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// SPDX-License-Identifier: AGPL-3.0-only
//! Two-part (high-precision) Julian dates.
//!
//! A Julian date held in a single `f64` carries ~15–16 significant digits, so near JD
//! 2 451 545 (J2000) the least significant bit is ~50 µs — too coarse for sub-µs timing,
//! phase, and frequency-transfer work. Splitting the date into an integer **day** part and
//! a fractional **frac** part (the SOFA / hifitime two-part convention) keeps the full
//! precision of the fraction regardless of the size of the day count, so differences of
//! nearby epochs are exact to the `f64` floor.
/// Seconds in a day.
const SEC_PER_DAY: f64 = 86_400.0;
/// A Julian date as an integer day plus a fractional remainder in `[0, 1)`.
/// `JD = day + frac`, but arithmetic keeps `frac` precise independent of `day`.
#[derive(Clone, Copy, Debug, PartialEq)]
pub struct Jd2 {
/// Integer Julian day (the bulk of the magnitude).
pub day: f64,
/// Fractional day in `[0, 1)`.
pub frac: f64,
}
impl Jd2 {
/// Split a single-`f64` Julian date into its two-part form.
pub fn new(jd: f64) -> Self {
let day = jd.floor();
Self {
day,
frac: jd - day,
}
}
/// Construct from explicit parts, renormalising so `frac ∈ [0, 1)`.
pub fn from_parts(day: f64, frac: f64) -> Self {
let mut j = Self { day, frac };
j.normalize();
j
}
fn normalize(&mut self) {
let carry = self.frac.floor();
self.day += carry;
self.frac -= carry;
}
/// Advance by `seconds` (which may be negative), keeping full precision.
pub fn add_seconds(self, seconds: f64) -> Self {
Self::from_parts(self.day, self.frac + seconds / SEC_PER_DAY)
}
/// The full Julian date as a single `f64` (loses sub-`f64`-floor precision for large
/// day counts — use [`Jd2::diff_seconds`] when precision matters).
pub fn total(self) -> f64 {
self.day + self.frac
}
/// Difference `self − other` in seconds, computed part-by-part so a small difference of
/// two large dates does not lose precision (the integer days cancel exactly).
pub fn diff_seconds(self, other: Jd2) -> f64 {
((self.day - other.day) + (self.frac - other.frac)) * SEC_PER_DAY
}
}
/// Gregorian calendar date `(year, month, day)` of the integer Julian day number `jdn`
/// (the Julian date of that day's noon), by the Fliegel and Van Flandern (1968) integer
/// algorithm.
fn calendar_of_jdn(jdn: i64) -> (i32, u32, u32) {
let l = jdn + 68_569;
let n = 4 * l / 146_097;
let l = l - (146_097 * n + 3) / 4;
let i = 4_000 * (l + 1) / 1_461_001;
let l = l - 1_461 * i / 4 + 31;
let j = 80 * l / 2_447;
let day = l - 2_447 * j / 80;
let l = j / 11;
let month = j + 2 - 12 * l;
let year = 100 * (n - 49) + i + l;
(year as i32, month as u32, day as u32)
}
/// Integer Julian day number (the Julian date of noon) of a Gregorian calendar date, by the
/// Fliegel and Van Flandern (1968) integer algorithm.
fn jdn_of_calendar(year: i32, month: u32, day: u32) -> i64 {
let (y, m, d) = (year as i64, month as i64, day as i64);
let a = (m - 14) / 12;
(1_461 * (y + 4_800 + a)) / 4 + (367 * (m - 2 - 12 * a)) / 12
- (3 * ((y + 4_900 + a) / 100)) / 4
+ d
- 32_075
}
/// TAI − UTC (s) in effect from 00:00 UTC of the day whose noon is Julian day number `jdn`
/// (the integer leap-second table of [`crate::timescales`], from 1972-01-01).
fn tai_minus_utc_on(jdn: i64) -> f64 {
let (y, m, d) = calendar_of_jdn(jdn);
crate::timescales::tai_minus_utc(crate::timescales::julian_date(y, m, d, 0, 0, 0.0))
}
/// Length in seconds of the UTC day whose noon is Julian day number `jdn`: 86 400 s, plus
/// the leap second inserted at its end (86 401 s) or minus one removed.
fn utc_day_length_s(jdn: i64) -> f64 {
SEC_PER_DAY + tai_minus_utc_on(jdn + 1) - tai_minus_utc_on(jdn)
}
/// The UTC day of a two-part quasi Julian date: its Julian day number and the fraction of
/// that day elapsed since 00:00 UTC, in `[0, 1)`.
fn utc_day_and_fraction(jd: Jd2) -> (i64, f64) {
if jd.frac >= 0.5 {
(jd.day as i64 + 1, jd.frac - 0.5)
} else {
(jd.day as i64, jd.frac + 0.5)
}
}
impl Jd2 {
/// A UTC calendar date and time as a two-part UTC quasi Julian date, with the
/// convention of SOFA (Standards of Fundamental Astronomy) `iauDtf2d` for days that end in
/// a leap second: such a day is 86 401 s long, `23:59:60.x` is a valid time, and the
/// fraction of the day is counted in units of its own length. Scope: UTC from 1972-01-01
/// (the integer leap-second era); the earlier drifting-rate UTC is not modelled.
///
/// Errors on a month, day, hour or minute out of range, or a second outside `[0, 60)`
/// (`[0, 61)` in the last minute of a day that ends in a leap second).
pub fn from_utc_calendar(
year: i32,
month: u32,
day: u32,
hour: u32,
minute: u32,
second: f64,
) -> Result<Self, String> {
if !(1..=12).contains(&month) || day == 0 || day > 31 || hour > 23 || minute > 59 {
return Err(format!(
"UTC calendar date out of range: {year}-{month}-{day} {hour}:{minute}"
));
}
let jdn = jdn_of_calendar(year, month, day);
if calendar_of_jdn(jdn) != (year, month, day) {
return Err(format!("no such calendar date: {year}-{month}-{day}"));
}
let length = utc_day_length_s(jdn);
let last_minute = hour == 23 && minute == 59;
let second_limit = if last_minute {
60.0 + (length - SEC_PER_DAY)
} else {
60.0
};
if !(0.0..second_limit).contains(&second) {
return Err(format!(
"UTC second {second} out of range at {hour}:{minute}"
));
}
let elapsed = 60.0 * (60.0 * hour as f64 + minute as f64) + second;
// 00:00 UTC of the day is Julian date (jdn - 1) + 0.5.
Ok(Self::from_parts((jdn - 1) as f64, 0.5 + elapsed / length))
}
}
/// UTC (a two-part quasi Julian date, the [`Jd2::from_utc_calendar`] convention) to TAI
/// (International Atomic Time), the convention of SOFA `iauUtctai`: the fraction of a
/// leap-second day is scaled by that day's 86 401 s length before TAI − UTC is added.
pub fn utc_to_tai(utc: Jd2) -> Jd2 {
let (jdn, fd) = utc_day_and_fraction(utc);
let elapsed = fd * utc_day_length_s(jdn);
Jd2::from_parts(
(jdn - 1) as f64,
0.5 + (elapsed + tai_minus_utc_on(jdn)) / SEC_PER_DAY,
)
}
/// TAI to the UTC quasi Julian date, inverting [`utc_to_tai`] by the fixed-point iteration
/// of SOFA `iauTaiutc` (three corrections, each the TAI residual of the current guess).
pub fn tai_to_utc(tai: Jd2) -> Jd2 {
let mut guess = tai;
for _ in 0..3 {
let back = utc_to_tai(guess);
guess = Jd2::from_parts(
guess.day + (tai.day - back.day),
guess.frac + (tai.frac - back.frac),
);
}
guess
}
/// UT1 from the UTC quasi Julian date and UT1 − UTC (s), the convention of SOFA `iauUtcut1`:
/// through TAI, `UT1 = TAI + (UT1 − UTC) − (TAI − UTC)`, with TAI − UTC of the UTC day. Adding
/// UT1 − UTC to the quasi Julian date directly would be wrong by up to a second near the end of
/// a day that ends in a leap second, whose fraction counts 86 401 s.
pub fn utc_to_ut1(utc: Jd2, ut1_minus_utc_s: f64) -> Jd2 {
let (jdn, _) = utc_day_and_fraction(utc);
utc_to_tai(utc).add_seconds(ut1_minus_utc_s - tai_minus_utc_on(jdn))
}
/// TT (Terrestrial Time) from TAI: TT = TAI + 32.184 s exactly.
pub fn tai_to_tt(tai: Jd2) -> Jd2 {
tai.add_seconds(crate::timescales::TT_MINUS_TAI)
}
/// The Earth rotation angle (rad, in `[0, 2Ï€)`) at a two-part UT1 Julian date, the IAU 2000
/// expression of SOFA `iauEra00` evaluated on the two parts so the angle keeps the
/// microsecond a single-`f64` Julian date would lose (about 3e-9 rad of rotation).
pub fn earth_rotation_angle(ut1: Jd2) -> f64 {
let t = (ut1.day - crate::timescales::JD_J2000) + ut1.frac;
let turns = ut1.frac + crate::timescales::ERA_TURNS_AT_J2000 + 0.002_737_811_911_354_48 * t;
std::f64::consts::TAU * turns.rem_euclid(1.0)
}
#[cfg(test)]
mod tests {
use super::*;
#[test]
fn round_trips_a_single_f64_date() {
let jd = 2_451_545.523_4;
let j = Jd2::new(jd);
assert_eq!(j.day, 2_451_545.0);
// The fraction only carries the input's own f64 precision (~1e-9 at JD 2.45e6) —
// which is exactly the coarseness this two-part form exists to escape.
assert!((j.frac - 0.523_4).abs() < 1e-9);
assert!((j.total() - jd).abs() < 1e-9);
}
#[test]
fn from_parts_normalizes_the_fraction() {
let j = Jd2::from_parts(2_451_545.0, 1.25); // 1.25 days of fraction
assert_eq!(j.day, 2_451_546.0);
assert!((j.frac - 0.25).abs() < 1e-15);
let k = Jd2::from_parts(2_451_545.0, -0.25);
assert_eq!(k.day, 2_451_544.0);
assert!((k.frac - 0.75).abs() < 1e-15);
}
#[test]
fn preserves_microsecond_precision_a_single_f64_loses() {
// One microsecond at J2000.
let t0 = Jd2::new(2_451_545.0);
let t1 = t0.add_seconds(1.0e-6);
// The two-part difference recovers the microsecond exactly…
assert!(
(t1.diff_seconds(t0) - 1.0e-6).abs() < 1e-15,
"Δ = {}",
t1.diff_seconds(t0)
);
// …whereas the naive single-f64 JD round-trip cannot resolve it near 2.45e6.
let naive = (2_451_545.0_f64 + 1.0e-6 / SEC_PER_DAY) - 2_451_545.0;
assert!(
(naive * SEC_PER_DAY - 1.0e-6).abs() > 1.0e-7,
"single-f64 unexpectedly kept the µs: {}",
naive * SEC_PER_DAY
);
}
#[test]
fn add_seconds_is_additive_and_reversible() {
let t = Jd2::new(2_460_000.0);
let forward = t.add_seconds(3600.0).add_seconds(-3600.0);
assert!(forward.diff_seconds(t).abs() < 1e-9);
// A day of seconds advances the day count by one.
let plus_day = t.add_seconds(SEC_PER_DAY);
assert_eq!(plus_day.day, 2_460_001.0);
assert!(plus_day.frac.abs() < 1e-9);
}
#[test]
fn a_leap_second_day_is_86401_seconds_long_and_tai_steps_once() {
// 2016-12-31 ended in a leap second: 23:59:60.5 is valid, 00:00:60 is not.
let a = Jd2::from_utc_calendar(2016, 12, 31, 23, 59, 60.5).unwrap();
assert!(Jd2::from_utc_calendar(2016, 12, 30, 23, 59, 60.5).is_err());
assert!(Jd2::from_utc_calendar(2017, 2, 29, 0, 0, 0.0).is_err());
let b = Jd2::from_utc_calendar(2017, 1, 1, 0, 0, 0.0).unwrap();
// TAI advances 0.5 s from 23:59:60.5 to the next midnight; TAI - UTC goes 36 -> 37 s.
let (ta, tb) = (utc_to_tai(a), utc_to_tai(b));
assert!((tb.diff_seconds(ta) - 0.5).abs() < 1e-9);
let noon = Jd2::from_utc_calendar(2017, 1, 1, 12, 0, 0.0).unwrap();
assert_eq!((noon.day, noon.frac), (2_457_755.0, 0.0));
assert!((utc_to_tai(noon).diff_seconds(noon) - 37.0).abs() < 1e-9);
}
#[test]
fn tai_to_utc_inverts_utc_to_tai_to_the_microsecond_across_a_leap_second() {
for s in [59.0, 59.999_999, 60.0, 60.5, 60.999_999] {
let u = Jd2::from_utc_calendar(2015, 6, 30, 23, 59, s).unwrap();
let back = tai_to_utc(utc_to_tai(u));
assert!(
back.diff_seconds(u).abs() < 1e-6,
"{s}: {}",
back.diff_seconds(u)
);
}
}
#[test]
fn the_two_part_earth_rotation_angle_matches_the_single_f64_one() {
let ut1 = Jd2::from_parts(2_460_000.0, 0.273_4);
let a = earth_rotation_angle(ut1);
let b = crate::timescales::earth_rotation_angle(ut1.total());
let d =
(a - b + std::f64::consts::PI).rem_euclid(std::f64::consts::TAU) - std::f64::consts::PI;
assert!(d.abs() < 1e-8, "{d}");
}
#[test]
fn ut1_runs_through_tai_across_a_leap_second_day() {
// Across the 2016-12-31 leap second UT1 - UTC steps from about -0.6 s to +0.4 s, and
// UT1 runs on with the Earth: 1.5 s of TAI separate 23:59:59.5 from the next UTC
// midnight, and so 1.5 s of UT1 (the quasi Julian date would be off by about 1 s).
let utc = Jd2::from_utc_calendar(2016, 12, 31, 23, 59, 59.5).unwrap();
let ut1 = utc_to_ut1(utc, -0.6);
let midnight = Jd2::from_utc_calendar(2017, 1, 1, 0, 0, 0.0).unwrap();
let ut1_mid = utc_to_ut1(midnight, 0.4);
assert!(
(ut1_mid.diff_seconds(ut1) - 1.5).abs() < 1e-9,
"{}",
ut1_mid.diff_seconds(ut1)
);
// On an ordinary day it is the plain sum.
let d = Jd2::from_utc_calendar(2020, 5, 5, 12, 0, 0.0).unwrap();
assert!((utc_to_ut1(d, 0.25).diff_seconds(d) - 0.25).abs() < 1e-9);
}
}