Abstract
A simple Brownian motion model is used to discuss thermal diffusion in dilute polymer solutions. The thermal diffusion coefficient is found to be independent of polymer at sufficiently large molecular weights and to be given by DT= − (DsEs) / RT2 where Ds is the self‐diffusion of the solvent and Es is the activation energy for this diffusion. This suggests that the thermal diffusion ratio α= TDT / D0 should show a marked temperature dependence, a molecular weight dependence proportional to M½, and a concentration dependence governed for the most part by that of D0. The results are shown to agree with published data in most respects and are contrasted to the results of other theoretical models. The results indicate that thermal diffusion is not a particularly promising method of fractionating various molecular weight molecules.

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