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Related Concept Videos

Diffusion01:12

Diffusion

Diffusion is the passive movement of substances down their concentration gradients—requiring no expenditure of cellular energy. Substances, such as molecules or ions, diffuse from an area of high concentration to an area of low concentration in the cytosol or across membranes. Eventually, the concentration will even out, with the substance moving randomly but causing no net change in concentration. Such a state is called dynamic equilibrium, which is essential for maintaining overall...
Diffusion01:21

Diffusion

Diffusion is a type of passive transport. In passive transport, a substance tends to move from an area of high concentration to an area of low concentration until the concentration is equal across the space. For example, take the diffusion of substances through the air. When someone opens a perfume bottle in a room filled with people, the perfume is at its highest concentration in the bottle and is at its lowest at the edges of the room. The perfume vapor will diffuse, or spread away, from the...
Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion03:48

Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion

Although gaseous molecules travel at tremendous speeds (hundreds of meters per second), they collide with other gaseous molecules and travel in many different directions before reaching the desired target. At room temperature, a gaseous molecule will experience billions of collisions per second. The mean free path is the average distance a molecule travels between collisions. The mean free path increases with decreasing pressure; in general, the mean free path for a gaseous molecule will be...
Protein Diffusion in the Membrane01:24

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Proteins show rotational as well as lateral diffusion across the membrane. The lateral diffusion of proteins was confirmed through the cell fusion experiment where mouse and human cells were fused, resulting in hybrid cells. When the human and mouse cells fused, the specific membrane proteins on human and mouse cells were marked with the red and green-fluorescent markers, respectively. Initially, the red and green fluorescence was located on the respective hemisphere of the cell. As time...
Van der Waals Interactions01:24

Van der Waals Interactions

Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model01:09

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Various dissolution theories provide insight into the factors that influence the dissolution rate. Danckwerts' Model suggests that turbulence, rather than a stagnant layer, characterizes the dissolution medium at the solid-liquid interface. In this model, the agitated solvent contains macroscopic packets that move to the interface via eddy currents, facilitating the absorption and delivery of the drug to the bulk solution. The regular replenishment of solvent packets maintains the concentration...

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The Diffusion of Passive Tracers in Laminar Shear Flow
08:01

The Diffusion of Passive Tracers in Laminar Shear Flow

Published on: May 1, 2018

Pair diffusion, hydrodynamic interactions, and available volume in dense fluids.

Jeetain Mittal1, Gerhard Hummer

  • 1Department of Chemical Engineering, Lehigh University, Bethlehem, Pennsylvania 18015, USA. jeetain@lehigh.edu

The Journal of Chemical Physics
|July 27, 2012
PubMed
Summary
This summary is machine-generated.

We calculated the pair diffusion coefficient for hard spheres in a dense fluid. Results agree with hydrodynamic theories at larger distances, but show deviations at short distances due to fluid structure and memory effects.

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Area of Science:

  • Fluid dynamics
  • Colloid science
  • Statistical mechanics

Background:

  • Hydrodynamic interactions are crucial for understanding polymer and colloid dynamics.
  • The pair diffusion coefficient D(r) quantifies these interactions between particles.
  • Accurate calculation of D(r) is essential for theoretical models.

Purpose of the Study:

  • To calculate the pair diffusion coefficient D(r) for hard spheres in a dense fluid.
  • To compare simulation results with macroscopic hydrodynamic theories and approximations.
  • To investigate the influence of fluid structure and memory effects on D(r).

Main Methods:

  • Molecular dynamics simulations were used to obtain particle pair propagators (Green's functions).
  • The pair diffusion coefficient D(r) was determined from these simulation data.
  • Comparison with exact macroscopic hydrodynamic theory and the Oseen approximation was performed.

Main Results:

  • D(r) agrees well with hydrodynamic theories for distances greater than ~3 molecular diameters.
  • The asymptotic 1/r dependence of D(r) appears only after long simulation times, indicating short-time memory effects.
  • Deviations from hydrodynamic models at short distances correlate with local available volume and many-body fluid structure.

Conclusions:

  • Macroscopic hydrodynamic theories accurately describe pair diffusion at larger scales.
  • Short-time dynamics are influenced by memory effects and local fluid structure, deviating from simple hydrodynamic predictions.
  • The methodology is applicable to single-particle diffusion in confined systems.