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The separation of the components of a liquid mixture induced by temperature gradients is known as thermal diffusion or the Ludwig (1856)–Soret (1879) effect. Under typical experimental conditions avoiding convection, thermally driven diffusion flows are often orders of magnitude smaller than diffusion flows caused by concentration gradients. Nevertheless, in the steady state the thermally driven diffusion flow and the diffusion flow are equal. The experimental investigation of the Soret effect is very difficult and sensitive methods are required for a reliable determination of the Soret coefficient.