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The temperature-dependent Young's modulus exhibits a monotonically decreasing trend with increasing temperature.
The equilibrium modulus exhibits a significantly weak power dependence on the cross-linking density (estimated from the modulus at the rubbery plateau and determined by dynamic viscoelastic measurements).
The topological restriction to ionic transport (i.e., to conductivity) is quantified by the obstruction factor, which increases monotonically with ξ, while the shear modulus exhibits a power law behavior, G∼ξ−3, in accordance to linear viscoelastic theory.
For quenched crystals, the Young's modulus exhibits a pronounced anomalous increase in the range 70 230 K, simultaneously with a significant decrease of the amplitude-independent and amplitude-dependent internal friction.
The modulus exhibits a tremendous increment of 350 and 520% with the addition of 4 and 8 wt.% of CNF, respectively.
The complex part of the electric modulus exhibits a peak in the low frequency range that can be associated with these conductive processes.
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The shear mechanical modulus exhibits an increase of the conservative and dissipative components after the poling step of nanocomposites.
The modulus exhibited a complicated behavior due to stiffening of the 0° plies and transverse cracks.
The relative modulus exhibited a power law dependence on relative density.
The tensile modulus exhibited a synergistic effect, as the blend has a greater modulus than neat PLA or POM.
The Young's modulus exhibited a similar dependence on Cu content as nano-hardness, though no significant differences were observed with increasing annealing temperatures.
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