Raj and Peskin. 10.1073/pnas.0601215103.
Supporting Figure 3
Supporting Figure 4
Supporting Appendix
Supporting Movie 1
Supporting Movie 2
Supporting Movie 3
Supporting Movie 4
Fig. 3. Convergence study of computed steady-state velocity with respect to Dx. The y axis is the error, defined as the difference between the computed velocity and the optimized "theoretical" velocity of 8.742 × 10-7 m/s. The convergence rate found is 1.76.
Fig. 4. Convergence study of computed steady-state velocity with respect to Ds. The y axis is the error, defined as the difference between the computed velocity and the optimized theoretical velocity of 8.777 × 10-7 m/s. The convergence rate found is 2.61.
Movie 1. Simulations of chromosome motion for long (3 mm, blue), medium (1 mm, green), and short (0.5 mm red) chromosomes with physiological Young’s modulus (38 N/m2) for Df = 8 kBT. All spatial dimensions in mm. All chromosomes here move at roughly the same speed, regardless of size.
Movie 2. Simulations of chromosome motion for long (3 mm, blue), medium (1 mm, green), and short (0.5 mm, red) chromosomes with a Young’s modulus of 2,423 N/m2 for Df = 8 kBT. All spatial dimensions in mm. In sharp contrast with the flexible case, the speed of the chromosome increases significantly as the size of the chromosome decreases.
Movie 3. Simulations of chromosome motion for long (3 mm) chromosomes with Young’s moduli of 38 and 2,423 N/m2 for Df = 8 kBT. All spatial dimensions in mm. Here, the more flexible chromosome moves significantly faster than the stiffer one.
Movie 4. Simulations of chromosome motion for short (0.5 mm) chromosomes with Young’s moduli of 38 and 2,423 N/m2 for Df = 8 kBT. All spatial dimensions in mm. Here, the stiffer chromosome moves faster than the more flexible one. This is the opposite of what happens for the long (3 mm) chromosomes.