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Techniques in oscillatory shear rheology - Indian Institute of ...

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<strong>Techniques</strong> <strong>in</strong> <strong>oscillatory</strong> <strong>shear</strong> <strong>rheology</strong> 7H(λ) = H e λ n e+ H g λ −n gλ 1 < λ < λ max= 0 λ > λ max , (15)where λ 1 is the shortest measurable relaxation time and λ max is largest relaxationtime <strong>of</strong> the polymer. When tested below 1/λ max (i.e. at stra<strong>in</strong> rate or frequencylower than this value), polymer would show Newtonian viscous behaviour. H e , n eand H g , n g are coefficients to capture the entanglement modes and glassy modes <strong>of</strong>the polymer, respectively.Examples <strong>of</strong> relaxation time spectrum for polymers and an emulsion are given <strong>in</strong>Fig. 1.3. As was observed <strong>in</strong> Fig. 2 with G ′ and G ′′ , there is marked difference <strong>in</strong>the relaxation time spectrum for both the materials.As discussed <strong>in</strong> Sects. 1.1– 1.3, material response can be described <strong>in</strong> terms<strong>of</strong> microscopic mechanisms. These mechanisms for complex fluids, such as poly-Fig. 3 Relaxation time spectrum <strong>of</strong> (a) monodisperse polybutadienes [1] (b) emulsion [9]

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