Article ID: 2015-0017
An improved interatomic potential model was proposed for molecular dynamics simulations of lithium borate melt/glass systems. Charge of ion was reconsidered and a new composition dependent ionic charge model was suggested. A new three-body potential model controlling B-O-B angles was also proposed. The three-body term functioned to avoid square network ring consisted of B-O bonds, without preventing the change of boron coordination number between three and four. The edge-shared tetrahedra of four-coordination boron observed in the previous simulation were cleared by applying this three-body potential model.
Schematic view of the undesirable local structure observed in MD results applied 2-body potential model with partial ionic charges for Li2O-B2O3 melt/glasses.
Three-body potential, U(θBOB, rOB1, rOB2)
B-O pair correlation function, PB-O of Li2O-B2O3 system at 500 K.
Snapshots of a part of MD cell of 0.33Li2O-0.67B2O3 melt at 1500 K simulated with IA2 model (a) and with IA3 model (b).
B-O-B angle distribution in xLi2O-(1−x) B2O3 at 500 K simulated by IA2 model (a) and by IA3 model (b).
Ratio of structural units in xLi2O-(1−x) B2O3 at 500 K and 11B NMR results [12].
Ring size distribution in xLi2O-(1−x) B2O3 at 500 K simulation applied IA2 (a) and IA3 (b) potential model.
x | Ntotal | NO | NB | NLi | zO | zB | zLi |
0.00 | 5000 | 3000 | 2000 | ― | −1.2000 | 1.8000 | ― |
0.10 | 5016 | 2926 | 1881 | 209 | −1.2145 | 1.7782 | 1.0 |
0.20 | 5014 | 2834 | 1744 | 436 | −1.2320 | 1.7520 | 1.0 |
0.33 | 5005 | 2695 | 1540 | 770 | −1.2615 | 1.7077 | 1.0 |
0.40 | 5019 | 2629 | 1434 | 956 | −1.2800 | 1.6800 | 1.0 |
Parameters for the two-body potential terms | ||||||||
element | z | a/nm | b/nm | c/J1/2mol−1/2 nm3 | ||||
O | −1.2 − 2α | 0.1861 | 0.0151 | 1.7720 | ||||
B | 1.8 − 3α | 0.0723 | 0.0082 | 0.0 | ||||
Li | 1.0 | 0.1110 | 0.0110 | 0.1940 | ||||
pair | D1/MJ mol−1 | β1/nm−1 | D2/MJ mol−1 | β2/nm−1 | ||||
B-O | 120.5582 | 51.0 | −7.3926 | 22.6 | ||||
Parameters for the three-body potential terms | ||||||||
relation | f/J | pθ/degree−1 | θ0/degree | pr/nm−1 | r0/nm | |||
B-O-B | 5.0 × 10−4 | 1.70 | 100.0 | 40.00 | 0.100 |
IA2 potential model | IA3 potential model | ||||||||||
Temp./K | x | x | |||||||||
0 | 0.1 | 0.2 | 0.33 | 0.4 | 0 | 0.1 | 0.2 | 0.33 | 0.4 | ||
2000 | RBIV | 2.65 | 6.06 | 31.19 | 12.65 | 12.34 | 0.15 | 2.50 | 6.65 | 7.79 | 5.02 |
RBIII | 97.20 | 93.89 | 68.8 | 86.95 | 87.38 | 99.85 | 97.45 | 93.24 | 92.09 | 94.85 | |
RBII | 0.15 | 0.05 | 0.40 | 0.38 | 0.28 | 0.00 | 0.05 | 0.29 | 0.13 | 0.14 | |
ROIII | 1.77 | 2.97 | 3.88 | 5.08 | 4.6 | 0.10 | 0.92 | 1.59 | 1.60 | 1.45 | |
ROII | 98.13 | 90.77 | 83.27 | 69.20 | 62.19 | 99.90 | 92.65 | 85.00 | 73.84 | 65.08 | |
ROI | 0.10 | 6.25 | 12.77 | 24.79 | 32.03 | 0.00 | 6.36 | 13.02 | 23.34 | 31.80 | |
RO0 | 0.00 | 0.00 | 0.07 | 0.93 | 1.18 | 0.00 | 0.07 | 0.39 | 1.22 | 1.67 | |
1500 | RBIV | 4.05 | 11.85 | 31.19 | 19.93 | 20.99 | 4.09 | 2.82 | 6.65 | 11.56 | 11.51 |
RBIII | 95.95 | 88.14 | 68.8 | 80.07 | 78.94 | 95.91 | 97.18 | 93.24 | 88.37 | 88.50 | |
RBII | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.12 | 0.06 | 0.00 | |
ROIII | 2.70 | 4.72 | 10.27 | 5.90 | 6.62 | 0.10 | 0.85 | 0.88 | 1.60 | 1.94 | |
ROII | 97.30 | 91.05 | 83.27 | 71.43 | 62.42 | 99.9 | 92.99 | 86.94 | 75.51 | 67.82 | |
ROI | 0.00 | 4.24 | 6.46 | 22.26 | 30.35 | 0.00 | 6.12 | 12.10 | 22.19 | 28.45 | |
RO0 | 0.00 | 0.00 | 0.00 | 0.41 | 0.61 | 0.00 | 0.03 | 0.07 | 0.71 | 1.79 | |
1000 | RBIV | 6.20 | 19.04 | 32.58 | 41.82 | 39.27 | 0.10 | 3.45 | 9.64 | 16.3 | 19.25 |
RBIII | 93.80 | 80.97 | 67.43 | 58.18 | 60.73 | 99.9 | 96.55 | 90.36 | 83.69 | 80.76 | |
RBII | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | |
ROIII | 4.13 | 7.38 | 10.48 | 11.84 | 9.43 | 0.07 | 1.09 | 1.80 | 2.71 | 1.83 | |
ROII | 95.87 | 90.33 | 83.70 | 71.80 | 66.76 | 99.93 | 92.89 | 87.12 | 75.99 | 71.81 | |
ROI | 0.00 | 2.29 | 5.82 | 16.22 | 23.24 | 0.00 | 6.02 | 10.9 | 20.63 | 25.03 | |
RO0 | 0.00 | 0.00 | 0.00 | 0.15 | 0.57 | 0.00 | 0.00 | 0.18 | 0.67 | 1.33 | |
500 | RBIV | 8.50 | 22.44 | 36.81 | 49.21 | 51.6 | 0.35 | 4.09 | 11.81 | 21.30 | 23.70 |
RBIII | 91.50 | 77.57 | 63.19 | 50.78 | 48.40 | 99.65 | 95.91 | 88.19 | 78.70 | 76.29 | |
RBII | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | |
ROIII | 5.67 | 9.26 | 12.1 | 14.25 | 13.39 | 0.23 | 1.40 | 2.33 | 2.67 | 2.74 | |
ROII | 94.33 | 88.76 | 83.06 | 71.21 | 65.12 | 99.77 | 92.69 | 87.4 | 78.89 | 72.08 | |
ROI | 0.00 | 1.98 | 4.83 | 14.40 | 20.92 | 0.00 | 5.91 | 10.09 | 17.81 | 24.19 | |
RO0 | 0.00 | 0.00 | 0.00 | 0.15 | 0.46 | 0.00 | 0.00 | 0.18 | 0.63 | 0.99 |