skymath 0.3.2

Planning-grade astronomy math for astrophotography tooling: angles, equatorial coordinates, sexagesimal parsing and formatting, angular separation and offsets, precession, MJD/JD/calendar conversions, sidereal time, and observer-local quantities (alt-az, airmass, transit).
Documentation
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228
229
230
231
232
233
234
235
236
237
238
239
240
241
242
243
244
245
246
247
248
249
250
251
252
253
254
255
256
257
258
259
260
261
262
263
264
265
266
267
268
269
270
271
272
273
274
275
276
277
278
279
280
281
282
283
284
285
286
287
288
289
290
291
292
293
294
295
296
297
298
299
300
301
302
303
304
305
306
307
308
309
310
311
312
313
314
315
316
317
318
319
320
321
322
323
324
325
326
327
328
329
330
331
332
333
334
335
336
337
338
339
340
341
342
343
344
345
346
347
348
349
350
351
352
353
354
355
356
357
358
359
360
361
362
363
364
365
366
367
368
369
370
371
372
373
374
375
376
377
378
379
380
381
382
383
384
385
386
387
388
389
390
391
392
393
394
395
396
397
398
399
400
401
402
403
404
405
406
407
408
409
410
411
412
413
414
415
416
417
418
419
420
421
//! Lunar position, separation, illumination, rise/set, and moon-avoidance.
//!
//! Provenance: the geocentric position implements the truncated ELP-2000/82
//! theory of Meeus, *Astronomical Algorithms* 2nd ed., ch. 47; the periodic
//! term tables (47.A / 47.B) are ported from `saurvs/astro-rust`
//! (`src/lunar.rs`, MIT — see `NOTICE`).
//! Topocentric correction is Meeus ch. 40 (written fresh); illumination is
//! Meeus ch. 48; the moon-avoidance Lorentzian is the classic ACP/Berry
//! criterion. Accuracy: ~10″ (λ) / 4″ (β) geocentric truncation; treating
//! UTC as dynamical time adds ≤ ~40″ (the Moon moves ~0.55″/s of ΔT) — the
//! documented public claim is ≤2′ vs AstroPy, comfortably absorbed by the
//! planning contract for site-relative use once parallax (up to ~61′!) is
//! corrected via [`moon_position_topocentric`].

use ::time::OffsetDateTime;

use crate::angle::Angle;
use crate::coords::{precess, separation, Equatorial};
use crate::frames::mean_obliquity;
use crate::observer::{moving_body_crossings, CrossingOutcome, Location};
use crate::sun::solar_coords;
use crate::time::{julian_date, julian_epoch_of, lst};

const J2000_JD: f64 = 2_451_545.0;
/// Kilometres per astronomical unit (IAU 2012).
const KM_PER_AU: f64 = 149_597_870.7;
/// Mean synodic elongation rate of the Moon from the Sun, degrees/day.
const SYNODIC_RATE_DEG_PER_DAY: f64 = 12.190_749;

/// Periodic terms for lunar longitude (Σl, 1e-6 °) and distance (Σr, 1e-3 km):
/// multiples of (D, M, M′, F) with the two coefficients.
/// Meeus table 47.A, ported from astro-rust `lunar.rs`.
#[rustfmt::skip]
const LR_TERMS: [(i8, i8, i8, i8, i32, i32); 60] = [
    (0, 0, 1, 0, 6_288_774, -20_905_355), (2, 0, -1, 0, 1_274_027, -3_699_111),
    (2, 0, 0, 0, 658_314, -2_955_968),    (0, 0, 2, 0, 213_618, -569_925),
    (0, 1, 0, 0, -185_116, 48_888),       (0, 0, 0, 2, -114_332, -3_149),
    (2, 0, -2, 0, 58_793, 246_158),       (2, -1, -1, 0, 57_066, -152_138),
    (2, 0, 1, 0, 53_322, -170_733),       (2, -1, 0, 0, 45_758, -204_586),
    (0, 1, -1, 0, -40_923, -129_620),     (1, 0, 0, 0, -34_720, 108_743),
    (0, 1, 1, 0, -30_383, 104_755),       (2, 0, 0, -2, 15_327, 10_321),
    (0, 0, 1, 2, -12_528, 0),             (0, 0, 1, -2, 10_980, 79_661),
    (4, 0, -1, 0, 10_675, -34_782),       (0, 0, 3, 0, 10_034, -23_210),
    (4, 0, -2, 0, 8_548, -21_636),        (2, 1, -1, 0, -7_888, 24_208),
    (2, 1, 0, 0, -6_766, 30_824),         (1, 0, -1, 0, -5_163, -8_379),
    (1, 1, 0, 0, 4_987, -16_675),         (2, -1, 1, 0, 4_036, -12_831),
    (2, 0, 2, 0, 3_994, -10_445),         (4, 0, 0, 0, 3_861, -11_650),
    (2, 0, -3, 0, 3_665, 14_403),         (0, 1, -2, 0, -2_689, -7_003),
    (2, 0, -1, 2, -2_602, 0),             (2, -1, -2, 0, 2_390, 10_056),
    (1, 0, 1, 0, -2_348, 6_322),          (2, -2, 0, 0, 2_236, -9_884),
    (0, 1, 2, 0, -2_120, 5_751),          (0, 2, 0, 0, -2_069, 0),
    (2, -2, -1, 0, 2_048, -4_950),        (2, 0, 1, -2, -1_773, 4_130),
    (2, 0, 0, 2, -1_595, 0),              (4, -1, -1, 0, 1_215, -3_958),
    (0, 0, 2, 2, -1_110, 0),              (3, 0, -1, 0, -892, 3_258),
    (2, 1, 1, 0, -810, 2_616),            (4, -1, -2, 0, 759, -1_897),
    (0, 2, -1, 0, -713, -2_117),          (2, 2, -1, 0, -700, 2_354),
    (2, 1, -2, 0, 691, 0),                (2, -1, 0, -2, 596, 0),
    (4, 0, 1, 0, 549, -1_423),            (0, 0, 4, 0, 537, -1_117),
    (4, -1, 0, 0, 520, -1_571),           (1, 0, -2, 0, -487, -1_739),
    (2, 1, 0, -2, -399, 0),               (0, 0, 2, -2, -381, -4_421),
    (1, 1, 1, 0, 351, 0),                 (3, 0, -2, 0, -340, 0),
    (4, 0, -3, 0, 330, 0),                (2, -1, 2, 0, 327, 0),
    (0, 2, 1, 0, -323, 1_165),            (1, 1, -1, 0, 299, 0),
    (2, 0, 3, 0, 294, 0),                 (2, 0, -1, -2, 0, 8_752),
];

/// Periodic terms for lunar latitude (Σb, 1e-6 °). Meeus table 47.B, ported
/// from astro-rust `lunar.rs`.
#[rustfmt::skip]
const B_TERMS: [(i8, i8, i8, i8, i32); 60] = [
    (0, 0, 0, 1, 5_128_122), (0, 0, 1, 1, 280_602),  (0, 0, 1, -1, 277_693),
    (2, 0, 0, -1, 173_237),  (2, 0, -1, 1, 55_413),  (2, 0, -1, -1, 46_271),
    (2, 0, 0, 1, 32_573),    (0, 0, 2, 1, 17_198),   (2, 0, 1, -1, 9_266),
    (0, 0, 2, -1, 8_822),    (2, -1, 0, -1, 8_216),  (2, 0, -2, -1, 4_324),
    (2, 0, 1, 1, 4_200),     (2, 1, 0, -1, -3_359),  (2, -1, -1, 1, 2_463),
    (2, -1, 0, 1, 2_211),    (2, -1, -1, -1, 2_065), (0, 1, -1, -1, -1_870),
    (4, 0, -1, -1, 1_828),   (0, 1, 0, 1, -1_794),   (0, 0, 0, 3, -1_749),
    (0, 1, -1, 1, -1_565),   (1, 0, 0, 1, -1_491),   (0, 1, 1, 1, -1_475),
    (0, 1, 1, -1, -1_410),   (0, 1, 0, -1, -1_344),  (1, 0, 0, -1, -1_335),
    (0, 0, 3, 1, 1_107),     (4, 0, 0, -1, 1_021),   (4, 0, -1, 1, 833),
    (0, 0, 1, -3, 777),      (4, 0, -2, 1, 671),     (2, 0, 0, -3, 607),
    (2, 0, 2, -1, 596),      (2, -1, 1, -1, 491),    (2, 0, -2, 1, -451),
    (0, 0, 3, -1, 439),      (2, 0, 2, 1, 422),      (2, 0, -3, -1, 421),
    (2, 1, -1, 1, -366),     (2, 1, 0, 1, -351),     (4, 0, 0, 1, 331),
    (2, -1, 1, 1, 315),      (2, -2, 0, -1, 302),    (0, 0, 1, 3, -283),
    (2, 1, 1, -1, -229),     (1, 1, 0, -1, 223),     (1, 1, 0, 1, 223),
    (0, 1, -2, -1, -220),    (2, 1, -1, -1, -220),   (1, 0, 1, 1, -185),
    (2, -1, -2, -1, 181),    (0, 1, 2, 1, -177),     (4, 0, -2, -1, 176),
    (4, -1, -1, -1, 166),    (1, 0, 1, -1, -164),    (4, 0, 1, -1, 132),
    (1, 0, -1, -1, -119),    (4, -1, 0, -1, 115),    (2, -2, 0, 1, 107),
];

/// Geocentric ecliptic λ, β (degrees, mean equinox of date) and distance Δ
/// (km) at `at` — Meeus ch. 47.
pub(crate) fn lunar_coords(at: OffsetDateTime) -> (f64, f64, f64) {
    let t = (julian_date(at) - J2000_JD) / 36_525.0;

    // Fundamental arguments (Meeus 47.1–47.6), degrees.
    let l1 = 218.316_447_7 + 481_267.881_234_21 * t - 0.001_578_6 * t * t + t * t * t / 538_841.0
        - t * t * t * t / 65_194_000.0;
    let d = 297.850_192_1 + 445_267.111_403_4 * t - 0.001_881_9 * t * t + t * t * t / 545_868.0
        - t * t * t * t / 113_065_000.0;
    let m = 357.529_109_2 + 35_999.050_290_9 * t - 0.000_153_6 * t * t + t * t * t / 24_490_000.0;
    let m1 = 134.963_396_4 + 477_198.867_505_5 * t + 0.008_741_4 * t * t + t * t * t / 69_699.0
        - t * t * t * t / 14_712_000.0;
    let f = 93.272_095_0 + 483_202.017_523_3 * t - 0.003_653_9 * t * t - t * t * t / 3_526_000.0
        + t * t * t * t / 863_310_000.0;
    let e = 1.0 - 0.002_516 * t - 0.000_007_4 * t * t;

    let a1 = (119.75 + 131.849 * t).to_radians();
    let a2 = (53.09 + 479_264.29 * t).to_radians();
    let a3 = (313.45 + 481_266.484 * t).to_radians();
    let (l1_rad, d, m, m1, f) = (
        l1.to_radians(),
        d.to_radians(),
        m.to_radians(),
        m1.to_radians(),
        f.to_radians(),
    );

    let ecc = |mult: i8| match mult.abs() {
        1 => e,
        2 => e * e,
        _ => 1.0,
    };

    let (mut sum_l, mut sum_r, mut sum_b) = (0.0, 0.0, 0.0);
    for &(td, tm, tm1, tf, cl, cr) in &LR_TERMS {
        let arg = f64::from(td) * d + f64::from(tm) * m + f64::from(tm1) * m1 + f64::from(tf) * f;
        sum_l += f64::from(cl) * ecc(tm) * arg.sin();
        sum_r += f64::from(cr) * ecc(tm) * arg.cos();
    }
    for &(td, tm, tm1, tf, cb) in &B_TERMS {
        let arg = f64::from(td) * d + f64::from(tm) * m + f64::from(tm1) * m1 + f64::from(tf) * f;
        sum_b += f64::from(cb) * ecc(tm) * arg.sin();
    }

    // Additive corrections (Venus, Jupiter, flattening terms).
    sum_l += 3_958.0 * a1.sin() + 1_962.0 * (l1_rad - f).sin() + 318.0 * a2.sin();
    sum_b += -2_235.0 * l1_rad.sin()
        + 382.0 * a3.sin()
        + 175.0 * ((a1 - f).sin() + (a1 + f).sin())
        + 127.0 * (l1_rad - m1).sin()
        - 115.0 * (l1_rad + m1).sin();

    let lambda = (l1 + sum_l / 1e6).rem_euclid(360.0);
    let beta = sum_b / 1e6;
    let delta_km = 385_000.56 + sum_r / 1e3;
    (lambda, beta, delta_km)
}

/// Ecliptic-of-date (λ, β) → equatorial-of-date, via the mean obliquity.
fn ecliptic_to_equatorial(lambda_deg: f64, beta_deg: f64, at: OffsetDateTime) -> Equatorial {
    let (l, b) = (lambda_deg.to_radians(), beta_deg.to_radians());
    let eps = mean_obliquity(at);
    let ra = (l.sin() * eps.cos() - b.tan() * eps.sin()).atan2(l.cos());
    let dec = (b.sin() * eps.cos() + b.cos() * eps.sin() * l.sin())
        .clamp(-1.0, 1.0)
        .asin();
    Equatorial::at_epoch(
        Angle::from_radians(ra).normalized_0_360(),
        Angle::from_radians(dec),
        julian_epoch_of(at),
    )
    .expect("rotation output is in domain by construction")
}

/// Geocentric lunar position (equatorial, epoch of date).
///
/// Truncated ELP-2000/82 (Meeus ch. 47): ~10″ in longitude against the full
/// theory; documented public claim ≤2′ vs AstroPy (which uses a fuller
/// theory; treating UTC as dynamical time contributes ≤ ~40″). For anything
/// site-relative use [`moon_position_topocentric`] — lunar parallax reaches
/// ~61′.
///
/// ```
/// use skymath::moon_position;
/// use time::OffsetDateTime;
///
/// let geocentric = moon_position(OffsetDateTime::now_utc());
/// assert!(geocentric.dec().degrees().abs() <= 90.0);
/// ```
pub fn moon_position(at: OffsetDateTime) -> Equatorial {
    let (lambda, beta, _) = lunar_coords(at);
    ecliptic_to_equatorial(lambda, beta, at)
}

/// Moon–Earth centre distance in kilometres.
///
/// ```
/// use skymath::moon_distance_km;
/// use time::macros::datetime;
///
/// // Meeus example 47.a.
/// let km = moon_distance_km(datetime!(1992-04-12 00:00 UTC));
/// assert!((km - 368_409.7).abs() < 1.0);
/// ```
pub fn moon_distance_km(at: OffsetDateTime) -> f64 {
    lunar_coords(at).2
}

/// Topocentric lunar position for an observer (equatorial, epoch of date) —
/// Meeus ch. 40 parallax correction with WGS-84-flattened site coordinates.
/// The shift from [`moon_position`] (geocentric) can reach ~61′ (the Moon's
/// horizontal parallax).
///
/// ```
/// use skymath::{moon_position, moon_position_topocentric, separation, Location};
/// use time::OffsetDateTime;
///
/// let site = Location::parse("+52 05 32", "+004 18 27", 6.0)?;
/// let now = OffsetDateTime::now_utc();
/// let parallax_shift = separation(moon_position(now), moon_position_topocentric(now, &site));
/// assert!(parallax_shift.arcminutes() <= 62.0);
/// # Ok::<(), skymath::Error>(())
/// ```
pub fn moon_position_topocentric(at: OffsetDateTime, site: &Location) -> Equatorial {
    let (lambda, beta, delta_km) = lunar_coords(at);
    let geocentric = ecliptic_to_equatorial(lambda, beta, at);
    let (ra, dec) = (geocentric.ra().radians(), geocentric.dec().radians());

    // Observer's geocentric coordinates (Meeus ch. 11).
    let phi = site.latitude().radians();
    let u = (0.996_647_19 * phi.tan()).atan();
    let h_frac = site.elevation_m() / 6_378_140.0;
    let rho_sin = 0.996_647_19 * u.sin() + h_frac * phi.sin();
    let rho_cos = u.cos() + h_frac * phi.cos();

    // Equatorial horizontal parallax and local hour angle.
    let sin_pi = 6_378.14 / delta_km;
    let h = (lst(at, site.longitude()) - geocentric.ra())
        .normalized_pm_180()
        .radians();

    // Meeus 40.2 / 40.3.
    let delta_ra = (-rho_cos * sin_pi * h.sin()).atan2(dec.cos() - rho_cos * sin_pi * h.cos());
    let dec_top = ((dec.sin() - rho_sin * sin_pi) * delta_ra.cos())
        .atan2(dec.cos() - rho_cos * sin_pi * h.cos());

    Equatorial::at_epoch(
        Angle::from_radians(ra + delta_ra).normalized_0_360(),
        Angle::from_radians(dec_top),
        julian_epoch_of(at),
    )
    .expect("parallax correction stays in domain")
}

/// Great-circle separation between the topocentric Moon and `target` at an
/// instant. The target is precessed to the epoch of date internally, matching
/// the observer-module semantics.
///
/// ```
/// use skymath::{lunar_separation, Equatorial, Location, ParseMode};
/// use time::OffsetDateTime;
///
/// let m31 = Equatorial::parse_j2000("00:42:44.3", "+41:16:09", ParseMode::Strict)?;
/// let site = Location::parse("+52 05 32", "+004 18 27", 6.0)?;
/// let sep = lunar_separation(m31, OffsetDateTime::now_utc(), &site);
/// assert!((0.0..=180.0).contains(&sep.degrees()));
/// # Ok::<(), skymath::Error>(())
/// ```
pub fn lunar_separation(target: Equatorial, at: OffsetDateTime, site: &Location) -> Angle {
    let target = precess(target, julian_epoch_of(at));
    separation(moon_position_topocentric(at, site), target)
}

/// When the topocentric Moon rises above and sets below `threshold` altitude,
/// around the lunar transit nearest `night_of` (moving-body iteration of the
/// analytic solver; the Moon moves ~13°/day). Matches astroplan within ±3 min.
///
/// ```
/// use skymath::{moon_crossings, Angle, CrossingOutcome, Location};
/// use time::OffsetDateTime;
///
/// let site = Location::parse("+52 05 32", "+004 18 27", 6.0)?;
/// match moon_crossings(Angle::from_degrees(0.0), OffsetDateTime::now_utc(), &site) {
///     CrossingOutcome::Crosses { rise, set } => println!("Moon: {rise} -> {set}"),
///     outcome => println!("{outcome:?}"),
/// }
/// # Ok::<(), skymath::Error>(())
/// ```
pub fn moon_crossings(
    threshold: Angle,
    night_of: OffsetDateTime,
    site: &Location,
) -> CrossingOutcome {
    moving_body_crossings(
        |t| moon_position_topocentric(t, site),
        threshold,
        night_of,
        site,
        0.0,
    )
}

/// The Moon's phase angle `i` (Sun–Moon–Earth angle, Meeus ch. 48 exact
/// form): 0° at full Moon, 180° at new. Feeds [`moon_illumination`] and
/// [`moon_avoidance_lorentzian`].
///
/// ```
/// use skymath::moon_phase_angle;
/// use time::macros::datetime;
///
/// // Meeus example 48.a.
/// let i = moon_phase_angle(datetime!(1992-04-12 00:00 UTC)).degrees();
/// assert!((i - 69.0756).abs() < 0.05);
/// ```
pub fn moon_phase_angle(at: OffsetDateTime) -> Angle {
    let (_, sun_r_au, _) = solar_coords(at);
    let r = sun_r_au * KM_PER_AU;
    let (lambda, beta, delta) = lunar_coords(at);
    // Geocentric elongation between the apparent Sun and Moon.
    let psi = separation(
        crate::sun::sun_position(at),
        ecliptic_to_equatorial(lambda, beta, at),
    )
    .radians();
    Angle::from_radians((r * psi.sin()).atan2(delta - r * psi.cos()))
}

/// Illuminated fraction of the Moon's disk, `k = (1 + cos i) / 2` ∈ [0, 1],
/// derived from [`moon_phase_angle`].
///
/// ```
/// use skymath::moon_illumination;
/// use time::macros::datetime;
///
/// // Meeus example 48.a.
/// let k = moon_illumination(datetime!(1992-04-12 00:00 UTC));
/// assert!((k - 0.6786).abs() < 0.005);
/// ```
pub fn moon_illumination(at: OffsetDateTime) -> f64 {
    (1.0 + moon_phase_angle(at).radians().cos()) / 2.0
}

/// The classic moon-avoidance Lorentzian (ACP/Berry): the required minimum
/// target–Moon separation at `at`, largest at full Moon and relaxing with
/// lunar age:
///
/// `S(d) = separation_at_full / (1 + (d / half_width_days)²)`
///
/// where `d` is the time from full Moon in days, derived from the phase angle
/// via the mean synodic rate. At full Moon it returns `separation_at_full`;
/// `half_width_days` from full it returns half of it.
///
/// ```
/// use skymath::{moon_avoidance_lorentzian, Angle};
/// use time::OffsetDateTime;
///
/// let min_separation =
///     moon_avoidance_lorentzian(Angle::from_degrees(60.0), 7.0, OffsetDateTime::now_utc());
/// assert!((0.0..=60.0).contains(&min_separation.degrees()));
/// ```
pub fn moon_avoidance_lorentzian(
    separation_at_full: Angle,
    half_width_days: f64,
    at: OffsetDateTime,
) -> Angle {
    let days_from_full = moon_phase_angle(at).degrees().abs() / SYNODIC_RATE_DEG_PER_DAY;
    let h = half_width_days.max(f64::MIN_POSITIVE);
    separation_at_full / (1.0 + (days_from_full / h).powi(2))
}

#[cfg(test)]
mod tests {
    use super::*;
    use ::time::macros::datetime;

    #[test]
    fn meeus_47a_lunar_position() {
        // Meeus example 47.a — 1992-04-12T00:00 TD (same numeric JD fed as
        // UTC, so the comparison pins the series itself, not ΔT):
        // λ = 133.162655°, β = −3.229126°, Δ = 368409.7 km.
        let (lambda, beta, delta) = lunar_coords(datetime!(1992-04-12 00:00 UTC));
        assert!((lambda - 133.162_655).abs() * 3600.0 < 1.0, "λ = {lambda}");
        assert!((beta + 3.229_126).abs() * 3600.0 < 1.0, "β = {beta}");
        assert!((delta - 368_409.7).abs() < 1.0, "Δ = {delta}");
        // Horizontal parallax π = 0.991990°.
        let pi = (6_378.14 / delta).asin().to_degrees();
        assert!((pi - 0.991_990).abs() < 1e-5, "π = {pi}");
    }

    #[test]
    fn topocentric_parallax_has_the_expected_magnitude() {
        // For a mid-latitude site with the Moon well above the horizon the
        // topocentric shift is a large fraction of the ~57′ mean horizontal
        // parallax — and never exceeds it.
        let site =
            Location::new(Angle::from_degrees(52.155), Angle::from_degrees(4.485), 6.0).unwrap();
        let at = datetime!(2026-07-11 22:00 UTC);
        let shift = separation(moon_position(at), moon_position_topocentric(at, &site));
        assert!(
            (10.0..62.0).contains(&shift.arcminutes()),
            "parallax shift {}′",
            shift.arcminutes()
        );
    }

    #[test]
    fn meeus_48a_illumination() {
        // Meeus example 48.a — 1992-04-12T00:00 TD: i = 69.0756°, k = 0.6786.
        let at = datetime!(1992-04-12 00:00 UTC);
        let i = moon_phase_angle(at).degrees();
        assert!((i - 69.075_6).abs() < 0.05, "i = {i}");
        let k = moon_illumination(at);
        assert!((k - 0.678_6).abs() < 0.005, "k = {k}");
    }

    #[test]
    fn avoidance_lorentzian_shape() {
        let at = datetime!(2026-07-11 22:00 UTC);
        let s = Angle::from_degrees(60.0);
        let d = moon_phase_angle(at).degrees().abs() / SYNODIC_RATE_DEG_PER_DAY;
        // Evaluated at the current instant the formula must equal the closed
        // form exactly.
        let expect = 60.0 / (1.0 + (d / 7.0_f64).powi(2));
        assert!((moon_avoidance_lorentzian(s, 7.0, at).degrees() - expect).abs() < 1e-9);
        // Degenerate half-width never divides by zero.
        assert!(moon_avoidance_lorentzian(s, 0.0, at).degrees() >= 0.0);
    }
}