Computing Elastic Constants 2: Difference between revisions

From Micro and Nano Mechanics Group
Jump to navigation Jump to search
No edit summary
No edit summary
Line 17: Line 17:


{| class="wikitable" style="margin: 1em auto 1em auto"
{| class="wikitable" style="margin: 1em auto 1em auto"
|+ '''Table 1.''' Elastic constants of DC Si. Potential Model : SW
|+ '''Table 1.''' Elastic constants (GPa) of DC Si. Potential Model : SW
|-
|-
! 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>
Line 38: Line 38:


{| class="wikitable" style="margin: 1em auto 1em auto"
{| class="wikitable" style="margin: 1em auto 1em auto"
|+ '''Table 2.''' Elastic constants of FCC Au. Potential Model : EAM
|+ '''Table 2.''' Elastic constants (GPa) of FCC Au. Potential Model : EAM
|-
|-
! 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>
Line 59: Line 59:


{| class="wikitable" style="margin: 1em auto 1em auto"
{| class="wikitable" style="margin: 1em auto 1em auto"
|+ '''Table 3.''' Elastic constants of FCC Cu. Potential Model : EAM Mishin
|+ '''Table 3.''' Elastic constants (GPa) of FCC Cu. Potential Model : EAM Mishin
|-
|-
! 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>
Line 80: Line 80:


{| class="wikitable" style="margin: 1em auto 1em auto"
{| class="wikitable" style="margin: 1em auto 1em auto"
|+ '''Table 4.''' Elastic constants of BCC W. Potential Model : FS
|+ '''Table 4.''' Elastic constants (GPa) of BCC W. Potential Model : FS
|-
|-
! 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>
Line 88: Line 88:
|-
|-
! 600
! 600
| 153.01 || 153.18 || 153.07 || 113.20 || 113.26 || 113.38 || 65.57 || 65.70 || 65.80
| 411.34 || 411.16 || 409.90 || 200.96 || 200.95 || 200.85 || 156.75 || 156.66 || 156.84
|-
|-
! 900
! 900
| 142.68 || 143.24 || 142.90 || 106.62 || 107.05 || 107.18 || 60.21 || 60.81 || 60.40
| 347.50 || 347.06 || 348.17 || 190.88 || 191.04 || 190.38 || 148.43 || 148.48 || 148.78
|-
|-
! 1200
! 1200
| 131.30 || 131.57 || 132.30 || 99.71 || 99.89 || 99.32 || 55.13 || 54.24 || 55.26
| 300.39 || 299.80 || 300.20 || 181.07 || 181.56 || 181.61 || 140.65 || 141.70 || 141.74
|-
|-
! 1500
! 1500
| 120.46 || 118.93 || 119.56 || 92.33 || 92.55 || 92.21 || 49.08 || 48.20 || 49.05
| 271.06 || 271.35 || 270.86 || 177.32 || 177.67 || 177.69 || 135.83 || 136.35 || 135.78
|}
|}

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

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 (GPa) 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 (GPa) 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 (GPa) 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 (GPa) 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
600 411.34 411.16 409.90 200.96 200.95 200.85 156.75 156.66 156.84
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