Summary Poly(styrene)-block-poly(ethyleneoxide), abbreviated as (PS-b-PEO) were used as emulsifiers in emulsion polymerization of styrene and methyl methacrylate. The block copolymers had a poly(styrene) block with Mn=1000 g/mol and a poly(ethyleneoxide) block with Mn=1000, 3000 or 5000 g/mol, respectively. Stable dispersions were obtained when the PEO block molecular weight was higher than 1000 g/mol. Also the amphiphilic properties of the copolymers depended on the PEO chain length. Block copolymer micelles with hydrodynamic radii between 11 and 17nm were observed. Emulsion polymerization was performed at different block copolymer concentration at 60 and 80°C. Particle size varied between 50 and 300nm and decreased with increasing copolymer concentration. The particle size was larger at higher temperature, but the size distribution was narrower. Polymerization of methyl methacrylate gave smaller particles when compared to styrene. The dispersions were very stable towards high electrolyte concentration, but flocculation occurred at elevated temperatures. Both observations indicate that the dispersions are sterically stabilized. 相似文献
Summary Organosolv lignin was used as organic filler for polypropylene (PP) and poly(ethene-co-vinylacetate) (EVA) containing 13wt-% vinylacetate. As a function of the lignin content, which was varied between 0 and 30wt-%, mechanical properties such as Young's modulus, yield stress, fracture stress, and elongation at break of the thermoplastic lignin-based compounds were measured. Both lignin-filled thermoplastics exhibit pronounced matrix reinforcement with increasing lignin content. Due to better interfacial adhesion between lignin and EVA, 30wt-% lignin addition to EVA doubles Young's modulus without sacrificing high elongation at break. 相似文献
The use of bis(methylcyclopentadienyl)magnesium (MCp2Mg) as ap-dopant source for MOCVD-grown InP has been investigated. The Mg incorporation was nonlinear. The relationship between the
H2 flow through the MCp2Mg bubbler and the Mg concentra-tion in the epilayers suggested that when [Mg] <20 ppb in the reactor it was mostly depleted
from the gas mixture, probably by means of reaction with O2 or H2O, but at higher concentrations a large fraction of the Mg diffusing to the epilayers was incor-porated. For concentrations
>1019 cms-3 the layer morphology deteriorated and stacking faults were observed by TEM, at a density greater than 109 cms−2. Significant diffusion of Mg into the substrates during the growth was observed, with diffusion depths up to 0.1 μm at a
concentration of 1019 cms−3 in S-doped, and up to 32 μm at 1017 cms-3 in Fe-doped substrates. These concentrations correspond to the S and Fe doping level in those substrates, and the results
are explained in terms of the formation of a complex between the S or Fe dopants and the diffusing Mg, which immobilizes the
latter species. At [Mg] >1018 cms−3, the net hole concentration, measured by means of electrochemical C-V pro-filing, decreases with increasing [Mg], indicating
significant self compensation. Com-pensation at high [Mg] was also suggested by the effect of excitation power density on
the peak shift of the donor to acceptor transition observed during photoluminescence measurements at 7 K. 相似文献
A boost biquad transfer function with two symmetrical zeros on the real axis is derived; it provides a technique for amplitude equalization with a second-order continuous-timegm-C section using current injection. The synthesis procedure yields a differential boost biquad consisting of three double-input OTAs and a single-input high-gmboost OTA. SPICE simulations show that for boost gain up to 20 dB the phase of the biquad is essentially unaffected. The presented technique is found suitable for amplitude equalization of disk-drive read channels operating in the range of 100 MHz. 相似文献
A one‐range and a two‐range model for the laminar velocity distribution in the entrance region of tubes and ducts are presented. These allow the calculation of the residence time distribution under the impact of the flow development in the hydrodynamic entrance region. For the dispersion‐free case, an analytical solution is given. A cell model with place‐changing probability (ZEMP) is applied for the consideration of dispersion. This approach allows the fast quantification of the influence of different parameters on the residence time distribution for relatively short pipes and ducts. The numerical results are compared with earlier presented results of semi‐empirical models. 相似文献
Graphene nanocomposites are prepared by chemical reduction of graphite oxide (GO) dispersion with vitamin C in the presence of SAN latex followed by melt compounding. In this process, GO is well dispersed in an aqueous SAN emulsion before reduction. During reduction the SAN latex is adsorbed on the graphene sheets of the chemically reduced GO (CRGO). After melt compounding of such hybrid particles with SAN, the nanocomposites show uniform dispersion of CRGO in SAN resulting in improved stiffness with respect to SAN/graphite. The reduction of GO in the presence of polymer latex represents a versatile route to graphene masterbatches and does not require either drying of GO or thermal GO expansion at high temperatures.