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Volume 37 Treatises 13: Calendar 7

Chapter 37 of 明史 · History of Ming
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Chapter 37
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1
Treatise Thirteen: Calendrics, Part Seven.
2
▲ The Islamic (Huihui) Calendar Method, Part One
3
西 西西 西
The Islamic Calendar Treatise was composed by Muhammad, king of Medina in the Western Regions. Its latitude is 24.5°; longitude lies 107° west [of the Chinese standard], roughly 8,000+ li west of Yunnan. Its epoch is Sui Kaihuang jiwei (599 CE)—the year of the kingdom's founding. Early in the Hongwu era the treatise was recovered at the Yuan capital (Dadu). In autumn of Hongwu 15 the Founder observed that Western astronomical prediction is unrivaled in precision, and that planetary latitudes in their system were unknown in Chinese astronomy. He ordered Hanlin academicians Li Chong and Wu Bozong, together with the Muslim astronomer Jamal al-Din (Ma Sha Yih Hei) and others, to translate the work. The system has no intercalary months; the solar year is fixed at 365 days. The year comprises twelve zodiac signs; signs receive leap days—31 leap days in every 128-year cycle. The lunar cycle is 354 days; each twelve-month cycle admits intercalary days in its months. Over 128 years the solar cycle gains 31 leap days; the lunar cycle is 354 days in twelve months, with intercalary days inserted in the months. Eleven intercalary days are added to the months every 30 years; after 1,941 years the solar sign, lunar month, day, and hour realign. Such are the broad principles of the system's design.
4
西
Western calendrical systems recorded in history include the Tang Nine Offices Calendar and Jamal al-Din's Eternal Calendar of the Yuan. The Nine Offices Calendar was the crudest; the Eternal Calendar was employed only briefly. Only the Islamic calendar was instituted as a formal curriculum at the Imperial Observatory and used alongside the Datong calendar for more than 270 years. Predictions of eclipse magnitude and visibility still varied at times, but the system far surpassed the Nine Offices and Eternal calendars. Yet the transmitted text is full of lacunae and errors. Presumably because observatory staff of that tradition relied on sand-board calculation and continued to use texts in their native script. Meanwhile Ming scholars of the tradition—Tang Shunzhi, Chen Rang, Yuan Huang, and others—produced treatises advancing independent interpretations. Hence the translated edition never gained currency; its incompleteness is understandable. We have now sought out specialists in the tradition, collated the original sources, filled lacunae and corrected errors, and set down the Islamic Calendar Method in this chapter.
5
西
Accumulated years: from the Western Hijra era through Sui Kaihuang jiwei. Down to Hongwu jiazi (1384 CE)—786 years in total.
6
Constants: celestial revolution = 360°. Each degree = 60 minutes; each minute = 60 seconds; smaller units follow the same ratio. Twelve zodiac signs. Each sign spans 30°. Diurnal arc = 1,440 parts; 24 hours per day, 60 parts per hour. Ninety-six quarter-hours (ke) per day. Each quarter-hour = 15 parts. Sign degrees begin at Aries; solar terms begin at the vernal equinox; clock hours begin at true noon. The first four ke after noon belong to the previous civil day.
7
Seven luminaries numbering: Sun 1, Moon 2, Mars 3, Mercury 4, Jupiter 5, Venus 6, Saturn 7. Dates are reckoned by the seven-day planetary week, not the sexagenary cycle.
8
Sign indices: Aries 0, Taurus 1, Gemini 2, Cancer 3, Leo 4, Virgo 5, Libra 6, Scorpio 7, Sagittarius 8, Capricorn 9, Aquarius 10, Pisces 11.
9
Sign days—Aries (xu palace): 31 days. Taurus (you palace): 31 days. Gemini (shen palace): 31 days. Cancer (wei palace): 32 days. Leo (zi/wu palace): 31 days. Virgo (si palace): 31 days. Libra (chen palace): 31 days. Scorpio (mao palace): 30 days. Sagittarius (yin palace): 29 days. Capricorn (chou palace): 29 days. Aquarius (zi palace): 30 days. Pisces (hai palace): 30 days. The twelve signs above constitute the "fixed months" of the solar year, totaling 365 days—the days of the annual circuit. In a year with a solar leap day, one day is added in Pisces, for 366 days total.
10
Lunar month lengths: odd months long, even months short. These twelve constitute the "moving months" of the lunar year. Long months have 30 days and short months 29, totaling 354 days for the twelve lunar months. When a lunar leap day is required, one day is added within the twelfth month, yielding 355 days.
11
Solar and planetary apogee longitudes, fixed by observation in Sui jiwei (599 CE). Sun: sign 2, 29°21′. Saturn: sign 8, 14°48′. Jupiter: sign 6, 0°08′. Mars: sign 4, 15°04′. Venus: sign 2, 17°06′. Mercury: sign 7, 6°17′.
12
西 滿 滿
Procedure to determine whether the year has a solar leap day, and the weekday of the first day if there is none. Set the accumulated years before the current Western year, subtract 1, and multiply by 159 (the total leap days per 128-year solar cycle). Add 15 inside for the intercalary adjustment. Repeatedly subtract 128; if the remainder is 97 or greater, there is a solar leap day that year. If so, the year has a solar leap day; otherwise it does not. To the quotient add 5—the sign tables begin with Mars (no. 3), hence the increment. Cast out complete sevens; the remainder is the weekday of the first day of Aries for the sought year. If there is a leap day, add one day; subsequent procedures are the same.
13
西 滿
Procedure to find lunar leap days and the weekday of the first day of the first month. Set the accumulated years before the current Western year, subtract 1, and multiply by 131. Add 194 inside for the intercalary adjustment. Repeatedly subtract 30; if the remainder is 19 or greater, there is a lunar leap day that year. If so, the year has a lunar leap day; otherwise it does not. Cast out complete sevens from the quotient; the remainder is the weekday of the first day of the first month.
14
Epoch correction: set accumulated days, combining the full accumulation with the solar leap-day count. Subtract the lunar leap count; add 331 days inside (the day before jiwei spring first). Divide by 354; from the remainder subtract the 331 added, then subtract 23 to complete one year's day count. Subtract 24 again for the Hongwu jiazi epoch correction. Subtract 1 again for the one-day revision adjustment. This yields the true interval in days from the jiwei epoch to the present. Alternate method: combine solar leap accumulation with general intercalation as the solar total; subtract lunar leap; set 11, multiply by years from epoch, add 14 outside, divide by 30 to obtain the lunar leap count. Divide by 354; from the remainder subtract the Hongwu correction (24), the supplement day (23), and the revision day (1)—as before. To find general intercalation: set 11 days and multiply by years from epoch. For solar leap days, see the procedure above.
15
▲ Solar Motion in Degrees
16
西 仿
Procedure for total apogee longitude: set accumulated years before the current Western year; enter the lookup table for whole years with zero month and day; for each component take the prior year, prior month, and prior day apogee longitudes and sum them. To find year 10, take the entry for year 9, and so on. Table entries give complete values for the current year, month, and day. Using the year-10 entry when computing through year 10 would overshoot. The same rule applies to months and days. Subsequent procedures follow this pattern.
17
Procedure for apogee longitude: set the total apogee longitude obtained and add the fixed solar apogee at epoch—sign 2, 29°21′. This is the solar apogee longitude in Aries for the sought year. For the next sign, add 5′06″ cumulatively. For the next month, add 4′56″.
18
西
Procedure for mean longitude and daily mean motion. Set accumulated years; enter the lookup table for whole years with zero month and day; take each day's mean longitude and sum them—same retrieval method as above. Subtract 1′04″ inside; this is the mean longitude for the first day of Aries in the sought year. To find each sign's month-days: accumulate the daily motion of 59 parts 8 seconds day by day. Subtract 1 part 4 seconds within; some call this the longitudinal difference between the Western Regions and China, but that is wrong—it is the adjustment for the jìwèi epoch's year-end degree.
19
To find the proper-motion degree: set that day's mean longitude and subtract that sign's apogee longitude. The result is the degree entered into the expansion–contraction sequence.
20
To find the equation correction. This is the expansion–contraction difference. Take the proper-motion sign-degree as the argument, enter the solar equation ready reckoner, and take the correction for that sign-degree. This is called the undetermined correction. For the fractional remainder below that degree, apply proportional interpolation: subtract this degree's correction from the next degree's correction, convert the remainder to seconds (one part equals sixty seconds), convert the argument's fractional remainder to seconds likewise and multiply; the product is in fibre units—seconds times seconds yield fibre. Collect by sixty into minute-fractions, seconds, and parts. If the amount is large, first collect by sixty into minute-fractions, then again into seconds, then again into parts. Compare the undetermined correction obtained above with the next value: if smaller, add the next degree's correction; if larger, subtract—this yields the fixed equation correction in parts. If there is no fractional remainder, use the undetermined correction directly as the fixed correction. Later cases follow the same rule.
21
To find the ecliptic longitude. Set that day's mean longitude and add or subtract the fixed equation correction in parts; where the argument's proper-motion sign lies in signs 1–5 the correction is subtractive, in signs 6–11 additive. The result is the ecliptic longitude.
22
滿
To find the planetary weekday: set the accumulated years, enter the ready reckoner, combine the weekday numbers under total years, zero years, month, and day, repeatedly discard sevens, and the remainder is the weekday for Aries day one. For the next sign, add that sign's weekday number within. For successive days, add one each day and discard sevens when full. The Moon, the five planets, and Rahu–Ketu weekdays all follow this rule.
23
▲ Lunar motion
24
To find mean longitude: set the accumulated years, enter the ready reckoner, combine the mean longitudes under total, zero years, month, and day, and subtract 14 parts within for the jìwèi epoch adjustment. This is the mean longitude for Aries day one of the year sought. For successive days, accumulate the daily motion. Daily motion: 13°10′35″.
25
To find the doubled-separation degree—the Moon's motion on the epicycle, its distance from the Sun after conjunction. Set the accumulated years, enter the ready reckoner, combine the doubled-separation under total years, zero years, month, and day, subtract 26 parts within, and obtain Aries day one. For successive days, accumulate the doubled-separation daily motion. 24°22′53″22‴; halve this for the epicycle center's distance from the Sun.
26
To find deferent motion—that is the lunar rotation degree. Set the accumulated years, enter the ready reckoner, combine deferent motion under total, zero years, month, and day, subtract 14 parts within, and obtain Aries day one. For each day sought, accumulate the deferent daily motion. Daily motion: 13°3′54″.
27
To find the first equation correction, also called the doubled-separation correction. Take the doubled-separation sign-degree as the argument, enter the lunar first-equation ready reckoner, and take the correction. This is the undetermined correction. Subtract from the next correction, multiply the remainder by the argument's fractional remainder for seconds, collect parts-times-parts by sixty into parts, and apply to the undetermined correction—add when the next value is larger, subtract when smaller, as for the Sun. The result is the first correction in parts.
28
To find deferent motion: set that day's deferent motion and add or subtract the first correction in parts. By the doubled-separation degree: add in the first six signs, subtract in the last six.
29
To find the second equation correction: take the deferent fixed motion as the argument, enter the lunar second-equation ready reckoner, take the undetermined correction, and interpolate proportionally as before. Obtain the fractional part and add or subtract it as the second correction in parts. By the argument: before sign 6 the correction is subtractive, after sign 6 additive.
30
To find the ratio parts: by the doubled-separation sign-degree, enter the first-equation ready reckoner and take the ratio parts. If the doubled-separation fractional part is 30 parts or more, take the next degree's ratio parts.
31
To find the proximity correction: by the deferent fixed sign-degree as argument, enter the lunar second-equation ready reckoner and take the proximity parts. The argument's fractional part is also obtained by proportional interpolation.
32
To find the general and fixed corrections: set the ratio parts, multiply by the proximity degree in common parts, and reduce by sixty to parts—this is the general correction. Add the general correction to the second correction to obtain the fixed correction.
33
To find longitude: set that day's lunar mean longitude, add or subtract the fixed correction, and obtain the lunar longitude. By the deferent fixed motion: subtract before, add after.
34
▲ Lunar latitude
35
To find the Rahu–Moon separation and nodal fixed degree. Set that day's lunar longitude and subtract that day's Rahu motion within to obtain the Rahu–Moon separation in parts.
36
To find latitude: take the Rahu–Moon separation sign-degree as the argument, enter the lunar-latitude ready reckoner—upper signs use right-motion direct degrees, lower signs left-motion retrograde degrees. Take the degree and parts, interpolate the fractional part proportionally, and add in the upper six signs or subtract in the lower six. The result is the latitude in parts. Arguments before sign 6 yield north latitude; after sign 6, south latitude.
37
To find Rahu's motion: set the accumulated years in the ready reckoner for total, zero years, month, and day, combine the Rahu mean motions, and obtain Aries day-one motion for that year. For each sign's first day: add that sign's daily motion and subtract from twelve signs; the remainder is Rahu's motion for that sign's day one. For Rahu's day-by-day fine motion: subtract the prior and following segment motions and divide the remainder by the intervening days to obtain the daily increment. Set the prior segment's Rahu motion and accumulate, subtracting the daily increment each day. For Ketu's motion: set it within that day's Rahu motion (opposite).
38
▲ Longitude of the five planets
39
To find apogee total degree: the reckoning matches the Sun; apply the solar procedure above.
40
To find apogee motion: set the planet's apogee total degree, add the observed fixed apogee motion (see above), and obtain that year's Aries apogee motion. This is the apogee motion for Aries day one of the year sought. For each sign and day, add that sign's daily motion.
41
To find mean longitude: follow the solar procedure.
42
To find proper motion: set accumulated years in the ready reckoner, combine each planet's proper motion under total, zero years, month, and day, and obtain Aries day-one proper motion for that year. Saturn, Jupiter, and Venus subtract 1 part; Mercury subtracts 3 parts; Mars subtracts none. For each sign and day, accumulate that planet's proper motion. For Mercury: from sign 3's initial degree compute in five-day segments; from sign 9's initial degree in ten-day segments—the same for latitude.
43
To find mean longitude and epicycle-center degree—that is the five planets' deferent entry into the sequence. Saturn, Jupiter, and Mars: set the Sun's mean longitude and subtract the planet's proper motion to obtain mean longitude. Subtract apogee motion within as well to obtain the epicycle-center degree. Venus and Mercury: mean longitude equals the Sun's mean longitude; subtract the planet's apogee within—the remainder is the epicycle-center degree. If subtraction fails, add twelve signs and subtract.
44
To find the first equation correction—the expansion–contraction difference. Take the planet's epicycle-center sign-degree as the argument, enter its first-equation ready reckoner, and interpolate proportionally. The method matches the Sun and Moon.
45
To find fixed proper motion and fixed epicycle center: where the first correction's argument lies in signs 1–5, add the correction to proper motion and subtract from the epicycle center—each yields a fixed degree. In signs 6–11, subtract the correction from proper motion and add to the epicycle center—each yields a fixed degree.
46
To find the second equation correction: by the planet's fixed proper motion, enter its second-equation ready reckoner, take degree and parts, and add or subtract proportionally. Same as before.
47
To find ratio parts: for Saturn, Jupiter, Venus, and Mercury, by the epicycle center's sign-degree enter the first-equation ready reckoner; if the argument's fractional part is 30 parts or more, take the next degree's ratio parts. For Mars, the proportional method must be used throughout.
48
To find proximity correction: by fixed proper-motion sign-degree, enter the second-equation ready reckoner, take the proximity value, and interpolate proportionally.
49
To find general and fixed corrections: same method as the Moon.
50
To find longitude: set the fixed epicycle-center degree, add or subtract the fixed correction—add before sign 6 by the fixed proper-motion argument, subtract after. Add the planet's apogee motion within.
51
退 退退
To find the station interval: take that segment's fixed epicycle-center sign-degree as the argument and enter each planet's sequence fixed limit in the ready reckoner. Enter the five-planet direct, retrograde, and station ready reckoner; at the nearest degree in the same sign take the planet's degree-parts and subtract from the prior and following motions. If the result falls in signs 1–6, subtract the following motion from this motion. From sign 6 back to sign 1, subtract the prior motion from this motion. Subtract the ready reckoner's nearest degree in the same sign from the argument sign-degree; convert both remainders to common parts, multiply, and divide by six (the table's six-degree interval). Collect by sixty parts; add for direct motion or subtract for retrograde from the prior degree-parts; when the result equals that day's fixed proper motion, that day is a station. If fixed proper motion is greater, the station day has passed; if less, it has not yet arrived. To obtain the fine ratio, subtract the value found from that day's proper-motion determined degree and divide the remainder by the planet's daily proper motion—for example, Saturn's daily proper motion of about 5°7′. The result is how many days before or after station fall on the current day. Saturn stations for seven days; the three days before and after the station day match the station count. Jupiter stations for five days; the two days before and after match the station count. Mars, Venus, and Mercury do not truly station; once retrograde begins they continue retrograde, pausing only at the extremity of their motion parts.
52
退
Procedure to derive fine motion parts: for Saturn, Jupiter, Venus, and Mars, subtract prior and subsequent segment longitudes and divide by the interval to obtain daily motion parts. For Mercury, subtract the prior day's longitude from the Aries-first-day longitude; the remainder is the initial day's motion parts. Again subtract prior and subsequent segment longitudes and divide by the interval to obtain parallel motion parts. Add or subtract the initial day's motion parts, double the result, and divide by the days from the day before the prior segment to the subsequent interval to obtain the daily difference. Add or subtract from the initial day's motion parts: if they are less than the parallel motion parts, add; if greater, subtract. The result is the daily motion parts. For each planet, set the prior segment's longitude and add or subtract daily motion parts forward or backward to obtain day-by-day longitudes.
53
Procedure to derive concealment and visibility: if a planet's proper-motion determined degree lies above the limit in the concealment-and-visibility ready reckoner, that marks morning or evening concealment or visibility.
54
Procedure to derive the five planets' latitudes: obtain apogee total travel, center travel, proper-motion, and epicycle degrees by the five-planet ratio-longitude method.
55
滿 滿
Procedure to derive the proper-motion determined degree: set proper-motion mansion degrees and minutes and multiply the mansion by ten for degrees. One mansion times ten yields ten degrees; this rounding shortcut builds the latitude ready reckoner. Multiply degrees by twenty for minutes and, when full, reduce by sixty to degrees. Multiply minutes by twenty for seconds and, when full, reduce by sixty to minutes. Combine them to obtain the value.
56
滿 滿
Procedure to derive the epicycle-center determined degree: set epicycle-center mansion degrees and minutes and multiply the mansion by five for degrees. One mansion times five yields five degrees. Multiply degrees by ten for minutes and, when full, reduce by sixty to degrees. Multiply minutes by ten for seconds and, when full, reduce by sixty to minutes. Combine them to obtain the value.
57
滿
Procedure to derive latitude: with epicycle-center and proper-motion determined degrees, enter the planet's latitude ready reckoner and take one vertical and one horizontal value. Subtract the value taken from the lower row. If the planet crosses the ecliptic, add to the lower row instead. Again subtract the upper epicycle-center determined value on the ready reckoner from the epicycle-center determined value in the upper horizontal row. Multiply the two remainders and divide by the epicycle-center cumulative increment on the ready reckoner. For example, Saturn's upper horizontal row steps epicycle-center degree every three degrees and Mars every two. Reduce by sixty to minutes and add or subtract the two values: if greater than the lower row, subtract; if less, add. At ecliptic crossing, subtract even when the lower-row value is larger. Set aside on the left. Again subtract the ready-reckoner proper-motion determined degree in the first vertical row from the proper-motion determined degree. With the two values again, subtract from the lower row; at ecliptic crossing, add to the lower row. Multiply the two remainders and divide by the proper-motion cumulative increment—as when Saturn's vertical row steps every ten degrees and Mars every four. Reduce to minutes. Add or subtract the left-stored value: if the two values exceed the lower row, subtract; if less, add. At ecliptic crossing, if the new minutes exceed the left-stored amount, subtract the left-stored amount from the result; the remainder is the arc north or south of the ecliptic crossed. The result is the fixed ecliptic latitude north or south.
58
退 退 退
Procedure to derive fine latitude daily motion: subtract prior-segment from subsequent-segment latitude and divide by the interval for the daily difference. Set the prior-segment latitude and add or subtract the daily difference forward or backward for day-by-day latitude. When the prior latitude is less than the subsequent, add forward and subtract backward. When the prior exceeds the subsequent, subtract forward and add backward. The two cases cannot share one rule. When north and south differ between segments, add prior and subsequent latitudes and divide by the interval for the daily difference. Set the prior latitude and subtract the daily difference repeatedly; when subtraction fails, take the remainder from the daily difference and add forward to obtain day-by-day latitude.
59
Procedure to derive solar eclipses: for eclipse parameters, use the prior day's values for pre-noon conjunction and the next day's for post-noon conjunction.
60
Discern eclipse limits: at conjunction, if lunar latitude is within 45′ south or 90′ north of the ecliptic, the eclipse is visible on Earth. If conjunction is total, the eclipse is seen in full. If the obscured new moon falls three watches before sunrise or a watch and a quarter (15 minutes) after sunset, there is a partial eclipse in every case. If conjunction falls in the night watches, do not compute it.
61
Derive the greatest-eclipse general time, which is conjunction. Set the Moon's longitude past the Sun at noon; see the lunar-eclipse procedure for the Moon's hourly motion past the Sun. Convert to seconds, multiply by 24 for the dividend, subtract solar from lunar daily motion (also in seconds) for the divisor, and divide to obtain hours. Convert the remainder below the hour to minutes and below minutes to seconds; carry at 30″ to the minute and 60′ to the hour—the sum is the greatest-eclipse general time.
62
滿
Derive solar longitude at each conjunction: convert greatest-eclipse general time to minutes, multiply by solar daily motion in seconds, divide by 24, reduce by 60, and add or subtract from noon solar longitude—subtract before noon, add after. The result is solar longitude at conjunction. This is the ecliptic degree on the day of greatest eclipse.
63
Derive add-subtract parts: at conjunction, enter the solar mansion in the latitude-longitude hourly add-subtract ready reckoner and obtain the parts by proportional method.
64
Derive midnight-to-conjunction time: set greatest-eclipse general time and add or subtract the add-subtract minutes—subtract before noon, add after. Then add or subtract twelve hours—subtract twelve for pre-noon conjunction, add twelve for post-noon. The result is midnight-to-conjunction time in minutes and seconds. Note: reckoning from midnight standard alters the procedure to match the Datong calendar and departs from the original method.
65
西 西
Derive the first east-west (longitude) difference. At conjunction, if the solar mansion lies in the right seven mansions of the hourly add-subtract ready reckoner, take the upper-row hourly value for direct motion. In the left seven mansions take the lower-row hourly value for retrograde motion. From midnight to conjunction, take the longitude difference and apply the proportional method. Use only the fractional remainder below the hour. The same applies below. This yields the first east-west difference.
66
西 西
Derive the second east-west difference: at conjunction, if the solar mansion lies in the ready reckoner, proceed as above. Take the next mansion's midnight-to-conjunction longitude difference and apply the proportional method to obtain the second east-west difference.
67
Derive the first north-south (latitude) difference. At conjunction, with solar mansion and midnight-to-conjunction time, enter the ready reckoner as above. Take the latitude difference and apply the proportional method to obtain the first north-south difference.
68
Derive the second north-south difference: with the conjunction solar mansion, take the next mansion's midnight-to-conjunction latitude difference by proportional method.
69
Derive the second time difference: with the obscured-new-moon solar mansion and midnight-to-obscured-new-moon time, enter the ready reckoner, take the time difference, and apply the proportional method.
70
For the second time difference, with the conjunction solar mansion take the next mansion's midnight-to-conjunction time difference by proportional method.
71
西西西 西西 西
Derive east-west difference at conjunction: subtract the second from the first east-west difference, convert to seconds, and multiply by conjunction solar longitude in seconds. Divide by 30° for filaments, reduce by 60 to micro, seconds, and minutes, and add or subtract from the first east-west difference—add if the first is less than the second, subtract if greater; the same below. The result is the east-west difference at conjunction.
72
Derive north-south difference at conjunction: subtract the two north-south differences, convert the remainder to seconds and multiply by solar longitude, divide by 30, reduce by rate, and add or subtract from the first north-south difference.
73
Derive time difference at conjunction: subtract the two time differences, multiply by solar longitude, divide by 30, reduce by rate, and add or subtract from the first time difference.
74
Derive deferent motion at conjunction: set deferent daily motion at 13°4′ (unified) and multiply by greatest-eclipse general time, also unified. Divide by 24 for seconds, reduce by rate to minutes and degrees, and add or subtract from noon deferent motion—subtract before noon, add after. The result is deferent motion at conjunction.
75
Derive the proportional factor: enter deferent motion into the solar-lunar hourly motion and shadow-radius ready reckoner. Take the lunar proportional factor for the same mansion and nearby degree and apply the proportional method.
76
西西西
Derive the east-west fixed difference: convert conjunction east-west difference and proportional factor to seconds, multiply for filaments, reduce by 60, and add to the conjunction east-west difference—always add, never subtract. The result is the fixed difference.
77
西
Derive the north-south fixed difference by the same method as the east-west fixed difference.
78
滿
Derive greatest-eclipse fixed time, that is, the fixed minutes of greatest eclipse. Inspect conjunction solar longitude in the ready reckoner: in the left seven mansions subtract black entries and add white for the time difference; in the right seven mansions reverse the signs; add or subtract from midnight-to-conjunction time, name from midnight, and subtract to obtain the watch's initial standard. Convert the remainder to seconds, multiply by 1,000, and divide by 144—since 60 minutes make one hour and the day has 1,440 minutes. Reduce by 60; at 100 parts make one ke—the result is greatest-eclipse fixed time.
79
西
Derive greatest-eclipse lunar longitude: add or subtract the east-west fixed difference from conjunction solar longitude. Add or subtract according to the sign of the time difference at greatest-eclipse fixed time.
80
滿
Derive conjunction Ketu longitude: convert greatest-eclipse general time to minutes, multiply by Ketu's daily motion of 3°11″, divide by 24, reduce by 60, and add or subtract from noon Ketu motion—Rahu and Ketu are retrograde: add before noon, subtract after. The result is Ketu's longitude at conjunction.
81
Procedure to derive the Moon's latitude at conjunction: at greatest eclipse, add or subtract Ketu's longitude at conjunction within the lunar longitude; the remainder is Ketu's separation from the Moon; look it up in the lunar-latitude ready reckoner.
82
Procedure to derive the greatest-eclipse lunar latitude: apply the north–south fixed parallax. Add or subtract the lunar latitude at conjunction: add if south of the ecliptic, subtract if north. The result is the greatest-eclipse latitude.
83
滿
Procedure to derive the Sun's proper-motion degree at conjunction: convert the Sun's daily motion of 59 parts 8 seconds to seconds, multiply by the greatest-eclipse general time (parts likewise converted to seconds). Divide by 24; collect fine parts by sixties into seconds and parts; add or subtract from the day's noon proper-motion degree—subtract before noon, add after noon at conjunction. The result is the Sun's proper-motion degree at conjunction.
84
Procedure to derive the Sun's diameter parts: set the Sun's proper-motion degree at conjunction as the argument, enter the shadow-and-diameter ready reckoner at the same palace and nearest degree, and obtain the solar diameter parts by proportional interpolation.
85
Procedure to derive the Moon's diameter parts: set the epicycle motion degree at conjunction as the argument, enter the same ready reckoner at the same palace and nearest degree, and obtain the lunar diameter parts by proportional interpolation.
86
Procedure to derive the two semi-diameter parts: add the solar and lunar diameter parts and halve the sum.
87
Procedure to derive the solar eclipse limit: set the two semi-diameter parts and subtract the greatest-eclipse lunar latitude; the remainder is the solar eclipse limit. If subtraction fails, there is no eclipse. If the Moon has no latitude, the eclipse is total. If the Moon has no latitude and the solar diameter exceeds the lunar diameter, the eclipse is annular.
88
Procedure to derive the solar greatest-eclipse fixed parts: convert the solar eclipse limit to seconds, multiply by 1000 as the dividend, divide by the solar diameter in seconds, and scale by 100 to obtain the solar greatest-eclipse fixed parts.
89
滿
Procedure to derive the hour equation, namely the fixed usable parts. Square the greatest-eclipse lunar latitude in seconds, square the two semi-diameter parts in seconds, subtract the squares, take the square root of the remainder, multiply by 24 for the dividend, and set that day's lunar daily motion minus solar daily motion (in seconds) as the divisor. Divide the dividend by the divisor; the quotient is parts, and 60 parts make one hour—this is the hour equation.
90
滿
Procedure to derive first contact: set the greatest-eclipse fixed time, subtract the hour equation, count the remainder forward from midnight (zi), and obtain the initial proper hour. Convert the fractional remainder to seconds, multiply by 1000, divide by 144, reduce by 60, and when the quotient reaches 100 parts form one quarter-hour mark—this is the first-contact quarter-hour.
91
Procedure to derive last contact: set the greatest-eclipse fixed time, add the hour equation, and apply the same counting from midnight as for first contact to obtain the restoration quarter-hour.
92
Procedure to derive the azimuths of first contact, greatest eclipse, and last contact: same method as the Grand Concordance calendar.
93
Procedure for lunar eclipse: for a pre-noon full moon reckon from the prior day; for a post-noon full moon reckon from the next day.
94
Discern the lunar-eclipse limit: if on the full-moon day the lunar longitude lies within 23° of Rahu or Ketu and the solar latitude is below 1°8′, an eclipse is possible. Also: if syzygy falls within two du before the Moon rises or within two hours before it sets, the eclipse may be visible only at the horizon. If the interval is two hours or more, do not reckon it.
95
Procedure to derive the greatest-eclipse general time, namely the mean full moon. Set the day's lunar longitude and subtract six palaces; if subtraction fails, add twelve palaces and subtract the day's noon solar longitude—this identifies a pre-noon full moon. If the solar longitude cannot be subtracted, add six palaces and subtract again—this identifies a post-noon full moon. Convert the subtraction remainder to seconds and multiply by 24 for the dividend; set the day's lunar longitude and subtract the prior day's lunar longitude—for a post-noon full moon subtract the next day's solar longitude instead. The remainder is the solar daily motion. Subtract the two daily motions, convert the remainder to seconds as the divisor, and divide the dividend to obtain hours. For the fractional remainder under the hour, convert by 60 into parts and seconds—this is the greatest-eclipse general time sought.
96
Procedure to derive the Moon's ecliptic palace at greatest eclipse: multiply the greatest-eclipse general time and solar daily motion (both in seconds), divide by 24, collect fine parts into micro-units, seconds, and parts, and add or subtract from the day's noon solar longitude—subtract before noon, add after noon at full moon. The result is the solar longitude at full moon; add six palaces to obtain the value sought.
97
Procedure to derive the day–night equation: set the solar palace at full moon as the argument, enter the day–night additive–subtractive ready reckoner, and obtain the correction by proportional interpolation.
98
Procedure to derive the greatest-eclipse fixed time: set the greatest-eclipse general time and apply the day–night equation. Subtract before noon at full moon; add after noon. Apply the result to twelve hours: for a post-noon full moon add 12 hours; for a pre-noon full moon subtract from 12 hours. Count from midnight (zi); obtain the initial proper hour. For the fractional remainder, collect quarter-hour marks by the same method as for solar eclipse. The result is the fixed time.
99
Procedure to derive Ketu's longitude at full moon: convert the greatest-eclipse general time to seconds as the dividend, multiply by Ketu's daily motion of 3 parts 11 seconds, divide by 24, collect fine parts into micro-units, seconds, and parts, and add or subtract from the day's noon Ketu longitude—Rahu and Ketu are retrograde: add before noon, subtract after noon at full moon. The result is obtained.
100
Procedure to derive the lunar latitude at full moon: set the Moon's ecliptic longitude at full moon and subtract Ketu's longitude at full moon; if subtraction fails, add twelve palaces and subtract again. The remainder is Ketu's separation from the Moon; look it up in the lunar-latitude ready reckoner.
101
Procedure to derive the epicycle motion degree at full moon, namely entry into the slow–fast sequence. Set the Moon's epicycle daily motion at 13 parts 4. Convert to a common denominator, multiply by the greatest-eclipse general time in seconds, divide by 24 for fine parts, collect by sixties into seconds, parts, and degrees, and add or subtract from the day's noon epicycle motion—subtract before noon, add after noon at full moon. The result is obtained.
102
Procedure to derive the lunar diameter parts: set the epicycle palace degree at full moon and obtain the value from the shadow-and-diameter ready reckoner. The method is the same as for solar eclipse.
103
Procedure to derive the lunar shadow diameter parts: set the epicycle palace degree at full moon and take the value from the shadow-diameter ready reckoner.
104
滿
Procedure to derive the Sun's proper-motion degree at full moon: convert the solar daily motion of 59 parts 8 seconds and the greatest-eclipse general time to seconds, multiply, divide by 24, collect fine parts into micro-units, seconds, and parts, and subtract from the day's noon solar proper-motion degree. The method matches solar-eclipse procedure for deriving solar longitude.
105
Procedure to derive the shadow-diameter reduction: set that day's solar proper-motion palace as the argument, enter the shadow-diameter ready reckoner, take the lunar shadow-diameter difference at the same palace and nearest degree, and obtain it by proportional interpolation. The method is as given above.
106
Procedure to derive the fixed shadow-diameter parts: set the lunar shadow-diameter parts and subtract the shadow-diameter reduction.
107
Procedure to derive the two semi-diameter parts: add the lunar diameter parts and the fixed shadow-diameter parts, then halve the sum.
108
Procedure to derive the lunar eclipse limit: set the two semi-diameter parts and subtract the lunar latitude at full moon.
109
Procedure to derive the greatest-eclipse fixed parts: convert the eclipse limit to seconds, multiply by 1000 as the dividend, divide by the lunar diameter in seconds, scale by 100 to parts, and obtain the greatest-eclipse fixed parts.
110
滿
Procedure to derive the Moon's hourly motion relative to the Sun: subtract the prior day's lunar longitude from the full-moon lunar longitude, and the prior day's solar proper motion from the full-moon solar proper motion; subtract the two remainders to obtain the Moon's diurnal motion past the Sun. Convert to seconds, divide by 24, and collect by sixties to obtain the hourly motion past the Sun in parts.
111
Procedure to derive the hour equation: square the lunar latitude in seconds and the two semi-diameter parts in seconds, subtract, take the square root as the dividend, divide by the Moon's hourly motion past the Sun in seconds, and obtain the hour-and-mark difference. This is the fixed usable interval from first contact to greatest eclipse.
112
Procedure to derive the quarter-hours of first contact and last contact: subtract the hour equation from the greatest-eclipse fixed time to obtain first contact. Add the hour equation to the greatest-eclipse fixed time to obtain last contact. The methods for counting hours and collecting quarter-hour marks are the same as for solar eclipse.
113
Procedure to derive the hour equation from totality to greatest eclipse: subtract the lunar diameter from the two semi-diameter parts, square in seconds, square the lunar latitude in seconds, subtract, and take the square root as the dividend. Divide by the Moon's hourly motion past the Sun in seconds; the quotient is the hour equation.
114
Procedure to derive the quarter-hours of totality and emergence of light: subtract the totality-to-greatest-eclipse hour equation from the greatest-eclipse fixed time to obtain totality. Add the hour equation to the greatest-eclipse fixed time to obtain emergence of light.
115
Procedure to derive the azimuths of first contact, greatest eclipse, and last contact: same method as the Grand Concordance calendar.
116
西
Procedure to derive sunrise and sunset times: set noon solar longitude as the argument, enter the Western Regions day–night-time ready reckoner, and obtain degree parts by proportional interpolation as the first provisional value. Also take the opposing palace in the reckoner—for example, 3° in the first palace paired with 3° toward the sixth palace—and obtain degree parts the same way. Obtain a second provisional value by proportional interpolation. Subtract the two provisional values; if subtraction fails, add 360° and subtract again. Convert the remainder to seconds, divide by 15, collect by sixties into parts and hours, and obtain that day's daylight in hours, parts, and seconds. Halve to obtain half the daylight for that day in hours, parts, and seconds. Subtract half-daylight from 12 hours for sunrise; add 12 hours for sunset.
117
Procedure to derive horizon-eclipse parts and seconds: if sunrise falls after first contact but before greatest eclipse and last contact, the eclipse is visible only at sunrise (horizon eclipse). Subtract the greatest-eclipse fixed time from that day's sunrise or sunset time; the remainder is the horizon-eclipse offset. Set the solar or lunar greatest-eclipse fixed parts, multiply by the horizon-eclipse offset in seconds, divide by the hour equation in seconds, and obtain the horizon-eclipse parts. Subtract the horizon-eclipse parts from the greatest-eclipse fixed parts; the remainder is the magnitude visible at the horizon.
118
滿 滿 滿 仿
Procedure to derive lunar-eclipse watches and marks: set 24 hours, subtract daylight, then subtract morning-and-evening time of 72 parts—this is the Central Calendar's 5 quarter-hours less a fraction. For the remaining night hours, convert to seconds and divide by 5 to obtain the watch divisor. Divide the fractional parts by the watch divisor to obtain the mark divisor. If the eclipse is before midnight: set first contact, greatest eclipse, last contact, and the like, subtract sunset time, then subtract half the morning-and-evening interval of 36 parts. Convert the remainder to seconds and divide by the watch divisor to obtain the watch count. For the remainder less than one watch, divide by the mark divisor to obtain the mark count. If the eclipse is after midnight: halve the night hours, add first contact, greatest eclipse, last contact, and the like, and divide by the watch divisor for the watch count. For the remainder less than one watch, divide by the mark divisor to obtain the mark count. In every case count from the first watch and first mark. Subtract repeatedly by the watch divisor; each subtraction counts as one watch; if the final remainder is less than one divisor, still count it nominally as one watch. The mark divisor follows the same rule.
119
▲ Lunar and Five-Planets Encroachment
120
Procedure to derive the Moon's diurnal motion in degrees: subtract this day's longitude from the next day's; the remainder is the day's diurnal motion.
121
Procedure to derive the Moon's morning-and-evening scale longitudes: set the day's noon lunar longitude, add that day's evening-quarter additive from the lunar ingress–egress morning–evening ready reckoner, and obtain the lunar longitude at evening quarter. Set the next day's noon lunar longitude, subtract that day's morning-quarter subtractive from the ready reckoner, and obtain the lunar longitude at morning quarter.
122
Procedure to derive the Moon's ingress and egress longitudes: set the day's noon lunar longitude, add that day's Sun–Moon ingress correction from the lunar ingress–egress ready reckoner, and obtain the lunar longitude at ingress. Add that day's Sun–Moon egress correction from the ready reckoner to obtain the lunar longitude at egress.
123
Procedure to derive the star the Moon encroaches: after new moon, reckon from evening-scale longitude to ingress longitude; after full moon, from egress longitude to morning-scale longitude; look up north and south of the ecliptic in the star-image ready reckoners and select any star whose longitude and latitude lie within 1°.
124
竿
Procedure to derive the time: subtract the selected star's longitude from the day's noon lunar longitude, convert to a common denominator, multiply by 24, divide by the lunar diurnal motion (also converted), and obtain the initial proper hour. For the fractional remainder, convert by 60 into parts, multiply by 1000, divide by 144, scale by 100 into quarter-hours, and obtain the time sought.
125
Procedure to derive the vertical separation: subtract the encroached star's latitude from the lunar latitude; the remainder is the vertical separation. If the Moon and star are both south of the ecliptic, the greater latitude is lower separation. If both are north, the greater latitude is upper separation and the lesser is lower separation. If they lie on opposite sides of the ecliptic, a northern Moon is upper separation and a southern Moon is lower separation.
126
Procedure to derive each planet's separation from encroached stars: set the day's planetary longitude and latitude, enter the ecliptic ready reckoner, and select any star whose longitude and latitude lie within 1° of the planet's. Subtract each star's latitude from the planet's latitude; the remainder is the vertical separation.
127
Procedure to derive the Moon encroaching the five planets and mutual planetary encroachment: compare lunar and planetary longitudes and latitudes and record any pair within 1°.
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