Journal of Computer Chemistry, Japan
Online ISSN : 1347-3824
Print ISSN : 1347-1767
ISSN-L : 1347-1767

This article has now been updated. Please use the final version.

Interatomic Potential Model for Molecular Dynamics Simulation of Lithium Borate Melts/Glasses
Naoya SAWAGUCHIKakeru YAMAGUCHIMakoto SASAKIKatsuyuki KAWAMURA
Author information
JOURNAL FREE ACCESS FULL-TEXT HTML Advance online publication

Article ID: 2015-0017

Details
Abstract

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.

Figures
Figure 1.

 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.

Figure 2.

 Three-body potential, U(θBOB, rOB1, rOB2)

Figure 3.

 B-O pair correlation function, PB-O of Li2O-B2O3 system at 500 K.

Figure 4.

 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).

Figure 5.

 B-O-B angle distribution in xLi2O-(1−x) B2O3 at 500 K simulated by IA2 model (a) and by IA3 model (b).

Figure 6.

 Ratio of structural units in xLi2O-(1−x) B2O3 at 500 K and 11B NMR results [12].

Figure 7.

 Ring size distribution in xLi2O-(1−x) B2O3 at 500 K simulation applied IA2 (a) and IA3 (b) potential model.

Figure 8.

 Density of xLi2O-(1−x) B2O3 melt/glasses. Open circle and solid circle are simulated by IA2 and IA3, respectively. Squares are the reference data at 298 K [18] and 1129 K [19].

Tables
Table 1. Number of atoms, N in MD cell and charges, z
xNtotalNONBNLizOzBzLi
0.00500030002000−1.20001.8000
0.10501629261881209−1.21451.77821.0
0.20501428341744436−1.23201.75201.0
0.33500526951540770−1.26151.70771.0
0.40501926291434956−1.28001.68001.0
Table 2. Potential parameters
Parameters for the two-body potential terms
elementza/nmb/nmc/J1/2mol−1/2 nm3
O−1.2 − 2α0.18610.01511.7720
B1.8 − 3α0.07230.00820.0
Li1.00.11100.01100.1940
pairD1/MJ mol−1β1/nm−1D2/MJ mol−1β2/nm−1
B-O120.558251.0−7.392622.6
Parameters for the three-body potential terms
relationf/Jpθ/degree−1θ0/degreepr/nm−1r0/nm
B-O-B5.0 × 10−41.70100.040.000.100
Table 3. Ratio, Ru of structural units (%)
IA2 potential modelIA3 potential model
Temp./Kxx
00.10.20.330.400.10.20.330.4
2000RBIV2.656.0631.1912.6512.340.152.506.657.795.02
RBIII97.2093.8968.886.9587.3899.8597.4593.2492.0994.85
RBII0.150.050.400.380.280.000.050.290.130.14
ROIII1.772.973.885.084.60.100.921.591.601.45
ROII98.1390.7783.2769.2062.1999.9092.6585.0073.8465.08
ROI0.106.2512.7724.7932.030.006.3613.0223.3431.80
RO00.000.000.070.931.180.000.070.391.221.67
1500RBIV4.0511.8531.1919.9320.994.092.826.6511.5611.51
RBIII95.9588.1468.880.0778.9495.9197.1893.2488.3788.50
RBII0.000.000.000.000.000.000.000.120.060.00
ROIII2.704.7210.275.906.620.100.850.881.601.94
ROII97.3091.0583.2771.4362.4299.992.9986.9475.5167.82
ROI0.004.246.4622.2630.350.006.1212.1022.1928.45
RO00.000.000.000.410.610.000.030.070.711.79
1000RBIV6.2019.0432.5841.8239.270.103.459.6416.319.25
RBIII93.8080.9767.4358.1860.7399.996.5590.3683.6980.76
RBII0.000.000.000.000.000.000.000.000.000.00
ROIII4.137.3810.4811.849.430.071.091.802.711.83
ROII95.8790.3383.7071.8066.7699.9392.8987.1275.9971.81
ROI0.002.295.8216.2223.240.006.0210.920.6325.03
RO00.000.000.000.150.570.000.000.180.671.33
500RBIV8.5022.4436.8149.2151.60.354.0911.8121.3023.70
RBIII91.5077.5763.1950.7848.4099.6595.9188.1978.7076.29
RBII0.000.000.000.000.000.000.000.000.000.00
ROIII5.679.2612.114.2513.390.231.402.332.672.74
ROII94.3388.7683.0671.2165.1299.7792.6987.478.8972.08
ROI0.001.984.8314.4020.920.005.9110.0917.8124.19
RO00.000.000.000.150.460.000.000.180.630.99
References
 
© 2015 Society of Computer Chemistry, Japan
feedback
Top