Study of the Microstructure, Crystallographic Structure and Thermal Stability of Al–Ti–Nb Alloys Produced by Selective Electron Beam Alloying
- Authors: Valkov S.1, Neov D.2, Bezdushnyi R.3, Beskrovnyi A.2, Kozlenko D.2, Petrov P.1
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Affiliations:
- Institute of Electronics
- Frank Laboratory of Neuron Physics
- Department of Solid State Physics and Microelectronics, Faculty of Physics
- Issue: Vol 12, No 3 (2018)
- Pages: 436-441
- Section: Article
- URL: https://journals.rcsi.science/1027-4510/article/view/195332
- DOI: https://doi.org/10.1134/S1027451018030187
- ID: 195332
Cite item
Abstract
This paper aims an investigation of the microstructure and crystallographic structure as well as the thermal stability of Al–Ti–Nb formed by selective electron beam surface alloying. The fabrication of the samples has been carried out using circular sweep mode, as two velocities of the sample movement have been chosen: V1 = 1 cm/s and V2 = 0.5 cm/s. The studied microstructure and crystallographic structure have been investigated by X-ray diffraction (XRD) and Scanning electron microscopy (SEM) respectively. The thermal behavior of the obtained surface alloys are evaluated by the coefficient of thermal expansion (CTE) which has been evaluated by neutron diffraction measurements at high temperature. The results show that in the earlier stages of formation, the microstructure of the intermetallic phase is mainly in the form of coarse fractions, but at the following moments they dissolve, forming separated alloyed zone and base Al substrate as the alloyed zone consists of fine (Ti,Nb)Al3 particles dispersed in the Al matrix with small amount of undissolved intermetallic fractions. Formation of preferred crystallographic orientation as a function of the speed of specimen motion has not been observed. The performed neutron diffraction measurements show that the lattice parameters of the obtained intermetallic (Ti,Nb)Al3 are less upshifted in comparison to pure Al. It has been found that the aluminium lattice is much more unstable at high temperatures than that of the intermetallic phase. The CTE for the intermetallic phase is 8.70 ppm/K for a axis and 7.75 ppm/K for c axis respectively while considering Al it is 12.95 ppm/K.
About the authors
S. Valkov
Institute of Electronics
Author for correspondence.
Email: stsvalkov@gmail.com
Bulgaria, Sofia, 1784
D. Neov
Frank Laboratory of Neuron Physics
Email: stsvalkov@gmail.com
Russian Federation, Dubna, Moscow Region
R. Bezdushnyi
Department of Solid State Physics and Microelectronics, Faculty of Physics
Email: stsvalkov@gmail.com
Bulgaria, Sofia, 1164
A. Beskrovnyi
Frank Laboratory of Neuron Physics
Email: stsvalkov@gmail.com
Russian Federation, Dubna, Moscow Region
D. Kozlenko
Frank Laboratory of Neuron Physics
Email: stsvalkov@gmail.com
Russian Federation, Dubna, Moscow Region
P. Petrov
Institute of Electronics
Email: stsvalkov@gmail.com
Bulgaria, Sofia, 1784
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