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MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...

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Reactions (R.1) and (R.2) are not written in rigorous form to make the mathematics more<br />

tractable. Although accuracy is lost, the general features are preserved according to the<br />

original authors. A nascent site C*, is created during the gasification step (R.3). For<br />

simplicity, only CO is considered as a product, and both regular and nascent active sites<br />

are assumed to form the same kind of surface oxide. The total active surface is thus<br />

comprised of regular bare sites C, nascent bare sites C*, and covered sites C(O). The<br />

assumption of steady-state values of these parts of the T<strong>AS</strong>A (Total Active Surface<br />

Area) results in an expression for the fraction of covered sites, , given below:<br />

=<br />

1<br />

2 kdP + kb P<br />

1<br />

2 k ckd / ka + (kc + kd )P + k bP . (2.31)<br />

The reaction rate equation is then easily obtained:<br />

r =<br />

1<br />

k<br />

c<br />

(k<br />

d<br />

P 2 + kbP) 1<br />

k<br />

c<br />

k<br />

d<br />

/ k<br />

a<br />

+ (k<br />

c<br />

+ k<br />

d<br />

)P2<br />

+ kbP 21<br />

. (2.32)<br />

This equation has four rate constants. Each rate constant has two parameters (E and A).<br />

Thus there are eight adjustable parameters in this rate equation. No values of the rate<br />

constants or quantitative examination of this equation were given in their paper.<br />

Data of Banin et al.<br />

Banin et al. (1997) studied the combustion behavior of pulverized char in drop-<br />

tube experiments. The gas temperature was varied between 1200 and 1800 K and the gas<br />

pressure was about 8 atm. The oxygen partial pressure was varied between 0.3 and 8<br />

atm. In all cases, 95% of the coal and char particles had diameters less than 6 μm. The<br />

apparent reaction order at high oxygen pressure was observed to be as low as 0.3. This<br />

could not be explained as Zone I combustion since the char particles were observed to

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