[1457] | 1 | /* heliocentric rectangular equatorial coordinates of Jupiter to Pluto;
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| 2 | * from Chapront's expansion of DE200/extension of DE200; mean equator J2000.0
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| 3 | *
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| 4 | * calculation time (milliseconds) on an HP 715/75, Jupiter to Pluto:
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| 5 | * (each coordinate component counted as 1 term,
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| 6 | * secular terms included for JD 2448908.5 = 1992 Oct 13.0)
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| 7 | *
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| 8 | * prec terms rates no rates
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| 9 | * 0.0 2256 5.1 4.6
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| 10 | *
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| 11 | * 1e-7 792 2.6 2.4 --> nominal precision rel. to DE200
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| 12 | * 1e-6 535 2.1 2.0
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| 13 | * 1e-5 350 1.8 1.6
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| 14 | * 1e-4 199 1.5 1.4
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| 15 | * 1e-3 96 1.2 1.1
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| 16 | *
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| 17 | * no drop 2256 4.5 3.9 (code without test criterion)
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| 18 | */
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| 19 |
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| 20 | #include <math.h>
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| 21 | #include "P_.h"
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| 22 | #include "astro.h"
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| 23 | #include "chap95.h"
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| 24 |
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| 25 | extern void zero_mem P_((void *loc, unsigned len));
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| 26 |
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| 27 | #define CHAP_MAXTPOW 2 /* NB: valid for all 5 outer planets */
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| 28 |
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| 29 | /* chap95()
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| 30 | *
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| 31 | * input:
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| 32 | * mjd modified JD; days from J1900.0 = 2415020.0
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| 33 | *
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| 34 | * prec precision level, in radians.
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| 35 | * if (prec = 0.0), you get the full precision, namely
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| 36 | * a deviation of not more than 0.02 arc seconds (1e-7 rad)
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| 37 | * from the JPL DE200 integration, on which this expansion
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| 38 | * is based.
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| 39 | *
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| 40 | * obj object number as in astro.h (jupiter=3, saturn=4, ...)
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| 41 | *
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| 42 | * output:
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| 43 | * ret[6] cartesian components of position and velocity
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| 44 | *
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| 45 | * return:
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| 46 | * 0 Ok
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| 47 | * 1 time out of range [CHAP_BEGIN .. CHAP_END]
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| 48 | * 2 object out of range [JUPITER .. PLUTO]
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| 49 | * 3 precision out of range [0.0 .. 1e-3]
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| 50 | */
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| 51 | int
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| 52 | chap95 (mjd, obj, prec, ret)
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| 53 | double mjd;
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| 54 | int obj;
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| 55 | double prec;
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| 56 | double *ret;
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| 57 | {
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| 58 | static double a0[] = { /* semimajor axes for precision ctrl */
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| 59 | 0.39, 0.72, 1.5, 5.2, 9.6, 19.2, 30.1, 39.5, 1.0
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| 60 | };
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| 61 | double sum[CHAP_MAXTPOW+1][6]; /* [T^0, ..][X,Y,Z,X',Y',Z'] */
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| 62 | double T, t; /* time in centuries and years */
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| 63 | double ca, sa, Nu; /* aux vars for terms */
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| 64 | double precT[CHAP_MAXTPOW+1]; /* T-augmented precision threshold */
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| 65 | chap95_rec *rec; /* term coeffs */
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| 66 | int cooidx;
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| 67 |
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| 68 | /* check parameters */
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| 69 | if (mjd < CHAP_BEGIN || mjd > CHAP_END)
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| 70 | return (1);
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| 71 |
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| 72 | if (obj < JUPITER || obj > PLUTO)
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| 73 | return (2);
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| 74 |
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| 75 | if (prec < 0.0 || prec > 1e-3)
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| 76 | return (3);
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| 77 |
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| 78 | /* init the sums */
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| 79 | zero_mem ((void *)sum, sizeof(sum));
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| 80 |
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| 81 | T = (mjd - J2000)/36525.0; /* centuries since J2000.0 */
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| 82 |
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| 83 | /* modify precision treshold for
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| 84 | * a) term storing scale
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| 85 | * b) convert radians to au
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| 86 | * c) account for skipped terms (more terms needed for better prec)
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| 87 | * threshold empirically established similar to VSOP; stern
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| 88 | * d) augment for secular terms
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| 89 | */
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| 90 | precT[0] = prec * CHAP_SCALE /* a) */
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| 91 | * a0[obj] /* b) */
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| 92 | / (10. * (-log10(prec + 1e-35) - 2)); /* c) */
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| 93 | t = 1./(fabs(T) + 1e-35); /* d) */
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| 94 | precT[1] = precT[0]*t;
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| 95 | precT[2] = precT[1]*t;
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| 96 |
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| 97 | t = T * 100.0; /* YEARS since J2000.0 */
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| 98 |
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| 99 | ca = sa = Nu = 0.; /* shut up compiler warning 'uninitialised' */
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| 100 |
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| 101 | switch (obj) { /* set initial term record pointer */
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| 102 | case JUPITER: rec = chap95_jupiter; break;
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| 103 | case SATURN: rec = chap95_saturn; break;
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| 104 | case URANUS: rec = chap95_uranus; break;
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| 105 | case NEPTUNE: rec = chap95_neptune; break;
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| 106 | case PLUTO: rec = chap95_pluto; break;
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| 107 | default:
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| 108 | return (2); /* wrong object: severe internal trouble */
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| 109 | }
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| 110 |
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| 111 | /* do the term summation into sum[T^n] slots */
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| 112 | for (; rec->n >= 0; ++rec) {
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| 113 | double *amp;
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| 114 |
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| 115 | /* NOTE: The formula
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| 116 | * X = SUM[i=1,Records] T**n_i*(CX_i*cos(Nu_k*t)+SX_i*sin(Nu_k*t))
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| 117 | * could be rewritten as SUM( ... A sin (B + C*t) )
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| 118 | * "saving" trigonometric calls. However, e.g. for Pluto,
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| 119 | * there are only 65 distinct angles NU_k (130 trig calls).
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| 120 | * With that manipulation, EVERY arg_i would be different for X,
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| 121 | * Y and Z, which is 3*96 terms. Hence, the formulation as
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| 122 | * given is good (optimal?).
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| 123 | */
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| 124 |
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| 125 | for (cooidx = 0, amp = rec->amp; cooidx < 3; ++cooidx) {
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| 126 | double C, S, term, termdot;
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| 127 | short n; /* fast access */
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| 128 |
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| 129 | C = *amp++;
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| 130 | S = *amp++;
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| 131 | n = rec->n;
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| 132 |
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| 133 | /* drop term if too small
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| 134 | * this is quite expensive: 17% of loop time
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| 135 | */
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| 136 | if (fabs(C) + fabs(S) < precT[n])
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| 137 | continue;
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| 138 |
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| 139 | if (n == 0 && cooidx == 0) { /* new Nu only here */
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| 140 | double arg;
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| 141 |
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| 142 | Nu = rec->Nu;
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| 143 | arg = Nu * t;
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| 144 | arg -= floor(arg/(2.*PI))*(2.*PI);
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| 145 | ca = cos(arg); /* blast it - even for Nu = 0.0 */
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| 146 | sa = sin(arg);
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| 147 | }
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| 148 |
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| 149 | term = C * ca + S * sa;
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| 150 | sum[n][cooidx] += term;
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| 151 | #if CHAP_GETRATE
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| 152 | termdot = (-C * sa + S * ca) * Nu;
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| 153 | sum[n][cooidx+3] += termdot;
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| 154 | if (n > 0) sum[n - 1][cooidx+3] += n/100.0 * term;
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| 155 | #endif
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| 156 | } /* cooidx */
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| 157 | } /* records */
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| 158 |
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| 159 | /* apply powers of time and sum up */
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| 160 | for (cooidx = 0; cooidx < 6; ++cooidx) {
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| 161 | ret[cooidx] = (sum[0][cooidx] +
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| 162 | T * (sum[1][cooidx] +
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| 163 | T * (sum[2][cooidx] )) )/CHAP_SCALE;
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| 164 | }
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| 165 |
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| 166 | /* TEST: if the MAIN terms are dropped, get angular residue
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| 167 | ret[0] = sqrt(ret[0]*ret[0] + ret[1]*ret[1] + ret[2]*ret[2])/a0[obj];
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| 168 | */
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| 169 |
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| 170 | #if CHAP_GETRATE
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| 171 | for (cooidx = 3; cooidx < 6; ++cooidx) {
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| 172 | ret[cooidx] /= 365.25; /* yearly to daily rate */
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| 173 | }
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| 174 | #endif
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| 175 |
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| 176 | return (0);
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| 177 | }
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| 178 |
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| 179 | /* For RCS Only -- Do Not Edit */
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| 180 | static char *rcsid[2] = {(char *)rcsid, "@(#) $RCSfile: chap95.c,v $ $Date: 2001-04-10 14:40:46 $ $Revision: 1.1.1.1 $ $Name: not supported by cvs2svn $"};
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