Angewandte
Chemie
as the instantaneous monomer concentration decreased
(Figure 3b). These results indicate that the tacticity is
governed by the remaining monomer concentration.
conformation of poly(TrMA).[15] The linear plot also gave the
ceiling temperature value of TrMA as 1048C at [M]0 = 1.0m.
This is also reasonable because almost no polymers were
obtained at 1008C for [M]0 = 1.0m.
We further utilized the unique isotactic-rich stereogra-
dient RAFT polymerization for a block copolymerization to
synthesize another novel stereocontrolled polymer. Thus we
first polymerized MMA with CDB to prepare the syndiotac-
tic-rich living poly(MMA) with RAFT moieties at the chain
ends and then employed it as a macroinitiator for the RAFT
polymerization of TrMA (Figure 5). After the copolymeriza-
The effects of the temperature were also examined on the
polymerizations. Upon raising the temperature, the initial
polymerization rate increased while the final monomer
conversions became lower. The mminst value increased with
temperature (see Figure S4 in the Supporting Information).
These results suggest that lowering the monomer concen-
tration or increasing the polymerization temperature makes
the formation of the more thermodynamically stable isotactic
propagating chain ends more favorable by the reversible
polymerization–depolymerization equilibrium.
The polymerization–depolymerization equilibrium was
further examined by increasing the temperature during the
polymerization. We first conducted the RAFT polymerization
at 608C and increased the temperature to 808C when the
conversion reached 70%. Upon increasing the temperature,
the monomer conversion decreased and remained constant at
around 60% (see Figure S5 in the Supporting Information).
The molecular weights also decreased and became constant
while the molecular weight distributions became broader.
This result also supports the presence of the polymerization–
depolymerization equilibrium by the reversible formation of
the growing radical species.
We then measured the final accessible monomer con-
versions by varying the temperatures (40–1008C) and the
initial monomer concentrations (0.25–1.0m) to obtain the
equilibrium monomer concentration ([M]eq) at each temper-
ature (see Table S1 in the Supporting Information). We
plotted the logarithmic monomer concentrations versus the
reciprocal of the temperatures (Figure 4). The plot showed a
good linear relationship, which indicated the propagation–
depropagation equilibrium for this a-substituted bulky mo-
nomer. The enthalpy (DHp) and entropy (DSp) values for the
polymerizations of TrMAwere calculated from this linear plot
(ln[M]eq = DHp/RTÀDSp/R), which yielded values of DHp =
À60.4 kJmolÀ1 and DSp = À160.5 JmolÀ1 KÀ1.[14] The enthalpy
value is almost the same as those of other methacrylate
monomers (DHp(MMA) = À56 kJmolÀ1, DHp(ethyl metha-
crylate) = À60 kJmolÀ1) while the entropy value is higher
(DSp(MMA) = À118 JmolÀ1 KÀ1, DSp(ethyl methacrylate) =
À124 JmolÀ1 KÀ1), probably because of the rigid main-chain
Figure 5. Stereoblock poly(MMA) obtained from the RAFT block
copolymerization of MMA and TrMA in toluene at 608C. For poly-
(MMA) macroinitiator: [MMA]0 =7.0m, [AIBN]0 =5.0 mm,
[CDB]0 =35 mm; for poly(MMA-b-TrMA): [TrMA]0 =1.0m,
[AIBN]0 =6.0 mm, [PMMA-CDB]0 =12 mm.
tion, we converted the trityl substituent into a methyl group
and obtained the homopoly(MMA) with narrow MWDs. The
cumulative and instantaneous mm contents versus the
normalized chain length are also shown in Figure 5. The
isotacticity was abruptly changed at the blocking point, after
which it gradually increased along the chain. The differential
spectrum of these polymers also indicates the formation of the
isotactic-rich segments in the second polymerization (cumu-
lative mm/mr/rr= 61:26:13; see Figure S6 in the Supporting
Information). These show the formation of the stereoblock
PMMA[16] with syndiotactic and isotactic-stereogradient seg-
ments.
In conclusion, we have demonstrated the formation of
stereogradient polymers by RAFT polymerization of a bulky
methacrylate monomer, in which the isospecificity gradually
increased with a decrease in the monomer concentrations.
This is caused by the propagation–depropagation equilibrium,
which can convert a less stable growing polymer terminal with
the r conformation into the more stable m form especially at a
lower monomer concentration. Further studies are now
directed to the controlled/living radical copolymerization of
bulky methacrylates with other monomers for the synthesis of
novel stereocontrolled polymers.[17]
Received: October 22, 2008
Revised: January 10, 2009
Figure 4. Dependence of equilibrium monomer concentration ([M]eq)
on temperature in the RAFT polymerizations of TrMA in toluene.
Published online: February 4, 2009
Angew. Chem. Int. Ed. 2009, 48, 1991 –1994
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
1993