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Related Concept Videos

Polymer Classification: Crystallinity01:21

Polymer Classification: Crystallinity

Unlike ionic or small covalent molecules, polymers do not form crystalline solids due to the diffusion limitations of their long-chain structures. However, polymers contain microscopic crystalline domains separated by amorphous domains.
Crystalline domains are the regions where polymer chains are aligned in an orderly manner and held together in proximity by intermolecular forces. For example, chains in the crystalline domains of polyethylene and nylon are bound together by van der Waals...
Molecular Weight of Step-Growth Polymers01:08

Molecular Weight of Step-Growth Polymers

Step growth polymerization involves bi or multifunctional monomers. Bifunctional monomers react to form linear step growth polymers, whereas multifunctional monomers react to form non-linear or branched polymers.
As the step-growth polymerization involves step-wise condensation of monomers, the molecular weight also builds up eventually. Consequently, high molecular weight polymers are obtained at the late stages of the polymerization, where 99% of monomers have been consumed.
The extent of the...
Step-Growth Polymerization: Overview01:03

Step-Growth Polymerization: Overview

Step-growth or condensation polymerization is a stepwise reaction of bi or multifunctional monomers to form long-chain polymers. As all the monomers are reactive, most of the monomers are consumed at the early stages of the reaction to form small chains of reactive oligomers, which then combine to form long polymer chains in the late stages. Hence, the reaction has to proceed for a long time to achieve high molecular weight polymers.
Many natural and synthetic polymers are produced by...
Temperature Dependent Deformation01:12

Temperature Dependent Deformation

In a nonhomogeneous rod made up of steel and brass, restrained at both ends and subjected to a temperature change, several steps are involved in calculating the stress and compressive load. Due to the problem's static indeterminacy, one end support is disconnected, allowing the rod to experience the temperature change freely. Next, an unknown force is applied at the free end, triggering deformations in the rod's steel and brass portions. These deformations are then calculated and added together...
Polymer Classification: Stereospecificity01:26

Polymer Classification: Stereospecificity

Polymerization generates chiral centers along the entire backbone of a polymer chain. Accordingly, the stereochemistry of the substituent group has a significant effect on polymer properties. Polymers formed from monosubstituted alkene monomers feature chiral carbons at every alternate position in the polymer backbone. Relative to the predominant orientation of substituents at the adjacent chiral carbons, the polymer can exist in three different configurations: isotactic, syndiotactic, and...
Polymers: Molecular Weight Distribution01:10

Polymers: Molecular Weight Distribution

For any given polymer, the weight average molecular weight (Mw) is higher than, if not equal to, the number average molecular weight (Mn). The only situation in which the weight average molecular weight and the number average molecular weight are equal is when a polymer consists only of chains with equal molecular weight. However, this never happens in a synthetic polymer, since it is difficult to control the polymerization process up to a molecular level with accuracy to a hundred percent.

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Related Experiment Video

Updated: Jun 17, 2026

Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses
08:55

Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses

Published on: June 7, 2018

Condensation transition in polydisperse hard rods.

M R Evans1, S N Majumdar, I Pagonabarraga

  • 1SUPA, School of Physics and Astronomy, University of Edinburgh, Mayfield Road, Edinburgh EH9 3JZ, United Kingdom. m.evans@ed.ac.uk

The Journal of Chemical Physics
|January 19, 2010
PubMed
Summary

This study introduces a mass transport model for polydisperse hard rods, revealing a factorized steady state distribution that minimizes free energy. The model predicts a condensation transition for particles with variable sizes (p>1).

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Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
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Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level

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Last Updated: Jun 17, 2026

Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses
08:55

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Published on: June 7, 2018

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Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level
06:55

Synthesis of Cyclic Polymers and Characterization of Their Diffusive Motion in the Melt State at the Single Molecule Level

Published on: September 26, 2016

Area of Science:

  • Statistical Mechanics
  • Soft Matter Physics
  • Thermodynamics

Background:

  • Studying polydispersity in physical systems is crucial for understanding complex fluid behavior.
  • Previous work focused on hard sphere fluids, but lacked a dynamic mass transport perspective.
  • The interplay between particle size distribution and phase transitions requires further investigation.

Purpose of the Study:

  • To develop and analyze a mass transport model for polydisperse hard rods with variable diameters.
  • To identify the steady-state size distribution and its relation to free energy minimization.
  • To investigate the emergence of phase transitions, specifically condensation, in this system.

Main Methods:

  • Stochastic mass transport simulations on a ring.
  • Analytical derivation of the steady-state distribution.
  • Application of density functional theory (DFT).

Main Results:

  • A factorized steady-state distribution was found, minimizing free energy for polydisperse hard rods.
  • The model accurately describes systems where particle size scales as v(i)^(1/p).
  • A real-space condensation transition occurs for p>1, forming macroscopic aggregates coexisting with a fluid phase.

Conclusions:

  • The study bridges stochastic mass transport and polydispersity in hard sphere fluids.
  • The derived distribution represents an optimal polydispersity for minimizing free energy.
  • The findings provide insights into condensation phenomena in systems with variable particle sizes.