Light entering a pinhole camera with a pinhole aperture of diameter $d$ forms an image on the back surface, a distance $L_2$ away, as in Fig. 11.61:
(a) By using geometrical arguments, show that a point source a distance $L_1$ from the pinhole, forms an image of dimension $\Delta=\left[\left(L_1+L_2\right) / L_1\right]$, which is $\simeq d$ for the usual case of $L_1 \gg L_2$.
(b) What is the improvement in the resolution of the human eye over a pinhole eye with $d=1 \mathrm{~mm}$ ?
(c) Let us say $d$ was made small enough so the resolution of the human and pinhole eye were the same. How much more light would be transmitted by the human lensing system? (If the pinhole were really that small, the transmitted light would diffract much and the imaging would, in fact, be very poor. Still, this illustrates that the human lensing system improves both resolution and light throughput over the pinhole analog.)