2020
DOI: 10.1021/acsmacrolett.0c00144
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Rouse 2D Diffusion of Polymer Chains in Low Density Precursor Films of Polybutadiene Melts

Abstract: We took advantage of pseudopartial wetting to promote the spreading of precursor films whose surface density smoothly decays to zero away from a sessile droplet. By following the spreading dynamics of semidilute precursor films of polybutadiene melts on silicon wafers, we measure molecular diffusion coefficients for different molar masses and temperatures. For homopolymers, chains follow a thermally activated 2D Rouse diffusion mechanism, with an activation energy revealing polymer segment interactions with th… Show more

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Cited by 3 publications
(23 citation statements)
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“…In this framework, we suggest the friction mechanism at stake for low-mass polymers consists of both monomer/monomer friction and monomer/substrate friction. This hypothesis was verified in a previous study: 29 for non-dense films with effective thickness below b, we showed monomer/substrate interactions were setting the diffusion coefficient of dilute or semi-dilute PBd or PBd-OH polymers on silica. In dense films, low-mass polymers exhibit low film thickness h 2 so that the ratio of the surface friction term to the chain/chain friction term becomes comparatively larger.…”
supporting
confidence: 90%
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“…In this framework, we suggest the friction mechanism at stake for low-mass polymers consists of both monomer/monomer friction and monomer/substrate friction. This hypothesis was verified in a previous study: 29 for non-dense films with effective thickness below b, we showed monomer/substrate interactions were setting the diffusion coefficient of dilute or semi-dilute PBd or PBd-OH polymers on silica. In dense films, low-mass polymers exhibit low film thickness h 2 so that the ratio of the surface friction term to the chain/chain friction term becomes comparatively larger.…”
supporting
confidence: 90%
“…Technical details on these computations are available in a previous paper. 29 Figure 5 presents thickness profiles with time of a secondary film of PBd-OH, and the corresponding D(h) curves. We observe that D increases with h. A temporal dependence of the diffusion coefficient is noted for h ≤ 0.7 × h 2 .…”
Section: Resultsmentioning
confidence: 99%
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“…Rouse-like motion for diffusive motion of polymer melts has been previously reported for precursor films of poly­(vinyl acetate) spreading on the air–water surface and for PDMS and polybutadiene droplets spreading on silicon wafers; however, such observation has not been made for polymers three dimensionally confined in porous media, to our best knowledge. Thus, the inverse scaling of D eff with chain size and the increase in dynamics with increasing humidity lead to the conclusion that the interfacial friction arising from strong hydrogen bonding interactions between the silica and PDMS dominates the dynamics of PDMS motion in the disordered SiO 2 nanoparticle packing. The nanoporous domain in the nanoparticle packings is an interconnected network of nanopores of varying sizes.…”
Section: Resultsmentioning
confidence: 90%