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Plane One-Dimensional Shock Waves

  • Jerry W. Forbes
Chapter
Part of the Shock Wave and High Pressure Phenomena book series (SHOCKWAVE)

Abstract

A plane one-dimensional shock wave goes from one stress and compression level (usually zero) to a higher stress and compression level in an almost discontinuous jump as a function of time as shown in Fig. 2.1. It can have a rise time (usually small fractions of a microsecond) to the front. It travels faster than the speed of sound in the medium ahead of the shock (George Duvall notes from shock wave class given at WSU, Personal communication, 1969) [1] (i.e. shock waves are supersonic).

Keywords

Shock Wave Shock Front Shock Wave Front Shock Velocity Compression Level 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

References

  1. 1.
    G.E. Duvall, G.R. Fowles, High Pressure Physics and Chemistry, vol. 2, ed. by R.S. Bradley (Academic, New York, 1963)Google Scholar
  2. 2.
    S.P. Marsh (ed.), LASL Shock Hugoniot Data (University of California Press, Berkeley, 1980)Google Scholar
  3. 3.
    D. Bancroft, E.L. Petersen, S. Minshall, Polymorphism of Iron at High Pressure. J. Appl. Phys. 27(3), 291 (1956)CrossRefGoogle Scholar
  4. 4.
    S.B. Segletes, Thermodynamic stability of the Mie-Grueneisen equation of state and its relevance to hydrocode computations. J. Appl. Phys. 70, 5, pp 2489–2499 (1991)Google Scholar

Copyright information

© Springer-Verlag Berlin Heidelberg 2012

Authors and Affiliations

  1. 1.Energetics Technology CenterSt. CharlesUSA

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