Table 3. Network structure statistics for the runs over 120 seconds for the B-In-M network with ω = 1 Hz.
Ld (μm) | γ | (μm−3) | % in B | G′ (Pa) | G′′ (Pa) | |
---|---|---|---|---|---|---|
3 | 0 | 12.6 | 2.3 | 24.1 | ||
3 | 0.01 | 12.5 | 2.2 | 23.2 | 0.37 | 0.64 |
3 | 0.025 | 12.5 | 2.2 | 23.5 | 0.36 | 0.63 |
3 | 0.05 | 12.8 | 2.2 | 23.9 | 0.39 | 0.67 |
3 | 0.10 | 13.2 | 2.3 | 25.1 | 0.52 | 0.77 |
3 | 0.15 | 13.9 | 2.4 | 26.6 | 0.79 | 0.96 |
3 | ± | 0.4 | 0.1 | 0.8 | 0.04 | 0.03 |
4 | 0.025 | 12.7 | 2.2 | 23.8 | 0.37 | 0.66 |
4 | 0.05 | 12.8 | 2.2 | 24.0 | 0.42 | 0.70 |
4 | ± | 0.1 | 0.1 | 0.5 | 0.02 | 0.02 |
We give the mean for each statistic, with uncertainties on the measurements (± row) equal to two standard deviations across five trials. The uncertainties in the viscoelastic moduli for γ = 0.15 are larger, G′ = 0.79±0.09 Pa and G′′ = 0.96±0.12 Pa. The comparable values of the statistics and moduli for Ld = 3 μm and Ld = 4 μm demonstrate that the finite-size errors are smaller than the statistical errors.