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Fill time Graphite

Rudolph and Bachmann [90,91] studied in detail isothermal chromatography of chlorides of several fission products. They used quartz columns filled with graphite, quartz or quartz coated with NaCl, KC1, MgCl2 or CsCl. They made careful measurements of the retention time versus column temperature, and of the peak widths. The best separation was achieved by temperature-programmed chromatography. It is illustrated by Fig. 1.23. [Pg.30]

Cotten and Boonstra (150) also investigated stress relaxation in swollen vulcanizates. In these experiments, very near elastic equilibrium, n was found to be of the order of 0.01 or less for unfilled vulcanizates and vulcanizates filled with graphitized black. For rubbers reinforced with fully reinforcing furnace black n was two to three times the value for the unfilled rubber. The additional relaxation appears to be due to slow desorption of polymer segments held relatively tightly at the filler surface. [Pg.204]

Fig. 19.10 TOC removal with electrolysis time for the degradation of 100 cm3 of 266 mg dm 3 2,4,5-T (2,4,5-trichlorophenoxyacetic add) solutions in 0.05 M Na2S04 + H2SO4 of pH 3.0 at 35°C. (Open circle) Anodic oxidation in a Pt/graphite cell at 100 mA. (Open square) Anodic oxidation with electrogenerated H202 in a Pt/02 cell at 100 mA. (Open triangle) Electro-Fenton with 1 mM Fe2+ in a Pt/02 cell at 100 mA. Photoelectro-Fenton with 1 mM Fe2+ and UVA irradiation in a Pt/02 cell at (open diamond) 100, (filled circle) 300, and (filled square) 450 mA (Boye et al. 2003c)... Fig. 19.10 TOC removal with electrolysis time for the degradation of 100 cm3 of 266 mg dm 3 2,4,5-T (2,4,5-trichlorophenoxyacetic add) solutions in 0.05 M Na2S04 + H2SO4 of pH 3.0 at 35°C. (Open circle) Anodic oxidation in a Pt/graphite cell at 100 mA. (Open square) Anodic oxidation with electrogenerated H202 in a Pt/02 cell at 100 mA. (Open triangle) Electro-Fenton with 1 mM Fe2+ in a Pt/02 cell at 100 mA. Photoelectro-Fenton with 1 mM Fe2+ and UVA irradiation in a Pt/02 cell at (open diamond) 100, (filled circle) 300, and (filled square) 450 mA (Boye et al. 2003c)...
Figure 8. Center-of-mass trajectories obtained from a simulation of a patch of nitrogen molecules adsorbed on the basal plane of graphite. (Carbon atoms are shown by the small dots.) In part (a) for T=36.9 K, the molecules are commensurate with theVSxVS lattice and vibrate around the site centers except at the edges of the patch. In part (b), 7M4.0 K and the patch has mehed to a 2D fluid that is characterized by chaotic trajectories in the him. (At longer simulation times, the molecules appear to fill the surfece as a 2D gas.) From Ref. [38], Mol. Phys. 55 (1985) 999-1016. Figure 8. Center-of-mass trajectories obtained from a simulation of a patch of nitrogen molecules adsorbed on the basal plane of graphite. (Carbon atoms are shown by the small dots.) In part (a) for T=36.9 K, the molecules are commensurate with theVSxVS lattice and vibrate around the site centers except at the edges of the patch. In part (b), 7M4.0 K and the patch has mehed to a 2D fluid that is characterized by chaotic trajectories in the him. (At longer simulation times, the molecules appear to fill the surfece as a 2D gas.) From Ref. [38], Mol. Phys. 55 (1985) 999-1016.
The electric furnaces, in which this reaction is carried out, are ca. 15 3 3 m- in size and are lined with refractory material. Electrodes at opposite ends are connected to a graphite core. The furnace is filled round this core with the reaction mixture and electrically heated to 2200 to 2400°C. The heating up time is ca. 18 h and the reaction time a further ca. 18 h. After cooling, the sides of the furnaces are removed and the unreacted material on the edges removed. The silicon carbide, which has formed round the graphite core, is broken up and separated into different qualities. [Pg.476]


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