Abstract
The dynamics of concentration fluctuations in a gel near phase separation is described by a mode-coupling theory. The scaling relations, E1ξ2 and f1ξ, where ξ is the correlation length of the concentration fluctuations in the network, are obtained for the elastic constant of the network, E, and the frictional coefficient between the network and the fluid medium, f. The theory fully explains the experimental results of Tanaka, Ishiwata, and Ishimoto on a polyacrylamide gel.