Minerals in rock sections : $b The practical methods of identifying minerals in rock sections with the microscope, especially arranged for students in technical and scientific schoolsLuquer, Lea McIlvaine
Science
Minerals in rock sections : $b The practical methods of identifying minerals in rock sections with the microscope, especially arranged for students in technical and scientific schools
Luquer, Lea McIlvaine
Petrology -- Laboratory manuals
_Orthorhombic crystals_ show the figures always in two of the pinacoids
and in white light the color distribution will be symmetrical to the
trace of the axial plane and the line through the centre at right angles
to this trace and also to the central point.
_Monoclinic crystals_ show the figures in the clino pinacoid or in
sections at right angles to this. In white light the color distribution
is never symmetrical to two lines, but is symmetrical either to the
trace of the axial plane (_inclined dispersion_[79]), or to the line
through the centre at right angles to this trace (_horizontal
dispersion_), or to the central point (_crossed dispersion_).
_Triclinic crystals_ show in white light figures with distribution of
color unsymmetrical to any line or point.
In white light the “color fringes” of the hyperbola are due to the
“_dispersion_”[79] of the optic axes and bisectrices. That is, for each
color (for light of each wave-length) there is a particular interference
figure; the overlapping of these superposed figures producing the color
fringes.
When the axial angle is larger for red light than for violet, the
dispersion is said to be ρ > ν and the interference figure, in the
position of Fig. 31, will show the hyperbolic curves fringed with red
towards the centre (inside). In general the color with the larger axial
angle is nearer the centre of the field. This is due to the
extinguishing of light of each color at the axial points, the resulting
colors at these points being produced by white light minus the absorbed
color. When the dispersion is ν > ρ the reverse distribution of color
fringes will take place.
By measuring the axial angle in red and blue light, this dispersion of
the optic axes can also be obtained.
RESUMÉ OF THE USES OF PARALLEL AND CONVERGENT POLARIZED LIGHT.
_Parallel_ light is used to detect pleochroism, to distinguish between
isotropic and anisotropic substances, to study interference colors, to
determine the strength of the double refraction, to locate directions of
vibration, to measure extinction angles, to find the directions of
vibration of the faster and slower rays, to determine the relative value
of the indices of refraction of the two rays, and to investigate the
crystal structure in general.
_Convergent_ light is used to distinguish between uniaxial and biaxial
crystals, to determine whether a section that appears to be isotropic is
really so or only perpendicular to an optic axis and to determine the
optical character, grade of symmetry (system), axial angle and
dispersion.
CHAPTER IV.
THE MICROSCOPIC AND OPTICAL CHARACTERS OF MINERALS.
OPAL.
ISOTROPIC. AMORPHOUS.
COMPOSITION: SiO_{2}.nH_{2}O, generally soluble in caustic alkalies.
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