Computational Contact and Impact Mechanics: Fundamentals of by Tod A. Laursen

By Tod A. Laursen

This booklet comprehensively treats the formula and finite aspect approximation of touch and effect difficulties in nonlinear mechanics. meant for college kids, researchers and practitioners attracted to numerical strong and structural research in addition to engineers and scientists facing applied sciences within which tribological reaction needs to be characterised, the ebook comprises an introductory yet targeted review of nonlinear finite aspect formulations prior to facing touch and impression in particular. themes encompassed comprise continuum mechanics, mathematical constitution, variational framework and finite aspect implementations linked to contact/impact interplay. also, very important and at the moment rising study themes in computational touch mechanics are brought, encompassing such themes as tribological complexity, conservative therapy of inelastic influence interplay and novel spatial discretization innovations.

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Extra info for Computational Contact and Impact Mechanics: Fundamentals of Modeling Interfacial Phenomena in Nonlinear Finite Element Analysis

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61). pt, but relies upon it for its own definition. pt to be a function of reference coordinates X, the framework is inherently Lagrangian. 117) are written in terms of reference quantities, clearly exposes the structure of the problem to be approximated. pt (0). 84), one can then write 8Uij 8XJ 8 [1 = 8XJ JPuFjI ] 1 8J 8FkK = - J2 8FkK 8XJ Pi/Fp 1 8 + J 8XJ [Pi/FjI]. 122) +FkNFN~8M3FilFj2] . Noting that J = eijkFilFj2Fk3, one may easily reason that eijkFiNFjMFkO = are equal (since this would represent the determinant of a rank deficient matrix).

3 Stress Definitions Appropriate for Large Deformations As might be suspected, increased generality in the definition of stress is necessary in the context of large deformations. A convenient approach to a broader understanding of this concept is to begin with the Cauchy stress tensor u, and to associate this object with the spatial configuration. 1. In the current context, we interpret the components of u, denoted as O"ij, as representing forces per unit areas in the spatial configuration at a given spatial point :1:.

One may note in particular that S is a symmetric tensor, while P is not symmetric in general. 87), are noteworthy in that the Jacobian of the transformation J appears in both. 2 The IBVP in the Finite Strain Case 27 a geometric interpretation of the relation between S and eT in particular, one cannot describe it as being a simple pull-back operation between the current and reference configurations (due to the presence of J). However, this interpretation can be given in terms of another spatial tensor, the Kirchhoff stress T, which is also useful in theories of finite strain plasticity to be discussed subsequently.

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