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t;ure ‘of 2;. Inches, s about x20 tiims,<br />
with as much diEn&nefs as OIE of a Foot in<br />
.BengtIl; with f of an Itich aperture, magnifies<br />
xj- times.<br />
l\aow were it not for this different Refi-angibility<br />
of Rays, Telekopes might be brought to<br />
a greater perfe&ion than we have yet defcrib’d,<br />
by compofing the ObjeA-Glafs of two (r;rla&<br />
with Water between thcrn. Let .A.DI;‘C[in .F&”<br />
28.1 reprelent the Obje&-glafs ~OIllpOfd of two<br />
Glafftes ABED and BEFC, alike convex on the<br />
outfides ACD and C I-IF, and alike concatre<br />
on the infides-B ME, B NE, with IVater in<br />
the concavity 13 bdEp\;T. ket the Sine of I[ncidence<br />
out of Glafs into Air be as I to R, and<br />
out of Water into Air as K to 14, and by COII-<br />
Sequence out of Glafs into Water , as I to M ‘:<br />
and let the diame of the Sphere to which the<br />
convex iides AG and C 111 II; are ground be<br />
D, and the dismeter of the Sphere to which<br />
the concave fides I3 .M lei: & I3 NE are wound<br />
be t@D, as the Cube Root of R K-K ,, t to the<br />
Cube Root of R K---!&I: ,and the RcfiacCEions<br />
on the concave ficles of theGMTcs, will very<br />
much cosseA the Errors of the RckaAions on<br />
the convex fides, fo fizr 3s they arife Corn r:hc-<br />
Cphericalnefs of the Figure. And by this 1n~a11s<br />
might Telekopes be brought to M~cIcI~I~ per-<br />
%ec(tion, were it not for the difkm~t ,Ij.cft*nngibility<br />
of Several forts of Knys. But I+ j*catbll<br />
of this different RefrangiMity, I do not yet fee<br />
any other means of impfov3ilGg Tclefccjpcs by<br />
Mefia&ions alone than that of incseafing their<br />
kngths, for which end the late Contrivance of<br />
$Ykgcrriw<br />
1