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Thermophoresis : ウィキペディア英語版
Thermophoresis
''Thermophoresis'' (also thermomigration, thermodiffusion, the Soret effect, or the Ludwig-Soret effect) is a phenomenon observed in mixtures of mobile particles where the different particle types exhibit different responses to the force of a temperature gradient. The term ''thermophoresis'' most often applies to aerosol mixtures, but may also commonly refer to the phenomenon in all phases of matter. The term ''Soret effect'' normally applies to liquid mixtures, which behave according to different, less well-understood mechanisms than gaseous mixtures. Thermophoresis may not apply to thermomigration in solids, especially multi-phase alloys.
==Thermophoretic force==
The phenomenon is observed at the scale of one millimeter or less. An example that may be observed by the naked eye with good lighting is when the hot rod of an electric heater is surrounded by tobacco smoke: the smoke goes away from the immediate vicinity of the hot rod. As the small particles of air nearest the hot rod are heated, they create a fast flow away from the rod, down the temperature gradient. They have acquired higher kinetic energy with their higher temperature. When they collide with the large, slower-moving particles of the tobacco smoke they push the latter away from the rod. The force that has pushed the smoke particles away from the rod is an example of a thermophoretic force. For illustration see (aerosols.wustl.edu ).
Thermodiffusion is labeled "positive" when particles move from a hot to cold region and "negative" when the reverse is true. Typically the heavier/larger species in a mixture exhibits positive thermophoretic behavior while the lighter/smaller species exhibit negative behavior. In addition to the sizes of the various types of particles and the steepness of the temperature gradient, the heat conductivity and heat absorption of the particles play a role. Recently, Braun and coworkers have suggested that the charge and entropy of the hydration shell of molecules play a major role for the thermophoresis of biomolecules in aqueous solutions.
The quantitative description is given by:
:\frac=\nabla\cdot( D\,\nabla \chi+ D_\, \chi(1-\chi)\,\nabla T)
D diffusion coefficient and D_T the thermodiffusion coefficient. The quotient of both coefficients
:S_T=\frac
is called Soret coefficient.
The thermophoresis factor has been calculated from molecular interaction potentials derived from known molecular models 〔J. Chem. Phys., 50, 4886, (1960)〕

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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