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On the electrostatic potential energy, and the rhombohedral angle, of carbonate and nitrate crystals of the calcite type
Publication year - 1926
Publication title -
proceedings of the royal society of london. series a, containing papers of a mathematical and physical character
Language(s) - English
Resource type - Journals
eISSN - 2053-9150
pISSN - 0950-1207
DOI - 10.1098/rspa.1926.0047
Subject(s) - calcite , aragonite , crystallography , ion , carbonate , chemistry , lattice energy , crystal (programming language) , crystal structure , lattice (music) , trigonal crystal system , mineralogy , physics , organic chemistry , computer science , acoustics , programming language
1.1. This paper is a sequel to, and an extension of, one with a somewhat similar title by W. L. Bragg and S. Chapman, in which it was shown that, on certain natural assumptions, the rhombohedral angle could be calculated for the well-known isomorphous series of carbonate crystals of the calcite type. The detailed results and the method of calculation were not described. This is done in the present paper, where also the results of a parallel calculation for a similar possible series of nitrate crystals is given; the only known nitrate crystal of this type, however, is that of sodium, the corresponding potassium salt crystallising in the aragonite form. 1.2. As the underlying principles of the method have been described in the paper cited, they need only receive brief mention here. The crystals considered are supposed to consist of positive and negative ions, namely, metallic ions (doubly charged, like Ca++ in the carbonate series, or singly charged like Na+ in the nitrate case), and ionised groups CO3 -- (i. e. , C++ ++ , O-- , O-- , O-- ) or NO3 - (i. e. , N+++ ++ , O-- , O-- , O-- ). The detailed arrangement of these groups is described in § 2.4, but if the CO3 or NO3 groups are treated as wholes, the arrangement of the positive and negative ions is similar to that of the ions in a simple cubic crystal of the rock-salt type, except that the cubic lattice is contracted—into a rhombohedral lattice—parallel to one diagonal; this diagonal thus becomes the trigonal axis of the crystal. The edges meeting in the trigonal axis are inclined to one another at an angle (the “rhombohedral angle”) of about 102°, instead of 90° in the case of rock-salt.

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