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In diamond the carbon atoms lie on two interpenetrating face-centred cubic lattices, and each carbon atom of one lattice is surrounded by four carbon atoms of the other arranged tetrahedron-wise.
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Related claim <https://w3id.org/delphi/resource/claim/thompson1917-ch09-10> (same-quantity): The tetrahedral angle, arccos(-1/3) = 109.47°, appears in both: in diamond as the C-C-C bond angle measured here from the refined structure, in Thompson as the angle between the rays of a four-rayed spicule formed at the junction of four equal cells. In the crystal it is a fact of the lattice; in the spicule it is a claim about cell packing that has not been tested on specimens.
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In diamond each carbon atom is surrounded tetrahedrally by four others on two interpenetrating face-centred lattices
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\text{CN}(\text{C}) = 4,\ \angle = 109.47^\circ
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Bragg WH et al., “X Rays and Crystal Structure”, G. Bell and Sons, London (1915); X Rays and Crystal Structure, ch. VIII, p. 108. Scope: Diamond structure.
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Bragg WH, Bragg WL. X Rays and Crystal Structure. G. Bell and Sons, London (1915)
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William Henry Bragg and William Lawrence Bragg
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1915
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First edition, University of Toronto copy.
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Public domain (1915).
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X Rays and Crystal Structure
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Reading copy of X Rays and Crystal Structure
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Page 108 of the reading copy; paragraph 1377 of the normalised text 1915-bragg-book.txt (sha256 61f0ad3ced5e5ea0acb3b9ad17a90be706ce23c8ff5888140b807bea94b3e55d), produced by build/fetch.py and checked by build/check-quotes.mjs. The text itself is not committed.
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the carbon atoms are arranged on two interpenetrating face-centred lattices. Each carbon atom of lattice B is surrounded by four carbon atoms belonging to lattice A, arranged tetrahedron-wise, and vice versa
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William Henry Bragg and William Lawrence Bragg 1915 claim: In diamond each carbon atom is surrounded tetrahedrally by four others on two interpenetrating face-centred lattices
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