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<bibitem type="J">   <ARLID>0346416</ARLID> <utime>20240103193749.4</utime><mtime>20100913235959.9</mtime>   <WOS>000280819300006</WOS>  <DOI>10.1080/14786430903449411</DOI>           <title language="eng" primary="1">Crystal plasticity model of shear and kink bands-energetic approach</title>  <specification> <page_count>14 s.</page_count> </specification>   <serial><ARLID>cav_un_epca*0296693</ARLID><ISSN>1478-6435</ISSN><title>Philosophical Magazine</title><part_num/><part_title/><volume_id>90</volume_id><volume>27 (2010)</volume><page_num>3729-3742</page_num><publisher><place/><name>Taylor &amp; Francis</name><year/></publisher></serial>    <keyword>crystal plasticity</keyword>   <keyword>kink bands-energetic approach</keyword>    <author primary="1"> <ARLID>cav_un_auth*0044342</ARLID> <name1>Kratochvíl</name1> <name2>J.</name2> <country>CZ</country>  </author> <author primary="0"> <ARLID>cav_un_auth*0101142</ARLID> <name1>Kružík</name1> <name2>Martin</name2> <full_dept language="cz">Matematická teorie rozhodování</full_dept> <full_dept>Department of Decision Making Theory</full_dept> <department language="cz">MTR</department> <department>MTR</department> <institution>UTIA-B</institution> <full_dept>Department of Decision Making Theory</full_dept>  <fullinstit>Ústav teorie informace a automatizace AV ČR, v. v. i.</fullinstit> </author> <author primary="0"> <ARLID>cav_un_auth*0226808</ARLID> <name1>Sedláček</name1> <name2>R.</name2> <country>DE</country>  </author>   <source> <url>http://library.utia.cas.cz/separaty/2010/MTR/kruzik-crystal plasticity model of shear and kink bands-energetic approach.pdf</url> </source>        <cas_special> <project> <project_id>IAA100750802</project_id> <agency>GA AV ČR</agency> <ARLID>cav_un_auth*0241214</ARLID> </project> <research> <research_id>CEZ:AV0Z10750506</research_id> </research>  <abstract language="eng" primary="1">We present a continuum crystal plasticity model of a lamellar deformation  substructure of shear and kink bands. An evolutionary problem for the  development of a spontaneous structural inhomogeneity is formulated in  the framework of energetic solutions. Conti and Theil proved that in the  case of an isothermal single-slip crystal, rigid plasticity with no hardening  lamellaea form an optimal microstructure. Moreover, their model predicts  the existence of a boundary layer which accommodates the lamellar  substructure to displacement boundary conditions. It is suggested that the  width of the shear and kink bands is a compromise: the minimization of  bulk energy tends to decrease their size, while the energy of the band  interfaces or the inner structure of the bands opposes this tendency.</abstract>     <reportyear>2011</reportyear>  <RIV>BM</RIV>      <permalink>http://hdl.handle.net/11104/0187453</permalink>          <unknown tag="mrcbT16-e">MATERIALSSCIENCEMULTIDISCIPLINARY|MECHANICS|METALLURGYMETALLURGICALENGINEERING|PHYSICSAPPLIED|PHYSICSCONDENSEDMATTER</unknown> <unknown tag="mrcbT16-f">1.368</unknown> <unknown tag="mrcbT16-g">0.41</unknown> <unknown tag="mrcbT16-h">&gt;10.0</unknown> <unknown tag="mrcbT16-i">0.02096</unknown> <unknown tag="mrcbT16-j">0.692</unknown> <unknown tag="mrcbT16-k">8424</unknown> <unknown tag="mrcbT16-l">283</unknown> <unknown tag="mrcbT16-q">44</unknown> <unknown tag="mrcbT16-s">1.034</unknown> <unknown tag="mrcbT16-y">31.91</unknown> <unknown tag="mrcbT16-x">1.33</unknown> <unknown tag="mrcbT16-4">Q2</unknown> <unknown tag="mrcbT16-B">56.488</unknown> <unknown tag="mrcbT16-C">59.909</unknown> <unknown tag="mrcbT16-D">Q2</unknown> <unknown tag="mrcbT16-E">Q2</unknown> <arlyear>2010</arlyear>       <unknown tag="mrcbU34"> 000280819300006 WOS </unknown> <unknown tag="mrcbU63"> cav_un_epca*0296693 Philosophical Magazine 1478-6435 1478-6443 Roč. 90 č. 27 2010 3729 3742 Taylor &amp; Francis </unknown> </cas_special> </bibitem>