1968
DOI: 10.1002/pssb.19680290206
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Dislocation Mobility in the {1122} 〈1123〉 Slip System of Zinc Single Crystals

Abstract: Results are presented of measurements of the stress dependence of screw dislocation velocities in the { 1122) (1123) slip system (pyramidal slip) of zinc single crystals. The investigations have been carried out on zinc single crystals of 99.999% purity at room temperature. The dislocation mobility has been studied within a wide range of velocities and shear stresses below and above the critical resolved shear stress. When the shear stress t changed from 20 to 4000 p/mm2 the dislocation velocity v varied from … Show more

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Cited by 21 publications
(4 citation statements)
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“…Further selective etch experiments in the next decades replicated these results in a vast number of materials, under different temperature ranges and under irradiation conditions [50]. Materials tested in this way include the metals W [51], Fe [44,52], Fe-C [53], Fe-Si [16,54,55], Al [56], Cu [57,58,59,60], irradiated Cu [61], Al-Cu alloys [17,21,57,62], Ni [63], Pb [64], Mg [65], Zn [66,67,68,59,69,70,71,72], Nb [73,74,75], α-Ti [76], In [77], K [52], Mo [65,78,79], Ag [80], and a number of ceramics and semiconductors, including pure Ge [81] and Si [82,83], LiF [48,84,85,86], BeO [87], KCl [88], Na...…”
Section: Experimental Evidencementioning
confidence: 95%
“…Further selective etch experiments in the next decades replicated these results in a vast number of materials, under different temperature ranges and under irradiation conditions [50]. Materials tested in this way include the metals W [51], Fe [44,52], Fe-C [53], Fe-Si [16,54,55], Al [56], Cu [57,58,59,60], irradiated Cu [61], Al-Cu alloys [17,21,57,62], Ni [63], Pb [64], Mg [65], Zn [66,67,68,59,69,70,71,72], Nb [73,74,75], α-Ti [76], In [77], K [52], Mo [65,78,79], Ag [80], and a number of ceramics and semiconductors, including pure Ge [81] and Si [82,83], LiF [48,84,85,86], BeO [87], KCl [88], Na...…”
Section: Experimental Evidencementioning
confidence: 95%
“…Hence, to accommodate c-axis strain, HCP structures require dislocation gliding in the non-basal directions which has a higher energy barrier. According to general consensus, the easiest non-basal dislocation to activate is the pyramidal /c þ aS (Price, 1961a;Lavrentev et al, 1968Lavrentev et al, , 1978Lavrentev and Pokhil, 1975), but it is still so difficult to activate that certain twin partials, notably those with Burgers vectors along the /1011S directions, can twice as easily accommodate either an expansion or even a reduction of the c-axis. These disparities in critical stresses of the deformation modes are mitigated with increasing temperature and/or decreasing strain rates.…”
Section: Introductionmentioning
confidence: 99%
“…Dislocations of this type are immobile and can cause stress concentrations that result in secondary twinning. [43] In Ti, the current treatment results in formation of small twins at grain boundaries and also in floating twin bands within the grains (Figure 7). Compared to classical twins described and shown in ref.…”
Section: Sem Analysis Of the Evolution The Dislocation And Twin Struc...mentioning
confidence: 99%