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Opticks 1717 - Up

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--<br />

the Objc& at 4 is f0 1llUch bi@$r -01 ldkr tRaP,<br />

~lle Obje& it felf at Q as the dlitance of the<br />

Image at ‘from the kens A13 is bigger or l&s<br />

tlla11 the x iitalice of the Objet% at Q from rhe ’<br />

fame Lens. And if the Obje& be ken througki<br />

tj570 or more fuch Convex or Concave--glaiEs,<br />

every Glafs hall make a new Image? and the<br />

C&j& fhall appr in the place and of the bign&i<br />

of the la11 Image. VVhich confideration un..+<br />

folds the Theory of,h%crolcopes and a’elefcopes.<br />

B;or that Theory confiits ‘in ahnoit nothing elk<br />

than the deicribing iiuA1 GlaiTes as fllall make<br />

E-he plait; Image of any Objekt ~ as difiir& ana<br />

large and luminous as it can convenient2y b,e<br />

made.<br />

I have now given in Axioms and their Explications<br />

the fumm of what hath hitherto been<br />

treated of in <strong>Opticks</strong>. For what hath been generally<br />

agreed on I content my felf to a&mc<br />

under the notion bEPrinciples, in order to wh&,<br />

1 have farther to write. An,d this may f$%ce<br />

for an Irkrodu&ion to Readers of q&Air %Vit<br />

and good Underftanding not yet verfi-d in Oyticks<br />

: Although thofe ,who are already acquain-,<br />

ted with this Science, and have handled C&&es,<br />

w-ill more readily apprehend what followeth.

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