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Finally, they do not form torus or shell distributions.
It is shown that the optimal catalyst distribution can give global pellet selectivities dramatically higher than those obtained with uniform or external shell distributions.
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Szego et al. (2005) fit the incident O+ to a shell distribution function.
Based on the assumption that the N+ component could be pickup ions, Ledvina et al. (2005) showed that the PLS data could be fit by a shell distribution.
These differences could be interpreted when using the bispherical shell distribution based on magnetic field vectors measured by the magnetometer.
The pellet geometry is shown to have a significant effect on the location and sharpness of a shell distribution.
However, at low bulk oxygen concentrations (CO2,L⩽0.3 mol/m3), the performance of the uniform or egg shell distribution catalyst is superior to the core catalyst.
Analytical expressions obtained for the catalyst distributions are used to obtain a condition under which a sharp shell distribution will always occur.
The maximum temperature gain which can be achieved by placing the active material at the optimum position in the pellet, in comparison to an infinitesimal shell distribution, was found to be 48°C at 95% conversion for 1.0% CO.
However, the tail does not emerge smoothly from the flat-topped PUI distribution function but instead appears as a discontinuous, lower intensity attachment to the cutoff step at v ({sim } 2U of the filled shell distribution (see e.g., Gloeckler et al. 1994, 2001), and so a cutoff is still present.
Other putative tasks can be inferred from the position of the other vertices of the pyramidal shell distribution.
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