Stress-strain curve: Fracture point

This tutorial demonstrates how to set up a molecular dynamics calculation with an increasingly deformed unit cell in order to study the mechanical properties of a small polymer chain model. During the simulation, the strain on the chain is increased slowly until the initial double bonds of the cis-Polyacetylene are successively converted into their trans configurations. Afterwards, an even larger strain causes the polymer chain to snap which immediately reduces the stress to zero. The stress tensor components computed during the MD simulation are then collected with a small Python script and plotted to demonstrate different changes in the molecular structure of chain.



With AMS2020 and later versions, the deformation of the Polyacetylene chain demonstrated in this tutorial can also be realized using a 1D periodic lattice. To use a 1D periodicity, the deformation of the x-axis needs to be set and the Polyacetylene chain needs to be rotated accordingly.

Step 1: Start the GUI

We will set up an MD simulation from the GUI. Alternatively, you can download this

Start AMSjobs
SCM → New input
Switch to ReaxFF: ADFPanel ReaxFFPanel

Step 2: Import Structure and Settings

We begin by setting the main calculation options for the molecular dynamics simulation.

In the menu bar, File → Import Coordinates…
In the main panel, select Force Field: → CHO.ff

Next, set the options for molecular dynamics:

Click on MoreBtn next to Molecular Dynamics
As Number of steps, enter 850000
As Sampling frequency, enter 10000
As Checkpoint frequency enter 50000

The simulation should run at constant temperature, so we add a thermostat:

Click on MoreBtn next to Thermostat and add a Thermostat
Select NHC
As Temperature, enter 300.15 K
As Damping Constant, enter 100.0 fs

Next, we have to set up the deformation so that the chain is stretched during the simulation.

Select Model → MD Deformations, and add a deformation
Set the second field in Length velocity 0.000020 A/fs.

Lastly, we need to calculate the stress tensor

Properties → Gradients, Stress Tensor Check stress tensor.

Step 3: Run the Calculation

After having set all calculation options we are now ready to start the run

In the menu bar, select File → Save and enter PolyStressStrain
In the menu bar, select File → Run
Switch to AMSmovie by clicking on SCM → Movie to see the polymer change under strain

Step 4: Evaluate the Results

Once the calculation has finished, the stress-strain curves can be extracted from the binary results file with the help of a Python script using the PLAMS library.

The script called can be run from the command line:

$AMSBIN/amspython PolyStressStrain

Be sure to match the job name correctly.

The stress-strain curve is written to a file called stress-strain-curve.csv:

# strain_x, strain_y, strain_z, stress_xx, stress_yy, stress_zz
0.0000 0.0000 0.0000 -0.000002123540 0.000041449314 -0.000000198040
0.0000 0.0026 0.0000 0.000001083810 0.000039450993 0.000000882455
0.0000 0.0053 0.0000 -0.000006368834 0.000040380759 0.000000145990
0.0000 0.0079 0.0000 0.000000862343 0.000039169395 0.000001048778
0.0000 0.0105 0.0000 0.000000339014 0.000050208909 -0.000000796209
0.0000 0.0132 0.0000 0.000000671946 0.000050569092 0.000001392349
0.0000 0.0158 0.0000 0.000009834386 0.000061383368 0.000003143092
0.0000 0.0184 0.0000 0.000000607648 0.000053138974 0.000005960118
0.0000 0.0211 0.0000 -0.000005062346 0.000046333020 0.000000554734

The resulting stress/strain curve can then be plotted as stress_yy (column 5) against strain_y (column 2) with any plotting software, e.g. matplotlib:


You can download an example script, which can be run with amspython to generate an image called stress-curve.png.

Note the different segments in the stress/strain plot. The first of these segments starts correspond to the polymer chain having increasingly more double bonds in trans configuration. After the last double bond has been converted the resulting trans-Polyacetylene chain exhibits different mechanical properties which results in a different slope of the stress/strain graph. At a certain strain, the chain snaps, immediately reducing the stress to zero as beyond this point the periodic polymer chain has turned into a molecular entity.