AMBER Archive (2008)Subject: AMBER: how to derive torsional angle parameters in gaff
From: Junmei Wang (junmwang_at_gmail.com)
Date: Tue Jun 24 2008  20:45:42 CDT
The following is the emails between Balazs Jojart, David Case and me. Maybe
you are interested in this topic.
Junmei
Hi Dave,
Now I understand why the two figures are so different: my one is total
energies and Balazs' is the total energy minus Ebond minus Eangle minus
Enonbonded. As a matter of fact, XccX has a V2 term in gaff, and this is
consistent to Balazs's figure, which has minimum at 180, 180 and 0.
The attached pdf files have rotation profiles for GAFF, QM (total energy),
MM2 and MMFF. They are all quite similar. GAFF has similar rotational
barrier to QM, while MM2 and MMFF have much big barriers. The discrepancy
between Balazs' QM profile to Figure 3 in the paper may be caused by (1)
ZPE, (2) different protocols in scanning calculations. I am not sure if
Gaussian 03 has improved 'scan' or not. In Gaussian 98, 'scan' first
optimizes the structure and does single point calculations for every
conformations. However, I don't think this is an ideal protocol to generate
rotational profile. For Figure 3, I performed 'popt' with the involved
torsional angle frozen.
Best
Junmei
Hi Balazs,
I am sorry for not replying your email earlier. I didn't rerun the QM
calculations to verify your QM data, I just perform torsional angle scanning
using MM2 and MMFF force fields. I got similar profiles as the one in Table
3 of GAFF paper. I will double check this issue when I upgrade gaff to gaff2
or uaff (universal amber force field). Thank you very much for your work on
gaff development.
Please find the attached pdf file for my rotational profile calculations.
Best
Junmei
 Original Message 
From: Balazs Jojart <jojartb_at_pharm.uszeged.hu>
To: junmwang_at_yahoo.com
Sent: Thursday, June 5, 2008 5:42:02 AM
Subject: gaff parametrization
Dear dr. Wang,
I wroe a mail directly to dr. Case yesterday, and he suggested me to
forward my message to you, because you prepared the torsional parameters
for the general amber forcefield.
You can read the mail as follows, and I attached the files, as well.
Dear dr. Case,
I write you diretly because you are the coresponding author of the
article 'Development and Testing of a General Amber Force Field'.
I started 3 or 4 weeks ago to learn the development philosophy of the
amber forcefield, especially the torsional parameter fitting.
I thought, the the paper mentioned above, is a good starting point,
because it contains the torsional profile of acethylacetone
(ch3cococh3).
Unfortunatelly, I wasn't able to reproduce the data (figure 3.)
I performed the following protocol:
(1) the small molecule (MOL) was prepeared using gaussview
(2) optimization was performed at the MP2/631G* level, anf frequency
calculations were also conducted. I found only one imaginary freqency,
but rotating 3 degree of a methyl rotor solved the problem.
(3) relax scan was performed on MOL with the following keywords:
MP2/631G* Opt(Zmatrix,maxcycle=100) nosym, and for the appropriate
dihedral angle : D2 179.97084591 S 11 30.0
(4) I prepared the input files form the gaussian log file using the
gaussview program.
(5) MP4 single point calculations were performed with the following
keywords: MP4/6311G**.
(6) the UMP4(SDTQ) energies were collected from the single point
calculations. (you can find it in the attached excel (GAFF_xccx.xls)
file in column D3:D14, the values were converted to kcalmol1 > column
E3:E14).
(7) for the lowest energy conformer optimization at the HF/631G* and
MEP calculation were performed (you can find the prepared prepi file as
attachment (MOL.prepi)).
(8) molmech minimization using AMBER 9 (input file min1.in), and the
appropriate dihedral angle was restrained during the minimization with a
100 force constant (RST).
(9) the BOND, ANGLE, VDW, ELE, 14 VDW and 14 ELE were collected form
the log file file (G:N).
(10) in the Amber8 manual a read the following :'Before Fitting the
torsional parameters, we must generate the energy profile for the
molecular mechanical nonbonded potential as was done for the quantum
potential, subtract this curve from the quantum curve, and ?t the
torsional potential to the difference potential'
(11) I calculated the MP4MM(bond,angle,ele,vdw,14)[D18:D29] and
MP4MM(ele,vdw,14) [D34:D45].
(12) the obtained curves are completly different compared to Figure 3 in
the article.
My qustetion are:
Did I made any mistake during the calculation? I don't understand the
parameter development strategy in amber?
For the XccX torsional term th V2=1.2 kcal/mol, multiplicity=4, phase
angle=180. It is not clear for me how came these values from Figure 3.
'PHASE = 180 degrees if an energy minimum is at 0 degrees.' 8form amber8
manual. As we can see on Figure 3 there is a maximum at 0 degree. The V
paranmeter is not the onehalf of the barrier? n=4, which means the
there is 4 minimums when during the rotation from 0 to 360 degree.(AR
LEach book).
Etors can be calculated with the following equation:
summaVn/2(1+cos(n×phiphase)). Am i right? Consider only the first trhee
term:
V1/2(1+(cos(1×phiphase))+V2/2(1(cos(2×phiphase))+V3/2(1+(cos(3×phiphase))
(as I read the article of Jorgensen: Development and Testing of the OPLS
AllAtom Force Field ... (J. Am. Chem. Soc. 1996, 118, 1122511236).
Then where can we set up the multiplicity parameter? The 'n' parameters
are not the same in the equation? Beacuese in the Gaff paper the 'n' is
described as the multiplicity, but in the Jorgensen paper n is equalt to
n in the Vn term.
Can you give me some notes where I made a mistake during the calculation
and the protocol?
Your help will be very appreciated!!!
Thank you for your help in advance!
Balazs Jojart Ph.D.
University Of Szeged
Department of Chemical Informatics

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