line |
stmt |
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cond |
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pod |
time |
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/* |
2
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*+ |
3
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* Name: |
4
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* palEl2ue |
5
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6
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* Purpose: |
7
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* Transform conventional elements into "universal" form |
8
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9
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* Language: |
10
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* Starlink ANSI C |
11
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12
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* Type of Module: |
13
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* Library routine |
14
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15
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* Invocation: |
16
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* void palEl2ue ( double date, int jform, double epoch, double orbinc, |
17
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* double anode, double perih, double aorq, double e, |
18
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* double aorl, double dm, double u[13], int *jstat ); |
19
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20
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* Arguments: |
21
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* date = double (Given) |
22
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* Epoch (TT MJD) of osculation (Note 3) |
23
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* jform = int (Given) |
24
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* Element set actually returned (1-3; Note 6) |
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* epoch = double (Given) |
26
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* Epoch of elements (TT MJD) |
27
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* orbinc = double (Given) |
28
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* inclination (radians) |
29
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* anode = double (Given) |
30
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* longitude of the ascending node (radians) |
31
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* perih = double (Given) |
32
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* longitude or argument of perihelion (radians) |
33
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* aorq = double (Given) |
34
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* mean distance or perihelion distance (AU) |
35
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* e = double (Given) |
36
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* eccentricity |
37
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* aorl = double (Given) |
38
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* mean anomaly or longitude (radians, JFORM=1,2 only) |
39
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* dm = double (Given) |
40
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* daily motion (radians, JFORM=1 only) |
41
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* u = double [13] (Returned) |
42
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* Universal orbital elements (Note 1) |
43
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* - (0) combined mass (M+m) |
44
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* - (1) total energy of the orbit (alpha) |
45
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* - (2) reference (osculating) epoch (t0) |
46
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* - (3-5) position at reference epoch (r0) |
47
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* - (6-8) velocity at reference epoch (v0) |
48
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* - (9) heliocentric distance at reference epoch |
49
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* - (10) r0.v0 |
50
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* - (11) date (t) |
51
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* - (12) universal eccentric anomaly (psi) of date, approx |
52
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* jstat = int * (Returned) |
53
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* status: 0 = OK |
54
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* - -1 = illegal JFORM |
55
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* - -2 = illegal E |
56
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* - -3 = illegal AORQ |
57
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* - -4 = illegal DM |
58
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* - -5 = numerical error |
59
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60
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* Description: |
61
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* Transform conventional osculating elements into "universal" form. |
62
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63
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* Authors: |
64
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* PTW: Pat Wallace (STFC) |
65
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* TIMJ: Tim Jenness (JAC, Hawaii) |
66
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* {enter_new_authors_here} |
67
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68
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* Notes: |
69
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* - The "universal" elements are those which define the orbit for the |
70
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* purposes of the method of universal variables (see reference). |
71
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* They consist of the combined mass of the two bodies, an epoch, |
72
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* and the position and velocity vectors (arbitrary reference frame) |
73
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* at that epoch. The parameter set used here includes also various |
74
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* quantities that can, in fact, be derived from the other |
75
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* information. This approach is taken to avoiding unnecessary |
76
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* computation and loss of accuracy. The supplementary quantities |
77
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* are (i) alpha, which is proportional to the total energy of the |
78
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* orbit, (ii) the heliocentric distance at epoch, (iii) the |
79
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* outwards component of the velocity at the given epoch, (iv) an |
80
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* estimate of psi, the "universal eccentric anomaly" at a given |
81
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* date and (v) that date. |
82
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* - The companion routine is palUe2pv. This takes the set of numbers |
83
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* that the present routine outputs and uses them to derive the |
84
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* object's position and velocity. A single prediction requires one |
85
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* call to the present routine followed by one call to palUe2pv; |
86
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* for convenience, the two calls are packaged as the routine |
87
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* palPlanel. Multiple predictions may be made by again calling the |
88
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* present routine once, but then calling palUe2pv multiple times, |
89
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* which is faster than multiple calls to palPlanel. |
90
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* - DATE is the epoch of osculation. It is in the TT timescale |
91
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* (formerly Ephemeris Time, ET) and is a Modified Julian Date |
92
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* (JD-2400000.5). |
93
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* - The supplied orbital elements are with respect to the J2000 |
94
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* ecliptic and equinox. The position and velocity parameters |
95
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* returned in the array U are with respect to the mean equator and |
96
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* equinox of epoch J2000, and are for the perihelion prior to the |
97
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* specified epoch. |
98
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* - The universal elements returned in the array U are in canonical |
99
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* units (solar masses, AU and canonical days). |
100
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* - Three different element-format options are available: |
101
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* |
102
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* Option JFORM=1, suitable for the major planets: |
103
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* |
104
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* EPOCH = epoch of elements (TT MJD) |
105
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* ORBINC = inclination i (radians) |
106
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* ANODE = longitude of the ascending node, big omega (radians) |
107
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* PERIH = longitude of perihelion, curly pi (radians) |
108
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* AORQ = mean distance, a (AU) |
109
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* E = eccentricity, e (range 0 to <1) |
110
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* AORL = mean longitude L (radians) |
111
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* DM = daily motion (radians) |
112
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* |
113
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* Option JFORM=2, suitable for minor planets: |
114
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* |
115
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* EPOCH = epoch of elements (TT MJD) |
116
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* ORBINC = inclination i (radians) |
117
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* ANODE = longitude of the ascending node, big omega (radians) |
118
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* PERIH = argument of perihelion, little omega (radians) |
119
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* AORQ = mean distance, a (AU) |
120
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* E = eccentricity, e (range 0 to <1) |
121
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* AORL = mean anomaly M (radians) |
122
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* |
123
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* Option JFORM=3, suitable for comets: |
124
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* |
125
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* EPOCH = epoch of perihelion (TT MJD) |
126
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* ORBINC = inclination i (radians) |
127
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* ANODE = longitude of the ascending node, big omega (radians) |
128
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* PERIH = argument of perihelion, little omega (radians) |
129
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* AORQ = perihelion distance, q (AU) |
130
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* E = eccentricity, e (range 0 to 10) |
131
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* |
132
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* - Unused elements (DM for JFORM=2, AORL and DM for JFORM=3) are |
133
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* not accessed. |
134
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* - The algorithm was originally adapted from the EPHSLA program of |
135
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* D.H.P.Jones (private communication, 1996). The method is based |
136
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* on Stumpff's Universal Variables. |
137
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* |
138
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* See Also: |
139
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* Everhart & Pitkin, Am.J.Phys. 51, 712 (1983). |
140
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141
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* History: |
142
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* 2012-03-12 (TIMJ): |
143
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* Initial version taken directly from SLA/F. |
144
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* Adapted with permission from the Fortran SLALIB library. |
145
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* {enter_further_changes_here} |
146
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147
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* Copyright: |
148
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* Copyright (C) 2005 Patrick T. Wallace |
149
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* Copyright (C) 2012 Science and Technology Facilities Council. |
150
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* All Rights Reserved. |
151
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152
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* Licence: |
153
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* This program is free software; you can redistribute it and/or |
154
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* modify it under the terms of the GNU General Public License as |
155
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* published by the Free Software Foundation; either version 3 of |
156
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* the License, or (at your option) any later version. |
157
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* |
158
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* This program is distributed in the hope that it will be |
159
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* useful, but WITHOUT ANY WARRANTY; without even the implied |
160
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* warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR |
161
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* PURPOSE. See the GNU General Public License for more details. |
162
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* |
163
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* You should have received a copy of the GNU General Public License |
164
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* along with this program; if not, write to the Free Software |
165
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* Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, |
166
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* MA 02110-1301, USA. |
167
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168
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* Bugs: |
169
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* {note_any_bugs_here} |
170
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*- |
171
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*/ |
172
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173
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#include |
174
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175
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#include "pal.h" |
176
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#include "palmac.h" |
177
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178
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3
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void palEl2ue ( double date, int jform, double epoch, double orbinc, |
179
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double anode, double perih, double aorq, double e, |
180
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double aorl, double dm, double u[13], int *jstat ) { |
181
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182
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/* Sin and cos of J2000 mean obliquity (IAU 1976) */ |
183
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const double SE=0.3977771559319137; |
184
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const double CE=0.9174820620691818; |
185
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186
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int J; |
187
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188
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double PHT,ARGPH,Q,W,CM,ALPHA,PHS,SW,CW,SI,CI,SO,CO, |
189
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X,Y,Z,PX,PY,PZ,VX,VY,VZ,DT,FC,FP,PSI, |
190
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UL[13],PV[6]; |
191
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192
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/* Validate arguments. */ |
193
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3
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50
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if (jform < 1 || jform > 3) { |
194
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0
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*jstat = -1; |
195
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0
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return; |
196
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} |
197
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3
|
50
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if (e < 0.0 || e > 10.0 || (e >= 1.0 && jform != 3)) { |
|
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50
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50
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0
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198
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0
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*jstat = -2; |
199
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0
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return; |
200
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} |
201
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3
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50
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if (aorq <= 0.0) { |
202
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0
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*jstat = -3; |
203
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0
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return; |
204
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} |
205
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3
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50
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if (jform == 1 && dm <= 0.0) { |
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0
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206
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0
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*jstat = -4; |
207
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0
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return; |
208
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} |
209
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210
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/* |
211
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* Transform elements into standard form: |
212
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* |
213
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* PHT = epoch of perihelion passage |
214
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* ARGPH = argument of perihelion (little omega) |
215
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* Q = perihelion distance (q) |
216
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* CM = combined mass, M+m (mu) |
217
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*/ |
218
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219
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3
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50
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if (jform == 1) { |
220
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221
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/* Major planet. */ |
222
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0
|
|
|
|
|
|
PHT = epoch-(aorl-perih)/dm; |
223
|
0
|
|
|
|
|
|
ARGPH = perih-anode; |
224
|
0
|
|
|
|
|
|
Q = aorq*(1.0-e); |
225
|
0
|
|
|
|
|
|
W = dm/PAL__GCON; |
226
|
0
|
|
|
|
|
|
CM = W*W*aorq*aorq*aorq; |
227
|
|
|
|
|
|
|
|
228
|
3
|
50
|
|
|
|
|
} else if (jform == 2) { |
229
|
|
|
|
|
|
|
|
230
|
|
|
|
|
|
|
/* Minor planet. */ |
231
|
0
|
|
|
|
|
|
PHT = epoch-aorl*sqrt(aorq*aorq*aorq)/PAL__GCON; |
232
|
|
|
|
|
|
|
ARGPH = perih; |
233
|
0
|
|
|
|
|
|
Q = aorq*(1.0-e); |
234
|
|
|
|
|
|
|
CM = 1.0; |
235
|
|
|
|
|
|
|
|
236
|
|
|
|
|
|
|
} else { |
237
|
|
|
|
|
|
|
|
238
|
|
|
|
|
|
|
/* Comet. */ |
239
|
|
|
|
|
|
|
PHT = epoch; |
240
|
|
|
|
|
|
|
ARGPH = perih; |
241
|
|
|
|
|
|
|
Q = aorq; |
242
|
|
|
|
|
|
|
CM = 1.0; |
243
|
|
|
|
|
|
|
|
244
|
|
|
|
|
|
|
} |
245
|
|
|
|
|
|
|
|
246
|
|
|
|
|
|
|
/* The universal variable alpha. This is proportional to the total |
247
|
|
|
|
|
|
|
* energy of the orbit: -ve for an ellipse, zero for a parabola, |
248
|
|
|
|
|
|
|
* +ve for a hyperbola. */ |
249
|
|
|
|
|
|
|
|
250
|
3
|
|
|
|
|
|
ALPHA = CM*(e-1.0)/Q; |
251
|
|
|
|
|
|
|
|
252
|
|
|
|
|
|
|
/* Speed at perihelion. */ |
253
|
|
|
|
|
|
|
|
254
|
3
|
|
|
|
|
|
PHS = sqrt(ALPHA+2.0*CM/Q); |
255
|
|
|
|
|
|
|
|
256
|
|
|
|
|
|
|
/* In a Cartesian coordinate system which has the x-axis pointing |
257
|
|
|
|
|
|
|
* to perihelion and the z-axis normal to the orbit (such that the |
258
|
|
|
|
|
|
|
* object orbits counter-clockwise as seen from +ve z), the |
259
|
|
|
|
|
|
|
* perihelion position and velocity vectors are: |
260
|
|
|
|
|
|
|
* |
261
|
|
|
|
|
|
|
* position [Q,0,0] |
262
|
|
|
|
|
|
|
* velocity [0,PHS,0] |
263
|
|
|
|
|
|
|
* |
264
|
|
|
|
|
|
|
* To express the results in J2000 equatorial coordinates we make a |
265
|
|
|
|
|
|
|
* series of four rotations of the Cartesian axes: |
266
|
|
|
|
|
|
|
* |
267
|
|
|
|
|
|
|
* axis Euler angle |
268
|
|
|
|
|
|
|
* |
269
|
|
|
|
|
|
|
* 1 z argument of perihelion (little omega) |
270
|
|
|
|
|
|
|
* 2 x inclination (i) |
271
|
|
|
|
|
|
|
* 3 z longitude of the ascending node (big omega) |
272
|
|
|
|
|
|
|
* 4 x J2000 obliquity (epsilon) |
273
|
|
|
|
|
|
|
* |
274
|
|
|
|
|
|
|
* In each case the rotation is clockwise as seen from the +ve end of |
275
|
|
|
|
|
|
|
* the axis concerned. |
276
|
|
|
|
|
|
|
*/ |
277
|
|
|
|
|
|
|
|
278
|
|
|
|
|
|
|
/* Functions of the Euler angles. */ |
279
|
3
|
|
|
|
|
|
SW = sin(ARGPH); |
280
|
3
|
|
|
|
|
|
CW = cos(ARGPH); |
281
|
3
|
|
|
|
|
|
SI = sin(orbinc); |
282
|
3
|
|
|
|
|
|
CI = cos(orbinc); |
283
|
3
|
|
|
|
|
|
SO = sin(anode); |
284
|
3
|
|
|
|
|
|
CO = cos(anode); |
285
|
|
|
|
|
|
|
|
286
|
|
|
|
|
|
|
/* Position at perihelion (AU). */ |
287
|
3
|
|
|
|
|
|
X = Q*CW; |
288
|
3
|
|
|
|
|
|
Y = Q*SW; |
289
|
3
|
|
|
|
|
|
Z = Y*SI; |
290
|
3
|
|
|
|
|
|
Y = Y*CI; |
291
|
3
|
|
|
|
|
|
PX = X*CO-Y*SO; |
292
|
3
|
|
|
|
|
|
Y = X*SO+Y*CO; |
293
|
3
|
|
|
|
|
|
PY = Y*CE-Z*SE; |
294
|
3
|
|
|
|
|
|
PZ = Y*SE+Z*CE; |
295
|
|
|
|
|
|
|
|
296
|
|
|
|
|
|
|
/* Velocity at perihelion (AU per canonical day). */ |
297
|
3
|
|
|
|
|
|
X = -PHS*SW; |
298
|
3
|
|
|
|
|
|
Y = PHS*CW; |
299
|
3
|
|
|
|
|
|
Z = Y*SI; |
300
|
3
|
|
|
|
|
|
Y = Y*CI; |
301
|
3
|
|
|
|
|
|
VX = X*CO-Y*SO; |
302
|
3
|
|
|
|
|
|
Y = X*SO+Y*CO; |
303
|
3
|
|
|
|
|
|
VY = Y*CE-Z*SE; |
304
|
3
|
|
|
|
|
|
VZ = Y*SE+Z*CE; |
305
|
|
|
|
|
|
|
|
306
|
|
|
|
|
|
|
/* Time from perihelion to date (in Canonical Days: a canonical day |
307
|
|
|
|
|
|
|
* is 58.1324409... days, defined as 1/PAL__GCON). */ |
308
|
|
|
|
|
|
|
|
309
|
3
|
|
|
|
|
|
DT = (date-PHT)*PAL__GCON; |
310
|
|
|
|
|
|
|
|
311
|
|
|
|
|
|
|
/* First approximation to the Universal Eccentric Anomaly, PSI, |
312
|
|
|
|
|
|
|
* based on the circle (FC) and parabola (FP) values. */ |
313
|
|
|
|
|
|
|
|
314
|
3
|
|
|
|
|
|
FC = DT/Q; |
315
|
3
|
|
|
|
|
|
W = pow(3.0*DT+sqrt(9.0*DT*DT+8.0*Q*Q*Q), 1.0/3.0); |
316
|
3
|
|
|
|
|
|
FP = W-2.0*Q/W; |
317
|
3
|
|
|
|
|
|
PSI = (1.0-e)*FC+e*FP; |
318
|
|
|
|
|
|
|
|
319
|
|
|
|
|
|
|
/* Assemble local copy of element set. */ |
320
|
3
|
|
|
|
|
|
UL[0] = CM; |
321
|
3
|
|
|
|
|
|
UL[1] = ALPHA; |
322
|
3
|
|
|
|
|
|
UL[2] = PHT; |
323
|
3
|
|
|
|
|
|
UL[3] = PX; |
324
|
3
|
|
|
|
|
|
UL[4] = PY; |
325
|
3
|
|
|
|
|
|
UL[5] = PZ; |
326
|
3
|
|
|
|
|
|
UL[6] = VX; |
327
|
3
|
|
|
|
|
|
UL[7] = VY; |
328
|
3
|
|
|
|
|
|
UL[8] = VZ; |
329
|
3
|
|
|
|
|
|
UL[9] = Q; |
330
|
3
|
|
|
|
|
|
UL[10] = 0.0; |
331
|
3
|
|
|
|
|
|
UL[11] = date; |
332
|
3
|
|
|
|
|
|
UL[12] = PSI; |
333
|
|
|
|
|
|
|
|
334
|
|
|
|
|
|
|
/* Predict position+velocity at epoch of osculation. */ |
335
|
3
|
|
|
|
|
|
palUe2pv( date, UL, PV, &J ); |
336
|
3
|
50
|
|
|
|
|
if (J != 0) { |
337
|
0
|
|
|
|
|
|
*jstat = -5; |
338
|
0
|
|
|
|
|
|
return; |
339
|
|
|
|
|
|
|
} |
340
|
|
|
|
|
|
|
|
341
|
|
|
|
|
|
|
/* Convert back to universal elements. */ |
342
|
3
|
|
|
|
|
|
palPv2ue( PV, date, CM-1.0, u, &J ); |
343
|
3
|
50
|
|
|
|
|
if (J != 0) { |
344
|
0
|
|
|
|
|
|
*jstat = -5; |
345
|
0
|
|
|
|
|
|
return; |
346
|
|
|
|
|
|
|
} |
347
|
|
|
|
|
|
|
|
348
|
|
|
|
|
|
|
/* OK exit. */ |
349
|
3
|
|
|
|
|
|
*jstat = 0; |
350
|
|
|
|
|
|
|
|
351
|
|
|
|
|
|
|
} |