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Since only two dimensionless moduli are involved in the model, the effectiveness factor for the three kinetic equations considered can be estimated by using only one generalized graph.
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These two elastic moduli are not equal since (1.10).
Thus, our calculated values of elastic moduli are justified.
Their specific consistent tangent stiffness moduli are also developed.
The measured Young's moduli are in good agreement with the moduli predicted from the Bergström Boybce model.
The influence of these moduli are depicted in the upper row of Fig. 1, The larger the moduli the more difficult it is to deform the material in response to the applied stresses indicated by the arrows.
The calculated storage moduli and loss moduli are shown in Fig. 11.
The shear moduli are defined as functions of the RVs representing the respective Young's moduli and Poisson ratios.
The values of H and Y moduli are influenced by the presence of PDMS.
We will assume the Young's moduli are independent of temperature.
In addition, the differences of elastic moduli are corresponding to slope steepness of the stress-strain curve.
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