2003
DOI: 10.1021/ma020856j
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Structural Studies of Extension-Induced Mesophase Formation in Poly(diethylsiloxane) Elastomers:  In Situ Synchrotron WAXS and SAXS

Abstract: Amorphous poly(diethylsiloxane) (PDES) elastomers undergo a transition to an aligned mesomorphic state when subjected to uniaxial tension. The structural changes associated with this transition and the kinetics of its formation have been investigated by in-situ synchrotron wide-angle and small-angle X-ray scattering. In the mesomorphic state, the PDES elastomers are biphasic, consisting of aligned mesophase domains and amorphous material. Because of the well-defined structure of the networks used, we were able… Show more

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Cited by 34 publications
(27 citation statements)
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“…However, cold drawing is rarely observed, if ever, in noncrystallizable elastomers above their respective glass transition temperatures. Previous reports of necking in elastomers have been limited to smectic polydomain MCLCE and mesomorphic poly(diethylsiloxane) (PDES) elastomers 30–35. Like semicrystalline polymers, smectic MCLCE are also thought to contain high concentrations of chain‐folded conformers (hairpins),5, 12 suggesting that the necking transition might involve loss of chain folding, a view supported by our recent X‐ray diffraction studies 12…”
Section: Introductionmentioning
confidence: 68%
“…However, cold drawing is rarely observed, if ever, in noncrystallizable elastomers above their respective glass transition temperatures. Previous reports of necking in elastomers have been limited to smectic polydomain MCLCE and mesomorphic poly(diethylsiloxane) (PDES) elastomers 30–35. Like semicrystalline polymers, smectic MCLCE are also thought to contain high concentrations of chain‐folded conformers (hairpins),5, 12 suggesting that the necking transition might involve loss of chain folding, a view supported by our recent X‐ray diffraction studies 12…”
Section: Introductionmentioning
confidence: 68%
“…The correlation length of the low‐angle (high intensity) peak was calculated using the Scherrer equation46 ( $L^\prime = k\Lambda \Big/ \beta^{\prime} \cos {\Theta}_{\max}$ , where k is a material parameter, commonly ∼1 for polymers, Λ the wavelength of the X‐ray, β′ the full width at half‐maximum of the WAXS peak, and θ max is the scattering angle of the peak under investigation). Under the assumption of a perfect two‐phase system, the correlation length L ′ can be identified to the domain size.…”
Section: In Situ X‐ray Results: Saxs and Waxs Measurements Combinedmentioning
confidence: 99%
“…For a system with a relatively low viscosity (1 wt.-% I.30E in Epon 862, g 25C = 15 Poise) alignment at room temperature occurred in less than 5 s for 2 V lm ±1 , whereas randomization upon removal of the field required 30 s. For a system with higher viscosity (10 wt.-% layered silicate in Epon 862/Cure W mixture, g 25C = 100 Poise) alignment at room temperature required longer than 5 min, and corresponding randomization took more than 10 h. The threshold voltage for alignment was slightly less than 1 V lm ±1 with no dependence on the examined range of frequencies (0.1± 50 MHz). In general, the orientation parameter (Hermans orientation function, see Koerner et al [13] ) of the fully aligned systems was consistently between 0.6±0.7. These values are comparable to aligned nematic liquid crystals.…”
mentioning
confidence: 88%