The effect of hydrogen on the variation with temperature of internal friction (Q ΓI ) and elastic modulus (E) of a number of Ti-based alloys has been studied in the Hz and kHz frequency ranges. A relaxation peak of internal friction with a high degree of relaxation (Q ΓI max $ 10 Γ1 ) and with a DE
Low-frequency internal friction of hydrogen-free and hydrogen-doped NiTi alloys
β Scribed by F.M. Mazzolai; A. Biscarini; B. Coluzzi; G. Mazzolai; E. Villa; A. Tuissi
- Publisher
- Elsevier Science
- Year
- 2007
- Tongue
- English
- Weight
- 431 KB
- Volume
- 55
- Category
- Article
- ISSN
- 1359-6454
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β¦ Synopsis
The internal friction (IF) and Young's modulus of the Ni 50.8 Ti 49.2 shape memory alloy have been measured as a function of temperature (130 K < T < 335 K) by a dynamic mechanical analyser at various strain amplitudes and frequencies. Besides the one associated with the austenite/martensite transformation, several other IF peaks have been observed both in the hydrogen-free and in the hydrogen-doped states of the material. Some of these peaks are non-thermally activated processes caused by stress-assisted hysteretic motions of twin boundaries and dislocations; some others represent thermally activated relaxations caused by reorientation of hydrogen elastic dipoles or by stress-induced motions of twin boundaries interacting with hydrogen. The present low-frequency measurements provide new information concerning the amplitude and frequency dependences of the damping processes, thus throwing new light on their structural mechanisms.
π SIMILAR VOLUMES
## Low frequency internal friction has been measured for vanadium. niobium and tantaium containing various amounts of hydrogen over the temperarure range from -190 to 1OO'C. The behaviour of the precipitation peak is similar for thz three metals. The precipitation peak decreases its height and new
It has been found that aging at room temperature or previous straining of hydrogen charged 1020 steel causes an internal friction peak at 105Β°K to appear, reach a maximum, decrease and finally disappear. This peak has been explained by a model which involves the dragging along of hydrogen atmosphere