Last chance! 50% off unlimited learning
Sale ends in
The calculations are based on formulae provided by Meeus [1982], primarily
in chapters 6, 18, and 30. The first step is to compute sidereal time as
formulated in Meeus [1982] chapter 7, which in turn uses Julian day computed
according to as formulae in Meeus [1982] chapter 3. Using these quantities,
formulae in Meeus [1982] chapter 30 are then used to compute geocentric
longitude (obliquity
of the ecliptic
is computed with Meeus [1982] equation 18.4. Equatorial coordinates (right
ascension and declination) are computed with equations 8.3 and 8.4 from
Meeus [1982], using eclipticalToEquatorial
. The hour angle
(equatorialToLocalHorizontal
.
moonAngle(t, longitude = 0, latitude = 0, useRefraction = TRUE)
time, a POSIXt object (converted to timezone "UTC"
,
if it is not already in that timezone), or a numeric value that
corresponds to such a time.
observer longitude in degrees east
observer latitude in degrees north
boolean, set to TRUE
to apply a correction for
atmospheric refraction. (Ignored at present.)
A list containing the following.
time
moon azimuth, in degrees eastward of north, from 0 to 360. Note: this is not the convention used by Meeus, who uses degrees westward of South. (See diagram below.)
moon altitude, in degrees from -90 to 90. (See diagram below.)
right ascension, in degrees
declination, in degrees
geocentric longitude, in degrees
geocentric latitude, in degrees
lunar diameter, in degrees.
earth-moon distance, in kilometers)
fraction of moon's visible disk that is illuminated
phase of the moon, defined in equation 32.3 of Meeus [1982]. The fractional part of which is 0 for new moon, 1/4 for first quarter, 1/2 for full moon, and 3/4 for last quarter.
Formulae provide by Meeus [1982] are used
for all calculations here. Meeus [1991] provides formulae that are similar,
but that differ in the 5th or 6th digits. For example, the formula for
ephemeris time in Meeus [1991] differs from that in Meeus [1992] at the 5th
digit, and almost all of the approximately 200 coefficients in the relevant
formulae also differ in the 5th and 6th digits. Discussion of the changing
formulations is best left to members of the astronomical community. For the
present purpose, it may be sufficient to note that moonAngle
, based
on Meeus [1982], reproduces the values provided in example 45.a of Meeus
[1991] to 4 significant digits, e.g. with all angles matching to under 2
minutes of arc.
Meeus, Jean, 1982. Astronomical formulae for calculators. Willmann-Bell. Richmond VA, USA. 201 pages.
Meeus, Jean, 1991. Astronomical algorithms. Willmann-Bell, Richmond VA, USA. 429 pages.
The equivalent function for the sun is sunAngle
.
Other things related to astronomy: eclipticalToEquatorial
,
equatorialToLocalHorizontal
,
julianCenturyAnomaly
,
julianDay
, siderealTime
,
sunAngle
# NOT RUN {
library(oce)
par(mfrow=c(3,2))
y <- 2012
m <- 4
days <- 1:3
## Halifax sunrise/sunset (see e.g. http://www.timeanddate.com/worldclock)
rises <- ISOdatetime(y, m, days,c(13,15,16), c(55, 04, 16),0,tz="UTC") + 3 * 3600 # ADT
sets <- ISOdatetime(y, m,days,c(3,4,4), c(42, 15, 45),0,tz="UTC") + 3 * 3600
azrises <- c(69, 75, 82)
azsets <- c(293, 288, 281)
latitude <- 44.65
longitude <- -63.6
for (i in 1:3) {
t <- ISOdatetime(y, m, days[i],0,0,0,tz="UTC") + seq(0, 24*3600, 3600/4)
ma <- moonAngle(t, longitude, latitude)
oce.plot.ts(t, ma$altitude, type='l', mar=c(2, 3, 1, 1), cex=1/2, ylab="Altitude")
abline(h=0)
points(rises[i], 0, col='red', pch=3, lwd=2, cex=1.5)
points(sets[i], 0, col='blue', pch=3, lwd=2, cex=1.5)
oce.plot.ts(t, ma$azimuth, type='l', mar=c(2, 3, 1, 1), cex=1/2, ylab="Azimuth")
points(rises[i], -180+azrises[i], col='red', pch=3, lwd=2, cex=1.5)
points(sets[i], -180+azsets[i], col='blue', pch=3, lwd=2, cex=1.5)
}
# }
Run the code above in your browser using DataLab