← data.backThe Science Behind Your Star
Every star we identify comes from a documented calculation you can check yourself. This page explains, in plain language, how the sky of one moment is reconstructed — the coordinates, the time conversion, the star catalog and the selection rule — including the parts we deliberately do not model.
A Star Named is an astronomical memorial service that reconstructs the sky at the recorded time and location of a person’s or pet’s passing and identifies the star closest to the zenith.
1. Location — where the sky is measured from
The place you enter is resolved to a latitude and a longitude. Latitude fixes which part of the sky passes overhead: at any instant the zenith’s declination equals the observer’s latitude. Longitude shifts local time and the sky’s rotation angle — it decides when that point comes overhead (section 3).
Elevation is not used — and here is why
We do not adjust for height above sea level. Altitude changes sunrise and sunset by a minute or two, but the star we identify lies within a few degrees of the zenith, where elevation has practically no effect. It also means we never ask you for a number you may not know. If a moment falls exactly at dawn or dusk, elevation could in principle shift the pick — we accept that small uncertainty instead of inventing precision.
2. Time — from a clock reading to an instant in UTC
You enter the local civil time at that place — the time that was on the clock. We convert it to UTC using the IANA timezone database, which carries the real history of clock rules for the region, including daylight saving. Every astronomical computation then runs on UTC alone.
- Daylight saving is handled from the database: the same clock reading means a different instant in summer and winter, and the correct one is used for your date.
- Impossible times are refused, not guessed: if the wall-clock time you enter never existed on that date (the hour skipped when daylight saving begins), the calculator asks you to adjust rather than silently computing a different moment.
- Incomplete records are corrected and disclosed: for daylight saving in China, 1986–1991 — a real period that today’s timezone databases omit — we apply a documented correction so the sky is still right.
- Historical dates: before standard time was adopted (the date varies by country; for the United States it was 1883), towns kept local mean time — solar time, not clock time. Databases model that era inconsistently, so on historical pages we record a confidence level for every date and time, and where the time is not documented we say so instead of guessing.
3. The astronomical calculation — sidereal time, hour angle, altitude, azimuth
Given an instant in UTC, a latitude and a longitude, we find the point of the sky directly overhead:
- The instant is converted to a Julian Date, the standard day-count that astronomical formulas take as input.
- Greenwich Mean Sidereal Time (GMST) is computed from the standard IAU 1982 polynomial — the sky’s rotation angle, in degrees.
- Local Sidereal Time (LST) = GMST + east longitude. LST is the right ascension currently crossing your meridian, the north–south line through the zenith.
- The zenith of that instant: right ascension = LST, declination = latitude. This single point is what we match against the catalog.
- Because the catalog is stored in J2000 coordinates, the zenith point is precessed back from the epoch of the date to J2000 with the IAU 1976 precession model — for a 2026 moment that shift is about 0.37°, far too large to ignore.
- Altitude is the angle above the horizon (the zenith is altitude 90°); azimuth is the compass bearing measured from true north through east; the hour angle measures how far the sky has turned since an object crossed the meridian (15° per hour). These are the coordinates we use to show your star’s position and its visibility windows.
- Deliberately not modelled: nutation, aberration and polar motion — together well under 0.02°, an order of magnitude below the typical separation between neighbouring stars. We state the error budget instead of pretending to precision we do not need.
4. The star catalog — HYG v4.1
Candidates come from the HYG catalog, a real public catalog merging the Hipparcos, Gliese and Yale surveys: J2000 positions (RA/Dec), distances from parallax, brightness and spectral type. We include 107,838 stars covering all 88 IAU constellations; every record is traceable to its source IDs. The full accounting lives on our data page.
The catalog spans magnitude 0.03 to magnitude 12 — far below the naked-eye limit of about 6.5. The star nearest the zenith is often a faint one. That is the honest trade-off of choosing by position rather than brightness, and your certificate states the magnitude so you know what to expect.
One more honest note: positions are stored at epoch J2000, and we do not yet propagate each star’s proper motion to the date of observation. For nearly every star that amounts to a few arc-seconds over a human lifetime — far below the selection resolution — but for a handful of very fast nearby stars it can matter. The correction code is in place; it will be switched on as proper-motion values are added to the catalog rows.
5. Choosing the star — the exact rule
Stated the way it is implemented:
- Take every catalog star whose declination is within 15° of the zenith’s declination — a wide-margin speed filter; the nearest star is never near the band edge.
- For each candidate, compute the angular distance from the zenith by spherical trigonometry.
- Choose the smallest angular distance: the real star closest to the zenith.
- Skip stars that are already named — each real star is used only once. On an exact tie in distance, the star closer to Earth wins.
- The same inputs always produce the same star: no randomness, no human touch. The chosen star’s catalog IDs and coordinates are printed on the certificate.
6. Check it yourself
You do not have to take any of this on faith — Stellarium (free and open source) or any planetarium app can confirm the result:
- Set the same date, time and location you entered.
- Look straight up: that point is the zenith. With the equatorial grid on, you can read its coordinates.
- Find the star by the catalog ID printed on your certificate (HIP number or similar) — it should sit nearest the zenith, at the angular distance your certificate reports.
7. Known limitations
- Mean positions only: nutation, aberration and polar motion are not modelled (together well under 0.02°).
- Proper motion is not propagated; it matters only for a few very fast nearby stars.
- Elevation above sea level is not used (section 1).
- Historical timekeeping varies by region and era; historical pages carry a confidence level per date, and we do not publish a star for a historical moment whose time of day is not documented.
- Visibility is computed geometrically (altitude > 0°); atmospheric refraction near the horizon is not applied. The star is identified by position, not brightness — it is usually too faint for the naked eye.