13. Thermochemistry Estimation

This section gives in-depth descriptions of the methods used for determining thermochemistry of species.

Thermochemistry of species is obtained via three possible ways:

  1. Species thermochemistry libraries
  2. Group contribution methods
  3. On-the-fly Quantum-chemical calculation of Thermochemical Properties (QMTP)

13.1. Species thermochemistry libraries

These databases contain thermochemical parameters for species. In these databases each entry contains an unambiguous definition of the species (through the adjacency list representation), along with a values for the thermochemistry in a format that allows the evaluation of each thermodynamic variable as a function of temperature.

RMG is shipped with a number of species thermochemistry libraries, located in the ‘libraries’ folder of RMG-database. More information on these species thermochemistry libraries can be found in Thermo Database.

13.2. Group contribution methods

When the thermochemistry of a species is not present in one of the available species thermochemistry libraries, RMG needs to estimate thermochemistry. One way to do so, is by using group contribution methods that estimate the thermochemistry of a molecule based on the sub-molecular fragments present in the molecule. The Benson group additivity framework is such an example of a group contribution method that has proven to provide accurate estimates of the ideal gas thermochemistry for a large range of molecules.

Benson’s Group Additivity approach ([Benson]), divides a molecule into functional groups, and the contribution of each functional group to the overall thermochemistry is included. For example, the molecule 2-methylnonane consists of three types of groups:

  • 1 tertiary carbon atom
  • 6 secondary carbon atoms
  • 3 primary carbon atoms
../../_images/BensonGA.PNG

Thermochemistry for the molecule X is calculated by summing up the values for each of the contributions \(C_{i}\). E.g.:

\[\Delta_fH_{298}^{o}(X) = \sum_{i}GAV(C_{i})\]

The term ‘group additive value’ (GAV) denotes a polyvalent (ligancy > 1) monoatomic central atom \(C_{i}\) surrounded by its nearest-neighbor ligands.

Values for each central atomtype (e.g. “tertiary carbon atom”) and its surrounding ligands can be found in the thermo group database, named group.py, of RMG. More information can be found here: Thermo Database.

13.2.1. NNIs

Besides the main group-centered (GAV) contributions, non-next-nearest neighbor interactions (NNI) may also be important to take into account. NNIs are interactions between atoms separated by at least 2 atoms, such as alkane 1,4-gauche, alkane 1,5 (cf. figure), alkene 1,4-gauche, alkene single and double cis, ene-yne cis and ortho interactions.

../../_images/15Alkanae.png

As a result, thermochemistry of the molecule X is determined as :

\[\Delta_fH_{298}^{o}(X) = \sum_{i}GAV(C_{i}) + \sum_{j}NNI_{j}\]

RMG contains a database with NNIs, named gauche.py and int15.py. More information on the nature on the available NNIs, and corresponding values can be found here: Thermo Database.

13.2.2. Ring Strain

To account for ring strain, ring strain corrections (RSC) were introduced. Because there is no obvious relation between the RSC and the ring structure, a specific RSC is required for every type of ring. For example, due to the significant ring strained induced in norbornane (cf. figure), a ring correction (RSC) needs to be added to the sum of the GAVs of the individual carbon atoms:

../../_images/norbornane.png

As a result, thermochemistry of the molecule X is determined as :

\[\Delta_fH_{298}^{o}(X) = \sum_{i}GAV(C_{i}) + RSC\]

RMG contains a database with single-ring corrections, ‘ring.py’ and polycyclic ring corrections, ‘polycyclic.py’. More information on the nature on the available NNIs, and corresponding values can be found here: Thermo Database.

13.2.3. Hydrogen Bond Increment (HBI) method

Lay et al. [Lay] introduced the hydrogen bond increment (HBI) method to predict thermochemical properties of radicals. In contrast to Benson’s method, the HBI method does not use the group-additivity concept. The HBI enthalpy of formation of a radical (R*) is calculated from the enthalpy of formation of the corresponding parent molecule (R-H) by adding a HBI to account for the loss of a hydrogen atom. Hence, for standard enthalpies of formation the HBI is defined as

\[HBI = \Delta_fH_{298}^{o}(R^*) - \Delta_fH_{298}^{o}(R-H) = BDE(R-H) - \Delta_fH_{298}^{o}(H*)\]

with BDE the bond dissociation enthalpy of the R-H bond at the radical position. Similar expressions are valid for the entropy and heat capacity.

As a result the thermochemistry of the radical is calculated as follows:

\[ \begin{align}\begin{aligned}\Delta_fH_{298}^{o}(R^*) = HBI(\Delta_fH_{298}^{o}) + \Delta_fH_{298}^{o}(R-H)\\C_{p}^{o}(R^*) = HBI(C_{p}^{o}) + C_{p}^{o}(R-H)\\S_{298}^{o}(R^*) = HBI(S_{298}^{o}) + S_{298}^{o}(R-H)\end{aligned}\end{align} \]

The HBI method is the default method use to estimate thermochemistry of radicals. Thus, the effect of resonance stabilization on the enthalpy of the radical will be accounted for through the corresponding HBI. For example, the HBI labeled as “C=CC=CCJ” will account for the resonance present in 1,4-pentadien-3-yl radical.

The HBI method can be applied to a variety of saturated compound thermochemistry values. In RMG, library values for saturated compounds are prioritized over group additivity values for saturated compounds. Note that if QMTP is on, the QM saturated value will get priority over group additivty but library value will have priority over QM value. This ensures that there is a systematic HBI correction for values used in the final model: if the saturated molecule thermo uses a library as a source, the radical thermo applies the HBI correction to that same library value.

RMG contains a database for with HBIs, named radical.py. More information on the nature on the available HBIs, and corresponding values can be found here: Thermo Database.

13.3. On-the-fly Quantum-chemical calculation of Thermochemical Properties (QMTP)

An interface for performing on-the-fly quantum and force field calculations has been developed and integrated into RMG to complement the species thermochemistry databases and group contribution methods [Magoon and Green]_. This interface is particularly interesting for the estimation of thermochemistry of molecules that are not present in one of the species thermochemistry databases, and which cannot be estimated with sufficient accuracy using the Benson group additivity framework. This pertains specifically to polycyclic fused ring containing species, whose ring strain cannot be modeled using the available ring corrections in RMG’s ring strain correction databases.

The QMTP interface involves a number of steps, summarized in the figure below.

../../_images/QMTP.jpg

In a first step the connectivity representation is converted into a three-dimensional structure of the molecule through the generation of 3D coordinates for the atoms in the molecule. This is accomplished using a combination of a distance geometry method, followed by a optimization using the UFF force field available in RDKit [RDKit]. Next, an input file is created containing the 3D atomic coordinates along with a number of keywords. This file is sent to a computational chemistry package, either OpenMopac or Gaussian, that calculates the thermochemistry of the given molecule “on-the-fly”. The keywords specify the type of calculation, and the level-of-theory. Finally, the calculated thermochemistry data is sent back to RMG.

The QMTP calculation creates a folder ‘QMfiles’ that contains a number of files that are created during the process. The filename of these files is a combination of the InChI key of the molecule, and a specific filename extension, e.g.

WEEGYLXZBRQIMU-UHFFFAOYSA.out is the output file produced by the QM package for the molecule cineole (SMILES: CC12CCC(CC1)C(C)(C)O2), represented by the InChI key WEEGYLXZBRQIMU-UHFFFAOYSA.

The table belows shows an overview of the used file extensions and their meaning.

File extension Meaning
.mop MOPAC input
.out MOPAC output
.gjf Gaussian input
.log Gaussian output
.arc MOPAC input created by MOPAC
.crude.mol Mol file using crude, unrefined
.refined.mol Mol file using UFF refined geometry
.symm SYMMETRY input
.thermo thermochemistry output file

For efficiency reasons, RMG minimizes the number of QMTP calculations. As a result, prior to initializing a QMTP routine, RMG checks whether the output files of a specific QMTP calculation are not already present in the QMfiles folder. It does so by comparing the InChI key of the given species to the filenames of the files in the QMfiles folder. If none of the InChI keys of the files correspond to the InChI key of the given species, RMG will initiate a new QMTP calculation.

13.3.1. Supported QM packages, and levels of theory

The following table shows an overview of the computational chemistry packages and levels of theory that are currently supported in the QMTP interface of RMG.

The MM4 force field software originates from Allinger and Lii. [Allinger].

QM Package Supported Levels of Theory
OpenMopac semi-empirical (PM3, PM6, PM7)
Gaussian03 semi-empirical (PM3)
MM4 molecular mechanics (MM4)

13.4. Symmetry and Chirality

13.4.1. Symmetry

The notion of symmetry is an essential part of molecules. Molecular symmetry refers to the indistinguishable orientations of a molecule and can be represented by molecular groups or a symmetry number. RMG uses a symmetry number which is the number of superimposible configurations, which includes external symmetry and internal free rotors, which is described by detail by [Benson]. This is macroscopically quantified as a decrease of the entropy S by a term \(-R * ln(\sigma)\) with R the universal gas constant and \(\sigma\) the global symmetry number, corresponding to the number of indistinguishable orientations of the molecule.

In RMG, \(\sigma\) is calculated as the product of contributions of three symmetry center types : atoms, bonds and axes, cf. below.

\[\sigma = \prod_{i}\sigma_{atom,i}.\prod_{j}\sigma_{bond,j}.\prod_{k}\sigma_{axis,k}\]

More information can be found in the Ph.D Thesis of Joanna Yu [Yu].

For molecules whose thermochemistry is calculated through group contribution techniques, the rotational symmetry number is calculated through graph algorithms of RMG based on the above equation. If the thermochemistry is calculated through the QMTP process, the external, rotational symmetry number is calculatedµ using the open-source software SYMMETRY “Brute Force Symmetry Analyzer” [Patchkovskii]. This program uses the optimized three-dimensional geometry and calculates the corresponding point group.

13.4.2. Chirality

RMG does not take stereochemistry into account, effectively assuming a racemic mixture of mirror image enantiomers. As a result, a chirality contribution of \(+R * ln(2)\) is included in the entropy of the molecule.

Chirality for molecules whose thermochemistry is determiend using group contribution techniques is detected using graph algorithms similar to those used for determining the symmetry number. If the thermochemistry is calculated through the QMTP process, chirality is detected using the point group information obtained via the software SYMMETRY.

Chiral molecules belong to point groups that lack a superposable mirror image (i.e. point groups lacking \(\sigma_h\), \(\sigma_d\), \(\sigma_v\), and \(S_n\) symmetry elements).

13.5. References

[Benson]Benson, Sidney William. “Thermochemical kinetics.” (1976)
[Lay]Lay, T.; Bozzelli, J.; Dean, A.; Ritter, E. J. Phys. Chem. 1995, 99,14514-14527
[Allinger]Allinger, N. L., & Lii, J.-H. (2008). MM4(2008) and MM4(2003).
[Patchkovskii]Patchkovskii, S. (2003). SYMMETRY, http://www.cobalt.chem.ucalgary.ca/ps/symmetry/.
[Yu]“Estimation method for the thermochemical properties of polycyclic aromatic molecules” (Ph.D), Joanna Yu, M.I.T (2005)
[RDKit]Landrum, G. (2012). RDKit, http://rdkit.org.
[Benson]

System Message: WARNING/2 (/home/mark/workspace/RMG-Py/documentation/source/users/rmg/thermo.rst, line 286); backlink

Duplicate explicit target name: “benson”.

Benson, S.W. (1965), https://en.wikipedia.org/wiki/Benson_group_increment_theory