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Related Concept Videos

¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the others.
Hybridization of Atomic Orbitals I03:24

Hybridization of Atomic Orbitals I

The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
¹H NMR: Pople Notation01:09

¹H NMR: Pople Notation

The Pople nomenclature system classifies spin systems based on the difference between their chemical shifts. Coupled spins are denoted by capital letters with subscripts indicating the number of equivalent nuclei. When the coupled nuclei have well-separated chemical shifts, they are assigned letters that are far apart in the alphabet, such as A and X. When the difference in chemical shifts is small, coupled nuclei are named using adjacent letters of the alphabet (AB, MN, or XY).
A proton...
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
Atomic Orbitals02:44

Atomic Orbitals

An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.

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Related Experiment Video

Updated: May 27, 2026

Spatial Separation of Molecular Conformers and Clusters
10:37

Spatial Separation of Molecular Conformers and Clusters

Published on: January 9, 2014

HPAM: Hirshfeld Partitioned Atomic Multipoles.

Dennis M Elking1, Lalith Perera, Lee G Pedersen

  • 1University of North Carolina, Department of Chemistry, Chapel Hill, NC 27599, USA.

Computer Physics Communications
|December 6, 2011
PubMed
Summary
This summary is machine-generated.

The Hirshfeld-Iterated (HD-I) method accurately calculates atomic charges and multipoles, outperforming the standard Hirshfeld (HD) method in reproducing molecular electrostatic properties. Increasing multipole rank improves precision for these essential chemical calculations.

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Area of Science:

  • Computational chemistry
  • Quantum chemistry
  • Theoretical chemistry

Background:

  • Accurate atomic charge and multipole calculations are crucial for understanding molecular electrostatic properties.
  • Existing methods like Hirshfeld (HD) provide foundational approaches to charge partitioning.
  • Limitations in reproducing electrostatic properties necessitate improved partitioning schemes.

Purpose of the Study:

  • To implement and evaluate the Hirshfeld-Iterated (HD-I) atomic charge density partitioning scheme.
  • To assess the accuracy of HD and HD-I methods for calculating atomic charges and multipoles.
  • To compare the performance of HD and HD-I against ab initio calculations for molecular electrostatic properties.

Main Methods:

  • Implementation of Hirshfeld (HD) and Hirshfeld-Iterated (HD-I) atomic charge density partitioning.
  • Calculation of atomic charges and multipoles up to l(max)=4 (hexadecapoles).
  • Comparison of calculated molecular multipole moments and electrostatic potentials (ESP) with reference ab initio data.

Main Results:

  • HD-I generally shows superior reproduction of ab initio electrostatic properties compared to HD.
  • Increasing the atomic multipole rank (l(max)) systematically enhances precision.
  • Atomic multipoles up to rank l(max) exactly reproduce ab initio molecular multipole moments for L ≤ l(max).
  • Using only atomic charges (l(max)=0) for HD or HD-I results in significant errors in molecular dipole moments.

Conclusions:

  • The HD-I method offers improved accuracy for atomic charge and multipole calculations.
  • Higher-rank multipoles are essential for precise electrostatic property reproduction.
  • Simple atomic charges from HD or HD-I alone are insufficient for accurate molecular dipole moment calculations.