Abstract
The application of an external force to a body is, by definition a dynamic process. However, when the rate of change of the applied forces is low, one can consider the process of deformation as a sequence of steps in which the body can be considered in static equilibrium. Figure 2.1 shows how the distance between the atoms changes upon the application of an external force F. For each of the stages of deformation shown in Figs. 2.1(b) and 2.1(c), the body can be considered under static equilibrium and one can apply the methods of mechanics of materials to determine the internally-resisting stresses (by the method of sections). Hence, a section made at AA or BB will yield identical stresses.
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Meyers, M.A., Murr, L.E. (1983). Propagation of Stress Waves in Metals. In: Blazynski, T.Z. (eds) Explosive Welding, Forming and Compaction. Springer, Dordrecht. https://doi.org/10.1007/978-94-011-9751-9_2
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