(Note: These tutorials are meant to provide
illustrative examples of how to use the AMBER software suite to carry out
simulations that can be run on a simple workstation in a reasonable period of
time. They do not necessarily provide the optimal choice of parameters or
methods for the particular application area.)
Copyright Ross Walker 2004
TUTORIAL 6 - AMBER 8 VERSION - SECTION 4
A Coupled Potential QMMM Simulation
By Ross Walker
PLEASE NOTE THIS TUTORIAL IS FOR AMBER 8 ONLY.
AN AMBER 9 QM/MM TUTORIAL IS AVAILABLE
HERE
4) Comparing the results
We will now qualitatively compare the results of the two simulations. First of all lets take a brief look at the two output files:
Classical |
NSTEP = 0 TIME(PS) = 0.000 TEMP(K) = 305.74 PRESS = 0.0 Etot = -1705.9816 EKtot = 1127.3405 EPtot = -2833.3221 BOND = 344.6722 ANGLE = 0.6147 DIHED = 2.4711 1-4 NB = 0.8346 1-4 EEL = -19.9098 VDWAALS = 935.3651 EELEC = -4097.3700 EHBOND = 0.0000 RESTRAINT = 0.0000 ------------------------------------------------------------------------------ NSTEP = 1 TIME(PS) = 0.001 TEMP(K) = 305.75 PRESS = 0.0 Etot = -1705.9601 EKtot = 1127.3620 EPtot = -2833.3221 BOND = 344.6722 ANGLE = 0.6147 DIHED = 2.4711 1-4 NB = 0.8346 1-4 EEL = -19.9098 VDWAALS = 935.3651 EELEC = -4097.3700 EHBOND = 0.0000 RESTRAINT = 0.0000 ------------------------------------------------------------------------------ |
QMMM |
NSTEP = 0 TIME(PS) = 0.000 TEMP(K) = 305.74 PRESS = 0.0 Etot = -3525.1146 EKtot = 1127.3405 EPtot = -4652.4551 BOND = 343.7005 ANGLE = 0.0000 DIHED = 0.0000 1-4 NB = 0.0000 1-4 EEL = 0.0000 VDWAALS = 982.1865 EELEC = -5917.1502 EHBOND = 0.0000 RESTRAINT = 0.0000 ESCF = -61.1920 ------------------------------------------------------------------------------ NSTEP = 1 TIME(PS) = 0.001 TEMP(K) = 305.75 PRESS = 0.0 Etot = -3525.0931 EKtot = 1127.3620 EPtot = -4652.4551 BOND = 343.7005 ANGLE = 0.0000 DIHED = 0.0000 1-4 NB = 0.0000 1-4 EEL = 0.0000 VDWAALS = 982.1865 EELEC = -5917.1502 EHBOND = 0.0000 RESTRAINT = 0.0000 ESCF = -61.1920 ------------------------------------------------------------------------------ |
The first thing you should notice is that the QMMM result has an extra field (ESCF). This is the energy due to the quantum part of the calculation (the NMA) within the presence of the charge field of the MM part (the water). You should also notice here that the QMMM result lacks ANGLE, DIHEDRAL, 1-4 NB and 1-4 EEL energies. This is exactly as we expect since the NMA bonds, angles, dihedrals and VDW and electrostatic terms are now dealt with inside the QM calculation. The only atoms remaining in the MM section are TIP3P water molecules. These are actually triangulated water and so only have bond terms (TIP3P water does not have an angle component). The water molecules are also only 3 atoms in size and so do not have any 1-4 NB or 1-4 EEL interactions.
If you compare the two output files further you should find that the temperatures are reasonably stable and similar. They will not be exactly the same since we are tracking different trajectories.
Now, lets compare the actual dynamics. First off lets load the QMMM mdcrd file into vmd:
Fire up VMD and load the NMA topology file (remember to select parm7) and then load the NMA_md_qmmm.mdcrd file into this molecule. Remember, we have not used periodic boundaries here so select "crd" (not "crdbox").
We should again remove the water molecules so our NMA is easier to see.
Graphics->Representations
In Selected Atoms type:
all not water
And hit apply
At the same time change the drawing method to CPK.
You should now be able to watch a movie of our NMA molecule "wiggling" about. How does the dynamics of the NMA differ from the classical simulation? If you want you can load both molecules into VMD and animate them together.
Rewind the current QMMM loaded trajectory to the beginning and then load a new molecule. Select the NMA.prmtop again and then load the NMA_md_classical.mdcrd file into this molecule. When you close the load molecule dialog box you should find that both molecules are displayed. You can now play through the trajectory slowly and watch the difference. (You can colour the two molecules differently in Graphics->Representations if you want).
You should notice that the dynamics of the NH group are different in the QMMM calculation. The nitrogen regularly forms a pyramidal structure and the amine hydrogen is more often out of the O-C-N plane. The QMMM behaviour here is believed to be the more accurate. The NH backbone dynamics are known to be troublesome to model accurately with classical force fields.
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(Note: These tutorials are meant to provide
illustrative examples of how to use the AMBER software suite to carry out
simulations that can be run on a simple workstation in a reasonable period of
time. They do not necessarily provide the optimal choice of parameters or
methods for the particular application area.)
Copyright Ross Walker 2004