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卷51 志二十六 时宪七

Volume 51 Treatises 26: Calendar 7

Chapter 51 of 清史稿 · Draft History of Qing
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Chapter 51
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1
Treatise 26
2
Shixian Calendar 7
3
Yongzheng guimao calendrical system — lower section
4
Constants for lunar eclipse calculation
5
New-moon interval constant: 29.53059053 days.
6
Full-moon interval constant: 14.765295265 days.
7
Moon's nodal motion per synodic month: 110,413 seconds, fractional remainder 0.92441334.
8
Moon's nodal motion per half-month: 6 mansions 15°20′06.58″.
9
Moon's diurnal parallax at mean distance: 57′30″.
10
Sun's maximum diurnal parallax: 10″.
11
Sun's geocentric distance at mean distance: 10,000,000.
12
Moon's geocentric distance at mean distance: 10,000,000.
13
Sun's apparent semidiameter at mean distance: 16′06″.
14
Moon's apparent semidiameter at mean distance: 15′40.30″.
15
Epoch new-moon offset: 15.12633 days.
16
At the epoch new moon, the moon's nodal longitude should be 23°36′52.49″ in the sixth mansion. For the remaining constants, see the sections on solar motion and lunar distance.
17
Procedure for computing lunar eclipses
18
To find the winter solstice of the civil year (as in the jiazi epoch method),
19
To find the cycle-day count (as in the jiazi epoch method),
20
To find the epoch new moon (as in the jiazi epoch method),
21
To determine whether the moon enters the eclipse zone, use the same method as in the jiazi epoch system. If in a given month the moon's mean nodal longitude falls within the eclipse zone, that month will have an eclipse. The eclipse zone extends from 14°51′ in the fifth mansion to 15°09′ in the sixth, and from 14°51′ in the eleventh mansion to 15°09′ in the first. Refine this at the true time by the distance from the true node.
22
To find the mean full moon, use the same method as in the jiazi epoch system.
23
To find the true time of full moon, first find the approximate time by comparing true motions over two days—by the same method as in the jiazi epoch system for new and full moon. Next set two times before and after, and compute the true ecliptic longitudes of the sun and moon at each. By comparing true motions at the two times, obtain the true time of full moon. At the true time, compute the true ecliptic longitudes of the sun and moon; if the moon's distance from the true node at that instant falls within the limit, an eclipse occurs. At true time the eclipse limits are from 17°43′ in the fifth mansion to 12°17′ in the sixth, and from 17°43′ in the eleventh mansion to 12°17′ in the first.
24
To find the apparent time of true full moon, compute the sun's equation of center at true time and the rising-degree correction by the same method as in the jiazi epoch system. The comparison with sunrise and sunset is the same as well.
25
To find the time of greatest eclipse, by plane triangle: convert the moon's hourly true motion along the white path to seconds as one side, and compare true motions at the current and following hours. Use the sun's hourly true ecliptic motion in seconds as the other side and the great ecliptic-lunar distance at true full moon as the included angle; the angle opposite the shorter side is the oblique-separation nodal-angle correction. Add this to the true-time great ecliptic-lunar distance to obtain the oblique-separation ecliptic nodal angle. Use the sine of the oblique-separation nodal-angle correction, the sun's hourly true motion, and the sine of the great ecliptic-lunar distance at true full moon; the fourth ratio is the hourly oblique separation of the two longitudes. Use the radius of ten million, the cosine and sine of the oblique-separation ecliptic nodal angle, and the moon's true ecliptic latitude at true full moon; the results give the north-south true latitude at greatest eclipse, equal to the true ecliptic latitude at true full moon. And the interval arc. Use the hourly oblique separation of the two longitudes, one hour in seconds, and the interval arc at greatest eclipse; the fourth ratio is the interval time to greatest eclipse. Add or subtract this from the apparent time of true full moon: subtract when the moon is at the first or sixth mansion from the true node, add at the fifth or eleventh. This yields the time of greatest eclipse.
26
To find the sun's and moon's true anomalies: take the sun's anomaly at true full moon and apply the equation of center at the current time to obtain the sun's true anomaly. Take the moon's anomaly at true full moon and apply the moon's first equation at the current time to obtain the moon's true anomaly.
27
To find the true umbral radius: use the moon's geocentric distance, the mean-distance lunar distance, and the moon's maximum diurnal parallax at mean distance; the fourth ratio is the moon's maximum parallax at the current time. Divide by sixty-nine to obtain the shadow correction. Use the sun's geocentric distance, the mean-distance solar distance, and the sun's apparent semidiameter at mean distance; subtract the result from the moon's maximum parallax at the current time. Add the sun's maximum parallax to obtain the shadow semidiameter; add the shadow correction to obtain the true umbral semidiameter.
28
To find the moon's apparent semidiameter: use the moon's geocentric distance, the mean-distance lunar distance, and the moon's apparent semidiameter at mean distance. With these known:
29
To find the eclipse magnitude: use the moon's full diameter as the first ratio and ten tenths (600 seconds) as the second; the third ratio is the sum of the true shadow and lunar semidiameters. Subtract the true latitude at greatest eclipse; convert the remainder to seconds as the third ratio; reduce the fourth ratio to minutes to obtain the eclipse magnitude.
30
To find the times of first and last contact: add and subtract the combined diameter and the true latitude at greatest eclipse, convert to seconds as first and last ratios; convert the middle ratio to minutes as the contact interval arcs. Use the hourly oblique separation, one hour in seconds, and the contact interval arcs; apply the resulting interval times to the time of greatest eclipse to obtain the times of first and last contact. Subtract for first contact; add for last contact.
31
To find the times when totality begins and light returns: take the difference of the two semidiameters—the true shadow and the lunar semidiameter. Add and subtract this from the true latitude at greatest eclipse and convert to seconds as first and last ratios; convert the middle ratio to minutes as the totality interval arcs. To find the interval times, use the same method as for first and last contact. If the eclipse magnitude is less than ten tenths, these two limits do not apply.
32
To find the total duration of the eclipse, use the same method as in the jiazi epoch system.
33
宿 宿
To find the moon's ecliptic longitude, latitude, and mansion at greatest eclipse: use one hour in seconds, the moon's hourly true motion along the white path, and the interval time to greatest eclipse in seconds; the fourth ratio is the moon's true motion over that interval. Add or subtract this from the moon's true white-path longitude at true full moon, with the same sign as the interval time to greatest eclipse. This yields the moon's white-path longitude at greatest eclipse. Take the moon's distance from the true node at true full moon and apply the interval motion to obtain the distance from the true node at greatest eclipse. Then compute the ecliptic longitude, latitude, and mansion by the same method as in the lunar-distance section.
34
宿 宿
To find the moon's equatorial longitude, latitude, and mansion at greatest eclipse: use the radius of ten million and the sine of the moon's ecliptic longitude measured from the equinox; if the moon's ecliptic longitude is less than three mansions, subtract from three mansions; if greater than three mansions, subtract three mansions; if greater than six mansions, subtract from nine mansions; if greater than nine mansions, subtract nine mansions. Use the cotangent of the moon's ecliptic latitude at greatest eclipse as the third ratio; look up the moon's angle with the solstitial arc in the tables; add or subtract the great ecliptic-equator distance—for ecliptic longitudes from the ninth to the third mansion, add for south latitude and subtract for north (all on the south side of the equator; reverse for the north). From the third to the ninth mansion, reverse the addition and subtraction. This is the moon's angle with the equator measured from the solstitial arc. Use the cosine of the moon's angle with the solstitial arc on the ecliptic, the radius of ten million, and the tangent of the moon's ecliptic longitude from the equinox; the fourth ratio is the tangent of the moon's distance from the solstitial arc. Use the radius of ten million, the cosine of the moon's angle with the solstitial arc on the equator, and the tangent of the distance from the solstitial arc; look up the result to obtain the equatorial longitude from the equinox. Apply the three- and nine-mansion corrections: if the ecliptic longitude is less than three mansions, subtract from three mansions; if greater, add three mansions. If greater than six mansions, subtract from nine; if greater than nine mansions, add nine. This yields the moon's equatorial longitude at greatest eclipse. To find the latitude and mansion, use the same method as in the jiazi epoch system.
35
西 西 西
To find the ecliptic altitude arc angles at first and last contact: use the radius of ten million, the sine of the great ecliptic-equator distance, and the sine of the shadow's ecliptic longitude from the equinox; look up the result to obtain the shadow's equatorial distance. The shadow's distance from the equinox matches the sun's: when the sun is north of the equator the shadow is south, and when the sun is south the shadow is north. Use the cosine of the shadow's ecliptic longitude from the equinox, the cotangent of the great ecliptic-equator distance, and the radius of ten million; look up the resulting tangent to obtain the ecliptic-equator right-ascension angle. Then by spherical triangle: use the distance from the north pole to the zenith as one side and the shadow's equatorial distance plus or minus ninety degrees as the other—subtract for north, add for south. For first and last contact, if the midnight time exceeds twelve hours, subtract from twenty-four hours. Convert to equatorial degrees as the included angle and obtain the angle opposite the north-pole-to-zenith side. Each gives an equatorial altitude arc angle; add or subtract the ecliptic-equator right-ascension angle—for the moon before summer solstice in the first six mansions, subtract if the eclipse is after midnight (western limit). Add if the eclipse is before midnight; if the sum exceeds ninety degrees, subtract from a semicircle for the eastern limit. If less than ninety degrees, do not subtract from a semicircle; this becomes the western limit. After summer solstice in the last six mansions, reverse the rule. This yields the ecliptic altitude arc angle for each contact. If the eclipse is at midnight and the shadow at noon, there is no equatorial altitude arc angle; the ecliptic-equator right-ascension angle is then the ecliptic altitude arc angle. Before summer solstice the limit is west; after, east.
36
西 西
To find the combined-diameter altitude arc angles at first and last contact: use the combined diameter, the true latitude at greatest eclipse, and the radius of ten million; look up the cosine to obtain the angle between the combined diameter and the true latitude. If there is no true latitude at greatest eclipse, this angle and the combined-diameter ecliptic angle do not exist. Set ninety degrees and add or subtract the oblique-separation ecliptic nodal angle to obtain the ecliptic angles with true latitude at first and last contact. At greatest eclipse, if the moon is at the first or sixth mansion from the true node: subtract for first contact, add for last contact. At the fifth or eleventh mansion: add for first contact, subtract for last contact. Subtract each from the combined-diameter with true-latitude angle to obtain the combined-diameter ecliptic angles at first and last contact. If the initial combined-diameter with true-latitude angle is small, the north-south latitude distance matches that at greatest eclipse. If large, the reverse holds. Add or subtract the ecliptic altitude arc angle: for the eastern eclipse limit and western last-contact limit, add for south latitude and subtract for north. For the western limit at first contact and the eastern limit at last contact, reverse the addition and subtraction. Each yields the combined-diameter altitude arc angle. If there is no combined-diameter ecliptic angle, the ecliptic altitude arc angle equals the combined-diameter altitude arc angle.
37
西 西
To find the orientation at first and last contact, take the combined-diameter altitude arc angle as the fixed contact angle; the method is the same as in the jiazi epoch system. But at the initial degree of the combined-diameter altitude arc angle: first contact at the eastern limit is directly below, at the western limit directly above; At last contact, the eastern limit is directly above and the western limit directly below. Determine the orientation from the capital's polar altitude, as in the jiazi epoch method.
38
To find the magnitude of a horizon eclipse, use the two-nodal oblique separation rather than the moon-sun true motion; the remaining steps follow the jiazi epoch method.
39
To find the horizon-eclipse orientation, use the center separation at the horizon rather than deriving the various nodal angles from the combined diameter, as for fixing the orientation at first and last contact. Before greatest eclipse, use the same rules as for first contact; after greatest eclipse, the same as for last contact.
40
To find the time and orientation of the lunar eclipse for each province, the principle is the same as in the jiazi epoch method.
41
The method for drawing the lunar eclipse diagram is the same as in the jiazi epoch system.
42
Constants for solar eclipse calculation
43
Solar limb (light-semidiameter): 15″; for the remaining constants, see the sections on solar motion, lunar distance, and lunar eclipse.
44
Procedure for computing solar eclipses
45
To find the winter solstice of the civil year,
46
To find the cycle-day count,
47
To find the epoch new moon,
48
To determine whether the moon enters the eclipse zone, use the same method as for lunar eclipses, but without the half-month interval—this gives the moon's nodal longitude at each new moon. If a given month falls within the possible-eclipse zone, that month will have an eclipse. The possible-eclipse zone runs from 8°42′ in the fifth mansion to 9°14′ in the sixth, and from 20°46′ in the eleventh mansion to 21°18′ in the first.
49
To find the mean new moon,
50
To find the true time of new moon, use the same method as for finding true full moon in the lunar-eclipse section, but without adding the half-month interval. If at that instant the moon's distance from the true node falls within the eclipse limit, an eclipse occurs. At true new moon the eclipse limits run from 11°34′ in the fifth mansion to 6°22′ in the sixth, and from 23°38′ in the eleventh mansion to 18°26′ in the first.
51
To find the apparent time of true new moon, use the same method as for the apparent time of true full moon in the lunar-eclipse section. The comparison with sunrise and sunset follows the jiazi epoch method.
52
To find the apparent time of greatest eclipse, use the same method as for the time of greatest eclipse in the lunar-eclipse section.
53
To find the true anomalies of the sun and moon,
54
To find the geocentric distances of the sun and moon, use the same method as for lunar eclipses.
55
To find the horizon altitude-parallax difference, first compute the moon's maximum diurnal parallax for that day by the lunar-eclipse method. Subtract the sun's maximum diurnal parallax to obtain the horizon altitude-parallax difference.
56
To find the sun's true semidiameter, first compute its apparent semidiameter by the lunar-eclipse method. Subtract the solar limb from within to obtain the sun's true semidiameter.
57
To find the moon's apparent semidiameter, use the same method as for lunar eclipses.
58
宿 宿
To find the sun's ecliptic longitude and lodge at greatest eclipse: the longitude is found by the same method as the moon's white-path longitude in the lunar-eclipse section; the lodge position by the same method as in the solar-motion section.
59
宿
To find the moon's equatorial longitude, latitude, and lodge at greatest eclipse, use the great ecliptic-equatorial distance and the same method as for the moon's ecliptic in the lunar-eclipse section.
60
西 西 西西 西 西 西
To find the ecliptic-equatorial, ecliptic-lunar, and equatorial-lunar nodal angles: use the cosine of the sun's ecliptic longitude from the equinox at greatest eclipse, the cotangent of the great ecliptic-equatorial distance, and the radius of ten million; look up the resulting cotangent in the tables to obtain the ecliptic-equatorial nodal angle. After the winter solstice the ecliptic longitude lies west of the equatorial longitude; after the summer solstice, east. If the sun is at either solstice, this angle does not exist. The oblique-separation ecliptic nodal angle obtained above is the ecliptic-lunar nodal angle. At true new moon, if the moon is at the first or eleventh mansion from the true node, the white-path longitude lies west of the ecliptic longitude; At the fifth or sixth mansion, it lies east of the ecliptic longitude. Combine the two nodal angles by addition or subtraction to obtain the equatorial-lunar nodal angle. If both angles lie on the same side (both east or both west), add them; the white-path longitude remains on the same side of the equatorial longitude. If one is east and one west, subtract. The east-west designation follows the larger angle. If subtraction reduces the angle to zero, this angle does not exist. If there is no ecliptic-equatorial nodal angle, the ecliptic-lunar angle is the equatorial-lunar angle, with the same east-west designation.
61
To find the sun's equatorial longitude from the meridian at apparent time: subtract the greatest-eclipse apparent time from twelve hours, convert the remainder to equatorial degrees, and obtain the sun's equatorial longitude from the meridian.
62
西
To find the right-ascension altitude arc angle at apparent time, by spherical triangle: use the polar distance to the zenith as one side and the sun's distance from the north pole as the other; if the declination is south, add ninety degrees; If north, subtract from ninety degrees. Use the sun's equatorial longitude from the meridian at apparent time as the included angle; the angle opposite the polar distance to the zenith is the right-ascension altitude arc angle at apparent time. Before noon the right ascension lies east of the altitude arc; after noon, west. If the sun is at noon, this angle does not exist.
63
To find the sun's zenith distance at apparent time: use the sine of the right-ascension altitude arc angle, the sine of the polar distance to the zenith, and the sine of the sun's equatorial longitude from the meridian; look up the resulting sine in the tables to obtain the sun's zenith distance.
64
To find the altitude-parallax difference at apparent time: use the radius of ten million, the horizon altitude-parallax difference in seconds, and the sine of the sun's zenith distance; convert the result to minutes to obtain the altitude-parallax difference at apparent time.
65
西西 西西 西
To find the white-path altitude arc angle at apparent time, add or subtract the equatorial-lunar nodal angle from the right-ascension altitude arc angle. If both lie on the same side, add; the white-path longitude remains on the same side of the altitude arc. If one is east and one west, subtract; the east-west designation follows the larger angle. If either the equatorial-lunar nodal angle or the right-ascension altitude arc angle is absent, use whichever angle exists, with the same east-west designation. If both angles are absent, or subtraction reduces them to zero, this angle does not exist. The apparent time of greatest eclipse is the true time. Add the altitude-parallax difference at apparent time to the true latitude at greatest eclipse for south latitude and subtract for north; the result is the apparent center separation at greatest eclipse.
66
西
To find the angle opposite the apparent center separation at apparent time: if the moon is north of the ecliptic, use the white-path altitude arc angle at apparent time; if south of the ecliptic, use the exterior angle of the white-path altitude arc angle. For the east-west position of the true separation relative to the altitude arc: if the moon is north, it matches the white path; if south, it is reversed. In each case this is the angle opposite the apparent center separation at apparent time. If the nodal altitude arc angle exceeds ninety degrees, treat south latitude as north and north as south.
67
To find the angle opposite the true center separation at apparent time, by plane triangle: use the true center separation at greatest-eclipse apparent time as one side—that is, the true latitude at greatest eclipse. Use the altitude-parallax difference at apparent time as the other side and the angle opposite the apparent center separation as the included angle; this yields the angle opposite the true center separation at apparent time.
68
西 西
To find the apparent center separation at apparent time: use the sine of the angle opposite the true center separation, the true center separation, and the sine of the angle opposite the apparent center separation; the fourth ratio is the apparent center separation at apparent time. If the white path is west of the altitude arc and the apparent center separation exceeds the combined diameter—indicating no eclipse or not yet contact—the apparent time is the true time of first contact; if east of the altitude arc, it is past greatest eclipse or the true time of last contact. If less than the combined diameter, west of the altitude arc falls between first contact and greatest eclipse; east, between last contact and greatest eclipse.
69
西
To find the provisional time of greatest eclipse: if the white-path altitude arc angle at apparent time is east, take a time forward; if west, backward. A large angle calls for a distant time, a small angle a near one—distant not beyond nine quarters of an hour, near perhaps only a few minutes. Measure an interval of several minutes before or after the apparent time to obtain the provisional time of greatest eclipse.
70
To find the interval in minutes from provisional to apparent time: subtract the greatest-eclipse apparent time from the provisional time.
71
To find the interval arc at provisional time: use one hour in seconds, the hourly two-nodal oblique separation, and the provisional interval in seconds; the fourth ratio is the interval arc.
72
To find the angle opposite the interval arc at provisional time: use the true latitude at greatest eclipse, the interval arc, and the radius of ten million; look up the resulting tangent in the tables.
73
To find the true center separation at provisional time: use the sine of the angle opposite the interval arc, the interval arc, and the radius of ten million; the fourth ratio is the true center separation.
74
To find the sun's equatorial longitude from the meridian at provisional time,
75
To find the right-ascension altitude arc angle at provisional time,
76
To find the sun's zenith distance at provisional time,
77
To find the altitude-parallax difference at provisional time,
78
To find the white-path altitude arc angle at provisional time—the above five steps all follow the apparent-time method, but each is computed separately using provisional-time values.
79
西 西
To find the angle opposite the apparent center separation at provisional time: if the moon is north of the ecliptic, subtract the angle opposite the interval arc from the white-path altitude arc angle; if south, add them, then subtract from a semicircle; the remainder is the angle opposite the apparent center separation. When subtracting: if the angle opposite the interval arc is small, the east-west position of the true separation relative to the altitude arc matches the white path; If large, it is reversed. When adding and then subtracting a semicircle, the east-west position of the true separation is always opposite to the white path. If the two angles are equal and subtraction leaves no remainder, or their sum exactly equals 180°, there is no nodal angle and no angle opposite the true center separation at provisional time; subtract the altitude-parallax difference from the true center separation to obtain the apparent center separation. If the white-path altitude arc angle exceeds ninety degrees, treat south latitude as north and north as south.
80
To find the angle opposite the true center separation at provisional time,
81
To find the apparent center separation at provisional time, use the same method as at apparent time.
82
To find the difference in white-path altitude arc angles: subtract the apparent-time angle from the provisional-time angle.
83
To find the angle between the altitude arc at provisional time and the apparent separation at apparent time: add or subtract the white-path altitude arc angle difference from the angle opposite the true center separation at apparent time. Subtract for north latitude, add for south. If the white-path altitude arc angle exceeds ninety degrees, reverse the addition and subtraction.
84
西 西
To find the angle opposite the apparent motion at provisional time: add or subtract the provisional-time angle opposite the true center separation from the angle between the altitude arc and the apparent separation. If both true separations lie on the same side of the altitude arc (both east or both west), subtract; If one is east and one west, add; If the sum exceeds a semicircle, subtract from the full circle and use the remainder. If there is no angle opposite the true center separation at provisional time: when the altitude-parallax difference at provisional time exceeds the true center separation at provisional time, the angle between the altitude arc at provisional time and the apparent separation at apparent time is the angle opposite the apparent motion at provisional time; When the altitude-parallax difference is less than the true center separation, subtract the angle between the altitude arc and the apparent separation from a semicircle; the remainder is the angle opposite the apparent motion at provisional time.
85
To find the angle opposite the apparent separation at provisional time, by plane triangle: use the apparent center separation at apparent time as one side, the apparent center separation at provisional time as the other, and the angle opposite the apparent motion at provisional time as the included angle; this yields the angle opposite the apparent separation at provisional time.
86
To find the apparent motion at provisional time: use the sine of the angle opposite the apparent separation, the apparent center separation at provisional time, and the sine of the angle opposite the apparent motion; the fourth ratio is the apparent motion at provisional time.
87
To find the apparent motion at true time: use the radius of ten million, the cosine of the angle opposite the apparent separation at provisional time, and the apparent center separation at apparent time; the fourth ratio is the apparent motion at true time.
88
To find the apparent center separation at true time. Use the radius of ten million, the sine of the angle opposite the apparent separation at provisional time, and the apparent center separation at apparent time; the fourth ratio is the apparent center separation at true time.
89
西
To find the true time of greatest eclipse: use the apparent motion at provisional time, the provisional-time interval in minutes, and the apparent motion at true time; the fourth ratio gives the true-time interval in minutes. Add or subtract this from the apparent time of greatest eclipse—add if the white path is west of the altitude arc, subtract if east. This yields the true time of greatest eclipse.
90
To find the interval arc at true time,
91
To find the angle opposite the interval arc at true time,
92
To find the true center separation at true time—the above three steps follow the provisional-time method, but all computations use true-time degrees separately.
93
To find the sun's equatorial longitude from the meridian at true time,
94
To find the right-ascension altitude arc angle at true time,
95
To find the sun's zenith distance at true time,
96
To find the altitude-parallax difference at true time,
97
To find the white-path altitude arc angle at true time,
98
To find the angle opposite the apparent center separation at true time,
99
To find the angle opposite the true center separation at true time,
100
To find the apparent center separation at verified true time—the above eight steps follow the apparent-time method, but all computations use true-time degrees separately.
101
To find the difference in white-path altitude arc angles at true time, use the same method as at provisional time, but compute with true-time degrees separately.
102
西 西
To find the angle between the altitude arc at true time and the apparent separation at provisional time: the method matches provisional time, but the addition and subtraction differ. If the moon is north of the ecliptic and the two true separations at provisional and true time lie on the same side of the altitude arc, only the white-path positions differ. If the white-path altitude arc angle at provisional time is small, add; if large, subtract. If the white-path positions also match, reverse the addition and subtraction. If the two true separations lie on opposite sides (one east, one west), subtract in both cases. If the moon is south of the ecliptic, add when the nodal angle at provisional time is small and subtract when it is large. If there is no angle opposite the true center separation at provisional time: when the altitude-parallax difference at provisional time exceeds the true center separation at provisional time, the white-path altitude arc angle difference at true time equals the angle between the altitude arc at true time and the apparent separation at provisional time; when the altitude-parallax difference is less than the true center separation, subtract the white-path altitude arc angle difference at true time from a semicircle; the remainder is the angle between the altitude arc at true time and the apparent separation at provisional time. If the white-path altitude arc angle exceeds ninety degrees, treat south latitude as north and north as south.
103
西
To find the angle opposite the apparent motion at verified true time, use the same method as at provisional time. If at provisional time the true separation coincides with the altitude arc with no east-west distinction: subtract when the altitude-parallax difference exceeds the true center separation, add when it is smaller. If the white-path altitude arc angle difference at true time equals the angle opposite the true center separation at provisional time and subtraction leaves no remainder, the angle opposite the true center separation at true time is the angle opposite the apparent motion at verified true time. Or if the sum exactly equals a semicircle, subtract the angle opposite the true center separation at true time from a semicircle; the result is the angle opposite the apparent motion at verified true time.
104
To find the angle opposite the apparent separation at verified true time,
105
To find the apparent motion at verified true time—the above two steps follow the provisional-time method, but compute with verified-true-time degrees separately.
106
To find the apparent motion at fixed true time: if the fixed-true-time apparent motion equals the verified-true-time apparent motion, the true time of greatest eclipse is the fixed true time. If it is greater or smaller, apply the method below again.
107
To find the apparent center separation at fixed true time—the above two steps follow the true-time method, using verified-true-time degrees separately.
108
西
To find the fixed true time of greatest eclipse: use the apparent motion at verified true time as the first ratio, the difference between the provisional-time and true-time interval minutes as the second ratio, and the apparent motion at fixed true time as the third ratio; the fourth ratio gives the fixed-true-time interval in minutes. Add or subtract this from the provisional time of greatest eclipse: if the white path is east of the altitude arc, subtract when the provisional-time interval is small and add when it is large. If the white path is west of the altitude arc, reverse the addition and subtraction. This yields the fixed true time of greatest eclipse.
109
To find the eclipse magnitude: use twice the solar true semidiameter as the first ratio and ten as the second; subtract the apparent center separation at fixed true time from the combined diameter as the third ratio; the fourth ratio is the eclipse magnitude.
110
西
To find the provisional time before first or last contact: if the white path is west of the altitude arc and the apparent center separation at greatest-eclipse apparent time is close to the combined diameter, use the apparent time of greatest eclipse as the provisional time before first contact; if smaller, take a time before; if larger, take a time after—measure several minutes before or after the apparent time of greatest eclipse to obtain the provisional time before first contact. Subtract this from the fixed true time of greatest eclipse and add the remainder to the fixed true time of greatest eclipse to obtain the provisional time before last contact. If the white path is east of the altitude arc, take last contact first and then first contact—the reasoning is the same.
111
To find the interval minutes at the provisional time before first contact,
112
To find the interval arc at the provisional time before first contact,
113
西
To find the angle opposite the interval arc at the provisional time before first contact: if that provisional time precedes the apparent time of greatest eclipse, it is west; if it follows, it is east.
114
To find the true center separation at the provisional time before first contact—the above four steps follow the greatest-eclipse provisional-time method, but compute with degrees at the provisional time before first contact.
115
To find the sun's equatorial longitude from the meridian at the provisional time before first contact,
116
To find the right-ascension altitude arc angle at the provisional time before first contact,
117
To find the sun's zenith distance at the provisional time before first contact,
118
To find the altitude-parallax difference at the provisional time before first contact,
119
To find the white-path altitude arc angle at the provisional time before first contact—the above five steps follow the greatest-eclipse apparent-time method.
120
西 西
To find the angle opposite the apparent center separation at the provisional time before first contact: the method matches greatest-eclipse apparent time, but addition and subtraction differ. If the moon is north of the ecliptic and both angles lie on the same side, add; if one is east and one west, subtract. If the moon is south of the ecliptic, reverse the rule. Then subtract from a semicircle. If the white-path altitude arc angle exceeds ninety degrees, interchange south and north latitude. The remaining steps follow the greatest-eclipse provisional-time method.
121
To find the angle opposite the true center separation at the provisional time before first contact,
122
To find the apparent center separation at the provisional time before first contact—the above two steps follow the greatest-eclipse apparent-time method, but compute with degrees at the provisional time before first contact.
123
To find the provisional time after first contact: if the apparent center separation at the provisional time before first contact is less than the combined diameter, take a time before; if greater, take a time after. Observe the magnitude of the difference and measure several minutes before or after to obtain the provisional time after first contact. For each step below, follow the before-provisional-time method, but compute with degrees at the after-provisional time.
124
To find the first-contact apparent-separation difference: subtract the apparent center separations at the before- and after-provisional times.
125
To find the first-contact provisional-time difference: subtract the interval minutes at the before- and after-provisional times.
126
To find the first-contact apparent-separation combined-diameter difference: subtract the combined diameter from the apparent center separation at the provisional time after first contact.
127
To find the fixed true time of first contact: use the apparent-separation difference, the provisional-time difference, and the apparent-separation combined-diameter difference as ratios; the fourth ratio gives the true-time interval minutes for first contact. Add or subtract this from the provisional time after first contact: add if the apparent center separation at the after-provisional time exceeds the combined diameter, subtract if it is smaller. This yields the true time of first contact. Then, at the true time of first contact, compute the apparent center separation by the previous method; if it equals the combined diameter, the true time of first contact is the fixed true time of first contact. The angle opposite the true center separation at the true time of first contact is the orientation angle at first contact. If it is too large or too small, compare whichever of the before- and after-provisional-time apparent center separations is nearest the combined diameter with the apparent center separation at verified true time, and by proportion obtain the fixed true time of first contact.
128
To find all quantities at the provisional time before last contact, use the first-contact method, but compute with degrees at the provisional time before last contact.
129
To find the provisional time after last contact: if the apparent center separation at the provisional time before last contact is less than the combined diameter, take a time after; if greater than the combined diameter, take a time before. Observe the magnitude of the difference and measure several minutes before or after to obtain the provisional time after last contact. Compute each step in sequence by the before-provisional-time method, but use degrees at the after-provisional time.
130
To find the last-contact apparent-separation difference,
131
To find the last-contact provisional-time difference,
132
To find the last-contact apparent-separation combined-diameter difference,
133
To find the fixed true time of last contact—the above four steps all follow the first-contact method, but compute with last-contact degrees separately.
134
To find the total duration of the eclipse: subtract the fixed true time of last contact from the fixed true time of first contact.
135
西
To find the fixed contact angles at first and last contact: if the white path at first contact is east of the altitude arc, subtract the orientation angle at first contact from a semicircle; if west, use the orientation angle at first contact directly; for last contact, reverse the rule. Each result is a fixed contact angle.
136
西 西
To find the orientation at first and last contact, use the jiazi epoch method, but at the initial degree of the fixed contact angle: if the white path at first contact is east of the altitude arc, the orientation is directly above; if west, directly below; at last contact, east is directly below and west is directly above.
137
To find the sunrise and sunset times for a horizon eclipse, use the same method as in the jiazi epoch system.
138
To find the interval time to the horizon: subtract the sunrise or sunset time from the apparent time of greatest eclipse.
139
To find the horizon interval arc, use the greatest-eclipse provisional-time method, but compute from the horizon interval time.
140
To find the right-ascension altitude arc angle at the horizon: use the cosine of the ecliptic-equatorial latitude distance, the sine of the polar altitude, and the radius of ten million; look up the resulting cosine in the tables to obtain the right-ascension altitude arc angle at the horizon.
141
To find the white-path altitude arc angle at the horizon, use the greatest-eclipse apparent-time method, but compute with horizon-eclipse degrees separately.
142
To find the angle opposite the interval arc at the horizon,
143
To find the true center separation at the horizon,
144
To find the angle opposite the apparent center separation at the horizon—the above three steps follow the greatest-eclipse provisional-time method, but compute with horizon-eclipse degrees separately.
145
To find the angle opposite the true center separation at the horizon, use the horizon altitude-parallax difference; the remaining steps follow the greatest-eclipse apparent-time method.
146
To find the apparent center separation at the horizon, use the greatest-eclipse apparent-time method, but compute with horizon-eclipse degrees separately.
147
To find the magnitude of the horizon eclipse, use the same method as for eclipse magnitude, computing from the separation at the horizon.
148
To find the orientation of a horizon eclipse: if the event occurs before greatest eclipse, use the first-contact method; if after greatest eclipse, use the last-contact method.
149
To find the time and orientation of the solar eclipse for each province, the principle is the same as in the jiazi epoch method.
150
To draw the solar eclipse diagram, use the jiazi epoch method.
151
輿 西 輿
To draw the terrestrial map of a solar eclipse, take the magnitude of greatest visibility and make each unit of magnitude one tier. This extends to twenty-one tiers. Also take the time of visibility, early or late, with each quarter-hour as one tier. This extends to ninety-six tiers. Cross the two scales and work backward to obtain the polar altitude and east-west deviation for each place of visibility. Then join the results by degree into a single map. Then, using the full terrestrial map, enter each place-name at its corresponding altitude and deviation.
152
Constants for close approach: see the sections on lunar distance and the motions of the five planets and fixed stars.
153
The procedure for close approach is the same as the jiazi epoch method for occultation and conjunction.
154
Tables for computational astronomy
155
Besides the present method, both the jiazi and guimao epoch systems include table-based procedures; their main features are summarized here.
156
Jiazi epoch method:
157
宿
First, epoch root tables: keyed by year count, day count, and lodge assignment, extend forward three hundred years from the epoch origin; for each year obtain the sun's mean motion and perigee mean motion at midnight after the civil winter solstice, and tabulate these as the solar epoch root table; the moon's mean motion together with apogee and true-node mean motions, tabulated as the lunar epoch root table; and the five planets' mean motions together with apogee, true node, and visibility values, each as a planetary epoch root table.
158
Second, tropical-year mean-motion tables: keyed by day count from 1 to 366, accumulate the mean motions of the sun, moon, five planets, and their perigee, apogee, true node, and visibility values, each tabulated separately.
159
Third, diurnal mean-motion tables: keyed by hours, minutes, and seconds and paired in three tiers with degrees, minutes, and seconds from 1 to 60, accumulate the mean motions of the sun, moon, five planets, apogee, true node, visibility, moon-sun distance, lunar anomaly, and nodal cycle, each tabulated separately.
160
Fourth, equation tables: keyed by anomaly, pre-compute the fast-slow variation for each degree and minute and tabulate the results. The moon has separate second- and third-equation tables keyed by anomaly and moon-sun distance, arranged in crosswise pairs. For Saturn, Jupiter, Venus, and Mercury, the first equation and middle term together with the second equation and correction term are combined in one table. For Mars, the first equation together with the epicycle-center geocentric distance, epicycle radius, and solar distance variation are combined in one table. These are all equation tables.
161
Fifth, latitude-distance tables: keyed by ecliptic mansion degree, list the corresponding north-south equatorial latitude distance as the ecliptic-equator latitude-distance table. Keyed by the moon's distance from the true node and divided into six tiers of great ecliptic-lunar distance, list the corresponding north-south ecliptic latitude distance as the ecliptic-lunar latitude-distance table.
162
Sixth, right-ascension tables: keyed by ecliptic mansion degree, list the corresponding equatorial degree as the ecliptic-equator right-ascension table.
163
Seventh, ecliptic right-ascension angle table: keyed by ecliptic mansion degree, list the corresponding ecliptic right-ascension angle.
164
Eighth, right-ascension difference tables: keyed by the moon's and five planets' distance from the node in mansion degrees, list the corresponding ecliptic degree correction for each body.
165
Ninth, time-equation tables: keyed by ecliptic degree, convert the corresponding equatorial degree difference to time and tabulate it as the right-ascension time-equation table. Also keyed by anomaly, convert the corresponding equation to time and tabulate it as the equation time-equation table.
166
Tenth, diurnal-parallax tables: keyed by true altitude, list the corresponding diurnal parallax for the sun, moon, Mars, Venus, and Mercury.
167
Eleventh, refraction tables: keyed by true altitude, list the corresponding atmospheric refraction.
168
Twelfth, true-motion tables: keyed by anomaly, list the corresponding true motions of the sun, moon, and moon-sun distance.
169
Thirteenth, nodal-equation and limit-distance table: keyed by moon-sun distance, list the corresponding nodal equation and limit distance together.
170
宿
Fourteenth, first-new-moon root tables: keyed by year count, day count, and lodge assignment, extend forward three hundred years from the epoch origin; for each year list the first new moon's date and time, solar mean motion, solar and lunar anomaly, and lunar nodal cycle in one table.
171
Fifteenth, new- and full-moon tabulation tables: keyed by month count from 1 to 13, list the new- and full-moon tabulations together with solar mean motion, solar and lunar anomaly, and lunar nodal cycle at new and full moon—ten items in one table.
172
Sixteenth, apparent-semidiameter tables: keyed by anomaly, list the solar semidiameter, lunar semidiameter, lunar distance from the earth-shadow semidiameter, and shadow correction together.
173
Seventeenth, eclipse lunar-motion tables: keyed by latitude distance at greatest eclipse from 1 to 64 minutes and crosswise paired with the sum of the two semidiameters of the sun, moon, and earth shadow from 25 to 64 minutes, list the corresponding lunar motion in minutes and seconds. The difference and sum of the lunar and earth-shadow semidiameters are used interchangeably.
174
Eighteenth, ecliptic horizon-quadrant tables: keyed by the ecliptic mansion degree at noon and polar altitude from 16° to 46° in thirty-one tiers, list the vernal-equinox meridian distance, ecliptic horizon quadrant, and limit geocentric altitude together.
175
Nineteenth, ecliptic altitude-arc angle table: keyed by solar limit distance from 0° to 90° and limit geocentric altitude from 20° to 89° in seventy tiers, list the corresponding ecliptic altitude-arc angle.
176
Twentieth, solar altitude-arc table: arranged by the same method as the ecliptic altitude-arc angle table.
177
西西
Twenty-first, east-west and north-south difference tables: keyed by nodal angle from 0° to 90° and crosswise paired with altitude-parallax difference from 1 to 63 minutes, list the corresponding east-west and north-south differences.
178
Twenty-second, latitude-difference angle tables: keyed by combined diameter from 31 to 64 minutes and crosswise paired with latitude distance from 1 to 64 minutes, list the corresponding latitude-difference angle.
179
Twenty-third, star ecliptic-distance tables: keyed by distance from the node in mansion degrees, list each star's ecliptic distance; for Mercury alone, divide the nodal angle from 4°55′32″ to 6°31′2″ into twenty tiers.
180
Twenty-fourth, star geocentric-distance tables: keyed by the star's distance from the sun in mansion degrees, list the corresponding geocentric distance.
181
Twenty-fifth, Mercury limit-distance table: keyed by distance from the node in mansion degrees, list the corresponding limit distance.
182
Twenty-sixth, five-planet heliacal visibility solar ecliptic-degree tables: keyed by the planetary ecliptic-longitude tables and divided into morning and evening, upper and lower positions, list each planet's corresponding solar ecliptic distance.
183
Twenty-seventh, five-planet heliacal visibility solar correction tables: arranged like the ecliptic-degree tables, but without separating the five planets and instead dividing ecliptic latitude from 1° to 8° north and south.
184
Additions in the guimao epoch method:
185
First, solar geocentric-distance table: keyed by true solar anomaly, list the corresponding true geocentric distance and its logarithm.
186
Second, lunar first mean-motion table: keyed by solar anomaly, list the corresponding first lunar mean motion together with apogee and true-node mean motions.
187
Third, lunar second mean-motion table: keyed by the sun's distance from the lunar apogee in mansion degrees, list the second mean motion when the sun is at apogee together with the distance variation in seconds.
188
Fourth, lunar third mean-motion table: keyed by the moon's distance from the true node in mansion degrees, list the corresponding third mean motion.
189
Fifth, lunar apogee equation and deferent-center geocentric-distance table: keyed by the sun's distance from the lunar celestial apogee in mansion degrees, list the apogee equation and deferent-center geocentric distance.
190
Sixth, lunar second-equation table: keyed by the moon's distance from the sun in mansion degrees, list the second equation when the sun is at apogee together with the distance variation.
191
Seventh, lunar third-equation table: keyed by the total conjunction number, list the corresponding third equation.
192
Eighth, lunar final-equation table: keyed by true moon-sun distance in mansion degrees and crosswise paired with sun-moon apogee separation, list the corresponding final equation.
193
Ninth, lunar true-node true-equation table: keyed by the sun's distance from the true node in mansion degrees, list the corresponding true-node equation.
194
Tenth, nodal-angle addition table: keyed by the sun's distance from the true node in mansion degrees, list the corresponding nodal addition and correction.
195
Eleventh, ecliptic-lunar latitude-distance table: arranged by the same method as the right-ascension difference table.
196
Twelfth, lunar geocentric-distance table: keyed by true lunar anomaly, list the geocentric distance and double minutes for the maximum and minimum two-center differences. Tables that share a name but differ in content: the lunar first-equation table is divided into large, middle, and small tiers; the ecliptic- and lunar right-ascension difference tables list the minimum nodal angle and large and small comparison seconds; the lunar diurnal-parallax and true-motion tables are each divided into large and small tiers.
197
To find the sun's and moon's geocentric distance, by plane triangle: take the solar double eccentricity as the side opposite the right angle and the true solar anomaly as the other angle; within three mansions use the degree as given, beyond three mansions subtract six mansions, beyond nine mansions subtract the full circle, and use the remainder. The side opposite the true solar anomaly is the base leg. The side opposite the originally unknown angle is the fractional leg; add or subtract it from 20,000,000—add when true anomaly is within three mansions or beyond nine mansions, subtract between three and nine mansions. With the sum of the leg and hypotenuse and the base leg, find the leg. Add or subtract the fractional leg—subtract when true anomaly is within three mansions or beyond nine mansions, add between three and nine mansions. This yields the sun's geocentric distance. Apply the same method using the moon's double eccentricity at true full moon to obtain the moon's geocentric distance.
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