Geometrical Optics

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Geometrical Optics
A S Archibald Stanley Percival
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We have then/' = Now suppose that the incident rays are parallel, or that p is infinite, K- ' uo = t^-^- or =-/- q oo r 54 GEOMETEICAL OPTICS The point at which incident parallel rays come to a focus is called the Second Principal Focus and is represented by F" in the figure, while the distance F"A is commonly denoted by /" ; so, replacing q' by its technical symbol, we M - Mo It should be noted that /" has the same sign as r, and indeed F" is seen to be on the same side of the surface as C ; F...', however, is on the opposite side, as is obvious from the expression for /' being preceded by a negative sign.
Now, since the effect of a concave surface is to render incident rays more divergent (unless p

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