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Titlebook: Irreversible Aspects of Continuum Mechanics and Transfer of Physical Characteristics in Moving Fluid; Symposia Vienna, Jun H. Parkus (Vice-

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樓主: 夸大
21#
發(fā)表于 2025-3-25 05:56:36 | 只看該作者
22#
發(fā)表于 2025-3-25 08:23:59 | 只看該作者
23#
發(fā)表于 2025-3-25 12:14:18 | 只看該作者
TIP Has Many Faces,, the so-called general non-linear continuum theory based on the Clausius-Duhem inequality and a recent approach which uses instead a fundamental inequality which follows from a thrifty application of the Second Law. Merits and shortcomings of these theories are discussed. It is also explained that
24#
發(fā)表于 2025-3-25 19:19:29 | 只看該作者
25#
發(fā)表于 2025-3-25 21:46:28 | 只看該作者
Couple-Stresses in the Theory of Thermoelasticity,each other: the displacement vector . and the rotation vector ...Basing on the thermodynamics of irreversible processes the constitutive equations and the expanded equation of heat conductivity for an isotropic medium are derived..The author succeeded in obtaining a basic system of differential equa
26#
發(fā)表于 2025-3-26 00:42:36 | 只看該作者
The Notion of State and Its Implications in Thermodynamics of Inelastic Solids,te space is finite dimensional, thermomechanical behavior of the material in the range of finite deformations can be represented by differential equations. The nature of this representation and the restrictions placed upon it by the second law of thermodynamics are discussed.
27#
發(fā)表于 2025-3-26 07:13:17 | 只看該作者
28#
發(fā)表于 2025-3-26 09:16:51 | 只看該作者
Thermodynamics and Wave Propagation in Non-Linear Materials with Memory,rium thermodynamics plays a basic role in this infant subject, we have prepared for this symposium a survey of its most developed part: the theory of one-dimensional waves in materials which do not conduct heat but have long-range viscoelastic memory.
29#
發(fā)表于 2025-3-26 13:06:13 | 只看該作者
30#
發(fā)表于 2025-3-26 18:06:09 | 只看該作者
The Notion of State and Its Implications in Thermodynamics of Inelastic Solids,te space is finite dimensional, thermomechanical behavior of the material in the range of finite deformations can be represented by differential equations. The nature of this representation and the restrictions placed upon it by the second law of thermodynamics are discussed.
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