other three, and thus we have the crystal represented by Fig. 69.
In
other cases the crystals are not terminated by pyramids, but by ridges,
as in Fig. 70. In this case the form of the crystals is greatly
altered, and the regularity, to a certain extent, disappears.
If in the regular crystal (Fig. 68) we suppose the prismatic part to be diminished little by little without the form being otherwise changed, then, when