| 000 | 03627nab a2200361 c 4500 | ||
|---|---|---|---|
| 001 | koha000997185 | ||
| 005 | 20230228180624.0 | ||
| 007 | cr | | ||
| 008 | 230221|2022 ne s a eng d | ||
| 024 | 7 |
_a10.1016/j.msea.2022.143586 _2doi |
|
| 035 | _akoha000997185 | ||
| 040 |
_aRU-ToGU _brus _cRU-ToGU |
||
| 245 | 1 | 0 |
_aCritical resolved shear stress for twinning and twinning-induced plasticity in single crystals of the CoCrFeNiMo0.2 high-entropy alloy _cI. V. Kireeva, Yu. I. Chumlyakov, A. V. Vyrodova, A. A. Saraeva |
| 336 | _aТекст | ||
| 337 | _aэлектронный | ||
| 504 | _aБиблиогр.: 67 назв. | ||
| 520 | 3 | _aThe effect of alloying with Mo atoms 4 at.% on the twinning deformation, critical resolved shear stresses (CRSS) for slip τslcr and twinning τtwcr and plasticity was studied in [111]-, [144]- and [001]- oriented crystals of the Co24Cr24Fe24Ni24Mo4 (at.%) high-entropy alloy (HEA) under tension at 296 and 77 K. The stacking fault energy of the Co24Cr24Fe24Ni24Mo4 HEA, measured in the resent paper on the triple dislocation nodes, is equal to 0.027 J/m2. It is shown that initial yield behavior along studied orientations is governed by dislocation slip and the CRSS for slip are independent of crystal orientation. Under tensile strain, twinning develops in the [111]- and [144]- oriented crystals only at 77 K and is not detected in the [001]-oriented crystals. Two types of twins are found in the [111]- and [144]-oriented crystals (thin nanotwins and macrotwins). Nanotwins develop after a low slip deformation of 5–10% and are observed only by transmission electron microscopy. Macrotwins are detected after a significant slip deformation of 20 and 60% and are determined metallographically and X-ray by the precession of the crystal axis, respectively, in the [111]- and [144]-oriented crystals. In the [111]- oriented crystals, there is no precession of the crystal axis due to the development of slip simultaneously in several systems. It is shown that CRSS for nano- and macrotwins are dependent on the crystal orientation. In the [144]-oriented crystals, τtw cr = 212 MPa for nanotwinning and τtw cr = 400 MPa for macrotwinning. In the [111]-oriented crystals, τtw cr = 250 MPa for nanotwinning and τtw cr = 335 MPa for macrotwinning. For the transition to deformation by macrotwinning, it is necessary that the effective stacking fault energy γef is approaching to zero and the condition τtwcr <τslcr is satisfied. Deformation by macrotwinning suppresses slip multiplicity and shifts the formation of the neck formation according to the Consid`ere condition to higher stress levels. This increases plasticity from 72% at 296 K to 108% at 77 K in [144]-oriented crystals and from 48% at 296 K to 57% at 77 K in [111]-oriented crystals. | |
| 653 | _aвысокоэнтропийные сплавы | ||
| 653 | _aмонокристаллы | ||
| 653 | _aдеформация растяжения | ||
| 653 | _aдеформационное двойникование | ||
| 653 | _aпластичность, вызванная двойникованием | ||
| 655 | 4 |
_aстатьи в журналах _9877202 |
|
| 700 | 1 |
_aKireeva, Irina V. _cфизик _989594 |
|
| 700 | 1 |
_aChumlyakov, Yuri I. _9100866 |
|
| 700 | 1 |
_aVyrodova, Anna V. _9877230 |
|
| 700 | 1 |
_aSaraeva, Anastasia A. _9877232 |
|
| 773 | 0 |
_tMaterials science and engineering A _d2022 _gVol. 850. P. 143586 (1-15) _x0921-5093 |
|
| 852 | 4 | _aRU-ToGU | |
| 856 | 4 | _uhttp://vital.lib.tsu.ru/vital/access/manager/Repository/koha:000997185 | |
| 908 | _aстатья | ||
| 999 | _c997185 | ||