Almagest Book IV: Alexandrian Eclipse Triple – Radius of the Epicycle

Continuing on with Ptolemy’s check on the radius of the epicycle, we’ll produce a new diagram based on the positions of the Alexandrian eclipses. However, instead of doing it piece-by-piece as I did when we explored the Babylonian eclipses, I’ll drop everything into a single diagram since we already have some experience and the configuration for this triple is a bit more for forgiving on the spacing:

As with before, the eclipses in order are at A, B, and G.

From the previous post, we determined that arcAB=110;21º of the epicycle and makes a corresponding angle from the center of the deferent (ADB) of 7;42º. Meanwhile, arcBG=81;36º on the ecliptic and produces BGZ=1;21º.

Again, we can ask why the diagram was set up this way. Ptolemy explains:

It is clear that the apogee must lie on arcAB, since it can lie neither on arcBG nor on arcGA, both of which produce an additive effect and are less than a semi-circle.

Again looking at the last post, we noted that the motion from A to B produced a rearwards effect along the ecliptic. Hence, B must be to the right of A. Similarly, B to G had a forwards effect, indicating that G must be to the left of B. Lastly, we could determine the angle between G and A by subtracting BDGGDA and we would find that from A to G should also produce a rearwards effect indicating G should be to the right of A.

The only way we can make these statements true is if apogee lies on arcAB. If we rotated it such that A was to the right of apogee, this would force G to be to the left of A. Similarly, if we rotated things so that B was to the left of apogee, then G would be to the right of B.

So with those three points in their relative positions, we again draw lines from D to each, producing point E where AD intersects the epicycle. We then connect point E to points B and G. Perpendiculars are dropped from point E onto BD and GD producing points Z and H respectively and making right triangles BEZ, EZD, and EHD. Lastly a perpendicular is dropped from point G onto BE producing point Θ and forming right EGΘ.

With all of that out of the way, back to the math!

As with when we did this for the Babylonian eclipses, we’ll be putting everything in the context of a circle drawn about E, Z, and D. And as we saw last time, point H is also on that circle, so let’s just call it circleEHZD from the outset this time.

In this circle, we have EDZ=7;42º. Thus, in this circle where D is on the circumference, the arc opposite it, arcEZ=15;24º. The corresponding chord, EZ=16;4,42p.

Turning our attention to the epicycle, arcAB=110;21º. So the angle it subtends on the circumference of the epicycle, AEB=55;11º1. We can then take the supplementary angle along AD to determine

DEB=180º55;11º=124;49º

Now looking at DEB we now know two of the angles (DEB and EDB) so we can subtract those from 180º to say

EBD=180º124;49º7;42º=47;29º

Next, we’ll create a circle around B, E, and Z to form circleBEZ. On this circle, we have EBZ which we just found, so the arc opposite it is twice of that which is to say, arcEZ=94;58º. Looking up the chord, EZ=88;26,17p, again in the context of circleBEZ.

But again, we already determined EZ in the context of our circle we’ll convert everything to, circleEHZD. This allows us to set up the conversion ratios, to solve for BE, which was the hypotenuse in circleBEZ, in the context of this circle:

BE120p=16;4,42p88;26,17p

BE=120p16;4,42p88;26,17p=21;48,59p

While we’re looking at the ecliptic, we can notice that

ADG=ADBGDZ=7;42º1;21º=6;21º

So in our circleEGZD, arcEH is opposite that meaning it will have twice the measure, so arcEH=12;42º allowing us to head to the chord table to determine EH=13;16,19p, again in the context of circleEGZD.

Now back to the epicycle. Here,

arcABG=arcAB+arcBG=110;21º+81;36º=191;57º

Thus, AEG, being on the circumference is half that measure, or 95;59º. We can then determine DEG=84;01º since it’s the supplement along AD. That allows for us to solve EGD for EGD:

EGD=180º6;21º84;01º=89;38º

Now we’ll create circleEGH since this puts the angle we just found on the circumference. Thus, in the context of this circle, arcEH is twice that angle or 179;16º. The arc that subtends this angle would then be EH=119;59,50p in the context of this circle.

But we want to convert back to circleEHZD. Fortunately, we’ve around found EH in that context, so we can now set up the conversion ratio to help us find GE:

GE120p=13;16,19p119;59,50p

GE=120p13;16,19p119;59,50p=13;16,20p

Recapping, we’ve now figured out EB and GE in the context of circleEHZD.

Again, we’ll return to the epicycle where arcBG=81;36º. Thus, BEG=40;48º.

Next, we’ll draw circleEGΘ. In the context of this circle, arcGΘ=81;36º and the chord, GΘ=78;24,37p.

We can also determine

EGΘ=180º90º40;48º=49;12º

Therefore the arc opposite this angle, arcEΘ=98;24º and its chord, EΘ=90;50,22p.

Now we’ll switch the context from this circle back to circleEHZD by using the chord we’ve found common to both EG2. First let’s do GΘ:

GΘ78;24,37p=13;16,20p120p

GΘ=78;24,37p13;16,20p120p=8;40,20p

Repeating for EΘ:

EΘ90;50,22p=13;16,20p120p

EΘ=90;50,22p13;16,20p120p=10;2,49p

Since everything is now in the context of circleEHZD, we can now subtract

BΘ=BEEΘ=21;48,59p10;2,49p=11;46,10p

Now we’ll check out circleBGΘ. We’ve determined two of the sides of this right triangle (BΘ and GΘ), so we can use the Pythagorean theorem to solve for the third (BG)3:

BG=11;46,10p2+8;40,20p2=14;37,12p

This is the chord we’ll use to finally switch context to the epicycle. For, in the epicycle, arcBG=81;36º and thus its chord, BG=78;24,37p.

So we’ll convert DE using another set of conversion ratios:

DE120p=78;24,37p14;37,12p

DE=120p78;24,37p14;37,12p=643;35,11p

Next, we’ll do the same for GE4:

GE13;16,20p=78;24,37p14;37,12p

GE=13;16,20p78;24,37p14;37,12p=71;11,55p

From this chord, now in the context of the epicycle, we can determine the corresponding arc, arcGE=72;47,10º5.

We’ve already shown that arcABG=191;57º, so the remainder, arcGA (going clockwise) will be 168;3º.  From this, we can subtract, arcGE to determine arcEA=95;15,50º. Again converting to the corresponding chord, EA=88;39,35p.

As with the last set of eclipses, Ptolemy pauses here to note arcAE wasn’t a semi circle and EA wasn’t 120p so the center of the epicycle isn’t falling on this line, indicating this A and E weren’t at apogee/perigee. As such, we’ll need to redraw our diagram, now including apogee (L), perigee (M), and the center of the epicycle (K).

 

We’ll again create the equal products based on Euclid’s Elements III.36, but this time we’ll chose the first eclipse at A instead of point B:

ADDE=LDDM

Here, we can calculate AD:

AD=AE+DE=88;39,35p+643;35,11p=732;14,46p

This gives us everything we need for the left side of this equation. So we can rewrite6:

732;14,46p643;35,11p=471263;37,49p=LDDM

And again based on Elements II.6 we can write:

LDDM+KM2=DK2

So plugging in and rearranging:

DK2=471263;37,49p+60p2=474863;37,49p

DK=689;6,12p

And now we’ll do one last context swap to determine the radius of the epicycle on the context of the deferent:

KM60p=60p689;6,12p

KM=60p60p689;6,12p=5;13,27p

Ptolemy’s value ends up being higher by just enough that he justifies rounding this up to 5;14p, but either way, this is in excellent agreement with the radius we found from the Babylonian eclipse triple.

So I’ll leave things here, and again save the equation of anomaly and position of the mean moon for the next post!


I think today may have been a record day for progress. The four posts that went up today covered almost 8 pages of material! The first one was definitely the hardest and I’d been working on it for a few days, but from these four posts, that was 1.11% of the Almagest right there! However, it was also a marathon day, spending somewhere around 12 hours working today.


 

  1. If you’re following along from Toomer’s translation, he starts switching into demi-degrees. Since this is unnecessary, I’m not going to follow along, but this will result in some minor differences in the values due to rounding differences.
  2. Which was 120p since it’s the diameter.
  3. Ptolemy comes up with a slightly different value of 14;37,10p which isn’t a lot here, but does start making a difference when we calculate DE in the context of the epicycle here in a moment, by 0;0,32p! However, since we’ll be rounding to only the first division in the end, this still won’t make much of a difference.
  4. Due to the aforementioned minor difference, my value for GE is now going to be 0;0,45p different than Ptolemy’s.
  5. Given my values are fairly discrepant from Ptolemy’s now, I couldn’t rationalize adopting his value for this arc, and didn’t feel like looking it up in the chord table, so for full transparency, this is based on modern trig and we’re a full 0;1º off from Ptolemy’s values now.
  6. Due to the large multiplication, the small variances I’ve been picking up from Ptolemy are getting pretty pronounced, but we’ll be taking square roots shortly so they’ll get quite small again.