 avr +1,91 ms31 déc
2007+0,85 ms+310,81 ms27 juil -0,63 ms16 avr +2,31 ms-
2006+0,82 ms+300,88 ms12 juin -0,40 ms7 oct +2,26 ms-
2005+0,43 ms+157,76 ms5 juil -1,05 ms27 fév +1,73 ms31 déc
2004+0,31 ms+114,01 ms15 juil -1,05 ms5 avr +1,56 ms-
2003+0,27 ms+100,16 ms13 juil -0,96 ms19 mar +1,55 ms-
2002+0,48 ms+173,79 ms6 aoû -0,74 ms2 mar +1,66 ms-
2001+0,57 ms+208,94 ms2 aoû -0,71 ms11 mar +1,64 ms-
2000+0,72 ms+262,42 ms11 aoû -0,25 ms26 oct +1,58 ms-
1999+0,99 ms+361,19 ms30 juin -0,13 ms15 avr +1,93 ms-
1998+1,37 ms+501,72 ms9 juil +0,01 ms1 mar +2,66 ms31 déc
1997+1,84 ms+671,08 ms4 juil +0,52 ms6 avr +2,98 ms30 juin
1996+1,82 ms+666,37 ms10 aoû +0,67 ms12 mai +2,68 ms-
1995+2,31 ms+843,66 ms25 juil +0,81 ms17 mar +3,29 ms31 déc
1994+2,19 ms+800,86 ms6 juil +0,86 ms27 fév +3,36 ms30 juin
1993+2,36 ms+862,66 ms17 juil +1,25 ms2 mai +3,49 ms30 juin
1992+2,22 ms+812,25 ms12 juil +0,84 ms18 mar +3,59 ms30 juin
1991+2,04 ms+743,88 ms27 juin +0,79 ms1 mar +3,00 ms-
1990+1,95 ms+710,04 ms20 juil +0,63 ms26 mar +3,28 ms31 déc
1989+1,52 ms+555,00 ms2 juil +0,25 ms10 nov +2,82 ms31 déc
1988+1,31 ms+480,30 ms12 juil -0,09 ms20 fév +2,76 ms-
1987+1,36 ms+497,35 ms23 juil -0,06 ms1 mar +2,67 ms31 déc
1986+1,24 ms+451,06 ms2 aoû -0,04 ms23 avr +2,30 ms-
1985+1,45 ms+528,83 ms16 juil +0,11 ms9 mar +2,64 ms30 juin
1984+1,51 ms+554,42 ms12 juil +0,16 ms18 mar +2,77 ms-
1983+2,28 ms+832,08 ms23 juil +1,01 ms1 fév +3,57 ms30 juin
1982+2,16 ms+789,64 ms2 aoû +0,84 ms23 avr +3,14 ms30 juin
1981+2,15 ms+786,03 ms16 juil +0,82 ms8 mar +3,42 ms30 juin
1980+2,30 ms+842,04 ms8 aoû +1,34 ms23 oct +3,24 ms-
1979+2,61 ms+953,02 ms23 juil +1,46 ms27 mar +3,65 ms31 déc
1978+2,88 ms+1051,83 ms31 juil +1,49 ms9 mar +3,83 ms31 déc
1977+2,77 ms+1012,60 ms14 juil +1,46 ms4 avr +3,72 ms31 déc
1976+2,91 ms+1064,67 ms26 juin +1,87 ms21 oct +3,90 ms31 déc
1975+2,69 ms+980,87 ms20 juil +1,54 ms1 nov +3,72 ms31 déc
1974+2,72 ms+991,99 ms30 juil +1,57 ms5 avr +3,79 ms31 déc
1973+3,04 ms+1106,21 ms2 jan +0,00 ms2 avr +4,03 ms31 déc
* For the current year, the average day length and total yearly difference are predictions; the shortest and longest day lengths are for the year so far (up to and including today).
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How Is True Day Length Measured?

Astronomers and timekeepers express mean solar time as Universal Time (UT1), a time standard based on the average speed of the Earth's rotation. UT1 is then compared to International Atomic Time (TAI), a super-precise time scale calculated by a network of atomic clocks.

The actual length of a day is expressed as the deviation of UT1 from TAI over 24 hours.

People in Grand Central Terminal by the Golden Clock.
Why Telling Time Is Complicated

The quirks and challenges behind keeping the world on schedule.

Why Isn't Earth's Rotation Constant?

The speed of the Earth's rotation varies from day to day. One of the main factors are the celestial bodies surrounding us.

For example, the Moon's gravitational pull causes tides and changes the Earth's shape, ultimately resulting in a lower rotational speed. The distance between Earth and Moon changes constantly, which makes for daily variations in the speed our planet rotates around its axis.

Find Day Length for Any Date

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How Far Back Does the Data Go?

Super-accurate atomic clocks were first developed in the 1950s and 1960s. So measurements of the Earth's rotation using atomic clocks only go back as far as then.

However, telescopic timings of stellar occultations by the Moon provide information about the Earth's rotation going back to the 17th century. An occultation is when the Moon, as seen from the Earth, passes in front of a star.

Illustration image
Illustration image

This chart, produced using data from the IERS, shows the length of day going back to 1830. It indicates that Earth was spinning particularly fast around the year 1870, and particularly slow around the start of the 1900s.

©timeanddate.com

Ancient Records Give Away Earth's Speed

Going back even further, records of solar and lunar eclipses provide information from the 8th century BCE onwards.

For example, a Babylonian clay tablet tells us that a total solar eclipse was observable in the ancient city of Babylon on April 15, 136 BCE.

Modern computer models can calculate the path of totality for this eclipse with a high degree of accuracy. From this, we can work out the Earth's spin. For instance, if the Earth had been spinning a bit faster at that time, the path of totality would have passed to the west of Babylon—not directly over the city.

Topics: Earth, Timekeeping, Astronomy