It will now prove of interest to examine the effects produced by two
plates of opposite varieties of quartz of half this thickness, namely,
3.75 mm. The phenomena are very similar to those just described, but the
rings are a little wider, and the larger area within the innermost ring
is now filled with yellow light instead of violet, when the analyser is
exactly crossed to the polariser. It passes into a bright green when the
analyser is rotated slightly on one side, and into orange when the Nicol
is rotated in the reverse direction. But the most interesting thing of
all is to observe what occurs when these two plates of 3.75 mm.
thickness, one of right-handed quartz and the other of left-handed, are
superposed and placed in contact together as one plate, of double the
thickness, 7.5 mm., at the convergent focus. A beautiful spiral figure
is produced on the screen, composed of the celebrated “Airy’s spirals”
as if the black cross were being reproduced in the central part, but
with each of its bars distorted into the shape of the letter S, as shown
in Fig. 78 at the foot of Plate XV. The contrary effects of the two
opposing rotations are thus extraordinarily indicated visually in the
interference figure afforded by the composite plate.
Now, it is of great practical interest that certain quartz crystals are
found in nature which show Airy’s spirals directly, on cutting a plate
7.5 mm. thick or thereabouts, perpendicular to the optic axis. For
instance, one in the author’s collection of quartzes, a single plate of
an apparently homogeneous and perfectly limpid crystal, shows the
spirals exceedingly well and clearly defined. As a matter of fact, it is
a twin, a right and a left-handed crystal being twinned together with an
invisible plane of composition, which is only revealed on examining the
crystal in polarised light, as will be demonstrated in the next chapter
by the use of parallel polarised light. The fact of such a plate of
quartz affording Airy’s spirals in convergent polarised light is,
however, of itself an excellent proof of the twinning of two crystal
individuals of the opposite varieties.
Now the very shape of these spiral figures suggests screw action of the
molecular structure of the crystals on the waves of light passing
through them, and moreover, of the action of two screws of opposite
directions of winding, one clockwise and the other anti-clockwise, thus
remarkably confirming the supposition that the point-systems of the
structure of the right and left-handed varieties of quartz are of a
helical nature and respectively of opposite modes of winding.
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