Abstract
On the assumption that the potential energy of the three cubic lattices of the Bravais type consists of two terms, an attractive one proportional tor−mand a repulsive one proportional tor−n,n>m,stability conditions are expressed in the form that two functions of the numbernshould be monotonically increasing. These functions have been calculated numerically forn= 4 to 15, and are represented as curves with the abscissan. The result is that the face-centred lattice is completely stable, that the body-centred lattice is unstable for large exponents in the law of force, and that the simple lattice is always unstable,—in complete agreement with the results of Part I.
References
7
Referenced
142
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Dates
Type | When |
---|---|
Created | 16 years, 9 months ago (Nov. 7, 2008, 10:59 a.m.) |
Deposited | 3 years, 11 months ago (Sept. 19, 2021, 11:31 p.m.) |
Indexed | 1 day ago (Aug. 23, 2025, 9:55 p.m.) |
Issued | 85 years, 4 months ago (April 1, 1940) |
Published | 85 years, 4 months ago (April 1, 1940) |
Published Online | 16 years, 10 months ago (Oct. 24, 2008) |
Published Print | 85 years, 4 months ago (April 1, 1940) |
@article{Misra_1940, title={On the stability of crystal lattices. II}, volume={36}, ISSN={1469-8064}, url={http://dx.doi.org/10.1017/s030500410001714x}, DOI={10.1017/s030500410001714x}, number={2}, journal={Mathematical Proceedings of the Cambridge Philosophical Society}, publisher={Cambridge University Press (CUP)}, author={Misra, Rama Dhar}, year={1940}, month=apr, pages={173–182} }