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8<br />

be to the Sine of Refrafiion as I to R : the Rays<br />

which come parallel to the Axis of the Glafs,<br />

fllall in the place where the Image of the CbjeA<br />

is In& &fiinCtljr made, be fcattered all over a<br />

#i7 *<br />

little Circle ~hofe diameter r’s iI x $ very.<br />

c .<br />

nearly, as.1 gather by computing the Eirrors of<br />

the Rays by the method of infimte~,~erres, and<br />

rej&ing the Terms whofe Quantrties are inconfiderabled<br />

As for inilancs, if the Sine of<br />

Incidence I4 be to the Sine of Refrac%on R, as,<br />

20 to 313. and if D the diameter of the Sphere<br />

to which the convex fide of the Glafs is ground,<br />

be xoo Feet or 1200 Inches, and s the iemidia-S<br />

meter of the Aperture be two Inches, the dia-<br />

., R-L: :t Y cd.<br />

meter of the little Circle (that .K ,qizTqq ) w7i11<br />

y%~rxX<br />

‘be --( Of<br />

ZC%ZO x 1200 x 1200<br />

$E&) ~ parts of 911 hch..<br />

But the diameter of the Iittlc Circle *through<br />

which thefe Rays are icattered by unequal Red<br />

frangibility, kill be about the 55th part of the<br />

Aperture of the Objefl-glafs which hcrc is four<br />

Inches. And therefore the k’~ror arifing from<br />

the fpherical Figure o? the Flak, is to the Krror<br />

arifing from the diflerent Kcfrangibiliry of<br />

961’<br />

he Rays, as so= $0 & that is as;x to f+Lt9;:<br />

and therefore being in comparifou fo ver; little,<br />

deferves not to be contidered,<br />

But you will iky, if the Errors caufed by the<br />

different Refrangibility be fo very .grcnt, how<br />

comes it to gafs tlyat Ob&je&s a pear through<br />

Telefcopcs, fo diitinCZ as they do, 7 I anfwer, ‘tis<br />

2<br />

becaufe

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