Numéro
J. Phys. Colloques
Volume 43, Numéro C4, Décembre 1982
ICOMAT-82
International Conference on Martensitic Transformations
Page(s) C4-231 - C4-236
DOI https://doi.org/10.1051/jphyscol:1982430
ICOMAT-82
International Conference on Martensitic Transformations

J. Phys. Colloques 43 (1982) C4-231-C4-236

DOI: 10.1051/jphyscol:1982430

TRANSFORMATION BEHAVIOR OF Ti50Ni47Fe3 ALLOY :
I. INCOMMENSURATE AND COMMENSURATE PHASES

C.M. Hwang, M. Meichle, M.B. Salamon et C.M. Wayman

University of Illinois, Urbana, Illinois 61801, U.S.A.


Abstract
The transformation behavior of TiNiFe alloys of nominal composition Ti50Ni47Fe3 has been studied by transmission electron microscopy and diffraction, and electrical resistance measurements, between room temperature and -196°C. Based on the present results and complementary neutron and x-ray diffraction data, charge density wave (CDW) phenomena and associated phase transitions were found to be involved in the "premartensitic" behavior of the Ti50Ni47Fe3 alloys. The crystal structure of the high temperature parent phase was confirmed to be the CsCl(B2) structure. Upon cooling below room temperature, 1/3(110) and 1/3(111) superlattice reflections appeared, coincident with the onset of an electrical resistance anomaly (increase). The "1/3" superlattice reflections were observed to intensify with decreasing temperature, and close inspection showed that such reflections deviate slightly from the exact 1/3 positions relative to the parent CsCl structure, suggesting the formation of an incommensurate superlattice over a 12°C temperature range. The appearance of the "1/3" superlattice reflections is interpreted to be associated with the formation of CDW's. A second "premartensitic" effect was found to occur approximately 12°C below the onset of the initial "normal-to-incommendurate" transition. This subsequent phase change involves a structural transition from a "distorted" CsCl parent to a rhombohedral product, during which the "1/3" superlattice reflections are shifted to precise 1/3 positions. The rhombohedral distortion is effected by a homogeneous expansion along <111> directions, allowing the lattice and CDW's to lock-in and become commensurate.