MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...
MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...
MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...
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The HP-CBK was used to predict the burnouts for all the experiments conducted at 1, 5,<br />
10 and 15 atm, using the above-mentioned gas temperature and wall temperature profiles.<br />
The experiments conducted at 15 atm had extremely low wall temperatures (e.g., 631 K)<br />
and low gas temperatures (e.g., 987 K), and hence were not considered due to ignition<br />
problems. Ignition problems were also observed by other researchers. For example, Field<br />
(1969) observed that a 38-μm char sample was not ignited at low gas temperature and<br />
wall temperature (< 1230 K).<br />
Results<br />
In minimizing the standard deviation of model predictions, two observations were<br />
made: 1) The Langmuir rate equation reduced to the zero-th order equation, implying an<br />
apparent reaction order of 0.5 in Zone II; and 2) The diffusivity contributed from<br />
micropores can be neglected compared to that from the macropores.<br />
The kinetic and pore structure parameters used in this study are listed in Table<br />
7.6. The best-fit calculations of burnouts from the HP-CBK are compared with the<br />
experimental measurements in Figures 7.6 and 7.7. The HP-CBK model was able to<br />
predict particle burnouts with a standard deviation of 14% and a maximum error of 36%.<br />
Table 7.6. Parameters Used in Modeling the Data by Monson (1992).<br />
A 0 = 2.42 × 10 3 mol/cm 3 /sec E 0 = 21.7 kcal/mol<br />
Total Porosity = 0.5 (Pre-set) Macro-porosity M = 0.25<br />
Macro-pore radius r p1 = 2000 Å (Pre-set)<br />
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