2023-Sustainable Industrial Processing Summit
SIPS2023 Volume 13. Intl. Symp on Physics, Mathematics and Multiscale Mechanics

Editors:F. Kongoli, A. B. Bhattacharya, A.C. Pandey, G. Sandhu, F. Quattrocchi, L. Sajo-Bohus, S. Singh, H.S. Virk, R.M. Santilli, M. Mikalajunas, E. Aifantis, T. Vougiouklis, P. Mandell, E. Suhir, D. Bammann, J. Baumgardner, M. Horstemeyer, N. Morgan, R. Prabhu, A. Rajendran
Publisher:Flogen Star OUTREACH
Publication Year:2023
Pages:298 pages
ISBN:978-1-989820-96-4 (CD)
ISSN:2291-1227 (Metals and Materials Processing in a Clean Environment Series)
CD-SIPS2023_Volume1
CD shopping page

    DYNAMICS FRENKEL-KONTOROVA MODEL

    Alexander Filonov1; Lyudmila Kveglis2; Artur Abkaryan2; Evgeniy Artemyev2;
    1INSTITUTE OF NONFERROUS METALS AND MATERIALS SCIENCE SIBERIAN FEDERAL UNIVERSITY KRASNOYARSK PR. IMENI GAZETY KRASNOYARSKII RABOCHII 95 RUSSIAN FEDERATION, Красноярск, Russian Federation; 2INSTITUTE OF ENGINEERING PHYSICS AND RADIOELECTRONICS, SIBERIAN FEDERAL UNIVERSITY, Krasnoyarsk, Russian Federation;
    Type of Paper: Regular
    Id Paper: 481
    Topic: 38

    Abstract:

    In order to develop the FK model, the DFK model (Developed Frenkel-Kontorova model) is put forward: - two one-dimensional sequences of N and L point atoms, masses m and M; with coordinates {xi} and {yj}, connected by elastic springs with the laws of elastic dispersion and . Chains CH1 and CH2 interact with each other by potential Vi,j.

    The Hamiltonian of the DFK model has the form:

    From the analysis of the ground state of the DFK model (N = L) [1], the following conclusion follows: - when one of the Hooke’s chains is stretched by force F, an abrupt transition to the incommensurate phase occurs (F>Fc), in which part of the atoms of the stretched chain CH1 leaves the interaction with CH2. The number of atoms falling out of the Vi,j interaction space , where V0 = max Vi,j.

    With strong interaction (V~ 1) and strong stretching (F>Fc ~1), the size of the dislocation is 2, and the number of precipitated atoms is N/2. In this case, the incommensurate phase will be a periodic chain of hole dislocations, i.e., commensurate crystal with doubled period.

    Keywords:

    Mathematics; FK model; Development

    References:

    [1] A.N. Filonov FTT, vol. 30, issue 1, 28, (1988)

    Cite this article as:

    Filonov A, Kveglis L, Abkaryan A, Artemyev E. (2023). DYNAMICS FRENKEL-KONTOROVA MODEL. In F. Kongoli, A. B. Bhattacharya, A.C. Pandey, G. Sandhu, F. Quattrocchi, L. Sajo-Bohus, S. Singh, H.S. Virk, R.M. Santilli, M. Mikalajunas, E. Aifantis, T. Vougiouklis, P. Mandell, E. Suhir, D. Bammann, J. Baumgardner, M. Horstemeyer, N. Morgan, R. Prabhu, A. Rajendran (Eds.), Sustainable Industrial Processing Summit Volume 13 Intl. Symp on Physics, Mathematics and Multiscale Mechanics (pp. 137-138). Montreal, Canada: FLOGEN Star Outreach