Convert anomalistic month to Gaussian year


anomalistic month
Gaussian year


More information from the unit converter

How many anomalistic month in 1 Gaussian year? The answer is 13.255774392977. We assume you are converting between anomalistic month and Gaussian year. You can view more details on each measurement unit: anomalistic month or Gaussian year The SI base unit for time is the second. 1 second is equal to 4.2004220987365E-7 anomalistic month, or 3.1687489347752E-8 Gaussian year. Note that rounding errors may occur, so always check the results. Use this page to learn how to convert between months and years. Type in your own numbers in the form to convert the units!



Date difference between calendar days

You may also want to find out how many days are between two dates on the calendar. Use the date calculatorto get your age in days or measure the duration of an event.


Quick conversion chart of anomalistic month to Gaussian year

1 anomalistic month to Gaussian year = 0.07544 Gaussian year

10 anomalistic month to Gaussian year = 0.75439 Gaussian year

20 anomalistic month to Gaussian year = 1.50878 Gaussian year

30 anomalistic month to Gaussian year = 2.26316 Gaussian year

40 anomalistic month to Gaussian year = 3.01755 Gaussian year

50 anomalistic month to Gaussian year = 3.77194 Gaussian year

100 anomalistic month to Gaussian year = 7.54388 Gaussian year

200 anomalistic month to Gaussian year = 15.08776 Gaussian year


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Common time conversions


Definition: Month

An anomalistic month is the average time the Moon takes to go from perigee to perigee - the point in the Moon's orbit when it is closest to Earth. An anomalistic month is about 27.55455 days on average.


Definition: 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 365.2568983 days (365 d 6 h 9 min 56 s).


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