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Relative Importance of the Effects of Seed and Feed Stage ...

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<strong>Seed</strong> <strong>and</strong> <strong>Feed</strong> <strong>Stage</strong> Agitations <strong>of</strong> BMA <strong>and</strong> NMA 371<br />

Figure 2.<br />

Table 2.<br />

Particle size distribution in seed <strong>and</strong> feed latexes for <strong>the</strong> experiments in<br />

<strong>the</strong> particle diameter in <strong>the</strong> seed was smaller when <strong>the</strong> agitation speed was<br />

higher. The figure shows a fairly good reproducibility <strong>of</strong> <strong>the</strong> particle size<br />

distributions. The final latexes show peaks at higher or lower particle<br />

diameters, corresponding to <strong>the</strong> particle sizes in <strong>the</strong> seed latexes. The<br />

diameter in <strong>the</strong> final latex is not affected by <strong>the</strong> feed stage agitation.<br />

The decrease in <strong>the</strong> particle diameter with an increase in <strong>the</strong> agitation<br />

is a recurring feature for particle nucleation in systems with surfactant<br />

concentrations near <strong>the</strong> critical micelle concentration. Arai et al. (1981)<br />

have observed an increase in <strong>the</strong> number <strong>of</strong> particles with <strong>the</strong> increase in<br />

<strong>the</strong> agitation speed during surfactant free emulsion polymerizations <strong>of</strong><br />

methyl methacrylate using KPS initiator at 65°C. Varela de la Rosa (1991)<br />

has reported <strong>the</strong> heat evolution rates during emulsion polymerizations <strong>of</strong><br />

styrene using KPS initiator at 70°C at an SDS concentration <strong>of</strong> 10 mmol<br />

dm 3 for agitator speeds <strong>of</strong> 300 rpm <strong>and</strong> 500 rpm. The particle diameter<br />

was smaller <strong>and</strong> <strong>the</strong> reaction rate higher, when <strong>the</strong> agitator speed was 500<br />

rpm. In <strong>the</strong> absence <strong>of</strong> any oxygen impurity in <strong>the</strong> reactor, this effect can<br />

be explained by <strong>the</strong> interfacial nucleation mechanism recently proposed by<br />

Ni et al. (2001). According to this mechanism, under <strong>the</strong> influence <strong>of</strong><br />

shear, minidroplets are formed at <strong>the</strong> interface <strong>of</strong> <strong>the</strong> monomer droplets<br />

<strong>and</strong> water. These minidroplets result in <strong>the</strong> nucleation <strong>of</strong> <strong>the</strong> polymer<br />

particles. The greater <strong>the</strong> agitation, <strong>the</strong> higher <strong>the</strong> number <strong>of</strong> <strong>the</strong>se minidroplets,<br />

<strong>and</strong> <strong>the</strong> resulting polymer particles. Trace amounts (ppm levels) <strong>of</strong><br />

oxygen impurity in <strong>the</strong> reactor headspace <strong>and</strong> <strong>the</strong> agitation dependent mass

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