Pyrometric measurement of the temperature of shocked molybdenum

Physical Review B - Condensed Matter and Materials Physics

Volumn 77, Issue 13, 2008, Pages

  Seifter, A ^a   Swift, D C ^b  

^a LOS ALAMOS NATIONAL LABORATORY   (United States)

^b LAWRENCE LIVERMORE NATIONAL LABORATORY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 42049109343     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.77.134104     Document Type: Article

References (33)

1. Y. M. Gupta (unpublished).
2. V. W. Yuan, J. D. Bowman, D. J. Funk, G. L. Morgan, R. L. Rabie, C. E. Ragan, J. P. Quintana, and H. L. Stacy, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.94.125504 94, 125504 (2005).
3. D. C. Swift, A. Seifter, D. B. Holtkamp, V. W. Yuan, D. Bowman, and D. A. Clark, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.77.092102 77, 092102 (2008).
4. R. L. Gustavsen and Y. M. Gupta, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.356176 75, 2837 (1994).
5. S. B. Kormer, M. V. Sinitsyn, G. A. Kirilliv, and V. D. Urlin, Sov. Phys. JETP SPHJAR 0038-5646 21, 689 (1965).
6. A. Seifter, K. Boboridis, D. A. Clark, R. B. Corrow, D. B. Holtkamp, C. W. McCLuskey, G. L. Morgan, J. R. Payton, P. Quintana, C. E. Ragan, P. Rodriguez, H. L. Stacy, W. S. Vogan, V. W. Yuan, and A. W. Obst, in Proceedings of the Ninth International Symposium on Temperature Measurements in Industry and Science (TEMPMEKO), edited by, D. Zvizdic,,, L. G. Bermanec,,, T. Veliki,, and, T. Stasic, (Laboratory for Process Measurement, Faculty of Mechanical Engineering and Naval Architecture, Zagreb, Croatia, 2004), Vol. 2, p. 1185.
7. C. A. Forest, J. Vorthman, L. Bennet, and R. L. Rabie, Los Alamos National Laboratory Technical Report No. LA-UR-98-3783, 1998 (unpublished).
8. J. R. Asay and M. Shahinpoor, High-Pressure Shock Compression of Solids (Springer, New York, 1992), pp. 32-34.
9. L. M. Barker and R. E. Hollenbach, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.1660986 43, 4669 (1972).
10. Chalcogenide glass fiber (C2) from Amorphous Materials Inc., Garland, TX, (www.amorphousmaterials.com).
11. Polymicro Technologies, Phoenix, AZ (www.polymicro.com).
12. One injection fiber in the center surrounded by seven receiving fibers each 100 μm in diameter.
13. P. L. Hereil and C. Mabire, J. Phys. IV JPICEI 1155-4339 10, Pr9-749 (2000).
14. A. Seifter, K. Boboridis, J. R. Payton, and A. W. Obst, in Proceedings of the 26th International Congress on High-Speed Photography and Photonics, edited by, D. L. Paisley,,, S. Kleinfelder,,, D. R. Snyder,, and, B. J. Thompson, (Los Alamos National Laboratory, Los Alamos, NM, 2005), Vol. 5580, pp. 93-105.
15. D. B. Holtkamp (unpublished).
16. D. C. Swift, C. A. Forest, D. A. Clark, W. T. Buttler, M. Marr-Lyon, and P. Rightley, Rev. Sci. Instrum. RSINAK 0034-6748 10.1063/1.2746769 78, 063904 (2007).
17. D. C. Swift, Los Alamos National Laboratory Report No. LA-UR-07-2051, 2007 (unpublished).
18. Program and Manuals for lagc1d Program (Wessex Scientific, Perth, 2006).
19. Program and Manuals for eul2d Program (Wessex Scientific, Perth, 2006).
20. D. J. Steinberg, Lawrence Livermore National Laboratory Technical Report No. UCRL-MA-106439, 1996 (unpublished).
21. K. S. Holian, Los Alamos National Laboratory Technical Report No LA-10160-MS-v.1C, 1984 (unpublished).
22. D. J. Steinberg, S. G. Cochran, and M. W. Guinan, J. Appl. Phys. 51, 1498 (1980). 0021-8979
23. A. Seifter and A. W. Obst, Int. J. Thermophys. IJTHDY 0195-928X 10.1007/s10765-007-0191-1 28, 934 (2007).
24. J. H. Gladstone and T. P. Dale, Philos. Trans. R. Soc. London PTRSAV 0370-2316 10.1098/rstl.1863.0014 153, 317 (1863).
25. At a pressure of 200 kbar in the anvil, the reflectivity R2 is less than 0.1%. It increases to 0.25% at 500 kbar and to 0.5% at 1 Mbar.
26. E. D. Palik, Handbook of Optical Constants of Solids (Academic, New York, 1990).
27. R. Gardon, J. Am. Ceram. Soc. JACTAW 0002-7820 10.1111/j.1151-2916.1956. tb15833.x 39, 278 (1956).
28. V. Vujnovic and B. Grzeta, Fizika (Zagreb) FZKAAA 0015-3206 4, 173 (1972).
29. The normal spectral emissivity for a flat surface is obtained by ε = 4 n1 n2 (n1 + n2) 2 + k22, with n1 and n2 the indices of refraction of the anvil and the sample, respectively, and k2 is the extinction coefficient of the sample.
30. The 10-3 Torr vacuum is intended to provide the same experimental conditions as for the NRS experiments (avoiding drag forces on the Al flyer plate). This vacuum is not low enough to prevent bright emissions from the shocked air.
31. D. C. Swift, A. Seifter, D. B. Holtkamp, and D. A. Clark, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.76.054122 76, 054122 (2007).
32. For both calculations (with and without strength), the temperature at 24.8 GPa is about 55 K lower than that at 27.1 GPa. The measured data point at 24.8 GPa is 79±35 K lower than that at 27.1 GPa.
33. M. D. Wilke, 2007 (private communication).