Summary: In copolymerization systems with implicit penultimate effect, there are two radical reactivity ratios, sa and sb, which influence the reaction kinetics in addition to the monomer reactivity ratios, ra and rb, which govern the copolymer composition. Here, an error in variables method has been developed to determine sa and sb. It is based on continuous on‐line monitoring of the polymerization process, where monomer and polymer concentrations are measured through the monitoring of two independent properties of the system. The ratios and the corresponding χ2 values were found by taking into account errors emanating from measurements and from calibration of the instruments. It is shown that the kinetic data allows both ratios to be found if both monomer reactivity ratios are less than one. If the system is near ideality (rarb ≅ 1) or if both reactivities are greater than one, only an average radical reactivity ratio, , can be reliably determined.
The 2σ confidence contours for the 3 individual experiments. The reactivity ratios are ra = 0.5, rb = 0.2, sa = 0.3, sb = 0.4. For clarity the contours are plotted as functions of 1/sa and 1/sb. 相似文献
4‐Vinylbenzoyl azide was synthesized from p‐vinylbenzoic acid and polymerized by free radical polymerization. The obtained polymer contained acyl azide groups which were thermally transformed to the corresponding isocyanato groups. Reactions on these polymers with ethanol, hydroxyethyl methacrylate and 1‐pyrenebutanol proceeded quantitatively. Time‐resolved FT‐IR studies of the reactions with ethanol were carried out by varying the concentration and temperature. The effect of the solvent polarity on the Curtius rearrangement was investigated.
Summary: We describe the development of different drop‐on‐demand systems particularly for applications for the liquid handling of biopolymers. Different designs of drop‐on‐demand systems developed by the authors are described. Experiments with these systems show the applicability for pipetting different liquids with different properties. Commercially available systems are also tested. A comparison of the different approaches leads to a discussion of the best fields of application of the different approaches or, alternatively, to the potential further development of the drop‐on‐demand technologies.
The adsorption of O on Ru(0001) is studied by means of Monte Carlo
simulation of lattice gas model on a triangular lattice. A recent STM
study shows that at low coverage the p(2×2) structure grows via island formation but the p(2×1) structure is abruptly formed at a critical coverage. Moreover, it also shows that there is a coexistence of the p(2×2) and p(2×1) structures. The above results seem not to coincide with the former studies of the system by both the LEED and Monte Carlo simulation. We therefore carried out the Monte Carlo study for the system again in the present paper and found that our simulation almost agrees with the results of the STM. 相似文献