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Reprinted fro~n "The Proceedings of the Indian Academy of Sciences", VoZ. XXXVZZZ, No. 6, See. A , 1953

T H E STRUCTURE AND OPTICAL BEHAVIOUR OF CHALCEDONY

BY

A. JAYARAMAN

(Memoir No. 43 from the Raman Research Institute, Bangalore) Received February 29, 1952

(Communicated by Prof. Sir C. V. Raman, P.R.s., N.L.)

CHALCEDONY

is a cryptocrystalline variety of silica occurring in a massive form and exhibiting a waxy lustre. It is only slightly inferior to quartz in hardness and has a density lying between 2.60 to 2-64. A small per- centage of water may often be found in the material. The refractive index averages at 1.537 and is thus not very different from that of quartz. Thin sections exhibit a fibrous character under the microscope and the material shows a distinct birefringence which is of the same order of magnitude as that of quartz.

Mineralogists formerly regarded chalcedony as a distinct crystalline species of silica and classed it under the orthorhombic system. But the X-ray pattern of powdered chalcedony is identical with that of quartz, as was first reported by Washburne and Naviasl and later confirmed by Rinne,a thus demonstrating that chalcedony is composed of crystallites of quartz.

The fibrous character of the material and the birefringence exhibited by it indicate that the crystallites have preferred orientations. Correns

and

NagelschmidtS showed that such orientation is actually observable in the X-ray patterns of unpowdered chalcedony. The crystallites were found to be orientated around the [1T00] direction in a specimen from Olomuczan and around the [1120] direction in a specimen from Iceland. More recently, Novak4 has reported that the fibres of chalcedony are usually elongated along the c-axis or the a-axis of quartz.

In a recent papefl by Sir

C.

V. R a m n and the present writer in these Proceedings, investigations on the origin of the iridescence exhibited by certain varieties of agate have been reported. By detailed optical and X-ray studies it was shown that the banded structure in iridescent agate responsible for the diffraction effects is

a

result of the orientation of the quartz crystal- lites with their a-axes common and the c-axes lying in the plane of banding

in a

periodic manner. It was thought worthwhile, in this connection, to 441

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