1 | 'use strict';
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2 |
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3 | Object.defineProperty(exports, "__esModule", {
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4 | value: true
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5 | });
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6 |
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7 | var _slicedToArray = function () { function sliceIterator(arr, i) { var _arr = []; var _n = true; var _d = false; var _e = undefined; try { for (var _i = arr[Symbol.iterator](), _s; !(_n = (_s = _i.next()).done); _n = true) { _arr.push(_s.value); if (i && _arr.length === i) break; } } catch (err) { _d = true; _e = err; } finally { try { if (!_n && _i["return"]) _i["return"](); } finally { if (_d) throw _e; } } return _arr; } return function (arr, i) { if (Array.isArray(arr)) { return arr; } else if (Symbol.iterator in Object(arr)) { return sliceIterator(arr, i); } else { throw new TypeError("Invalid attempt to destructure non-iterable instance"); } }; }(); |
8 |
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12 |
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13 |
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14 |
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15 |
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16 |
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17 | exports.physical = physical;
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18 |
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19 | var _base = require('./base');
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20 |
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21 | var _base2 = _interopRequireDefault(_base);
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22 |
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23 | var _coord = require('./coord');
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24 |
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25 | var _coord2 = _interopRequireDefault(_coord);
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26 |
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27 | var _illum = require('./illum');
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28 |
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29 | var _illum2 = _interopRequireDefault(_illum);
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30 |
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31 | var _nutation = require('./nutation');
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32 |
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33 | var _nutation2 = _interopRequireDefault(_nutation);
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34 |
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35 | var _planetposition = require('./planetposition');
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36 |
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37 | var _planetposition2 = _interopRequireDefault(_planetposition);
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38 |
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39 | function _interopRequireDefault(obj) { return obj && obj.__esModule ? obj : { default: obj }; }
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40 |
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41 |
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42 |
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43 |
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44 |
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45 |
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46 |
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47 |
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48 |
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49 |
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50 |
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51 |
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52 |
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53 |
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54 |
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55 |
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56 |
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57 |
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58 |
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59 |
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60 | function physical(jde, earth, mars) {
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61 |
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62 |
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63 | var T = _base2.default.J2000Century(jde);
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64 | var p = Math.PI / 180;
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65 |
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66 | var λ0 = 352.9065 * p + 1.1733 * p * T;
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67 | var β0 = 63.2818 * p - 0.00394 * p * T;
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68 |
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69 | var earthPos = earth.position(jde);
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70 | var R = earthPos.range;
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71 | var fk5 = _planetposition2.default.toFK5(earthPos.lon, earthPos.lat, jde);
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72 | var _ref = [fk5.lon, fk5.lat],
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73 | l0 = _ref[0],
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74 | b0 = _ref[1];
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75 |
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76 |
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77 | var _base$sincos = _base2.default.sincos(l0),
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78 | _base$sincos2 = _slicedToArray(_base$sincos, 2),
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79 | sl0 = _base$sincos2[0],
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80 | cl0 = _base$sincos2[1];
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81 |
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82 | var sb0 = Math.sin(b0);
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83 | var Δ = 0.5;
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84 | var τ = _base2.default.lightTime(Δ);
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85 | var l = void 0,
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86 | b = void 0,
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87 | r = void 0,
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88 | x = void 0,
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89 | y = void 0,
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90 | z = void 0;
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91 | function f() {
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92 | var marsPos = mars.position(jde - τ);
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93 | r = marsPos.range;
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94 | var fk5 = _planetposition2.default.toFK5(marsPos.lon, marsPos.lat, jde);
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95 | l = fk5.lon;
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96 | b = fk5.lat;
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97 |
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98 | var _base$sincos3 = _base2.default.sincos(b),
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99 | _base$sincos4 = _slicedToArray(_base$sincos3, 2),
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100 | sb = _base$sincos4[0],
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101 | cb = _base$sincos4[1];
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102 |
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103 | var _base$sincos5 = _base2.default.sincos(l),
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104 | _base$sincos6 = _slicedToArray(_base$sincos5, 2),
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105 | sl = _base$sincos6[0],
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106 | cl = _base$sincos6[1];
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107 |
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108 |
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109 |
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110 | x = r * cb * cl - R * cl0;
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111 | y = r * cb * sl - R * sl0;
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112 | z = r * sb - R * sb0;
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113 |
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114 | Δ = Math.sqrt(x * x + y * y + z * z);
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115 | τ = _base2.default.lightTime(Δ);
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116 | }
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117 | f();
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118 | f();
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119 |
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120 | var λ = Math.atan2(y, x);
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121 | var β = Math.atan(z / Math.hypot(x, y));
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122 |
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123 |
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124 | var _base$sincos7 = _base2.default.sincos(β0),
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125 | _base$sincos8 = _slicedToArray(_base$sincos7, 2),
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126 | sβ0 = _base$sincos8[0],
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127 | cβ0 = _base$sincos8[1];
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128 |
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129 | var _base$sincos9 = _base2.default.sincos(β),
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130 | _base$sincos10 = _slicedToArray(_base$sincos9, 2),
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131 | sβ = _base$sincos10[0],
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132 | cβ = _base$sincos10[1];
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133 |
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134 | var DE = Math.asin(-sβ0 * sβ - cβ0 * cβ * Math.cos(λ0 - λ));
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135 |
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136 | var N = 49.5581 * p + 0.7721 * p * T;
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137 | var lʹ = l - 0.00697 * p / r;
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138 | var bʹ = b - 0.000225 * p * Math.cos(l - N) / r;
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139 |
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140 |
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141 | var _base$sincos11 = _base2.default.sincos(bʹ),
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142 | _base$sincos12 = _slicedToArray(_base$sincos11, 2),
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143 | sbʹ = _base$sincos12[0],
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144 | cbʹ = _base$sincos12[1];
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145 |
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146 | var DS = Math.asin(-sβ0 * sbʹ - cβ0 * cbʹ * Math.cos(λ0 - lʹ));
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147 |
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148 | var W = 11.504 * p + 350.89200025 * p * (jde - τ - 2433282.5);
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149 |
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150 | var ε0 = _nutation2.default.meanObliquity(jde);
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151 |
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152 | var _base$sincos13 = _base2.default.sincos(ε0),
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153 | _base$sincos14 = _slicedToArray(_base$sincos13, 2),
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154 | sε0 = _base$sincos14[0],
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155 | cε0 = _base$sincos14[1];
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156 |
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157 | var eq = new _coord2.default.Ecliptic(λ0, β0).toEquatorial(ε0);
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158 | var _ref2 = [eq.ra, eq.dec],
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159 | α0 = _ref2[0],
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160 | δ0 = _ref2[1];
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161 |
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162 |
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163 | var u = y * cε0 - z * sε0;
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164 | var v = y * sε0 + z * cε0;
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165 | var α = Math.atan2(u, x);
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166 | var δ = Math.atan(v / Math.hypot(x, u));
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167 |
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168 | var _base$sincos15 = _base2.default.sincos(δ),
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169 | _base$sincos16 = _slicedToArray(_base$sincos15, 2),
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170 | sδ = _base$sincos16[0],
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171 | cδ = _base$sincos16[1];
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172 |
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173 | var _base$sincos17 = _base2.default.sincos(δ0),
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174 | _base$sincos18 = _slicedToArray(_base$sincos17, 2),
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175 | sδ0 = _base$sincos18[0],
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176 | cδ0 = _base$sincos18[1];
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177 |
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178 | var _base$sincos19 = _base2.default.sincos(α0 - α),
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179 | _base$sincos20 = _slicedToArray(_base$sincos19, 2),
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180 | sα0α = _base$sincos20[0],
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181 | cα0α = _base$sincos20[1];
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182 |
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183 | var ζ = Math.atan2(sδ0 * cδ * cα0α - sδ * cδ0, cδ * sα0α);
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184 |
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185 | var ω = _base2.default.pmod(W - ζ, 2 * Math.PI);
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186 |
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187 |
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188 | var _nutation$nutation = _nutation2.default.nutation(jde),
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189 | _nutation$nutation2 = _slicedToArray(_nutation$nutation, 2),
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190 | Δψ = _nutation$nutation2[0],
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191 | Δε = _nutation$nutation2[1];
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192 |
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193 |
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194 |
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195 | var _base$sincos21 = _base2.default.sincos(l0 - λ),
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196 | _base$sincos22 = _slicedToArray(_base$sincos21, 2),
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197 | sl0λ = _base$sincos22[0],
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198 | cl0λ = _base$sincos22[1];
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199 |
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200 | λ += 0.005693 * p * cl0λ / cβ;
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201 | β += 0.005693 * p * sl0λ * sβ;
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202 |
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203 | λ0 += Δψ;
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204 | λ += Δψ;
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205 | var ε = ε0 + Δε;
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206 |
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207 |
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208 | var _base$sincos23 = _base2.default.sincos(ε),
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209 | _base$sincos24 = _slicedToArray(_base$sincos23, 2),
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210 | sε = _base$sincos24[0],
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211 | cε = _base$sincos24[1];
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212 |
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213 | eq = new _coord2.default.Ecliptic(λ0, β0).toEquatorial(ε);
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214 | var _ref3 = [eq.ra, eq.dec],
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215 | α0ʹ = _ref3[0],
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216 | δ0ʹ = _ref3[1];
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217 |
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218 | eq = new _coord2.default.Ecliptic(λ, β).toEquatorial(ε);
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219 | var _ref4 = [eq.ra, eq.dec],
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220 | αʹ = _ref4[0],
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221 | δʹ = _ref4[1];
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222 |
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223 |
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224 | var _base$sincos25 = _base2.default.sincos(δ0ʹ),
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225 | _base$sincos26 = _slicedToArray(_base$sincos25, 2),
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226 | sδ0ʹ = _base$sincos26[0],
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227 | cδ0ʹ = _base$sincos26[1];
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228 |
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229 | var _base$sincos27 = _base2.default.sincos(δʹ),
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230 | _base$sincos28 = _slicedToArray(_base$sincos27, 2),
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231 | sδʹ = _base$sincos28[0],
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232 | cδʹ = _base$sincos28[1];
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233 |
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234 | var _base$sincos29 = _base2.default.sincos(α0ʹ - αʹ),
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235 | _base$sincos30 = _slicedToArray(_base$sincos29, 2),
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236 | sα0ʹαʹ = _base$sincos30[0],
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237 | cα0ʹαʹ = _base$sincos30[1];
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238 |
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239 |
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240 |
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241 | var P = Math.atan2(cδ0ʹ * sα0ʹαʹ, sδ0ʹ * cδʹ - cδ0ʹ * sδʹ * cα0ʹαʹ);
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242 | if (P < 0) {
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243 | P += 2 * Math.PI;
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244 | }
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245 |
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246 | var s = l0 + Math.PI;
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247 |
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248 | var _base$sincos31 = _base2.default.sincos(s),
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249 | _base$sincos32 = _slicedToArray(_base$sincos31, 2),
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250 | ss = _base$sincos32[0],
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251 | cs = _base$sincos32[1];
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252 |
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253 | var αs = Math.atan2(cε * ss, cs);
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254 | var δs = Math.asin(sε * ss);
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255 |
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256 | var _base$sincos33 = _base2.default.sincos(δs),
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257 | _base$sincos34 = _slicedToArray(_base$sincos33, 2),
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258 | sδs = _base$sincos34[0],
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259 | cδs = _base$sincos34[1];
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260 |
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261 | var _base$sincos35 = _base2.default.sincos(αs - α),
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262 | _base$sincos36 = _slicedToArray(_base$sincos35, 2),
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263 | sαsα = _base$sincos36[0],
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264 | cαsα = _base$sincos36[1];
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265 |
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266 | var χ = Math.atan2(cδs * sαsα, sδs * cδ - cδs * sδ * cαsα);
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267 | var Q = χ + Math.PI;
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268 |
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269 | var d = 9.36 / 60 / 60 * Math.PI / 180 / Δ;
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270 | var k = _illum2.default.fraction(r, Δ, R);
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271 | var q = (1 - k) * d;
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272 | return [DE, DS, ω, P, Q, d, k, q];
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273 | }
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274 |
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275 | exports.default = {
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276 | physical: physical
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277 | }; |
\ | No newline at end of file |