Pairwise intermolecular interaction energies between molecules of arbitrary symmetry: rotational averages in the weak interaction limit

1982 ◽  
Vol 35 (8) ◽  
pp. 1513 ◽  
Author(s):  
PE Schipper
Keyword(s):  
Interaction Energy ◽  
Intermolecular Interaction ◽  
Weak Interaction ◽  
Analytic Form ◽  
Interaction Energies ◽  
Dispersion Interactions ◽  
Intermolecular Interaction Energy ◽  
Electrostatic Induction ◽  
Moment Functions ◽  
Λ Point

The fully expanded expression for the Boltzmann-averaged pairwise intermolecular interaction energy of two molecules B and C of arbitrary symmetry is determined in the weak interaction limit (<kT), including all electrostatic, induction and dispersion interactions having an r-n dependence (where r is the B-C separation) for which n < 11. The method exploits the 'point moment function' (PMF) approach in which the Boltzmann-averaged energy is shown to reduce to a sum of terms, each containing a product of a PMF on B, and one on C. The point moment functions may be obtained in a general analytic form by averaging an arbitrary multipolar product for the isolated molecule. Two types of PMF (Δ, point chirality function, and Λ, point achirality function) are identified, leading to a natural division of contributions to the intermolecular interaction energy into those that are insensitive (ΛΛ contributions) and sensitive (ΔΔ contributions) to molecular chirality.

scholarly journals Dataset of Noncovalent Intermolecular Interaction Energy Curves for 24 Small High-Spin Open-Shell Dimers

2021 ◽  
Author(s):  
Katarzyna Madajczyk ◽  
Piotr Zuchowski ◽  
Filip Brzęk ◽  
Łukasz Rajchel ◽  
Dariusz Kędziera ◽  
...  
Keyword(s):  
Interaction Energy ◽  
Intermolecular Interaction ◽  
High Spin ◽  
Open Shell ◽  
Basis Set ◽  
Interaction Energies ◽  
Intermolecular Interaction Energy ◽  
Complete Basis ◽  
Complete Basis Set ◽  
Basis Set Extrapolation

<div>We introduce a dataset of 24 interaction energy curves of open-shell noncovalent dimers, referred to as the O24x5 dataset. The dataset consists of high-spin dimers up to eleven atoms selected to assure diversity with respect to interactions types: dispersion, electrostatics and induction. The benchmark interaction energies are obtained at the restricted open-shell CCSD(T) level of theory with complete basis set extrapolation aug-cc-pVQZ--> aug-cc-pV5Z.</div>

scholarly journals Dataset of Noncovalent Intermolecular Interaction Energy Curves for 24 Small High-Spin Open-Shell Dimers

2021 ◽  
Author(s):  
Katarzyna Madajczyk ◽  
Piotr Zuchowski ◽  
Filip Brzęk ◽  
Łukasz Rajchel ◽  
Dariusz Kędziera ◽  
...  
Keyword(s):  
Interaction Energy ◽  
Intermolecular Interaction ◽  
High Spin ◽  
Open Shell ◽  
Basis Set ◽  
Interaction Energies ◽  
Intermolecular Interaction Energy ◽  
Complete Basis ◽  
Complete Basis Set ◽  
Basis Set Extrapolation

<div>We introduce a dataset of 24 interaction energy curves of open-shell noncovalent dimers, referred to as the O24x5 dataset. The dataset consists of high-spin dimers up to eleven atoms selected to assure diversity with respect to interactions types: dispersion, electrostatics and induction. The benchmark interaction energies are obtained at the restricted open-shell CCSD(T) level of theory with complete basis set extrapolation aug-cc-pVQZ--> aug-cc-pV5Z.</div>

Dataset of noncovalent intermolecular interaction energy curves for 24 small high-spin open-shell dimers

2021 ◽  
Vol 154 (13) ◽  
pp. 134106
Author(s):  
Katarzyna Madajczyk ◽  
Piotr S. Żuchowski ◽  
Filip Brzȩk ◽  
Łukasz Rajchel ◽  
Dariusz Kȩdziera ◽  
...  
Keyword(s):  
Interaction Energy ◽  
Intermolecular Interaction ◽  
High Spin ◽  
Open Shell ◽  
Intermolecular Interaction Energy

scholarly journals Crystal structures and Hirshfeld surface analyses of (E)-N′-benzylidene-2-oxo-2H-chromene-3-carbohydrazide and the disordered hemi-DMSO solvate of (E)-2-oxo-N′-(3,4,5-trimethoxybenzylidene)-2H-chromene-3-carbohydrazide: lattice energy and intermolecular interaction energy calculations for the former. Corrigendum

2019 ◽  
Vol 75 (12) ◽  
pp. 1952-1952
Author(s):  
Ligia R. Gomes ◽  
John Nicolson Low ◽  
James L. Wardell ◽  
Camila Capelini ◽  
José Daniel Figueroa Villar ◽  
...  
Keyword(s):  
Interaction Energy ◽  
Crystal Structures ◽  
Intermolecular Interaction ◽  
Lattice Energy ◽  
Hirshfeld Surface ◽  
Intermolecular Interaction Energy ◽  
Acta Cryst ◽  
Energy Calculations

In the paper by Gomes et al. [Acta Cryst. (2019), E75, 1403–1410], there was an error and omission in the author and affiliation list.

scholarly journals Intermolecular Non-Covalent Carbon-Bonding Interactions with Methyl Groups: A CSD, PDB and DFT Study

Molecules ◽  
2019 ◽  
Vol 24 (18) ◽  
pp. 3370 ◽  
Author(s):  
Tiddo J. Mooibroek
Keyword(s):  
Hydrogen Bonding ◽  
Solid State ◽  
Dft Calculations ◽  
Interaction Energy ◽  
Weak Interaction ◽  
Systematic Evaluation ◽  
Methyl Groups ◽  
Interaction Energies ◽  
Hydrogen Bonding Interactions ◽  
Carbon Bonding

A systematic evaluation of the CSD and the PDB in conjunction with DFT calculations reveal that non-covalent Carbon-bonding interactions with X–CH3 can be weakly directional in the solid state (P ≤ 1.5) when X = N or O. This is comparable to very weak CH hydrogen bonding interactions and is in line with the weak interaction energies calculated (≤ –1.5 kcal·mol−1) of typical charge neutral adducts such as [Me3N-CH3···OH2] (2a). The interaction energy is enhanced to ≤–5 kcal·mol−1 when X is more electron withdrawing such as in [O2N-CH3··O=Cdme] (20b) and to ≤18 kcal·mol−1 in cationic species like [Me3O+-CH3···OH2]+ (8a).

AN AB INITIO STUDY OF INTERMOLECULAR INTERACTION OF HYDROGEN FLUORIDE TETRAMER

2006 ◽  
Vol 05 (02) ◽  
pp. 187-196 ◽  
Author(s):  
JINSHAN LI
Keyword(s):  
Interaction Energy ◽  
Intermolecular Interaction ◽  
Density Functional ◽  
Ring Structure ◽  
Membered Ring ◽  
Basis Set ◽  
Intermolecular Interaction Energy ◽  
B3lyp Method ◽  
Three Body ◽  
Intermolecular Distances

Possible HF tetramer geometries have been optimized employing the density functional B3LYP method and the aug-cc-pVQZ basis set. Deformation energy has been calculated at the B3LYP/aug-cc-pVQZ level. After the BSSE correction with the CP method, two-body intermolecular interaction energy, three-body nonadditive intermolecular interaction energy, and four-body nonadditive intermolecular interaction energy (Δ E c[4]) have been obtained at the levels of B3LYP/aug-cc–pVQZ, B3LYP/aug-cc-pVTZ//B3LYP/aug-cc-pVQZ, and MP2/aug-cc-pVTZ//B3LYP/aug-cc-pVQZ. Calculated results show that the three-body nonadditive intermolecular interaction energy is important for the optimized structures of HF tetramer. At the MP2/aug-cc-pVTZ//B3LYP/aug-cc-pVQZ level, the four-body nonadditive intermolecular interaction strength arrives at -4.5kJ/mol in the optimized eight-membered ring structure, but is extremely weak in other optimized structures. The comparison between MP2 and B3LYP calculated intermolecular interaction energies shows that the B3LYP method is applicable to the calculation of the intermolecular interaction energy of HF tetramer when the basis set reaches aug-cc-pVTZ. ΔEc[4] occupies 8–32% of the total intermolecular interaction energy when the intermolecular distances of the eight-membered ring structure are in the range of 1.06–1.37 Å.

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