Acoustic characteristics of Ni–Nb–Zr–H glassy alloys by ultrasonic shear waves
Source abstract
Abstract
Abstract The propagation characteristics of shear horizontally polarized (SH) waves passing through (Ni42Nb28Zr30)100–x Hx (x = 0–15.2) glassy alloys were investigated as a function of hydrogen content. With an increase in hydrogen content, the propagation time and main frequency of the receiving waves show increase and decrease, respectively, indicating expan‐ sion in average atomic distance which comes from solution of hydrogen. In sharp contrast to crystalline alloys, the decrease in damping ratio and the delay in phase with increasing hydrogen suggest a strong settlement of hydrogen into four‐coordination sites surrounded tetrahedrally by four Zr atoms and the resulting increase in dynamic elasticity, respectively. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Metallic Glasses and Amorphous Alloys · Thermodynamic and Structural Properties of Metals and Alloys · Glass properties and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (14)
Show source-provided references
1. 10.1016/j.actamat.2005.04.02310.1016/j.actamat.2005.04.023 ↗
2. 10.2320/matertrans.47.152310.2320/matertrans.47.1523 ↗
3. 10.1121/1.40186510.1121/1.401865 ↗
4. 10.1016/0041-624X(94)90035-310.1016/0041-624X(94)90035-3 ↗
5. Fukuhara M. · Acoust. Lett. · 1999 · 23 · 60
6. 10.1143/JJAP.33.289010.1143/JJAP.33.2890 ↗
7. 10.1016/S0009-2614(03)00241-010.1016/S0009-2614(03)00241-0 ↗
8. 10.1016/0022-5088(82)90005-410.1016/0022-5088(82)90005-4 ↗
9. 10.1016/0925-8388(94)01455-810.1016/0925-8388(94)01455-8 ↗
10. Fukuhara M. · Fusion Technol. · 1998 · 34 · 15110.13182/FST98-A61 ↗
11. 10.4131/jshpreview.7.64710.4131/jshpreview.7.647 ↗
12. 10.1002/(SICI)1099-0488(19990315)37:6<497::AID-POLB2>3.0.CO;2-L10.1002/(SICI)1099-0488(19990315)37:6<497::AID-POLB2>3.0.CO;2-L ↗
13. 10.1063/1.218915610.1063/1.2189156 ↗
14. 10.5254/1.353840210.5254/1.3538402 ↗