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The Fluid Mosaic Model01:34

The Fluid Mosaic Model

The fluid mosaic model was first proposed as a visual representation of research observations. The model comprises the composition and dynamics of membranes and serves as a foundation for future membrane-related studies. The model depicts the structure of the plasma membrane with a variety of components, which include phospholipids, proteins, and carbohydrates. These integral molecules are loosely bound, defining the cell’s border and providing fluidity for optimal function.
Fluid Mosaic Model01:19

Fluid Mosaic Model

Scientists identified the plasma membrane in the 1890s and its principal chemical components (lipids and proteins) by 1915. The model for plasma membrane structure, proposed in 1935 by Hugh Davson and James Danielli, was the first model to be widely accepted in the scientific community. The model was based on the plasma membrane's "railroad track" appearance in early electron micrographs. Davson and Danielli theorized that the plasma membrane's structure resembled a sandwich with the analogy of...
Structures of Solids02:22

Structures of Solids

Solids in which the atoms, ions, or molecules are arranged in a definite repeating pattern are known as crystalline solids. Metals and ionic compounds typically form ordered, crystalline solids. A crystalline solid has a precise melting temperature because each atom or molecule of the same type is held in place with the same forces or energy. Amorphous solids or non-crystalline solids (or, sometimes, glasses) which lack an ordered internal structure and are randomly arranged. Substances that...
Dimensionless Groups in Fluid Mechanics01:15

Dimensionless Groups in Fluid Mechanics

Dimensionless groups in fluid mechanics provide simplified ratios that help analyze fluid behavior without relying on specific units. The Reynolds number (Re), which represents the ratio of inertial to viscous forces, distinguishes between laminar and turbulent flows, making it essential in the design of pipelines and aerodynamic surfaces. The Froude number (Fr), the ratio of inertial to gravitational forces, is particularly useful in predicting wave formation and hydraulic jumps in...
First Law: Particles in Two-dimensional Equilibrium01:18

First Law: Particles in Two-dimensional Equilibrium

Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
Newton's first law tells us about the...
First Law: Particles in One-dimensional Equilibrium01:10

First Law: Particles in One-dimensional Equilibrium

Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If we...

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Related Experiment Video

Updated: May 15, 2026

Confocal Imaging of Confined Quiescent and Flowing Colloid-polymer Mixtures
10:56

Confocal Imaging of Confined Quiescent and Flowing Colloid-polymer Mixtures

Published on: May 20, 2014

Three-dimensional patchy lattice model for empty fluids.

N G Almarza1, J M Tavares, E G Noya

  • 1Instituto de Química Física Rocasolano, CSIC, Serrano 119, E-28006 Madrid, Spain.

The Journal of Chemical Physics
|January 3, 2013
PubMed
Summary
This summary is machine-generated.

This study reveals unusual reentrant liquid-vapor phase equilibria in a 2A10B lattice model, occurring at lower interaction ratios than previously expected. The findings challenge universality assumptions and suggest implications for understanding dipolar hard sphere condensation.

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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Related Experiment Videos

Last Updated: May 15, 2026

Confocal Imaging of Confined Quiescent and Flowing Colloid-polymer Mixtures
10:56

Confocal Imaging of Confined Quiescent and Flowing Colloid-polymer Mixtures

Published on: May 20, 2014

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Area of Science:

  • Statistical Mechanics
  • Condensed Matter Physics
  • Computational Chemistry

Background:

  • Understanding phase diagrams is crucial for predicting material behavior.
  • Reentrant phase transitions, where a system returns to a previous phase upon changing a parameter, are complex phenomena.
  • Lattice models provide simplified yet powerful frameworks for studying phase equilibria.

Purpose of the Study:

  • To calculate and analyze the phase diagram of a 2A10B lattice model.
  • To investigate the occurrence and characteristics of reentrant liquid-vapor phase equilibria.
  • To compare findings with existing theories and related models.

Main Methods:

  • Utilized a combination of theoretical calculations and simulation methods.
  • Focused on a face-centered cubic lattice model with specific patch interactions (2A10B).
  • Analyzed the system's behavior based on the ratio of AB and AA interaction strengths (r).

Main Results:

  • Observed reentrant liquid-vapor phase equilibria for specific interaction parameters.
  • Found that these equilibria occur at interaction ratios (r) below the previously assumed universal threshold of 1/3.
  • Predicted extreme reentrancy, including a closed-loop liquid-vapor equilibrium with a lower critical point, below r=1/3.
  • Identified an order-disorder transition at higher densities, confirming reentrancy occurs in an equilibrium region.

Conclusions:

  • The universality of the 1/3 threshold for reentrant liquid-vapor equilibria in 2AnB models is challenged.
  • The 2A10B model exhibits unique phase behavior, including unusual closed-loop equilibria.
  • Findings offer insights into the condensation of systems like dipolar hard spheres due to model analogies.