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CHAPTER 18
TIME
TIME IN NAVIGATION
1800. Solar Time
Sun will be on the observer’s meridian again when the Earth
has moved to point C in its orbit. Thus, during the course of
a day the Sun appears to move eastward with respect to the
stars.
The apparent positions of the stars are commonly
reckoned with reference to an imaginary point called the
vernal equinox , the intersection of the celestial equator and
the ecliptic. The period of the Earth’s rotation measured
with respect to the vernal equinox is called a sidereal day .
The period with respect to the Sun is called an apparent
solar day .
When measuring time by the Earth’s rotation, using the
actual position of the Sun, or the apparent Sun, results in
apparent solar time . Use of the apparent Sun as a time ref-
erence results in time of non-constant rate for at least three
reasons. First, revolution of the Earth in its orbit is not con-
stant. Second, time is measured along the celestial equator
and the path of the real Sun is not along the celestial equa-
tor. Rather, its path is along the ecliptic, which is tilted at an
angle of 23
The Earth’s rotation on its axis causes the Sun and
other celestial bodies to appear to move across the sky from
east to west each day. If a person located on the Earth’s
equator measured the time interval between two successive
transits overhead of a very distant star, he would be
measuring the period of the Earth’s rotation. If he then
made a similar measurement of the Sun, the resulting time
would be about 4 minutes longer. This is due to the Earth’s
motion around the Sun, which continuously changes the
apparent place of the Sun among the stars. Thus, during the
course of a day the Sun appears to move a little to the east
among the stars, so that the Earth must rotate on its axis
through more than 360
°
in order to bring the Sun overhead
again.
See Figure 1800 . If the Sun is on the observer’s meridian
when the Earth is at point A in its orbit around the Sun, it will
not be on the observer’s meridian after the Earth has rotated
through 360
27' with respect to the celestial equator. Third,
rotation of the Earth on its axis is not constant.
°
Figure 1800. Apparent eastward movement of the Sun with respect to the stars.
275
because the Earth will have moved along its
orbit to point B. Before the Sun is again on the observer’s
meridian, the Earth must turn a little more on its axis. The
°
 
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276
TIME
To obtain a constant rate of time, we replace the appar-
ent Sun with a fictitious mean Sun . This mean Sun moves
eastward along the celestial equator at a uniform speed equal
to the average speed of the apparent Sun along the ecliptic.
This mean Sun, therefore, provides a uniform measure of
time which approximates the average apparent time. The
speed of the mean Sun along the celestial equator is 15
listed in the Almanac to find the dividing line marking where
the equation of time changes between positive and negative
values. Examine the trend of the values near this dividing line
to determine the correct sign for the equation of time.
°
per
Example 2: See Figure 1801 . Determine the time of the
upper meridian passage of the Sun on April 16, 1995.
Solution: From Figure 1801 , upper meridian passage
of the Sun on April 16, 1995, is given as 1200. The dividing
line between the values for upper and lower meridian
passage on April 16th indicates that the sign of the equation
of time changes between lower meridian passage and upper
meridian passage on this date; the question, therefore,
becomes: does it become positive or negative? Note that on
April 18, 1995, upper meridian passage is given as 1159,
indicating that on April 18, 1995, the equation of time is
positive. All values for the equation of time on the same side
of the dividing line as April 18th are positive. Therefore, the
equation of time for upper meridian passage of the Sun on
April 16, 1995 is (+) 00 m 05 s . Upper meridian passage,
therefore, takes place at 11 h 59 m 55 s .
hour of mean solar time.
1801. Equation of Time
Mean solar time ,or mean time as it is commonly
called, is sometimes ahead of and sometimes behind
apparent solar time. This difference, which never exceeds
about 16.4 minutes, is called the equation of time .
The navigator most often deals with the equation of time
when determining the time of upper meridian passage of the
Sun. The Sun transits the observer’s upper meridian at local
apparent noon . Were it not for the difference in rate between
the mean and apparent Sun, the Sun would be on the observer’s
meridian when the mean Sun indicated 1200 local time. The
apparent solar time of upper meridian passage, however, is
offset from exactly 1200 mean solar time. This time difference,
the equation of time at meridian transit, is listed on the right hand
daily pages of the Nautical Almanac .
The sign of the equation of time is negative if the time
of Sun’s meridian passage is earlier than 1200 and positive
if later than 1200. Therefore: Apparent Time = Mean Time
+ (equation of time).
SUN
MOON
Day
Eqn. of Time
Mer.
Mer. Pass.
00 h
12 h
Pass.
Upper Lower Age Phase
ms
ms
h
mh
mh
m d
16
00 02 00 05 12 00 00 26 12 55 16
17
00 13 00 20 12 00 01 25 13 54 17
18
00 27 00 33 11 59 02 25 14 55 18
Figure 1801. The equation of time for April 16, 17, 18, 1995.
Example 1: Determine the time of the Sun’s meridian
passage (Local Apparent Noon) on June 16, 1994.
Solution: See Figure 2008 in Chapter 20, the Nautical
Almanac’s right hand daily page for June 16, 1994. The
equation of time is listed in the bottom right hand corner of
the page. There are two ways to solve the problem,
depending on the accuracy required for the value of
meridian passage. The time of the Sun at meridian passage
is given to the nearest minute in the “Mer. Pass.”column.
For June 16, 1994, this value is 1201.
To determine the exact time of meridian passage, use
the value given for the equation of time. This value is listed
immediately to the left of the “Mer. Pass.” column on the
daily pages. For June 16, 1994, the value is given as 00 m 37 s .
Use the “12 h ” column because the problem asked for
meridian passage at LAN. The value of meridian passage
from the “Mer. Pass.” column indicates that meridian
passage occurs after 1200; therefore, add the 37 second
correction to 1200 to obtain the exact time of meridian
passage. The exact time of meridian passage for June 16,
1994, is 12 h 00 m 37 s .
To calculate latitude and longitude at LAN, the navigator
seldom requires the time of meridian passage to accuracies
greater than one minute. Therefore, use the time listed under
the “Mer. Pass.” column to estimate LAN unless extraordinary
accuracy is required.
1802. Fundamental Systems of Time
Atomic time is defined by the Systeme International
(SI) second, with a duration of 9,192,631,770 cycles of
radiation corresponding to the transition between two
hyperfine levels of the ground state of cesium 133.
International Atomic Time ( TAI ) is an international time
scale based on the average of a number of atomic clocks.
Universal time ( UT ) is counted from 0 hours at
midnight, with a duration of one mean solar day, averaging
out minor variations in the rotation of the Earth.
UT0 is the rotational time of a particular place of
observation, observed as the diurnal motion of stars or
extraterrestrial radio sources.
UT1 is computed by correcting UT0 for the effect of
polar motion on the longitude of the observer, and varies
because of irregularities in the Earth’s rotation.
Coordinated Universal Time ,or UTC , used as a
standard reference worldwide for certain purposes, is kept
The equation of time’s maximum value approaches
16 m 22 s in November.
If the Almanac lists the time of meridian passage as
1200, proceed as follows. Examine the equations of time
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TIME
277
within one second of TAI by the introduction of leap
seconds. It differs from TAI by an integral number of
seconds, but is always kept within 0.9 seconds of TAI.
Dynamical time has replaced ephemeris time in
theoretical usage, and is based on the orbital motions of the
Earth, Moon, and planets.
Terrestrial time ( TT ), also known as Terrestrial
Dynamical Time ( TDT ), is defined as 86,400 seconds on
the geoid.
Sidereal time is the hour angle of the vernal equinox,
and has a unit of duration related to the period of the Earth’s
rotation with respect to the stars.
Delta T is the difference between UT1 and TDT.
Dissemination of time is an inherent part of various
electronic navigation systems. The U.S. Naval Observatory
Master Clock is used to coordinate Loran signals, and GPS
signals have a time reference encoded in the data message.
GPS time is normally within 15 nanoseconds with SA off,
about 70 nanoseconds with SA on. One nanosecond (one
one-billionth of a second) of time is roughly equivalent to
one foot on the Earth for the GPS system.
1. Multiply the hours by 15 to obtain degrees of arc.
2. Divide the minutes of time by four to obtain
degrees.
3. Multiply the remainder of step 2 by 15 to obtain
minutes of arc.
4. Divide the seconds of time by four to obtain
minutes of arc
5. Multiply the remainder by 15 to obtain seconds of arc.
6. Add the resulting degrees, minutes, and seconds.
Example 1: Convert 14 h 21 m 39 s to arc.
Solution:
(1) 14 h
´
15
= 210
°
00' 00"
(2) 21 m
¸
4
= 005
°
00' 00" (remainder 1)
(3) 1
´
15
= 000
°
15' 00"
(4) 39 s
¸
4
= 000
°
09' 00" (remainder 3)
(5) 3
´
15
= 000
°
00' 45"
(6) 14 h 21 m 39 s
= 215
°
24' 45"
1803. Time and Arc
To convert arc to time:
One day represents one complete rotation of the Earth.
Each day is divided into 24 hours of 60 minutes; each
minute has 60 seconds.
Time of day is an indication of the phase of rotation of
the Earth. That is, it indicates how much of a day has
elapsed, or what part of a rotation has been completed.
Thus, at zero hours the day begins. One hour later, the Earth
has turned through 1/24 of a day, or 1/24 of 360
°
, or 360
°¸
1. Divide the degrees by 15 to obtain hours.
2. Multiply the remainder from step 1 by four to
obtain minutes of time.
3. Divide the minutes of arc by 15 to obtain minutes
of time.
4. Multiply the remainder from step 3 by four to
obtain seconds of time.
5. Divide the seconds of arc by 15 to obtain seconds
of time.
6. Add the resulting hours, minutes, and seconds.
°
Smaller intervals can also be stated in angular units;
since 1 hour or 60 minutes is equivalent to 15
°
of arc, 1
Example 2: Convert 215
°
24' 45" to time units.
minute of time is equivalent to 15
60 = 0.25
°
= 15' of arc,
and 1 second of time is equivalent to 15'
¸
60 = 0.25' = 15"
Solution:
of arc.
(1) 215
°¸
15
= 14 h 00 m 00 s
remainder 5
Summarizing in table form:
(2) 5
´
4
= 00 h 20 m 00 s
(3) 24'
¸
15
= 00 h 01 m 00 s
remainder 9
1 d
=24 h
=360
°
(4) 9
´
4
= 00 h 00 m 36 s
(5) 45"
¸
15
= 00 h 00 m 03 s
60 m
=1 h
=15
°
4 m
=1
°
=60'
(6) 215
°
24' 45" = 14 h 21 m 39 s
60 s
=1 m
= 15'
4 s
= 1'
= 60"
Solutions can also be made using arc to time conversion
tables in the almanacs. In the Nautical Almanac , the table
given near the back of the volume is in two parts, permitting
separate entries with degrees, minutes, and quarter minutes
of arc. This table is arranged in this manner because the
navigator converts arc to time more often than the reverse.
1 s
= 15"
= 0.25'
Therefore any time interval can be expressed as an
equivalent amount of rotation, and vice versa. Intercon-
version of these units can be made by the relationships
indicated above.
18'22" to time units, using the
Nautical Almanac arc to time conversion table.
°
To convert time to arc:
24 = 15
°¸
Example 3: Convert 334
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278
TIME
Solution:
exactly one hour. The time is changed as convenient,
usually at a whole hour, when crossing the boundary
between zones. Each time zone is identified by the number
of times the longitude of its zone meridian is divisible by
15
Convert the 22" to the nearest quarter minute of arc for
solution to the nearest second of time. Interpolate if more
precise results are required.
, positive in west longitude and negative in east
longitude . This number and its sign, called the zone
description (ZD) , is the number of whole hours that are
added to or subtracted from the zone time to obtain
Greenwich Mean Time (GMT). The mean Sun is the
celestial reference point for zone time. See Figure 1806.
Converting ZT to GMT, a positive ZT is added and a
negative one subtracted; converting GMT to ZT, a positive
ZD is subtracted, and a negative one added.
°
334
°
00.00 m
= h 16 m 00 s
000
°
18.25 m
= 00 h 01 m 13 s
334
°
18' 22"
= 22 h 17 m 13 s
1804. Time and Longitude
Suppose the Sun were directly over a certain point on
the Earth at a given time. An hour later the Earth would
have turned through 15
Example: The GMT is 15 h 27 m 09 s .
°
, and the Sun would then be directly
farther west. Thus, any difference of
longitude between two points is a measure of the angle
through which the Earth must rotate to separate them.
Therefore, places east of an observer have later time, and
those west have earlier time, and the difference is exactly
equal to the difference in longitude, expressed in time units.
The difference in time between two places is equal to the
difference of longitude between their meridians, expressed
in units of time instead of arc.
°
Required: (1) ZT at long. 156
°
24.4' W.
(2) ZT at long. 039
°
04.8' E.
Solutions:
(1)
GMT
15 h 27 m 09 s
ZD
+10 h (rev.)
ZT
05 h 27 m 09 s
1805. The Date Line
(2)
GMT
15 h 27 m 09 s
ZD
–03 h (rev.)
Since time grows later toward the east and earlier toward
the west of an observer, time at the lower branch of one’s
meridian is 12 hours earlier or later, depending upon the
direction of reckoning. A traveler circling the Earth gains or
loses an entire day depending on the direction of travel, and
only for a single instant of time, at precisely Greenwich
noon, is it the same date around the earth. To prevent the date
from being in error and to provide a starting place for each
new day, a date line is fixed by informal agreement. This line
coincides with the 180th meridian over most of its length. In
crossing this line, the date is altered by one day. If a person is
traveling eastward from east longitude to west longitude,
time is becoming later, and when the date line is crossed the
date becomes 1 day earlier. At any instant the date
immediately to the west of the date line (east longitude) is 1
day later than the date immediately to the east of the line.
When solving celestial problems, we convert local time to
Greenwich time and then convert this to local time on the
opposite side of the date line.
ZT
18 h 27 m 09 s
1807. Chronometer Time
Chronometer time (C) is time indicated by a
chronometer. Since a chronometer is set approximately to
GMT and not reset until it is overhauled and cleaned about
every 3 years, there is nearly always a chronometer error
(CE) , either fast (F) or slow (S). The change in chronometer
error in 24 hours is called chronometer rate ,or daily rate ,
and designated gaining or losing. With a consistent rate of 1 s
per day for three years, the chronometer error would total
approximately 18 m . Since chronometer error is subject to
change, it should be determined from time to time,
preferably daily at sea. Chronometer error is found by radio
time signal, by comparison with another timepiece of known
error, or by applying chronometer rate to previous readings of
the same instrument. It is recorded to the nearest whole or half
second. Chronometer rate is recorded to the nearest 0.1 second.
1806. Zone Time
Example: At GMT 1200 on May 12 the chronometer reads
12 h 04 m 21 s . At GMT 1600 on May 18 it reads 4 h 04 m 25 s .
At sea, as well as ashore, watches and clocks are
normally set to some form of zone time (ZT) . At sea the
nearest meridian exactly divisible by 15
is usually used as
the time meridian or zone meridian . Thus, within a time
zone extending 7.5
°
Required: . 1. Chronometer error at 1200 GMT May 12.
2. Chronometer error at 1600 GMT May 18.
3. Chronometer rate.
4. Chronometer error at GMT 0530, May 27.
on each side of the time meridian the
time is the same, and time in consecutive zones differs by
°
over a meridian 15
 
Figure 1806. Time Zone Chart.
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