Computing Elastic Constants 2: Difference between revisions
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Manual 08 for MD++
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|+ '''Table 1.''' Elastic constants of DC Si. Potential Model : SW |
|+ '''Table 1.''' Elastic constants (GPa) of DC Si. Potential Model : SW |
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! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
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|+ '''Table 2.''' Elastic constants of FCC Au. Potential Model : EAM |
|+ '''Table 2.''' Elastic constants (GPa) of FCC Au. Potential Model : EAM |
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! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
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|+ '''Table 3.''' Elastic constants of FCC Cu. Potential Model : EAM Mishin |
|+ '''Table 3.''' Elastic constants (GPa) of FCC Cu. Potential Model : EAM Mishin |
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! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
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|+ '''Table 4.''' Elastic constants of BCC W. Potential Model : FS |
|+ '''Table 4.''' Elastic constants (GPa) of BCC W. Potential Model : FS |
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! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub> |
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! 600 |
! 600 |
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| 411.34 || 411.16 || 409.90 || 200.96 || 200.95 || 200.85 || 156.75 || 156.66 || 156.84 |
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! 900 |
! 900 |
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| 347.50 || 347.06 || 348.17 || 190.88 || 191.04 || 190.38 || 148.43 || 148.48 || 148.78 |
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! 1200 |
! 1200 |
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| 300.39 || 299.80 || 300.20 || 181.07 || 181.56 || 181.61 || 140.65 || 141.70 || 141.74 |
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! 1500 |
! 1500 |
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| 271.06 || 271.35 || 270.86 || 177.32 || 177.67 || 177.69 || 135.83 || 136.35 || 135.78 |
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Revision as of 23:12, 14 July 2009
Manual 08 for MD++
Computing elastic constants at nonzero temperature
Keonwook Kang, Seunghwa Ryu and Wei Cai
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.
| 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 |
| 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 |
| 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 |
| 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 | 411.34 | 411.16 | 409.90 | 200.96 | 200.95 | 200.85 | 156.75 | 156.66 | 156.84 |
| 900 | 347.50 | 347.06 | 348.17 | 190.88 | 191.04 | 190.38 | 148.43 | 148.48 | 148.78 |
| 1200 | 300.39 | 299.80 | 300.20 | 181.07 | 181.56 | 181.61 | 140.65 | 141.70 | 141.74 |
| 1500 | 271.06 | 271.35 | 270.86 | 177.32 | 177.67 | 177.69 | 135.83 | 136.35 | 135.78 |