In the preceding chapter, we discussed the geometric properties of the present configuration κt under the assumption that the parameter t describing temporal changes of the body is kept fixed. That is, the motion function \(\vec \chi \) is considered to be a deformation map \(\vec \chi (\cdot ,t)\). Now, we turn our attention to the problem in the case of motion, that is, where the function
... [Show full abstract] \(\vec \chi \) is treated as the map \(\vec \chi (\vec X,\cdot )\) for a fixed point \(\vec X\). We assume that the mapping \(\vec \chi (\vec X,\cdot )\) is twice differentiable.