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Published on: April 12, 2019
Mathematical modeling and physical reality in noncovalent interactions.
Peter Politzer1, Jane S Murray, Timothy Clark
1Department of Chemistry, University of New Orleans, New Orleans, LA, 71048, USA, ppolitze@uno.edu.
The Hellmann-Feynman theorem interprets noncovalent bonding via Coulombic forces, not mathematical constructs. Physical forces like charge transfer are equivalent to polarization, distinguishing models from reality.
Area of Science:
- Quantum Chemistry
- Chemical Bonding Theory
Background:
- Noncovalent interactions are crucial in molecular systems.
- Existing interpretations often conflate mathematical formalisms with physical forces.
Purpose of the Study:
- To clarify the physical interpretation of noncovalent bonding using the Hellmann-Feynman theorem.
- To distinguish between mathematical components and physical forces in electronic structure calculations.
Main Methods:
- Application of the Hellmann-Feynman theorem to analyze noncovalent interactions.
- Interpretation of electronic density and wave function components.
Main Results:
- The Hellmann-Feynman theorem frames noncovalent bonding as Coulombic interactions, including polarization and dispersion.
- Mathematical terms like exchange and Pauli repulsion are artifacts of calculation, not physical forces.
- Charge transfer in noncovalent interactions is fundamentally polarization.
Conclusions:
- The Hellmann-Feynman theorem offers a physically meaningful interpretation of noncovalent bonding.
- It is essential to differentiate between the mathematical tools used in quantum chemistry and the underlying physical reality.
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