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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