upper
end by the planes of the rhombohedrons R and—2R, and on the lower end
by the basal pinacoid. In fig. 68 of electric calamine the upper
extremity shows the basis k, two brachydomes o and p, and two macrodomes m and I; while
on the lower end it is bounded by the faces P of the primary form. This
appearance becomes more interesting from the fact that most hemimorphic
crystals acquire polar electricity from heat,—that is, exhibit opposite
kinds of electricity at opposite ends of the crystal.
The faces of crystals are very frequently rendered imperfect by striae, or
minute linear and parallel elevations and depressions. These arise in
the oscillatory combination of two crystal forms, alternately
prevailing through small spaces. The striae, therefore, are in reality
the edges of combined forms. They are very common on quartz, sliorl,
and some other minerals; and frequently indicate combinations where
only a simple form would otherwise appear to exist. The cubes and
pentagonal dodecahedrons of iron