The Sky as a Sphere: Days, Seasons and the Phases of the Moon
The celestial sphere as a model of the sky, and how it explains the day, the seasons, the phases of the Moon and why eclipses do not happen every month.
At a glance · about 2 minutes
The Sky in Six Ideas
- Daily turnOne turn against the stars takes 23.93 hours; the sky circles the poles.
- Yearly pathThe Sun moves east along the ecliptic, about 1 degree a day.
- SeasonsFrom the 23.44-degree tilt, not the distance; perihelion is in early January.
- Day lengthSet by latitude and the Sun's declination.
- PhasesThe lit half seen from a changing angle (elongation); 29.53-day average cycle.
- EclipsesNeed a new or full Moon near a node; the orbit is tilted 5.1 degrees.
In brief
The sky can be modelled as a sphere around you, with poles, an equator, a horizon and the ecliptic, the Sun's yearly path, tilted 23.44 degrees to the equator. That tilt, not the Earth's distance from the Sun, makes the seasons and sets the day length at each latitude. The Moon's phases are the changing view of its lit half, and eclipses are not monthly because the Moon's orbit is tilted about 5.1 degrees to the ecliptic.
Key ideas
- The celestial sphere is a model of directions, with poles, a celestial equator, a horizon and the ecliptic, the Sun's yearly path, which is tilted 23.44 degrees (the obliquity) to the equator.
- The seasons come from the tilt, not from distance: the Earth is nearest the Sun in early January, in northern winter, and the hemispheres have opposite seasons, while the tilt sets the Sun's noon height and the day length at each latitude.
- The Moon's phases are the changing view of its lit half, set by its elongation from the Sun and repeating on average every 29.53 days; eclipses do not happen every month because the Moon's orbit is tilted about 5.1 degrees to the ecliptic, so they need a new or full Moon near a node.
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Astronomy is the art of magnitude in motion. Nicomachus gives geometry the part of size that "abides and is at rest" and astronomy "that which moves and revolves" (Introduction to Arithmetic I.3, D'Ooge's translation, Attested; see The Order of the Seven Liberal Arts: Substance, Quantity and the Mind). This lesson builds the celestial sphere, a model of the sky as it appears, and uses it to explain days, seasons, phases and eclipses.
The celestial sphere as a model
Established Picture a sphere of enormous radius centred on you, with the stars fixed to its inside. The Earth's axis, extended, meets it at the two celestial poles, and the Earth's equator, projected outwards, makes the celestial equator. The horizon is the circle where ground meets sky. Like the celestial equator, it is a great circle, cutting the sphere in half. A third is the ecliptic, the Sun's apparent yearly path through the stars. It is inclined to the celestial equator by the obliquity, 23.44 degrees (NASA).
The sphere maps directions, not distances; nothing below needs the stars to lie on a real shell. The planets, which wander across the sphere, need a different account: Models of the Heavens: Ptolemy, Copernicus, Tycho and Kepler.
The altitude of the celestial pole above your horizon equals your latitude, so a traveller going north sees the pole rise. Aristotle used this effect as evidence (De Caelo II.14, 297b30 to 298a9): some stars seen in Egypt and near Cyprus are not seen in the northern regions. A small change of position, he argues, changes the horizon markedly, so the Earth is "a sphere of no great size" (Attested, Stocks's translation).
The daily turn
Established The Earth turns once in 23.9345 hours relative to the stars, so the sphere seems to turn about the poles in that time. Because the Earth also moves along its orbit, the Sun slides eastwards along the ecliptic, 360 degrees in about 365.25 days, or 0.986 degrees a day. Turning that extra degree to bring the Sun back to noon takes the Earth 3 minutes 56 seconds, so the mean solar day is 24 hours. A star therefore rises about four minutes earlier each night, and the stars seen at a fixed clock time repeat yearly.
The seasons come from the tilt
Established The Earth's axis leans 23.44 degrees from the perpendicular to its orbit, the same angle as the obliquity. The Sun's declination, its angular distance north or south of the celestial equator, therefore swings between plus and minus 23.44 degrees. The solstices are the two extremes and the equinoxes the two crossings of the celestial equator. In 2026 they fell on 20 March, 21 June, 23 September and 21 December (US Naval Observatory, Universal Time; local dates can differ by a day).
The Sun's noon altitude is 90 degrees minus the size of the difference between latitude and declination, counting south as negative. At 45 degrees north it is 45 degrees at the equinoxes, 68.44 at the June solstice and 21.56 at the December solstice. The Sun can stand directly overhead only between 23.44 degrees south and north, a fact Eratosthenes' measurement builds on. A higher Sun's light strikes the ground more directly, concentrating each beam on less ground, and a higher Sun stays up longer. Both make summer. When the declination is north, the north has the high Sun and the south the low one, so the hemispheres have opposite seasons.
Refuted The rival explanation, that summer comes when the Earth is nearest the Sun, predicts summer in both hemispheres at once, at the nearest point of the orbit. Both parts fail. The hemispheres have opposite seasons, and the Earth is nearest the Sun (perihelion), 147.095 million km away, between 2 and 5 January (Universal Time) in every year from 2015 to 2030, by the Observatory's tables. It is farthest (aphelion), 152.100 million km, in early July. At perihelion sunlight is about 6.9 per cent stronger than at aphelion, since light weakens with the square of distance, yet the north is then in winter.
Distance does leave a trace in the calendar. The Earth moves faster near perihelion, as Kepler's second law says: the line to the Sun sweeps equal areas in equal times (Kepler's laws in the lab). So the quarter containing perihelion (December 2025 solstice to March 2026 equinox) lasted 88.99 days, and the quarter containing aphelion (June to September 2026) 93.65 days.
Day length depends on latitude
Demonstrated (by spherical trigonometry, not shown here; for the Sun's centre on the horizon). The sunrise equation is cos H = −tan(latitude) × tan(declination). H is the angle the sky turns between sunrise and noon, at 15 degrees an hour, so with H in degrees the day lasts 2H/15 hours. It uses the cosine from the unit circle in Geometry, Euclid and Trigonometry.
At the equator the day is 12 hours all year. At the June and December solstices it is 15.4 and 8.6 hours at 45 degrees north, and 18.5 and 5.5 hours at 60 degrees north. North of latitude 90 − 23.44 = 66.56 degrees, the Arctic Circle, the equation has no solution at the solstices: the Sun does not set in June and does not rise in December.
Almanacs instead time sunrise with the Sun's centre 0.833 degrees below the horizon, for refraction (the air bends sunlight) and the Sun's width. Real days are therefore longer, by about 7 minutes at the equator and over 20 at 60 degrees at the solstices, and the limits of the midnight Sun and polar night shift about 0.8 degrees.
The phases of the Moon
Established The Sun always lights half of the Moon, and the phase is how much of that lit half we can see (NASA). It depends on the elongation, the angle between the Sun and the Moon as seen from Earth. At 0 degrees the lit half faces away: new Moon. At 90 degrees half the disc is lit: a quarter. At 180 degrees the lit half faces us: full Moon. The lit fraction is very nearly (1 − cos E)/2, because the Sun is about 390 times farther away than the Moon, so its light reaches both from almost the same direction.
The cycle repeats on average every 29.53 days, the synodic month. The Moon circles the Earth in 27.32 days relative to the stars, but the Sun's direction moves on by about 27 degrees in that time, and the Moon needs a little over two more days to catch up. The Moon gains on the Sun 1/27.32166 − 1/365.256 = 1/29.5306 of a turn a day. Single months vary because the Moon's orbit is elliptical: in 2025 and 2026, new to full Moon took 14.0 to 15.6 days (US Naval Observatory).
The phases are not caused by the Earth's shadow, which falls on the Moon only in a lunar eclipse, at full Moon. Aristotle already relied on the difference (De Caelo II.14, 297b23 to 30): the Moon's monthly shapes are "straight, gibbous, and concave", but in eclipses "the outline is always curved". Because "it is the interposition of the earth that makes the eclipse", he takes the curve to show that the Earth's surface is spherical (Attested).
Why eclipses are not monthly
Established The Moon's orbit is inclined 5.145 degrees to the ecliptic. It crosses the ecliptic at two nodes and otherwise lies north or south of the Sun's path. The Moon's disc is about 0.52 degrees wide and the Sun's about 0.53 (NASA data). At new Moon, a Moon 5 degrees off the ecliptic misses the Sun by about ten Moon-widths. At full Moon it misses the Earth's shadow likewise.
An eclipse needs a new Moon (solar) or a full Moon (lunar) near a node; for a solar eclipse, within about 17 degrees of it. The Sun reaches a node about every 173.3 days, so eclipses cluster in eclipse seasons, usually two a year. Each season lasts about 34.5 days, longer than a synodic month, so each brings at least one solar eclipse somewhere on Earth (NASA).
Try this
- Choose any city and look up its latitude. Predict the Sun's noon altitude there at the equinoxes and both solstices, as Hypotheses, Predictions and Tests advises, then check in the sky lab.
- For January in both hemispheres, write what the distance and tilt explanations each predict. Then say whether any perihelion date could have saved the distance explanation.
- Predict the phase at an elongation of 90 degrees and check it in the phases lab. Then, from a published new Moon date and the average month, predict the next first quarter and full Moon, and check the table.
- On clear evenings in the week after a new Moon, sketch the lit side and check that it faces where the Sun set.
Further reading
- Aristotle, On the Heavens II.14, translated by J. L. Stocks: MIT Classics text.
- NASA, the seasons and Moon phases.
- U.S. Naval Observatory, Earth's seasons and apsides.
- Fred Espenak, Eclipses and the Moon's orbit.
Check yourself
Answer each question from memory before you open it. Retrieval, not rereading, is what makes learning last (see the weekly loop). Grade yourself honestly and the study dashboard will bring each card back just before you'd forget it.
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recall
What is the obliquity of the ecliptic, and how large is it?
Show answer
It is the angle between the ecliptic (the Sun's apparent yearly path) and the celestial equator. It equals the tilt of the Earth's axis from the perpendicular to its orbit, 23.44 degrees, so the Sun's declination swings between plus and minus 23.44 degrees.
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recall
What is the synodic month, and how long is it?
Show answer
It is the time after which the Moon's phases repeat, for example from one new Moon to the next: 29.53 days on average. It is longer than the Moon's 27.32-day orbit relative to the stars because the Sun's direction moves on by about 27 degrees in that time, and the Moon needs a little over two more days to catch up.
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explain
Why does the date of perihelion show that distance from the Sun cannot be the cause of the seasons?
Show answer
The Earth is nearest the Sun (perihelion, 147.095 million km) in early January and farthest (aphelion, 152.100 million km) in early July. If distance caused the seasons, the north would have summer in January, when sunlight is about 6.9 per cent stronger. Instead January is northern winter. A distance cause would also give both hemispheres summer at once, but their seasons are opposite, as the tilt predicts.
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apply
A place lies at latitude 40 degrees north. How high is the Sun at local noon at the equinoxes and at the June solstice?
Show answer
The noon altitude is 90 degrees minus the size of the difference between latitude and declination. At the equinoxes the Sun is on the celestial equator, so the declination is zero and the altitude is 90 - 40 = 50 degrees. At the June solstice the declination is +23.44 degrees, so the difference is 40 - 23.44 = 16.56 degrees and the altitude is 73.44 degrees.
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connect
The lesson 'Eratosthenes Measures the Earth' depends on the Sun's height at noon. Where on Earth can the Sun stand directly overhead at noon, and when does that happen at latitude 23.44 degrees north?
Show answer
Only between 23.44 degrees south and 23.44 degrees north, because the noon altitude reaches 90 degrees only when latitude equals declination, and the declination never goes beyond plus or minus 23.44 degrees. At 23.44 degrees north it happens at the June solstice, when the declination reaches +23.44 degrees.
Open questions
No answer key. Think them through, write a paragraph, or argue them out with someone; the aim is a better question.
- At De Caelo II.14 (297b23 to 30) Aristotle says the Moon shows straight, gibbous and concave shapes in a month, but that in eclipses the outline is always curved, and he concludes that the Earth's surface is spherical. State his argument as numbered premises and a conclusion. Which premise would you test first, and how?
- In the same chapter (297b30 to 298a9) Aristotle adds a second observation: stars seen in Egypt and near Cyprus are not seen in the northern regions. If you had only one of his two observations, which would persuade you more that the Earth is round, and what would you still have to assume?
- Aristotle says that the evidence of the senses further corroborates an argument he has just made from the way heavy bodies move towards the centre (De Caelo II.14, 297a8 to 297b23). Does the argument from the eclipse depend on that earlier argument? Answer from his words, and respond to the other readers in your group.
Sources
- Aristotle. On the Heavens (De Caelo), II.14 (297a8-298a9). Translated by J. L. Stocks (Oxford: Clarendon Press, 1922). Free text: classics.mit.edu/Aristotle/heavens.2.ii.html; scan with Bekker numbers: archive.org/details/decaelo00aris. Bekker lines checked against the Greek text ed. C. Prantl (Leipzig: Teubner, 1881), First1KGreek tlg0086.tlg005.1st1K-grc1.
- Nicomachus of Gerasa. Introduction to Arithmetic, I.3.1-2. Translated by M. L. D'Ooge (New York: Macmillan, 1926), p. 184. Scan: archive.org/details/nicomachus-introduction-to-arithmetic.
- NASA Goddard Space Flight Center. Earth, Moon and Sun Fact Sheets (nssdc.gsfc.nasa.gov/planetary/factsheet/).
- U.S. Naval Observatory, Astronomical Applications Department. Earth's Seasons and Apsides (aa.usno.navy.mil/data/Earth_Seasons; API aa.usno.navy.mil/api/seasons?year=YYYY) and Phases of the Moon (API aa.usno.navy.mil/api/moon/phases/year?year=YYYY), times in Universal Time.
- NASA Space Place. What Causes the Seasons? (spaceplace.nasa.gov/seasons/en).
- U.S. National Weather Service, Sioux Falls. What Causes the Seasons? (weather.gov/fsd/season).
- NASA Science. Moon Phases (science.nasa.gov/moon/moon-phases/) and the eclipse geometry page (science.nasa.gov/eclipses/geometry/).
- Espenak, F. Eclipses and the Moon's Orbit (eclipse.gsfc.nasa.gov/SEhelp/moonorbit.html) and Periodicity of Solar Eclipses (eclipse.gsfc.nasa.gov/SEsaros/SEperiodicity.html). NASA Eclipse Web Site.
- J. J. O'Connor and E. F. Robertson. Johannes Kepler. MacTutor History of Mathematics (mathshistory.st-andrews.ac.uk/Biographies/Kepler/).
- Wikipedia articles Sunrise equation, Celestial pole, Celestial equator, Ecliptic, Axial tilt, Solstice, Equinox, Lunar phase and Eclipse season, used for definitions and standard formulas, each result recomputed here.