The Flow-Stress Asymmetry of Ultra-Pure Molybdenum Single Crystals
Cyclic deformation experiments by the Mughrabi–Ackermann technique (predeformation with plastic shear-strain amplitude εpl0⁄2=1×10−3 at 530 K till saturation) have been performed on a molybdenum single crystal of ultra-high purity (residual resistivity ratio RRR0≈4×105; angle χ=29° between the plane...
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Published in | Materials Transactions, JIM Vol. 41; no. 1; pp. 141 - 151 |
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Main Authors | , |
Format | Journal Article Conference Proceeding |
Language | English |
Published |
Sendai
The Japan Institute of Metals
2000
Japan Institute of Metals |
Subjects | |
Online Access | Get full text |
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Summary: | Cyclic deformation experiments by the Mughrabi–Ackermann technique (predeformation with plastic shear-strain amplitude εpl0⁄2=1×10−3 at 530 K till saturation) have been performed on a molybdenum single crystal of ultra-high purity (residual resistivity ratio RRR0≈4×105; angle χ=29° between the plane of maximum resolved shear stress and the 〈111〉{110} slip system with largest Schmid factor), covering the temperature range 123K≤T≤460K and seven logarithmically spaced strain rates (1.0×10−6s−1≤|\dotεpl|≤1.0×10−3s−1). The analysis of the effective flow stress σ* in terms of the kink pair-formation theory gave the same results as the earlier experiments on Mo crystals of the same high purity but with smaller χ [Hollang, L., M. Hommel, and Seeger, A., phys. stat. sol. (a) 160 (1996) 329] both for the energy of two isolated kinks in 〈111〉a0⁄2 screw dislocations, 2Hk=1.27 eV, and for the kink height a, which agreed with the distance a{112} between neighbouring Peierls valleys on the {112} planes. The transition between the elastic-interaction approximation and the line-tension approximation of the kink pair-formation theory, which is responsible for the strain rate-dependent “upper bend” in the σ*-T relationship, occurred at \hatσ*=110 MPa. In agreement with theoretical predictions, at effective stresses less than \hatσ* the flow stress was the same in tension and compression, i.e., there was no flow-stress asymmetry. Below the upper-bend temperature, \hatT, the flow-stress asymmetry Δσ (=algebraic sum of the positive flow stress in tension and the negative flow stress in compression) increased with decreasing temperature, was positive in agreement with the “twinning–anti-twinning rule”, and reached a plateau at the lowest temperatures investigated. Since for reasons of symmetry, slip on {110} cannot give rise to a flow-stress asymmetry, together with a=a{112} this result confirms that over the entire temperature range investigated the elementary slip steps take place on {112} planes. In the other two ultrahigh-purity crystals investigated (χ=0°, 21°), the flow-stress asymmetry has the opposite sign (in violation of the “twinning–anti-twinning rule”) and, at low temperatures, much smaller absolute values than at χ≈30°. Furthermore, Δσ<0 extends to temperatures well above \hatT. Hence there must exist, in addition to the “twinning–anti-twinning asymmetry”, a further asymmetry-producing mechanism (dubbed “straining asymmetry”), for which the following model is proposed. In the bcc metals the screw-dislocation cores of lowest energy have {110} slip planes; the configuration with {112} slip planes is populated by thermal activation. Tensile strain normal to the {112} slip plane reduces the difference in the line energy of the two configurations and, as a consequence, the Peierls potential on the {112} slip plane. Compression strain has the opposite effect. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0916-1821 2432-471X |
DOI: | 10.2320/matertrans1989.41.141 |