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Figure 3 | BMC Biophysics

Figure 3

From: Many-particle Brownian and Langevin Dynamics Simulations with the Brownmove package

Figure 3

Normalised center-of-mass diffusion coefficient D CM of bead-spring polymers vs. the number of beads, N. Without HI, DCM scaled as N-1 independent of the stiffness, i.e., the "folding" state of the polymer. With HI, a stiffer polymer with a higher k2N diffuses slower because then the beads are on average further away from each other and the velocity correlation introduced by the HI is weaker.

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