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卷三十五 志第十一 曆五

Volume 35 Treatises 11: Calendar 5

Chapter 35 of 明史 · History of Ming
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1
Treatise Eleven: Calendrics, Part Five.
2
▲ Grand Concordance Calendar Method, Part Three (Upper): Stepwise Computation.
3
便
Grand Concordance stepwise computation follows the Season Granting Calendar throughout, omitting only the solar expansion–contraction tables. Yet the shortcut procedures in the Comprehensive Track are indispensable for tabular computation, and their ordering also diverges slightly from the Calendar Classic. Solar terms, lunations, and the issuing-and-gathering sequence, for example, formed two chapters in the Season Granting; here the older and newer treatments are combined into one. In the Season Granting, the equation of center belonged to solar motion and the anomaly to lunar motion, while mean and true conjunction were computed separately. Here, once the mean conjunction is found, the true conjunction follows at once—a considerable practical advantage. There are seven sections: qi and lunation; solar motion; lunar motion; culminating stars; nodes and eclipses; the five planets; and the four residues.
4
▲ Stepwise Computation: Qi, Lunation, and Issuing-and-Gathering (attached)
5
The epoch is the jiazi year, Hongwu 17. The interval back to the Zhiyuan xinsi epoch is 104 counts.
6
Tropical year length: 3,652,425 parts; by observation, without solar equation correction. Halve it for the half-year circuit; quarter it for the qi-image limit; divide by twenty-four for the qi divisor.
7
Day unit: 10,000. That is one hundred quarter-hours; each quarter-hour has one hundred minutes, each minute one hundred seconds; finer subdivisions below all descend by hundreds.
8
Qi offset: 550,375 parts.
9
滿
Set the interval count at 104 to obtain a middle accumulation of 376,199,775 parts; add the xinsi qi offset of 550,600 parts for a universal accumulation of 376,750,375 parts; divide by the era divisor of 60 and take the remainder as the Grand Concordance qi offset.
10
Intercalation offset: 182,070 parts 18 seconds.
11
滿
Set the middle accumulation and add the xinsi intercalation offset of 202,050 parts to obtain an intercalation accumulation of 376,401,825 parts; divide by the synodic-month divisor and take the remainder as the Grand Concordance intercalation offset.
12
Rotation offset: 209,690 parts.
13
滿
Set the middle accumulation and add the xinsi rotation offset of 130,205 parts, totaling 376,329,980 parts; divide by the rotation cycle and take the remainder as the Grand Concordance rotation offset.
14
Node offset: 115,105 parts 08 seconds.
15
滿
Set the middle accumulation and add the xinsi node offset of 260,388 parts, totaling 376,460,163 parts; divide by the nodal cycle and take the remainder as the Grand Concordance node offset.
16
After the Season Granting Calendar was completed, its intercalation, rotation, and node offsets were soon revised. The Yuan History and Calendar Classic give an intercalation offset of 201,850 parts, whereas the Comprehensive Track records 202,050 parts—an increase of 200 parts that then advanced the mean conjunction by two quarter-hours. The Calendar Classic gives a rotation offset of 131,904 parts; the Comprehensive Track records 130,205 parts—a reduction of 1,699 parts that delayed nodal entry by seventeen quarter-hours and a fraction. The Calendar Classic gives a node offset of 260,187 parts 86 seconds; the Comprehensive Track records 260,388 parts—an increase of 200 parts 14 seconds that advanced true conjunction by two quarter-hours and a fraction. Some treat the Comprehensive Track's three xinsi offsets, which differ from the Yuan History, as Yuan–Ming revisions—this is mistaken. Calendar reform must rest on measurement and verification, and should then record the full course of events—why instead retroactively rewrite the Season Granting Calendar and efface their labor? Accordingly, the Comprehensive Track preserves the Season Granting's subsequently fixed constants, while the Calendar Classic retains its earlier, unfixed draft.
17
Universal remainder: 52,425 parts.
18
Synodic-month divisor: 295,305 parts 93 seconds, also called the synodic-month constant. Halve it for the full-moon divisor, also called the nodal full moon. Halve again for the quarter-moon divisor.
19
Universal intercalation: 108,753 parts 84 seconds.
20
Monthly intercalation unit: 9,062 parts 82 seconds.
21
Intercalation threshold: 186,552 parts 09 seconds. Also called the intercalation criterion.
22
Expansion-initial and contraction-final interval: 889,092 parts 25 seconds.
23
Contraction-initial and expansion-final interval: 937,120 parts 25 seconds.
24
Rotation cycle: 275,546 parts; halve it for rotation midpoint.
25
New-moon rotation increment: 19,759 parts 93 seconds.
26
Daily rotation limit: 12 limits 20.
27
Rotation midpoint limit: 168 limits 083060. Multiply the rotation midpoint by the daily rotation limit. Also called the limit aggregate.
28
New-moon rotation limit: 24 limits 1071146. Multiply the new-moon rotation increment by the daily rotation limit.
29
Quarter-moon rotation limit: 90 limits 06830865. Multiply the quarter-moon divisor by the daily rotation limit. Also called the limit divisor.
30
Nodal cycle: 272,122 parts 24 seconds.
31
New-moon node increment: 23,183 parts 69 seconds.
32
Qi expansion: 2,184 parts 37 seconds 50 micro-parts.
33
New-moon void: 4,694 parts 07 seconds.
34
Submergence threshold: 7,815 parts 62 seconds 50 micro-parts.
35
Expansion divisor: 96,695 parts 28 seconds.
36
Void divisor: 29,104 parts 22 seconds.
37
Earth-king divisor: 30,436 parts 87 seconds 50 micro-parts.
38
宿
Lodging divisor: 15,305 parts 93 seconds.
39
Era divisor: 600,000. That is the sixty-day decad cycle.
40
滿滿
To find the winter solstice of the civil year: set the interval from the Hongwu jiazi epoch, subtract one, multiply by the tropical year length for the middle accumulation, add the qi offset for the universal accumulation, and divide by the era divisor; the remainder not reaching a full cycle is the winter solstice of the civil year. Take 10,000 as one day; count off from the jiazi origin to obtain the winter solstice date and double-hour. Add the universal remainder repeatedly to obtain the next year's civil winter solstice.
41
滿滿
To find the civil-year intercalation remainder: set the middle accumulation, add the intercalation offset, divide by the synodic-month divisor, and take the remainder not reaching a full month as the civil intercalation remainder. Add the universal intercalation repeatedly to obtain the next year's civil intercalation remainder.
42
滿
To find the civil mean conjunction: set the winter solstice and subtract the intercalation remainder; if subtraction fails, add the era divisor and subtract again—this is the civil mean conjunction. In a common year, add 543,671,116. Twelve synodic-month divisors equal the era divisor. In an intercalary year, add 238,977,709. Thirteen synodic-month constants subtract the era divisor. When the era divisor is full, subtract it again to obtain the next year's civil mean conjunction. If the civil intercalation remainder lies above the intercalation threshold, that year has an intercalary month.
43
To find the civil-year solar equation at the winter solstice: set half the tropical year and subtract that year's full intercalation remainder; the remainder is the sought contraction sequence for the civil year. To proceed directly to the next year, subtract the universal intercalation from the civil contraction sequence. After subtraction, if the value falls below 153 days 09, add the synodic-month constant again for the next year's civil contraction sequence.
44
滿 滿 滿
To find the civil lunar anomaly: set the middle accumulation, add the rotation offset, subtract that year's full intercalation remainder, and divide the remainder by the rotation cycle—this is the civil entry into rotation. If below the rotation midpoint, it is the rapid sequence; if above, subtract the midpoint for the slow sequence. To proceed directly to the next year, add 237,191,916—the accumulated twelve rotation increments. In an intercalary year add the rotation increment again; divide by the rotation cycle whenever full; slow and rapid each retain their prior state. When the rotation cycle is full, subtract it and slow and rapid alternate in turn.
45
滿 滿
To find the civil nodal entry: set the middle accumulation, subtract the intercalation remainder, add the node offset, and divide by the nodal cycle—this is the civil nodal entry in days. To proceed directly to the next year, add 6,082 parts 04 seconds—the twelve node increments, subtracting the nodal cycle within. In an intercalary year add 29,265 parts 73 seconds—the thirteen node increments, subtracting the nodal cycle within. Whenever the nodal cycle is full, subtract it again to obtain the result.
46
滿
To find each month's mean conjunction and quarter- and full moons: set the civil mean conjunction divisor; divide by the era divisor; the remainder is the first month's mean conjunction. Add the quarter-moon divisor repeatedly and subtract the era divisor to obtain the quarter- and full moons and successive conjunctions.
47
滿
To find each mean solar term: set the civil winter solstice, add three qi divisors, divide by the era divisor, and obtain the constant day of Beginning of Spring. Add the qi divisor repeatedly and subtract the era divisor to obtain the constant days of all twenty-four terms.
48
退
To find which month receives the intercalation: set the synodic-month divisor and subtract that intercalary year's intercalation remainder; take the remainder as dividend and the monthly intercalation unit as divisor; the quotient, counted from the month after the civil new year, names the intercalary month. Intercalation may advance or retreat; the true conjunction lacking a mid-term qi remains the final criterion. If the remainder after subtraction falls short of one monthly intercalation unit, or only reaches one such unit, the intercalation belongs to the preceding year.
49
滿滿
To find each month's solar equation sequence: set the civil contraction sequence, add two synodic-month divisors, and subtract half the tropical year to obtain the expansion sequence below the first month's mean conjunction. Add the quarter-moon divisor repeatedly for each quarter- and full moon and successive conjunction; when half the tropical year is full, subtract it for nodal contraction; when half a cycle is full again, subtract once more to return to nodal expansion.
50
To find the initial and final limits: if the expansion sequence lies below the expansion-initial and contraction-final interval, or the contraction sequence below the contraction-initial and expansion-final interval, each is initial. Above those thresholds, subtract half the tropical year for the final interval.
51
To find the solar equation correction: set the small remainder of the initial or final interval, add the expansion–contraction entry from the ready reckoners and multiply for the dividend; divide by the day unit of 10,000; add the resulting lou number to the underlying equation accumulation to obtain the equation correction.
52
滿
To find each month's lunar anomaly sequence: set the civil mean-conjunction anomaly sequence and add two rotation increments to obtain the anomaly sequence below the first month's mean conjunction. Add the quarter-moon divisor repeatedly for quarter- and full moons and successive conjunctions; whenever the rotation cycle is full, subtract it and slow and rapid alternate in turn.
53
滿 滿
To find the anomaly limits: for each slow-interval count, multiply by the daily rotation limit to obtain the limit number. Add the quarter-moon rotation limit repeatedly; when the rotation midpoint limit is full, subtract it to obtain the limit for each quarter- and full moon and successive conjunction. To find the next month directly, add the new-moon revolution limit; when it fills the revolution midpoint, discard the excess to obtain the result. Alternate method: take the day-rate from the ready reckoners; where it is close to the small cloth value in the slow-rapid ephemeris, subtract it; a remainder of 820 or less gives the applicable limit.
54
退
To find the slow-rapid difference: set the slow-rapid ephemeris and subtract the ready-reckoner day-rate; if subtraction is impossible, shift back one decimal place. Multiply the remainder by the increase-decrease increment below as dividend; divide by 820 parts as divisor; add the quotient to the underlying slow-rapid accumulation to obtain the slow-rapid difference.
55
To find the additive-subtractive difference: take the expansion-contraction and slow-rapid differences below each mean new moon, first quarter, full moon, and last quarter; combine like cases (surplus with slow, deficit with rapid) and compare unlike cases (surplus with rapid, deficit with slow); multiply each by 820 parts as dividend; subtract 820 from the degrees within the slow-rapid limit to form the fixed-limit divisor; divide to obtain the additive-subtractive difference. Surplus paired with slow yields addition; deficit paired with rapid yields subtraction. In cross-comparison: if surplus exceeds slow, add; if rapid exceeds surplus, subtract; if deficit exceeds slow, subtract; if slow exceeds deficit, add.
56
退
To find the true new and full moons: set each mean new moon, first quarter, full moon, and last quarter, then add or subtract the additive-subtractive difference to obtain the true date. Check the sexagenary day of the true new moon: if it matches the next new moon the month is long; if not, short; if no mean qi falls within the month, it is intercalary. If a quarter or full moon shares the same ready-reckoner day but sunrise parts have already elapsed, name it one day earlier.
57
滿
To find each month's nodal entry: set the mean new moon's nodal entry at the celestial first month; add twice the nodal difference to obtain the first civil month's mean new moon nodal entry. Accumulate nodal quarter intervals; when full, discard the nodal cycle to obtain each month's nodal entry. To find the next month directly, add the nodal difference.
58
To find the Earth-king dominion: set the mean-qi days of Grain Rain, Great Heat, Frost's Descent, and Great Cold; subtract the Earth-king parameter; if insufficient, add the era cycle and subtract again to obtain each dominion day.
59
滿 滿 滿
To find emission-contraction with time-of-day: for each true new moon, quarter, full moon, and mean qi, take the lesser remainder, multiply by twelve, and divide by 10,000 for the double-hour, counting from zi midnight. At 5,000 parts, advance one further double-hour, counting from the first quarter of zi. After the double-hour is fixed, divide the remainder by 1,200 for quarter-hours, counting from the first quarter-hour. For the first quarter-hour at midnight, only the first through fourth quarter-hours are used in naming; the remainder is named beyond the count. The fourth quarter-hour is fractional, taking one-third of a quarter-hour unit; three such double-hours complete one quarter-hour, filling out twelve double-hours and one hundred quarter-hours.
60
便
In antiquity and in the Season Granting Calendar, emission-contraction formed its own chapter. Emission-contraction records the fine gradations of the sun's path opening southward and closing northward; attaching time-of-day further fixes the double-hours and quarter-hours of that process—hence emission-contraction with time-of-day. The Grand Concordance favored ease of calculation and merged emission-contraction with qi and new moon into one chapter, or thinned emission-contraction through multiplication and division—neither preserves its true substance.
61
滿
To find surplus days: inspect the mean qi's lesser remainder; if it lies above the extinction limit, that qi has surplus. Set the parameter remainder at 10,014,562.5 and divide the qi parameter by fifteen days. Subtract the surplus qi's lesser remainder; with the remainder, apportion the qi surplus over fifteen days at 68 parts 66. Multiply to obtain a value, add it to the mean qi's greater remainder, discard the era cycle when full, and count from jiazi beyond the count for the surplus day. To find the surplus day with parts and seconds, add the surplus parameter and again discard the era cycle.
62
滿
To find void days: inspect the mean new moon's lesser remainder; if below the new-moon void limit, that new moon carries void. Set the void new moon's lesser remainder; apportion the new-moon void over thirty days at 63 parts 91. Multiply to obtain a value, add it to the mean new moon's greater remainder, discard the era cycle when full, and count from jiazi beyond the count for the void day. To find the next void day. Set the day with parts and seconds; add the void parameter and again discard the era cycle.
63
宿 宿宿宿 宿宿宿宿 宿宿 宿
To find the lodge directly below: set the general accumulation and add the qi correspondence to the central accumulation. Subtract the intercalation correspondence; repeatedly remove the lodge conjunction of 280,000; with the remainder count from Wings beyond the count for the celestial first month's mean new moon lodge. Set the celestial first month's lodge; add two lodge parameters for the first civil month's mean new moon lodge. Accumulate by adding the lodge parameter to obtain each month's mean new moon lodge. Then add or subtract each month's new-moon additive-subtractive difference to obtain the true new moon's lodge.
64
▲ Solar motion.
65
The celestial circuit is 365°25′75″; half is half the celestial circuit; half again is the quadrant limit.
66
Precession: 1′50″ per year.
67
Circuit correspondence: 315°10′75″.
68
退
This is the Zhiyuan xinsi circuit correspondence—the arc from Void 7° to Winnowing Basket 10°. Hongwu jiazi lies one hundred four years later; precession has already shifted heaven by 54′50″, yet the circuit correspondence still uses the old value—likely a transmission error.
69
宿 滿宿
To find the winter solstice's solar position in equatorial lodges: set the central accumulation, add the circuit correspondence, and subtract precession accumulated since the epoch jiazi. Discard full celestial circuits; with the remainder start at Void 7° and subtract each lodge in turn to obtain the equatorial solar degree at winter solstice with time-of-day. For the following year, subtract precession cumulatively.
70
[Table omitted.]
71
宿
To find the winter solstice solar position in ecliptic lodges: set the equatorial solar degree at winter solstice with time-of-day, subtract the post-solstice equatorial accumulation, and multiply the remainder by the ecliptic rate. Divide by the equatorial rate, add the quotient to the ecliptic accumulation, and obtain the ecliptic solar degree at winter solstice with time-of-day. Ecliptic and equatorial accumulations and degree-rates all appear in Origins of the Method.
72
[Table omitted.]
73
To find the fixed quadrant limit: subtract the ecliptic winter-solstice solar degree from the equatorial to obtain the ecliptic-equatorial difference. Subtract the following year's ecliptic-equatorial difference from this year's; divide the remainder by four and add it within the qi image limit to obtain the fixed quadrant limit.
74
滿
To find the four fixed qi days: set the computed winter solstice parts as the winter fixed qi; add the expansion-initial and contraction-final limit; discard the era cycle when full; the remainder is the spring fixed qi. Add the contraction-initial and expansion-final limit, discard the era cycle, and obtain the autumnal fixed qi. Add the contraction-initial and expansion-final limit again, discard the era cycle, and obtain the next year's winter fixed qi.
75
To find the four fixed intervals in days: subtract the next fixed qi's greater remainder from the previous and add sixty days. If the next fixed qi is smaller, add sixty days before subtracting; add sixty days again for the interval.
76
To find the four fixed ecliptic accumulations at time-of-day: set the winter solstice ecliptic solar degree and add the fixed quadrant limit cumulatively for each fixed time.
77
To find the four fixed reduction parts at time-of-day: take each fixed qi's lesser remainder, multiply by its first-day travel degree, and divide by the solar circuit.
78
The winter fixed qi travels 1°0.51085 per day. From the spring fixed qi, at ninety-three days to the summer fixed qi the travel is 0°0.999703 per day; at ninety-four days, 1° per day. The summer fixed qi travels 0°0.951516 per day. From the autumn fixed qi, at eighty-eight days to the winter fixed qi the travel is 1°0.000505 per day; at eighty-nine days, 1° per day.
79
To find the four fixed midnight ecliptic accumulations: set each fixed time's ecliptic accumulation and subtract its time-of-day reduction.
80
宿滿宿
To find the four fixed midnight ecliptic lodges: set each midnight ecliptic accumulation and discard full ecliptic lodge degrees.
81
To find the four fixed midnight interval degrees: subtract the previous midnight ecliptic accumulation from the next; if insufficient, add the celestial circuit before subtracting.
82
To find the four fixed travel day-differences: subtract the travel accumulation below the interval from twice the interval degree; divide the remainder by the interval in days for the day-difference. If the travel accumulation is subtracted from within the interval degree, the day-difference is additive; if the interval degree is subtracted from within the travel accumulation, it is subtractive.
83
From the autumn fixed qi to the winter solstice, and from the winter solstice to the spring fixed qi: at eighty-eight days the travel accumulation is 90°4009; at eighty-nine days, 91°4014. From the spring fixed qi to the summer solstice, and from the summer solstice to the autumn fixed qi: at ninety-three days the travel accumulation is 90°5990; at ninety-four days, 91°5987.
84
滿宿
To find each day's midnight solar degree: set the daily travel after each fixed time from the ready reckoners. Add or subtract the day-difference to obtain the fixed daily travel. Set the four fixed midnight solar degrees; add the fixed daily travel each day; discard full ecliptic lodge degrees to obtain each midnight solar degree.
85
宿
Ecliptic degrees of the twelve stations.
86
Rooftop (Wei): 12°6491, entering Maidens' Mantle (Ziju zi); chronogram hai.
87
Striding Legs (Kui): 1°7362, entering Sinking Barrens (Jiang lou); chronogram xu.
88
Striding Legs: 4°56, entering Great Bridge (Daliang); chronogram you.
89
Stomach (Wei): 37°7456, entering Great Bridge; chronogram you.
90
Net (Bi): 6°8805, entering Established Quiescence (Shishen); chronogram shen.
91
Well (Jing): 8°3494, entering Quail's Head (Chunshou); chronogram wei.
92
Willow (Liu): 3°8680, entering Quail's Fire (Chunhuo); chronogram wu.
93
Extended Net (Zhang): 15°2606, entering Quail's Tail (Chunwei); chronogram si.
94
Chariot Shaft (Zhen): 10°0797, entering Longevity Star (Shouxing); chronogram chen.
95
Root (Di): 1°1452, entering Great Fire (Dahuo); chronogram mao.
96
Tail (Wei): 3°115, entering Split Wood (Ximu); chronogram yin.
97
Dipper (Dou): 3°7685, entering Star Chronicle (Xingji); chronogram chou.
98
Girl (Nü): 2°0638, entering Dark Axletree (Xuanxiao); chronogram zi.
99
宿
To find the time when solar motion enters each of the twelve stations: set the entry lodge degree; subtract the midnight solar degree on the entry night; multiply the remainder by the solar circuit, treating one part as one hundred. That is the dividend. Subtract the entry night's midnight solar degree from the next night's midnight solar degree for the divisor. Divide dividend by divisor; apply emission-contraction with time-of-day to obtain the station-entry moment.
100
▲ Lunar motion.
101
Mean lunar travel: 13°36′87.5″ per day.
102
Cycle limit: 336; half is the middle limit; half again is the initial limit.
103
Limit mean travel: 0°0.962 per day.
104
Solar limit travel: 0°8′20″ per day.
105
First quarter: 91°31′43″ excess.
106
Full moon: 182°62′87.5″.
107
Last quarter: 273°94′31″ deficit.
108
Nodal cycle: 363°79′34.196.
109
Mean new-moon parallel motion: 394.78711516875°.
110
To find the mean nodal day after new moon: set the nodal-cycle remainder and apply the solar-term and conjunction sequence. Subtract the civil first-month mean new-moon nodal-entry parts to obtain the mean nodal day after new moon. For the following month, subtract the nodal difference of 2 days 31869 repeatedly to obtain each month's mean nodal day after new moon. If subtraction fails, add the nodal cycle and subtract again; when the node again falls within the month, this is the double-nodal month's mean nodal day after new moon. Every year necessarily contains one double-nodal month.
111
To find mean nodal entry into the rotation anomaly sequence: set the mean new-moon anomaly sequence and add the mean nodal day after new moon to obtain mean nodal rotation entry. Below the rotation midpoint the anomaly matches the mean new moon; above it, subtract the midpoint—fast at the node becomes slow, slow becomes fast. For the following month, subtract the nodal-rotation difference of 3423.76 parts repeatedly, deducting the rotation difference from within the nodal difference. The result follows. If subtraction fails, add the rotation midpoint and subtract again; slow and rapid alternate as before.
112
To find the mean nodal limit anomaly difference: set the mean nodal rotation-entry anomaly sequence and derive the anomaly difference by the solar-term and conjunction procedure.
113
To find the mean nodal crossing fixed correction: set the mean nodal limit anomaly difference, multiply by the paired-day rate of 820 parts, and divide by the travel degrees within the applicable anomaly limit. Add in the slow interval; subtract in the fast interval.
114
滿
To find the mean new-moon time-of-day accumulation: set the mean new-moon expansion–contraction sequence, as in the solar-term and conjunction section. In the expansion sequence it is the time-of-day central accumulation; in the contraction sequence add half the tropical year. For the following month, add the synodic-month divisor repeatedly and discard the tropical year when full to obtain each conjunction's time-of-day central accumulation, naming days as degrees. When a month contains two nodes, the later node uses the former node's mean new-moon time-of-day central accumulation.
115
宿 滿宿 仿
To find the true node's ecliptic accumulation and lodge from the winter solstice time-of-day: set the mean nodal day after new moon, multiply by mean lunar travel for the post-node degrees, and add the mean new-moon time-of-day central accumulation to obtain each month's true nodal ecliptic accumulation from the winter solstice moment. Add the winter solstice ecliptic solar degree at time-of-day to inspect solar motion. Subtract successive entries from the ecliptic accumulation tally until the remainder falls within one lodge to obtain the true nodal month's lodge. For the following month, subtract the mean nodal new-moon difference of 1.463102° repeatedly. Subtract the nodal-cycle arc from the celestial circuit; the value should be 1.464080°. In a double-nodal month, proceed as for the next mean new moon. Apply the same rule thereafter.
116
▲ Ecliptic accumulation tally.
117
[Table omitted.]
118
滿
To seek true nodal day double-hour and quarter-hour: set the mean nodal day after new moon (text reads symptom-node day), add the mean new moon, remove the era cycle, add or subtract the mean nodal fixed difference; for the day count from jiazi beyond the count, for the small remainder seek by emission-contraction with time-of-day—then obtain the true nodal day, double-hour, and quarter-hour. For the following month, add the nodal cycle repeatedly and discard the era cycle when full. In a double-nodal month, add the nodal cycle once more.
119
宿滿
To find the four cardinal equatorial lodges: set the winter solstice equatorial solar degree, add the qi quadrant repeatedly, and discard the equatorial accumulation when full to obtain the four cardinal equatorial degrees at time-of-day.
120
▲ Equatorial accumulation tally.
121
[Table omitted.]
122
滿
To find the initial and final limits of the true nodal ecliptic arc after the solstices: set the true nodal ecliptic accumulation from the winter solstice moment; below half the tropical year counts as post-winter-solstice, above that subtract half the year for post-summer-solstice. Inspect the arc after each solstice: below the qi quadrant is the initial limit; above it, subtract half the tropical year for the final limit. For the next month: if the current month is in the initial limit, subtract the mean nodal new-moon difference repeatedly; the remainder is the next month's initial limit. If subtraction fails, subtract the mean nodal new-moon difference in reverse; the remainder is the next month's final limit. If the current month is in the final limit, add the mean nodal new-moon difference repeatedly for the next month's final interval; when the qi quadrant is full, subtract half the tropical year—the remainder is the next month's initial limit.
123
To find the fixed-difference degree: set the initial or final limit and multiply by the quadrant-to-pole total difference of 1.605508 to obtain the fixed difference in degrees. The quadrant-to-pole total difference divides the pole difference by the quadrant; the value should be 16.05442 parts. For the next month's initial limit subtract the pole mean difference of 23.4902 parts repeatedly; for the final limit add it repeatedly. The pole mean difference is the mean nodal new-moon difference multiplied by the quadrant-to-pole total difference; the value should be 23.5049 parts.
124
To find the distance-difference degree: set the pole difference at 14.66° and subtract the fixed-difference degree. For the following month, add or subtract the pole mean difference. Add in the initial limit; subtract in the final limit.
125
To find the fixed-limit degree: set the fixed-difference degree and multiply by the fixed-pole total difference of 1.637107; this is the pole difference divided by 24°, which should equal 1.637107°. Apply the product as subtraction after the winter solstice and addition after the summer solstice, in each case against the base of 98°.
126
宿 滿
To find the lunar-path and equator true-nodal lodge: after the winter solstice set the spring equinox accumulation and add the distance difference in the initial limit while subtracting it in the final limit; after the summer solstice set the autumn equinox accumulation and subtract in the initial limit while adding in the final limit. Discard full cycles from the equatorial accumulation tally to obtain the lodge.
127
宿宿宿 宿滿 滿 滿
To find post-true-nodal accumulation with initial and final limits: identify the lodge of true nodal crossing, set that lodge's full equatorial arc, subtract the true-nodal lodge degree, and the remainder is the post-true accumulation. Accumulate each lodge's full equatorial arc and discard the qi quadrant when full to obtain the post-half-node interval. Discard the qi quadrant again when full to obtain the post-middle-node interval. Discard once more when full to obtain the second post-half-node interval. For each crossing accumulation: below half the quadrant is the initial limit; above it, subtract the quadrant from above for the final limit.
128
To find the fixed difference: multiply each crossing's fixed-limit degree by the initial or final limit, scale by a thousand, and express the result in degrees. Add after true and middle nodal crossings; subtract after half-node crossings.
129
宿宿 宿宿 宿宿
To find the lunar-path fixed accumulation and lodge: set the per-lodge accumulation after each crossing, apply the fixed difference, and obtain each crossing's lunar-path accumulation. Add the true-nodal fixed lodge degree on the lunar path and equator to obtain the post-true-nodal lodge degree. Subtract the preceding lodge's fixed accumulation to obtain each crossing's lunar-path lodge.
130
▲ Examples for the active quadrant limit.
131
宿宿 宿宿 宿宿 宿 宿
Set the post-true-nodal lodge and add the previous crossing's post-half-node final-lodge fixed accumulation. This yields the active quadrant limit. If the post-true-nodal lodge degree is too small to absorb the previous crossing's addition, set the post-true-nodal lodge and add the qi quadrant instead. In a node-shift month, set the post-true-nodal lodge and add the previous crossing's first-half final-lodge fixed accumulation to obtain the node-shift active quadrant limit. Suppose the previous true node lies in Axletree (Zhen) and the later in Horn (Jiao), with the previous crossing one Axletree lodge short. To find the active quadrant limit: set the post-true-nodal lodge, do not add the fixed accumulation from below Wings (Yi), but still add that from below Axletree (Zhen). Again, if the previous true node is Axletree and the later is Wings (Yi), the previous crossing exceeds by one Wings lodge. To find the active quadrant limit: set the post-true-nodal lodge, do not add from below Wings, but add the fixed accumulation from below Extended Net (Zhang).
132
仿
To find the interval in days: subtract the fixed new-moon large remainder from the fixed first-quarter large remainder. Apply the same method from first quarter to full moon, full moon to last quarter, and last quarter to new moon. If subtraction fails, add the era cycle and subtract again.
133
To find true new moon, quarters, and full moons entering the equation sequence and fixed equation correction: set each month's equation sequence at conjunction and quarters, apply the conjunction–quarter correction, all by the solar-term and conjunction procedure. This is the true equation sequence. In the expansion sequence, below the expansion-initial interval is expansion-initial; above it, subtract half the tropical year for expansion-final. In the contraction sequence, at or below the contraction-initial interval is contraction-initial; above it, subtract half the tropical year for contraction-final. Derive the equation correction by the solar-term and conjunction procedure to obtain the fixed equation correction.
134
便 便滿
To find the true conjunction and quarters' time-of-day central accumulation: set the true equation sequence; at new moon in expansion it is the central accumulation; add the qi quadrant at first quarter, half the tropical year at full moon, and three quadrants at last quarter. At new moon in the contraction sequence, add half the tropical year. Add three quadrants at first quarter; at full moon use the central accumulation directly; add the qi quadrant at last quarter; discard the full celestial circuit when the sum is full.
135
To find the ecliptic central fixed accumulation at true new moon, quarters, and full moon: set the time-of-day central accumulation and add or subtract the underlying fixed equation correction—add for expansion, subtract for contraction.
136
宿滿滿 滿宿
To find the equatorial accumulation and lodge at time-of-day: set the ecliptic fixed accumulation at time-of-day; below one celestial quadrant is post-solstice, above is post-equinox; discard two quadrants for post-solstice and three for post-equinox. Set the post-solstice or post-equinox ecliptic accumulation, subtract the tabulated value, multiply the remainder by the equatorial rate and divide by the ecliptic rate, add to the interval accumulation, then restore the discarded quadrants to obtain the equatorial fixed accumulation at time-of-day. Add the civil winter solstice equatorial degree at time-of-day to the equatorial fixed accumulation and discard full cycles from the equatorial tally to obtain the true conjunction and quarters' equatorial lodges at time-of-day.
137
宿 宿宿滿
To find the post-true, post-half, and combined-crossing accumulation: set the equatorial lodge at true conjunction or quarters and determine whether the event falls after the true-half or middle-half crossing. Add the crossing-generated accumulation from the preceding lodge to obtain the post-true or post-middle accumulation, discarding the qi quadrant when full to mark a node shift.
138
To find the initial and final limits: if the post-true or post-middle accumulation is below half the quadrant it is initial; above, subtract the qi quadrant for the final limit.
139
To find the lunar-path and equator fixed difference: multiply the crossing's fixed-limit degree by the initial or final limit, scale by a thousand, and express in degrees. Add at true and middle nodal crossings. Subtract at half-node crossings.
140
宿宿
To find the lunar-path lodge at true new moon, quarters, and full moon at time-of-day: set the lunar-path fixed accumulation at time-of-day, take the post-crossing lunar-path fixed accumulation, and subtract that of the lodge before the one set. At a node shift the prior accumulation is larger and the current value smaller, so subtraction fails. When shifting from half-node to true-node, add the active quadrant limit for that crossing and subtract. From true to half, half to middle, or middle to half, add the qi quadrant and subtract in each case.
141
便
To find midnight rotation-entry day: set the mean conjunction and quarter anomaly sequences and apply the true conjunction–quarter correction. In the fast sequence this is the rotation-entry day at true conjunction or quarter at time-of-day. In the slow sequence add the rotation midpoint to the time-of-day rotation-entry day and subtract the small remainder for midnight entry; if the entry day is too small, add the rotation cycle and subtract again.
142
To find rotation degrees at time-of-day: take the small remainder without seconds, multiply by the fixed rotation degree under the midnight rotation-entry day, and scale by ten thousand to obtain fen.
143
▲ Slow–rapid rotation fixed-degree tally.
144
[Table omitted.]
145
宿 宿宿
To find the midnight rotation accumulation and lodge for true new moon, quarters, and full moon: subtract the time-of-day rotation degrees from the lunar-path fixed accumulation at time-of-day to obtain the midnight accumulation. If the fixed accumulation at new moon, first quarter, full moon, or last quarter first crosses a node at time-of-event, subtraction falls short. Where half and major adjoin, apply the variable quadrant; where major-half and middle-half adjoin, add the qi quadrant; then subtract the rotation degrees entered at time-of-event. Major becomes later half, later half middle, middle first half, and first half major. Set the midnight lunar-path fixed accumulation for new moon, first quarter, full moon, or last quarter; subtract by the procedure for time-of-event lunar-path lodge positions to obtain the midnight lodge.
146
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Procedure to derive morning-and-evening rotation-entry day and rotation degrees: Set the midnight rotation-entry day, look up the morning fraction for that day in the fixed expansion–contraction ready reckoner and add it to obtain the morning rotation-entry day, discarding the rotation period when full. Set the day's morning fraction, multiply by the fixed rotation degree under the midnight rotation-entry day, scale by ten thousand to obtain fen, and the product is the morning rotation degree. To find the evening rotation day and rotation degree, look up the evening fraction for that day by the same procedure.
147
宿 滿 宿 宿
Procedure to derive morning-and-evening rotation accumulated degrees and lodge positions: Set the midnight lunar-path fixed accumulation for new moon, first quarter, full moon, or last quarter and add the morning rotation degree to obtain the morning rotation accumulation. For the evening rotation accumulation, add the evening rotation degree; when the sum reaches the qi quadrant, discard it—this marks a node change. If, when deriving the midnight accumulation, the time-of-event fixed accumulation could not subtract the rotation degree and half and major adjoined so that the variable quadrant was added, then on a further change to the major node subtract the variable quadrant instead. Set the morning rotation accumulation and subtract by the preceding method to obtain the morning-fraction lodge. Set the evening rotation accumulation and subtract by the same method to obtain the evening-fraction lodge.
148
Procedure to derive separation degrees: From new moon to first quarter and from first quarter to full moon, use the evening rotation accumulation. From full moon to last quarter and from last quarter to new moon, use the morning rotation accumulation. Set the later segment's morning-or-evening rotation accumulation; if it lies on the same node as the earlier segment, subtract the earlier segment's morning-or-evening rotation accumulation in full—the remainder is the separation degree. If the later and earlier segments span two nodes—from major to half, half to middle, or middle to half—add the qi quadrant. From half to major, add the variable quadrant. Then subtract the earlier segment's morning-or-evening rotation accumulation. If the later and earlier segments span three nodes: when no half-to-major transition occurs within, add two qi quadrants; when a half-to-major transition does occur within, add one variable quadrant and one qi quadrant; then subtract the earlier segment's morning-or-evening rotation accumulation.
149
Procedure to derive the fixed rotation accumulation: Set the morning-or-evening rotation-entry day. From new moon to quarter and from quarter to full moon, use evening. From full moon to quarter and from quarter to new moon, use morning. Subtract the earlier segment from the later; if subtraction fails, add twenty-eight days and subtract again to obtain the morning-and-evening separation in days. Under the earlier segment, look up the matching morning-and-evening separation day in the register and take its fixed rotation accumulation. If the new-moon-to-quarter separation in days is one day shorter than the morning-and-evening separation, find the matching morning-and-evening separation day, take its rotation accumulation, subtract the fixed rotation extreme difference of 14°7154, and the remainder is the fixed rotation accumulation from the earlier to the later segment.
150
▲ Register of Fixed Rotation Accumulations
151
[Table below omitted.]
152
Procedure to derive the addition-and-subtraction difference: Subtract the fixed rotation accumulation from the separation degree as dividend and divide by the number of days from new moon to quarter (or the corresponding interval) as divisor. If the separation exceeds the quotient's basis, the result is an addition difference; if less, a subtraction difference.
153
Procedure to derive the Moon's fixed daily motion: Set the morning-or-evening rotation-entry day at new moon, first quarter, full moon, or last quarter; take the fixed rotation degree under that day from the slow–rapid fixed-rotation register; accumulate day by day, adding or subtracting the addition-and-subtraction difference, until the separation day—the result is obtained.
154
宿宿滿宿
Procedure to derive the lunar-departure lodge at morning and evening each day: Set the morning-or-evening lodge at new moon, first quarter, full moon, or last quarter; add the fixed daily lunar motion each day and, when the sum fills the lunar-path lodges, subtract—the lodge is obtained.
155
宿
▲ Equatorial Twelve-Palace Boundary Lodges
156
[Table omitted.]
157
宿宿便 滿
Procedure to derive the accumulated degree after a palace boundary following the Moon's major equatorial node crossing: After the major crossing of the lunar path and equator, identify each lodge's accumulated degree at a palace boundary; add the lodge that lies next behind to obtain that palace's post-crossing boundary accumulation. For the next palace, add the palace rate of 20°4381 cumulatively; discard the qi quadrant when full—each sum gives a palace's lower-half post-crossing boundary accumulation.
158
Procedure to derive the fixed palace-boundary accumulation: If the boundary degree lies below the half-quadrant, it is the initial limit; if above, subtract the qi quadrant in reverse—the remainder is the terminal limit. Set the fixed limit degree for the node in question; subtract and multiply against the initial and terminal limits; scale the product by a thousand to degrees. At major and middle nodes this yields an addition difference; at half nodes, a subtraction difference. Set the accumulated degree after the major, half, or middle palace boundary and add or subtract the fixed difference to obtain the fixed palace-boundary accumulation.
159
宿宿
Procedure to derive the palace-boundary lodge: Set the fixed palace-boundary accumulation; within the lunar path subtract the lodge immediately preceding the one placed—if subtraction fails, add the qi quadrant and subtract again.
160
宿宿 宿宿
Procedure to derive the time of palace entry below the node for each day of each month: Set the month's palace-boundary lodge and subtract the morning-or-evening lunar-departure lodge on the node-palace-entry day. If subtraction fails, add the lodge before the palace-boundary lodge and subtract; multiply the remainder by the day circuit and divide by that day's fixed lunar motion; then look up the morning-and-evening fraction for the day in the fixed expansion–contraction ready reckoner and add it. For morning, add the morning fraction; for evening, add the evening fraction.
161
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If the sum fills the day circuit, palace entry falls on the next day; if not, on the current day. Apply the emission-and-collection procedure to obtain the time of node-palace entry.
162
▲ Stepping the Culminating Stars
163
Procedure to derive the midnight equator for each day: Take the midnight ecliptic derived for each day (see Solar Progression). By the prescribed method subtract the ecliptic accumulation; divide the remainder by the ecliptic ratio and add the quotient to the equatorial accumulation. Add the equator at the celestial origin's seasonal nodes. After the spring standard add one quadrant; after the summer solstice add half a circumpolar circuit; after the autumn standard add three quadrants—the sum is each day's midnight equatorial accumulation.
164
宿宿宿
Procedure to derive the midnight equatorial lodge: Set the midnight equatorial degree and subtract successive equatorial lodge widths to obtain this day's midnight equatorial lodge.
165
Procedure to derive the morning separation degree and watch-interval difference: Take each day's morning fraction from the ready reckoner, multiply by 366°25′75″ as dividend, and divide by the day circuit to obtain the morning separation degree. Double the morning separation degree and divide by five to obtain the watch-interval difference degree.
166
宿 宿
Procedure to derive the culminating stars at midnight each day: Set the midnight equatorial lodge derived for each day, add half a circumpolar circuit, and the sum is the midnight culminating accumulation. Subtract successive equatorial lodge widths to obtain the midnight culminating-star lodge.
167
滿宿
Procedure to derive the dusk and dawn culminating stars: Set the midnight culminating accumulation and subtract the morning separation degree to obtain the dusk culminating accumulation. Add the watch-interval difference cumulatively to obtain the culminating accumulations for successive watches and for dawn. Whenever any sum fills the equatorial lodges, discard the circuit—the lodges are obtained. Take one-fifth of the morning fraction and add it to the watches to obtain the watch rate. Divide the watch rate by five to obtain the point rate. Each dusk fraction equals one watch and one point; add the watch rate cumulatively for successive watches. Each change of watch equals one point; add the point rate cumulatively for successive points.
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