Abstract
As repeatedly mentioned earlier, see Subsections 2.3.6 and 2.3.9, the tensors of finite strain can be replaced by a linear strain tensor \( \hat \varepsilon \) provided that the components of the gradient of the displacement vector ∇u are small. The latter is equivalent to the components of tensor \( \hat \varepsilon \) and the rotation vector ω being small
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© 2005 Springer-Verlag Berlin Heidelberg
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Lurie, A.I., Belyaev, A. (2005). The constitutive law in the linear theory of elasticity. In: Theory of Elasticity. Foundations of Engineering Mechanics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-26455-2_3
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DOI: https://doi.org/10.1007/978-3-540-26455-2_3
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-540-24556-8
Online ISBN: 978-3-540-26455-2
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