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p ≪ L, could conceivably have little effect on high-frequency short-wavelength modes and strong effects on low-frequency long-wavelength modes, leading to a frequency-dependent effective exponent.
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85034466064
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p and is never more than a few percent of the total perturbation of f given in (A7). For simplicity, this slight variation with s has been ignored.
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58
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85034484449
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note
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⊥ as a constant in the frequency range of interest.
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61
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85034476255
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2〉 is expressed in terms of an integral of the PSD over all ω(as here) or only over ω > 0 (as in ref 18), has been accounted for in Figure 8.
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Morse, D. C. Viscoelasticity of concentrated isotropic solutions of semiflexible polymers. 3. Nonlinear rheology. Macromolecules, submitted for publication.
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Macromolecules
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Morse, D.C.1
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