Figure 7.

(a) Mean square end-to-end distances and (b) local slopes (Equation (39)) as function of the polymer length ($pL$) for the Péclet numbers $Pe=0$, 3, 10, 30, ${10}^2$ and ${10}^3$ (bottom to top at $pL={10}^3$). The other parameters are the same as in Figure 2. The dashed lines in (a) represent the analytical solution of Equation (40) with the Lagrangian multiplier of Equation (31).