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Titlebook: Configurational Forces as Basic Concepts of Continuum Physics; Morton E. Gurtin Book 2000 Springer Science+Business Media New York 2000 Co

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樓主: Thoracic
11#
發(fā)表于 2025-3-23 10:19:21 | 只看該作者
12#
發(fā)表于 2025-3-23 14:17:45 | 只看該作者
Ruth Stock-Homburg,Lea Heitlingermulation that allows for thermal variations associated with the transfer of heat. The treatment is nonclassical; it accounts for configurational working and heating associated with the transfer of material to a migrating control volume.
13#
發(fā)表于 2025-3-23 18:18:13 | 只看該作者
Transformation der Sicherheitspolitikes . and . are inertial. Then . has the form (7-1 ). I now characterize . through the equivalence of inertial force and temporal changes in momentum, and, knowing ., . is determined through the equivalence of inertial working and temporal changes in kinetic energy.
14#
發(fā)表于 2025-3-23 22:20:19 | 只看該作者
Transformationsprozesse im Vergleichterms of displacement. The working now has the form . with . and . velocity fields for . and ., and with . and ., respectively, corresponding time derivatives of . following the evolutions of . and .. (The field . is defined by (10-4) with . replaced by . and transforms in the same manner as do . an
15#
發(fā)表于 2025-3-24 05:48:26 | 只看該作者
16#
發(fā)表于 2025-3-24 07:16:44 | 只看該作者
17#
發(fā)表于 2025-3-24 11:10:27 | 只看該作者
J?rg von Ditfurth,Tobias LinzmaierTo characterize the manner in which configurational forces perform work, a means of capturing the kinematics associated with the transfer of material is needed. I accomplish this with the aid of three notions, none of which is a standard. The first, that of material observers, has been examined in Chapter 2. The other two notions are:
18#
發(fā)表于 2025-3-24 18:40:24 | 只看該作者
19#
發(fā)表于 2025-3-24 20:53:18 | 只看該作者
Transformation der KernexekutiveIf the external body force . is inertial, then, granted an inertial observer, . with ρ(.) ≥ 0, assumed smooth, the . in the reference configuration. (ρ = 0 characterizes quasi-static situations.) Then, by (5-20), . and the equations of motion (3-6a) and (5-10) take the form
20#
發(fā)表于 2025-3-25 03:03:50 | 只看該作者
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