The bulk modulus and Poisson's ratio of “incompressible” materials
By P. H. Mott, J. Dorgan, C. M. Roland. 2008
330 citations recorded by the source corpus.
Subfields: Biomedical Engineering, Mechanical Engineering, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/e662f05e75b6e8d8c6c6ec8d0b0fd29bf1c63fa4
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In Biomedical Engineering
In Mechanical Engineering
In Mechanics of Materials
Citations in the corpus
- On the feasibility of pentamode mechanical metamaterials (2012, background): “In three dimensions, one either needs materials with anisotropic mass density tensors [3,7,8,9] or pentamode materials [3,10,11,12] to implement the counterpart of invisibility cloaks or other devices.”
- Limits to Poisson's ratio in isotropic materials—general result for arbitrary deformation (2009, background): “ discontinuity. This common point is defined as ν*(y,) at Hy**/I ; it divides Poisson’s ratio into the ranges −1 < ν ≤ ν* and ν* ≤ ν < . Since the upper span corresponds to experimental data [28,29], it is of interest to determine the lower limit ν*. This point is found when the two roots are ”