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m. This dependence was successfully utilized to make short extrapolation of the G′ and G′ data of neat PEO to the temperatures examined in Figures 4 and 5
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m (characterized by an activation energy ΔE that agreed, within 30%, with ΔE for the viscoelastic moduli). This dependence was successfully utilized to make short extrapolation of the ε′ and ε″ data of neat PEO to the temperature examined in Figures 2 and 3.
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4 system could not stay in the gap between the cone and plate (electrodes) over long times because of its significant elasticity (cf. Figure 4c). Thus, the gradual shear thinning behavior of this system under fast shear could not be tested experimentally, though this behavior is naturally expected.
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42
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0442269281
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note
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39c). This small ΔT is not responsible for the significant decrease of η(γ̇) under fast shear (Figure 7).
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