Kinetics for dislocation structure formation in contact area of squeezed crystalline solids

Evolution of dislocation structure during formation of the contact area was studied in modeling experiments "wedge-plane" for KCl single crystal under loading at room and high (0.8Tm) temperatures. It was shown that at the first (rapid) stage of the process, a quasi-stationary dislocation...

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Published in:Functional Materials
Date:2013
Main Authors: Boyko, Yu.I., Volosyuk, M.A., Kononenko, V.G.
Format: Article
Language:English
Published: НТК «Інститут монокристалів» НАН України 2013
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/119800
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:Kinetics for dislocation structure formation in contact area of squeezed crystalline solids / Yu.I. Boyko, M.A. Volosyuk, V.G. Kononenko // Functional Materials. — 2013. — Т. 20, № 1. — С. 44-51. — Бібліогр.: 25 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
id nasplib_isofts_kiev_ua-123456789-119800
record_format dspace
spelling Boyko, Yu.I.
Volosyuk, M.A.
Kononenko, V.G.
2017-06-09T17:17:52Z
2017-06-09T17:17:52Z
2013
Kinetics for dislocation structure formation in contact area of squeezed crystalline solids / Yu.I. Boyko, M.A. Volosyuk, V.G. Kononenko // Functional Materials. — 2013. — Т. 20, № 1. — С. 44-51. — Бібліогр.: 25 назв. — англ.
1027-5495
DOI: dx.doi.org/10.15407/fm20.01.044
https://nasplib.isofts.kiev.ua/handle/123456789/119800
Evolution of dislocation structure during formation of the contact area was studied in modeling experiments "wedge-plane" for KCl single crystal under loading at room and high (0.8Tm) temperatures. It was shown that at the first (rapid) stage of the process, a quasi-stationary dislocation assemblage is formed due to emission of dislocations. It was established that at high temperature (0.8Tm), the cellar structure (CS) was formed at the earliest stages of annealing under loading. The experimentally determined dislocation critical density ρ c at which the CS is formed ρ c≈ 10⁷ cm⁻² is by the order of value corresponds to the calculated one (10⁶< ρc< 10¹⁰) cm⁻². The crystal-likeness of the CS predicted by the theory is supported qualitatively; the CS contains a mixture of cells-polygons with the number of sides predominantly from 4 to 6.
en
НТК «Інститут монокристалів» НАН України
Functional Materials
Characterization and properties
Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
Article
published earlier
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
title Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
spellingShingle Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
Boyko, Yu.I.
Volosyuk, M.A.
Kononenko, V.G.
Characterization and properties
title_short Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
title_full Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
title_fullStr Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
title_full_unstemmed Kinetics for dislocation structure formation in contact area of squeezed crystalline solids
title_sort kinetics for dislocation structure formation in contact area of squeezed crystalline solids
author Boyko, Yu.I.
Volosyuk, M.A.
Kononenko, V.G.
author_facet Boyko, Yu.I.
Volosyuk, M.A.
Kononenko, V.G.
topic Characterization and properties
topic_facet Characterization and properties
publishDate 2013
language English
container_title Functional Materials
publisher НТК «Інститут монокристалів» НАН України
format Article
description Evolution of dislocation structure during formation of the contact area was studied in modeling experiments "wedge-plane" for KCl single crystal under loading at room and high (0.8Tm) temperatures. It was shown that at the first (rapid) stage of the process, a quasi-stationary dislocation assemblage is formed due to emission of dislocations. It was established that at high temperature (0.8Tm), the cellar structure (CS) was formed at the earliest stages of annealing under loading. The experimentally determined dislocation critical density ρ c at which the CS is formed ρ c≈ 10⁷ cm⁻² is by the order of value corresponds to the calculated one (10⁶< ρc< 10¹⁰) cm⁻². The crystal-likeness of the CS predicted by the theory is supported qualitatively; the CS contains a mixture of cells-polygons with the number of sides predominantly from 4 to 6.
issn 1027-5495
url https://nasplib.isofts.kiev.ua/handle/123456789/119800
citation_txt Kinetics for dislocation structure formation in contact area of squeezed crystalline solids / Yu.I. Boyko, M.A. Volosyuk, V.G. Kononenko // Functional Materials. — 2013. — Т. 20, № 1. — С. 44-51. — Бібліогр.: 25 назв. — англ.
work_keys_str_mv AT boykoyui kineticsfordislocationstructureformationincontactareaofsqueezedcrystallinesolids
AT volosyukma kineticsfordislocationstructureformationincontactareaofsqueezedcrystallinesolids
AT kononenkovg kineticsfordislocationstructureformationincontactareaofsqueezedcrystallinesolids
first_indexed 2025-12-07T17:38:35Z
last_indexed 2025-12-07T17:38:35Z
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