Abstract:The ultrasonic logarithmic decrement and modulus defect in high purity copper crystals was measured at 10, 30 and 50 MHz in the temperature interval 5-373 K. The samples were deformed at room temperature in the 3-20% range along the
111
crystallographic direction. The experimental data were fitted over the whole interval of temperatures, assuming the contribution of two kink mechanisms: (i) relaxation by kink pair formation with diffusion in the dislocation line and (ii) overdamped resonance of the kink chai… Show more
“…In this equation a is the interatomic distance in the dislocation line direction, N o is the number of geometrical kinks in the dislocation line, H k = enthalpy of creation of one kink, k B is the Boltzmann's constant, and A is a constant [2]. For high purity copper it holds that B(T) T [2] and, as we shown from experimental results,…”
Section: ( ) / 1 ( )mentioning
confidence: 81%
“…For comparison, the inset shows the ultrasonic attenuation for a high purity copper measured in an hydrogen free [2] and 3 days aged [6] hydrogenated samples, where the respective dislocation background were subtracted from the experimental data.…”
Section: Resultsmentioning
confidence: 99%
“…Both o and v o were measured in a <111> non-deformed copper sample, irradiated with -rays until total pinning of dislocations [8]. We assume that the temperature dependence of the dislocations free attenuation and velocity on a deformed sample is the same as that in undeformed samples [2]. Also corrections due to pulse path length variation with temperature were introduced [7].…”
Section: Methodsmentioning
confidence: 99%
“…zero applied stress [2]. In this equation a is the interatomic distance in the dislocation line direction, N o is the number of geometrical kinks in the dislocation line, H k = enthalpy of creation of one kink, k B is the Boltzmann's constant, and A is a constant [2].…”
Section: ( ) / 1 ( )mentioning
confidence: 99%
“…The kink picture has proven to be the best approach to explain the internal friction and ultrasonic attenuation of cold-worked samples of high purity FCC metals [1]. At 10 MHz to 50 MHz frequencies the two attenuation peaks known as Niblet-Wilks and Bordoni peaks (hereafter denominated NWP and BP, respectively) are present in cold-worked high purity copper crystals, superposed to a dislocation related background, which were well described in terms of the kink picture [2]. While the NWR and BR relaxations are considered to be produced by the mechanism of kink pair formation with kink diffusion in the phonon field (KPF), the dislocation background is attributed to the resonance of the oscillating kink-chain with a kink density T [2].…”
In this paper we present experimental data of ultrasonic velocity and attenuation obtained in a high purity crystalline sample of cooper hydrogenated by gaseous charge. The sample is oriented in the <111> crystallographic direction and aged for this work in three stages between 64 and 97 days. The results indicate that the hydrogen is mainly segregated at the dislocation core, inhibiting the Hydrogen Snoek-Köster relaxations verified at earlier aging stages. Despite of this, a contribution to viscosity in the kink-chain resonance is provided by the mobile hydrogen in the dislocations core by its side movement along the dislocation line. At temperatures at which the hydrogen begins to freeze in the lattice the geometrical kinks find a gradual increase on the hindering of their movements along dislocation lines, becoming immobile when the hydrogen is completely frozen in the crystal, anchoring the dislocations in short loops. Although the viscosity associated with the mobile hydrogen is removed, the resonance associated with geometrical kinks is not completely cancelled. The interaction hydrogen-dislocation can be fully described in terms of kinks in dislocations.
“…In this equation a is the interatomic distance in the dislocation line direction, N o is the number of geometrical kinks in the dislocation line, H k = enthalpy of creation of one kink, k B is the Boltzmann's constant, and A is a constant [2]. For high purity copper it holds that B(T) T [2] and, as we shown from experimental results,…”
Section: ( ) / 1 ( )mentioning
confidence: 81%
“…For comparison, the inset shows the ultrasonic attenuation for a high purity copper measured in an hydrogen free [2] and 3 days aged [6] hydrogenated samples, where the respective dislocation background were subtracted from the experimental data.…”
Section: Resultsmentioning
confidence: 99%
“…Both o and v o were measured in a <111> non-deformed copper sample, irradiated with -rays until total pinning of dislocations [8]. We assume that the temperature dependence of the dislocations free attenuation and velocity on a deformed sample is the same as that in undeformed samples [2]. Also corrections due to pulse path length variation with temperature were introduced [7].…”
Section: Methodsmentioning
confidence: 99%
“…zero applied stress [2]. In this equation a is the interatomic distance in the dislocation line direction, N o is the number of geometrical kinks in the dislocation line, H k = enthalpy of creation of one kink, k B is the Boltzmann's constant, and A is a constant [2].…”
Section: ( ) / 1 ( )mentioning
confidence: 99%
“…The kink picture has proven to be the best approach to explain the internal friction and ultrasonic attenuation of cold-worked samples of high purity FCC metals [1]. At 10 MHz to 50 MHz frequencies the two attenuation peaks known as Niblet-Wilks and Bordoni peaks (hereafter denominated NWP and BP, respectively) are present in cold-worked high purity copper crystals, superposed to a dislocation related background, which were well described in terms of the kink picture [2]. While the NWR and BR relaxations are considered to be produced by the mechanism of kink pair formation with kink diffusion in the phonon field (KPF), the dislocation background is attributed to the resonance of the oscillating kink-chain with a kink density T [2].…”
In this paper we present experimental data of ultrasonic velocity and attenuation obtained in a high purity crystalline sample of cooper hydrogenated by gaseous charge. The sample is oriented in the <111> crystallographic direction and aged for this work in three stages between 64 and 97 days. The results indicate that the hydrogen is mainly segregated at the dislocation core, inhibiting the Hydrogen Snoek-Köster relaxations verified at earlier aging stages. Despite of this, a contribution to viscosity in the kink-chain resonance is provided by the mobile hydrogen in the dislocations core by its side movement along the dislocation line. At temperatures at which the hydrogen begins to freeze in the lattice the geometrical kinks find a gradual increase on the hindering of their movements along dislocation lines, becoming immobile when the hydrogen is completely frozen in the crystal, anchoring the dislocations in short loops. Although the viscosity associated with the mobile hydrogen is removed, the resonance associated with geometrical kinks is not completely cancelled. The interaction hydrogen-dislocation can be fully described in terms of kinks in dislocations.
An atomistic calculation of the Peierls stress in Al and Cu is undertaken in order to assess consistency with experiments. The measured yield stress extrapolated to 0 K results at least one order of magnitude smaller than the Peierls stress commonly derived from internal friction data. On the theoretical side, some calculations for Al are already available (using different approaches than presently) however none is for Cu. The simulations employ semi-empirical many-body interatomic potentials, fitted here to the generalized stacking fault energy surface (calculated elsewhere with ab initio electronic structure methods), as well as others from the literature. After a critical assessment, reasonable agreement is demonstrated between our results and the Peierls stress values derived from internal friction experiments within the framework of the kink pair formation model.
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