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A Simple Aromatic
Structure of liquid benzene from isotopic neutron data
80 minutes
Summary
You might always be asking the question “How much does quantity X differ between the equilibrated simulation at the reference forcefield parameters, and the refined simulation at the empirical parameters?”. This is a very important question, and this example will show how to checkpoint simulation data for comparison later on. It will also introduce the utility of size factor scaling when dealing with molecular systems containing rings.
You will set up and equilibrate a small liquid benzene simulation before calculating a few properties of interest, and then refine the potential against experimental data and recalculate the properties of interest to see how much they change. The data are three neutron scattering datasets measured on the NIMROD instrument at the ISIS Pulsed Neutron and Muon Source in 2014. We’ll be referencing the paper by Headen et al. along the way - “Structure of π-π Interactions in Aromatic Liquids”, T. F. Headen, C. A. Howard, N. T. Skipper, M. A. Wilkinson, D. T. Bowron and A. K. Soper, J. Am. Chem. Soc. 132, 5735 (2010).
Preparation
Download the example data as a zip or tar.gz and unpack it if you haven’t done so already. Alternatively, download the data files listed below and save them to a location of your choice.
- C6H6: C6H6.mint01
- C6H6:C6D6 (50:50): 5050.mint01
- C6D6: C6D6.mint01
File ⇨ New
File ⇨ Save As…
Save your input file under a sensible name in same directory as the example data
Step 1 - Create the Species
Draw the Molecule
The first thing we’ll do is draw a benzene molecule as best we can:
Species ⇨ Create ⇨ Draw…
A new editor window opens in which we can draw the rough geometry and connectivity for our molecule.
Select draw mode from the toolbar above the species viewer
Draw a roughly hexagonal ring of six carbon atoms (carbon is the default drawing element) by left-click-dragging in the viewer
Change the drawing element from
C
toH
by clicking on the button next to the draw mode icon
Connect a single hydrogen atom to each carbon by left-click-dragging from each carbon site
Your final species will look something like this:You can create bonds by left-click-dragging between two existing atoms.
A very badly drawn benzene molecule
Click
to close the editor and create the new species
Double-click on the NewSpecies tab and change its name to Benzene
Apply a Forcefield
Time to make it a little prettier! We’ll assign a standard forcefield to it, and optimise the geometry:
Species ⇨ Add Forcefield Terms…
From the available forcefields choose
OPLSAA2005/Aromatics
and click
You can filter forcefields by keywords in name and description by using the filter box at the top-right of the forcefield selection controls.
We will use the default Determine atom types for all atoms option to add atom types for every atom in the species, so click
There will be no conflicts with existing atom types as there are no atom types already defined, so click
For the intramolecular terms we want to assign them and reduce to master terms (the default settings) so click
to proceed
There will be no conflicts with existing master terms, so click
to exit the wizard
Click the
icon in the species viewer toolbar to optimise the geometry of the molecule using the forcefield we’ve just applied
We will also get ahead here and edit the master terms to reflect the geometry observed in the experimental data, since the forcefield we’ve applied here doesn’t get things quite right.
Go to the Forcefield tab, section
In the Bonds table change the equilibrium bond length parameter (eq) of the ‘CA-HA’ bond term from
1.08
to1.09
Å
Change the equilibrium bond length of the ‘CA-CA’ bond term from
1.40
to1.38
Å
Create Deuterated Isotopologue
Since some of the experimental data was measured on deuterated benzene, we’ll need to create a suitable C6D6 isotopologue:
Go to the Benzene species tab, and click on the section
Click
to create a new isotopologue for the species
Change the isotope for the HA atom type from
Natural (bc = -3.739 fm)
to2 (bc = 6.671 fm)
by clicking on the isotopologue entry and choosing from the drop-down menu
Change the name of the isotopologue to ‘C6D6’ (double-click on its name to do so)
The Natural
isotopologue is always available and doesn’t need to be created, but doesn’t appear in the list of user-defined isotopologues. It is also not necessary to create “mixed” isotopologues (e.g. for 50:50 mixtures of H:D) as these are created by mixing individual isotopologues.
Add Analysis Sites
We’ll locate our analysis site at the centre of the benzene ring and give it some axes so that we may calculate orientational / spatial functions around it. The figure below shows the atoms we’ll select to define the origin (purple), x-axis (red) and y-axis (blue). Using these atoms as reference points for our coordinate system will set the XY plane to that of the ring, with the z axis perpendicular to the ring, pointing out of its center.
Origin (purple), x-axis (red) and y-axis (blue) atoms defining the oriented benzene site
Go to the Benzene species tab
Select all six carbon atoms by shift-clicking on them in the viewer (you may need to click reset view first, to see the whole molecule)
Right-click the selected atoms and click
⇨ This creates a new site with the Carbon atoms as the Origin Atoms
Now select the single carbon atom (as depicted in the image above) and right click it.
Click
⇨ to define the direction of the x axis
Finally, shift-click the pair of adjacent carbon atoms and right click on them
Click
⇨ to define the direction of the y axis
Rename the site to
COG
by double-clicking its name
Step 2 - Set up a Configuration
Time to create a suitable liquid configuration for our simulation using the predefined “simple random mix” generator:
Configuration ⇨ Create…
Choose the benzene species and press
Leave the configuration type as Mixture and press
Leave the box style as Fixed Geometry, Undefined Size and press
Set the Density to
0.876
and the units tog/cm3
, and the Multiplier to100
. You’ll see that this gives us a box with side length of just over 24.5 Å which is fairly small, but in the interests of speed we’ll go with it for now so hit .
Double-click on the NewConfiguration tab’s title and change its name to Liquid
Initial, randomised benzene box containing 100 molecules
Since the molecules were added to the box completely at random, there will most likely be some that overlap quite a lot. Benzene has a ring which makes it possible for molecules to become permanently “interlocked”, but we can do our best to remove such contacts by using what Dissolve (and EPSR) call “size factor scaling”. Basically, this allows the configuration box and the positions of the molecules to be scaled (but keeping the internal geometry intact), removing bad overlaps and letting molecules move safely apart. The factor by which the box is scaled is reduced gradually until the initial requested system size is regained (i.e. corresponding to a size factor of 1.0).
In anticipation of some bad contacts:
Go to the Liquid configuration tab
Click the
on the bottom-left of the window
Drag the SizeFactor node into the Procedure section to add it
Set the value for the Size Factor to 10.0
Finally, before we move on, we will have to reduce our pair potential range from the default of 15 Å since this is larger than the half the maximum width of our simulation box.
Go to the Forcefield tab, section
In Control, reduce the pair potential Range from
15
to12
Å
For a cubic box, you can’t have a cutoff value greater than half the box length, as this means that a given atom will ‘see’ other atoms twice because of the periodic boundary conditions.
Step 3 - Set up Equilibration
To equilibrate our system we’ll now add a standard Monte Carlo / Molecular Dynamics processing layer:
Layer ⇨ Create ⇨ Evolution ⇨ Standard Molecular (MC/MD)
We can now start running our simulation and start to equilibrate the configuration box.
Ctrl-R
If you’re watching the box in the configuration tab you’ll notice that it intially “explodes” because of our defined size factor of 10.0, but the box will quickly reduce in size back to normal and result in a condensed phase with no interlocked benzene rings.
When the size factor has reduced the inter-molecular energy of the simulation will fluctuate a little, but should oscillate around some equilibrium value, at which point you can proceed. You can check this from the graphs of the Energy module:
Go to the Evolve (Standard) layer tab
Select the Energy module and go to its tab
Once this has been achieved, we can make a snapshot of the current simulation and store this equilibrated point as a backup. The restart file written by Dissolve as it runs stores all the information necessary to continue a stopped simulation, but there is no going back to a previous point in the simulation (e.g. to undo a bad analysis choice, or to reference earlier data) unless we have a suitable restart point to go back to. At any time we can write a new restart file from the GUI, independent of the standard restart file, and which we can keep to load in at a later date.
Esc
File ⇨ Save Restart Point…
Change the filename to
equilibrated.restart
and click
Now we can move on to set up the analysis of the structural properties we’re interested in.
Step 4 - Set up Analysis
For our “properties of interest” we’ll calculate both the centre-of-geometry RDF and the out-of-plane angle between molecules as a function of distance. We can get both from the AxisAngle module:
Module | Purpose |
---|---|
AxisAngle | Calculates the distance vs. axis angle map between two sites |
Since our site (COG
) is set up for the Z axis to be pointing out of the plane of the benzene ring, it is the angle formed between these axes on the different molecules that we’ll focus on.
Let’s add an empty processing layer to to the simulation, add on our module, and set it up:
Layer ⇨ Create ⇨ Empty
Double-click the layer tab and rename it to
Analysis
Show the module palette for the current layer by clicking the
button at the bottom of the module list on the left
Drag a AxisAngle module up to the module list
Select the new AxisAngle module to show its
For the DistanceRange change the Bin Width to
10
For the AngleRange change the Max to
90
Enable the Symmetric option
This will account for the planar symmetry of the benzene ring, and map any calculated angles in the range 90 - 180° back in to 0 - 90°
Now we must tell the module which sites to use for its calculation:
Set both SiteA and SiteB to
COG
Set the AxisA and AxisB to
ZAxis
Enable the ExcludeSameMolecule to prevent the unwanted self-correlation spike at $r$ = 0 in the resulting RDF
It would also be nice here to calculate the spatial density function (the three-dimensional distribution of molecules around a reference point) and compare it, but this takes more iterations than a (sane) example will allow.
Step 5 - Calculate Baseline Properties
Now that the analysis processing layer is prepared, we need to run it for a while in order to get some good statistics on our quantities. A good 500 iterations (preferably 1000) is needed to get the statistics for the 2D map, so let’s ask Dissolve to run for a set number of steps:
Simulation ⇨ Run For…
Enter
1000
and click
Dissolve will now iterate for 1000 iterations and stop - you can see the estimated time remaining to complete these 1000 steps in the status bar at the bottom of the main window. Now might be a good time to have a drink, or write that email you’ve been putting off. If you think 1000 iterations is going to take too long, press Escape to stop the simulation and go for 500 iterations instead.
To see what’s being calculated, go back to the AxisAngle module and look at its output section:
Go to the Analysis layer
Click the AxisAngle module and select the section
We have three graphs - top-left is the radial distribution function between the centres-of-geometry of the benzene, while the bottom-left is the angle histogram of the z-axis angles (averaged over all distances). The main graph to the right shows the distance-angle map of the two quantities. You might want to explore the latter in 3D space, rather than a top-down view - you can change the view style for the plot in the toolbar at the top (change the view type from XY
to 3D
).
Once the iterations have completed, we need to do a bit of housekeeping.
Snapshot the Current Data
Let’s save the current data now, as it represents our reference point against which we’ll compare things later on:
File ⇨ Save Restart Point…
Change the filename to
reference.restart
and click
You might also find it useful to copy images of the graphs here to help with comparison later on - right-click on an empty part of the graph and select Copy to clipboard - or you can right-click on a particular curve and save the data directly in order to plot it in some other external software.
Clear the Current Data
Since we’re about to refine our simulation against experimental data and re-run the analysis, we don’t want to retain any of the currently-calculated quantities. We can request that Dissolve clear all of the data generated by modules and reset the simulation back to an “empty” state. Critically, the current contents of any configurations will remain untouched (i.e. our equilibrated box will remain in its present state, so we can proceed directly on with the simulation). It will also reset the iteration counter to zero.
Time to get rid of that data…
Simulation ⇨ Clear Module Data
Accept the consequences, and click
Turn off the Analysis Layer
We need to refine the simulation before we calculate our properties again, so we need to temporarily turn off our analysis layer:
Go to the Analysis layer
Disable the layer by clicking the Layer Enabled? button at the top-left of the tab so it displays
Step 6 - Set up Refinement
Time to refine. We’ll need two processing layers - one to calculate the g(r) and S(Q) from the simulation, and one to refine it against experimental data.
As noted in the introduction we have neutron-weighted experimental data, so we need a layer to calculate g(r) and neutron-weighted S(Q) for our three experimental datasets:
Layer ⇨ Create ⇨ Correlations ⇨ RDF and Neutron S(Q)
Open the module palette for the layer by clicking the
button at the bottom left of the tab
Drag two additional NeutronSQ modules from the Correlation Functions category to the module list, placing them after the existing NeutronSQ module
We need to set the instrumental broadening in the SQ module first:
Click on the SQ module to select it
Set the QBroadening to
OmegaDependentGaussian
with a FWHM of0.02
Now let’s set up the three NeutronSQ modules to calculate what we want:
C6H6
Click on the first NeutronSQ module to select it
Double-click on its name and change it to
C6H6
In the Reference Data settings group find the Reference keyword, select the file
C6H6.mint01
and set the format of the data tomint
C6D6
Click on the second NeutronSQ module to select it
Change its name to
C6D6
In the Control section click the button for the Isotopologue option
Press the
button to add the natural isotopologue for the first species present
Change the isotopologue from
Natural
toC6D6
Find the Reference Data settings group, and for the Reference keyword select the file
C6D6.mint01
and set the format of the data tomint
50:50 Mix
Click on the third NeutronSQ module to display its options
Change its name to
5050
In the Control section click the button for the Isotopologue option
Press the
button to add the natural isotopologue for the first species present
Select either row in the table and click the
button to insert the next unused isotopologue (i.e. the deuterated analogue)
The isotopologue mixture you’ve just defined has equal parts (weight = 1.0) of the
Natural
andC6D6
benzene isotopologues. You can use whatever ratios make sense - Dissolve will always normalise the total weight back to 1.0 internally.
Finally, find the Reference Data settings group and for the Reference keyword select the file
5050.mint01
and set the format of the data tomint
All that remains is to add our EPSR refinement layer:
Layer ⇨ Create ⇨ Refinement ⇨ Standard EPSR
All of the default values set there will be sufficient.
Step 7 - Refine the Simulation
Restart the simulation and monitor the progress of the r-factors and eReq value in the EPSR module.
Go to the Refine (EPSR) layer tab
Select the EPSR module and show its tab
Click the
tab to display the errors
You’ll see here a graph of the individual R-factors for the three datasets, as well as the total (summed) R-factor. The current “strength” of applied potential is shown at the bottom-left of the plot (Current EReq). Once you’ve been running for a few hundred steps the ereq value should have increased to 3.0, and the fits might look something like this (on the EPSR module):
tab of the
Comparison of reference vs simulated structure factors at ereq=3.0
The fits should be really quite good, but you might observe some “ripples” in the simulated structure factors at lower $Q$ values, as is the case in the image above. These do not arise from structure in the system, but rather are high-frequency Fourier ripples caused by truncation of the partial radial distribution functions, made worse in the present case because our system isn’t that large (100 molecules). We can remove some of that effect by introducing a window function into the Fourier transform when generating our structure factors:
First, stop the simulation if it’s running:
Esc
Go to the RDF / Neutron S(Q) layer tab
Select the SQ module
In the Control settings group change the WindowFunction to
Lorch0
Start the simulation running again and after a few steps you should see much smoother structure factors:
Comparison of reference vs simulated structure factors at ereq=3.0, and with the Lorch0 window function applied during Fourier transform of g(r) to S(Q)
Applying a window function in this way can have unwanted effects as well, with structural features “smoothed out”. Look closely at the C6D6 data around 1.5 < $Q$ < 2.0 and you can see that the pair of peaks has been somewhat blended together with the Lorch0 function applied.
With our refinement progressed to an acceptable level (in the data shown above the total r-factor is of the order of 5.5×10-4), we’re now in a position to save another restart point:
File ⇨ Save Restart Point…
Change the filename to
ereq3.restart
and click
Step 8 - Calculate Refined Properties
We now have our refined simulation that is in better agreement with the experimental data, so its time to recalculate our properties so that we can compare them to those we saved earlier. All the processing layers should now be enabled and remain on for the production run, including the refinement layer.
Go to the Analysis layer tab
Enable the layer by clicking the button in the Layer Control section so it displays
Simulation ⇨ Run For…
Enter 1000 and click
If you’re ready for another drink, now would be another opportune moment, or perhaps there’s another pressing email that needs hammering out?
Once those iterations have completed, we can move on to do the comparison of the data. Also, we can snapshot our production run data:
File ⇨ Save Restart Point…
Change the filename to
production.restart
and click
Step 9 - Compare Data
In the next two sections we’ll compare both the centre-of-geometry RDF and the axis angle map between the reference and refined simulations. How you do this is really up to you - you can load any of your restart points into Dissolve to see the data contained within, and then either:
- Export specific datasets to files and re-plot them side-by-side in your graphing software of choice.
- Take image snapshots / copy graphs to the clipboard and paste them in a document elsewhere.
- Run two copies of Dissolve, and load different restart points into each, and compare “interactively”.
In the following sections we’ve exported the basic 1D curves and plotted them in external software, and we compare the 2D data side-by-side. Your results won’t look exactly the same, but should show the same trends.
Centre-of-mass Radial Distribution Functions
We’ll begin with the centre-of-mass (ring centre) RDFs.
Equilibrated and refined centre-of-mass RDFs
As you can see the differences are quite subtle, but they are there. The refined (red) simulation shows a decrease in the main peak intensity, and an increase in probability of finding molecules at the shortest contact distances (around 4 Å). Looking at the probabilities between z-axis angles we observe that “flatter” angles are more likely in the refined simulation:
Equilibrated and refined Z-axis angle distributions
These functions only give us a hint at what the structural changes in the liquid are, however, and we need to combine them with the distance-angle map.
Distance/Angle Correlations
Equilibrated and refined distance/angle maps
The 2D function calculated by AxisAngle shows us variations in the centre-of-mass RDF with z-axis angle - the key feature is at the lowest angles (tending towards zero, at the bottom of the picture). The refined data on the right shows the emergence of a clear shoulder at 4 Å - as discussed in the paper by Headen et al. this corresponds to the presence of offset, parallel molecule stacking (see Figure 9 in that paper) which is minimal in the reference simulation. While it might be argued that this is a rather subtle change, it’s important to bear in mind that a typical off-the-shelf forcefield does not show this feature, and it only appears in a meaningful way when we refine against real-world, experimental data.