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Thermodynamics of Shock Waves

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Shock Wave Compression of Condensed Matter

Part of the book series: Shock Wave and High Pressure Phenomena ((SHOCKWAVE))

Abstract

The use of continuum thermodynamic parameters (i.e. quantity per gram) doesn’t change thermodynamic equations. Therefore, the continuum thermodynamic state parameters will be used. Following Callen [1], the first law of thermodynamics using continuum variables for E, v, Q is:

$$ \mathrm{ dE} = \mathrm{ d}{{\mathrm{ W}}_1} + \mathrm{ dQ} = - \mathrm{ P} \ \mathrm{ dv} + \mathrm{ dQ} $$

which states that the change in internal energy is equal to work done plus heat flow. In general the first law can include dissipative forces, which allows for irreversible as well as reversible processes. Thermodynamics used in this class is the description of equilibrium final states.

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Authors and Affiliations

  1. Energetics Technology Center, St. Charles, Maryland, 20603, USA

    Jerry W. Forbes

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  1. Jerry W. Forbes
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© 2012 Springer-Verlag Berlin Heidelberg

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Forbes, J.W. (2012). Thermodynamics of Shock Waves. In: Shock Wave Compression of Condensed Matter. Shock Wave and High Pressure Phenomena. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-32535-9_5

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  • DOI: https://doi.org/10.1007/978-3-642-32535-9_5

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  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-642-32534-2

  • Online ISBN: 978-3-642-32535-9

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