/rust/registry/src/index.crates.io-1949cf8c6b5b557f/sofars-0.6.1/src/star/hfk5z.rs
Line | Count | Source |
1 | | use crate::consts::{DJ00, DJY}; |
2 | | use crate::star::fk5hip; |
3 | | use crate::vm::{anp, pv2s, rv2m, rxp, rxr, s2c, sxp, trxp, pxp}; |
4 | | |
5 | | /// Transform a Hipparcos star position into FK5 J2000.0, assuming |
6 | | /// zero Hipparcos proper motion. |
7 | | /// |
8 | | /// Status: support function. |
9 | | /// |
10 | | /// Given: |
11 | | /// rh f64 Hipparcos RA (radians) |
12 | | /// dh f64 Hipparcos Dec (radians) |
13 | | /// date1,date2 f64 TDB date (Note 1) |
14 | | /// |
15 | | /// Returned (all FK5, equinox J2000.0, date date1+date2): |
16 | | /// r5 f64 RA (radians) |
17 | | /// d5 f64 Dec (radians) |
18 | | /// dr5 f64 RA proper motion (rad/year, Note 4) |
19 | | /// dd5 f64 Dec proper motion (rad/year, Note 4) |
20 | | /// |
21 | | /// Notes: |
22 | | /// |
23 | | /// 1) The TT date date1+date2 is a Julian Date, apportioned in any |
24 | | /// convenient way between the two arguments. For example, |
25 | | /// JD(TT)=2450123.7 could be expressed in any of these ways, |
26 | | /// among others: |
27 | | /// |
28 | | /// date1 date2 |
29 | | /// |
30 | | /// 2450123.7 0.0 (JD method) |
31 | | /// 2451545.0 -1421.3 (J2000 method) |
32 | | /// 2400000.5 50123.2 (MJD method) |
33 | | /// 2450123.5 0.2 (date & time method) |
34 | | /// |
35 | | /// The JD method is the most natural and convenient to use in |
36 | | /// cases where the loss of several decimal digits of resolution |
37 | | /// is acceptable. The J2000 method is best matched to the way |
38 | | /// the argument is handled internally and will deliver the |
39 | | /// optimum resolution. The MJD method and the date & time methods |
40 | | /// are both good compromises between resolution and convenience. |
41 | | /// |
42 | | /// 2) The proper motion in RA is dRA/dt rather than cos(Dec)*dRA/dt. |
43 | | /// |
44 | | /// 3) The FK5 to Hipparcos transformation is modeled as a pure rotation |
45 | | /// and spin; zonal errors in the FK5 catalog are not taken into |
46 | | /// account. |
47 | | /// |
48 | | /// 4) It was the intention that Hipparcos should be a close |
49 | | /// approximation to an inertial frame, so that distant objects have |
50 | | /// zero proper motion; such objects have (in general) non-zero |
51 | | /// proper motion in FK5, and this function returns those fictitious |
52 | | /// proper motions. |
53 | | /// |
54 | | /// 5) The position returned by this function is in the FK5 J2000.0 |
55 | | /// reference system but at date date1+date2. |
56 | | /// |
57 | | /// 6) See also fk52h, h2fk5, fk5hz. |
58 | | /// |
59 | | /// Called: |
60 | | /// s2c spherical coordinates to unit vector |
61 | | /// fk5hip FK5 to Hipparcos rotation and spin |
62 | | /// rxp product of r-matrix and p-vector |
63 | | /// sxp multiply p-vector by scalar |
64 | | /// rv2m r-vector to r-matrix |
65 | | /// rxr product of two r-matrices |
66 | | /// trxp product of transpose of r-matrix and p-vector |
67 | | /// pxp vector product of two p-vectors |
68 | | /// pv2s pv-vector to spherical |
69 | | /// anp normalize angle into range 0 to 2pi |
70 | | /// |
71 | | /// Reference: |
72 | | /// F.Mignard & M.Froeschle, 2000, Astron.Astrophys. 354, 732-739. |
73 | 0 | pub fn hfk5z(rh: f64, dh: f64, date1: f64, date2: f64) -> (f64, f64, f64, f64) { |
74 | 0 | let mut sh = [0.0; 3]; |
75 | 0 | let mut rst = [[0.0; 3]; 3]; |
76 | 0 | let mut r5ht = [[0.0; 3]; 3]; |
77 | 0 | let mut pv5e = [[0.0; 3]; 2]; |
78 | | |
79 | | /* Time interval from fundamental epoch J2000.0 to given date (JY). */ |
80 | 0 | let t = ((date1 - DJ00) + date2) / DJY; |
81 | | |
82 | | /* Hipparcos barycentric position vector (normalized). */ |
83 | 0 | let ph = s2c(rh, dh); |
84 | | |
85 | | /* FK5 to Hipparcos orientation matrix and spin vector. */ |
86 | 0 | let (r5h, s5h) = fk5hip(); |
87 | | |
88 | | /* Rotate the spin into the Hipparcos system. */ |
89 | 0 | rxp(&r5h, &s5h, &mut sh); |
90 | | |
91 | | /* Accumulated Hipparcos wrt FK5 spin over that interval. */ |
92 | 0 | let vst = sxp(t, &s5h); |
93 | | |
94 | | /* Express the accumulated spin as a rotation matrix. */ |
95 | 0 | rv2m(&vst, &mut rst); |
96 | | |
97 | | /* Rotation matrix: accumulated spin, then FK5 to Hipparcos. */ |
98 | 0 | rxr(&r5h, &rst, &mut r5ht); |
99 | | |
100 | | /* De-orient & de-spin the Hipparcos position into FK5 J2000.0. */ |
101 | 0 | trxp(&r5ht, &ph, &mut pv5e[0]); |
102 | | |
103 | | /* Apply spin to the position giving a space motion. */ |
104 | 0 | let vv = pxp(&sh, &ph); |
105 | | |
106 | | /* De-orient & de-spin the Hipparcos space motion into FK5 J2000.0. */ |
107 | 0 | trxp(&r5ht, &vv, &mut pv5e[1]); |
108 | | |
109 | | /* FK5 position/velocity pv-vector to spherical. */ |
110 | 0 | let (w, d5, _, dr5, dd5, _) = pv2s(&pv5e); |
111 | 0 | let r5 = anp(w); |
112 | | |
113 | 0 | (r5, d5, dr5, dd5) |
114 | 0 | } |