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Titlebook: Analysis and Thermomechanics; A Collection of Pape Bernard D. Coleman,Martin Feinberg,James Serrin Book 1987 Springer-Verlag Berlin Heidelb

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Messungen am MPEG-2-Transportstrom,placement vector remains parallel to the .-axis, and if the temperature .(., .) and the displacement .(., .) depend upon . and the time . only, the linear theory of thermoelasticity implies that .(., .) and .(., .) satisfy the energy equation.and the equation of motion
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On the Failure of the Maximum Principle in Coupled Thermoelasticity,placement vector remains parallel to the .-axis, and if the temperature .(., .) and the displacement .(., .) depend upon . and the time . only, the linear theory of thermoelasticity implies that .(., .) and .(., .) satisfy the energy equation.and the equation of motion
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Continua with Latent Microstructure, lectures [2] at the Banach Institute, Warsaw, and reported later in a paper [3]. Further arguments in favour of the model can be found in [4], where, in particular, the case of a fluid with microstructure is studied in some detail.
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Some Surface Defects in Unstressed Thermoelastic Solids,, p. 406], things which seem to me more reminiscent of the multiple births we commonly describe by other words, like triplets or sextuplets. Whatever one calls them, they are of physical interest, as are other somewhat similar phenomena. My purpose is to present elements of thermoelasticity theory for things of this general kind.
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Basic Theory of Small-Amplitude Waves in a Constrained Elastic Body,gation and growth of acceleration waves of arbitrary shape in an elastic body experiencing one or two constraints. Subsequently . & . [1980] have discussed the energetics of acceleration waves in an arbitrarily constrained elastic body and, in the same context, an analysis of simple waves has been presented by . [1982].
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