Shock Hugoniot of porous nanosized nickel.

Autor: Dolgoborodov, A. Yu., Ananev, S. Yu., Yakushev, V. V., Rostilov, T. A., Ziborov, V. S., Kuskov, M. L., Zhigach, A. N., Kirilenko, V. G., Pirog, V. A., Grishin, L. I., Valyano, G. E.
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Zdroj: Journal of Applied Physics; 3/28/2022, Vol. 131 Issue 12, p1-8, 8p
Abstrakt: The shock compression of porous nickel from nanosized particles nNi was studied at a pressure range of 4–61 GPa. The average size of the nNi particles was 50 nm, and the porosity of the samples was 50%. Plane shock waves in the samples were generated by the impact of aluminum plates accelerated to velocities ranging from 0.8 to 5 km/s. Laser interferometry was used to monitor particle velocity histories at the interface between the samples and water or LiF windows. The data obtained at pressures below 8 GPa showed a complex shock wave profile with the formation of an elastic precursor wave. The shock Hugoniot and data on the expansion isentropes were obtained. The Hugoniot of nanosized nNi coincided within the experimental errors with the Hugoniot of micron-sized nickel. The Hugoniot calculated on the basis of the equation of state for porous nickel was in good agreement with that of experimental data. It has been established that in the middle pressure range (20–35 GPa), the expansion isentropes in the "pressure–particle velocity" coordinates become noticeably flatter with a significant increase in the particle velocity. The reason for this phenomenon is still unclear. An assumption was made about the onset of particle melting upon reaching pressures above 15 GPa. [ABSTRACT FROM AUTHOR]
Databáze: Complementary Index