PH290 Astronomy
Practical TIME systems.
Knowing time is simple in everyday life. You look at a clock. You assume
that everyone else's clock in your time zone reads the same. And that's
that.
For astronomers, however, time can become quite complex. The reason is that
our units of time measurement - the day and its subdivisions of hour,
minute, and second - are based on astronomical phenomena that are
themselves more complex than you might at first think.
Most of these complications have been smoothed out of our everyday civil
time system by official edict. The result is a simple, easy-to-use
timekeeping arrangement that serves society well - as long as nobody looks
too closely at the sky. Do so, and all the carefully hidden fudge factors
erupt back into view.
Here, then, is a summary of the time systems that every physicist
should know.
Local Apparent Time (LAT)
also called apparent solar time or sundial time,
is what everyone used long ago when they told time by the Sun. Noon was what
most people still think is noon: when the Sun crosses the meridian - that
is, when the Sun is due south (for people at north temperate latitudes), at
its highest point of the day, and halfway between sunrise and sunset. The
very word "meridian" is from the Latin for "mid-day."
But when reasonably accurate clocks were invented, careful timekeepers
noticed that something was wrong with solar time. The Sun sometimes runs up
to 16 minutes fast in its daily travels across the sky, and sometimes as
much as 14 minutes slow, depending on the season.
This effect arises from the tilt of the Earth's axis and the ellipticity of
the Earth's orbit around the Sun. To escape the problem, our next time
system was invented.
Local Mean Time (LMT). Astronomers created an imaginary, well-behaved mean Sun that travels along the celestial equator at a uniform rate to make its annual circuit around the constellations. The mean Sun has the average or mean right ascension of the real Sun. Noon became the moment when the mean Sun crossed the meridian. The number of minutes the real Sun lags behind or runs ahead of the mean Sun was named the equation of time. Its value for any date can be looked up in an almanac or can be calculated (see the appropriate section of Roy and Clarke).
But this adjustment wasn't enough. An even worse problem results from the
fact that the Earth is round.
Standard time.
Because the Earth's surface curves, ``overhead" at your
location is a different direction than ``overhead" just a few miles away.
Similarly, when the Sun or a star is on your meridian it has not yet reached
the meridian of someone to your west, and it has already crossed the
meridian of someone to your east.
At
latitude the difference amounts to one minute of time for
every 13 miles east or west. To a person watching the sky 13 miles west of you,
the time seems to be 11:59 when you swear it's 12:00 and someone 13 miles east
insists it's 12:01. This is why Local Mean Time is local. It depends on your
location.
This didn't matter when travel and communication were slow. The problem grew
more acute in the 19th century. The widespread use of telegraphs and
railways finally forced a change. How could you catch a train when every
town and every railway company kept a slightly different time?
In 1883 the United States was divided into standard time zones; the rest of
the world soon followed. In each zone, all clocks are set to the Local Mean
Time of a standard longitude:
west for Eastern Standard Time,
for Central,
for Mountain, and
for
Pacific. Each time zone differs from its neighbors by one hour because these
longitudes are
apart i.e. 1/24 of the way around the Earth.
Standard time was a great advance for society. But not for skywatchers.
Planispheres (star wheels) still work in Local Mean Time (LMT). So does
every all-sky map that shows horizons, such as the ones in astronomy texts
which show the``Local Time of Transit" scale of our Sun and Moon etc, and
and every other map, device, or calculation that
shows astronomical objects with respect to your horizon, zenith, or meridian
without taking your local longitude explicitly into account.
However, correcting for LMT is simple. For every degree you are west of your
time zone's standard longitude, add four minutes to LMT to get standard
time. For each degree you are east, subtract four minutes.
To get daylight saving time, of course, add an hour to standard time.
Universal Time (UT).
Standard time (and its daylight-saving variant) serves
fine within a given time zone. But when a time applies worldwide, such as in
an astronomical almanac, which time zone should be favoured?
Logically enough, the "universal" time zone that was agreed upon is that of
longitude. This longitude is, by definition, that of a line
engraved in a brass plate in the floor of the Old Royal Observatory at
Greenwich.
Hence UT was originally known as Greenwich Mean Time (GMT).
By tradition UT is stated in the 24-hour system, whereby noon is called
12:00, 1 p.m. is 13:00, 2 p.m. is 14:00, and so on. Midnight is called 0:00.
One of the first things a beginner must learn is how to turn UT into
standard time. It's easy. To get Eastern Standard Time, just subtract 5
hours from UT. For CST subtract 6 hours, for MST 7, for PST 8. Other time
zones have their relations to UT listed in many places. (To get daylight
saving time, remember to subtract one hour less than these values.)
Of course the date must be given in the same system as the time!! If you get
a negative time by subtracting from UT, add 24 hours. In this case the
result is on the date before the UT date. For instance, 2:00 April 15th UT
is 10:00 p.m. Eastern Daylight Time April 14th.
Many amateurs find it easiest just to remember when 0:00 UT (often written
0h) happens in their time zone. For example, 0h UT is 7 p.m. EST (8 p.m.
EDT) on the previous date.
Ephemeris Time or Dynamical Time. Once the worldwide system of time zones was in place, with UT proudly heading up the list, all should have been well forever after. But such was not to be. Astronomers working with solar system dynamics noticed something very disturbing. The day itself varies in length. The Earth's rotation slows down and speeds up by small amounts unpredictably, while undergoing a very long-term slowing trend. The gradual slowing is caused by the friction of tides raised by the Moon and Sun. Slow, irregular changes are thought to involve motions of material in the Earth's fluid interior. Changes in winds, air masses, snow packs, and other factors cause shorter-term variations. Faced with this problem, astronomers in 1960 instituted Ephemeris Time (ET). This time system runs perfectly steadily regardless of the Earth's rotation, almost as if the Earth didn't exist. It is used for most celestial calculations and almanac (ephemeris) predictions, especially those having to do with the motions of the Moon, planets, and other solar system bodies in space. Ephemeris Time matched UT around 1902. Since then UT has gradually drifted away from it, so that now (as of 1996) UT lags behind by about 62 seconds.
In 1984 ET was renamed Terrestrial Dynamical Time (TDT or TT); also created
was Barycentric Dynamical Time (TDB), which is referred to the solar
system's center of mass. For amateur purposes they can be considered
identical, since they differ by only milliseconds.
If you encounter a time given in ET or Dynamical Time, and if one-minute
accuracy matters, you need to know the difference from UT. Almanacs list
this difference, which is known as Delta T. Use the formula UT = Dynamical
Time - Delta T. It is impossible to forecast Delta T precisely because the
Earth's fitful rotation rate is too unpredictable.
Coordinated Universal Time (UTC). Civilization at large, not just astronomers, needs a smoothly running time system like Dynamical Time. But most of humanity is also tied to the natural cycle of the day, variable though it may be. What is done about this? Part of the solution has been to redefine the basic time unit, the second. No longer is a second exactly 1/86,400 of a mean solar day. Since 1967 the second has been defined as how long cesium-133 atoms take to emit 9,192,631,770 cycles of a certain microwave radiation in an atomic clock.
With the second no longer defined astronomically, the Earth can spin as it
pleases without upsetting the world's clocks. But there is a price to pay. A
day no longer has 24 hours. In 1983 there were an average of 24.00000063
hours in a day, and in 1986 there were 24.00000034.
To keep our clocks in close step with the turning of the Earth, a leap
second is inserted into Universal Time every year or so when required. A
leap second may be added at the end of June 30th or December 31st UT, giving
the last minute of the chosen day 61 seconds.
The result is Coordinated Universal Time or UTC (its acronym in French), the
system by which all the world's clocks are set. UTC is the basis for all
time-signal radio broadcasts and other time services. In non-astronomical
circles it is sometimes called World time, Z time, or Zulu.
But the occasional leap-second jerks in UTC go unfelt, of course, by the
Earth, planets, and stars. Almanac predictions given in "UT" are actually in
a system known as UT1, which is always within 0.9 second of UTC. Therefore,
when specifying "UT" to better than 1-second accuracy, you should state
whether you mean UTC or UT1 unless this is obvious from the context - such
as if the time came from a radio time-station signal.
There is also a UT0, which is nearly the same as UT1 but includes the tiny
effect of the Earth's crust moving with respect to its axis (polar motion),
and a UT2, which is obsolete.
Sidereal time.
This is simply the right ascension of stars on your local
meridian at any moment. Sidereal time runs about 4 minutes a day faster than
all the time systems described above. An old amateur astronomer's trick is
to adjust a wind-up clock to run 4 minutes a day fast, set it to local
sidereal time, and use it to tell what constellations are on the meridian
and what star charts to use. For instance if the clock reads 5:30 a.m.,
right ascension 5h 30m is on your meridian, and there you'll find Orion.
More useful information may be found in the RGO Web site, see eg.
Time.
For a further discussion of Sidereal Time
Click here.