Figure 6.

Predictions for ${\eta }_2(\dot{ϵ})/G\lambda$, analogous to Figure 4, as a function of dimensionless elongation rate $\mathrm{Wi}$ for $N=100$ and various values of the parameters ${\epsilon }_0$ and ${\epsilon }_0^{\prime }$. (a) ${\epsilon }_0=0$, various ${\epsilon }_0^{\prime }$, (b) ${\epsilon }_0=0.1$, various ${\epsilon }_0^{\prime }$, (c,d) ${\epsilon }_0^{\prime }=0.1$, various ${\epsilon }_0$. The solid lines mark the predictions of the small rate expansion, Equation (24), or Equation (25) for the case of ${\epsilon }_0^{\prime }=0$.