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Atom transfer radical polymerizations of styrene and butadiene as ...

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46 J. Hua et al.<br />

8 6 4 2 0 ppm<br />

Fig. 10 1 H NMR spectrum <strong>of</strong> poly(<strong>butadiene</strong>-<strong>styrene</strong>)<br />

Fig. 8 FTIR spectra <strong>of</strong> PSt (a), St/Bd copolymer (Bd/St=1/4) (b), St/<br />

Bd copolymer (Bd/St=1/3) (c), St/Bd copolymer (Bd/St=1/2) (d), St/<br />

Bd copolymer (Bd/St=1/1) (e), PBd (f)<br />

absorption peaks <strong>of</strong> the <strong>styrene</strong> units became stronger <strong>and</strong><br />

those <strong>of</strong> the <strong>butadiene</strong> structure unit became weaker <strong>as</strong> the<br />

molar ratio <strong>of</strong> <strong>styrene</strong> in the copolymer incre<strong>as</strong>ed. At the<br />

same time, the characteristic peaks <strong>of</strong> the 1,2-<strong>butadiene</strong><br />

structural units incre<strong>as</strong>ed while those <strong>of</strong> the cis-1,4- <strong>and</strong><br />

trans-1,4-<strong>butadiene</strong> structural units decre<strong>as</strong>ed.<br />

Figure 9 shows 13 C NMR spectra <strong>of</strong> the <strong>styrene</strong> <strong>and</strong><br />

<strong>butadiene</strong> copolymer. The peaks between 40.9 <strong>and</strong><br />

45.5 ppm (40.9, 42.6, 42.8, 43.0, 43.2, 45.5 ppm) in<br />

Fig. 9 correspond to the carbons <strong>of</strong> the S*V, S*c, V*S, <strong>and</strong><br />

S*t chain structures (here, S, V, c <strong>and</strong> t denote <strong>styrene</strong> <strong>and</strong><br />

1,2-, cis-1,4- <strong>and</strong> trans-1,4-<strong>butadiene</strong> structural units,<br />

respectively); the peak at 145.15 ppm corresponds to the<br />

carbon <strong>of</strong> the S unit between c <strong>and</strong> t [25].<br />

There is no absorption peak over 6.800 in the 1 HNMR<br />

spectrum <strong>of</strong> the copolymer (Fig. 10), which shows that<br />

there is no block <strong>styrene</strong> chain segmental structure in this<br />

copolymer [26]. This verifies that the copolymer is a<br />

r<strong>and</strong>om copolymer.<br />

Figure 11 shows the single gl<strong>as</strong>s transition temperature<br />

in the DSC curve <strong>of</strong> the <strong>styrene</strong> <strong>and</strong> <strong>butadiene</strong> copolymer.<br />

The T g <strong>of</strong> the copolymer dropped from 16.2°C to −16.6°C<br />

<strong>as</strong> the molar ratio <strong>of</strong> Bd/St incre<strong>as</strong>ed from 1/3 to 1/2. These<br />

results further prove that the copolymer is a r<strong>and</strong>om<br />

copolymer.<br />

Analysis <strong>of</strong> the polymerization mechanism<br />

Figure 12 shows UV-vis spectra <strong>of</strong> toluene solutions <strong>of</strong><br />

MoCl 3 (OC 8 H 17 ) 2 , MoCl 3 (OC 8 H 17 ) 2 / P(Ph) 3 ,<br />

MoCl 3 (OC 8 H 17 ) 2 / P(Ph) 3 / C 6 H 5·CH 2 Cl, <strong>and</strong> St /<br />

MoCl 3 (OC 8 H 17 ) 2 / P(Ph) 3 / C 6 H 5·CH 2 Cl. In the UV-vis<br />

spectrum <strong>of</strong> MoCl 3 (OC 8 H 17 ) 2 , characteristic absorption<br />

b<strong>and</strong>s were observed for Mo 5+ near 430 nm <strong>and</strong> 730 nm<br />

<strong>and</strong> for Mo 4+ near 510 nm [27]. Mo 4+ w<strong>as</strong> probably present<br />

because the reduction <strong>of</strong> MoCl 3 (OC 8 H 17 ) 2 took place to a<br />

small degree when creating the 1-octanol-substituted MoCl 5<br />

solution. The absorption peak at 730 nm w<strong>as</strong> caused by a<br />

d–d transition in the Mo atom in MoCl 3 (OC 8 H 17 ) 2 .After<br />

Fig. 9 13 C NMR spectra <strong>of</strong> the <strong>styrene</strong> <strong>and</strong> <strong>butadiene</strong> copolymer. The<br />

molar monomer ratio <strong>of</strong> St/Bd w<strong>as</strong> 3/1<br />

Fig. 11 DSC curves for <strong>styrene</strong> <strong>and</strong> <strong>butadiene</strong> copolymers with<br />

different monomer ratios

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