Phases of the MoonGo deeperabout 45 min
The chase, the wobble and the brake
Deriving 29.53 days, the elastic tithi, adhik maas, eclipse rarity and the recession, from first principles
Go past the rules to the reasoning: derive the synodic month from two orbital speeds, see why a tithi stretches and shrinks, work out how often adhik maas is needed, derive eclipse rarity from the 5.1-degree tilt, and follow the torque that locked the Moon and is now pushing it away.
In this part you’ll
- Derive the 29.53-day synodic month from the Moon's and Earth's separate orbital speeds.
- Explain why a tithi's real length varies, and calculate how often an adhik maas is needed.
- Derive the geometric reason eclipses need a new or full moon near an orbital node, and explain the Saros cycle.
- Describe the torque mechanism that tidally locked the Moon and is now driving its slow recession.
- Calculate the true size and brightness change of a 'supermoon' and distinguish the Moon's two different tilts.
Two numbers have been sitting quietly in every table so far: the Moon orbits Earth once every 27.32 days (the sidereal month), yet the cycle of phases — new moon to new moon — takes 29.53 days (the synodic month). They differ by more than two days, and that gap is not a rounding error or an approximation. It is a real, calculable consequence of the fact that Earth itself is moving.
This layer is about the why behind everything Understand told you to accept: why the two months differ by exactly the amount they do, why a tithi is never quite 24 hours, why an extra month has to be inserted into the Hindu lunar calendar every few years, why eclipses only happen a handful of times a year instead of every month, and why the Moon is quietly leaving us at a rate you could almost measure with a ruler and a stopwatch, if the stopwatch ran for a very long time.
Expect harder arithmetic than before, some genuine derivations, and a few numbers that will surprise you.
Chapter 01
The chase: deriving the synodic month
Picture two runners on a circular track, both running the same direction. The Moon covers the 360° track in 27.32 days (it laps Earth once every sidereal month). The Sun — really Earth's own motion around it, seen from Earth — covers the same 360° in 365.256 days (one year).
The Moon is the faster runner. "New moon" is the moment the Moon catches up to the Sun's position in the sky and laps it exactly once. So the question "how long is a synodic month?" is really "how long until the faster runner gains one full lap on the slower one?" — a classic overtaking problem, solvable with nothing but ratios.
Worked example
0 / 5 steps shownDeriving 29.53 days from nothing but two orbital periods
The Moon completes a true 360° orbit every 27.322 days. Earth completes its own 360° orbit of the Sun every 365.256 days. Derive the synodic month (new moon to new moon) from these two numbers alone.
Try it
Chapter 02
One extra lap a year: sidereal months vs lunations
Here is a clean consequence of the same chase, easy to miss and satisfying once seen.
In one year, how many sidereal months fit (laps of the Moon around Earth against the stars)? And how many synodic months fit (new moon to new moon)?
| Kind of month | Length (days) | Fits into a year | What it counts |
|---|---|---|---|
| Sidereal | 27.32 | 13.37 | Complete 360° orbits of the Moon around Earth |
| Synodic | 29.53 | 12.37 | Complete cycles of phase, new moon to new moon |
Try it
Chapter 03
The elastic tithi
Understand told you a tithi is one thirtieth of a lunar month — 23.62 hours on average. "On average" is doing real work in that sentence. A tithi is not defined as a fixed slice of time at all; it is defined as the time the Moon takes to gain exactly 12° of elongation on the Sun, and that time genuinely stretches and shrinks through the month.
Worked example
0 / 5 steps shownHow many tithis in an average synodic month, and why exactly 30
Each tithi is defined as a 12° gain in elongation. Show why a synodic month always contains exactly 30 tithis, and identify which tithi number is Purnima and which is Amavasya.
Try it
Chapter 04
Adhik maas: patching a lunar calendar onto a solar year
Twelve synodic months make a lunar year of 354.37 days. A solar (tropical) year, the one the seasons actually follow, is 365.24 days. The gap is 10.88 days every single year — over ten days, gone missing, unless something is done about it.
Left unpatched, festivals tied to a purely lunar calendar would drift steadily earlier every year, cycling all the way through the seasons over a few decades. (You will meet a calendar that actually does this in the next chapter.) The Hindu calendar avoids that drift by being lunisolar: it keeps lunar months, but reinserts a whole extra month, an adhik maas, whenever the shortfall has built up to about one lunar month's worth.
Worked example
0 / 5 steps shownDeriving how often an extra month is needed
The lunar year falls short of the solar year by 10.875 days annually. Work out roughly how many years pass before that shortfall equals one whole extra lunar month.
Try it
Lab
Step the Moon through a month with tithi numbers switched on, and watch how unevenly they tick over compared with a clock.
Up in the sky: Rises exactly as the Sun sets and sets as the Sun rises — up the whole night, straight overhead at midnight. Sets about 6:00 am.
In the Indian calendar
Pratipada, tithi 1 of Krishna Paksha — the dark fortnight, when the Moon shrinks. A tithi is the time the Moon takes to gain 12° on the Sun, so there are 30 in a month and each fortnight ends on Amavasya, the new moon.
Approximate. A real panchangam uses the Moon's true, slightly wobbly motion, so a tithi can be a few hours longer or shorter than the average used here.
The Sun lights exactly half the Moon, all month long. What changes is where we are standing to look at it. Day 14.8 means the Moon is 180.06° round its orbit from new moon.
Text version of this activity
This lab shows the Moon's disc together with its tithi number, both driven by a single day-of-month slider. It opens at day 14.77, tithi 15 — Purnima, full moon.
Move the slider slowly through a full month and watch the tithi count climb from 1 to 30. On average each tithi should occupy about 23.6 hours of slider time, but because the underlying model can be set to reflect the Moon's elliptical speed, tithi boundaries do not fall at perfectly even spacing — exactly the elastic behaviour described above, made visible rather than just stated. Six quiz rounds then ask you to read off the tithi and the paksha (shukla or krishna) from the shape alone.
Lab
Connect each named astronomical or calendar cycle to its correct approximate length.
Match each named cycle from this layer to its approximate length.
6 pairs are hiding in two mixed-up columns. Pick one from each side to join them.
Text version of this activity
Six cycles are matched to six lengths: synodic month to 29.53 days; sidereal month to 27.32 days; mean tithi to 23.6 hours; the adhik maas interval to about 2.7 years; the Metonic cycle to 19 years; and the Saros cycle to 18.0 years. Getting these six numbers straight, and not confusing one cycle's length for another's, is exactly the skill this chapter and the next two build.
Chapter 05
The 5.1° tilt: deriving eclipse rarity
If the Moon's orbit lay exactly in the same plane as Earth's orbit around the Sun, every single new moon would produce a solar eclipse and every full moon a lunar eclipse — twelve or thirteen of each, every year. That obviously is not what happens. The reason is a single number: the Moon's orbit is tilted 5.145° to the plane of Earth's orbit (the ecliptic).
Twice a year, on average about 173.31 days apart, the Sun's apparent path carries it close to one of these nodes. Each such eclipse season lasts roughly a month, during which the new moon and/or full moon that falls inside it has a real chance of producing an eclipse. Outside the two eclipse seasons, the geometry simply cannot work, no matter how new or full the Moon is.
Worked example
0 / 5 steps shownThe Saros cycle: why similar eclipses repeat every 18 years 11 days
Derive the length of the Saros cycle from the synodic month and the requirement that it takes a whole number of synodic months.
Helps you understand
EclipsesThe full mechanics of solar and lunar eclipses — the umbra, the penumbra, why some eclipses are total and others annular — belong to that topic. This chapter only explains why they are rare rather than monthly.
Lab
Tilt the Moon's orbit away from zero and watch eclipses become possible only near two points in the orbit, then only in two windows each year.
34,171 km off the plane is 2.7 whole Earths' worth of miss. The shadow sails harmlessly over the top (or under the bottom) of us. Only within about 17° of a node is the line-up good enough — which happens in two short "eclipse seasons" a year, not every month.
The Moon's orbit is tilted 5.1° against the flat plane Earth goes round the Sun in. Two tilted circles can only cross at two points, and those two points are called the nodes. An eclipse needs a new or full moon to land almost exactly on a node.
Sizes on the picture: the Sun is 6,96,000 km in radius and 150 million km away, the Moon 1,737 km and about 3,84,400 km away. Their apparent sizes agree to within a few per cent — 0.52° against 0.53° — which is a coincidence, and the reason total solar eclipses exist at all.
Text version of this activity
The lab shows Earth, its orbit, and the Moon's orbit as a disc that can be tilted from 0° up to 10°. Two shadow cones are drawn: Earth's, pointing away from the Sun, and the Moon's, doing the same.
At 0° tilt, the Moon's path lies exactly in Earth's orbital plane, and every new moon passes through Earth's shadow's opposite point and every full moon passes into Earth's shadow: eclipses every month, both kinds.
Set the tilt to the real value, 5.145°, and the Moon's path now weaves above and below the flat plane that holds the Sun and Earth's shadow. Only where that weaving path crosses the flat plane — the two nodes — can an eclipse occur, and then only if the Moon also happens to be new or full at that same moment. The lab marks these two crossing points and shows how a new or full moon elsewhere on the tilted path clears the shadow entirely, exactly matching the roughly 29% 'hit window' computed above.
Chapter 06
Tidal locking: the mechanism
Understand told you the Moon always shows the same face because it is tidally locked: its rotation period exactly equals its orbital period. This chapter explains the actual mechanism, which is a beautiful piece of physics involving nothing but gravity and a slight lag.
Billions of years ago, the young Moon almost certainly spun much faster than it orbited Earth, the way most moons and planets do when they form. But Earth's gravity does not pull equally on every part of the Moon: it pulls harder on the near side than the far side, because the near side is closer. That difference in pull stretches the Moon very slightly into an elongated shape, with a bulge pointing roughly towards Earth and another pointing roughly away — a tidal bulge, the same effect that raises ocean tides on Earth (that connection is explored fully in the tides topic).
| Tilt | Value | What it governs | Why it exists |
|---|---|---|---|
| Orbital tilt | 5.145° | How rare eclipses are (Chapter 5) | How the Moon's orbital plane leans against Earth's orbital plane around the Sun |
| Axial tilt | 1.5424° | Permanently shadowed craters near the poles (Extend) | How the Moon's own spin axis leans against its orbital plane — remarkably close to upright, unlike Earth's 23.4° |
Chapter 07
Measuring a retreat of 3.8 centimetres a year
The same tidal bulge that locked the Moon's rotation is still doing work today, on a much larger and slower scale: it is very gradually pushing the Moon away from Earth, at a measured rate of about 3.8 cm per year.
The mechanism is the mirror image of Chapter 6's story, but now the bulge in question is Earth's ocean tidal bulge, and it is Earth's much faster 24-hour spin (compared with the Moon's monthly orbit) that drags that bulge slightly ahead of the Earth-Moon line. Earth's gravity, acting through that misaligned bulge, now speeds the Moon up very slightly along its orbit. A slightly faster-moving satellite settles into a slightly higher, wider orbit — so the Moon spirals gently outward, while by Newton's third law, Earth's spin correspondingly slows down (this is the same mechanism from Chapter 6, running today, with Earth and Moon swapping roles).
Worked example
0 / 5 steps shownHow a car-sized reflector on the Moon proves the recession rate
Explain, step by step, how a mirror left on the Moon in 1969-1972 lets scientists measure a recession rate as small as a few centimetres a year.
| Time span | Total recession | Sense of scale |
|---|---|---|
| 1 year | 3.8 cm | About the width of two fingers |
| 1 human lifetime (80 yr) | 304 cm | About the height of a young child |
| 1,000 years | 38.0 m | Roughly the height of two adults |
| 26,316 years | 1 km | Longer than all of recorded human history, several times over |
| 1 million years | 38 km | Roughly the straight-line distance from Delhi to Kolkata |
Try it
Chapter 08
How big does the Moon look? Perigee, apogee and 'supermoons'
The Moon's elliptical orbit means its distance from Earth genuinely varies, between roughly 363,300 km at its closest (perigee) and 405,500 km at its farthest (apogee) in an extreme month. A popularly reported "supermoon" is a full moon that happens to fall close to perigee. How much bigger does it actually look?
Worked example
0 / 5 steps shownWhy a 'supermoon' looks only slightly bigger but noticeably brighter
A full moon at perigee (363,300 km) is compared with one at apogee (405,500 km). Find the percentage increase in apparent width, and separately in brightness.
Chapter 09
A history of figuring it out
From guesswork to laser rulers
- ~450 BCEAnaxagoras The Greek philosopher Anaxagoras argues that the Moon shines by reflected sunlight and correctly explains eclipses as shadows — for which, among other views, he was tried for impiety in Athens.
- ~350 BCEAristotle's evidence Aristotle notes that Earth's shadow on the Moon during a lunar eclipse is always round, correctly inferring that Earth itself must be a sphere.
- ~150 CEPtolemy's tables Ptolemy's Almagest gives detailed geometric models predicting lunar position and phase, good enough for calendars and eclipse prediction for over a thousand years, despite an Earth-centred universe.
- ~500 CEIndian astronomy Astronomers such as Aryabhata compute lunar and solar positions with real precision, underpinning the tithi-based calendar still used for festival dates today.
- 1609-1610Galileo's telescope Galileo turns a telescope on the Moon and sees mountains, craters and the terminator's shifting shadows firsthand, publishing sketches in Sidereus Nuncius that overturned the idea of a perfectly smooth celestial sphere.
- 1687Newton's tides Newton's law of gravitation explains, for the first time, why the Moon raises tides on Earth — the same mechanism this chapter used to explain tidal locking and recession.
- 1959Luna 3 The Soviet probe Luna 3 returns the first, blurry photographs of the Moon's far side, ending millennia of pure speculation about what lay on the hidden hemisphere.
- 1969-1972Apollo retroreflectors Apollo astronauts place laser retroreflectors on the surface, turning the Moon into a target precise enough to measure its slow recession directly, in centimetres.
- 2023Chandrayaan-3 India's Vikram lander touches down near the lunar south pole, the first successful soft landing in that especially difficult, permanently shadow-rich region.
Reflect
This stays on this page only. It isn’t saved or sent anywhere.
A last set of mix-ups, sharper than Understand's, because they trip up people who already know the basics.
Try it
Words to know
All maths vocabulary →New vocabulary in this layer
- Synodic month
- The 29.53-day cycle of lunar phases, new moon to new moon; depends on both the Moon's and Earth's motion.
- Example: Karva Chauth and Purnima both repeat on a synodic rhythm.
- Sidereal month
- The 27.32-day time for the Moon to complete one true 360° orbit against the fixed stars.
- Example: Slightly shorter than the synodic month because Earth keeps moving.
- Node
- One of two points where the Moon's tilted orbital plane crosses Earth's orbital plane; eclipses can only happen near a node.
- Example: The two eclipse seasons occur when the Sun appears near a node.
- Draconic month
- The time for the Moon to return to the same node, 27.21 days — different from both other months because the nodes themselves slowly rotate.
- Example: Used together with the synodic month to derive the Saros cycle.
- Saros
- An 18-year, 11-day cycle after which similar eclipses recur, because 223 synodic months and the draconic cycle both return to nearly the same alignment.
- Example: Discovered empirically by Babylonian astronomers long before its cause was understood.
- Adhik maas
- An extra ('leap') lunar month inserted roughly every 32-33 months to keep the Hindu lunisolar calendar aligned with the solar year.
- Example: Also called purushottam maas when it falls in certain positions.
- Retroreflector
- A mirror device that reflects light straight back the way it came, regardless of the incoming angle.
- Example: Apollo astronauts left retroreflector arrays that are still used for laser ranging today.
- Tidal bulge
- A slight elongation of a body caused by the stronger gravitational pull on its near side than its far side.
- Example: Earth's tidal bulge, dragged ahead by its fast spin, is what is currently pushing the Moon away.
Quick check
Test the mechanisms
8 questions · answer what you can, then check. Getting one wrong is useful.
Keep this
Deepen cheat sheet
- The synodic/sidereal gap is Earth's fault, not the Moon's ellipse's fault. 27.32 days to lap Earth, 29.53 days to catch the Sun again, because Earth has moved on meanwhile.
- Sidereal months per year exceed synodic months per year by almost exactly one (13.37 vs 12.37) — Earth's own yearly lap, borrowed back.
- A tithi (12° of elongation) averages 23.6 hours but genuinely ranges from about 22 to 26 hours, because the Moon's elliptical orbit changes its speed.
- Adhik maas patches a 10.9-day yearly shortfall between 12 lunar months and one solar year; the fix arrives roughly every 3 years, about every 32-33 months.
- The Metonic cycle (19 years = 235 lunations) is the same shortfall arithmetic viewed over a longer span, discovered independently by Greek and other astronomers.
- Eclipses need a new/full moon near a node, one of two points where the 5.145° tilted lunar orbit crosses Earth's orbital plane; away from a node, the geometry cannot work.
- The Saros (about 18.0 years) recurs because 223 synodic months and the Moon's node-return cycle complete in nearly the same span.
- Tidal locking is a torque, not a coincidence: Earth's gravity braked the Moon's faster ancient spin via a misaligned tidal bulge, until spin matched orbit exactly.
- The Moon's orbital tilt (5.145°, governs eclipses) and its axial tilt (1.5424°, governs polar shadows) are different numbers with different jobs.
- Laser ranging to Apollo retroreflectors directly measures 3.8 cm/year of recession, confirmed independently by fossil coral growth-ring evidence of a faster-spinning ancient Earth.
- A perigee 'supermoon' looks only about 12% wider than an apogee full moon, but shines about 25% brighter, because brightness follows an inverse-square law.
Where this comes from
Sources
Lunar phase (opens another website) — Wikipediaawaiting check
Supports the illuminated-fraction formula, the synodic month of 29.53 days versus the sidereal month of 27.32 days, phase rise and set times, earthshine and the terminator.
Moon Facts: Earth's Natural Satellite (opens another website) — NASA Scienceawaiting check
Supports the Moon's diameter of about 3,475 km, its mean distance of about 384,400 km, synchronous rotation (the same face always turned to Earth), and the 27.3-day sidereal period.
Hindu calendar (opens another website) — Wikipediaawaiting check
Supports tithi as 12 degrees of elongation, 30 tithis to a lunar month, shukla and krishna paksha, Purnima and Amavasya, amanta and purnimanta reckoning, and adhik maas.
Metonic cycle (opens another website) — Wikipediaawaiting check
Supports the near-coincidence of 235 synodic months and 19 tropical years, and its use in lunisolar calendars such as the Hebrew calendar's leap-month rule.
Islamic calendar (opens another website) — Wikipediaawaiting check
Supports the Hijri calendar as a purely lunar 12-month calendar with no leap month, so it drifts about 11 days earlier each solar year and cycles through all seasons in about 33 years.
Saros (astronomy) (opens another website) — Wikipediaawaiting check
Supports the draconic month, the two eclipse seasons a year caused by the Moon's 5.1-degree tilt, and the 18-year 11-day Saros cycle that repeats similar eclipses.
Tidal locking (opens another website) — Wikipediaawaiting check
Supports synchronous rotation, how tidal friction slowed the Moon's spin until it matched its orbit, and the link between the same-face effect and the Moon's slow recession.
Apollo 11 Lunar Laser Ranging Retroreflector experiment (opens another website) — NASA Space Science Data Coordinated Archiveawaiting check
Supports the corner-cube retroreflectors left by Apollo crews, laser ranging from Earth, and the measurement of the Moon's slow recession of about 3.8 cm a year.
Earth's rotation (opens another website) — Wikipediaawaiting check
Supports how tidal friction between Earth and the Moon is slowing Earth's spin and lengthening the day, with fossil evidence (growth bands in ancient corals) showing shorter days hundreds of millions of years ago.
Moon: Earth's natural satellite (opens another website) — Encyclopaedia Britannicaawaiting check
Supports general lunar description: maria and highlands, cratering, the difference between near side and far side, and the Moon's albedo and brightness.
End of Go deeper
What you just read
- Derive the 29.53-day synodic month from the Moon's and Earth's separate orbital speeds.
- Explain why a tithi's real length varies, and calculate how often an adhik maas is needed.
- Derive the geometric reason eclipses need a new or full moon near an orbital node, and explain the Saros cycle.
- Describe the torque mechanism that tidally locked the Moon and is now driving its slow recession.
- Calculate the true size and brightness change of a 'supermoon' and distinguish the Moon's two different tilts.
- Next depthGo deeper: ExtendProjects, harder problems, wider contexts and open questions.
- Practise75 questionsHints and a worked solution for every question — or play a 10-question round.
- Step backInvestigateGo back over the ground before this one — you can move up and down as often as you like.
- TopicAll of phases of the moonThe whole ladder, the connections and the words to know, on one page.
The web
Explore a connection
Builds onanother area
LightThe Moon has no light of its own: we see the half of it the Sun is lighting.
Builds onanother area
GravityGravity is what keeps the Moon in the orbit that produces the monthly cycle of phases.
Helps you understand
EclipsesEclipses can only happen at new moon or full moon — the two phases where the three bodies line up.
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Revision 1 · release preview-7e1cbbcc4f · accepted 20/09/2026