Dynamic Compression of Liquids from Measurements on Strong Shock Waves
1.These three relations, called the Rankine‐Hugoniot equations, are derived in any text on shock‐wave hydrodynamics. See, for example, R. Courant and K. O. Friedrichs, Supersonic Flow and Shock Waves (Interscience Publishers, Inc., New York, 1948).
2.J. M. Walsh and R. H. Christian, Phys. Rev. 97, 1544 (1955). Equation (6) is an analytical fit of 24ST aluminum data between and and is based on more extensive data than given in the preceding reference.
3.R. Schall, Z. Angew. Phys. 2, 252–254 (1950).
4.Dapoigny, Kieffer, and Vodar, Acad. Sci. 215–217 (1954).
5.J. G. Kirkwood and E. W. Montroll, “The pressure wave produced by an underwater explosion, II,” Office of Scientific Research and Development (OSRD), No. 670 (June, 1942).
6.J. G. Kirkwood and J. M. Richardson, “The pressure wave produced by an underwater explosion, III,” Office of Scientific Research and Development (OSRD), No. 813 (August, 1942).
7.Richardson, Arons, and Halverson, J. Chem. Phys. 15, 785 (1947).
8.W. Doering and H. Burkhardt, “Beitrage zur theorie der detonation,” Air Materiel Command, Wright Field, Ohio, Air Documents Division.
9.H. G. Snay and J. H. Rosenbaum, NAVORD Report 2383, “Shockwave parameters in fresh water for pressures up to 95 kilobars,” U.S. Naval Ordnance Laboratory, White Oak, Maryland (April, 1952). These workers also employed Bridgman ice VII data to estimate possible (i.e., provided the freezing time is sufficiently short) effects of shock‐induced freezing for water. Their results quoted above are for water which remains liquid; their freezing calculation is mentioned in Sec. III.
10.P. W. Bridgman, J. Chem. Phys. 9, 794 (1941).
11.P. W. Bridgman, Proc. Am. Acad. Arts Sci. 74, 399 (1942).
12.G. C. Kennedy, Am. J. Sci. 248, 540 (1950).
13.H. Schardin, “Problem der detonation,” Schriften der Deuts Akad. Luft. (1941).
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