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~xwer tA the Obje 11 the Focus of the<br />
leai? refrangible ones 9 by about the s?f-th part<br />
of the difiarlce between the Obje&-glafs and the<br />
Focus of the mean sefiangiblc ones.<br />
And if Rays of all forts, flowing from ally<br />
one lucid point in the Axis of any umvex Lens,<br />
bc made by the Refra&ion of the kens to tollverge<br />
to points not too reniot~ fro111 the Lens,<br />
the FOCUS of the inoft refrai-rgible Rays ihall be<br />
nearer to the Lens than the FOCUS of the leafi<br />
refrangible ones , by’s dii’cance which is to the<br />
274th part of the difiance of the ~‘QCUS of the<br />
mea11 refrangible Rays from the LcnS as the difhnce<br />
bem7ee11 that Focus and the luc.id oint<br />
from whence the Rays flov7 is to the dii P Aance<br />
between that iucid point and the Lens very’ ‘<br />
amine whether the difference be-’<br />
fra&tions which the moit &km& !<br />
blc and the kafi refrangible &I’ s flow~.~~g~i-om<br />
the fame point fuffeer in the C Y bjecd’c-glalks~ of<br />
Telefcopcs and fuch like GMIks, be .6 great a$’<br />
is here d’efcribcd, E contrived the fol.lowingE&<br />
periment.<br />
Expr. 16 The Lens which X wkd in the fe,<br />
eond and eighth Experiments, being pln~d iix<br />
Feet and an I& diitant from any OlrjcA, c&<br />
&Aed the Species qf that Obje& by the mean<br />
refrangible Rays at the dii?ance of Gx :I/‘Icct aa&<br />
cl1 Inch from the LenB on the otk3 Me. Ancf<br />
therefore by the foregoing Rule it ought to CC&~<br />
le& the Species of that ObjeB by the lc:zit se-f<br />
fialigible Rays ‘at the diftalrce of iix V’cer amt.<br />
3-i- Inches fi:om the Lens, qd by the rnoit I+<br />
fmgi blc