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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 />

146

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