Lunar Node Calculator

Pick any date from 1700 to 2200 and see where the Moon's nodes are, the two points where its tilted orbit crosses the ecliptic, the plane of Earth's orbit around the Sun: ascending where the Moon climbs north through that plane, descending where it sinks back south. You get the standard mean node and the true node from the Moon's actual crossing, compared at the same instant, then the nearby crossing dates, your place in the 18.6-year cycle and the current draconic month (the Moon's node-to-node month), and the next solar and lunar eclipses.

Choose a date

Anything from 1700 to 2200. Everything is worked out live in your browser.

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Next eclipse season jumps to the first day the Sun is within 18.5 degrees of the mean node, the window a new moon must fall in for a solar eclipse; a lunar eclipse that enters Earth's umbra, the dark core of its shadow, needs the Sun within 12.2 degrees.

Mean node vs. true node

The mean node is a smooth average model; the true node is where the Moon is actually found crossing the ecliptic. The two agree only on average: the true node oscillates around the mean by about 1.5 degrees, and nearly 2 at the extremes, on a rhythm of about 173 days (half an eclipse year, the 346.62 days the Sun takes to return to the same node) set by the Sun's pull on the Moon's orbit, and can briefly move forward (direct) before resuming its slow westward drift, the regression.

Node positions are given as ecliptic longitude: degrees around the ecliptic counted eastward from the spring equinox point, the same zero the zodiac signs use, and "of date" means measured from where that point sits on your chosen day, since it drifts slowly with precession.

The mean node is shown below for your chosen date at 12:00 UTC and the true node at the crossing nearest it, with the gap between them at that same instant. A positive difference means the true node sits east of the mean node, at higher ecliptic longitude. Between crossings the true node keeps moving, so the gap on your chosen date can differ from the one at the nearest crossing.

Node crossings around this date

The previous and next times the Moon actually crosses the ecliptic plane, ascending and descending, with its right ascension and declination at that instant: the sky's own longitude and latitude, measured from the celestial equator, with right ascension counted in hours because the sky turns through 15 degrees of it every hour (as seen from Earth's center, equinox of date; from the surface the Moon appears shifted by up to about a degree by parallax).

KindWhen (UTC)Relative to your dateRADec

The 18.6-year nodal cycle

The line joining the two nodes drifts westward, or regresses, all the way around the ecliptic, 360 degrees, in about 18.6 years. Position measured from the mean ascending node's last crossing of 0 degrees Aries, the same zero point every zodiac position on this site uses.

The draconic month

The Moon's shortest month: the time from one ascending-node crossing back to the next one, shorter than a full orbit because the node itself keeps drifting west to meet the Moon.

Eclipse proximity

About every 173 days, half an eclipse year, the Sun passes one of the Moon's nodes, and the roughly month-long window around each passage, while the Sun is inside the solar limit, is an eclipse season.

An eclipse needs a new or full moon near a node. A solar eclipse needs the Sun within about 18.5 degrees of a node at new moon; a lunar eclipse that enters Earth's umbra, the dark core of its shadow, partial or total, needs it within about 12.2 degrees at full moon, while a penumbral-only eclipse, where the Moon dims without touching the umbra, can occur with the Sun about as far from the mean node as the solar limit. This shows how close the Sun sits to a node on your date, and the next solar and lunar eclipses on or after it.

Being inside a limit on your date means the Sun is in that season's window, not that the next new or full moon will produce an eclipse: just after a season's last eclipse the Sun is still inside the window while the next new moon has moved well past it. The distance above uses the mean node, matching the rest of the site (the Eclipse Control Center included) to within 0.02 degrees, so a season right at either limit could still tip either way under the true node's own swing of up to about 2 degrees.

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What the mean and true node are

For the models, accuracy and data behind these figures, see the methodology and sources page.

The Moon's orbit is tilted about 5 degrees to the ecliptic, the plane of Earth's own orbit, so it crosses that plane at exactly two points on opposite sides of the sky: the ascending node, where the Moon climbs from south of the ecliptic to north, and the descending node, half an orbit later, where it sinks back from north to south. Because the Sun's gravity constantly tugs on the tilted orbit, the whole line joining the two nodes slowly turns westward, a full circuit every 18.6 years, the regression of the nodes. See the lunar nodes explained for the full picture with a scrubbable 3-D view.

The mean node is a polynomial that models only the steady average regression and ignores the smaller wobbles; it is the figure this site's eclipse year page and Celestial Return Calculator use as "the node". Jean Meeus's version (Astronomical Algorithms, chapter 47) is the one used here. But the Moon does not actually follow the smooth mean curve. Solar gravity perturbs the Moon's orbital plane on a shorter rhythm as well as the long one, so the point where the Moon truly crosses the ecliptic, the true node, oscillates around the mean position by roughly 1.5 degrees, nearly 2 at the extremes, and occasionally appears to pause or even move briefly forward before the regression resumes. This calculator finds the true node directly: by searching the vendored astronomy engine for the actual instants the Moon's ecliptic latitude passes through zero, then reading the Moon's own longitude at that moment. It is the same lunar theory that positions the Moon everywhere else on this site, evaluated at the crossing itself. Ephemerides that print a true node for every day usually give the osculating node, the orbital element fitted to the Moon's position and velocity at that instant: it coincides with the crossing longitude at the crossing itself and drifts from it by up to about a degree in between, so this page reports the true node only at its crossings.

Why the difference is worth showing

Eclipses depend on the Moon's real position, not a smoothed average: the gap between the two is not a rounding error, and it can shift a marginal eclipse season in or out of range.

It answers a narrow question, for any date from 1700 to 2200: what the Moon's node is actually doing, from the same engine that drives this site's eclipse pages, and what that means for the next eclipse season.

How this tool works

The mean node comes from Meeus's published polynomial (Astronomical Algorithms, chapter 47). The true node comes from the vendored Astronomy Engine's own search for the Moon crossing the ecliptic plane, refined to about a second of time, the search tolerance rather than the error; right ascension and declination are geocentric, referred to the true equator and equinox of date (precession and nutation applied). The mean node is Meeus's mean-equinox figure and the crossing longitude is true-equinox, a nutation difference under 0.005 degrees, below the two decimals shown. Light-time and aberration are not applied: at the Moon's distance they together amount to about 0.7 arcsecond, far below the arcminute shown. Positions come from the open-source Astronomy Engine, running entirely in your browser, and the model is reliable for roughly the years 1700 to 2200, with future crossing times carrying the delta-T uncertainty described in the accuracy study. The zodiac positions are the tropical ecliptic longitude of date, with 0° at the spring equinox, the same convention used across CycleCalcs.

Frequently asked questions

What is the difference between the mean node and the true node?

The mean node is a smooth model, a polynomial that regresses westward at a steady average rate and completes one circuit of the ecliptic every 18.6 years. The true node is where the Moon is actually found crossing the ecliptic plane, which wobbles around the mean position by about 1.5 degrees either side, and nearly 2 at the extremes, because of periodic solar perturbations, and can briefly appear to move forward before resuming its regression. This calculator reports the mean node for your chosen date and the true node at the Moon's nearest actual crossing, with the difference between them at that same instant.

What are the ascending and descending lunar nodes?

The lunar nodes are the two points where the Moon's orbit crosses the ecliptic, the plane of Earth's orbit around the Sun. At the ascending node the Moon crosses from south of the ecliptic to north of it; at the descending node, half an orbit later, it crosses back from north to south. An eclipse can only happen when a new or full moon falls near one of these two points.

Is this astrology?

No. This calculator reports only real astronomical positions and crossing times computed from an astronomy engine, the same lunar nodes used in eclipse prediction and orbital mechanics. It makes no claims about personality, destiny, or future events, and no interpretation is offered for the mean node, true node, or any other figure on this page.

How accurate are these figures?

The true node crossings come directly from the vendored astronomy engine searching the Moon's actual position, refined to about a second of time, which is the search's stopping tolerance rather than its error: checked against JPL Horizons, this engine puts present-day crossings about 15 to 25 seconds early, so the printed minute can differ from Horizons by one. Turning that instant into UTC needs delta-T, the offset between the uniform time the ephemeris runs on and the Earth-rotation time our clocks follow, which is measured for the past but can only be extrapolated for the future: for dates decades ahead the printed minute is an extrapolation, and by 2190 this engine's delta-T model and JPL Horizons put the same crossing more than six minutes apart (measured against Horizons for this page); most of that gap is the delta-T divergence the API accuracy study measures. The mean node uses Jean Meeus's published polynomial (Astronomical Algorithms, chapter 47). The positions themselves are reliable for dates from about 1700 to 2200.