Table 1 Parameters and physical constants used in the models. aThis value was determined from the average of 28 MD simulations at P = 0 and T = 933 K containing spherical cavities of various sizes using the tungsten EAM potential used in our prior studies58,59,60. Values for specific planar surfaces range from 2.58 J/m2 to 3.30 J/m2 with this potential19. bDetermined from a molecular statics simulation using the same potential.
From: Theoretical Model of Helium Bubble Growth and Density in Plasma-Facing Metals
Parameter | Value | Ref. |
|---|---|---|
T | 933 K | |
γ | 2.67 J/m2 | (this worka) |
a0 | 0.3180 nm | |
Ω | \({a}_{0}^{3}/2=1.6079\times 1{0}^{-29}\) m3 | (deduced from a0) |
G | 156.1 GPa | (this work)b |
b | \(\frac{{a}_{0}\sqrt{3}}{2}=\) 0.2755 nm | (deduced from a0) |
k | 1.380649 × 10−23 J K−1 | |
B (at 933 K) | 9.63 cm3/mol = 1.60 × 10−29 m3 | |
A−1,1 | − 5.5991 × 10−27 m3 K1/2 Pa1/3 | |
A0,1 | 1.7400 × 10−26 m3 Pa1/3 | |
A2,1 | 4.9833 × 10−30 m3 K−1 Pa1/3 | |
A0,2 | − 4.4658 × 10−24 m3 Pa2/3 | |
A2,2 | − 8.7825 × 10−27 m3 K−1 Pa2/3 | |
A0,3 | 1.7595 × 10−22 J | |
A2,3 | 1.7608 × 10−23 J K−1 | |
A−1,3 | − 3.2615 × 10−21 J K1/2 | |
A−2,3 | 3.1524 × 10−20 J K |