diffusive$21261$ - ορισμός. Τι είναι το diffusive$21261$
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Τι (ποιος) είναι diffusive$21261$ - ορισμός

THERMAL MOTION OF LIQUID OR GAS PARTICLES AT TEMPERATURES ABOVE ABSOLUTE ZERO
Simple diffusion; Diffusion equilibrium; Diffusion (mathematics); Diffusion processes; Collective diffusion; Electrodiffusion; Concentration gradient; Diffusion in materials; Diffused; Diffusing; Diffusive; Diffusively; Diffusion and Life Processes
  • Example of chemical (classical, Fick's, or Fickian) diffusion of sodium chloride in water
  • Diffusion from a microscopic and macroscopic point of view. Initially, there are [[solute]] molecules on the left side of a barrier (purple line) and none on the right. The barrier is removed, and the solute diffuses to fill the whole container. <u>Top:</u> A single molecule moves around randomly. <u>Middle:</u> With more molecules, there is a clear trend where the solute fills the container more and more uniformly. <u>Bottom:</u> With an enormous number of solute molecules, all randomness is gone: The solute appears to move smoothly and systematically from high-concentration areas to low-concentration areas, following Fick's laws.
  • Schematic representation of mixing of two substances by diffusion
  • Self diffusion, exemplified with an isotopic tracer of radioactive isotope <sup>22</sup>Na

Diffusive–thermal instability         
  • Diffusive-thermal instability diagram
INSTRINSIC FLAME INSTABILITY
Diffusive-thermal instability
Diffusive–thermal instability or thermo–diffusive instability is an instrinsic flame instability that occurs both in premixed flames and in diffusion flames and arises because of the difference in the diffusion coefficient values for the fuel and heat transport, characterized by non-unity values of Lewis numbers. The instability mechanism that arises here is the same as in Turing instability explaining chemical morphogenesis, although the mechanism was first discovered in the context of combustion by Yakov Zeldovich in 1944 to explain the cellular structures appearing in lean hydrogen flames.
Diffuse optical imaging         
  • A fiber-optic array for breast cancer detection by way of diffuse optical tomography.
ALSO KNOWN AS DIFFUSE OPTICAL TOMOGRAPHY, A MEDICAL IMAGING TECHNIQUE
Diffuse optical tomography; Diffuse Optical Tomography; Diffusive Optical Imaging; Diffuse Optical Imaging; Diffuse optical topography
Diffuse optical imaging (DOI) is a method of imaging using near-infrared spectroscopy (NIRS) or fluorescence-based methods.
Diffuse panbronchiolitis         
  • Molecular structure of Erythromycin A, an antibiotic used to treat DPB
  • The genes for human HLA are located on chromosome 6.
  • High resolution computed tomography (HRCT) images of the lower chest in a 16-year-old boy initially diagnosed with DPB (''left''), and 8 weeks later (''right'') after a 6-week course of treatment with erythromycin. The bilateral bronchiectasis and prominent centri-lobular nodules with a "tree-in-bud" pattern shows noticeable improvement.
INFLAMMATORY LUNG DISEASE
Panbronchiolitis
Diffuse panbronchiolitis (DPB) is an inflammatory lung disease of unknown cause. It is a severe, progressive form of bronchiolitis, an inflammatory condition of the bronchioles (small air passages in the lungs).

Βικιπαίδεια

Molecular diffusion

Molecular diffusion, often simply called diffusion, is the thermal motion of all (liquid or gas) particles at temperatures above absolute zero. The rate of this movement is a function of temperature, viscosity of the fluid and the size (mass) of the particles. Diffusion explains the net flux of molecules from a region of higher concentration to one of lower concentration. Once the concentrations are equal the molecules continue to move, but since there is no concentration gradient the process of molecular diffusion has ceased and is instead governed by the process of self-diffusion, originating from the random motion of the molecules. The result of diffusion is a gradual mixing of material such that the distribution of molecules is uniform. Since the molecules are still in motion, but an equilibrium has been established, the result of molecular diffusion is called a "dynamic equilibrium". In a phase with uniform temperature, absent external net forces acting on the particles, the diffusion process will eventually result in complete mixing.

Consider two systems; S1 and S2 at the same temperature and capable of exchanging particles. If there is a change in the potential energy of a system; for example μ12 (μ is Chemical potential) an energy flow will occur from S1 to S2, because nature always prefers low energy and maximum entropy.

Molecular diffusion is typically described mathematically using Fick's laws of diffusion.