An Elementary Text-book of the Microscope: including a description of the methods of preparing and mounting objects, etc.Griffith, J. W. (John William)
Science
An Elementary Text-book of the Microscope: including a description of the methods of preparing and mounting objects, etc.
Griffith, J. W. (John William)
Microscopy
The power of doubly refracting and polarizing is not possessed by all
crystalline bodies, but only those belonging to other than the cubic
system; crystals belonging to this system neither doubly refract nor
polarize light. In all doubly refracting crystals there are one or more
lines or directions in which the light is not doubly refracted. These
are called the optic axes, and sometimes they coincide with the
geometric axis of the crystals, at others they do not; and they may be
regarded as positions or directions of equilibrium of certain molecular
forces existing within the crystal, which, acting in opposition,
neutralize each other.
If light, polarized by the polarizer, be transmitted through thin doubly
refracting crystals, and analyzed by the analyzer, splendid colours will
become visible; and on rotating separately either the polarizer or the
analyzer, at each quarter rotation the colours will change, being
complementary to those at first visible, or such as are requisite with
the first to make white light. We have seen (fig. 19) that white light
consists of seven coloured rays, or of three primary colours--red,
yellow, and blue, which, by superposition, form the others; and thus red
is complementary to green, which consists of blue and yellow, the two
sets of complementary colours appearing and vanishing as the light and
darkness did when the crystals were not used.
These colours are produced by interference. The compound rays of white
light (fig. 30 _l_) passing through the polarizer (_t_) are all
polarized in one plane; the crystal (_d_) depolarizes this light, _i.
e._ doubly refracts and resolves it into two sets of rays polarized in
planes at right angles to each other, forming the ordinary, O, and the
extraordinary ray, E. Each of these two sets of rays is resolved by the
analyzer (_s_) into two other sets, polarized in planes at right angles
to each other; so that in all there are four sets, two in one plane and
two in the other; and, the primary rays of the two sets in each plane
being in different stages or phases of undulation, in consequence of the
retardation of the extraordinary rays, the undulations of certain
coloured rays check and annihilate each other, while the remainder or
complementary conspire and pursue their course, producing the appearance
of colour, this effect being reversed at each quarter-revolution of the
analyzer.
An idea of what is meant by phases of undulation may be obtained by
reference to fig. 29, in which the undulations, _a_, _b_, are in similar
states or phases, and so conspire in action, while the wave _c_ is in a
different phase and half an undulation behind the others; hence it would
check or interfere with either of the other waves (_a_, _b_), the
etherial molecules of the two, which vibrate perpendicularly or at right
angles to the direction of the wave, acting to the same extent and in
opposite directions.
Public-domain text, read in full here on John Shaqi.
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