142 Advances in Polymer Science Editorial Board: A. Abe. A.-C ...
142 Advances in Polymer Science Editorial Board: A. Abe. A.-C ...
142 Advances in Polymer Science Editorial Board: A. Abe. A.-C ...
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170 K. Ito, S. Kawaguchi<br />
size was found to <strong>in</strong>crease with <strong>in</strong>creas<strong>in</strong>g the neutralization of the polyelectrolyte<br />
macromonomers.<br />
The rate of polymerization, R p , <strong>in</strong> the emulsion polymerization is generally<br />
given by the equation<br />
(30)<br />
where n<br />
is the average number of radicals per particle, N the number of latex<br />
particles per unit volume, and [M] p, the equilibrium concentration of the monomer<br />
swell<strong>in</strong>g the latex particle. Accord<strong>in</strong>g to the Smith-Ewart theory [147], <strong>in</strong><br />
which the ma<strong>in</strong> locus for particle nucleation is assumed to take place <strong>in</strong> the surfactant<br />
micelles, the number of particles is given as<br />
(31)<br />
where r' is the rate of radical generation, µ is the rate of particle volume growth,<br />
a s is the area occupied by a surfactant molecule, and C s is the total amount of<br />
surfactant <strong>in</strong> the micelles. Gardon [148, 149] thoroughly reviewed and confirmed<br />
the assumptions of Smith-Ewart theory and derived the more convenient<br />
equation for numerical calculation:<br />
(32)<br />
where r'=2N A k d f[I], C s =N A ([C s ]–[cmc]), and K=[(3/4p)(k p /N A )(d m /d p )f m ]/(1–<br />
f m ) with the monomer and polymer density, d m , d p , and the volume fraction of<br />
monomers swell<strong>in</strong>g the particles at equilibrium, f m . These equations have been<br />
well established to hold for the conventional emulsion polymerization of hydrophobic,<br />
water <strong>in</strong>soluble monomers such as styrene. Therefore, when one assumes<br />
that micellar entry dom<strong>in</strong>ates the particle nucleation <strong>in</strong> the emulsion copolymerization<br />
of styrene with a macromonomer, N may be written by the follow<strong>in</strong>g<br />
power law relationship:<br />
(33)<br />
Sauer and coworkers [138] obta<strong>in</strong>ed Nµ [I] 0.82 [Macromonomer] –0.2~+0.82 <strong>in</strong><br />
the styrene emulsion copolymerization with various types of PEO macromonomers,<br />
26, 27, 51, and 52. On the other hand, it has been found that us<strong>in</strong>g a PEO<br />
macromonomer, 26 (m=1, 4, 7), with a relatively short PEO cha<strong>in</strong> (n=16), Nµ<br />
[Macromonomer] 0.6 while us<strong>in</strong>g a macromonomer with a moderately long PEO<br />
cha<strong>in</strong> (n=45), Nµ [Macromonomer] 1.8 [140]. A mechanistic model for the emulsion<br />
copolymerization us<strong>in</strong>g amphiphilic macromonomers is under study [140]<br />
<strong>in</strong> which both micellar and homogeneous nucleations by homo- and copolymerization<br />
with macromonomer <strong>in</strong> the cont<strong>in</strong>uous phase are considered.<br />
Another <strong>in</strong>terest<strong>in</strong>g heterogeneous polymerization us<strong>in</strong>g macromonomers is<br />
a microemulsion copolymerization to produce particles 10–100 nm <strong>in</strong> diameter.<br />
Gan and coworkers [150] have prepared transparent nanostructured polymeric<br />
materials by direct polymerization of bicont<strong>in</strong>uous microemulsions consist<strong>in</strong>g