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Ch. 2: Minerals: Physical Properties

Ch. 2: Minerals: Physical Properties Page of 515 Ch. 2: Minerals: Physical Properties Text size:minus plus Restore normal size   Mail page  Print this page
PHYSICAL PROPERTIES OF MINERALS..                   89
allel lines, passing through every atom of the crystal. It is also important to remark that this property divides the systems of crystallization into three precise groups,—the tesseral, with single refraction ; the tetragonal and hexago­nal, with double refraction, and monoaxial; the other three systems also double, but binaxial. It is therefore of use to determine the system to which a mineral belongs, but is not of great value as a character for distinguishing species.
Polarization of Light.—Intimately connected with this property is that of the polarization of light, which being more easily and precisely observable than double refraction, is in many cases of higher value as a mineralogical character. By this term is meant a peculiar modification which a ray of light undergoes, in consequence of which its capability of being transmitted or reflected towards particular sides is either wholly or partially destroyed. Thus, if from a transparent prism of tourmaline two thin plates are cut parallel to its axis, they will transmit light, as well as the prism it self when they are placed above each other with the chief axis of both in the same direction. But when the one slip of tourmaline is turned at right angles to the other, either no light at all or verv little is transmitted, and the plates consequently appear black. Hence, in passing through the first slip the rays of light have acquired a pe­culiar property, which renders them incapable of being transmitted through the second, except in a parallel posi-tion, and they are then said to be polarized. The same property is acquired by a ray of light when reflected, at an angle of 35 1/2° (or angle of incidence 54 1/2°), from a plate of glass, one side of which is blackened, or from some other non-metallic body. When such a ray falls on a second similar mirror at an equal angle, but so that the plane of reflection in the second is at right angles to that in the first, it is no longer reflected, but wholly absorbed.
Ch. 2: Minerals: Physical Properties Page of 515 Ch. 2: Minerals: Physical Properties
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