Low-fraction polymer solutions show peculiar behaviour when quenched deeply into the unstable region of the phase diagram. Whereas in a quenched off-symmetric binary liquid the minority phase forms droplets in a matrix of the majority phase, in the polymer solution it is the majority phase (i.e., the solvent) that rapidly forms droplets in a matrix of a mixed polymer-solvent phase. As the solvent is gradually squeezed out of this matrix, a polymer network or transient gel remains which eventually breaks up under its own stress. In the final stable state, the minority phase (i.e., the polymer) forms droplets against a backdrop of the majority phase, just as for the off-symmetric binary liquid. A similar evolution has been observed in the phase separation of some colloidal systems.
Dynamical asymmetry between a fast moving solvent and a slow moving solute. The bulk modulus of the solute also plays an important role. We want to simulate the various stages of this so-called “viscoelastic phase separation” process on a mesoscopic scale, using a particle-based simulation method, with the aims of improving the understanding of the process and of elucidating the parameters entering the current phenomenological model.
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