line |
stmt |
bran |
cond |
sub |
pod |
time |
code |
1
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/* |
2
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*+ |
3
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* Name: |
4
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* palUe2el |
5
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6
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* Purpose: |
7
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* Universal elements to heliocentric osculating elements |
8
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9
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* Language: |
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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 palUe2el ( const double u[13], int jformr, |
17
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* int *jform, double *epoch, double *orbinc, |
18
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* double *anode, double *perih, double *aorq, double *e, |
19
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* double *aorl, double *dm, int *jstat ); |
20
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21
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* Arguments: |
22
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* u = const double [13] (Given) |
23
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* Universal orbital elements (Note 1) |
24
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* (0) combined mass (M+m) |
25
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* (1) total energy of the orbit (alpha) |
26
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* (2) reference (osculating) epoch (t0) |
27
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* (3-5) position at reference epoch (r0) |
28
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* (6-8) velocity at reference epoch (v0) |
29
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* (9) heliocentric distance at reference epoch |
30
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* (10) r0.v0 |
31
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* (11) date (t) |
32
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* (12) universal eccentric anomaly (psi) of date, approx |
33
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* jformr = int (Given) |
34
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* Requested element set (1-3; Note 3) |
35
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* jform = int * (Returned) |
36
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* Element set actually returned (1-3; Note 4) |
37
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* epoch = double * (Returned) |
38
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* Epoch of elements (TT MJD) |
39
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* orbinc = double * (Returned) |
40
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* inclination (radians) |
41
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* anode = double * (Returned) |
42
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* longitude of the ascending node (radians) |
43
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* perih = double * (Returned) |
44
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* longitude or argument of perihelion (radians) |
45
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* aorq = double * (Returned) |
46
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* mean distance or perihelion distance (AU) |
47
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* e = double * (Returned) |
48
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* eccentricity |
49
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* aorl = double * (Returned) |
50
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* mean anomaly or longitude (radians, JFORM=1,2 only) |
51
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* dm = double * (Returned) |
52
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* daily motion (radians, JFORM=1 only) |
53
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* jstat = int * (Returned) |
54
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* status: 0 = OK |
55
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* -1 = illegal combined mass |
56
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* -2 = illegal JFORMR |
57
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* -3 = position/velocity out of range |
58
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59
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* Description: |
60
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* Transform universal elements into conventional heliocentric |
61
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* osculating elements. |
62
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63
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* Authors: |
64
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* PTW: Patrick T. Wallace |
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 2). |
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 universal elements are with respect to the mean equator and |
83
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* equinox of epoch J2000. The orbital elements produced are with |
84
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* respect to the J2000 ecliptic and mean equinox. |
85
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* - Three different element-format options are supported: |
86
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* |
87
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* Option JFORM=1, suitable for the major planets: |
88
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* |
89
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* EPOCH = epoch of elements (TT MJD) |
90
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* ORBINC = inclination i (radians) |
91
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* ANODE = longitude of the ascending node, big omega (radians) |
92
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* PERIH = longitude of perihelion, curly pi (radians) |
93
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* AORQ = mean distance, a (AU) |
94
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* E = eccentricity, e |
95
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* AORL = mean longitude L (radians) |
96
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* DM = daily motion (radians) |
97
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* |
98
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* Option JFORM=2, suitable for minor planets: |
99
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* |
100
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* EPOCH = epoch of elements (TT MJD) |
101
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* ORBINC = inclination i (radians) |
102
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* ANODE = longitude of the ascending node, big omega (radians) |
103
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* PERIH = argument of perihelion, little omega (radians) |
104
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* AORQ = mean distance, a (AU) |
105
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* E = eccentricity, e |
106
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* AORL = mean anomaly M (radians) |
107
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* |
108
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* Option JFORM=3, suitable for comets: |
109
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* |
110
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* EPOCH = epoch of perihelion (TT MJD) |
111
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* ORBINC = inclination i (radians) |
112
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* ANODE = longitude of the ascending node, big omega (radians) |
113
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* PERIH = argument of perihelion, little omega (radians) |
114
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* AORQ = perihelion distance, q (AU) |
115
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* E = eccentricity, e |
116
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* |
117
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* - It may not be possible to generate elements in the form |
118
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* requested through JFORMR. The caller is notified of the form |
119
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* of elements actually returned by means of the JFORM argument: |
120
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* |
121
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* JFORMR JFORM meaning |
122
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* |
123
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* 1 1 OK - elements are in the requested format |
124
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* 1 2 never happens |
125
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* 1 3 orbit not elliptical |
126
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* |
127
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* 2 1 never happens |
128
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* 2 2 OK - elements are in the requested format |
129
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* 2 3 orbit not elliptical |
130
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* |
131
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* 3 1 never happens |
132
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* 3 2 never happens |
133
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* 3 3 OK - elements are in the requested format |
134
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* |
135
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* - The arguments returned for each value of JFORM (cf Note 6: JFORM |
136
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* may not be the same as JFORMR) are as follows: |
137
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* |
138
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* JFORM 1 2 3 |
139
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* EPOCH t0 t0 T |
140
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* ORBINC i i i |
141
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* ANODE Omega Omega Omega |
142
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* PERIH curly pi omega omega |
143
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* AORQ a a q |
144
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* E e e e |
145
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* AORL L M - |
146
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* DM n - - |
147
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* |
148
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* where: |
149
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* |
150
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* t0 is the epoch of the elements (MJD, TT) |
151
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* T " epoch of perihelion (MJD, TT) |
152
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* i " inclination (radians) |
153
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* Omega " longitude of the ascending node (radians) |
154
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* curly pi " longitude of perihelion (radians) |
155
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* omega " argument of perihelion (radians) |
156
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* a " mean distance (AU) |
157
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* q " perihelion distance (AU) |
158
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* e " eccentricity |
159
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* L " longitude (radians, 0-2pi) |
160
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* M " mean anomaly (radians, 0-2pi) |
161
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* n " daily motion (radians) |
162
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* - means no value is set |
163
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* |
164
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* - At very small inclinations, the longitude of the ascending node |
165
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* ANODE becomes indeterminate and under some circumstances may be |
166
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* set arbitrarily to zero. Similarly, if the orbit is close to |
167
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* circular, the true anomaly becomes indeterminate and under some |
168
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* circumstances may be set arbitrarily to zero. In such cases, |
169
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* the other elements are automatically adjusted to compensate, |
170
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* and so the elements remain a valid description of the orbit. |
171
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172
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* See Also: |
173
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* - Sterne, Theodore E., "An Introduction to Celestial Mechanics", |
174
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* Interscience Publishers Inc., 1960. Section 6.7, p199. |
175
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* - Everhart, E. & Pitkin, E.T., Am.J.Phys. 51, 712, 1983. |
176
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177
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* History: |
178
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* 2012-03-09 (TIMJ): |
179
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* Initial version |
180
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* Adapted with permission from the Fortran SLALIB library. |
181
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* {enter_further_changes_here} |
182
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183
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* Copyright: |
184
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* Copyright (C) 1999 Rutherford Appleton Laboratory |
185
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* Copyright (C) 2012 Science and Technology Facilities Council. |
186
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* All Rights Reserved. |
187
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188
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* Licence: |
189
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* This program is free software; you can redistribute it and/or |
190
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* modify it under the terms of the GNU General Public License as |
191
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* published by the Free Software Foundation; either version 3 of |
192
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* the License, or (at your option) any later version. |
193
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* |
194
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* This program is distributed in the hope that it will be |
195
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* useful, but WITHOUT ANY WARRANTY; without even the implied |
196
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* warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR |
197
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* PURPOSE. See the GNU General Public License for more details. |
198
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* |
199
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* You should have received a copy of the GNU General Public License |
200
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* along with this program; if not, write to the Free Software |
201
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* Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, |
202
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* MA 02110-1301, USA. |
203
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204
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* Bugs: |
205
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* {note_any_bugs_here} |
206
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*- |
207
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*/ |
208
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209
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#include "pal.h" |
210
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#include "palmac.h" |
211
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212
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2
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void palUe2el ( const double u[], int jformr, |
213
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int *jform, double *epoch, double *orbinc, |
214
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double *anode, double *perih, double *aorq, double *e, |
215
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double *aorl, double *dm, int *jstat ) { |
216
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217
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/* Canonical days to seconds */ |
218
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const double CD2S = PAL__GCON / PAL__SPD; |
219
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220
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int i; |
221
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double pmass, date, pv[6]; |
222
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223
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/* Unpack the universal elements */ |
224
|
2
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pmass = u[0] - 1.0; |
225
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2
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date = u[2]; |
226
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8
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100
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for (i=0; i<3; i++) { |
227
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6
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|
|
pv[i] = u[i+3]; |
228
|
6
|
|
|
|
|
|
pv[i+3] = u[i+6] * CD2S; |
229
|
|
|
|
|
|
|
} |
230
|
|
|
|
|
|
|
|
231
|
|
|
|
|
|
|
/* Convert the position and velocity etc into conventional elements */ |
232
|
2
|
|
|
|
|
|
palPv2el( pv, date, pmass, jformr, jform, epoch, orbinc, anode, |
233
|
|
|
|
|
|
|
perih, aorq, e, aorl, dm, jstat ); |
234
|
2
|
|
|
|
|
|
} |