1979
DOI: 10.1002/pssa.2210540125
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Analysis of Dislocation Mobility under Concentrated Loads at Indentations of Single Crystals

Abstract: An approximate solution is given for the dependence of the dislocation track length, t , around a microhardness indentation in single crystals on the load applied t o the indenter (P), the temperature (T), and the duration under load ( t ) :The assumption is made that dislocations move from the indenter in plane arrays alid that the dislocation velocity is vt m exp (-U / k T ) , where t is an effective stress, U is the activation energy.I n a definite range of parameters the equation agrees satisfactorily with… Show more

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Cited by 23 publications
(7 citation statements)
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“…These observations are consistent with the model of Gridneva et al [13] (Fig. 4) ; 2 1 and Hv are minimum for the indenter diagonal parallel to 110 > (Fig.…”
Section: Hardness In Various Crystallographicsupporting
confidence: 92%
“…These observations are consistent with the model of Gridneva et al [13] (Fig. 4) ; 2 1 and Hv are minimum for the indenter diagonal parallel to 110 > (Fig.…”
Section: Hardness In Various Crystallographicsupporting
confidence: 92%
“…The stress dependence of the dislocation velocity is usually described by the empirical formula V=V0true(ττ0true)mexp(ΔE/kT) where the constants V 0 and τ 0 are usually determined experimentally for different materials and Δ E is the activation energy for dislocation mobility . As shown in, if the dislocation velocity can be described by the Equation and τ is equal to AP / r 2 , where A=true(12νtrue)/true(π6true), ν is the Poisson ratio and P is the applied load, the Equation can be rewritten as V=drdt=V0(APτ0r2)mexp(ΔE/kT) and 0Lr2mdr=L2m+1=0tdV0true(APτ0true)mexp(ΔE/kT)=V0true(APτ0true)mtdexp(ΔE/kT) where L is the traveling distance of leading dislocations measured from the imprint center and t d is the deformation dwell time. From Equation it can be obtained that L=V0…”
Section: Resultsmentioning
confidence: 99%
“…In this case the distance from the imprint center to the leading dislocation varies from a to ( a 2 + L 1 2 ) 0.5 , where a is the distance between the acting slip plane and the imprint center and L 1 is the traveling distance of cross‐slip dislocation. These parameters are illustrated by (Figure ) on the CL image of imprint made by indentation at 573 K. The integration procedure similar to that used in and in Equation , assuming that m is the integer, gives for L 1 L12m+12m+1+m1!(2m1)L12m1a2+m(m1)2!(2m3)L12m3a4++a2mL1=V0true(APτ0true)mtdexptrue[normalΔEkTtrue] …”
Section: Resultsmentioning
confidence: 99%
“…In the framework of the dislocation theory, the zone of elastoplastic deformation with the radius bS is the zone with a sharp increase in the dislocation density around the indentation imprint with a symmetry center at the very point 0 in Figure 1. Dislocations are nucleated near the indenter and move in the radial directions to the boundaries of the elastoplastic zone under the action of shear stress, caused by the load on indenter [19]. The comparison of calculated values of bS with the experimental data is given in the Section 3.6.…”
Section: Introductionmentioning
confidence: 99%