Computing Elastic Constants 2

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Manual 08 for MD++
Computing elastic constants at nonzero temperature

Keonwook Kang, Seunghwa Ryu and Wei Cai

Jul 08 , 2009



In the previous manual, the elastic constants of bulk silicon of diamond cubic structure are computed at 0 K. In this manual, we compute the elastic constants at nonzero finite temperature using fluctuation-dissipation theorem.

Table 1. Elastic constants of DC Si. Potential Model : SW
T (K) C11 C22 C33 C12 C13 C23 C44 C55 C66
300 149.41 149.36 149.45 76.26 76.18 76.24 62.45 75.00 54.93
625 146.35 146.29 146.35 75.80 75.77 75.71 53.72 50.03 46.98
888 142.74 142.86 142.84 75.07 75.17 74.99 60.78 53.54 56.76
1164 139.11 139.06 139.29 74.28 74.33 74.27 47.30 60.86 51.17
1477 135.02 134.84 134.69 73.84 73.85 73.80 44.96 41.41 47.66
Table 2. Elastic constants of FCC Au. Potential Model : EAM
T (K) C11 C22 C33 C12 C13 C23 C44 C55 C66
170 177.48 177.45 177.53 151.05 150.80 151.04 36.32 36.34 36.41
300 170.72 170.25 170.44 146.01 146.00 146.06 34.16 34.07 34.20
600 152.37 152.40 151.99 132.33 132.30 131.92 29.05 29.35 29.10
900 132.23 132.02 132.78 118.10 117.71 117.08 23.90 23.44 23.99
1200 107.14 105.48 106.68 98.54 99.04 98.22 17.82 17.70 17.46
Table 3. Elastic constants of FCC Cu. Potential Model : EAM Mishin
T (K) C11 C22 C33 C12 C13 C23 C44 C55 C66
315 164.06 164.05 163.99 119.99 119.93 119.90 71.60 71.69 71.69
600 153.01 153.18 153.07 113.20 113.26 113.38 65.57 65.70 65.80
800 142.68 143.24 142.90 106.62 107.05 107.18 60.21 60.81 60.40
1000 131.30 131.57 132.30 99.71 99.89 99.32 55.13 54.24 55.26
1200 120.46 118.93 119.56 92.33 92.55 92.21 49.08 48.20 49.05
Table 4. Elastic constants of BCC W. Potential Model : FS
T (K) C11 C22 C33 C12 C13 C23 C44 C55 C66
310 489.45 491.04 489.23 209.52 209.81 209.69 162.63 163.67 163.52
600 153.01 153.18 153.07 113.20 113.26 113.38 65.57 65.70 65.80
900 142.68 143.24 142.90 106.62 107.05 107.18 60.21 60.81 60.40
1200 131.30 131.57 132.30 99.71 99.89 99.32 55.13 54.24 55.26
1500 120.46 118.93 119.56 92.33 92.55 92.21 49.08 48.20 49.05