Abstract
The surface fluctuation dynamics of melt films of densely branched comb polystyrene of thickness greater than 55 nm and at temperatures 23–58 °C above the bulk Tg can be rationalized using the hydrodynamic continuum theory (HCT) known to describe melts of unentangled linear and cyclic chains. Film viscosities (ηXPCS) inferred from fits of the HCT to X-ray photon correlation spectroscopy (XPCS) data are the same as those measured in bulk rheometry (ηbulk) for three combs. For the comb most like a star polymer and the comb closest to showing bulk entanglement behavior, ηXPCS > ηbulk. These discrepancies are much smaller than those seen for less densely branched polystyrenes. We conjecture that the smaller magnitude of ηXPCS – ηbulk for the densely grafted combs is due to a lack of interpenetration of the side chains when branching is most dense. Both Tg,bulk and the specific chain architecture play key roles in determining the surface fluctuations.
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