Pseudoelasticity in Fe3Al Single Crystals under Cyclic Loading

2006 ◽  
Vol 512 ◽  
pp. 25-30 ◽  
Author(s):  
Hiroyuki Y. Yasuda ◽  
Keisuke Yamaoka ◽  
Yukichi Umakoshi

D03-ordered Fe3Al single crystals containing 23, 25 and 28at.%Al were cyclically deformed at [ 49 1 ] loading axis in tension-compression mode. Giant pseudoelasticity took place in Fe-23 and 25at.%Al single crystals at an early stage of cyclic deformation, while a slight strain recovery was observed in Fe-28at.%Al. In Fe-23 and 25at.%Al single crystals, superpartial dislocations with Burgers vector of 1/4[111] moved individually dragging the nearest neighbour anti-phase boundary (NNAPB). The NNAPB pulled back the superpartials during unloading, resulting in giant pseudoelasticity and low residual dislocation density. In contrast, a couplet of the superpartials was observed to bow out leaving two superpartials in Fe-28at.%Al. This means that the dislocation couplet dragged the next-nearest neighbour anti-phase boundary (NNNAPB). The surface tension of NNNAPB is lower than that of NNAPB resulting in a slight strain recovery in Fe-28at%Al. As cyclic deformation proceeded, residual dislocation density increased with an increase in the number of cycles even in Fe-23 and 25at.%Al. In particular, persistent slip bands (PSB) were formed in Fe-23at.%Al single crystals, though PSB is seldom observed in fatigued intermetallic compounds. To-and-fro motion of superpartials during loading and unloading was suppressed by dislocation bundles, resulting in a reduced shape recovery. However, large strain recovery occurred in Fe-25at.%Al single crystals at a strain amplitude of 1.0% even at 20cycles. It was also noted that Fe-23 and 25at.%Al demonstrated tension-compression asymmetry even at [ 49 1 ] orientation; the yield stress in compression was higher than that in tension. This implies that the core structure of <111> screw dislocation played an important role in the deformation behaviour of Fe3Al single crystals.

1986 ◽  
Vol 53 (6) ◽  
pp. 887-896 ◽  
Author(s):  
Han-Ryong Pak ◽  
Lieh-Ming Hsiung ◽  
Masaharu Kato

2015 ◽  
Vol 48 (4) ◽  
pp. 1080-1088 ◽  
Author(s):  
Wanneng Ye ◽  
Chaojing Lu ◽  
Yongcheng Zhang ◽  
Yichun Zhou

In the ferroelectric Bi4Ti3O12, the major componentPs(a)of spontaneous polarizationPslies along theaaxis; the componentPs(c)along thecaxis is small. The two switchable components are expected to make up various types of domain walls (DWs). According to group-theory analysis, 11 permissible types of DWs are predicted to exist theoretically, and they include five types of ferroelectric DWs, one type of anti-phase boundary (APB) and five types of APB-combined ferroelectric DWs. The five types of ferroelectric DWs arePs(a)-90° DWs,Ps(a)-180° DWs,Ps(c)-180° DWs,Ps(a)-90°/Ps(c)-180° DWs andPs-180° DWs. In Bi4Ti3O12single crystals, just the five types of ferroelectric DWs were observed using transmission electron microscopy, with no trace of APBs or APB-combined ferroelectric DWs seen. ThePs(a)-90° domains are lamellar and do not have even thickness. Both thePs(a)-90° DWs andPs(a)-90°/Ps(c)-180° DWs lie mainly on the (110) plane, but often fold to the (001) plane. ThePs(a)-180° domains are predominantly flaky. Both thePs(a)-180° DWs andPs-180° DWs lie mainly on the (001) plane. ThePs(c)-180° DWs observed are irregularly curved.


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