1 | #include "erfa.h"
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2 |
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3 | void eraApcg(double date1, double date2,
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4 | double ebpv[2][3], double ehp[3],
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5 | eraASTROM *astrom)
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6 | /*
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7 | ** - - - - - - - -
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8 | ** e r a A p c g
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9 | ** - - - - - - - -
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10 | **
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11 | ** For a geocentric observer, prepare star-independent astrometry
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12 | ** parameters for transformations between ICRS and GCRS coordinates.
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13 | ** The Earth ephemeris is supplied by the caller.
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14 | **
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15 | ** The parameters produced by this function are required in the
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16 | ** parallax, light deflection and aberration parts of the astrometric
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17 | ** transformation chain.
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18 | **
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19 | ** Given:
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20 | ** date1 double TDB as a 2-part...
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21 | ** date2 double ...Julian Date (Note 1)
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22 | ** ebpv double[2][3] Earth barycentric pos/vel (au, au/day)
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23 | ** ehp double[3] Earth heliocentric position (au)
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24 | **
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25 | ** Returned:
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26 | ** astrom eraASTROM* star-independent astrometry parameters:
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27 | ** pmt double PM time interval (SSB, Julian years)
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28 | ** eb double[3] SSB to observer (vector, au)
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29 | ** eh double[3] Sun to observer (unit vector)
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30 | ** em double distance from Sun to observer (au)
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31 | ** v double[3] barycentric observer velocity (vector, c)
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32 | ** bm1 double sqrt(1-|v|^2): reciprocal of Lorenz factor
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33 | ** bpn double[3][3] bias-precession-nutation matrix
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34 | ** along double unchanged
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35 | ** xpl double unchanged
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36 | ** ypl double unchanged
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37 | ** sphi double unchanged
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38 | ** cphi double unchanged
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39 | ** diurab double unchanged
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40 | ** eral double unchanged
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41 | ** refa double unchanged
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42 | ** refb double unchanged
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43 | **
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44 | ** Notes:
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45 | **
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46 | ** 1) The TDB date date1+date2 is a Julian Date, apportioned in any
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47 | ** convenient way between the two arguments. For example,
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48 | ** JD(TDB)=2450123.7 could be expressed in any of these ways, among
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49 | ** others:
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50 | **
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51 | ** date1 date2
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52 | **
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53 | ** 2450123.7 0.0 (JD method)
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54 | ** 2451545.0 -1421.3 (J2000 method)
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55 | ** 2400000.5 50123.2 (MJD method)
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56 | ** 2450123.5 0.2 (date & time method)
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57 | **
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58 | ** The JD method is the most natural and convenient to use in cases
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59 | ** where the loss of several decimal digits of resolution is
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60 | ** acceptable. The J2000 method is best matched to the way the
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61 | ** argument is handled internally and will deliver the optimum
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62 | ** resolution. The MJD method and the date & time methods are both
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63 | ** good compromises between resolution and convenience. For most
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64 | ** applications of this function the choice will not be at all
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65 | ** critical.
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66 | **
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67 | ** TT can be used instead of TDB without any significant impact on
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68 | ** accuracy.
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69 | **
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70 | ** 2) All the vectors are with respect to BCRS axes.
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71 | **
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72 | ** 3) This is one of several functions that inserts into the astrom
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73 | ** structure star-independent parameters needed for the chain of
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74 | ** astrometric transformations ICRS <-> GCRS <-> CIRS <-> observed.
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75 | **
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76 | ** The various functions support different classes of observer and
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77 | ** portions of the transformation chain:
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78 | **
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79 | ** functions observer transformation
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80 | **
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81 | ** eraApcg eraApcg13 geocentric ICRS <-> GCRS
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82 | ** eraApci eraApci13 terrestrial ICRS <-> CIRS
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83 | ** eraApco eraApco13 terrestrial ICRS <-> observed
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84 | ** eraApcs eraApcs13 space ICRS <-> GCRS
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85 | ** eraAper eraAper13 terrestrial update Earth rotation
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86 | ** eraApio eraApio13 terrestrial CIRS <-> observed
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87 | **
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88 | ** Those with names ending in "13" use contemporary ERFA models to
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89 | ** compute the various ephemerides. The others accept ephemerides
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90 | ** supplied by the caller.
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91 | **
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92 | ** The transformation from ICRS to GCRS covers space motion,
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93 | ** parallax, light deflection, and aberration. From GCRS to CIRS
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94 | ** comprises frame bias and precession-nutation. From CIRS to
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95 | ** observed takes account of Earth rotation, polar motion, diurnal
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96 | ** aberration and parallax (unless subsumed into the ICRS <-> GCRS
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97 | ** transformation), and atmospheric refraction.
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98 | **
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99 | ** 4) The context structure astrom produced by this function is used by
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100 | ** eraAtciq* and eraAticq*.
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101 | **
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102 | ** Called:
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103 | ** eraApcs astrometry parameters, ICRS-GCRS, space observer
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104 | **
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105 | ** Copyright (C) 2013-2016, NumFOCUS Foundation.
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106 | ** Derived, with permission, from the SOFA library. See notes at end of file.
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107 | */
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108 | {
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109 | /* Geocentric observer */
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110 | double pv[2][3] = { { 0.0, 0.0, 0.0 },
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111 | { 0.0, 0.0, 0.0 } };
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112 |
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113 |
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114 | /* Compute the star-independent astrometry parameters. */
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115 | eraApcs(date1, date2, pv, ebpv, ehp, astrom);
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116 |
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117 | /* Finished. */
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118 |
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119 | }
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120 | /*----------------------------------------------------------------------
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121 | **
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122 | **
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123 | ** Copyright (C) 2013-2016, NumFOCUS Foundation.
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124 | ** All rights reserved.
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125 | **
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126 | ** This library is derived, with permission, from the International
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127 | ** Astronomical Union's "Standards of Fundamental Astronomy" library,
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128 | ** available from http://www.iausofa.org.
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129 | **
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130 | ** The ERFA version is intended to retain identical functionality to
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131 | ** the SOFA library, but made distinct through different function and
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132 | ** file names, as set out in the SOFA license conditions. The SOFA
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133 | ** original has a role as a reference standard for the IAU and IERS,
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134 | ** and consequently redistribution is permitted only in its unaltered
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135 | ** state. The ERFA version is not subject to this restriction and
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136 | ** therefore can be included in distributions which do not support the
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137 | ** concept of "read only" software.
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138 | **
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139 | ** Although the intent is to replicate the SOFA API (other than
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140 | ** replacement of prefix names) and results (with the exception of
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141 | ** bugs; any that are discovered will be fixed), SOFA is not
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142 | ** responsible for any errors found in this version of the library.
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143 | **
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144 | ** If you wish to acknowledge the SOFA heritage, please acknowledge
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145 | ** that you are using a library derived from SOFA, rather than SOFA
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146 | ** itself.
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147 | **
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148 | **
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149 | ** TERMS AND CONDITIONS
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150 | **
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151 | ** Redistribution and use in source and binary forms, with or without
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152 | ** modification, are permitted provided that the following conditions
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153 | ** are met:
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154 | **
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155 | ** 1 Redistributions of source code must retain the above copyright
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156 | ** notice, this list of conditions and the following disclaimer.
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157 | **
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158 | ** 2 Redistributions in binary form must reproduce the above copyright
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159 | ** notice, this list of conditions and the following disclaimer in
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160 | ** the documentation and/or other materials provided with the
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161 | ** distribution.
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162 | **
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163 | ** 3 Neither the name of the Standards Of Fundamental Astronomy Board,
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164 | ** the International Astronomical Union nor the names of its
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165 | ** contributors may be used to endorse or promote products derived
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166 | ** from this software without specific prior written permission.
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167 | **
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168 | ** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
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169 | ** "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
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170 | ** LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
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171 | ** FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
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172 | ** COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
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173 | ** INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
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174 | ** BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
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175 | ** LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
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176 | ** CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
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177 | ** LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
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178 | ** ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
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179 | ** POSSIBILITY OF SUCH DAMAGE.
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180 | **
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181 | */
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