Abstract
It has been established experimentally that during a deformation process the defect structure of materials evolves from a single distribution of the defects to an ensemble of interacting particles which consists of nondisoriented or disoriented substructures, depending on the magnitude of the deformation. The conditions for the existence of disoriented defect substructures are examined on the basis of a field description of the dynamics of an ensemble of defects, and a generalization of previously known dynamical equations of nondisoriented defect substructures to the case of disoriented substructures is obtained. These equations show which quantities characterize the field of defects in the presence of disoriented substructures.
| Original language | English |
|---|---|
| Pages (from-to) | 1128-1129 |
| Number of pages | 2 |
| Journal | Technical Physics |
| Volume | 43 |
| Issue number | 9 |
| DOIs | |
| Publication status | Published - 1998 |
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ASJC Scopus subject areas
- Physics and Astronomy (miscellaneous)
Cite this
Dynamical equations of an ensemble of defects in the presence of disoriented substructures. / Grinyaev, Yu V.; Chertova, N. V.; Panin, V. E.
In: Technical Physics, Vol. 43, No. 9, 1998, p. 1128-1129.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Dynamical equations of an ensemble of defects in the presence of disoriented substructures
AU - Grinyaev, Yu V.
AU - Chertova, N. V.
AU - Panin, V. E.
PY - 1998
Y1 - 1998
N2 - It has been established experimentally that during a deformation process the defect structure of materials evolves from a single distribution of the defects to an ensemble of interacting particles which consists of nondisoriented or disoriented substructures, depending on the magnitude of the deformation. The conditions for the existence of disoriented defect substructures are examined on the basis of a field description of the dynamics of an ensemble of defects, and a generalization of previously known dynamical equations of nondisoriented defect substructures to the case of disoriented substructures is obtained. These equations show which quantities characterize the field of defects in the presence of disoriented substructures.
AB - It has been established experimentally that during a deformation process the defect structure of materials evolves from a single distribution of the defects to an ensemble of interacting particles which consists of nondisoriented or disoriented substructures, depending on the magnitude of the deformation. The conditions for the existence of disoriented defect substructures are examined on the basis of a field description of the dynamics of an ensemble of defects, and a generalization of previously known dynamical equations of nondisoriented defect substructures to the case of disoriented substructures is obtained. These equations show which quantities characterize the field of defects in the presence of disoriented substructures.
UR - http://www.scopus.com/inward/record.url?scp=0032347414&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0032347414&partnerID=8YFLogxK
U2 - 10.1134/1.1259150
DO - 10.1134/1.1259150
M3 - Article
AN - SCOPUS:0032347414
VL - 43
SP - 1128
EP - 1129
JO - Technical Physics
JF - Technical Physics
SN - 1063-7842
IS - 9
ER -