ORIENTATION DEPENDENCE OF THE PSEUDOELASTIC BEHAVIOR OF SINGLE-CRYSTALS OF CU-AL-NI IN TENSION

Authors
Citation
Tw. Shield, ORIENTATION DEPENDENCE OF THE PSEUDOELASTIC BEHAVIOR OF SINGLE-CRYSTALS OF CU-AL-NI IN TENSION, Journal of the mechanics and physics of solids, 43(6), 1995, pp. 869-895
Citations number
13
Categorie Soggetti
Physics, Condensed Matter",Mechanics
ISSN journal
00225096
Volume
43
Issue
6
Year of publication
1995
Pages
869 - 895
Database
ISI
SICI code
0022-5096(1995)43:6<869:ODOTPB>2.0.ZU;2-2
Abstract
Uniaxial tension experiments were performed on single crystals of Cu-1 3.95 wt% Al-3.93 wt% Ni. Three specimens were prepared with tension ax es in directions that were chosen based on Schmid law calculations usi ng the 96 possible Austenite-Martensite (A-M) interface orientations i n this alloy. Specimen number one was chosen to have a tensile axis of [2,43,1,0] which results in a very near minimum value for its predict ed tension transformation stress. Specimen number two was oriented 15 degrees from [111] direction and has a [1,1,1.73] tensile axis directi on. The third specimen has the [111] direction as its tensile axis, wh ich is the direction of maximum tensile transformation stress. A stron g relationship is found between the mechanical behavior of the specime ns in tension and their observed microstructure. Specimen one exhibits an extremely flat stress plateau during transformation and almost no hysteresis. The microstructure observed in this specimen consists of t wo nearly perpendicular A-M interfaces that interact to form an X-stru cture that results in a purely uniaxial deformation. This microstructu re is completely reversible and seems to present no restriction on the motion of either interface. Specimen two was observed to have only a single A-M interface after transformation. This interface appears to p reclude the formation of any other interfaces. Specimen three required five times the normal stress of that needed to transform specimen one . This specimen also exhibited a large amount of hysteresis. The micro structure observed consisted of two A-M interface systems that meet to form wedges. Because the interfaces must end at the wedge apex, the f ormation of the wedges resulted in a kinematic coupling between the tw o A-M interface systems. The amount of coupling between the interfaces in the microstructure correlates to the amount of hysteresis observed .