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29144437799
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0021-8979 10.1063/1.2132521
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W. S. Vogan, W. W. Anderson, M. Grover, J. E. Hammerberg, N. S. P. King, S. K. Lamoreaux, G. Macrum, K. B. Morley, P. A. Rigg, G. D. Stevens, W. D. Turley, L. R. Veeser, and W. T. Buttler, J. Appl. Phys. 0021-8979 10.1063/1.2132521 98, 113508 (2005).
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W. T. Buttler, M. B. Zellner, R. T. Olson, P. A. Rigg, R. S. Hixon, J. E. Hammerberg, A. W. Obst, and J. R. Payton, J. Appl. Phys., 0021-8979 101, 063547 (2007).
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6
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34547275695
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J. R. Asay, Report No. SAND-76-0542, 1976.
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Asay, J.R.1
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34547315534
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Partial melt-on-release refers to a region of mixed solid and liquid material, not full melt-on-shock.
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Partial melt-on-release refers to a region of mixed solid and liquid material, not full melt-on-shock.
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12
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1542412279
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edited by Y. M.Gupta (North-Holland Physics Publishing, Spokane, WA
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P. Elias and P. Chapron, in Experimental Techniques for Measuring Mass Ejection from Shock-Loaded Metallic Sample, edited by, Y. M. Gupta, (North-Holland Physics Publishing, Spokane, WA, 1985), p. 645.
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Experimental Techniques for Measuring Mass Ejection from Shock-Loaded Metallic Sample
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Elias, P.1
Chapron, P.2
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34547349761
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edited by J. R.Asay, R. A.Graham, and G. K.Straub (North-Holland Physics Publishing, Sante Fe, NM
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P. Andriot, P. Chapron, V. Lambert, and F. Olive, in Influence of Melting on Shocked Free Surface Behavior Using Doppler Laser Interferometry and X-Ray Densitometry, edited by, J. R. Asay, R. A. Graham, and, G. K. Straub, (North-Holland Physics Publishing, Sante Fe, NM, 1983), p. 276.
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34547249033
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Report No. ASME B46.1-2002, 2002.
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(2002)
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17
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34547358702
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To reduce variables related to target fabrication, the materials are machined by the same individual in the materials science division (MST-7) of LANL, F. Garcia.
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To reduce variables related to target fabrication, the materials are machined by the same individual in the materials science division (MST-7) of LANL, F. Garcia.
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22
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34547275694
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The dynamic volume density (ρ ) is the apparent volume density that encompases the density of ejecta particles (similar to the density of pure Sn, 7.287 g cm3) as well as regions of empty space.
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The dynamic volume density (ρ ) is the apparent volume density that encompases the density of ejecta particles (similar to the density of pure Sn, 7.287 g cm3) as well as regions of empty space.
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23
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34547373626
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Dynasen
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Dynasen, www.dynasen.com, Goleta, CA.
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25
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34547249032
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The OHV ejecta signals are characterized by single wavelength Mie scattering. If the scattering cross section is strong enough, the OHV diagnostic may not even scatter light from the free surface.
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The OHV ejecta signals are characterized by single wavelength Mie scattering. If the scattering cross section is strong enough, the OHV diagnostic may not even scatter light from the free surface.
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26
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0037113008
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0021-8979 10.1063/1.1515125
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D. S. Sorenson, R. W. Minich, J. L. Romero, T. W. Tunnell, and R. M. Malone, J. Appl. Phys. 0021-8979 10.1063/1.1515125 92, 5830 (2002).
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Minich, R.W.2
Romero, J.L.3
Tunnell, T.W.4
Malone, R.M.5
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0031-9007 10.1103/PhysRevLett.89.285501
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B. L. Holian, T. C. Germann, J. Maillet, and C. T. White, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.89.285501 89, 285501 (2002).
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, vol.89
, pp. 285501
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Holian, B.L.1
Germann, T.C.2
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34547291648
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D. Hayes, Los Alamos National Lab (private communication).
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Hayes, D.1
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, vol.505
, pp. 93
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Hereil, P.L.2
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34547370280
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edited by S. C.Schmidt and N. C.Holmes (North-Holland Physics Publishing, Monterey, CA
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P. Chapron, P. Elias, and B. Laurent, in Experimental Determination of the Pressure Inducing Melting in Release for Shock-Loaded Metallic Sample, edited by, S. C. Schmidt, and, N. C. Holmes, (North-Holland Physics Publishing, Monterey, CA, 1987), p. 171.
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Experimental Determination of the Pressure Inducing Melting in Release for Shock-Loaded Metallic Sample
, pp. 171
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Laurent, B.3
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33
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34547297043
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Equation (8) relates the defect volume of triangular fly-cut grooves, Vd, to 12×L×W×4 Ra.
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Equation (8) relates the defect volume of triangular fly-cut grooves, Vd, to 12×L×W×4 Ra.
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34
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34547332591
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We observe that analysis of the surface with optical profilometry showed the most common groove frequency for the 16 μin surface finish was a factor of ≈1.4 higher than the 32 μin surface finish. The correlation of increased groove frequency with an decrease in ejecta production over the pressures spanned is interesting and warrants further investigation.
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We observe that analysis of the surface with optical profilometry showed the most common groove frequency for the 16 μin surface finish was a factor of ≈1.4 higher than the 32 μin surface finish. The correlation of increased groove frequency with an decrease in ejecta production over the pressures spanned is interesting and warrants further investigation.
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