Numéro |
J. Phys. IV France
Volume 06, Numéro C8, Décembre 1996
ICIFUAS 11Eleventh International Conference on Internal Friction and Ultrasonic Attenuation in Solids |
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Page(s) | C8-317 - C8-319 | |
DOI | https://doi.org/10.1051/jp4:1996869 |
Eleventh International Conference on Internal Friction and Ultrasonic Attenuation in Solids
J. Phys. IV France 06 (1996) C8-317-C8-319
DOI: 10.1051/jp4:1996869
Internal Friction and Creep-Recovery in Indium
H. Ledbetter1, N. Sizova1, S. Kim1, H. Kobayashi2, S. Sgobba3 and L. Parrini41 Materials Science and Engineering Laboratory, National Institute of Standards and Technology, Boulder, Colorado 80303, U.S.A.
2 National Research Laboratory of Metrology, Tsukuba, Ibaraki, Japan
3 CERN, Geneva, Switzerland
4 Ecole Polytechnique Fédérale de Lausanne, Institut de Génie Atomique, 1015 Lausanne, Switzerland
Abstract
Using low-stress pseudoshear deformation, we measured the ambient-temperature creep-recovery behavior of polycrystalline indium. The ε-σ diagram shows three regions with increasing stress : stress exponents of 1.05, 7.4, and 2.0. The diagram resembles remarkably the dislocation-velocity-shear-stress diagrams reported for various materials by many authors, who interpreted the diagrams by dislocation dynamics. Applying an extended Burgers model (two Kelvin-Voigt elements) gave for the three regions the following relaxation times τ2 and τ3 (in seconds) : (1) 11, 123 ; (2) 10, 132 ; (3) 12, 154. Thus, τ1 is nearly stress independent, and τ2 increases with increasing stress. Laplacean transformation of our ε(t) measurements to get the retardation-time distribution function g(ln τ) indicates in all three regions a strong peak near τ2=3s and a weaker, broader peak near τ3=150s. These agree surprisingly well with the Burgers dashpot-spring-model results. We analyzed the recovery part of the strain ε(t) obtain Q-1(f) curves.
© EDP Sciences 1996