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When the matrix is stressed, the cells develop isometric tension which is equal to the mechanical tensional force exerted upon them by the ECM [ 24].
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The power of the Kronecker product of matrices in this application is stressed.
Note that the term η(i) in (2), which accounts for IBI in non-ZP guard interval systems, is removed by the joint operation of matrices T and R. It should be stressed that the guard interval length must be at least the channel order in order to avoid IBI, i.e., L gi ≥ L - 1 [23].
However, it should be stressed that in our studies only the initial matrix compositions are specified.
When the polymer matrix is deformed, stress is transferred by interfacial stress transfer to the two outer graphene layers (both will be A-type layers) as has been found before for monolayer and bilayer specimens.
A remarkable relation between derived stresses and shear strength of respective parent matrix is discovered: plane stress in the diffusion zone amounts consistently to about 80% of the ideal shear strength.
The CNTs strengthening effect on the matrix is shown through lower stresses at the CNTs and matrix interface in comparison to the applied stress.
During this process, the matrix is under compressive stress.
The viscoelastic behavior of the polymeric matrix is considered as stress-dependent and thermo-rheologically complex.
To account for the importance of fiber architecture, the fracture process zone (FPZ) characterised by discrete embedded reinforcement and cracking matrix, is of discontinuous bridging stresses.
In the formulation discussed in this article, the same matrix is used to relate stress to constant stress parameters, and strain to constant strain parameters.
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