| line |
stmt |
bran |
cond |
sub |
pod |
time |
code |
|
1
|
|
|
|
|
|
|
#include "erfa.h" |
|
2
|
|
|
|
|
|
|
|
|
3
|
0
|
|
|
|
|
|
double eraEect00(double date1, double date2) |
|
4
|
|
|
|
|
|
|
/* |
|
5
|
|
|
|
|
|
|
** - - - - - - - - - - |
|
6
|
|
|
|
|
|
|
** e r a E e c t 0 0 |
|
7
|
|
|
|
|
|
|
** - - - - - - - - - - |
|
8
|
|
|
|
|
|
|
** |
|
9
|
|
|
|
|
|
|
** Equation of the equinoxes complementary terms, consistent with |
|
10
|
|
|
|
|
|
|
** IAU 2000 resolutions. |
|
11
|
|
|
|
|
|
|
** |
|
12
|
|
|
|
|
|
|
** Given: |
|
13
|
|
|
|
|
|
|
** date1,date2 double TT as a 2-part Julian Date (Note 1) |
|
14
|
|
|
|
|
|
|
** |
|
15
|
|
|
|
|
|
|
** Returned (function value): |
|
16
|
|
|
|
|
|
|
** double complementary terms (Note 2) |
|
17
|
|
|
|
|
|
|
** |
|
18
|
|
|
|
|
|
|
** Notes: |
|
19
|
|
|
|
|
|
|
** |
|
20
|
|
|
|
|
|
|
** 1) The TT date date1+date2 is a Julian Date, apportioned in any |
|
21
|
|
|
|
|
|
|
** convenient way between the two arguments. For example, |
|
22
|
|
|
|
|
|
|
** JD(TT)=2450123.7 could be expressed in any of these ways, |
|
23
|
|
|
|
|
|
|
** among others: |
|
24
|
|
|
|
|
|
|
** |
|
25
|
|
|
|
|
|
|
** date1 date2 |
|
26
|
|
|
|
|
|
|
** |
|
27
|
|
|
|
|
|
|
** 2450123.7 0.0 (JD method) |
|
28
|
|
|
|
|
|
|
** 2451545.0 -1421.3 (J2000 method) |
|
29
|
|
|
|
|
|
|
** 2400000.5 50123.2 (MJD method) |
|
30
|
|
|
|
|
|
|
** 2450123.5 0.2 (date & time method) |
|
31
|
|
|
|
|
|
|
** |
|
32
|
|
|
|
|
|
|
** The JD method is the most natural and convenient to use in |
|
33
|
|
|
|
|
|
|
** cases where the loss of several decimal digits of resolution |
|
34
|
|
|
|
|
|
|
** is acceptable. The J2000 method is best matched to the way |
|
35
|
|
|
|
|
|
|
** the argument is handled internally and will deliver the |
|
36
|
|
|
|
|
|
|
** optimum resolution. The MJD method and the date & time methods |
|
37
|
|
|
|
|
|
|
** are both good compromises between resolution and convenience. |
|
38
|
|
|
|
|
|
|
** |
|
39
|
|
|
|
|
|
|
** 2) The "complementary terms" are part of the equation of the |
|
40
|
|
|
|
|
|
|
** equinoxes (EE), classically the difference between apparent and |
|
41
|
|
|
|
|
|
|
** mean Sidereal Time: |
|
42
|
|
|
|
|
|
|
** |
|
43
|
|
|
|
|
|
|
** GAST = GMST + EE |
|
44
|
|
|
|
|
|
|
** |
|
45
|
|
|
|
|
|
|
** with: |
|
46
|
|
|
|
|
|
|
** |
|
47
|
|
|
|
|
|
|
** EE = dpsi * cos(eps) |
|
48
|
|
|
|
|
|
|
** |
|
49
|
|
|
|
|
|
|
** where dpsi is the nutation in longitude and eps is the obliquity |
|
50
|
|
|
|
|
|
|
** of date. However, if the rotation of the Earth were constant in |
|
51
|
|
|
|
|
|
|
** an inertial frame the classical formulation would lead to |
|
52
|
|
|
|
|
|
|
** apparent irregularities in the UT1 timescale traceable to side- |
|
53
|
|
|
|
|
|
|
** effects of precession-nutation. In order to eliminate these |
|
54
|
|
|
|
|
|
|
** effects from UT1, "complementary terms" were introduced in 1994 |
|
55
|
|
|
|
|
|
|
** (IAU, 1994) and took effect from 1997 (Capitaine and Gontier, |
|
56
|
|
|
|
|
|
|
** 1993): |
|
57
|
|
|
|
|
|
|
** |
|
58
|
|
|
|
|
|
|
** GAST = GMST + CT + EE |
|
59
|
|
|
|
|
|
|
** |
|
60
|
|
|
|
|
|
|
** By convention, the complementary terms are included as part of |
|
61
|
|
|
|
|
|
|
** the equation of the equinoxes rather than as part of the mean |
|
62
|
|
|
|
|
|
|
** Sidereal Time. This slightly compromises the "geometrical" |
|
63
|
|
|
|
|
|
|
** interpretation of mean sidereal time but is otherwise |
|
64
|
|
|
|
|
|
|
** inconsequential. |
|
65
|
|
|
|
|
|
|
** |
|
66
|
|
|
|
|
|
|
** The present function computes CT in the above expression, |
|
67
|
|
|
|
|
|
|
** compatible with IAU 2000 resolutions (Capitaine et al., 2002, and |
|
68
|
|
|
|
|
|
|
** IERS Conventions 2003). |
|
69
|
|
|
|
|
|
|
** |
|
70
|
|
|
|
|
|
|
** Called: |
|
71
|
|
|
|
|
|
|
** eraFal03 mean anomaly of the Moon |
|
72
|
|
|
|
|
|
|
** eraFalp03 mean anomaly of the Sun |
|
73
|
|
|
|
|
|
|
** eraFaf03 mean argument of the latitude of the Moon |
|
74
|
|
|
|
|
|
|
** eraFad03 mean elongation of the Moon from the Sun |
|
75
|
|
|
|
|
|
|
** eraFaom03 mean longitude of the Moon's ascending node |
|
76
|
|
|
|
|
|
|
** eraFave03 mean longitude of Venus |
|
77
|
|
|
|
|
|
|
** eraFae03 mean longitude of Earth |
|
78
|
|
|
|
|
|
|
** eraFapa03 general accumulated precession in longitude |
|
79
|
|
|
|
|
|
|
** |
|
80
|
|
|
|
|
|
|
** References: |
|
81
|
|
|
|
|
|
|
** |
|
82
|
|
|
|
|
|
|
** Capitaine, N. & Gontier, A.-M., Astron.Astrophys., 275, |
|
83
|
|
|
|
|
|
|
** 645-650 (1993) |
|
84
|
|
|
|
|
|
|
** |
|
85
|
|
|
|
|
|
|
** Capitaine, N., Wallace, P.T. and McCarthy, D.D., "Expressions to |
|
86
|
|
|
|
|
|
|
** implement the IAU 2000 definition of UT1", Astron.Astrophys., 406, |
|
87
|
|
|
|
|
|
|
** 1135-1149 (2003) |
|
88
|
|
|
|
|
|
|
** |
|
89
|
|
|
|
|
|
|
** IAU Resolution C7, Recommendation 3 (1994) |
|
90
|
|
|
|
|
|
|
** |
|
91
|
|
|
|
|
|
|
** McCarthy, D. D., Petit, G. (eds.), IERS Conventions (2003), |
|
92
|
|
|
|
|
|
|
** IERS Technical Note No. 32, BKG (2004) |
|
93
|
|
|
|
|
|
|
** |
|
94
|
|
|
|
|
|
|
** Copyright (C) 2013-2019, NumFOCUS Foundation. |
|
95
|
|
|
|
|
|
|
** Derived, with permission, from the SOFA library. See notes at end of file. |
|
96
|
|
|
|
|
|
|
*/ |
|
97
|
|
|
|
|
|
|
{ |
|
98
|
|
|
|
|
|
|
/* Time since J2000.0, in Julian centuries */ |
|
99
|
|
|
|
|
|
|
double t; |
|
100
|
|
|
|
|
|
|
|
|
101
|
|
|
|
|
|
|
/* Miscellaneous */ |
|
102
|
|
|
|
|
|
|
int i, j; |
|
103
|
|
|
|
|
|
|
double a, s0, s1; |
|
104
|
|
|
|
|
|
|
|
|
105
|
|
|
|
|
|
|
/* Fundamental arguments */ |
|
106
|
|
|
|
|
|
|
double fa[14]; |
|
107
|
|
|
|
|
|
|
|
|
108
|
|
|
|
|
|
|
/* Returned value. */ |
|
109
|
|
|
|
|
|
|
double eect; |
|
110
|
|
|
|
|
|
|
|
|
111
|
|
|
|
|
|
|
/* ----------------------------------------- */ |
|
112
|
|
|
|
|
|
|
/* The series for the EE complementary terms */ |
|
113
|
|
|
|
|
|
|
/* ----------------------------------------- */ |
|
114
|
|
|
|
|
|
|
|
|
115
|
|
|
|
|
|
|
typedef struct { |
|
116
|
|
|
|
|
|
|
int nfa[8]; /* coefficients of l,l',F,D,Om,LVe,LE,pA */ |
|
117
|
|
|
|
|
|
|
double s, c; /* sine and cosine coefficients */ |
|
118
|
|
|
|
|
|
|
} TERM; |
|
119
|
|
|
|
|
|
|
|
|
120
|
|
|
|
|
|
|
/* Terms of order t^0 */ |
|
121
|
|
|
|
|
|
|
static const TERM e0[] = { |
|
122
|
|
|
|
|
|
|
|
|
123
|
|
|
|
|
|
|
/* 1-10 */ |
|
124
|
|
|
|
|
|
|
{{ 0, 0, 0, 0, 1, 0, 0, 0}, 2640.96e-6, -0.39e-6 }, |
|
125
|
|
|
|
|
|
|
{{ 0, 0, 0, 0, 2, 0, 0, 0}, 63.52e-6, -0.02e-6 }, |
|
126
|
|
|
|
|
|
|
{{ 0, 0, 2, -2, 3, 0, 0, 0}, 11.75e-6, 0.01e-6 }, |
|
127
|
|
|
|
|
|
|
{{ 0, 0, 2, -2, 1, 0, 0, 0}, 11.21e-6, 0.01e-6 }, |
|
128
|
|
|
|
|
|
|
{{ 0, 0, 2, -2, 2, 0, 0, 0}, -4.55e-6, 0.00e-6 }, |
|
129
|
|
|
|
|
|
|
{{ 0, 0, 2, 0, 3, 0, 0, 0}, 2.02e-6, 0.00e-6 }, |
|
130
|
|
|
|
|
|
|
{{ 0, 0, 2, 0, 1, 0, 0, 0}, 1.98e-6, 0.00e-6 }, |
|
131
|
|
|
|
|
|
|
{{ 0, 0, 0, 0, 3, 0, 0, 0}, -1.72e-6, 0.00e-6 }, |
|
132
|
|
|
|
|
|
|
{{ 0, 1, 0, 0, 1, 0, 0, 0}, -1.41e-6, -0.01e-6 }, |
|
133
|
|
|
|
|
|
|
{{ 0, 1, 0, 0, -1, 0, 0, 0}, -1.26e-6, -0.01e-6 }, |
|
134
|
|
|
|
|
|
|
|
|
135
|
|
|
|
|
|
|
/* 11-20 */ |
|
136
|
|
|
|
|
|
|
{{ 1, 0, 0, 0, -1, 0, 0, 0}, -0.63e-6, 0.00e-6 }, |
|
137
|
|
|
|
|
|
|
{{ 1, 0, 0, 0, 1, 0, 0, 0}, -0.63e-6, 0.00e-6 }, |
|
138
|
|
|
|
|
|
|
{{ 0, 1, 2, -2, 3, 0, 0, 0}, 0.46e-6, 0.00e-6 }, |
|
139
|
|
|
|
|
|
|
{{ 0, 1, 2, -2, 1, 0, 0, 0}, 0.45e-6, 0.00e-6 }, |
|
140
|
|
|
|
|
|
|
{{ 0, 0, 4, -4, 4, 0, 0, 0}, 0.36e-6, 0.00e-6 }, |
|
141
|
|
|
|
|
|
|
{{ 0, 0, 1, -1, 1, -8, 12, 0}, -0.24e-6, -0.12e-6 }, |
|
142
|
|
|
|
|
|
|
{{ 0, 0, 2, 0, 0, 0, 0, 0}, 0.32e-6, 0.00e-6 }, |
|
143
|
|
|
|
|
|
|
{{ 0, 0, 2, 0, 2, 0, 0, 0}, 0.28e-6, 0.00e-6 }, |
|
144
|
|
|
|
|
|
|
{{ 1, 0, 2, 0, 3, 0, 0, 0}, 0.27e-6, 0.00e-6 }, |
|
145
|
|
|
|
|
|
|
{{ 1, 0, 2, 0, 1, 0, 0, 0}, 0.26e-6, 0.00e-6 }, |
|
146
|
|
|
|
|
|
|
|
|
147
|
|
|
|
|
|
|
/* 21-30 */ |
|
148
|
|
|
|
|
|
|
{{ 0, 0, 2, -2, 0, 0, 0, 0}, -0.21e-6, 0.00e-6 }, |
|
149
|
|
|
|
|
|
|
{{ 0, 1, -2, 2, -3, 0, 0, 0}, 0.19e-6, 0.00e-6 }, |
|
150
|
|
|
|
|
|
|
{{ 0, 1, -2, 2, -1, 0, 0, 0}, 0.18e-6, 0.00e-6 }, |
|
151
|
|
|
|
|
|
|
{{ 0, 0, 0, 0, 0, 8,-13, -1}, -0.10e-6, 0.05e-6 }, |
|
152
|
|
|
|
|
|
|
{{ 0, 0, 0, 2, 0, 0, 0, 0}, 0.15e-6, 0.00e-6 }, |
|
153
|
|
|
|
|
|
|
{{ 2, 0, -2, 0, -1, 0, 0, 0}, -0.14e-6, 0.00e-6 }, |
|
154
|
|
|
|
|
|
|
{{ 1, 0, 0, -2, 1, 0, 0, 0}, 0.14e-6, 0.00e-6 }, |
|
155
|
|
|
|
|
|
|
{{ 0, 1, 2, -2, 2, 0, 0, 0}, -0.14e-6, 0.00e-6 }, |
|
156
|
|
|
|
|
|
|
{{ 1, 0, 0, -2, -1, 0, 0, 0}, 0.14e-6, 0.00e-6 }, |
|
157
|
|
|
|
|
|
|
{{ 0, 0, 4, -2, 4, 0, 0, 0}, 0.13e-6, 0.00e-6 }, |
|
158
|
|
|
|
|
|
|
|
|
159
|
|
|
|
|
|
|
/* 31-33 */ |
|
160
|
|
|
|
|
|
|
{{ 0, 0, 2, -2, 4, 0, 0, 0}, -0.11e-6, 0.00e-6 }, |
|
161
|
|
|
|
|
|
|
{{ 1, 0, -2, 0, -3, 0, 0, 0}, 0.11e-6, 0.00e-6 }, |
|
162
|
|
|
|
|
|
|
{{ 1, 0, -2, 0, -1, 0, 0, 0}, 0.11e-6, 0.00e-6 } |
|
163
|
|
|
|
|
|
|
}; |
|
164
|
|
|
|
|
|
|
|
|
165
|
|
|
|
|
|
|
/* Terms of order t^1 */ |
|
166
|
|
|
|
|
|
|
static const TERM e1[] = { |
|
167
|
|
|
|
|
|
|
{{ 0, 0, 0, 0, 1, 0, 0, 0}, -0.87e-6, 0.00e-6 } |
|
168
|
|
|
|
|
|
|
}; |
|
169
|
|
|
|
|
|
|
|
|
170
|
|
|
|
|
|
|
/* Number of terms in the series */ |
|
171
|
|
|
|
|
|
|
const int NE0 = (int) (sizeof e0 / sizeof (TERM)); |
|
172
|
|
|
|
|
|
|
const int NE1 = (int) (sizeof e1 / sizeof (TERM)); |
|
173
|
|
|
|
|
|
|
|
|
174
|
|
|
|
|
|
|
/*--------------------------------------------------------------------*/ |
|
175
|
|
|
|
|
|
|
|
|
176
|
|
|
|
|
|
|
/* Interval between fundamental epoch J2000.0 and current date (JC). */ |
|
177
|
0
|
|
|
|
|
|
t = ((date1 - ERFA_DJ00) + date2) / ERFA_DJC; |
|
178
|
|
|
|
|
|
|
|
|
179
|
|
|
|
|
|
|
/* Fundamental Arguments (from IERS Conventions 2003) */ |
|
180
|
|
|
|
|
|
|
|
|
181
|
|
|
|
|
|
|
/* Mean anomaly of the Moon. */ |
|
182
|
0
|
|
|
|
|
|
fa[0] = eraFal03(t); |
|
183
|
|
|
|
|
|
|
|
|
184
|
|
|
|
|
|
|
/* Mean anomaly of the Sun. */ |
|
185
|
0
|
|
|
|
|
|
fa[1] = eraFalp03(t); |
|
186
|
|
|
|
|
|
|
|
|
187
|
|
|
|
|
|
|
/* Mean longitude of the Moon minus that of the ascending node. */ |
|
188
|
0
|
|
|
|
|
|
fa[2] = eraFaf03(t); |
|
189
|
|
|
|
|
|
|
|
|
190
|
|
|
|
|
|
|
/* Mean elongation of the Moon from the Sun. */ |
|
191
|
0
|
|
|
|
|
|
fa[3] = eraFad03(t); |
|
192
|
|
|
|
|
|
|
|
|
193
|
|
|
|
|
|
|
/* Mean longitude of the ascending node of the Moon. */ |
|
194
|
0
|
|
|
|
|
|
fa[4] = eraFaom03(t); |
|
195
|
|
|
|
|
|
|
|
|
196
|
|
|
|
|
|
|
/* Mean longitude of Venus. */ |
|
197
|
0
|
|
|
|
|
|
fa[5] = eraFave03(t); |
|
198
|
|
|
|
|
|
|
|
|
199
|
|
|
|
|
|
|
/* Mean longitude of Earth. */ |
|
200
|
0
|
|
|
|
|
|
fa[6] = eraFae03(t); |
|
201
|
|
|
|
|
|
|
|
|
202
|
|
|
|
|
|
|
/* General precession in longitude. */ |
|
203
|
0
|
|
|
|
|
|
fa[7] = eraFapa03(t); |
|
204
|
|
|
|
|
|
|
|
|
205
|
|
|
|
|
|
|
/* Evaluate the EE complementary terms. */ |
|
206
|
|
|
|
|
|
|
s0 = 0.0; |
|
207
|
|
|
|
|
|
|
s1 = 0.0; |
|
208
|
|
|
|
|
|
|
|
|
209
|
0
|
0
|
|
|
|
|
for (i = NE0-1; i >= 0; i--) { |
|
210
|
|
|
|
|
|
|
a = 0.0; |
|
211
|
0
|
0
|
|
|
|
|
for (j = 0; j < 8; j++) { |
|
212
|
0
|
|
|
|
|
|
a += (double)(e0[i].nfa[j]) * fa[j]; |
|
213
|
|
|
|
|
|
|
} |
|
214
|
0
|
|
|
|
|
|
s0 += e0[i].s * sin(a) + e0[i].c * cos(a); |
|
215
|
|
|
|
|
|
|
} |
|
216
|
|
|
|
|
|
|
|
|
217
|
0
|
0
|
|
|
|
|
for (i = NE1-1; i >= 0; i--) { |
|
218
|
|
|
|
|
|
|
a = 0.0; |
|
219
|
0
|
0
|
|
|
|
|
for (j = 0; j < 8; j++) { |
|
220
|
0
|
|
|
|
|
|
a += (double)(e1[i].nfa[j]) * fa[j]; |
|
221
|
|
|
|
|
|
|
} |
|
222
|
0
|
|
|
|
|
|
s1 += e1[i].s * sin(a) + e1[i].c * cos(a); |
|
223
|
|
|
|
|
|
|
} |
|
224
|
|
|
|
|
|
|
|
|
225
|
0
|
|
|
|
|
|
eect = (s0 + s1 * t ) * ERFA_DAS2R; |
|
226
|
|
|
|
|
|
|
|
|
227
|
0
|
|
|
|
|
|
return eect; |
|
228
|
|
|
|
|
|
|
|
|
229
|
|
|
|
|
|
|
} |
|
230
|
|
|
|
|
|
|
/*---------------------------------------------------------------------- |
|
231
|
|
|
|
|
|
|
** |
|
232
|
|
|
|
|
|
|
** |
|
233
|
|
|
|
|
|
|
** Copyright (C) 2013-2019, NumFOCUS Foundation. |
|
234
|
|
|
|
|
|
|
** All rights reserved. |
|
235
|
|
|
|
|
|
|
** |
|
236
|
|
|
|
|
|
|
** This library is derived, with permission, from the International |
|
237
|
|
|
|
|
|
|
** Astronomical Union's "Standards of Fundamental Astronomy" library, |
|
238
|
|
|
|
|
|
|
** available from http://www.iausofa.org. |
|
239
|
|
|
|
|
|
|
** |
|
240
|
|
|
|
|
|
|
** The ERFA version is intended to retain identical functionality to |
|
241
|
|
|
|
|
|
|
** the SOFA library, but made distinct through different function and |
|
242
|
|
|
|
|
|
|
** file names, as set out in the SOFA license conditions. The SOFA |
|
243
|
|
|
|
|
|
|
** original has a role as a reference standard for the IAU and IERS, |
|
244
|
|
|
|
|
|
|
** and consequently redistribution is permitted only in its unaltered |
|
245
|
|
|
|
|
|
|
** state. The ERFA version is not subject to this restriction and |
|
246
|
|
|
|
|
|
|
** therefore can be included in distributions which do not support the |
|
247
|
|
|
|
|
|
|
** concept of "read only" software. |
|
248
|
|
|
|
|
|
|
** |
|
249
|
|
|
|
|
|
|
** Although the intent is to replicate the SOFA API (other than |
|
250
|
|
|
|
|
|
|
** replacement of prefix names) and results (with the exception of |
|
251
|
|
|
|
|
|
|
** bugs; any that are discovered will be fixed), SOFA is not |
|
252
|
|
|
|
|
|
|
** responsible for any errors found in this version of the library. |
|
253
|
|
|
|
|
|
|
** |
|
254
|
|
|
|
|
|
|
** If you wish to acknowledge the SOFA heritage, please acknowledge |
|
255
|
|
|
|
|
|
|
** that you are using a library derived from SOFA, rather than SOFA |
|
256
|
|
|
|
|
|
|
** itself. |
|
257
|
|
|
|
|
|
|
** |
|
258
|
|
|
|
|
|
|
** |
|
259
|
|
|
|
|
|
|
** TERMS AND CONDITIONS |
|
260
|
|
|
|
|
|
|
** |
|
261
|
|
|
|
|
|
|
** Redistribution and use in source and binary forms, with or without |
|
262
|
|
|
|
|
|
|
** modification, are permitted provided that the following conditions |
|
263
|
|
|
|
|
|
|
** are met: |
|
264
|
|
|
|
|
|
|
** |
|
265
|
|
|
|
|
|
|
** 1 Redistributions of source code must retain the above copyright |
|
266
|
|
|
|
|
|
|
** notice, this list of conditions and the following disclaimer. |
|
267
|
|
|
|
|
|
|
** |
|
268
|
|
|
|
|
|
|
** 2 Redistributions in binary form must reproduce the above copyright |
|
269
|
|
|
|
|
|
|
** notice, this list of conditions and the following disclaimer in |
|
270
|
|
|
|
|
|
|
** the documentation and/or other materials provided with the |
|
271
|
|
|
|
|
|
|
** distribution. |
|
272
|
|
|
|
|
|
|
** |
|
273
|
|
|
|
|
|
|
** 3 Neither the name of the Standards Of Fundamental Astronomy Board, |
|
274
|
|
|
|
|
|
|
** the International Astronomical Union nor the names of its |
|
275
|
|
|
|
|
|
|
** contributors may be used to endorse or promote products derived |
|
276
|
|
|
|
|
|
|
** from this software without specific prior written permission. |
|
277
|
|
|
|
|
|
|
** |
|
278
|
|
|
|
|
|
|
** THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS |
|
279
|
|
|
|
|
|
|
** "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT |
|
280
|
|
|
|
|
|
|
** LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS |
|
281
|
|
|
|
|
|
|
** FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE |
|
282
|
|
|
|
|
|
|
** COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, |
|
283
|
|
|
|
|
|
|
** INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, |
|
284
|
|
|
|
|
|
|
** BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; |
|
285
|
|
|
|
|
|
|
** LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER |
|
286
|
|
|
|
|
|
|
** CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT |
|
287
|
|
|
|
|
|
|
** LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN |
|
288
|
|
|
|
|
|
|
** ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE |
|
289
|
|
|
|
|
|
|
** POSSIBILITY OF SUCH DAMAGE. |
|
290
|
|
|
|
|
|
|
** |
|
291
|
|
|
|
|
|
|
*/ |