The Herbert-Smith Refractometer. There is on the market an instrument called the Herbert-Smith refractometer, by means of which anyone with a little practice can read at once on the scale within the instrument the refractive index, as it is called, of any precious stone that is not too highly refractive. (Its upper limit is 1.80. This would exclude very few stones of importance, i. e., zircon, diamond, sphene, and demantoid garnet.)
Those readers who wish to make a more intensive study of the construction and use of the refractometer will find a very full and complete account of the subject in Gem-Stones and their Distinctive Characters, by G. F. Herbert-Smith, New York; James Pott & Co., 1912. Chapter IV., pp. 21-36. The Herbert-Smith refractometer is there described fully, its principle is explained and directions for using it are given. The price of the refractometer is necessarily so high (duty included) that its purchase might not be justified in the case of the smaller retailer. Every large dealer in colored stones, whether importer, wholesaler, or retailer, should have one, as by its use very rapid and very accurate determinations of stones may be made, and its use is not confined to unmounted stones, for any stone whose table facet can be applied to the surface of the lens in the instrument can be determined.
LESSON III
DOUBLE REFRACTION
Explanation of Double Refraction. In [Lesson II.] we learned what is meant by refraction of light. While glass and a small number of precious stones (diamond, garnet, and spinel) bend light as was illustrated in [Fig. 1], practically all the other stones cause a beam of light on entering them to separate, and the path of the light in the stone becomes double, as shown in [Fig. 2].
This behavior is called double refraction. It may be used to distinguish those stones which are doubly refracting from those which are not. For example, in the case of a stone which is doubly refracting to a strong degree, such as a peridot (the lighter yellowish-green chrysolite is the same material and behaves similarly toward light), the separation of the light is so marked that the edges of the rear facets, as seen through the table, appear double when viewed through a lens. A zircon will also similarly separate light and its rear facets also appear double-lined as seen with a lens from the table of the stone. The rarer stones, sphene and epidote, likewise exhibit this property markedly. Some colorless zircons, when well cut, so closely resemble diamonds that even an expert might be deceived, if caught off his guard, but this simple test of looking for the doubled lines at the back of the stone would alone serve to distinguish the two stones.
