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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Table A.2. Measured Centerline Reactor Temperatures<br />
Condition number #1 #2 #3 #4<br />
Condition name CH 4 fuel-rich CH 4 fuel-lean CO fuel-rich CO fuel-lean<br />
Height Above Burner Gas Temperature Profile (K)*<br />
0.25 1542 1677 1650 1718<br />
0.50 1637 1628 1687 1670<br />
0.75 1640 1608 1703 1647<br />
1.00 1644 1592 1696 1630<br />
* Measured along reactor centerline, corrected for radiation loss.<br />
Procedures and Apparatus<br />
Char Preparation<br />
Coal particles were injected through the flame, reacted, captured by a suction<br />
probe at a certain distance away from the injection point, quenched by nitrogen in the<br />
probe tip, and separated from the soot and the gas in a virtual impactor and cyclone<br />
system. The distance between the injection point and the suction probe (called the<br />
reaction length or sampling height) was set to one inch for most of the experiments,<br />
corresponding to a residence time of 14 ms. Studies of Koonfontain char were also made<br />
at the methane fuel-lean condition at increased residence times by sampling at heights of<br />
2, 4, and 6 inches (corresponding to about 25, 44, and 63 ms, respectively).<br />
The particle residence time as a function of sampling height was measured for<br />
several different coals with a high-speed video camera by Ma (1996). The residence time<br />
was found to be dependent on the gas temperature profile and the total flow rate through<br />
the reactor, but almost independent on the coal type. The total flow rate and gas<br />
temperature profile were therefore kept very similar from one reactor condition to another<br />
in order to achieve similar particle residence times. In this project the particle residence<br />
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