# hyperspeed forward and backwards analytics engine import numpy.typing as npt from scipy.integrate import solve_bvp, solve_ivp from jax import jit, grad, vmap import jax.numpy as np # TODO: define 3d vector space - x,y,z oriented around car/world? # solvers should not care about position but we should be able to convert # transforms between car/world spaces. # let's define x as the forward-backward axis (with forward being positive) # y as the lateral axis, with right being positive # and z being the vertical, with up being positive. # for simplicities’ sake, the car only rotates on the y-axis (up and down hills). # z rotation can be determined from distance along the route. # some data (wind) is only a 2d vector at a given time point. def fsolve_discrete(): ... def dist_to_pos(dist: float): "convert a distance along the race path to a position in 3d space" ### All units are BASE SI (no prefix except for kilogram) ATM_MOLAR_MASS = 0.0289644 # kg/mol STANDARD_TEMP = 288.15 # K STANDARD_PRES = 101325.0 # Pa AIR_GAS_CONSTANT = 8.31432 # N*m/s^2 EARTH_TEMP_LAPSE = -0.0065 EARTH_GRAVITY = 9.80665 # m/s^2 EARTH_RADIUS = 6378140.0 # m EARTH_AXIS_INCLINATION = 23.45 # degrees # FIXME: use named constants here @jit def get_pressure_el( el: float, Ps=STANDARD_PRES, Ts: float = STANDARD_TEMP, T_lapse: float = EARTH_TEMP_LAPSE, ): """Gets the pressure at a point given eleveation - assumes standard pressure,temperature, gas constants, etc""" return Ps * (Ts / (Ts + T_lapse * el)) ** ( (ATM_MOLAR_MASS * EARTH_GRAVITY) / (AIR_GAS_CONSTANT / T_lapse) ) @jit def estimate_temp(el: float, Ts: float = STANDARD_TEMP, T_lapse=EARTH_TEMP_LAPSE): return Ts + el * T_lapse def make_cubic(a, b, c, d): """returns a simple cubic function""" def poly(x): return a + b * x + c * (x**2) + (x**3) / d return jit(poly) @jit @vmap def get_radiation_direct(yday, altitude_deg): """Calculate the direct radiation at a given day of the year given the angle of the sun from the horizon.""" flux = 1160 + (75 * np.sin(2 * np.pi / 365 * (yday - 275))) optical_depth = 0.174 + (0.035 * np.sin(2 * np.pi / 365 * (yday - 100))) air_mass_ratio = 1 / np.sin(np.radians(altitude_deg)) # from Masters, p. 412 return flux * np.exp(-1 * optical_depth * air_mass_ratio) * (altitude_deg > 0) # We start by defining MANY constants. # to skip this, Ctrl-F to END COEFF # START COEFF # heliocentric longitude, latitude, radius (section 3.2) coefficients # heliocentric longitude coefficients L0_TABLE = np.array( [ [175347046.0, 0.0, 0.0], [3341656.0, 4.6692568, 6283.07585], [34894.0, 4.6261, 12566.1517], [3497.0, 2.7441, 5753.3849], [3418.0, 2.8289, 3.5231], [3136.0, 3.6277, 77713.7715], [2676.0, 4.4181, 7860.4194], [2343.0, 6.1352, 3930.2097], [1324.0, 0.7425, 11506.7698], [1273.0, 2.0371, 529.691], [1199.0, 1.1096, 1577.3435], [990.0, 5.233, 5884.927], [902.0, 2.045, 26.298], [857.0, 3.508, 398.149], [780.0, 1.179, 5223.694], [753.0, 2.533, 5507.553], [505.0, 4.583, 18849.228], [492.0, 4.205, 775.523], [357.0, 2.92, 0.067], [317.0, 5.849, 11790.629], [284.0, 1.899, 796.298], [271.0, 0.315, 10977.079], [243.0, 0.345, 5486.778], [206.0, 4.806, 2544.314], [205.0, 1.869, 5573.143], [202.0, 2.458, 6069.777], [156.0, 0.833, 213.299], [132.0, 3.411, 2942.463], [126.0, 1.083, 20.775], [115.0, 0.645, 0.98], [103.0, 0.636, 4694.003], [102.0, 0.976, 15720.839], [102.0, 4.267, 7.114], [99.0, 6.21, 2146.17], [98.0, 0.68, 155.42], [86.0, 5.98, 161000.69], [85.0, 1.3, 6275.96], [85.0, 3.67, 71430.7], [80.0, 1.81, 17260.15], [79.0, 3.04, 12036.46], [75.0, 1.76, 5088.63], [74.0, 3.5, 3154.69], [74.0, 4.68, 801.82], [70.0, 0.83, 9437.76], [62.0, 3.98, 8827.39], [61.0, 1.82, 7084.9], [57.0, 2.78, 6286.6], [56.0, 4.39, 14143.5], [56.0, 3.47, 6279.55], [52.0, 0.19, 12139.55], [52.0, 1.33, 1748.02], [51.0, 0.28, 5856.48], [49.0, 0.49, 1194.45], [41.0, 5.37, 8429.24], [41.0, 2.4, 19651.05], [39.0, 6.17, 10447.39], [37.0, 6.04, 10213.29], [37.0, 2.57, 1059.38], [36.0, 1.71, 2352.87], [36.0, 1.78, 6812.77], [33.0, 0.59, 17789.85], [30.0, 0.44, 83996.85], [30.0, 2.74, 1349.87], [25.0, 3.16, 4690.48], ] ) L1_TABLE = np.array( [ [628331966747.0, 0.0, 0.0], [206059.0, 2.678235, 6283.07585], [4303.0, 2.6351, 12566.1517], [425.0, 1.59, 3.523], [119.0, 5.796, 26.298], [109.0, 2.966, 1577.344], [93.0, 2.59, 18849.23], [72.0, 1.14, 529.69], [68.0, 1.87, 398.15], [67.0, 4.41, 5507.55], [59.0, 2.89, 5223.69], [56.0, 2.17, 155.42], [45.0, 0.4, 796.3], [36.0, 0.47, 775.52], [29.0, 2.65, 7.11], [21.0, 5.34, 0.98], [19.0, 1.85, 5486.78], [19.0, 4.97, 213.3], [17.0, 2.99, 6275.96], [16.0, 0.03, 2544.31], [16.0, 1.43, 2146.17], [15.0, 1.21, 10977.08], [12.0, 2.83, 1748.02], [12.0, 3.26, 5088.63], [12.0, 5.27, 1194.45], [12.0, 2.08, 4694.0], [11.0, 0.77, 553.57], [10.0, 1.3, 6286.6], [10.0, 4.24, 1349.87], [9.0, 2.7, 242.73], [9.0, 5.64, 951.72], [8.0, 5.3, 2352.87], [6.0, 2.65, 9437.76], [6.0, 4.67, 4690.48], ] ) L2_TABLE = np.array( [ [52919.0, 0.0, 0.0], [8720.0, 1.0721, 6283.0758], [309.0, 0.867, 12566.152], [27.0, 0.05, 3.52], [16.0, 5.19, 26.3], [16.0, 3.68, 155.42], [10.0, 0.76, 18849.23], [9.0, 2.06, 77713.77], [7.0, 0.83, 775.52], [5.0, 4.66, 1577.34], [4.0, 1.03, 7.11], [4.0, 3.44, 5573.14], [3.0, 5.14, 796.3], [3.0, 6.05, 5507.55], [3.0, 1.19, 242.73], [3.0, 6.12, 529.69], [3.0, 0.31, 398.15], [3.0, 2.28, 553.57], [2.0, 4.38, 5223.69], [2.0, 3.75, 0.98], ] ) L3_TABLE = np.array( [ [289.0, 5.844, 6283.076], [35.0, 0.0, 0.0], [17.0, 5.49, 12566.15], [3.0, 5.2, 155.42], [1.0, 4.72, 3.52], [1.0, 5.3, 18849.23], [1.0, 5.97, 242.73], ] ) L4_TABLE = np.array([[114.0, 3.142, 0.0], [8.0, 4.13, 6283.08], [1.0, 3.84, 12566.15]]) L5_TABLE = np.array([[1.0, 3.14, 0.0]]) HELIO_L = [L0_TABLE, L1_TABLE, L2_TABLE, L3_TABLE, L4_TABLE, L5_TABLE] # heliocentric latitude coefficients B0_TABLE = np.array( [ [280.0, 3.199, 84334.662], [102.0, 5.422, 5507.553], [80.0, 3.88, 5223.69], [44.0, 3.7, 2352.87], [32.0, 4.0, 1577.34], ] ) B1_TABLE = np.array([[9.0, 3.9, 5507.55], [6.0, 1.73, 5223.69]]) HELIO_B = [B0_TABLE, B1_TABLE] # heliocentric radius coefficients R0_TABLE = np.array( [ [100013989.0, 0.0, 0.0], [1670700.0, 3.0984635, 6283.07585], [13956.0, 3.05525, 12566.1517], [3084.0, 5.1985, 77713.7715], [1628.0, 1.1739, 5753.3849], [1576.0, 2.8469, 7860.4194], [925.0, 5.453, 11506.77], [542.0, 4.564, 3930.21], [472.0, 3.661, 5884.927], [346.0, 0.964, 5507.553], [329.0, 5.9, 5223.694], [307.0, 0.299, 5573.143], [243.0, 4.273, 11790.629], [212.0, 5.847, 1577.344], [186.0, 5.022, 10977.079], [175.0, 3.012, 18849.228], [110.0, 5.055, 5486.778], [98.0, 0.89, 6069.78], [86.0, 5.69, 15720.84], [86.0, 1.27, 161000.69], [65.0, 0.27, 17260.15], [63.0, 0.92, 529.69], [57.0, 2.01, 83996.85], [56.0, 5.24, 71430.7], [49.0, 3.25, 2544.31], [47.0, 2.58, 775.52], [45.0, 5.54, 9437.76], [43.0, 6.01, 6275.96], [39.0, 5.36, 4694.0], [38.0, 2.39, 8827.39], [37.0, 0.83, 19651.05], [37.0, 4.9, 12139.55], [36.0, 1.67, 12036.46], [35.0, 1.84, 2942.46], [33.0, 0.24, 7084.9], [32.0, 0.18, 5088.63], [32.0, 1.78, 398.15], [28.0, 1.21, 6286.6], [28.0, 1.9, 6279.55], [26.0, 4.59, 10447.39], ] ) R1_TABLE = np.array( [ [103019.0, 1.10749, 6283.07585], [1721.0, 1.0644, 12566.1517], [702.0, 3.142, 0.0], [32.0, 1.02, 18849.23], [31.0, 2.84, 5507.55], [25.0, 1.32, 5223.69], [18.0, 1.42, 1577.34], [10.0, 5.91, 10977.08], [9.0, 1.42, 6275.96], [9.0, 0.27, 5486.78], ] ) R2_TABLE = np.array( [ [4359.0, 5.7846, 6283.0758], [124.0, 5.579, 12566.152], [12.0, 3.14, 0.0], [9.0, 3.63, 77713.77], [6.0, 1.87, 5573.14], [3.0, 5.47, 18849.23], ] ) R3_TABLE = np.array([[145.0, 4.273, 6283.076], [7.0, 3.92, 12566.15]]) R4_TABLE = np.array([[4.0, 2.56, 6283.08]]) HELIO_R = [R0_TABLE, R1_TABLE, R2_TABLE, R3_TABLE, R4_TABLE] # longitude and obliquity nutation coefficients NUTATION_ABCD_ARRAY = np.array( [ [-171996, -174.2, 92025, 8.9], [-13187, -1.6, 5736, -3.1], [-2274, -0.2, 977, -0.5], [2062, 0.2, -895, 0.5], [1426, -3.4, 54, -0.1], [712, 0.1, -7, 0], [-517, 1.2, 224, -0.6], [-386, -0.4, 200, 0], [-301, 0, 129, -0.1], [217, -0.5, -95, 0.3], [-158, 0, 0, 0], [129, 0.1, -70, 0], [123, 0, -53, 0], [63, 0, 0, 0], [63, 0.1, -33, 0], [-59, 0, 26, 0], [-58, -0.1, 32, 0], [-51, 0, 27, 0], [48, 0, 0, 0], [46, 0, -24, 0], [-38, 0, 16, 0], [-31, 0, 13, 0], [29, 0, 0, 0], [29, 0, -12, 0], [26, 0, 0, 0], [-22, 0, 0, 0], [21, 0, -10, 0], [17, -0.1, 0, 0], [16, 0, -8, 0], [-16, 0.1, 7, 0], [-15, 0, 9, 0], [-13, 0, 7, 0], [-12, 0, 6, 0], [11, 0, 0, 0], [-10, 0, 5, 0], [-8, 0, 3, 0], [7, 0, -3, 0], [-7, 0, 0, 0], [-7, 0, 3, 0], [-7, 0, 3, 0], [6, 0, 0, 0], [6, 0, -3, 0], [6, 0, -3, 0], [-6, 0, 3, 0], [-6, 0, 3, 0], [5, 0, 0, 0], [-5, 0, 3, 0], [-5, 0, 3, 0], [-5, 0, 3, 0], [4, 0, 0, 0], [4, 0, 0, 0], [4, 0, 0, 0], [-4, 0, 0, 0], [-4, 0, 0, 0], [-4, 0, 0, 0], [3, 0, 0, 0], [-3, 0, 0, 0], [-3, 0, 0, 0], [-3, 0, 0, 0], [-3, 0, 0, 0], [-3, 0, 0, 0], [-3, 0, 0, 0], [-3, 0, 0, 0], ] ) NUTATION_YTERM_ARRAY = np.array( [ [0, 0, 0, 0, 1], [-2, 0, 0, 2, 2], [0, 0, 0, 2, 2], [0, 0, 0, 0, 2], [0, 1, 0, 0, 0], [0, 0, 1, 0, 0], [-2, 1, 0, 2, 2], [0, 0, 0, 2, 1], [0, 0, 1, 2, 2], [-2, -1, 0, 2, 2], [-2, 0, 1, 0, 0], [-2, 0, 0, 2, 1], [0, 0, -1, 2, 2], [2, 0, 0, 0, 0], [0, 0, 1, 0, 1], [2, 0, -1, 2, 2], [0, 0, -1, 0, 1], [0, 0, 1, 2, 1], [-2, 0, 2, 0, 0], [0, 0, -2, 2, 1], [2, 0, 0, 2, 2], [0, 0, 2, 2, 2], [0, 0, 2, 0, 0], [-2, 0, 1, 2, 2], [0, 0, 0, 2, 0], [-2, 0, 0, 2, 0], [0, 0, -1, 2, 1], [0, 2, 0, 0, 0], [2, 0, -1, 0, 1], [-2, 2, 0, 2, 2], [0, 1, 0, 0, 1], [-2, 0, 1, 0, 1], [0, -1, 0, 0, 1], [0, 0, 2, -2, 0], [2, 0, -1, 2, 1], [2, 0, 1, 2, 2], [0, 1, 0, 2, 2], [-2, 1, 1, 0, 0], [0, -1, 0, 2, 2], [2, 0, 0, 2, 1], [2, 0, 1, 0, 0], [-2, 0, 2, 2, 2], [-2, 0, 1, 2, 1], [2, 0, -2, 0, 1], [2, 0, 0, 0, 1], [0, -1, 1, 0, 0], [-2, -1, 0, 2, 1], [-2, 0, 0, 0, 1], [0, 0, 2, 2, 1], [-2, 0, 2, 0, 1], [-2, 1, 0, 2, 1], [0, 0, 1, -2, 0], [-1, 0, 1, 0, 0], [-2, 1, 0, 0, 0], [1, 0, 0, 0, 0], [0, 0, 1, 2, 0], [0, 0, -2, 2, 2], [-1, -1, 1, 0, 0], [0, 1, 1, 0, 0], [0, -1, 1, 2, 2], [2, -1, -1, 2, 2], [0, 0, 3, 2, 2], [2, -1, 0, 2, 2], ] ) # END COEFF # now, we write to the actual code DELTA_T = 67 @jit def helio_vector(vec, jme): """This function calculates equation 9 across the vector""" return np.sum( vec[:, 0] * np.cos(vec[:, 1] + vec[:, 2] * jme[..., np.newaxis]), axis=-1 ) def solar_position(timestamp, latitude, longitude): """Calculate the position of the sun at a given location and time. Args: timestamp (array-like): The timestamp(s) to calculate. Returns: ndarray: An array containing the altitude and azimuth for each timestamp. """ timestamp = np.array(timestamp) jd = timestamp / 86400.0 + 2440587.5 jc = (jd - 2451545) / 36525 jde = jd + DELTA_T / 86400.0 jce = (jde - 2451545) / 36525 jm = jc / 10 jme = jce / 10 # todo: make more elegant? # TODO: vectorize later? it's kinda complex # heliocentric longitude l_rad = np.zeros_like(timestamp) for idx, vec in enumerate(HELIO_L): l_rad = l_rad + helio_vector(vec, jme) * jme**idx l_rad = l_rad / 10e8 l_deg = np.rad2deg(l_rad) % 360 # heliocentric latitude b_rad = np.zeros_like(timestamp) for idx, vec in enumerate(HELIO_B): b_rad = b_rad + helio_vector(vec, jme) * jme**idx b_rad = b_rad / 10e8 b_deg = np.rad2deg(b_rad) % 360 # heliocentric radius r_rad = np.zeros_like(timestamp) for idx, vec in enumerate(HELIO_R): r_rad = r_rad + helio_vector(vec, jme) * jme**idx r_rad = r_rad / 10e8 r_deg = np.rad2deg(r_rad) % 360 theta = (l_deg + 180) % 360 beta = -1 * b_deg def cubic_poly(a, b, c, d): return a + b * jce + c * jce**2 + (jce**3) / d X0 = cubic_poly(297.85036, 445267.111480, -0.0019142, 189474) X1 = cubic_poly(357.52772, 35999.050340, -0.0001603, -300000) X2 = cubic_poly(134.96298, 477198.867398, 0.0086972, 56250) X3 = cubic_poly(93.27191, 483202.017538, -0.0036825, 327270) X4 = cubic_poly(125.04452, 1934.136261, 0.0020708, 450000) X = np.vstack([X0, X1, X2, X3, X4]).T nut = NUTATION_ABCD_ARRAY ## TODO: these are gross - use loops instead of broadcasting? d_psi = (nut[:, 0] + jce[..., np.newaxis] * nut[:, 1]) * np.sin( np.sum(X[:, np.newaxis, :] * NUTATION_YTERM_ARRAY[np.newaxis, ...], axis=2) ) d_psi = np.sum(d_psi, axis=-1) / 36, 000, 000 d_epsilon = (nut[:, 2] + jce[..., np.newaxis] * nut[:, 3]) * np.cos( np.sum(X[:, np.newaxis, :] * NUTATION_YTERM_ARRAY[np.newaxis, ...], axis=2) ) d_epsilon = np.sum(d_epsilon, axis=-1) / 36, 000, 000 u = jme[:, np.newaxis] / 10 * np.arange(0,10).reshape((1,-1)) epsilon_0 = np.array( [ 84381.448, -4680.93, 1.55, 1999.25, -51.38, -249.67, -39.05, 7.12, 27.87, 5.79, 2.45, ] ) epsilon = np.sum(u * epsilon_0, axis=-1) / 3600 + d_epsilon d_tau = -20.4898 / (3600 * r_deg) sun_longitude = theta + d_psi + d_tau