posted on 2018-12-04, 18:41authored byRonald
M. Lewis, Haley K. Beech, Grayson L. Jackson, Michael J. Maher, Kyungtae Kim, Suresh Narayanan, Timothy P. Lodge, Mahesh K. Mahanthappa, Frank S. Bates
We report the dynamic behavior of
a sphere-forming poly(styrene)-block-poly(1,4-butadiene)
(PS–PB) diblock copolymer
comprising 20 vol % PB below the order–disorder transition
temperature (TODT = 153 °C) using
dynamic mechanical spectroscopy (DMS) and X-ray photon correlation
spectroscopy (XPCS). A time–temperature transformation diagram
was constructed by monitoring the elasticity of the sample as a function
of time following rapid quenches of the disordered melt to various
temperatures T < TODT. Isothermal frequency spectra acquired prior to nucleation of the
ordered BCC phase were time–temperature superposed, and the
shift factors were fit using the Williams–Landel–Ferry
(WLF) equation. For comparison, XPCS measurements were used to extract
relaxation times from the supercooled liquid as a function of the
quench temperature. Alignment of the temperature dependence of the
XPCS-based relaxation times with that of the WLF shift factors in
the range T = 125–140 °C indicates that
both techniques probe the fluctuating mesomorphic micelle dynamics
mediated by the relaxation modes of individual chains, including interparticle
chain exchange. For deeper quench temperatures, TODT – T ≥ 28 °C, departure
of the XPCS time constant from WLF behavior is consistent with a jamming
transition, analogous to that encountered in concentrated colloidal
systems. We postulate that the dominant relaxation mode in the supercooled
disordered liquid transitions from ergodic dynamics governed by chain
exchange to a nonergodic regime dominated by local rearrangement of
micellar particles at T ≈ Terg, where Terg denotes the
ergodicity temperature.