the coking properties of coal at elevated pressures. - Argonne ...
the coking properties of coal at elevated pressures. - Argonne ...
the coking properties of coal at elevated pressures. - Argonne ...
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Intrinsic R<strong>at</strong>io <strong>of</strong> Fuel Nitrogen Conversion to Nitric Oxide<br />
The significant magnitude <strong>of</strong> nitric oxide destruction by char or<br />
o<strong>the</strong>r reducing gas suggests th<strong>at</strong> <strong>the</strong> concentr<strong>at</strong>ion <strong>of</strong> nitric oxide<br />
measured <strong>at</strong> <strong>the</strong> top <strong>of</strong> <strong>the</strong> bed or freeboard did not reflect <strong>the</strong> intrin-<br />
sic evolution level <strong>of</strong> nitric oxide from <strong>the</strong> combustion. Thus <strong>the</strong><br />
measured value depended on <strong>the</strong> rel<strong>at</strong>ive importance <strong>of</strong> <strong>the</strong> r<strong>at</strong>e <strong>of</strong> "NO"<br />
form<strong>at</strong>ion reaction and <strong>the</strong> r<strong>at</strong>e <strong>of</strong> "NO" reduction. The experimentally<br />
obtained concentr<strong>at</strong>ion pr<strong>of</strong>iles along <strong>the</strong> height <strong>of</strong> <strong>the</strong> bed and free-<br />
board may verify this mechanism. Inform<strong>at</strong>ion concerning <strong>the</strong> intrinsic<br />
evolution level <strong>of</strong> "NO" from char particles is required to describe <strong>the</strong><br />
above process quantit<strong>at</strong>ively. The response curve <strong>of</strong> "NO" formed within<br />
<strong>the</strong> combustor by <strong>the</strong> puls input char was measured so th<strong>at</strong> <strong>the</strong> effect <strong>of</strong><br />
<strong>the</strong> subsequent "NO" reduction by char or o<strong>the</strong>r reducing gas could be<br />
minimized. This is shown schem<strong>at</strong>ically in Fig.5(a). The response peak<br />
<strong>of</strong> "NO" formed by <strong>the</strong> combustion with <strong>the</strong> reduced intensity <strong>of</strong> <strong>the</strong> input<br />
puls tends to a certain value from which <strong>the</strong> intrinsic r<strong>at</strong>ion <strong>of</strong> fuel<br />
nitrogen conversion to nitric oxide could be evalu<strong>at</strong>ed. Typical results<br />
are illustr<strong>at</strong>ed in Fig. 5(b). This value seems to be a little smaller<br />
than <strong>the</strong> value obtained by continuous combustion in a small experimental<br />
facility. This fact suggests th<strong>at</strong> <strong>the</strong> emission level <strong>of</strong> nitric oxide is<br />
affected by <strong>the</strong> intensity <strong>of</strong> combustion, consequently <strong>the</strong> steady st<strong>at</strong>e<br />
carbon concentr<strong>at</strong>ion within <strong>the</strong> bed. However, <strong>the</strong>se results do not<br />
reduce <strong>the</strong> validity <strong>of</strong> <strong>the</strong> experimental results obtained by a small<br />
scale combustion facility concerning <strong>the</strong> behavior <strong>of</strong> nitric oxide<br />
emission.<br />
11. KINETICS OF "NO" DESTRUCTION<br />
R<strong>at</strong>e <strong>of</strong> "NO" reduction by char')<br />
An iso<strong>the</strong>rmal fixed bed tubular reactor <strong>of</strong> diluted char particles<br />
and activ<strong>at</strong>ed carbon (char 11, carbon in table 2) was used to measure<br />
<strong>the</strong> reaction r<strong>at</strong>e over a temper<strong>at</strong>ure range which is <strong>of</strong> practical importance<br />
in fluidized bed combustion. Since <strong>the</strong> "NO" concentr<strong>at</strong>ions<br />
employed in <strong>the</strong> experiment were <strong>of</strong> <strong>the</strong> order <strong>of</strong> several hundred ppm, <strong>the</strong><br />
amount <strong>of</strong> carbon could be assumed to be constant.<br />
reported elsewhere.<br />
The details were<br />
The reduction <strong>of</strong> "NO" by char and activ<strong>at</strong>ed carbon was first order<br />
with respect to "NO" concentr<strong>at</strong>ion. Figure 6 represents <strong>the</strong> Arrhenius<br />
plot for char where alpha (a) denotes <strong>the</strong> r<strong>at</strong>io <strong>of</strong> <strong>the</strong> concentr<strong>at</strong>ion <strong>of</strong><br />
oxygen to <strong>the</strong> concentr<strong>at</strong>ion <strong>of</strong> "NO" <strong>at</strong> <strong>the</strong> inlet. Thus <strong>the</strong> line coresponding<br />
to a=O indic<strong>at</strong>es this r<strong>at</strong>e.<br />
At lower temper<strong>at</strong>ure ranges <strong>the</strong> activ<strong>at</strong>ion energy for char was<br />
16.3 kcal/mol and coincided with <strong>the</strong> d<strong>at</strong>a reported previously. Above<br />
680T <strong>the</strong> activ<strong>at</strong>ion energy was 58.6 kcal/mol. The reason for <strong>the</strong><br />
increase in <strong>the</strong> activ<strong>at</strong>ion energy has not been explained. In <strong>the</strong> lower<br />
temper<strong>at</strong>ures <strong>the</strong> desorption <strong>of</strong> carbon-oxygen surface complex was considered<br />
to control <strong>the</strong> overall r<strong>at</strong>e. The gaseous reaction product was<br />
Nz, CO and COz. As <strong>the</strong> temper<strong>at</strong>ure was elev<strong>at</strong>ed, <strong>the</strong> fraction <strong>of</strong> CO<br />
in <strong>the</strong> reaction product increased.<br />
268<br />
c