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Related Concept Videos

Newman Projections02:06

Newman Projections

Different notations are used to represent the three-dimensional structure of molecules on two-dimensional surfaces. One of the most commonly used representations is the dash-wedge formula. The dashed wedges, solid wedges, and the plane lines indicate the groups situated behind the plane, coming out of the plane, and in the plane, respectively.
The organic molecules rotate across the single bonds leading to numerous temporary three-dimensional structures of varying energy known as conformers.
Noncovalent Attractions in Biomolecules02:35

Noncovalent Attractions in Biomolecules

Noncovalent attractions are associations within and between molecules that influence the shape and structural stability of complexes. These interactions differ from covalent bonding in that they do not involve sharing of electrons.
Four types of noncovalent interactions are hydrogen bonds, van der Waals forces, ionic bonds, and hydrophobic interactions.
Hydrogen bonding results from the electrostatic attraction of a hydrogen atom covalently bonded to a strong-electronegative atom like oxygen,...
Noncovalent Attractions in Biomolecules02:35

Noncovalent Attractions in Biomolecules

Noncovalent attractions are associations within and between molecules that influence the shape and structural stability of complexes. These interactions differ from covalent bonding in that they do not involve sharing of electrons.
Four types of noncovalent interactions are hydrogen bonds, van der Waals forces, ionic bonds, and hydrophobic interactions.
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Molecular Orbital Theory II03:51

Molecular Orbital Theory II

Molecular Orbital Energy Diagrams
Molecular Shapes01:18

Molecular Shapes

Molecules have characteristic shapes that are crucial for their function. The arrangement of various electron groups around the central atom dictates their molecular geometry. Electron pairs in the valence shell of a central atom will adopt an arrangement that minimizes repulsions between the electron pairs by maximizing the distance between them. The valence electrons form either bonding pairs, located primarily between bonded atoms, or lone pairs.
Two regions of electron density in a diatomic...
Structure of Conjugated Dienes01:16

Structure of Conjugated Dienes

Introduction
Conjugated dienes are compounds characterized by the presence of alternating double and single bonds. In a conjugated system like 1,3-butadiene, the unhybridized 2p orbital on each carbon overlaps continuously, allowing the π electrons to be delocalized across the entire molecule. In contrast, this type of overlap does not occur in cumulated and isolated dienes, such as 2,3-pentadiene and 1,4-pentadiene, respectively. Instead, the π electrons remain localized between the double...

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Related Experiment Video

Updated: May 16, 2026

Hybrid Ensemble and Single-molecule Assay to Image the Motion of Fully Reconstituted CMG
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Published on: July 26, 2024

Collective motion of dimers.

Catherine J Penington1, Karolína Korvasová, Barry D Hughes

  • 1Department of Mathematics and Statistics, University of Melbourne, Victoria 3010, Australia.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|December 11, 2012
PubMed
Summary

This study models dimer agents on lattices, developing equations for collective motion. The findings offer insights into how elongated cell populations move together.

Area of Science:

  • Physics
  • Mathematical Biology
  • Statistical Mechanics

Background:

  • Collective cellular motion is crucial in biological processes.
  • Many cell types are elongated, influencing their collective behavior.
  • Existing models often simplify cell shapes or interactions.

Purpose of the Study:

  • To develop a discrete agent-based model for collective motion of dimer agents.
  • To derive continuum partial differential equations describing population dynamics.
  • To investigate the influence of exclusion rules on agent movement.

Main Methods:

  • Agent-based modeling on one- and two-dimensional lattices.
  • Application of indicator variables and probability arguments.
  • Derivation of discrete-time master equations and continuum limit equations.

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  • Mean-field approximation and analysis of advection-diffusion equations.
  • Main Results:

    • A systematic derivation of master equations for dimer agent dynamics.
    • Obtained nonlinear diffusion equations for average dimer occupancy.
    • Showed that interacting subpopulations lead to advection-diffusion equations.
    • Validated continuum models against discrete simulation data.

    Conclusions:

    • The developed models accurately describe dimer agent collective motion.
    • The framework provides insights into the population-level behavior of elongated cells.
    • This work bridges discrete modeling and continuum partial differential equations for biological systems.