DFT |
• more accurate calculation based on the
electronic
state |
• high computational cost |
|
• capable of simulating: |
• small simulation size |
|
- charge polarization/transfer |
• incapable of calculating dynamic properties |
|
- bond formation/cleavage |
•
incapable of including temperature effect (all simulations
are performed at 0 K) |
|
- electronic-based
properties, e.g., band structure, DOS, etc. |
|
|
- chemical reactions |
|
|
- transition state |
|
AIMD |
• includes
finite temperature effect in DFT calculations |
•
high computational cost |
|
|
• small simulation size |
QM/MM |
• takes advantage of both DFT and MM methods |
• complexity in the implementation, especially
at QM-MM boundary region |
|
•
suitable for larger systems |
ReaxFF |
• includes charge polarization to the classical force
field |
• force field availability and transferability |
|
• adds bond formation/cleavage
simulation into MD |
• shorter time- and length
scales than MD |
MD |
•
includes the effect of temperature, pressure, volume,
etc. in the simulations |
• incapable of simulating
chemical reactions and bond
formation/cleavage |
|
•
larger time (up to μs) and length (up to μm)
scale |
• lower accuracy compared to DFT calculations |
|
• capable of calculating: |
• accuracy and feasibility depend on the availability
of proper force fields |
|
- dynamic properties,
e.g. wettability, diffusion, etc. |
|
|
- thermodynamic
properties |
|