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The LV endocardium always experienced higher fibre stress compared to the epicardium for all five subjects.
Similarly the 3DH2 fibre showed that the increase in the embedded length from 10 to 30 mm slightly enhancing the maximum fibre stress (Fig. 7).
The tensile stress induced in fibre or the maximum fibre stress is then interpreted and summarized in Table 4 and Figs. 6 and 7.
It can be observed that the maximum fibre stress of the 3DH1 fibres is somewhat higher than that generated by the 3DH2 fibres.
It is noteworthy from Table 4 that for the matrix with 0.20 W/B ratio the increase in embedded length of both types of fibres did not improve fibre stress and the values of the maximum fibre stress is found to be very similar.
The maximum fibre stress of the 3DH2 fibre with embedded length of 10 mm is increased by 25.41%, while for the 3DH1 fibre only 5.90% when W/B ratio decreases from 0.25 to 0.20.
Similar(43)
For the fibre stress-slip, the induced stress in the 3DH1 fibres which have smaller fibre diameter (d f = 0.55), is higher than that of the 3DH2 fibres with (d f = 0.90) (Fig. 12).
The fibre stresses were computed based on force equilibrium considerations.
While boudins elongate parallel to the maximum finite extension, X, the internal stress state within boudins (shown in inset) arising from fibre stresses differs markedly from the far-field stress field driving thrust-sense shear across the SISZ.
The simplified equations are proposed for estimating the fibre tensile stress, elastic modulus and toughness.
Maximum fibre tensile stress, σ max that can be obtained by dividing the maximum pullout load, Pmax over nominal cross-sectional area of the fibre, ( A_{f} ).
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