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Systematic development of coarse-grained polymer models Patrick ...

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6.7 Comparison <strong>of</strong> the different criteria for λ and their effect on the elongational viscosity<br />

fortheMarko-Siggiaforcelaw. ..............................112<br />

6.8 Calculation <strong>of</strong> the elongational viscosity as a function <strong>of</strong> the number <strong>of</strong> beads for<br />

constant Wi and α using the first two terms in the asymptotic expansion for the<br />

FENE force law with λ =1.................................116<br />

6.9 Comparison <strong>of</strong> the different criteria for λ and their effect on the elongational viscosity<br />

fortheFENEforcelaw. ..................................117<br />

6.10 Coefficient <strong>of</strong> the Pe −1/2 term, C, as a function <strong>of</strong> the number <strong>of</strong> beads with and<br />

withoutHI. .........................................121<br />

7.1 Sketch<strong>of</strong>thesystemwithastepchangeinelectrophoreticvelocity...........124<br />

7.2 Contours <strong>of</strong> constant stretch for the toy model as a function <strong>of</strong> the two parameters<br />

DeandWi. .........................................126<br />

7.3 This shows a comparison <strong>of</strong> Brownian dynamics simulations in the long chain limit<br />

tothetoymodel.......................................127<br />

7.4 Results from simulations with increasing finite extensibility. . . . . . . . . . . . . . . 128<br />

7.5 Approach <strong>of</strong> the nonlinear bead-spring chains to full extension. . . . . . . . . . . . . 129<br />

A.1 Relative error in extension between the real infinitely long WLC (numerical data<br />

fromBouchiatetal.)andapproximateformulas. ....................141

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