2007
DOI: 10.1122/1.2754293
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The dynamics of the coil-stretch transition for long, flexible polymers in planar mixed flows

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Cited by 15 publications
(18 citation statements)
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“…The length scale l H = √ k B T/H and time scale λ H = ζ/4H (where, k B is the Boltzmann constant, T is the temperature, H is the spring constant and ζ is the hydrodynamic friction coefficient associated with a bead), have been used for the purpose of non-dimensionalising Eq (8). The 3 × 3 tensor κ is equal to (∇v) T , with v being the unperturbed solvent velocity.…”
Section: Bd Simulations Of Flowing Polymer Solutions At Finite Concenmentioning
confidence: 99%
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“…The length scale l H = √ k B T/H and time scale λ H = ζ/4H (where, k B is the Boltzmann constant, T is the temperature, H is the spring constant and ζ is the hydrodynamic friction coefficient associated with a bead), have been used for the purpose of non-dimensionalising Eq (8). The 3 × 3 tensor κ is equal to (∇v) T , with v being the unperturbed solvent velocity.…”
Section: Bd Simulations Of Flowing Polymer Solutions At Finite Concenmentioning
confidence: 99%
“…Static and dynamic properties of polymer solutions at equilibrium can be calculated once the trajectories of the time evolution of all the beads on all the chains are obtained using Eq. (8). For rheological properties, not only are the bead configurations required, it is also necessary to know the forces acting on them.…”
Section: Macroscopic Propertiesmentioning
confidence: 99%
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