Properties of Dislocation Drag from Phonon Wind at Ambient Conditions
It is well known that, under plastic deformation, dislocations are not only created but also move through the crystal, and their mobility is impeded by their interaction with the crystal structure. At high stress and temperature, this “drag„ is dominated by phonon wind, i.e., pho...
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doaj-f57bf7dbb41b47a7b09f38edd66e70d52020-11-25T00:32:56ZengMDPI AGMaterials1996-19442019-03-0112694810.3390/ma12060948ma12060948Properties of Dislocation Drag from Phonon Wind at Ambient ConditionsDaniel N. Blaschke0Los Alamos National Laboratory, Computational Physics Division, Los Alamos, NM 87545, USAIt is well known that, under plastic deformation, dislocations are not only created but also move through the crystal, and their mobility is impeded by their interaction with the crystal structure. At high stress and temperature, this “drag„ is dominated by phonon wind, i.e., phonons scattering off dislocations. Employing the semi-isotropic approach discussed in detail in a previous paper (<i>J. Phys. Chem. Solids</i> <b>2019</b>, <i>124</i>, 24–35), we discuss here the approximate functional dependence of dislocation drag <i>B</i> on dislocation velocity in various regimes between a few percent of transverse sound speed <inline-formula> <math display="inline"> <semantics> <msub> <mi>c</mi> <mi mathvariant="normal">T</mi> </msub> </semantics> </math> </inline-formula> and <inline-formula> <math display="inline"> <semantics> <msub> <mi>c</mi> <mi mathvariant="normal">T</mi> </msub> </semantics> </math> </inline-formula> (where <inline-formula> <math display="inline"> <semantics> <msub> <mi>c</mi> <mi mathvariant="normal">T</mi> </msub> </semantics> </math> </inline-formula> is the effective average transverse sound speed of the polycrystal). In doing so, we find an effective functional form for dislocation drag <inline-formula> <math display="inline"> <semantics> <mrow> <mi>B</mi> <mo>(</mo> <mi>v</mi> <mo>)</mo> </mrow> </semantics> </math> </inline-formula> for different slip systems and dislocation characters at fixed (room) temperature and low pressure.https://www.mdpi.com/1996-1944/12/6/948dislocations in crystalsdrag coefficientphonon wind |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Daniel N. Blaschke |
spellingShingle |
Daniel N. Blaschke Properties of Dislocation Drag from Phonon Wind at Ambient Conditions Materials dislocations in crystals drag coefficient phonon wind |
author_facet |
Daniel N. Blaschke |
author_sort |
Daniel N. Blaschke |
title |
Properties of Dislocation Drag from Phonon Wind at Ambient Conditions |
title_short |
Properties of Dislocation Drag from Phonon Wind at Ambient Conditions |
title_full |
Properties of Dislocation Drag from Phonon Wind at Ambient Conditions |
title_fullStr |
Properties of Dislocation Drag from Phonon Wind at Ambient Conditions |
title_full_unstemmed |
Properties of Dislocation Drag from Phonon Wind at Ambient Conditions |
title_sort |
properties of dislocation drag from phonon wind at ambient conditions |
publisher |
MDPI AG |
series |
Materials |
issn |
1996-1944 |
publishDate |
2019-03-01 |
description |
It is well known that, under plastic deformation, dislocations are not only created but also move through the crystal, and their mobility is impeded by their interaction with the crystal structure. At high stress and temperature, this “drag„ is dominated by phonon wind, i.e., phonons scattering off dislocations. Employing the semi-isotropic approach discussed in detail in a previous paper (<i>J. Phys. Chem. Solids</i> <b>2019</b>, <i>124</i>, 24–35), we discuss here the approximate functional dependence of dislocation drag <i>B</i> on dislocation velocity in various regimes between a few percent of transverse sound speed <inline-formula> <math display="inline"> <semantics> <msub> <mi>c</mi> <mi mathvariant="normal">T</mi> </msub> </semantics> </math> </inline-formula> and <inline-formula> <math display="inline"> <semantics> <msub> <mi>c</mi> <mi mathvariant="normal">T</mi> </msub> </semantics> </math> </inline-formula> (where <inline-formula> <math display="inline"> <semantics> <msub> <mi>c</mi> <mi mathvariant="normal">T</mi> </msub> </semantics> </math> </inline-formula> is the effective average transverse sound speed of the polycrystal). In doing so, we find an effective functional form for dislocation drag <inline-formula> <math display="inline"> <semantics> <mrow> <mi>B</mi> <mo>(</mo> <mi>v</mi> <mo>)</mo> </mrow> </semantics> </math> </inline-formula> for different slip systems and dislocation characters at fixed (room) temperature and low pressure. |
topic |
dislocations in crystals drag coefficient phonon wind |
url |
https://www.mdpi.com/1996-1944/12/6/948 |
work_keys_str_mv |
AT danielnblaschke propertiesofdislocationdragfromphononwindatambientconditions |
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1725318295321575424 |