42. The low-temperature polymerisation of isobutene. Part VI. Polymerisation by titanium tetrachloride and water in methylene dichloride

Author(s):  
R. H. Biddulph ◽  
P. H. Plesch ◽  
P. P. Rutherford

The yield of polymer formed by low-temperature irradiation of styrene in methylene dichloride has been measured at various concentrations of monomer and at different intensities. Corresponding yields were also determined when polymerization occurred in the presence of Aerosil (fine silica powder). Analysis of the results by means of a Mayo type of plot shows that the increased yield with Aerosil is due to a reduction in the termination step. Chain transfer during propagation is found to explain the relatively small difference in measured molecular weights. Over much of the range studied the intensity exponent is about 1 without and 0.5 with Aerosil. The former agrees with the usual kinetics involving a termination by the original gegenion, whereas the latter requires termination by a species produced in a separate ionizing event.


1989 ◽  
Vol 31 (3) ◽  
pp. 547-553
Author(s):  
V.G. Sergeyev ◽  
V.Yu. Baranowskii ◽  
G.M. Lukovkin ◽  
V.A. Kabanov

Catalysts ◽  
2020 ◽  
Vol 10 (10) ◽  
pp. 1187
Author(s):  
Huyen Duong Ngoc ◽  
Dung Mai Xuan ◽  
Tuan Mai Van

The titanium dioxide (TiO2) nanostructures resulted by the pyrolysis of titanium tetrachloride (TiCl4) at a low temperature of 80 °C were found to be a mixture of amorphous TiO2 complexes and anatase nanostructures, whose ratio depends on the pH of the pyrolysis medium. At a low pH level, the resulting TiO2 nanostructures are predominantly anatase and gradually shift to amorphous TiO2 complexes as the pH level increases. Moreover, the amorphous TiO2 complexes can convert back to anatase nanostructures by a post-heating treatment, and can then transform to rutile with elevating temperature. Amongst the TiO2 nanostructures recovered from the amorphous TiO2 complexes, anatase appears to be the most effective photocatalyst in the decomposition of methylene blue.


Author(s):  
P.P.K. Smith

Grains of pigeonite, a calcium-poor silicate mineral of the pyroxene group, from the Whin Sill dolerite have been ion-thinned and examined by TEM. The pigeonite is strongly zoned chemically from the composition Wo8En64FS28 in the core to Wo13En34FS53 at the rim. Two phase transformations have occurred during the cooling of this pigeonite:- exsolution of augite, a more calcic pyroxene, and inversion of the pigeonite from the high- temperature C face-centred form to the low-temperature primitive form, with the formation of antiphase boundaries (APB's). Different sequences of these exsolution and inversion reactions, together with different nucleation mechanisms of the augite, have created three distinct microstructures depending on the position in the grain.In the core of the grains small platelets of augite about 0.02μm thick have farmed parallel to the (001) plane (Fig. 1). These are thought to have exsolved by homogeneous nucleation. Subsequently the inversion of the pigeonite has led to the creation of APB's.


Author(s):  
S. Edith Taylor ◽  
Patrick Echlin ◽  
May McKoon ◽  
Thomas L. Hayes

Low temperature x-ray microanalysis (LTXM) of solid biological materials has been documented for Lemna minor L. root tips. This discussion will be limited to a demonstration of LTXM for measuring relative elemental distributions of P,S,Cl and K species within whole cells of tobacco leaves.Mature Wisconsin-38 tobacco was grown in the greenhouse at the University of California, Berkeley and picked daily from the mid-stalk position (leaf #9). The tissue was excised from the right of the mid rib and rapidly frozen in liquid nitrogen slush. It was then placed into an Amray biochamber and maintained at 103K. Fracture faces of the tissue were prepared and carbon-coated in the biochamber. The prepared sample was transferred from the biochamber to the Amray 1000A SEM equipped with a cold stage to maintain low temperatures at 103K. Analyses were performed using a tungsten source with accelerating voltages of 17.5 to 20 KV and beam currents from 1-2nA.


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