| line |
stmt |
bran |
cond |
sub |
pod |
time |
code |
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1
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/* |
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2
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*+ |
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3
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* Name: |
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4
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* palUe2el |
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5
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6
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* Purpose: |
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7
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* Universal elements to heliocentric osculating elements |
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8
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9
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* Language: |
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10
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* Starlink ANSI C |
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11
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12
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* Type of Module: |
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13
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* Library routine |
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14
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15
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* Invocation: |
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16
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* void palUe2el ( const double u[13], int jformr, |
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17
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* int *jform, double *epoch, double *orbinc, |
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18
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* double *anode, double *perih, double *aorq, double *e, |
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19
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* double *aorl, double *dm, int *jstat ); |
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20
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21
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* Arguments: |
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22
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* u = const double [13] (Given) |
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23
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* Universal orbital elements (Note 1) |
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24
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* (0) combined mass (M+m) |
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25
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* (1) total energy of the orbit (alpha) |
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26
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* (2) reference (osculating) epoch (t0) |
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27
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* (3-5) position at reference epoch (r0) |
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28
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* (6-8) velocity at reference epoch (v0) |
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29
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* (9) heliocentric distance at reference epoch |
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30
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* (10) r0.v0 |
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31
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* (11) date (t) |
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32
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* (12) universal eccentric anomaly (psi) of date, approx |
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33
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* jformr = int (Given) |
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34
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* Requested element set (1-3; Note 3) |
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35
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* jform = int * (Returned) |
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36
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* Element set actually returned (1-3; Note 4) |
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37
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* epoch = double * (Returned) |
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38
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* Epoch of elements (TT MJD) |
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39
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* orbinc = double * (Returned) |
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40
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* inclination (radians) |
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41
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* anode = double * (Returned) |
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42
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* longitude of the ascending node (radians) |
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43
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* perih = double * (Returned) |
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44
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* longitude or argument of perihelion (radians) |
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45
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* aorq = double * (Returned) |
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46
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* mean distance or perihelion distance (AU) |
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47
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* e = double * (Returned) |
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48
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* eccentricity |
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49
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* aorl = double * (Returned) |
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50
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* mean anomaly or longitude (radians, JFORM=1,2 only) |
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51
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* dm = double * (Returned) |
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52
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* daily motion (radians, JFORM=1 only) |
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53
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* jstat = int * (Returned) |
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54
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* status: 0 = OK |
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55
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* -1 = illegal combined mass |
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56
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* -2 = illegal JFORMR |
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57
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* -3 = position/velocity out of range |
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58
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59
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* Description: |
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60
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* Transform universal elements into conventional heliocentric |
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61
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* osculating elements. |
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62
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63
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* Authors: |
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64
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* PTW: Patrick T. Wallace |
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65
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* TIMJ: Tim Jenness (JAC, Hawaii) |
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66
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* {enter_new_authors_here} |
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67
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68
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* Notes: |
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69
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* - The "universal" elements are those which define the orbit for the |
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70
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* purposes of the method of universal variables (see reference 2). |
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71
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* They consist of the combined mass of the two bodies, an epoch, |
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72
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* and the position and velocity vectors (arbitrary reference frame) |
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73
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* at that epoch. The parameter set used here includes also various |
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74
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* quantities that can, in fact, be derived from the other |
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75
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* information. This approach is taken to avoiding unnecessary |
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76
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* computation and loss of accuracy. The supplementary quantities |
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77
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* are (i) alpha, which is proportional to the total energy of the |
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78
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* orbit, (ii) the heliocentric distance at epoch, (iii) the |
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79
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* outwards component of the velocity at the given epoch, (iv) an |
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80
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* estimate of psi, the "universal eccentric anomaly" at a given |
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81
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* date and (v) that date. |
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82
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* - The universal elements are with respect to the mean equator and |
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83
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* equinox of epoch J2000. The orbital elements produced are with |
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84
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* respect to the J2000 ecliptic and mean equinox. |
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85
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* - Three different element-format options are supported: |
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86
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* |
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87
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* Option JFORM=1, suitable for the major planets: |
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88
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* |
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89
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* EPOCH = epoch of elements (TT MJD) |
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90
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* ORBINC = inclination i (radians) |
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91
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* ANODE = longitude of the ascending node, big omega (radians) |
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92
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* PERIH = longitude of perihelion, curly pi (radians) |
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93
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* AORQ = mean distance, a (AU) |
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94
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* E = eccentricity, e |
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95
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* AORL = mean longitude L (radians) |
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96
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* DM = daily motion (radians) |
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97
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* |
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98
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* Option JFORM=2, suitable for minor planets: |
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99
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* |
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100
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* EPOCH = epoch of elements (TT MJD) |
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101
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* ORBINC = inclination i (radians) |
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102
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* ANODE = longitude of the ascending node, big omega (radians) |
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103
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* PERIH = argument of perihelion, little omega (radians) |
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104
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* AORQ = mean distance, a (AU) |
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105
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* E = eccentricity, e |
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106
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* AORL = mean anomaly M (radians) |
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107
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* |
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108
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* Option JFORM=3, suitable for comets: |
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109
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* |
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110
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* EPOCH = epoch of perihelion (TT MJD) |
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111
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* ORBINC = inclination i (radians) |
|
112
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* ANODE = longitude of the ascending node, big omega (radians) |
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113
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* PERIH = argument of perihelion, little omega (radians) |
|
114
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* AORQ = perihelion distance, q (AU) |
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115
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* E = eccentricity, e |
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116
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* |
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117
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* - It may not be possible to generate elements in the form |
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118
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* requested through JFORMR. The caller is notified of the form |
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119
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* of elements actually returned by means of the JFORM argument: |
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120
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* |
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121
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* JFORMR JFORM meaning |
|
122
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* |
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123
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* 1 1 OK - elements are in the requested format |
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124
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* 1 2 never happens |
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125
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* 1 3 orbit not elliptical |
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126
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* |
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127
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* 2 1 never happens |
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128
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* 2 2 OK - elements are in the requested format |
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129
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* 2 3 orbit not elliptical |
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130
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* |
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131
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* 3 1 never happens |
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132
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* 3 2 never happens |
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133
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* 3 3 OK - elements are in the requested format |
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134
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* |
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135
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* - The arguments returned for each value of JFORM (cf Note 6: JFORM |
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136
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* may not be the same as JFORMR) are as follows: |
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137
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* |
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138
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* JFORM 1 2 3 |
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139
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* EPOCH t0 t0 T |
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140
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* ORBINC i i i |
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141
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* ANODE Omega Omega Omega |
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142
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* PERIH curly pi omega omega |
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143
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* AORQ a a q |
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144
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* E e e e |
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145
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* AORL L M - |
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146
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* DM n - - |
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147
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* |
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148
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* where: |
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149
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* |
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150
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* t0 is the epoch of the elements (MJD, TT) |
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151
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* T " epoch of perihelion (MJD, TT) |
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152
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* i " inclination (radians) |
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153
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* Omega " longitude of the ascending node (radians) |
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154
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* curly pi " longitude of perihelion (radians) |
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155
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* omega " argument of perihelion (radians) |
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156
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* a " mean distance (AU) |
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157
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* q " perihelion distance (AU) |
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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) |
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161
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* n " daily motion (radians) |
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162
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* - means no value is set |
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163
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* |
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164
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* - At very small inclinations, the longitude of the ascending node |
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165
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* ANODE becomes indeterminate and under some circumstances may be |
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166
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* set arbitrarily to zero. Similarly, if the orbit is close to |
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167
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* circular, the true anomaly becomes indeterminate and under some |
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168
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* circumstances may be set arbitrarily to zero. In such cases, |
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169
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* the other elements are automatically adjusted to compensate, |
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170
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* and so the elements remain a valid description of the orbit. |
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171
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172
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* See Also: |
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173
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* - Sterne, Theodore E., "An Introduction to Celestial Mechanics", |
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174
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* Interscience Publishers Inc., 1960. Section 6.7, p199. |
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175
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* - Everhart, E. & Pitkin, E.T., Am.J.Phys. 51, 712, 1983. |
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176
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177
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* History: |
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178
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* 2012-03-09 (TIMJ): |
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179
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* Initial version |
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180
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* Adapted with permission from the Fortran SLALIB library. |
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181
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* {enter_further_changes_here} |
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182
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183
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* Copyright: |
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184
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* Copyright (C) 1999 Rutherford Appleton Laboratory |
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185
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* Copyright (C) 2012 Science and Technology Facilities Council. |
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186
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* All Rights Reserved. |
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187
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188
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* Licence: |
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189
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* This program is free software; you can redistribute it and/or |
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190
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* modify it under the terms of the GNU General Public License as |
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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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* |
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194
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* This program is distributed in the hope that it will be |
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195
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* useful, but WITHOUT ANY WARRANTY; without even the implied |
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196
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* warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR |
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197
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* PURPOSE. See the GNU General Public License for more details. |
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198
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* |
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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. |
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203
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204
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* Bugs: |
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205
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* {note_any_bugs_here} |
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206
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*- |
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207
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*/ |
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208
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209
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#include "pal.h" |
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210
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#include "palmac.h" |
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211
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212
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2
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void palUe2el ( const double u[], int jformr, |
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213
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int *jform, double *epoch, double *orbinc, |
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214
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double *anode, double *perih, double *aorq, double *e, |
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215
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double *aorl, double *dm, int *jstat ) { |
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216
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217
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/* Canonical days to seconds */ |
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218
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const double CD2S = PAL__GCON / PAL__SPD; |
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219
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220
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int i; |
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221
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double pmass, date, pv[6]; |
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222
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223
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/* Unpack the universal elements */ |
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224
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2
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pmass = u[0] - 1.0; |
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225
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2
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date = u[2]; |
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226
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8
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100
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for (i=0; i<3; i++) { |
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227
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6
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pv[i] = u[i+3]; |
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228
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6
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pv[i+3] = u[i+6] * CD2S; |
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229
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} |
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230
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231
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/* Convert the position and velocity etc into conventional elements */ |
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232
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2
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palPv2el( pv, date, pmass, jformr, jform, epoch, orbinc, anode, |
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233
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perih, aorq, e, aorl, dm, jstat ); |
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234
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2
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} |