Research Article
Molecular Dynamics Simulations of CO2 Molecules in ZIF-11 Using Refined AMBER Force Field
Table 2
The AMBER force field parameters for ZIF-11 flexible framework.
| Bond potential: = | Bond type | (kcalmolÅ−2) | (Å) |
| Zn–N | 157.0 | 2.011 | C1–H1 | 734.0 | 1.080 | C1–N | 954.0 | 1.343 | C2–C2 | 1,024.0 | 1.375 | C2–N | 844.0 | 1.385 | C2–C3 | 1,036.0 | 1.371 | C3–C4 | 938.0 | 1.400 | C3–H3 | 734.0 | 1.080 | C4–H4 | 734.0 | 1.080 | C4–C4 | 938.0 | 1.400 |
| Bending potential: | Angle type | (kcalmol−1·rad−2) | (degree) |
| C2–C3–C4 | 126.00 | 120.00 | C3–C4–C4 | 126.00 | 120.00 | N–C1–N | 140.00 | 120.00 | N–C1–H | 70.00 | 120.00 | C1–N–C2 | 140.00 | 120.00 | N–C2–C3 | 140.00 | 132.80 | C2–C3–H3 | 70.00 | 120.00 | H3–C3–C4 | 70.00 | 120.00 | C3–C4–H4 | 70.00 | 120.00 | H4–C4–C4 | 70.00 | 120.00 | N–C2–C2 | 140.00 | 120.00 | N–Zn–N | 70.48 | 109.48 | Zn–N–C1 | 97.36 | 128.33 | Zn–N–C2 | 64.95 | 126.40 | C2–C3–C4 | 126.00 | 120.00 | C3–C4–C4 | 126.00 | 120.00 |
| Dihedral: | Dihedral type | (kcal·mol−1) | | (degree) |
| C1–N–C2–C2 | 5.40 | 2.0 | 180.0 | C3–C2–C2–C3 | 0.00 | 2.0 | 0.0 | N–C2–C2–C3 | 21.50 | 2.0 | 180.0 | Zn–N–C1–H1 | 9.30 | 2.0 | 180.0 | C2–N–C1–H1 | 9.30 | 2.0 | 180.0 | Zn–N–C2–C2 | 5.60 | 2.0 | 180.0 | N–C2–C2–N | 21.50 | 2.0 | 180.0 | N–C2–C3–H3 | 21.50 | 2.0 | 180.0 | N–C2–C3–C4 | 21.50 | 2.0 | 180.0 | C2–C2–C3–C4 | 0.00 | 2.0 | 180.0 | C2–C2–C3–H3 | 21.50 | 2.0 | 180.0 | C2–C3–C4–H4 | 14.50 | 2.0 | 180.0 | C2–C3–C4–C4 | 14.50 | 2.0 | 0.0 | H3–C3–C4–H4 | 14.50 | 2.0 | 180.0 | H3–C3–C4–C4 | 14.50 | 2.0 | 180.0 | C3–C4–C4–H4 | 14.50 | 2.0 | 180.0 | H4–C4–C4–H4 | 14.50 | 2.0 | 180.0 |
| Improper: | Improper type | (kcal·mol−1·rad−2) | (degree) |
| C4–C4–C3–H4 | 2.2 | 180 | C3–C4–C2–H3 | 2.2 | 180 | C2–C2–C3–N | 2.2 | 180 | C1–N–N–H1 | 2.2 | 180 | N–Zn–C1–C2 | 2.2 | 180 |
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