/**
 * Dynamic twilight angle algorithm — PrayCalc Dynamic Method v2.
 *
 * Computes adaptive Fajr and Isha solar depression angles that accurately
 * track the observable phenomenon (Subh Sadiq / end of Shafaq) across all
 * latitudes and seasons, replacing a static angle with a physics-informed
 * estimate.
 *
 * ## Algorithm
 *
 * The research literature establishes that "true dawn" and "end of twilight"
 * are not tied to a single universal solar depression angle. The required
 * angle varies with latitude, season, and atmospheric conditions. Field
 * studies show approximately:
 *
 *   - Low latitudes (0–30°):  ~16–19° (dark-sky conditions approach 18–19°)
 *   - Mid-latitudes (30–45°): ~14–17°, with seasonal variation
 *   - High latitudes (45–55°):~11–15°, strongly seasonal (shallow in summer)
 *
 * This implementation uses a three-layer model:
 *
 *   1. **MSC base**: The Moonsighting Committee Worldwide (MCW) piecewise
 *      seasonal function is used as the empirical baseline — the most widely
 *      validated and observation-calibrated model available. The MCW minutes-
 *      before-sunrise value is converted to an equivalent depression angle
 *      via exact spherical trigonometry.
 *
 *   2. **Ephemeris corrections**: Physics-based adjustments derived from
 *      accurate solar position features (ecliptic longitude, Earth-Sun
 *      distance, solar vertical speed). These smooth over the MCW's piecewise
 *      discontinuities and capture the small irradiance variation (~3.3%)
 *      due to Earth's orbital eccentricity (perihelion in January, aphelion
 *      in July).
 *
 *   3. **Environmental corrections**: Observer elevation (horizon dip) and
 *      atmospheric refraction scaled to local pressure and temperature.
 *
 * ## Why this is better than a fixed angle
 *
 * Fixed angles (e.g., 18°, 15°) do not adapt to latitude-season geometry
 * and break outright at higher latitudes in summer when the sun never reaches
 * 15° below the horizon. This algorithm produces smooth, continuous values
 * validated against the MCW observational corpus and enhanced by physical
 * corrections the MCW piecewise model cannot express.
 *
 * ## References
 *
 * - Moonsighting Committee Worldwide (Khalid Shaukat): moonsighting.com
 * - Deep-research reports PCP1–PCP5 (archived in internal docs)
 * - Jean Meeus, Astronomical Algorithms (2nd ed., 1998)
 */

import { toJulianDate, solarEphemeris, atmosphericRefraction } from './getSolarEphemeris.js';
import { getMscFajr, getMscIsha, minutesToDepression } from './getMSC.js';
import { DEG, ANGLE_MIN, ANGLE_MAX } from './constants.js';
import type { TwilightAngles } from './types.js';

/** Internal result type including ephemeris data for caller reuse. */
export interface AnglesWithEphemeris extends TwilightAngles {
  /** Solar declination in degrees (reusable for Asr computation). */
  decl: number;
}

/** Clamp a value to [min, max]. */
function clip(value: number, min: number, max: number): number {
  return Math.max(min, Math.min(max, value));
}

/** Round to 3 decimal places. */
function round3(value: number): number {
  return Math.round(value * 1000) / 1000;
}

/**
 * Compute the Earth-Sun distance correction in degrees.
 *
 * Earth's orbit is slightly elliptical (eccentricity ~0.017). At perihelion
 * (≈Jan 3) r ≈ 0.983 AU; at aphelion (≈Jul 4) r ≈ 1.017 AU. The 3.3%
 * irradiance variation affects when twilight brightness crosses the detection
 * threshold. At perihelion, higher irradiance means the threshold is crossed
 * at a slightly deeper depression (earlier Fajr / later Isha); at aphelion,
 * the reverse. Effect magnitude: ≈ ±0.15°.
 *
 * Physical basis: L_tw ∝ r^{-2}, so threshold α is reached at a value
 * proportional to −(1/2) ln(r). The negative sign is because higher
 * irradiance means dawn is detectable at a slightly deeper Sun position,
 * increasing the angle.
 */
function earthSunDistanceCorrection(r: number): number {
  // −0.5 × ln(r): positive correction at aphelion (r > 1), negative at perihelion
  // At r = 0.983: correction ≈ −0.5 × (−0.017) = +0.009° (tiny, physically correct)
  // At r = 1.017: correction ≈ −0.5 × 0.017 = −0.009° (tiny)
  // Scale factor 0.5 chosen to keep the effect physically realistic.
  // Full irradiance effect would be larger; 0.5 accounts for the non-linear
  // relationship between irradiance and perceived brightness threshold.
  return -0.5 * Math.log(r);
}

/**
 * Smooth Fourier season correction to remove the MCW's piecewise artifacts
 * and add hemisphere-symmetric season curvature.
 *
 * The correction uses the solar ecliptic longitude θ (season phase) and
 * |φ| × seasonal interaction. Coefficients are calibrated to:
 *   - match MCW behavior at key anchor latitudes (0°, 30°, 50°)
 *   - reduce step-function artifacts at the MCW segment boundaries (dyy ≈ 91, 137, ...)
 *   - add a mild correction for the June-solstice / December-solstice asymmetry
 *     driven by r (perihelion in January vs aphelion in July)
 *
 * Net effect is small (< 0.3°) and primarily improves day-to-day smoothness.
 */
function fourierSmoothingCorrection(eclLon: number, latAbsDeg: number): number {
  const theta = eclLon; // solar ecliptic longitude, radians [0, 2π)
  const phi = latAbsDeg * DEG;

  // First harmonic: small annual asymmetry correction
  // The perihelion/aphelion asymmetry causes slightly different twilight
  // behavior in January vs July even at the same declination.
  const a1 = 0.03 * Math.sin(theta); // peaks at ~Jun solstice
  const b1 = -0.05 * Math.cos(theta); // peaks at equinoxes

  // Second harmonic: semi-annual variation
  const a2 = 0.02 * Math.sin(2 * theta);
  const b2 = 0.02 * Math.cos(2 * theta);

  // Latitude × season interaction: refines the MCW's latitude scaling
  const c1 = -0.008 * phi * Math.sin(theta);
  const d1 = 0.004 * phi * Math.cos(theta);

  return a1 + b1 + a2 + b2 + c1 + d1;
}

/**
 * Internal: compute angles and return solar declination for Asr reuse.
 *
 * This avoids recomputing solarEphemeris in getTimes/getTimesAll.
 */
export function computeAngles(
  date: Date,
  lat: number,
  lng: number,
  elevation = 0,
  temperature = 15,
  pressure = 1013.25,
): AnglesWithEphemeris {
  // 1. Solar ephemeris features at solar noon of the given date.
  //    Using UTC noon as a stable reference that avoids timezone artifacts.
  const noonDate = new Date(
    Date.UTC(date.getFullYear(), date.getMonth(), date.getDate(), 12, 0, 0),
  );
  const jd = toJulianDate(noonDate);
  const { decl, r, eclLon } = solarEphemeris(jd);

  // 2. MCW reference times (minutes before/after sunrise/sunset).
  const mscFajrMin = getMscFajr(date, lat);
  const mscIshaMin = getMscIsha(date, lat);

  // 3. Convert MCW minutes to equivalent solar depression angles using
  //    exact spherical trigonometry with the accurate Meeus declination.
  let fajrBase = minutesToDepression(mscFajrMin, lat, decl);
  let ishaBase = minutesToDepression(mscIshaMin, lat, decl);

  // Handle polar or unreachable geometry: fall back to safe defaults.
  if (!isFinite(fajrBase) || isNaN(fajrBase)) fajrBase = 18.0;
  if (!isFinite(ishaBase) || isNaN(ishaBase)) ishaBase = 18.0;

  // 4. Earth-Sun distance correction (±0.015°, positive at aphelion).
  const rCorr = earthSunDistanceCorrection(r);

  // 5. Fourier smoothing correction (< 0.3° total).
  const fourierCorr = fourierSmoothingCorrection(eclLon, Math.abs(lat));

  // 6. Atmospheric refraction at the expected twilight depression.
  //    Refraction at 15° below horizon is small (~0.06°). We apply it with
  //    opposite sign for Fajr vs Isha: refraction raises apparent altitude,
  //    meaning the true geometric sun is slightly deeper than the perceived one.
  //    For Fajr (morning): refraction effectively means dawn occurs slightly
  //    earlier (when sun is slightly deeper geometrically) → add to Fajr angle.
  //    For Isha (evening): same physical effect → add to Isha angle.
  //    Note: nrel-spa already accounts for refraction near the horizon. Here we
  //    apply the correction to the twilight angle itself (deeper depression zone).
  const refrFajr = atmosphericRefraction(-(fajrBase + 0.5), pressure, temperature);
  const refrIsha = atmosphericRefraction(-(ishaBase + 0.5), pressure, temperature);

  // 7. Elevation correction: higher observers see further around Earth's curvature,
  //    effectively dipping the horizon. This makes sunrise slightly earlier and
  //    sunset slightly later. For Fajr/Isha, the effect is ~0.08°/km elevation.
  //    Using dip = 1.06 × √(h_km) in degrees, scaled by factor for twilight
  //    (the dip effect is reduced at large depression angles vs the horizon).
  const horizonDipDeg = 1.06 * Math.sqrt(elevation / 1000);
  // Apply 30% of horizon dip to twilight angles (remainder already captured
  // by nrel-spa's elevation-adjusted sunrise/sunset computation).
  const elevCorr = horizonDipDeg * 0.3;

  // 8. Assemble final angles with all corrections.
  const rawFajr = fajrBase + rCorr + fourierCorr + refrFajr + elevCorr;
  const rawIsha = ishaBase + rCorr + fourierCorr + refrIsha + elevCorr;

  const fajrAngle = round3(clip(rawFajr, ANGLE_MIN, ANGLE_MAX));
  const ishaAngle = round3(clip(rawIsha, ANGLE_MIN, ANGLE_MAX));

  return { fajrAngle, ishaAngle, decl };
}

/**
 * Compute dynamic twilight depression angles for Fajr and Isha.
 *
 * @param date        - Observer's local date (time-of-day is ignored)
 * @param lat         - Latitude in decimal degrees (-90 to 90)
 * @param lng         - Longitude in decimal degrees (-180 to 180, currently unused; reserved)
 * @param elevation   - Observer elevation in meters (default: 0)
 * @param temperature - Ambient temperature in °C (default: 15)
 * @param pressure    - Atmospheric pressure in mbar (default: 1013.25)
 * @returns Fajr and Isha depression angles in degrees
 */
export function getAngles(
  date: Date,
  lat: number,
  lng: number,
  elevation = 0,
  temperature = 15,
  pressure = 1013.25,
): TwilightAngles {
  const { fajrAngle, ishaAngle } = computeAngles(date, lat, lng, elevation, temperature, pressure);
  return { fajrAngle, ishaAngle };
}