Proton lineshape and proton spin-lattice relaxation, T-1 rho, measurem
ents were made on blends of bisphenol chloral polycarbonate and perdeu
tero poly(methyl methacrylate) (PMMA). The solution-cast blends are op
tically clear and display a single thermal glass transition temperatur
e, T-g, as reported. The proton lineshape and proton relaxation data a
re used to follow the dynamics of the polycarbonate in the blend. The
glass transition process is monitored by lineshape collapse as a funct
ion of temperature and the sub-glass transition process associated wit
h pi flips of the phenylene group is monitored by the proton T-1 rho v
alues as a function of temperature. The glass transition as viewed fro
m the polycarbonate remains similar in character to the behaviour obse
rved in pure polycarbonate. Below T-g, the lineshape consists of a bro
adened Fake doublet and above T-g a narrow Lorentzian grows in on top
of the Fake pattern. The bimodal behaviour and the growth of the narro
w line with temperature can be described by the Vogel-Tamman-Fulcher e
quation with T-0 values which decrease with PMMA concentration. The pr
oton T-1rho data show antiplasticization in the form of suppression of
the pi flip process as PMMA is added. In addition, a new minimum asso
ciated with the motion of the polycarbonate is observed at the tempera
ture and time scale of the ester group rotation of the PMMA. This appa
rent coupling of the sub-T-g relaxation processes is related to the be
haviour of polycarbonate upon addition of low-molecular-weight ester d
iluents. The level of antiplasticization and the amount of coupling is
underestimated by a lattice model and an assumption of random mixing.
On the very local scale of the pi flip motion and at the higher conce
ntrations of PMMA, there are apparently fewer PMMA-polycarbonate conta
cts than a random mixing assumption indicates.