1 | #include "erfa.h"
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2 |
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3 | void eraHfk5z(double rh, double dh, double date1, double date2,
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4 | double *r5, double *d5, double *dr5, double *dd5)
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5 | /*
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6 | ** - - - - - - - - -
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7 | ** e r a H f k 5 z
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8 | ** - - - - - - - - -
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9 | **
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10 | ** Transform a Hipparcos star position into FK5 J2000.0, assuming
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11 | ** zero Hipparcos proper motion.
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12 | **
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13 | ** Given:
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14 | ** rh double Hipparcos RA (radians)
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15 | ** dh double Hipparcos Dec (radians)
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16 | ** date1,date2 double TDB date (Note 1)
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17 | **
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18 | ** Returned (all FK5, equinox J2000.0, date date1+date2):
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19 | ** r5 double RA (radians)
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20 | ** d5 double Dec (radians)
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21 | ** dr5 double FK5 RA proper motion (rad/year, Note 4)
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22 | ** dd5 double Dec proper motion (rad/year, Note 4)
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23 | **
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24 | ** Notes:
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25 | **
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26 | ** 1) The TT date date1+date2 is a Julian Date, apportioned in any
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27 | ** convenient way between the two arguments. For example,
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28 | ** JD(TT)=2450123.7 could be expressed in any of these ways,
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29 | ** among others:
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30 | **
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31 | ** date1 date2
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32 | **
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33 | ** 2450123.7 0.0 (JD method)
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34 | ** 2451545.0 -1421.3 (J2000 method)
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35 | ** 2400000.5 50123.2 (MJD method)
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36 | ** 2450123.5 0.2 (date & time method)
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37 | **
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38 | ** The JD method is the most natural and convenient to use in
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39 | ** cases where the loss of several decimal digits of resolution
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40 | ** is acceptable. The J2000 method is best matched to the way
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41 | ** the argument is handled internally and will deliver the
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42 | ** optimum resolution. The MJD method and the date & time methods
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43 | ** are both good compromises between resolution and convenience.
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44 | **
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45 | ** 2) The proper motion in RA is dRA/dt rather than cos(Dec)*dRA/dt.
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46 | **
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47 | ** 3) The FK5 to Hipparcos transformation is modeled as a pure rotation
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48 | ** and spin; zonal errors in the FK5 catalogue are not taken into
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49 | ** account.
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50 | **
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51 | ** 4) It was the intention that Hipparcos should be a close
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52 | ** approximation to an inertial frame, so that distant objects have
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53 | ** zero proper motion; such objects have (in general) non-zero
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54 | ** proper motion in FK5, and this function returns those fictitious
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55 | ** proper motions.
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56 | **
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57 | ** 5) The position returned by this function is in the FK5 J2000.0
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58 | ** reference system but at date date1+date2.
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59 | **
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60 | ** 6) See also eraFk52h, eraH2fk5, eraFk5zhz.
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61 | **
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62 | ** Called:
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63 | ** eraS2c spherical coordinates to unit vector
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64 | ** eraFk5hip FK5 to Hipparcos rotation and spin
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65 | ** eraRxp product of r-matrix and p-vector
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66 | ** eraSxp multiply p-vector by scalar
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67 | ** eraRxr product of two r-matrices
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68 | ** eraTrxp product of transpose of r-matrix and p-vector
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69 | ** eraPxp vector product of two p-vectors
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70 | ** eraPv2s pv-vector to spherical
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71 | ** eraAnp normalize angle into range 0 to 2pi
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72 | **
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73 | ** Reference:
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74 | **
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75 | ** F.Mignard & M.Froeschle, 2000, Astron.Astrophys. 354, 732-739.
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76 | **
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77 | ** Copyright (C) 2013-2017, NumFOCUS Foundation.
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78 | ** Derived, with permission, from the SOFA library. See notes at end of file.
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79 | */
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80 | {
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81 | double t, ph[3], r5h[3][3], s5h[3], sh[3], vst[3],
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82 | rst[3][3], r5ht[3][3], pv5e[2][3], vv[3],
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83 | w, r, v;
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84 |
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85 |
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86 | /* Time interval from fundamental epoch J2000.0 to given date (JY). */
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87 | t = ((date1 - ERFA_DJ00) + date2) / ERFA_DJY;
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88 |
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89 | /* Hipparcos barycentric position vector (normalized). */
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90 | eraS2c(rh, dh, ph);
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91 |
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92 | /* FK5 to Hipparcos orientation matrix and spin vector. */
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93 | eraFk5hip(r5h, s5h);
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94 |
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95 | /* Rotate the spin into the Hipparcos system. */
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96 | eraRxp(r5h, s5h, sh);
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97 |
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98 | /* Accumulated Hipparcos wrt FK5 spin over that interval. */
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99 | eraSxp(t, s5h, vst);
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100 |
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101 | /* Express the accumulated spin as a rotation matrix. */
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102 | eraRv2m(vst, rst);
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103 |
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104 | /* Rotation matrix: accumulated spin, then FK5 to Hipparcos. */
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105 | eraRxr(r5h, rst, r5ht);
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106 |
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107 | /* De-orient & de-spin the Hipparcos position into FK5 J2000.0. */
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108 | eraTrxp(r5ht, ph, pv5e[0]);
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109 |
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110 | /* Apply spin to the position giving a space motion. */
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111 | eraPxp(sh, ph, vv);
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112 |
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113 | /* De-orient & de-spin the Hipparcos space motion into FK5 J2000.0. */
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114 | eraTrxp(r5ht, vv, pv5e[1]);
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115 |
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116 | /* FK5 position/velocity pv-vector to spherical. */
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117 | eraPv2s(pv5e, &w, d5, &r, dr5, dd5, &v);
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118 | *r5 = eraAnp(w);
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119 |
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120 | return;
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121 |
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122 | }
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123 | /*----------------------------------------------------------------------
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124 | **
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125 | **
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126 | ** Copyright (C) 2013-2017, NumFOCUS Foundation.
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127 | ** All rights reserved.
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128 | **
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129 | ** This library is derived, with permission, from the International
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130 | ** Astronomical Union's "Standards of Fundamental Astronomy" library,
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131 | ** available from http://www.iausofa.org.
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132 | **
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133 | ** The ERFA version is intended to retain identical functionality to
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134 | ** the SOFA library, but made distinct through different function and
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135 | ** file names, as set out in the SOFA license conditions. The SOFA
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136 | ** original has a role as a reference standard for the IAU and IERS,
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137 | ** and consequently redistribution is permitted only in its unaltered
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138 | ** state. The ERFA version is not subject to this restriction and
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139 | ** therefore can be included in distributions which do not support the
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140 | ** concept of "read only" software.
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141 | **
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142 | ** Although the intent is to replicate the SOFA API (other than
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143 | ** replacement of prefix names) and results (with the exception of
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144 | ** bugs; any that are discovered will be fixed), SOFA is not
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145 | ** responsible for any errors found in this version of the library.
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146 | **
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147 | ** If you wish to acknowledge the SOFA heritage, please acknowledge
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148 | ** that you are using a library derived from SOFA, rather than SOFA
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149 | ** itself.
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150 | **
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151 | **
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152 | ** TERMS AND CONDITIONS
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153 | **
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154 | ** Redistribution and use in source and binary forms, with or without
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155 | ** modification, are permitted provided that the following conditions
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156 | ** are met:
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157 | **
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158 | ** 1 Redistributions of source code must retain the above copyright
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159 | ** notice, this list of conditions and the following disclaimer.
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160 | **
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161 | ** 2 Redistributions in binary form must reproduce the above copyright
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162 | ** notice, this list of conditions and the following disclaimer in
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163 | ** the documentation and/or other materials provided with the
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164 | ** distribution.
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165 | **
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166 | ** 3 Neither the name of the Standards Of Fundamental Astronomy Board,
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167 | ** the International Astronomical Union nor the names of its
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168 | ** contributors may be used to endorse or promote products derived
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169 | ** from this software without specific prior written permission.
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170 | **
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171 | ** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
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172 | ** "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
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173 | ** LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
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174 | ** FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
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175 | ** COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
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176 | ** INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
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177 | ** BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
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178 | ** LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
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179 | ** CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
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180 | ** LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
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181 | ** ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
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182 | ** POSSIBILITY OF SUCH DAMAGE.
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183 | **
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184 | */
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