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Introductory Case Studies
 

Using mdgx to manipulate small molecules

Whether you are a beginner or a seasoned user, molecular dynamics is about sampling relevant conformations of a molecule on a rugged energy surface. It is common to find the molecule trapped in one conformation or another, with steep energy barriers on all sides. For some applications, it is important to understand the heights of these barriers and the relative depths of the wells that different conformations represent. For other situations, it is simply important to find new local minima, perhaps with some geometric stipulations about the rest of the molecule. If the system is small, the mdgx program in AmberTools offers an effective, accessible CPU-based platform for computing hundreds of a molecule's local minima at one time. This facility is the &configs module. It is utilized in other tutorials, but this page will provide a dedicated overview of its features. Some of the other literature on this module, in particular the manual inside the mdgx executable itself, refers to different configurations but the terms should be taken as interchangeable.

The basic operations of the module are:

  • Read a single topology file.
  • Read one or more input conformations.
  • Read a series of restraint operations with ranges to differentiate the target coordinates.
  • Read some minimization run conditions (number of cycles, step size, etc.
  • Perform minimization using steepest descent followed by conjugate gradient methods.
  • Prune conformations that do not meet criteria for tolerable strain.
  • If requested, shuffle and recycle successful optimizations as the initial conformations for another round of optimizations. (This can be repeated as required and is an effective method for jumping out of local minima as well as reaching restraint targets with a minimum of restraint strain.)
  • Report general statistics on conformations produced and the specific flaws in any rejected conformations.
  • Print successfully optimized conformations to an Amber trajectory, PDB files, or quantum chemical program inputs.

Here is a small peptide that can nonetheless sample thousands of unique minima:

Ace-Ala-Hid-Ala-Nme

All of the input mimics the sander &namelist format, but some of it is more intuitive as will be discussed. Here is basic input that illustrates all of the above concepts in the &configs module. The topology HID.top and associated initial coordinates HID.crd are actually a tetrapeptide Ace-Ala-Hid-Ala-Nme. We will continue to refer to this system as we make the input more elaborate.

&files
  -p    HID.top
  -c    HID.crd
  -o    cfsamp_I.out
&end

&configs

  % Backbone phi and psi sampling
  GridSample  :2@C  :3@N  :3@CA :3@C  { -180.0 180.0 }  fbhw  10.0  Krst 64.0,
  GridSample  :3@N  :3@CA :3@C  :4@N  { -180.0 180.0 }  fbhw  10.0  Krst 64.0,
  combine 1 2,

  % General minimization instructions
  count = 64,
  verbose 1,
  maxcyc = 5000,
  strainlim = 20.0,
  bstrain = 10.0,
  astrain = 10.0,

  % Reshuffling conformations to best achieve each minimum
  nshuffle = 2,
  shuffle bootstrap,

  % Output controls
  outbase 'Conf', 'Conf',
  write   'cdf',  'pdb',
  outsuff 'cdf',  'pdb',
&end

The command file looks a lot like sander &namelist input, on purpose. However, it is C underneath emulating the look and feel, and there are some important extensions. It is not necessary to specify commas after every argument, or even the "=" sign, in fact. More significant, certain keywords will trigger mdgx to take in many subsequent arguments, often in a free format order. It is a sort of keyword list within a keyword list, and the only requirement is that all of the grouped keywords appear on the same input file line. The GridSample keyword is a great example: it triggers a search for subsequent keywords like "{ }" (beginning and end of value range), "fbhw" (Flat Bottom Half Width) and "Krst" (harmonic restraint stiffness). Any other values it finds (until it finds another &namelist-specific keyword) are going ot be assumed to be ambmask atom masks specifying a single atom. If it finds two such masks, it says "bond restraints." Three, "angles," and four, "dihedral restraints." All of this is in the service of making NMR-like restraints with an array of target values covering the range. The mdgx onboard manual is a good reference for additional keywords in the &configs namelist. Run mdgx -CONFIGS on the command line to see this namelist description. (Note: most of these keywords are case-sensitive.

All that may look complicated, but it accomplishes things that would take a long, dedicated bash script driving sander to do the same thing. Such a script would be full of awk commands to post-process intermediate outputs as the MD program performed a total of 128 optimizations. The input above should run in under a minute, and when it does the following things happen:

  • 64 conformations are produced, sampling conformations of the center residue's Φ and Ψ coordinates every 45°, starting from the initial state in HID.top. The "combine" keyword is crucial here: it splits the sampling across two dimensions given in restraints "1" and "2." Without it, the restraints would increment at the same time, making a line of conformations with Φ and Ψ increasing at the same time.
  • The results of the first round of energy minimizations are reshuffled and become input coordinates for the same set of targets. The reshuffling follows a 'bootstrap' approach: random reordering, with replacement. For each minimization, a random number between 1 and 64 is chosen, and that number points to the minimized conformation produced with one of the Φ / Ψ restraint targets. The same solution can become an input to more than one subsequent optimization with 'bootstrap.' For random resampling without replacement, choose a 'jackknife' shuffle.
  • If the next round of optimizations produces structures with lower energy than the first round, they are accepted and replace the first round solutions.
  • The shuffling process is repeated a second time.
  • Conformations wherein the sum of all restraint penalties in the problem exceeds 20.0 kcal/mol, or any one bond or angle is strained by more than 10.0 kcal/mol, are purged form the results, not printed to the output. Only the best conformation for each Φ / Ψ target is printed, but statistics will be reported for the success rate and progress made by the reshuffling.
  • Acceptable conformations are printed in NetCDF and PDB formats.

To run this example, download the HID topology and associated coordinates, then run the mdgx executable with the above input (I've called the command file cfsamp_I.in):

>> ${AMBERHOME}/bin/mdgx -O -i cfsamp_I.in

The output, which the reader may examine as needed, indicates several important aspects of the run. First, the average energies for all conformations improve considerably with respect to the force field guiding the optimization.

Initial E(Model)         42.3151      0.0000      42.3151      42.3151
Initial E(Restraint)    149.8428     77.9343       1.0140     314.4673
Final E(Model)          -12.8046      5.0342     -22.2319       0.0364
Final E(Restraint)        0.2397      0.3362       0.0000       1.8405
Delta E(Model)          -55.1197      5.0342     -64.5469     -42.2787
Delta E(Restraint)     -149.6031     78.0114    -314.1727      -0.6323
Reoptimization           -1.2848      2.4688      -9.8811       0.0000

All structures started from one initial state, so the standard deviation in their initial energies is zero. The minimizations required, on average, 1745 steps to converge, all configuration minimizations did converge, and all resulting structures passed the sanity checks. There were 18 successful reoptimizations and 17 of these produced lower energy configurations than the original attempts.

No motivation was given for optimizing this tetrapeptide all over its Φ and Ψ space, but the example comes from a protein force field development project wherein conformations were needed for charge fitting to quantum electrostatic potentials. In order to get a good result that can guide force field development of a fixed charge model, it is important not to let the molecule get into conformations that would change its electronic state. Hydrogen bonding is the biggest risk along those lines, so it is important not to let any of the conformations bring a hydrogen donor too close to another atom with a free Lewis electron pair. Visual inspection is tedious, error prone, and subjective. Instead, we will add the following input to prevent hydrogen bonding between atoms of subsequent residues in the backbone:

  Set  :1@O  :2@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :1@O  :3@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :1@O  :4@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :1@O  :5@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :2@O  :3@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :2@O  :4@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :2@O  :5@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :3@O  :4@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :3@O  :5@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,
  Set  :4@O  :5@H  { 50.0 50.0 }  fbhw 47.5  Krst 64.0,

Looks can be deceiving: if the goal is to keep two atoms apart, why add restraints that will compel them to come together? The trick lies in the range of the restraints. Two masked atoms tell mdgx "distance" and the program then looks for a range inside of the { } braces. The upper and lower bounds of this range are 50Å, but there is another important number: the Flat Bottom Half Width. Setting this to 47.5Å turns the restraint into: "let the atoms get up to 97.5Å apart (which they never will), but if they get closer than 2.5Å start applying a 64 kcal/mol harmonic penalty." This will effectively block the molecular mechanics model from forming anything like a hydrogen bond.

Another important feature of a force field training set is sampling in the relevant degrees of freedom. The position of the side chain should vary from one conformation to the next, but perhaps not in a systematic way alongside the backbone. In order to accomplish this, we can add a RandomSample instruction. RandomSample works like GridSample, but the restraint values are randomly chosen from within the range given in { }. No "combine" keyword is needed to decorrelate RandomSample instructions. The restraint stiffness is also reduced in this case, to let the conformations stick to one rotamer or another.

  RandomSample  :3@CG  :3@CB  :3@CA  :3@N   { -180.0 180.0 }  Krst 16.0,
  RandomSample  :3@ND1 :3@CG  :3@CB  :3@CA  { -180.0 180.0 }  Krst 16.0,

The input file is here. The Flat Bottom Half Width is of little consequence with this lighter restraint, but still we can see that there are conformations that fail the sanity checks:

- Configurations passing all sanity checks:       60
- Configurations failing bond sanity check:        0
- Configurations failing angle sanity check:       0
- Configurations failing restraint sanity check:   4

The failures are described in the next section of the output. These exercises also generate loads of PDB files and two amber trajectories. The PDB files, one of which from the second exercise is here, are a very low-density, low-precision way to record the output, but they are easy to visualize. The &configs module hijacks the PDB format to deliver more information about each conformation in the PDB REMARK fields. Look at the top of Conf5.pdb:

HEADER  Printed by mdgx
REMARK  4
REMARK  4 Topology used to create this configuration:
REMARK  4  HID.top
REMARK  4
REMARK  4 Restraints used to create this configuration:
REMARK  4 &rst
REMARK  4  iat=15,17,19,32,
REMARK  4  r1=-196.1479, r2=-167.5000, r3=-147.5000, r4=-118.8521,
REMARK  4  rk2=64.0000, rk3=64.0000,
REMARK  4 &end
...
REMARK  4 &rst
REMARK  4  iat=25,24,21,19,
REMARK  4  r1=149.6376, r2=178.2855, r3=178.2855, r4=206.9334,
REMARK  4  rk2=16.0000, rk3=16.0000,
REMARK  4 &end
REMARK  4
REMARK  4 Molecular mechanics energy decomposition (kcal/mol):
REMARK  4  Bond                1.7605
REMARK  4  Angle              25.4248
REMARK  4  Dihedral            0.5556 (sum of proper and improper terms)
REMARK  4  van-der Waals       0.7023 (includes 1-4 interactions)
REMARK  4  Electrostatic     -30.9217 (includes 1-4 interactions)
REMARK  4  Restraints          1.3396
REMARK  4  Total energy       -1.1389 (includes restraint energy)

The restraints given in that REMARK section are what sander would read to perform the same optimization in vacuo. It is an exercise for the reader to isolate the fifth conformation and then make a short minimization input file with the attached restraints to see that sander cannot, in fact, minimize the structure any further. Notice how the sander restraints would require atom numbers in the topology--this is another convenience of the &configs module, that atoms may be specified by their names, rather than counting their positions in the topology. The four restraint parameters in each of the &rst namelists are also computed by mdgx based on more intuitive input in the { } ranges. It is not covered in this tutorial, but the user can also specify the point at which the NMR restraints go from quadratic to linear.

Here are some examples of the conformations produced:

Ace-Ala-Hid-Ala-Nme conformations

The &configs module of mdgx makes it very simple to manage huge numbers of elaborate energy minimizations for manipulating small molecules in vacuo. The code has recently gained a modest Generalized Born capability in other areas, so this feature may become part of &configs in a future patch. For complex molecules with 80-100 atoms, the minimizations can easily get stuck in local minima, or access desired regions of conformational space only under great strain. In these cases the shuffling feature is especially useful, as it can find less and less strained ways to get the molecule's internal coordinates into the desired conformations. Another feature that may be added, in time, is a loop builder based on this technology.

"How's that for maxed out?"

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