Astronomia Britannica exhibiting the doctrine of the sphere, and theory of the planets decimally by trigonometry, and by tables : fitted for the meridian of London ... / by John Newton ...

About this Item

Title
Astronomia Britannica exhibiting the doctrine of the sphere, and theory of the planets decimally by trigonometry, and by tables : fitted for the meridian of London ... / by John Newton ...
Author
Newton, John, 1622-1678.
Publication
London :: Printed for the author by R. and W. Leybourn, and are to be sold by Thomas Piercepoint ...,
1657.
Rights/Permissions

To the extent possible under law, the Text Creation Partnership has waived all copyright and related or neighboring rights to this keyboarded and encoded edition of the work described above, according to the terms of the CC0 1.0 Public Domain Dedication (http://creativecommons.org/publicdomain/zero/1.0/). This waiver does not extend to any page images or other supplementary files associated with this work, which may be protected by copyright or other license restrictions. Please go to http://www.textcreationpartnership.org/ for more information.

Subject terms
Astronomy -- Early works to 1800.
Planetary theory -- Early works to 1800.
Astronomy -- Mathematics -- Early works to 1800.
Cite this Item
"Astronomia Britannica exhibiting the doctrine of the sphere, and theory of the planets decimally by trigonometry, and by tables : fitted for the meridian of London ... / by John Newton ..." In the digital collection Early English Books Online. https://name.umdl.umich.edu/a52255.0001.001. University of Michigan Library Digital Collections. Accessed May 12, 2024.

Pages

CHAP. 9. Of the Theory and Motion of the Moon.

THe Moon according to our Hypothesis is a secondary planet, mo∣ving about the earth, as the earth and other planets doe about the Sun, and so not onely the earth, but the whole Systeme of the Moone is also carryed about the Sun in a yeare, And hence according to Hypparchus there ariseth a twofold, but according to Tycho a threefold inequality in the Moons motion. The first is periodicall, and is to be obtained, after the same manner, as was the excentrique Equation of the Sun or Earth; in order whereunto her middle motions should be first stated, the which Bullialdus by the rules delivered in the fourth and fifth Chapters preceding hath for the Meridian of Uraniburge determined to be as followeth.

From the Equinoctiall to the beginning of the Christian Aera, the

Moons middle motion was135d.16′27″
The Meane Anomalie355518
And the Radix of her latitude3662956

These then we will take for granted, until there be a more exact, and true Geometrical way propounded to us,; onely we will convert them into Decimall numbers, and reduce them to the Meridian of London.

Page 99

From the Equinoctial to the beginning of the Christian Aera, The Moons middle motion in decimal numbers at Uraniburge was 135. 27417

For the Difference of Merid. adde
. 45750
The Moons mean longitude at London
135. 73167
The Meane Anomaly,
At Uraniburge
355. 08833
Differ. Merid. adde
. 45361
Mean Anomaly at London
355. 54194
The Radix of Latitude
At Vraniburge
366. 49889
Differ. Merid. adde
. 45944
Latitude at London
366. 95833 d.
The Diurnal Motion of the Moons
Mean longitude
13. 17639
Anomaly
13. 06500
Latitude
13. 22944
The Annual Motion.
In longitude
129. 38389
Anomaly
88. 71889
Latitude
148. 71278

According to which limitations of the Moones middle motions, we have composed our Tables, by help whereof and the Semi-excentricity of the Moons Orbe, which according to Bullialdus is 4362 the Moons excentrique equation, or place first equated may be found, as before was shewed in the Sun. Save onely that here the Moons Anomaly is given without subtraction.

Example.

Anno 1587, August 17 ho. 19. 41667 in the apparent time, or ho. 19. 28973 in the middle time, the Moon being in the meridian of Vraniburge noble Tycho observed her in 26 deg. 38333 of Gemini with latitude 5 deg. 23333 S. from which middle time if you subtract 83333 for the difference of the meridians of London and Vraniburge, the time in our meridian is, ho. 18. 45640.

And the Suns true place
154. 07347.
The Suns distance from the Earth
100895.
The Logrithme of that distance
5. 0038707

The Moons middle motions for the same time are as here you see them.

Page 100

Time given☽ Longitud☽ Anomaly☽ Latitude
Years 1500072. 88194313. 06916017. 17805
80174. 24805158. 80139281. 61167
6069. 4802818. 37750185. 50583
Iuly27. 39555249. 77639284. 62194
Dyes 1610. 82222209. 0972211. 66944
H••••res 189. 882229. 798619. 92222
Paris 4564. 2501. 24848. 25152
Mean Longitude810. 960771126. 11125990. 76067
Dedct720.1080.720.
There rests90. 9607746. 11125270. 76067

The Moones meane Anomaly 46. 11125 is the angle A M E in the preceding Ellipis, or the summe of the angles M E H and M H E. Therefore in the triangle M E H we have given, 1. The side M E 200000. 2. The side M H 8724. 3. The angle E M H the complements of the Moones Anomaly, to find M E H, whose double, is the excentrique E∣quation M B H. I say then,

As the summe of M E and M H208724 co. ar.4. 6804276
Is to their difference1912765. 2816605
So is the tang. half summe of the opposite angles,23. 055629. 6290228
To the tang halfe diff.21. 307869. 5911109
Differ.1. 74776 is the angle M E H 

Differ▪ doubled 3. 49552 is the angle M B H or the equation sought which being subtracted from the Moons mean longitude, because the Anomaly is lesse then a semicircle you shall have the Moones place first equated.

Example.
The Moones meane longitude
90. 96077
Equation subtract
3. 49552
The Moones place first equated
87. 46525

And to find her distance from the Umbilique point at H.
As the sine of M B H3. 49552 co. ar.1. 2148808
Is to the side M H87243. 9407156
So is the Sine of B M H46. 111259. 8577468
To the side B H1031205. 0133432

Page 101

But whilest the Moone is thus making her owne periodicall revoluti∣on, her whole Systeme is by the motion of the Earth removed from the proper seats thereof, whence there ariseth another revolution which is called Synodicall, the beginning whereof is the line which passeth through the center of the earth to the Sun, and therefore the Moone in that line is void of this second inequality, which is both at the Conjunction and op∣position, but being in or about her quarters, where she is farthest removed from the said Zyzigiacal line the angle of her evection is 2 deg. 50′ as is cleerely proved by the observations of Tycho and Bullialdus, whose me∣thod we follow, in our calculation of this inequality of the Moon, ma∣king 4362 the sine of the greatest evection to be the Diameter K D in the little circle K C D H. The motion of this libration of the Moone must be measured by her double distance from the Sun, because she is void of this inequality at her conjunctions and oppositions as was said before.

Now then let the angle M H B represent the Moones equated Anoma∣ly, found by subtracting the former Equation from the simple Anomaly, which is 46. 11125

Aequation subtract
3. 49552
Aequated Anomaly
42. 61573

[illustration]

    Page 102

    And if from the place of the moon first equated
    87. 46525
    You subtract the Suns true place
    154. 07347
    Their distance is
    293. 39178
    The double distance
    226. 78356

    is the arch K C D H and drawing the lines F H and H K there shall be made the equicrurall Triangle H F K, whose exteriour angle H F D is known, viz. the excesse of the Sun and Moons double distance above a se micircle 46. 78356. The halfe whereof is the angle D K H 23. 9178, e∣qual to the angle A H G, which being subtracted from the Equated A∣nomaly A H B 42. 61573. The angle G H B or the Synodical Anomaly will be 19. 2239, whose complement to a semicircle is the angle B H K 160. 77605. The side H B 103120 as before, and the side H K may be found in this manner. The arch H V K is the complement of the double distance of the Sun and Moon to a whole circle 13. 21644 the subtense of this arch is H K, H V the halfe arch is 66. 60822, and H X is the right sine thereof.

    Now then, As the Radius,  
    Is to the Diameter K D462.3. 6396857
    So is the sine of H V or H X66. 608229. 9627533
    To the Subtense H K40033. 6024390
    Therefore in the Triangle B H K we have known,
    1. The angle B H K160. 77605. 
    2. The side H B103120 To find the angle H B K. 
    3. The side H K4003 To find the angle H B K. 
    As the summe107123 co. ar.4. 9701173
    To the differ.991174. 9961481
    So tang. ½ the opposite ang.9. 611979. 2287638
    To the tang. ½ differ.8. 905029. 1950292

    Their difference 0. 70695 is the angle of the evection, H B K to be added if the Synodicall Anomaly be more then 180, and to be sub∣tracted from the place of the Moone first equated when lesse, as here it is in our example, and therefore to be subtracted from the Moons place 87 46525, and then her place secondly equated will be 86. 7830.

    And according to this Analogie may be made a table of the Moons e∣vection, when she is in quadrature or 90 degrees distant from the Sun; for then the equated and Synodicall Anomalies are both the same, and therefore in the Triangle E M H we have give the angle E H M, or the e∣quated

    Page 103

    Anomaly which suppose 25 degrees, the side M H 8724 and the side H E 00000, to find the angle at E.

    [illustration]

    As the sum of H E and M H208724 co. ar.4. 6804276
    Is to their difference1912765. 2816605
    So is the tang. half summe 10. 6542447
    To tang. half differ.76. 4043510. 6163328
    Their differ.1. 09565 is the angle M E H 
    Whose double is2. 19130 is the angle M B H 
    Then as the sine of M B H2. 1913 co. ar.1. 4175273
    To the sine of B M H27. 19139. 6598808
    So is the side M H. 87243. 9407156
    To the side B H10. 41615. 0181235
    or the Moons distance from the umbilique.  

    Hence in the first Diagram of this Chapter, in the Triangle B H K we have given A H B the equated Anomaly, 25 degrees, the Moons di∣stance H B 104161, with the side H K, or rather D K, the Diameter of the little circle 4362, to find the angle H B K.

    Page 104

    As the summe of H B and H K108523 co. ar.4. 9644782
    To their difference997994. 9991262
    So is tang. halfe summe12. 509. 3447552
    To tang. halfe differ.11. 523149. 3093596

    whose difference . 97686 is the evection sought and by Bullial∣dus . 97805 which is so little differing from what we have found, that I have taken his Table and converted it into Deci∣mall numbers.

    And for the finding the part proportial between the quadrature and the Zyzygia, Bullialdus whom we follow, hath annexed scruples of pro∣portion in this manner.

    As Radius to 60 minutes or one degree; so is the fine of halfe the de∣grees of the equated Anomaly to the scruples of proportion required.

    But this proportion in the Sexagenary Canon will not give the scruples either so easily or so exactly as the Decimal Canon will, because the seconds must still be found in that Canon by the part proportional, which in the beginning of the Canon cannot be true, but working by a Decimal Canon the natural sines of halfe the degrees, are the Decimall parts required, as the naturall sine of 4 degrees; 069756, are the Decimall parts for 8 degrees of equated anomaly, and so of the rest.

    Having done with the first and second inequalities of the Moon, we come to the third which Tycho calls the variation, Bullialdus the Reflecti∣on for as the Moons Systeme is carryed about by the earth, the place of her Apogaeon is changed, or doth reflect contrary to the succession of the Signes, by reason of which reflection the angle of her Evection is some∣times more sometimes lesse then it will be found by the former directions, but the quantity of this variation according to Tycho doth never exceed 40′ 30″ or in Decimal numbers 67500, to be added to or subtracted from the place of the Moone secondly equated, and the proportion by which he finds it is thus,

    As the Radius

    To the sine of the complement of the double distance of the Sun and Moon if lesse then a Semicircle: To the excesse if more:

    So is the sine of the greatest variation, or Reflection.

    To the variation required, which is to be added to the Moons place, secondly, equated if the double distance be lesse then 180 deg. to be sub∣tracted, when it is more.

    Page 105

    Therefore in our Example,
    As the Radius  
    To the sine of H F D46. 783569. 8625917
    So is the sine of675008. 0711591
    To the variation491897. 9337508

    The Moones place secondly equated
    86. 75830
    Variation subtract
    49189
    The Moones place in her Orbe
    86. 26641

    Lastly, to find the Moones latitude and place in the Ecliptique, take the middle motion of her latitude for the time propounded, the which rejecting the whole circles is 270. 76067 and in which according to Tycho there is a twofold variation, The first is occasioned by the various intersection of the Moones orbe with the Zodiack, and the o∣ther by the reciprocal progression and retrogradation of the Nodes. In the New and Full Moones the limits of her greatest latitude, are 4. 97500, but in her quarters 5. 29167, as Tycho hath experimented by many dili∣gent and accurate observations, whose method of calculation is as fol∣loweth.

    From the meane motion of the Moones latitude
    270. 76067
    Subtract the Moones absolute Equation
    4. 694 6
    The Equated latitude of the Moon
    266. 06631

    Then to find the Equation of the Nodes, let the line A D or the angle A T D 5. 13333 represent the meane inclination of the Moones Orbe with the Ecliptique, let the least inclination be represented by A B 4. 97500, and the greatest by A C 5. 29166. And from the distance of the Sun and Moon before found,

     
    293. 39178
    Subtract the evection and variation
    ••••1. 9884
    True distance of the Sun and Moon
    292. 1994
    The double thereof is
    224. 3858

    which being numbred from B by C to F in the Triangle F D A we have known A D 5. 13333 the meane inclination of the Moones Orbe. 2. D F 15833 the halfe difference of the least and greatest inclination. 3. With the angle F D A 135. 61412, the complement of the double di∣stance of the Sun and Moon to a whole circle: whence to find the angle F A D the Aequation of the Nodes, by the Doctrine of spherical Triangles say,

    Page 106

    [illustration]

    First, As the Radius  
    To the cosine of F D C44. 385889. 8540905
    So is the tang. of D F158337. 4413175
    To the tang of D C113217. 2954080
    Adde the arch A D5. 13333 
    Summe is A C5. 24654 
    2 As sine D C11321 c. ar.2. 7046002
    To the sine A C5. 246548. 9611430
    So cotang. F D C44. 3858810. 0093107
    To cotang. F A D1. 2106211. 6750539
    From the Moones latitude equated 266. 06787
    Equation Nodes subtract 1. 21062
    True motion of the Moones latitude. 264. 85725
    whose complement to a whole circle 95. 14275

    Page 107

    And to find A F or the angle of 〈◊〉〈◊〉 A T , the 〈…〉〈…〉 of the Sun and Moone being more than 180 degrees, and lesse th•••• ••••••▪ I deduct the Moones double distance 224 d. 3858 being numbred •••• the little circle, from B by C to F, from the Arch B C F G 270, there re∣maines F G 45. 61412, and then the Aalogie is,

    As the Radius D C 10. 0000000
    To the sine of F G or D F45. 614129. 8540305
    So is the sine of the arch, D C. 158337. 4413159
    To the sine of the arch D E. 113197. 2953464

    The aggregate is B E . 27152 which being added to the least angle of inclination A T B, or the arch A B 4. 97500 the present inclina∣tion is A F or the angle A T F 5. 24652.

    Hence to find the Moones true latitude, I say,
    As Radius 10. 0000000
    To the sine of A T F5. 246528. 9611413
    So is the sine of A T84. 857259. 9982481
    To the sine of A F5. 225338. 9593894
    or the angle A S F.  

    And by these Analogies may be made the Table of the Moons latitude wc we have borrowed of Tycho, converting it onely into Decimall numbers.) For supposing the Moon to be in her Syzygial points, the angle of Incli∣nation is alwayes A T B 4. 975, and then her latitude for every degree of her true motion of latitude may be found by the last Analogie; As Radius

    Example.

    To the sine of A T B4. 9758. 9381242
    So is the sine of A T45.9. 8494850
    To the sine of A B3. 515648. 7876092

    And her latitude when she is in Quadratue or 90 degrees distant from the Sun may be found by the same analogie, if you make the angle of In∣clination A T C 5. 29166.

    Example.

    As Radius  
    To the sine of A T C5. 291668. 9648517
    So is the sine of A T45.9. 8494850
    To the sine of A F3. 739108. 8143367

    Subtract A B 3. 51564 there rests the Excesse to be placed in the Table 0. 22346.

    The proportipnal part of which excesse to be added to the Moones la∣itude

    Page 108

    must be found by scruples of proportion, and the Scruples themselves for every degree of the Moones distance from the Sunne may thus be had.

    [illustration]

    As Radius▪  
    To the Coine of the Moones double distance D H409. 8842539
    So is the sine of D B0. 158337. 4413575
    To the sine of D H0. 121427. 3256114
    Their differ▪ is B H0. 03691 
    Then as the Diameter B C316665. 4994068
    Is to the Diameter B C100. 0005. 0000000
    So is B H0. 036913. 5671440
    To B H0, 116564. 0665508

    Or more readily thus D H 76604 is the sine of 50 or the Cosine of 40 the Moones double distance from the Sun, which being deducted from Radius, the remainder is the versed sine B H 23396 the halfe 11698, are the scruples of proportion answering to 20 deg. of the Moones single di∣stance from the Sun,

    From the Moones place in her Orbe
    86. 26641
    Subtract the Moones true latitude
    264. 85725
    The Moones Node ascending
    181. 40916

    Lastly, for her Reduction▪

    Page 109

    As Radius  
    To the Cosine of A T F5. 247759. 9981757
    So tang. of A T84. 8572511. 0458587
    To tang. of T F84. 8368911. 0440344

    Difference 02036 is the Reduction sought
    From the place in her Orbe
    86. 26641
    Subtract her Reduction
    . 02036
    The Moones place in the Ecliptique
    86. 24605
    Do you have questions about this content? Need to report a problem? Please contact us.