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The culmination
of a celestial body means that the body is at
its greatest altitude, whereas the transit
is the
passage of its center through the meridian.
Only the fixed stars culminate really in the meridian. The Sun, Moon, and the planets culminate out of the meridian. At midlatitudes (50°) the difference may be up to 18 seconds for the Sun, and more than 6 minutes for the Moon. To compute the difference in time between transit and culmination we start by the well known equation
^{(1)}
h = altitude
δ = declination Φ = latitude H = hour angle = Local Sidereal Time  Right Ascension Differentiating the above equation with respect to time: _{}
^{(2)}
At
the instant of culmination we have _{}.
If _{}
(constant declination) the culmination
is at H=0°.
For non constant declination the hour angle of culmination H_{C} is very small_{ } and we get as an
approximation of (2):
_{} ^{
(3)
}
The altitude at
culmination is by
∆h
greater
than the
altitude on the meridian:
^{
}_{}
(4)
The Sun
In
(3) the
derivative
_{} may
be replaced by differentiating the
classical equation
^{(5)}
β = ecliptic latitude
γ = obliquity of the ecliptic L = ecliptic longitude The ecliptic latitude β of the Sun is very small:  β <0.0002°, _{}, cos β=1, and therefore from (5): L =
heliocentric ecliptic longitude
H = hour angle = Local Sidereal Time  Right Ascension γ = obliquity of the ecliptic = 23.44° δ = declination Φ = latitude For the Sun the rates of change in time (derivatives) of L and H can be approximated by: For
equinoxes (δ=0°,
L=0°, L=180°) H_{K}
is an extremum:
_{} (7) At Φ = 40°
we get H_{C} =
9,14·10^{4} rad = 0,0524° = 0.210 min
= 12.6 s
At Φ = 50° we get H_{C} = 1,30·10^{3} rad = 0,0744° = 0.298 min = 17.9 s The altitude at culmination is only 0.14'' more than at transit. For solstices (L=90°, L=270°) H_{C} = 0. Between winter solstice and summer solstice culmination occurs later then transit, between summer solstice and winter solstice culmination occurs earlier then transit. horizontal
axis: day of the year
vertical axis: time difference in seconds between culmination and transit red: latitude Φ = 40°, blue: latitude Φ = 50°. ∆T = (48/PI)*(tanΦtanδ)*(vLatvDec) (8) On 2012,
Mar 20 at 05:14 UT (spring equinox):
∆T =
18.0 svLat = hourly latitude speed is arcminutes per hour = 0 (observer at rest) vDec = hourly declination change _{} is arcminutes per hour = 0,988 arcmin/hour δ = 0.0° at Φ = 50°: This
result agrees with (7).
*** The Moon The
orbital plane of the Moon is inclined (
β
< 5.1°)
aganst the ecliptic, and formula (6) is not
valid.
On 2024, Oct 15 at 50°N, 0°E (computed by MICA, Multiyear Interactive Computer Almanac by USNO) there is an extreme value of difference: culmination 22:31:14.5 UT transit 22:25:19.3 UT difference 5 min 55 s The result from calsky is 6 min 03 s. On 2024,
Oct 15 at 22:30 UT we apply the formula (3)
for the Moon using MICA:
_{} = dδ/dt = 0.303°/hour dH/dt = 14.56°/hour δ = 0.00° H_{C} = 0.0248 rad = 1.42° = 5.68 min H_{C}
= 5 min 41 s
∆T = [10800°/(PI*(dH/dt)^{2})]*(tanΦtanδ)*(vLatvDec) (9) ∆T =
difference is seconds of time between
culmination and meridian transit
∆H/dt = hourly change of hour angle, H in degrees vLat = hourly latitude speed of the observer is arcminutes per hour For the Moon: 14.38°/hour
< dH/dt
<
14.61°/hour
mean: 14.495°/hour = 360°/24h 50min 16.105
hour^{2}/° < 10800°/[PI*(dH/dt)^{2}]^{
}<
16.625 hour^{2}/°
mean: 10800°/[PI*(dH/dt)^{2}] = 16.365 hour^{2}/° On 2024, Oct 15 at 22:30 UT using MICA: vLat = 0 (observer is at rest) vDec = hourly declination change _{} in arcminutes per hour = 18.19 arcmin/hour = = (18.19/60) °/hour δ = 0.025° dH/dt = 14.49°/hour 10800°/[PI*(dH/dt)^{2}] = 16.37 hour^{2}/° = 16.37 hour·60 s/° ∆T =
355 s = 5 min 55 s
Vertical axis: Difference ∆T = t_{Trans}  t_{Culm} (minutes) at 50°N horizontal axis: day in MayJun 2012 computed by my Planet applet Urs Klaeger pointed out to me: With increasing declinations AND at geolatitudes north of the subsolar/sublunar point, Culmination is after Transit. Vice versa south of the Sun/Moon. Jean Meeus writes: If culmination occurs south of the zenith and ∆δ is positive, the highest altitude is reached after the meridian passage; if the culmination occurs between the pole and the zenith, the situation is reversed. („More Mathematical Astronomy Morsels“, page 320) Moon at 50°N, MayJun 2012: daily change of declination (∆δ), and ∆T = t_{Trans}  t_{Culm} (minutes) e.g. on
May 10:
∆δ>0, and ∆T<0: culmination is after transit, horizontal axis: day of
the year 2012
vertical axis: time difference in seconds between culmination and transit latitude Φ = 50° computed by my Planet applet Vertical axis: Difference t_{Trans}  t_{Culm} (minutes) at 50°N 0°E horizontal axis: day in SepOct 2015 computed by my Planet applet Vertical axis: Difference t_{Trans}  t_{Culm} (minutes) at 50°N 0°E horizontal axis: day in SepOct 2024 computed by my Planet Applet It seems that the
variation of ∆T is dominated by the
18.6year cycle of lunar
standstills:
small values of ∆T (up to 4 minutes) are occuring in years of minor lunar standstills (1996, 2015), and large values (more than 6 minutes) in years of major lunar standstills (2006, 2024/2025). Max. declination in 2024 on Sep 24 at 17 UT: 28.70° Min. declination in 2024 on Oct 09 at 12 UT: 28.70° Change in declination: 14.22 arcmin/h < _{}< 18.21 arcmin/h Max. declination in 2015 on Jan 03 at 18 UT: 18.65° Min. declination in 2015 on Jan 18 at 06 UT: 18.58° Change in declination: 9.42 arcmin/h < _{}< 11.64 arcmin/h 2006 (major lunar
standstill) Aug 10, 50°N, 0°E
transit
00:40:34 UT MICA:
culmination 00:46:48 UT ∆T = 6 min 14 s Planet Applet: transit 00:40:34 UT culmination 00:46:49 UT ∆T = 6 min 15 s calsky:
transit:
00h 40m 34.2s UT
culmination:
00h 46.9m UT
∆T = 6 min 20 s StarryNight SN7 CSAP transit: 00h 40m 34.2s UT culmination: 00h 46.8m UT ∆T = 6 min 15 s The altitude at culmination is only 0.81' more than at transit. by formula (3) and MICA: ^{} = dδ/dt = 0,2585°/hour dH/dt = 14.45°/hour δ = 15.55° ∆T = 6 min 02 s Vertical axis: hourly change of Declination (degrees) horizontal axis: day in SepOct 2015 minor lunar standstill Vertical axis: hourly change of Declination (degrees) horizontal axis: day in SepOct 2024 major lunar standstill The result by formula (3) or formula (8) will be large for northern latitudes, if δ<0, and if _{}is large. dH/dt is nearly constant (14.38°/hour to 14.61°/hour). The Planets As an example
transit and culmination of Mars at
50°N, 0°E:
Mars, 2012 May 25 (computed by
MICA):
Transit
18:41:50
UT, 18:41:51.2 UT
Culmination 18:41:43 UT, 18:41:45 UT ∆T = 7 s Mars, 2012 May 25 (computed
by StarryNight):
Transit
18:41:50
UT, 18:41:51.2 UTCulmination 18:41:43 UT, 18:41:44.5 UT ∆T = 6,7 s Mars, 2012 Aug 01 (computed by MICA): Transit 16:17:38 UT Culmination 16:17:26 UT ∆T = 12 s Mars, 2012 Aug 01 (computed by StarryNight): Transit 16:17:38 UT, 16:17:40.7 UT Culmination 16:17:26 UT, 16:17:28.5 UT ∆T = 12.2 s Mars, 2013 Apr 01 (computed by MICA): Transit 12:18:20 UT Culmination 12:18:34 UT ∆T = 14 s Mars, 2013 Apr 01 (computed by StarryNight): Transit 12:18:20 UT, 12:18:22.9 UT Culmination 12:18:34 UT, 12:18:36 UT ∆T = 13.1 s
Table from Wilson Using the diagram
above to get ∆T for the Sun, look up the
value of F (depending on latitude
and declination), and multiply F
by the hourly
declination change _{} in arcminutes per
hour:
Φ = 50°, δ = 0°, F = 18, _{}= 1 arcmin/h, ∆T = 18 s ***
A paper by
Pio (1899) describes the
determination of the longitude (at known
latitude) from the culmination of the Moon:
The instants of two equal altitudes are
measured by a chronometer and a sextant, and
the time of culmination is "reduced to the
meridian". The practical advantage of the
method is that it does not require any transit
instruments.


D. A. Pio: Longitude from the Moon
Culminations, Monthly Notices of the Royal
Astronomical Society, from November 1998 to
November 1999, Volume LIX, London 1899. [NavList 9938] Re: Time of meridian passage accuracy James N. Wilson: Position from Observation of a Single Body (Appendix I) 
Books 
Jörg
Meyer: Die Sonnenuhr und ihre Theorie, Verlag
Harry Deutsch, Frankfurt 20 Jean Meeus: More Mathematical Astronomy Morsels, WillmannBell, 2002. 
Software 
MICA
Multiyear Interactive Computer Almanac 18002050
by U.S. Naval Observatory StarryNight 7 CSAP 
(c)
20122017 J. Giesen
Last update:
2017,
Jan
13