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Then let another Priiili 5) I3 G de& parallel to<br />
the former 9 be placed at X ,’ to refia& that<br />
wllil:e Light upwards towards Y. Let the refiatking<br />
Angles of the l-‘rilills, and their diitances<br />
from t$e Lens be equal,- i;, that the Rays which<br />
cdnverged from the Lens towards X, and without<br />
Refraktion, would there have crofikd and<br />
diverged again, may by the Rcfrafiion of the<br />
fecond priiin be reduced into I’nrakfifk and<br />
diverge no more., For then thok Ra s will recompolfe<br />
a beam of white Light X c ‘. If the<br />
refracrting Angle of either Priiin be the bigger,<br />
that Prifin muff be So much the nearer to the<br />
IL&. You wi1.l know when the Prifms and the<br />
Lens are well fet together, by obkrving if the<br />
beam of Light XY which comes out of the j‘econd’Prifm<br />
be perfeAly white to the very edges<br />
of the Light; and at all diitances from the Priiin<br />
continue perfeAly and totally white like a bcatn<br />
of the Sun’s Light. For till” this happens, the<br />
pofition of the Prifms and Lens to one mother<br />
muit be correkkd, and then if by the help of a<br />
long beam of Wood ,’ as is roprefentcd in the,<br />
Figure, or by a Tube, or fame other frrch Infirument<br />
made for that purpol’e, they be made<br />
MI in that fituation, you may try all the fame<br />
Expenrimentg in this compounded beam ofLight<br />
X Y, which have been made in the Sun’s dire&<br />
Light. For this compounded beam df Light<br />
has the fame appearance, and is cndow’d with<br />
all the fame Properties with a dire& beam of<br />
the’Sun’s Light, fo far as my Obfervatiol~ reaches,<br />
And in trying Experiments in this beam yo’u<br />
may by fiopping any of the Colours p, g, r, I<br />
ad