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On top of it we model the fiber associated material properties with an elastic Cosserat network.
In the model the fiber segments between rigid fiber-fiber bonds can be stretching, shearing and bending.
More specifically, the Bodies of Revolution (BOR) FDTD numerical simulation method will be used to model the fiber Bragg Grating (FBG) and the direct integration method will be employed to include the effect of Self Phase Modulation (SPM) in this model.
Under the DT model, the fiber orientation is given by a single delta function pointed in the direction of the primary eigenvector.
This is the first study to investigate and model the fiber bundle architecture of the pathologic supraspinatus throughout the muscle volume including the anterior and posterior regions and their respective parts.
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The cohesive zone model has been utilized to model the fiber-matrix debonding.
To support this framework, a new heterogeneous feature model (HFM) has been developed to model the fiber-reinforced objects and to be transferred between engineering modules.
The purpose of this study was to model the fiber-reinforced mechanical response of ATAA specimens from patients with either BAV or TAV.
In such a model, the fibers correspond to the collagen fibers and the matrix corresponds to the striated-sheet matrix of non-collagenous proteins.
Thus, the ability of a FEM model to predict mechanical properties depends upon the accuracy of modeling the fiber geometry in a unit cell.
This paper presents an experimental and analytical study aimed at better understanding and modeling the fiber reinforced polymer (FRP) debonding failures in strengthened RC beams under monotonic and cyclic loads.
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