Fig. III.]

389. This done, make a Scale of any convenient length as _W_, whereof

each division is a minute of a degree; and take from it in your

Compasses 54 Minutes 50 Seconds, the Sum of Semi-diameters of the Moon

and Earth’s shadow; and with that extent as a Radius, describe that

Circle _OVLG_ round _C_ as a Center.

From the same Scale take 39 Minutes 48 Seconds, the Semi-diameter of the

Earth’s shadow, and therewith as a Radius, describe the Circle _UUUU_

for the Earth’s shadow, round _C_ as a Center. Subtract the Moon’s

Semi-diameter from the Semi-diameter of the Shadow, and with the

difference 24 Minutes 46 seconds as a Radius, taken from the Scale _W_,

describe the Circle _YZ_ round the Center _C_.

Draw the right line _AB_ through the Center _C_ for the Ecliptic, and

cross it at right Angles with the line _EG_ for the Axis of the

Ecliptic.

Because the Moon’s Latitude in this Eclipse is North Descending, § 384,

set off the Angle of her visible Path with the Ecliptic 5 Degrees 38

Minutes (Page 202.) from _E_ to _V_; and draw _VCv_ for the Axis of the

Moon’s Orbit. Had the Moon’s Latitude been North Ascending, this Angle

must have been set off from _E_ to _f_. _N. B._ When the Moon’s Latitude

is South Ascending, the Axis of her Orbit lies the same way as when she

has North Ascending Latitude; and when her Latitude is North Descending,

the Axis of her Orbit lies the same way as when her Latitude is South

Descending.

Take the Moon’s true Latitude 9ʹ 56ʺ in your Compasses from the Scale

_W_, and set it off from _C_ to _F_ on the Axis of the Ecliptic because

the Moon is north of the Ecliptic; (had she been to the South of it, her

Latitude must have been set off the contrary way, as from _C_ towards

_v_:) and through _F_, at right Angles to the Axis of the Moon’s Orbit

_VCv_, draw the right line _LMHNO_ for the Moon’s Orbit, or her Path

through the Earth’s shadow. _N. B._ When the Moon’s Latitude is North

Ascending, or North Descending, she is above the Ecliptic: but when her

Latitude is South Ascending, or South Descending, she is below it.

Take the Moon’s true horary motion from the Sun, _viz._ 28 Minutes 22

Seconds, from the Scale _W_ in your Compasses; and with that extent make

marks in the line of the Moon’s Path _LMHNO_: then divide each of these

equal spaces into 60 equal parts or minutes of time: and set the hours

to them as in the Figure, in such a manner that the precise time of Full

Moon, as shewn by the Tables, may fall in the Axis of the Ecliptic at

_F_, where the line of the Moon Path cuts it.

Lastly, Take the Moon’s Semi-diameter 15 Minutes 2 Seconds from the

Scale _W_ in your Compasses, and therewith as a Radius describe the

Circles _P_, _Q_, _R_, _S_, and _T_ on the Centers _L_, _M_, _H_, _N_,

and _O_; the Circles _P_ and _T_ just touching the Earth’s Shadow _UU_,

but no part of them within it; the Circles _Q_ and _S_ all within it,

but touching at its edges; and the Circle _R_ in the middle of the

Moon’s Path through the shadow. So the Circle _P_ shall be the Moon

touching the shadow at the moment the Eclipse begins; the Circle _Q_ the

Moon just immersed into the shadow at the moment she is totally

eclipsed; the Circle _R_ the Moon at the greatest obscuration, in the

middle of the Eclipse; the Circle _S_ the Moon just beginning to be

enlightened on her western limb at the end of total darkness; and the

Circle _T_ the Moon quite clear of the Earth’s shadow at the moment the

Eclipse ends. The moments of time marked at the points _L_, _M_, _H_,

_N_ and _O_ answer to these Phenomena: and according to this small

projection are as follow. The beginning of the Eclipse at 8 Hours 36

Minutes _P. M._ The total immersion at 9 Hours 42 Minutes. The middle of

the Eclipse at 10 Hours 26 Minutes. The end of total darkness at 11

Hours 12 Minutes. And the end of the Eclipse at 12 Hours 18 Minutes; but

the Figure is too small to admit of precision.

[Sidenote: The examination of antient Eclipses.]

390. By computing the times of New and Full Moons, together with the

distance of the Sun and Moon from the Nodes; and knowing that when the

Sun is within 17 Degrees of either Node at New Moon he must be eclipsed;

and when the Moon is within 12 Degrees of either Node at Full she cannot

escape an Eclipse; and that there can be no Eclipses without these

limits; ’tis easy to examine whether the accounts of antient Eclipses

recorded in history be true. I shall take the liberty to examine two of

those mentioned in the foregoing catalogue, namely, that of the Moon at

_Babylon_ on the 19th of _March_ in the 721st year before CHRIST; and

that of the Sun at _Athens_, on the 20th of _March_, in the 424th year

before CHRIST.

The time of Full Moon for the former of these Eclipses is already

calculated, Page 198, and the time of New Moon for the latter, Page 196,

both to the _Old Style_; so that we have nothing now to do but find the

Sun’s distance from the Nodes the same way as we did the Anomalies; and

if the Full Moon in _March_ 721 years before CHRIST was within 12

degrees of either Node, she was then eclipsed; and if the Sun, at the

time of New Moon in _March_ 424 years before CHRIST was within 17

degrees of either Node, he must have been eclipsed at that time.

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