Emulsion polymerization. IV. Experimental verification of the theory based on slow termination rate within latex particles

Abstract A large body of data shows that the time dependence of conversion fits the equation P = At 2 + Bt in the interval where, according to the Smith‐Ewart model, the relationship should be linear. For latexes of very small particle size the Smith‐Ewart linear relationship ( P = Bt ) is often observed, and for latexes of very large particle size the conversion was found to be proportional to t 2 . The experimental value of parameter B was in good agreement with independent theoretical predictions. From A and B the ratio between termination and propagation constants was calculated and was in the 5–200 range. Independent estimates of this ratio give the same order of magnitude. These independent estimates are from the literature and are obtained from the increase in conversion rate at catalyst post‐addition during emulsion polymerization or from emulsion polymerization initiated by intermittent irradiation or from homogeneous polymerization in the presence of inert polymers of high viscosity. The conversion–time curves describing the whole conversion process generally have sigmoid shape. The molecular weight is often found to pass through a maximum as the conversion increases. In one experiment this maximum coincided with the calculated maximum in the average number of radicals per particle Q . The variation of experimental molecular weights with conversion accurately followed the theoretical predictions. The deviation from the Smith‐Ewart model was often significant. The value of Q was not 0.5, as the Smith‐Ewart model requires it to be, but often reached values much larger, as large as 10. The particle size distribution broadened with increasing conversion and became increasingly skew. Numerous data taken from the literature are in good quantitative or qualitative agreement with the theory proposed in Part III and for these data the observed deviations from the Smith‐Ewart theory are readily explainable. The new data obtained with styrene, n ‐butyl methacrylate, and methyl methacrylate are also in quantitative agreement with the new theory. One experiment involving methyl methacrylate is analyzed in great detail. The variation of time, of Q , of molecular weight, of average particle size, and of particle size distribution with conversion are reported. The molecular weight distribution is also calculated from the conversion dependence of molecular weight.