More about Regiomontanus directions
Let us take again the Primum mobile of Placidus. The 1st theme is that of Charles V (Quint) which we have already analyzed. Here we will consider the directions in a more traditional way using the direct teachings of Placidus and Magini. On Magini, we have in the History of Astronomy of the Middle Ages, an entire chapter devoted to the calculation proposed by Delambre, the complete details of which will be seen below on the example of the SA opp MO arc. I give again the theme of Charles V, according to the data of Placidus (Primum Mobile, pp. 59-61: Exemplum Primum Caroli V Austriaci Imperatoris).
https://primarydirections.blogspot.com/2017/04/charles-quint.html
https://primarydirections.blogspot.com/2017/09/carolus-v.html
https://primarydirections.blogspot.com/2018/02/carolus-v-3.html
IOANNIS ANTONII MAGINI PRIMI MOBILIS LIBER NONUS QUI AGIT DE DIRECTIONIBUS pp, 214-232 PROBLEMA XVIII p, 230
We take the direction : ꝏSA C MO.
1) - MAGINI - REGIOMONTANUS
direct
modified from [ Delambre, Hist Astron Moyen Âge, Magini, pp, 486-491 Paris 1819]
Eq for Fig 129 (pl 12) see fig for location and explanation of spherical triangles
Figure 129 is mixed. It represents a state of the sky at the moment when star A' arrives in a situation similar to star A. The reference element for the observer is the horizon OBH. The arc OAA'H is the position circle (or incident horizon) whose pole is PR. PA is the hour angle counted from midnight. When A' reaches the arc OAA'H, A is no longer on the circle; we must therefore imagine its image on the incident circle. Furthermore, EBQ is the equator. T is the pole of RS (or of A'V') and ET the symmetry axis.
The time when opp SA is on the circle of position of MO is 7h 31 33 TU and the initial time is 3h 52 (corresponding to 58.57 Y for the date of death, the 12 September 1558 (OS), so : 1558.72.
h (altitude of the promissor) - H (latitude of the observer) - D (declination of the promissor) –
D' (declination of incident horizon = position circle of promissor) - PH=H -
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PARAMETERS |
24 Fev 1500 | JUL | |
house = pcd |
DIRECTION |
PROMISSOR |
SIGNIFICATOR |
ꝏ SA C MO |
ꝏ SA |
C MO |
long |
226,15 N E |
279,12 S E |
lat |
2,023 |
-2,097 |
☊ (***) |
na |
72,218 |
AR |
224,27 |
280,09 |
dec |
-14,78 |
-25,28 |
h |
23,87 |
-4,26 |
OA |
243,32 |
315,84 |
Dom Campa |
286,71 |
5,27 |
Dom Regio |
280,69 |
8,35 |
Dom Placidus |
279,15 |
6,29 |
Pôle Regio |
12,92 |
50,75 |
Pôle Campa |
12,92 |
50,75 |
Pôle Placidus |
7,30 |
49,26 |
DM D|N |
D |7,216- N |172,784 |
D |63,03- N |116,97 |
DA pôle D|N (Placidus) |
D |1,937- N |30,18 |
D |41,544- N |33,257 |
DA |
19,05 |
35,75 |
SA D|N |
D |70,95- N |109,05 |
D |54,25- N |125,75 |
D Horiz (SA-DM) (min E W) |
63,74 (E) |
8,78 (E) |
temporal hour (*) ꝏ SA (HTn) | C MO (HTd) |
11,83 |
9,04 |
horary distance (**) |
0,61 |
5,58 |
horary angle (TS – AR) from midnight (W from S) |
352,78 |
296,97 |
Azimuth (0-360 W from S) |
352,37 |
306,09 |
ARMC | TSN |
217° 3' 19" |
14h 28' 13" |
latgeo, |
51,05 |
Equ time |
ecliptic |
23,51 |
+ 356° 55' 15" |
Length SU |
1,00 |
Luna motion |
Length MO |
14,61 |
2,34 (for y time + key EQU) |
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One can see hereunder : label of angles, left : value for each equation of angle and right formulas.
PA (horary angle, from midnight)
172,78 || cosP = (sinh-sin Hsin D)/(cosHcosD)
PHA (HAO angle)
-16,71 || TanPHA = sinP/((sinD+cosP)cosH)
PR (pole HAO)
-12,919 || sinPR=sinPHsinPHA
ET (arc meridian/HAO)
169,31 || tanET=cosHtanPHA
H' || H' (incident horizon = pole [ꝏ SA]
12,92 || tanH'=sinETtanH
PAR (position angle)
13,37 || sinPAR=sinH'/cosD
QS, HPR (Az PR)
79,31 || cosQS=sinET
ΔAR' (DA/HAO)
-3,47 || sinΔAR'=tanDtangH'
OTE, HTQ, ETH (equat/HAO angle)
77,08 || tanOTE=cotH/sinET
Eq for Fig 130 (pl 12) see fig for location and explanation of spherical triangles
Figure 130 resembles a sagittal shot of the sky. The element of symmetry is the ETQ equator. Point S is the significator (point A in figure 129) and point R is the promissor (point A' in figure 129). Point Z is the image of point R at the instant when R reaches a position similar to S. AQC is the observer's horizon; ASZC is the position circle of S (incident horizon). PR, PZ and PS are arcs of position of the points R, Z and S. ZV is the boreal [+] declination of Z and OS the austral [-] declination of S. TO is the ascensionnal difference (AR) of S while TV is the ascensionnal difference (AR') of Z. They allow the calculation of the distance OV which must be added or subtracted from the arc KO (difference of the right ascensions of S and Z) to obtain the arc of direction whose the common equation is:
KV = KO - OT - TV
If the OS declination is boreal, OT would change sign; if RK is austral, TV would change sign (adapted from Delambre, History of Astronomy of the Middle Ages, Magini article, p. 490, 1819).
KO (≠AR ꝏ SA C MO)
53,23 || KO=ARꝏ SA - ARC MO
A (AET angle) || EA = 90-H
16,71 || sinA=sinETsinOTE/sinEA
T (angle horizon/OTH) || pole of PRS (=90-H')
77,08 || cosT=sinAETsinH
[-] TO ΔAR' ꝏ SA || D boreal --> sign [-] = switch for [+]
-3,47 || sinTO=tanDcotT
[+] TV ΔAR' C MO || D' boreal-> sign [+] = switch for [-]
-6,26 || sinTV=tanVZcotT
-----------------------------------------------------------------
tasyir || If OS (D) [+], TO ~ sign, If RK (D') [-], TV ~ sign
56,02 || KV=KO – OT – TV
-----------------------------------------------------------------
VZ || D' (declin of C MO)
-25,43
OS || D (declin of ꝏ SA)
-14,78
ST distance ST
-15,17 || sinST=sinD/sinT
TZ distance TZ
-26,13 || sinTZ=sinD'/sinT
ZS ≠dist
10,96 || If D/D'<0 [-]
EPA (EPV, EV) ± ΔAR' horary angle of ꝏ SA
172,78 || if d is [-] ~ ΔAR'
So, the direction is tasyir = 56.02 (Regiomontanus).
we see superimposed the arc of direction with opp SA emanating from SA (at 46.27° ♉), arriving in conjunction with MO at 280° ♑.
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