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卷49 志二十四 时宪五

Volume 49 Treatises 24: Calendar 5

Chapter 49 of 清史稿 · Draft History of Qing
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Chapter 49
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1
Treatise 24
2
Shixian Calendar 5
3
Kangxi jiazi calendrical system — lower section
4
Constants for lunar eclipse calculation
5
New-moon interval constant: 29.530593 days.
6
Full-moon interval constant: 14.7652965 days.
7
Sun's mean motion per synodic month: 104,784 seconds, fractional remainder 0.304324.
8
Sun's equation per synodic month: 104,779 seconds, fractional remainder 0.358865.
9
Moon's anomaly per synodic month: 92,940 seconds, fractional remainder 0.24859.
10
Moon's nodal motion per synodic month: 110,414 seconds, fractional remainder 0.016574.
11
Sun's mean motion per half-month: 14°33′12.09″.
12
Sun's equation per half-month: 14°33′09.41″.
13
Moon's anomaly per half-month: 6 mansions 12°54′30.07″.
14
Moon's nodal motion per half-month: 6 mansions 15°20′07″.
15
Sun's hourly mean motion: 147 seconds, fractional remainder 0.8471049.
16
Sun's hourly equation: 147 seconds, fractional remainder 0.840127.
17
Moon's hourly anomaly: 1,959 seconds, fractional remainder 0.7476542.
18
Moon's hourly nodal motion: 1,984 seconds, fractional remainder 0.402549.
19
Moon's hourly mean elongation from the sun: 1,828 seconds, fractional remainder 0.6121108.
20
Solar semidiameter (light-seconds): 637.
21
Lunar true semidiameter: 27.
22
Terrestrial semidiameter: 100.
23
Solar apogee distance: 10,179,208 units; ratio to Earth's semidiameter: 116,200.
24
Lunar apogee distance: 10,172,500 units; ratio to Earth's semidiameter: 5,816.
25
Epoch new-moon offset: 26.3852666 days.
26
At the epoch new moon, the sun's mean longitude should be 26°20′42.57″ in the first mansion.
27
At the epoch new moon, the sun's equation should be 19°10′27.21″ in the first mansion.
28
At the epoch new moon, the moon's anomaly should be 18°34′26.16″ in the ninth mansion.
29
At the epoch new moon, the moon's nodal longitude should be 0°30′55.14″ in the sixth mansion; other constants appear in the sections on solar motion and lunar distance.
30
Procedure for computing lunar eclipses
31
To find the winter solstice of the civil year, use the same method as in the section on solar motion.
32
To find the cycle-day count, add one day to the winter-solstice day-number of the civil year.
33
To find the epoch new moon, first compute the accumulated days by the same method as in the lunar-distance section. Subtract the new-moon epoch offset from the accumulated days to obtain the general new-moon interval. When projecting backward into antiquity, add instead of subtract. Divide by the new-moon interval constant; add one to the quotient to obtain the count of accumulated new moons. Subtract the remainder from the new-moon interval constant to obtain the epoch new-moon fraction. For backward projection, the quotient itself is the accumulated new-moon count; do not add one. The remainder itself is the epoch new-moon fraction; no reverse subtraction is needed.
34
滿
To determine whether the moon enters the eclipse zone: multiply the accumulated new-moon count by the nodal motion per synodic month, cast out full circuits of the celestial seconds, and the remainder is the nodal longitude at accumulated new moon. Add the epoch nodal longitude at new moon to obtain the nodal longitude at the first new moon. For backward projection, subtract the accumulated nodal longitude from the epoch nodal offset instead. Add the nodal motion per half-month, then add the nodal motion per synodic month thirteen times in succession to obtain the mean nodal longitude at each month's full moon. If a given month's nodal longitude falls within the possible-eclipse zone, that month may witness a lunar eclipse. The possible-eclipse zone runs from 15°06′ in the fifth mansion to 14°54′ in the sixth, and from 15°06′ in the eleventh mansion to 14°54′ in the first. Refine the result using the true nodal longitude.
35
滿
To find the mean full moon: multiply the eclipse-month index by the new-moon interval, add the half-month interval, then add the epoch new-moon day-fraction and cycle-day count; cast out full cycle periods, and the remainder is the mean full-moon day-fraction. Count the sexagenary day from the epoch jiazi day to obtain the mean full-moon day stem-branch; convert the fractional remainder through sub-quarter parts and reduce by the standard rule. Starting from exact zi as the initial hour, obtain the hour, quarter, minute, and second.
36
滿
To find the sun's mean longitude: take the accumulated new-moon count, add the eclipse-month index to obtain the general month-count, and multiply by the sun's mean motion per synodic month. Cast out full circuits of celestial seconds, add the epoch sun mean longitude at new moon; for backward projection, subtract instead. Add the sun's mean motion per half-month to obtain the result.
37
To find the sun's mean equation: multiply the general month-count by the sun's equation per synodic month, cast out full circuits, and add the epoch sun equation; for backward projection, subtract. Add the sun's equation per half-month to obtain the result.
38
To find the moon's mean anomaly: multiply the general month-count by the moon's anomaly per synodic month, cast out full circuits, and add the epoch moon anomaly; for backward projection, subtract. Add the moon's anomaly per half-month to obtain the result.
39
To find the moon's true anomaly: use one hour converted to seconds as the first ratio, the moon's hourly anomaly as the second, and the interval time in seconds as the third; the fourth ratio gives the correction in seconds. Convert to degrees and minutes to obtain the moon's anomaly arc. Apply addition or subtraction according to the sign of the interval time. Add or subtract this from the moon's mean anomaly to obtain the true anomaly.
40
滿退
To find the true full moon: from the sun's true anomaly compute the equation of center as the sun's true equation, and also obtain the sun's geocentric distance. This is the side opposite the right angle in the second plane triangle of the true equation. From the moon's true anomaly compute the equation of center as the moon's true equation, and also obtain the moon's geocentric distance. The method is the same as for the sun. Add or subtract the two equations to obtain the true elongation arc. The sign of addition or subtraction follows that of the elongation arc. By the previous method for interval time, convert to hours and minutes as the true interval time, and add or subtract from the mean full moon with the same sign. This yields the true full moon. If the addition reaches twenty-four hours, the true full moon advances one day; if subtraction is insufficient, borrow one day as twenty-four hours, and the true full moon retreats one day.
41
To find the true nodal longitude: use one hour in seconds, the moon's hourly nodal motion, and the true interval time in seconds; convert the result to degrees and minutes as the nodal interval arc. Add or subtract from the moon's nodal longitude according to the sign of the true interval time. Further add or subtract the moon's true equation to obtain the true nodal longitude. If the true nodal longitude falls within the certain-eclipse zone, an eclipse will occur. The certain-eclipse zone runs from 17°43′05″ in the fifth mansion to 12°16′55″ in the sixth, and from 17°43′05″ in the eleventh mansion to 12°16′55″ in the first. If the longitude does not fall within this zone, no further calculation is required.
42
To find the sun's true ecliptic and equatorial longitude: use one hour in seconds, the sun's hourly mean motion, and the true interval time; convert to degrees and minutes as the solar interval arc. Apply addition or subtraction according to the sign of the interval time. Add or subtract from the sun's mean longitude and further apply the sun's true equation to obtain the ecliptic longitude. Use a spherical triangle to obtain the equatorial longitude as well. See the section on lunar distance for the method of finding the moon's rising and setting times.
43
To find the apparent time of true full moon: convert the sun's true equation to time as the equation time correction; the rising-degree correction is the difference between ecliptic and equatorial longitudes. Convert the rising-degree difference to time; combine the two time corrections; for the rules of addition and subtraction, see the section on lunar distance concerning apparent time and mean motion. Apply these corrections to the true full moon to obtain the apparent time of true full moon. An eclipse can be observed if it falls within nine quarters of an hour after sunrise or before sunset. If it lies beyond nine quarters, the event falls entirely in daylight and need not be calculated.
44
To find the time of greatest eclipse: use the celestial radius as the first ratio, the cosine of the great ecliptic-lunar distance as the second, and the tangent of the true nodal longitude as the third; look up the resulting tangent in the tables to obtain the nodal longitude at greatest eclipse. Subtract this from the true nodal longitude to obtain the nodal rising-degree difference. Add the moon's hourly anomaly to its true anomaly and compute by the first-equation method in the lunar-distance section to obtain the second equation. Combine the second equation with the moon's true equation: subtract if they share the same sign, add if opposite. Combine this result with the hourly mean moon-sun elongation: if both equations call for addition, add the larger second equation and subtract the smaller; if both call for subtraction, subtract the larger and add the smaller. If both equations call for subtraction, subtract the larger second equation and add the smaller. If one equation calls for addition and the other for subtraction, follow the sign of the second equation. This yields the moon's true elongation from the sun. Use the true moon-sun elongation in seconds as the first ratio, one hour in seconds as the second, and the nodal rising-degree difference in seconds as the third; the fourth ratio gives the correction in seconds. Convert to hours and minutes to obtain the interval time to greatest eclipse. Apply this to the apparent time of true full moon: subtract if the true nodal longitude is in the first or sixth mansion, add if in the fifth or eleventh. This yields the time of greatest eclipse.
45
To find the latitude distance at greatest eclipse: use the celestial radius, the sine of the great ecliptic-lunar distance, and the sine of the true nodal longitude; look up the resulting sine in the tables. If the true nodal longitude is in the first or fifth mansion, the latitude is north; if in the sixth or eleventh, south.
46
To find the lunar semidiameter: use the lunar apogee distance as the first ratio, the Earth-semidiameter ratio as the second, and the moon's geocentric distance minus the deferent epicycle radius as the third; the fourth ratio gives the moon's distance from Earth. Further use the moon's distance from Earth as the first ratio, its true semidiameter as the second, and the celestial radius as the third; the fourth ratio is a sine. Look up the result in the tables to obtain the lunar semidiameter.
47
To find the Earth's shadow semidiameter: use the solar apogee distance, the Earth-semidiameter ratio, and the sun's geocentric distance; the fourth ratio gives the sun's distance from Earth. Use the solar light-semidiameter minus the Earth's semidiameter as the first ratio, the sun's distance as the second, and the Earth's semidiameter as the third; the fourth ratio gives the length of the Earth's shadow. Use the shadow length, Earth's semidiameter, and celestial radius; look up the resulting sine in the tables to obtain the Earth-shadow angle. Use the celestial radius, the tangent of the shadow angle, and the shadow length minus the moon's distance; the fourth ratio gives the width of shadow entered by the moon. Use the moon's distance, the shadow width, and the celestial radius; look up the resulting tangent to obtain the Earth's shadow semidiameter.
48
To find the eclipse magnitude: use the moon's full diameter as the first ratio and ten as the second; the third ratio is the sum of the lunar and Earth-shadow semidiameters. Subtract the latitude distance at greatest eclipse; if the combined diameter cannot cover the latitude separation, no eclipse occurs. This serves as the third ratio; the fourth ratio is the eclipse magnitude.
49
To find the times of first and last contact: use the cosine of the latitude at greatest eclipse, the cosine of the combined diameter, and the radius of ten million; look up the arc intervals in the tables. Use the true moon-sun elongation in seconds, one hour in seconds, and the contact interval arcs in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes to obtain the interval times to first and last contact. Apply these to the time of greatest eclipse to obtain the times of first and last contact. Subtract for first contact; add for last contact.
50
To find the times when totality begins and light returns: use the cosine of the latitude at greatest eclipse, the cosine of the difference of the two semidiameters, and the radius of ten million; look up the arc intervals in the tables. Use the true moon-sun elongation in seconds, one hour in seconds, and the totality interval arcs in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes to obtain the interval times to totality and light return. Apply these to the time of greatest eclipse to obtain the times of totality and light return. Subtract for the beginning of totality; add for the return of light.
51
To find the total duration of the eclipse, double the interval time from greatest eclipse to first or last contact.
52
To find the moon's ecliptic longitude and latitude: take the sun's ecliptic longitude and add or subtract six mansions; if the result exceeds six mansions, subtract six; if insufficient, add six. Further add or subtract the interval arc at greatest eclipse and the ecliptic-lunar rising-degree difference; for the method of finding the rising-degree difference, see the lunar-distance section on true ecliptic motion. This yields the moon's ecliptic longitude. To find the latitude, see the section on lunar distance.
53
To find the moon's equatorial longitude and latitude, see the section on lunar distance concerning rising and setting times.
54
宿
To find the lodge position, use the same method as in the section on solar motion.
55
滿 西 西 西西 西 西 西 西 西 西
To find the ecliptic-horizon angle: convert the time of greatest eclipse to equatorial degrees, with each quarter-hour equal to one degree. Subtract three mansions from the sun's equatorial longitude; if insufficient, add twelve mansions before subtracting. The remainder is the sun's equatorial longitude measured from the spring equinox. Add the two values and cast out full circuits. This gives the spring equinox's equatorial longitude from exact zi. Subtract from a semicircle to obtain the spring equinox's east-west equatorial distance from noon. If it exceeds a semicircle, subtract the semicircle to place it west of noon. If it falls short of a semicircle, subtract it from the semicircle to place it east of noon. If the spring equinox's east-west distance from noon exceeds a quadrant, subtract from a semicircle; the remainder is the autumn equinox's east-west equatorial distance from noon. The autumn equinox's east-west relation to noon is the reverse of the spring equinox. Subtract the equinox's east-west distance from noon from ninety degrees; the remainder is the equinox's equatorial distance from the horizon. Use this as one side of a spherical triangle, with the obliquity of the ecliptic and the equator-horizon angle (the equatorial altitude); apply when the spring equinox lies west of noon or the autumn equinox east of noon. If the spring equinox lies east of noon or the autumn equinox west of noon, subtract this value from a semicircle and use the remainder. With these as the two adjacent angles, solve for the opposite angle to obtain the ecliptic-horizon angle. When the spring equinox is east of noon or the autumn equinox west of noon, the result is the ecliptic-horizon angle directly. When the spring equinox is west of noon or the autumn equinox east of noon, subtract the result from a semicircle; the remainder is the ecliptic-horizon angle.
56
西 西 西西
To find the ecliptic altitude arc angle: use the sines of the ecliptic-horizon angle, the equator-horizon angle, and the equinox's equatorial distance from the horizon; look up the result to obtain the equinox's ecliptic distance from the horizon. When the equinox is on the horizon, subtract the moon's ecliptic longitude from the third or ninth mansion: subtract the third mansion at spring equinox and the ninth at autumn equinox. The remainder is the moon's ecliptic longitude measured from the equinox. If the equinox mansion longitude exceeds the moon's mansion longitude, the moon lies before the equinox; otherwise it lies after. Combine the equinox's ecliptic distance from the horizon with the moon's distance from the equinox to obtain the moon's ecliptic distance from the horizon; when the equinox is west of noon, add if the moon is after the equinox and subtract if before; when the equinox is east of noon, reverse the rule. Adjust according to whether the eclipse limit lies to the east or west. When the equinox is west of noon, if the moon's ecliptic distance from the horizon is less than ninety degrees the limit is west; if greater, east; when the equinox is east of noon, reverse the rule. Use the cosine of the moon's ecliptic distance from the horizon, the celestial radius, and the cotangent of the ecliptic-horizon angle; look up the resulting tangent to obtain the ecliptic altitude arc angle.
57
西
To find the fixed contact angles: take the nodal longitude at greatest eclipse and add or subtract the contact interval arcs to obtain the nodal longitudes at first and last contact. Subtract for first contact; add for last contact. Use the celestial radius, the sine of the great ecliptic-lunar distance, and the sine of the nodal longitude at first contact; look up the result to obtain the latitude distance at first contact. Use the sine of the nodal longitude at last contact as the third ratio, with the first and second unchanged. Look up the resulting sine to obtain the latitude distance at last contact. If the nodal longitude is in the first or fifth mansion, latitude is north; if in the sixth or eleventh, south. Use the sine of the combined diameter and the sines of the latitude distances at first and last contact, with the radius of ten million; look up the two latitude-difference angles. Combine each latitude-difference angle with the ecliptic altitude arc angle to obtain the fixed contact angles. At first contact in the eastern limit: add for south latitude, subtract for north; in the western limit: subtract for south latitude, add for north. For last contact, reverse the rule. If there is no latitude-difference angle at contact, use the ecliptic altitude arc angle directly as the fixed contact angle.
58
西
To find the orientation at first and last contact: when the eclipse is in the eastern limit and the fixed angle is within forty-five degrees, first contact lies lower-left and last contact upper-right. Beyond forty-five degrees, first contact is to the lower left and last contact to the upper right. At exactly ninety degrees, first contact is directly to the left and last contact directly to the right. Past ninety degrees, first contact is to the upper left and last contact to the lower right. When the eclipse is in the western limit and the fixed angle is within forty-five degrees, first contact lies upper-left and last contact lower-right. Beyond forty-five degrees, first contact is to the upper left and last contact to the lower right. At exactly ninety degrees, first contact is directly to the left and last contact directly to the right. Past ninety degrees, first contact is to the lower left and last contact to the upper right. At the capital, the ecliptic-horizon quadrant always lies south of the zenith; determine orientation accordingly. If the quadrant lies north of the zenith, reverse the orientation.
59
To find the magnitude of a horizon eclipse: if first contact or greatest eclipse occurs before sunset, it is an eclipse emerging from the horizon—use the sunset time. If greatest eclipse or last contact occurs after sunrise, it is an eclipse setting below the horizon—use the sunrise time. Subtract from the time of greatest eclipse; the remainder is the interval time to the horizon. Use one hour in seconds, the hourly true moon-sun elongation in seconds, and the horizon interval time in seconds; the fourth ratio gives the correction in seconds. Convert to degrees and minutes to obtain the horizon interval arc. Use the radius of ten million, the cotangent of the horizon interval arc, and the cosine of the latitude at greatest eclipse; look up the arc between the two centers at the horizon. Use the moon's full diameter and ten as ratios; subtract the center separation from the combined diameter as the third ratio; the fourth ratio is the horizon eclipse magnitude.
60
西 西
To find lunar eclipse times for each province: convert by the province's longitudinal offset from the capital, with each degree equal to one quarter-hour. Add or subtract this from the capital's eclipse time to obtain the provincial time. Add for provinces to the east; subtract for those to the west.
61
To find the eclipse orientation for each province: use the provincial equatorial altitude and eclipse time, applying the same orientation method as for the capital.
62
To draw the lunar eclipse diagram: first draw horizontal and vertical lines at right angles—the horizontal for the ecliptic, the vertical for the ecliptic meridian—and at the center draw a circle with the Earth's shadow semidiameter to represent the umbra. Next draw an outer circle with the combined diameter as the limit for first and last contact. Draw an inner circle with the difference of the two semidiameters as the limit for totality and the return of light. On the outer circle along the vertical line, mark five degrees to the left or right: if the true nodal longitude is in the first or eleventh mansion, mark on the right; if in the fifth or sixth, on the left. Draw a line from the mark through the center to the lower edge of the outer circle; this is the lunar-path meridian. Along this line from the center, mark the latitude distance at greatest eclipse to locate the moon's center at greatest eclipse. From this point draw a horizontal cross-line representing the lunar path. The points where the lunar path cuts the inner and outer circles mark the moon's center at the four contact phases before and after greatest eclipse. Finally draw small circles at each of the five moon-center positions using the lunar semidiameter; the five phases of the eclipse are now complete.
63
Constants for solar eclipse calculation
64
Solar true semidiameter: 507; for the remaining constants and methods, see the lunar-eclipse section on computing solar eclipses.
65
To find the winter solstice of the civil year, use the same method as in the section on solar motion.
66
To find the cycle-day count, use the same method as for lunar eclipses.
67
To find the epoch new moon, use the same method as for lunar eclipses.
68
To determine whether the moon enters the eclipse zone, use the same method as for finding each month's mean nodal longitude at full moon in the lunar-eclipse section, but without the half-month interval—this gives the mean nodal longitude at each new moon. If a given month's nodal longitude falls within the possible-eclipse zone, that month may witness a solar eclipse. The possible-eclipse zone runs from 9°08′ in the fifth mansion to 8°51′ in the sixth, and from 21°09′ in the eleventh mansion to 20°52′ in the first.
69
To find the mean new moon,
70
To find the sun's mean longitude,
71
To find the sun's mean equation,
72
To find the moon's mean anomaly—the above four steps all follow the lunar-eclipse method for mean full moon, but without adding the half-month interval.
73
To find the sun's true anomaly, use the same method as for lunar eclipses.
74
To find the moon's true anomaly, use the same method as for lunar eclipses.
75
To find the true new moon, use the same method as for finding the true full moon in the lunar-eclipse section.
76
To find the true nodal longitude, use the same method as for lunar eclipses. If the true nodal longitude falls within the eclipse zone, an eclipse will occur. The possible-eclipse zone at true new moon runs from 11°45′ in the fifth mansion to 6°14′ in the sixth, and from 23°46′ in the eleventh mansion to 18°15′ in the first.
77
To find the sun's true ecliptic and equatorial longitude, use the same method as for lunar eclipses.
78
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 apparent time of true new moon must fall before sunrise or after sunset. If it lies more than five quarters of an hour from sunrise or sunset, the event falls at night and need not be calculated.
79
To find the apparent time of greatest eclipse, use the same method as in the lunar-eclipse section.
80
滿 西 西
To find the equinox's east-west equatorial distance from noon at apparent time: subtract three mansions from the sun's equatorial longitude; if insufficient, add twelve mansions before subtracting. This gives the sun's equatorial longitude measured from the spring equinox. Convert the apparent time of greatest eclipse to equatorial degrees and add or subtract a semicircle; if it exceeds a semicircle, subtract one; if insufficient, add one. This gives the sun's equatorial longitude measured from noon. Add the two values and cast out full circuits. If the result does not exceed a quadrant, it is the spring equinox's equatorial distance west of noon. If past one quadrant, subtract from a semicircle; the remainder is the autumn equinox's equatorial distance east of noon. If past two quadrants, subtract two quadrants; the remainder is the autumn equinox's equatorial distance west of noon. If past three quadrants, subtract from the full circuit; the remainder is the spring equinox's equatorial distance east of noon.
81
To find the equinox's ecliptic distance from noon at apparent time: use the cosine of the obliquity, the celestial radius, and the tangent of the equatorial distance; look up the result in the tables.
82
To find the ecliptic-equator latitude separation at noon for apparent time: use the celestial radius, the sine of the obliquity, and the sine of the ecliptic distance from noon; look up the result in the tables.
83
To find the angle between the ecliptic and the meridian at apparent time: use the sines of the ecliptic and equatorial distances from noon and the celestial radius; look up the result in the tables.
84
西 西
To find the ecliptic mansion at noon for apparent time: take the equinox's ecliptic distance from noon and, at spring equinox, add or subtract three mansions. If west of noon, add three mansions; if east of noon, subtract from three mansions. At autumn equinox, add or subtract nine mansions; if west of noon, add nine; if east of noon, subtract from nine. This yields the ecliptic mansion at noon for apparent time.
85
To find the ecliptic altitude at noon for apparent time: set the equatorial altitude to the north polar altitude minus a quadrant. Add or subtract the noon ecliptic-equator latitude separation: add for mansions three through eight, subtract for nine through two. This yields the result.
86
To find the ecliptic-horizon quadrant's distance from noon at apparent time: use the cosine of the ecliptic-meridian angle, the celestial radius, and the tangent of the noon ecliptic altitude; look up the degrees and minutes in the tables. Subtract from ninety degrees; the remainder is the quadrant's distance from noon.
87
To find the quadrant mansion at apparent time: combine the quadrant distance from noon with the noon ecliptic mansion—add for mansions one through five, subtract for six through eleven; if noon ecliptic altitude exceeds ninety degrees, reverse the signs. This yields the result.
88
西 西
To find the moon's distance from the eclipse limit at apparent time: subtract the quadrant mansion from the sun's ecliptic longitude; adjust according to whether the limit lies east or west. If the sun's ecliptic longitude exceeds the quadrant mansion, the limit is east; if less, west.
89
To find the limit's altitude above the horizon at apparent time: use the celestial radius, the sine of the ecliptic-meridian angle, and the cosine of the noon ecliptic altitude; look up the result in the tables.
90
To find the moon's altitude arc at apparent time: use the celestial radius, the sine of the limit altitude, and the cosine of the moon's distance from the limit; look up the result in the tables.
91
To find the ecliptic altitude arc angle at apparent time: use the sine of the moon's distance from the limit, the cotangent of the limit altitude, and the celestial radius; look up the result in the tables.
92
西 西西
To find the lunar-path altitude arc angle at apparent time: take the ecliptic altitude arc angle and add or subtract the great ecliptic-lunar distance; if the nodal longitude at greatest eclipse is in the first or eleventh mansion, add when the limit is east and subtract when west. For the fifth and sixth mansions, reverse the rule. This yields the result. If the angle exceeds ninety degrees, east and west limits interchange; if subtraction is insufficient, reverse it. If the ecliptic-horizon quadrant lies south of the zenith, the lunar-path horizon quadrant lies north; if the ecliptic-horizon quadrant lies north of the zenith, the lunar-path horizon quadrant lies south.
93
To find the sun's distance from Earth, see the lunar-eclipse section on the Earth's shadow semidiameter.
94
To find the moon's distance from Earth, see the lunar-eclipse section on the lunar semidiameter.
95
To find the parallax in altitude at apparent time: in a plane triangle with the Earth's semidiameter and the sun's distance as sides, use the moon's altitude arc minus a quadrant as the included angle and solve for the angle opposite the sun's distance. Subtract a quadrant to obtain the sun's apparent altitude. Subtract from the moon's altitude arc; the remainder is the sun's parallax due to the Earth's semidiameter. Again in a plane triangle with the Earth's semidiameter and the moon's distance, use the moon's altitude arc minus a quadrant and solve for the angle opposite the moon's distance. Subtract a quadrant to obtain the moon's apparent altitude. Subtract from the altitude arc; the remainder is the moon's parallax due to the Earth's semidiameter. Subtract the two parallaxes to obtain the difference in altitude parallax.
96
西西
To find the east-west correction at apparent time: use the radius of ten million, the cosine of the lunar-path altitude arc angle, and the tangent of the altitude parallax; look up the result in the tables.
97
西 西
To find the near time of greatest eclipse: use the true moon-sun elongation in seconds, one hour in seconds, and the east-west correction in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes as the near-time interval. Apply to the apparent time of greatest eclipse: add if the limit is west, subtract if east—still governed by whether the lunar-path altitude arc angle reverses the limit. This yields the near time of greatest eclipse.
98
仿
To find the equinox's equatorial distance from noon at near time: convert using the near time of greatest eclipse; the remaining steps follow the apparent-time method. The following steps follow the same pattern, but all calculations use the near-time values.
99
Find the equinox's ecliptic distance from noon at near time.
100
Find the noon ecliptic-equator latitude separation at near time.
101
Find the ecliptic-meridian angle at near time.
102
Find the noon ecliptic mansion at near time.
103
Find the noon ecliptic altitude at near time.
104
Find the ecliptic-horizon quadrant's distance from noon at near time.
105
Find the ecliptic-horizon quadrant mansion at near time.
106
西
To find the moon's distance from the limit at near time: take the sun's ecliptic longitude and add or subtract the apparent-time east-west correction according to the sign of the near-time interval. This gives the moon's ecliptic longitude at near time. Subtract the near-time quadrant mansion to obtain the moon's distance from the limit. The remaining steps follow the apparent-time method.
107
Find the limit's altitude above the horizon at near time.
108
Find the moon's altitude arc at near time.
109
Find the ecliptic altitude arc angle at near time.
110
Find the lunar-path altitude arc angle at near time.
111
Find the parallax in altitude at near time.
112
西
Find the east-west correction at near time.
113
西西
To find the apparent motion at greatest eclipse: double the apparent-time east-west correction and subtract the near-time correction.
114
西
To find the true time of greatest eclipse: use the apparent motion in seconds, the near-time interval in seconds, and the apparent-time east-west correction in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes as the true-time interval, apply to the apparent time of greatest eclipse, and obtain the true time of greatest eclipse. The sign of addition or subtraction follows that of the near-time interval.
115
仿
To find the equinox's equatorial distance from noon at true time: convert using the true time of greatest eclipse; the remaining steps follow the apparent-time method. The following steps follow the same pattern, but all calculations use the true-time values.
116
Find the equinox's ecliptic distance from noon at true time.
117
Find the noon ecliptic-equator latitude separation at true time.
118
Find the ecliptic-meridian angle at true time.
119
Find the noon ecliptic mansion at true time.
120
Find the noon ecliptic altitude at true time.
121
Find the ecliptic-horizon quadrant's distance from noon at true time.
122
Find the ecliptic-horizon quadrant mansion at true time.
123
西
To find the moon's distance from the limit at true time: take the sun's ecliptic longitude and add or subtract the near-time east-west correction according to the sign of the true-time interval. This gives the moon's ecliptic longitude at true time. The remaining steps follow the apparent-time method.
124
Find the limit's altitude above the horizon at true time.
125
Find the moon's altitude arc at true time.
126
Find the ecliptic altitude arc angle at true time.
127
Find the lunar-path altitude arc angle at true time.
128
Find the parallax in altitude at true time.
129
西
Find the east-west correction at true time.
130
To find the north-south correction at true time: use the radius of ten million, the sine of the lunar-path altitude arc angle, and the sine of the altitude parallax; look up the result in the tables.
131
To find the apparent latitude at greatest eclipse: apply the lunar-eclipse method for latitude at greatest eclipse to obtain the true latitude. Add or subtract the true-time north-south correction to obtain the apparent latitude at greatest eclipse. If the lunar-path horizon quadrant lies south of the zenith, add for south latitude and the apparent latitude remains south; subtract for north latitude and the apparent latitude remains north. If the true latitude is north but the north-south correction exceeds it, reverse the subtraction and the apparent latitude becomes south. If the quadrant lies north of the zenith, reverse the rule.
132
To find the solar semidiameter: use the sun's distance from Earth, its true semidiameter, and the celestial radius; look up the resulting sine in the tables.
133
To find the lunar semidiameter, see the lunar-eclipse section.
134
To find the eclipse magnitude: use the sun's full diameter as the first ratio and ten as the second; the third ratio is the sum of the solar and lunar semidiameters. Subtract the apparent latitude as the third ratio; the fourth ratio is the eclipse magnitude.
135
To find the apparent times of first and last contact: use the cosine of the apparent latitude at greatest eclipse, the cosine of the combined diameter, and the radius of ten million; look up the arc intervals in the tables. Use the true moon-sun elongation in seconds, one hour in seconds, and the contact interval arcs in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes to obtain the interval times to first and last contact. Apply these to the true time of greatest eclipse to obtain the apparent times of first and last contact. Subtract for first contact; add for last contact.
136
仿
To find the equinox's equatorial distance from noon at first contact: convert using the apparent time of first contact; the remaining steps follow the apparent-time method. The following steps follow the same pattern, but all calculations use the first-contact values.
137
Find the equinox's ecliptic distance from noon at first contact.
138
Find the noon ecliptic-equator latitude separation at first contact.
139
Find the ecliptic-meridian angle at first contact.
140
Find the noon ecliptic mansion at first contact.
141
Find the noon ecliptic altitude at first contact.
142
Find the ecliptic-horizon quadrant's distance from noon at first contact.
143
Find the ecliptic-horizon quadrant mansion at first contact.
144
西
To find the moon's distance from the limit at first contact: take the sun's ecliptic longitude, subtract the contact interval arc, and add or subtract the true-time east-west correction according to the sign of the true-time interval. This gives the moon's ecliptic longitude at first contact. The remaining steps follow the apparent-time method.
145
Find the limit's altitude above the horizon at first contact.
146
Find the moon's altitude arc at first contact.
147
Find the ecliptic altitude arc angle at first contact.
148
Find the lunar-path altitude arc angle at first contact.
149
Find the parallax in altitude at first contact.
150
西
Find the east-west correction at first contact.
151
Find the north-south correction at first contact.
152
西西西 西 西
To find the apparent motion at first contact: combine the first-contact and true-time east-west corrections—subtract if first contact and greatest eclipse share the same limit, add if the first-contact limit is east and the greatest-eclipse limit is west. This difference is applied to the contact interval arc to obtain the apparent motion. When the difference is obtained by subtraction: if the eclipse is in the eastern limit, subtract if the first-contact east-west correction is larger, add if smaller. If the eclipse is in the western limit, reverse the rule. When the difference is obtained by addition, always subtract.
153
To find the true time of first contact: use the apparent motion in seconds, the contact interval time in seconds, and the contact interval arc in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes as the first-contact interval. Subtract from the true time of greatest eclipse to obtain the true time of first contact.
154
仿
To find the equinox's equatorial distance from noon at last contact: convert using the apparent time of last contact. The remaining steps follow the apparent-time method. The following steps follow the same pattern, but all calculations use the last-contact values.
155
Find the equinox's ecliptic distance from noon at last contact.
156
Find the noon ecliptic-equator latitude separation at last contact.
157
Find the ecliptic-meridian angle at last contact.
158
Find the noon ecliptic mansion at last contact.
159
Find the noon ecliptic altitude at last contact.
160
Find the ecliptic-horizon quadrant's distance from noon at last contact.
161
Find the ecliptic-horizon quadrant mansion at last contact.
162
西
To find the moon's distance from the limit at last contact: take the sun's ecliptic longitude, add the contact interval arc, and add or subtract the true-time east-west correction according to the sign of the true-time interval. This gives the moon's ecliptic longitude at last contact. The remaining steps follow the apparent-time method.
163
Find the limit's altitude above the horizon at last contact.
164
Find the moon's altitude arc at last contact.
165
Find the ecliptic altitude arc angle at last contact.
166
Find the lunar-path altitude arc angle at last contact.
167
Find the parallax in altitude at last contact.
168
西
Find the east-west correction at last contact.
169
Find the north-south correction at last contact.
170
西西 西 西 西
To find the apparent motion at last contact: combine the last-contact and true-time east-west corrections—subtract if last contact and greatest eclipse share the same limit; add if the greatest-eclipse limit is east and the last-contact limit is west. Apply this to the contact interval arc to obtain the apparent motion. When the difference is obtained by subtraction: if the eclipse is in the eastern limit, add if the last-contact east-west correction is larger, subtract if smaller. If in the western limit, reverse the rule; when obtained by addition, always subtract.
171
To find the true time of last contact: use the apparent motion in seconds, the contact interval time in seconds, and the contact interval arc in seconds; the fourth ratio gives the correction in seconds. Convert to hours and minutes as the last-contact interval. Add to the true time of greatest eclipse to obtain the true time of last contact.
172
To find the total duration of the eclipse, add the first-contact and last-contact intervals.
173
宿
To find the sun's ecliptic lodge position, use the same method as in the section on solar motion.
174
宿宿
To find the sun's equatorial lodge position: use the fixed-star method to obtain the year's equatorial lodge register; the remaining steps follow the ecliptic method in the solar-motion section.
175
To find the fixed contact angles: compute the apparent latitude at first and last contact by the same method as at greatest eclipse. Then obtain each latitude-difference angle. Combine each with the ecliptic altitude arc angle to obtain the fixed contact angles at first and last contact. The method is the same as for lunar eclipses.
176
西
To find the orientation at first and last contact: when the eclipse is in the eastern limit and the fixed angle is within forty-five degrees, first contact lies upper-right and last contact lower-left. Beyond forty-five degrees, first contact is to the upper right and last contact to the lower left. At exactly ninety degrees, first contact is directly to the right and last contact directly to the left. Past ninety degrees, first contact is to the lower right and last contact to the upper left. When the eclipse is in the western limit and the fixed angle is within forty-five degrees, first contact lies lower-right and last contact upper-left. Beyond forty-five degrees, first contact is to the lower right and last contact to the upper left. At exactly ninety degrees, first contact is directly to the right and last contact directly to the left. Past ninety degrees, first contact is to the upper right and last contact to the lower left. At the capital, the ecliptic-horizon quadrant always lies south of the zenith; determine orientation accordingly; if north of the zenith, reverse the rule.
177
To find the magnitude of a horizon eclipse: if first contact or greatest eclipse occurs before sunrise, it is an eclipse emerging at sunrise—use the sunrise time; if greatest eclipse or last contact occurs after sunset, it is an eclipse setting at sunset—use the sunset time. Subtract from the true time of greatest eclipse; the remainder is the interval time to the horizon. Use the contact interval time in seconds as the first ratio and the contact apparent motion in seconds as the second; if the horizon event precedes greatest eclipse, use the apparent motion at first contact; if it follows greatest eclipse, use the apparent motion at last contact. Use the horizon interval time in seconds as the third ratio; the fourth ratio gives the correction in seconds. Convert to degrees and minutes to obtain the horizon interval arc. Use the radius of ten million, the cotangent of the horizon interval arc, and the cosine of the latitude at greatest eclipse; look up the separation between the two centers at the horizon. Use the sun's full diameter and ten as ratios; subtract the center separation from the combined diameter as the third ratio; the fourth ratio is the horizon eclipse magnitude.
178
西
To find the time and magnitude of the solar eclipse for each province: start from the capital's apparent time of greatest eclipse and adjust by each province's longitudinal offset. Then apply each province's polar altitude using the same method as for the capital.
179
To find the eclipse orientation for each province: use the provincial ecliptic altitude arc angle and the apparent latitudes at first and last contact to obtain the fixed contact angle.
180
The method for drawing the solar eclipse diagram is the same as for lunar eclipses, but use only the solar and lunar semidiameters to draw one large circle marking where the moon's center reaches at first and last contact. No inner circle is used, as there are no totality or light-return phases.
181
Constants for occultation and close approach, covering the motions of the seven planets, fixed stars, and eclipses.
182
Procedure for occultation and close approach: to determine entry into the zone, when the moon occults a fixed star, compare the moon's longitude today and tomorrow against the year's fixed-star table; if a star's latitude does not exceed ten degrees and its longitude falls within the limit, the event qualifies. Further determine whether the moon passes above or below each qualifying star: if both latitudes are north of the ecliptic, the higher latitude is above and the lower below. If both are south of the ecliptic, reverse the rule. If one is north and one south, the northern body is above and the southern below. When the moon passes above, apply if the latitudes are within two degrees; when it passes below, within one degree. A separation of seventeen arcminutes or less is an occultation; eighteen or more is a close approach; identical latitude is a covering. When the moon occults a planet: if today's lunar longitude lies before the planet and tomorrow's after, it enters the zone; the remaining rules match those for fixed stars. When a planet occults a fixed star, apply if the latitudes are within one degree. Three arcminutes or less is an occultation; four or more is a close approach; the remaining rules match those for the moon. When planets occult one another, the faster planet is the occulting body and the slower the body occulted. If speeds are equal but motions differ in direction, the direct-moving planet occults the retrograde one; entry requires today's longitude before the other body and tomorrow's after. The remaining rules match those for fixed stars.
183
To find the daily motion: for the moon occulting a fixed star, use the moon's true motion over one day. For occulting a planet: combine the moon's and planet's true daily motions—subtract if the planet is direct, add if retrograde. This yields the daily motion. When a planet occults a fixed star, use that planet's true motion over one day. When planets occult each other: combine their true daily motions—subtract if both move in the same direction, add if opposite. This yields the daily motion.
184
To find the time of occultation: use the daily motion in seconds, sub-quarter parts, and the separation from exact zi at today's epoch in seconds; the fourth ratio gives minutes. Convert to clock time starting from exact zi to obtain the result.
185
西
To find parallax for lunar occultation: planetary parallax is negligible and may be ignored. Use sub-quarter parts, the sun's true daily motion in seconds, and the occultation time in minutes; the fourth ratio gives seconds. Convert to degrees and minutes and add to the sun's true motion from exact zi to obtain the solar ecliptic longitude at that moment. Apply the solar-eclipse method to find the east-west and north-south corrections.
186
To find the moon's apparent latitude: take its true latitude and apply the north-south correction by the same rules as for solar eclipses. This yields the result. To find the moon's latitude separation from the star: combine the moon's apparent latitude with the star's latitude—subtract if both lie on the same side of the ecliptic, add if opposite. This gives the moon's latitude separation from the star. Apply if the separation is within one degree.
187
西 西
To find the apparent time of occultation: use the moon's hourly true motion in seconds, one hour in seconds, and the east-west correction in seconds; the fourth ratio gives seconds. Convert to minutes and apply to the occultation time: add if the limit is west, subtract if east. This yields the apparent time of occultation.
188
To find the sun's true anomaly: from the sun's mean anomaly compute its equation by the solar-motion method; from the moon's mean anomaly compute its first equation by the lunar-distance method; combine the two equations to obtain the elongation arc. Subtract if they share the same sign, add if opposite. Use the moon's hourly mean elongation from the sun, one hour in seconds, and the elongation arc in seconds; the fourth ratio gives the interval time in seconds, with sign determined accordingly. If both equations share the same sign: if the sun's is larger, keep the sign; if smaller, reverse it; if one calls for addition and one for subtraction, follow the sign of the sun's equation. Further use one hour in seconds, the sun's hourly equation, and the interval time in seconds; the fourth ratio gives the correction in seconds. Convert to degrees and minutes to obtain the sun's anomaly arc. Apply addition or subtraction according to the sign of the interval time. Add or subtract this from the sun's mean anomaly to obtain the true anomaly.
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