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Most of the available network descriptions model the fibres essentially as uni-axial elements, thereby not explicitly considering the role of the bonds.
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In order to use the Kelly Tyson model, the fibre fragments of the samples should be fully saturated before failure of the matrix.
Most of the work is focused on modelling the fibre-yarn relationship, yarn tenacity, fault detection, compression, elastic properties and hand values of woven, nonwoven and knitted fabrics.
It is beyond all doubt that for an accurate finite element (FE) model a correct modelling of the fibre orientations and material properties is required.
The toughening mechanisms related to the fabric structure are studied by embedding a meso-scale model of the fibre architecture in the delamination zone into a macro-scale model of a DCB specimen.
A microscopic truss finite element is used to model the short fibre reinforcements.
The main problem in predicting the dynamics of these machines is to model the complicated fibre breaking process, since the refining process leads to a three-phase flow (solid wood, water and steam) between the stator and rotor.
For example a compact chromatin fibre will sediment more rapidly than a chromatin fibre that is unfolded or interspersed with many disruption and previously we have used the sedimentation properties to model the chromatin fibre structure [19].
These coupled analyses have revealed the discontinuous character of the microfibrillar structure and have enabled a microstructural model for the fibre to be proposed.
A three-dimensional periodic unit cell is established with the matrix described by a nonlinear viscoelastic model and the fibre by an elastic one.
The refinement of the pilus structure was performed using a 3D model of the fibre composed of 2 averaged subunits.
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