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Opticks 1717 - Up

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j2di-attion be made<br />

into kvater, the<br />

Sine of Incidence of the red Light-is to the Sine<br />

pfits IXefraCtion as 4 to 3;. If out of Air into Glafs,,<br />

the Sines are as 17 to 11. In Light of other<br />

CoTours the Sines have other .Proportions : hut<br />

t&i &&ye&x is f~ little that !t peed feldom be<br />

&niid&ed I ’<br />

Snppofe therefore, that R S [in Fig. I .I’ reprefents<br />

the Surface of fkgnating Water, and that C<br />

ence in which anyRay coming<br />

ln the Line A c is refleCted or<br />

ould know whither this Ray<br />

exion ‘of Refra&ion : I ere&<br />

e of the Water fi-om the; point<br />

e Perpendicular @ I? and produce<br />

o Q, an&concIudc by the fir@<br />

e Ray after Reflexion and R.eS’<br />

fra&ion, filall be found fomewhere in the Plane<br />

of the Angle of Incidekc A C P produced. I let<br />

fall therefore upqn the Perpendicular C P the<br />

Sine of Ipeidence AD 8 and if the refleCted<br />

?‘kay be defired? I produce AD to’ B f~ that<br />

.bB be equal to A.Dj and draw<br />

il,iile C B ihall be the rei-leAed W<br />

irpf Reflexion BCP and its Sin<br />

gual to the Angle and Sine of Incidence<br />

ought to be by the fecond Axiom. I3<br />

iefiaAei1 Ray be d&red, ‘I produce A<br />

fo that I3 II may be tcr AD as the Sine of Ike-:<br />

@$‘i.jo~~ tcp &e Sine wf Incidence, that is. (if the<br />

.&,g$$; ;;z)gs 3 to 4 ; ~n(l about the ,Center<br />

ane 4 & I? wrth the Radms G A<br />

$zfcpil$g a Circle A H9 E I draw Parallel to’the<br />

Z$erpendq@ C.P Q, the r,ilr,” II E, ctatting tl$<br />

.:<br />

‘CkCuxaz,

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