Diffusion is the spontaneous spreading of something such as particles, heat, or momentum. The phenomenon is readily observed when a drop of colored water is added to clear water, or when smoke from a chimney dissipates into the air. In these cases, diffusion is the result of turbulent fluid motion rather than chemical reactions or the application of external force. In cell biology, diffusion is described as a form of "passive transport", by which substances cross membranes.
2.2 Diffusion in chemical engineering
Diffusion is one kind of transport phenomenon: compare it, for example, to radiation. All diffusion can be modelled quantitatively using the diffusion equation, the solutions of which go by different names depending on the physical situation. Steady state bi-molecular diffusion is governed by Fick's first law. Steady-state thermal diffusion is governed by Fourier's Law. Diffusion of electrons in an electrical field is essentially Ohm's law. In each, a flux (of atoms or energy or electrons) is equal to a physical property (diffusivity or thermal conductivity or electrical conductivity) multiplied by a gradient (concentration gradient or thermal gradient or electric field). The generic diffusion equation is time dependent (i.e. also applies to non-steady-state situations).
In each case, there is only a noticeable diffusion if there is a gradient: for example in thermal diffusion, if the temperature is constant, heat will move as quickly in one direction as in the other, producing no change.
In mammalian lungs, a process of diffusion takes place in the aveoli: due to differences in partial pressures across the alveolar-capillary membrane, oxygen diffuses into the blood and carbon dioxide diffuses out.
The passive transport of ions or molecules by a specific carrier protein in a membrane. As in simple diffusion, net transport is down a concentration gradient, and no additional energy has to be supplied. Compare with diffusion and active transport.
Net flux is used to measure diffusion.
Nonpolar molecules diffuse faster through the lipid portion of the membranes.
Diffusion of ions depends on the concentration gradient, and the membrane potential. The net flux of ions can be altered by opening or closing ion channels.
Diffusion is the movement of matter due to the movement of the individual molecules (or atoms). Diffusion occurs in solids, in liquids, in gases and in supercritical fluids. Diffusion is caused by the thermal movement of individual molecules. Some examples of diffusion are:
This is the process whereby the random thermally activated hopping of atoms in a solid results in the net transport of atoms. For example, helium atoms inside a balloon can diffuse through the wall of the balloon and escape, resulting in the balloon slowly deflating. Other air molecules (e.g. oxygen, nitrogen) have lower mobilities and thus diffuse more slowly through the balloon wall. There is a concentration gradient in the balloon wall because the balloon was filled up with helium, and thus there is plenty of helium on the inside, but there is relatively little helium on the outside, because helium is not a major component of air. The rate of transport is governed by the diffusivity and the concentration gradient.
See also Kirkendall effect.
Brownian motion occurs when discrete particles diffuse in a liquid medium. Since the energy is thermal, the mass of the particles must be very small in order that the motion be observable (). The direction of the motion is random and thus constantly changing. In principle, Brownian motion also occurs in gases, but usually the motion of particulates in gases, e.g. smoke, is dominated by turbulence.
Electric current flows by diffusion in most conductors. Charge carriers (usually electrons) move randomly in the absence of an electric field. When an electric field is applied, carriers drift preferentially in the field, causing a net current. The rate of transport is governed by the electrical conductivity of the conductor and the electric field.
In the case of laminar flow of a liquid flowing past a solid surface, momentum diffuses across the boundary layer near the surface. The gradient in this case is between the liquid in contact with the surface (which isn't moving at all and has zero momentum) and the liquid far away from the wall, which has momentum proportional to the speed at which it is flowing. The rate of transport is governed by the viscosity of the fluid and the momentum gradient.
When photons travel through a material with a high optical depth and a very short mean free path, their behavior is dominated by scattering and the path of any given photon's path is effectively a random walk. The behavior of a large ensemble of photons in this situation can be described with a diffusion equation.
In general, diffusion results in transport down the gradient -- i.e. things move from regions of high concentration to low concentration. However, this is not always the case: during a phase separation, material can diffuse towards regions of higher concentration. This is referred to as reverse diffusion.
When heat travels through a material with a thermal gradient (for example, heat traveling through the wall of a coffee mug), the rate of transport is governed by the thermal conductivity and the temperature gradient.
|Active transport||Barotropic vorticity equation|
|Bipolar junction transistor||Brownian motion||Cell membrane|
|Circulatory system||Diffusion equation||Effusion|
|Electrochemical potential||Emulsion polymerization||Fick's law of diffusion|
|Fokker-Planck equation||Gel permeation chromatography||Hydrothermal circulation|
|Isotope separation||Kirkendall effect||Laminar flow|
|Liposomes||List of biochemistry topics||List of biology topics|
|List of physics topics||Mass transfer||Materials science|
|Mechanical ventilation||NaKATPase||Nervous system|
|Neurotransmitter||Nitric oxide||Nobel Prize in Physiology or Medicine|
|Respiration||Reverse osmosis||Second messenger|
|Semipermeable membrane||SI derived unit||Sintering|