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On the Formation of Nitrogen Oxides During the Combustion of ...

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3.2 Measurement Techniques and Data Acquisition<br />

Calibration <strong>of</strong> Chemiluminescent NO x Analyzer<br />

The chemiluminescent NO x analyzer was calibrated with NO at concentrations<br />

<strong>of</strong> 2.00, 8.66, and 9.80 ppm in an N 2 balance [111]. However, when sampling<br />

from combustion systems, additional species apart from N 2 are introduced,<br />

including H 2 O, CO 2 , CO, H 2 , UHCs, and soot. Under certain circumstances,<br />

<strong>the</strong> composition <strong>of</strong> <strong>the</strong> exhaust can affect <strong>the</strong> measurement value indicated<br />

for NO due to differences in third body quenching reactions between<br />

<strong>the</strong> span gas used and <strong>the</strong> final sample gas (Eq. (3.4)). Fitz and Welch [136],<br />

for instance, report on an NO concentration that is 30% lower than <strong>the</strong> actual<br />

concentration, using syn<strong>the</strong>tic exhaust simulated for a gas-fired power<br />

plant with water vapor at 17% by volume. For such an exhaust analysis, <strong>the</strong><br />

water must ei<strong>the</strong>r be removed prior to NO x detection, <strong>the</strong> detector be calibrated<br />

with saturated span gas, or <strong>the</strong> NO x reading be corrected on <strong>the</strong> basis<br />

<strong>of</strong> third body quenching. The third body quenching effect is most crucial in<br />

samples that have large concentrations <strong>of</strong> non-diatomic constituents. Gärtner<br />

[144], Mat<strong>the</strong>ws et al. [273], and Tidona et al. [439] investigated interferences<br />

in <strong>the</strong> chemiluminescent measurement <strong>of</strong> NO and NO 2 emissions from combustion<br />

systems. Generally, <strong>the</strong> NO x measurement error increases with an increasing<br />

H/C ratio <strong>of</strong> <strong>the</strong> fuel and an increasing equivalence ratio φ. Measurements<br />

taken in very fuel-rich systems or in <strong>the</strong> fuel-rich regions <strong>of</strong> diffusion<br />

flames may be subject to error well above 20% due to <strong>the</strong> potential presence<br />

<strong>of</strong> polyatomic fuel molecules with high quenching characteristics.<br />

As third body quenching may be such a significant source <strong>of</strong> error in NO<br />

measurement with <strong>the</strong> effect <strong>of</strong> excessively low NO x indication, <strong>the</strong> relative<br />

quenching efficiencies <strong>of</strong> various third bodies were included in <strong>the</strong> postprocessing.<br />

The calculation follows <strong>the</strong> procedure <strong>of</strong> Mat<strong>the</strong>ws et al. [273],<br />

which was also employed in <strong>the</strong> work <strong>of</strong> Gärtner [144], Baessler [31], and<br />

Brückner-Kalb [57]. If <strong>the</strong> concentrations <strong>of</strong> <strong>the</strong> important third bodies are<br />

known, <strong>the</strong> actual NO concentration can be calculated from <strong>the</strong> concentration<br />

indicated using <strong>the</strong> following relations:<br />

where<br />

[NO] actual<br />

= X NO,actual<br />

= 1+<br />

[NO] indicated X NO,indicated<br />

J∑<br />

(R M − 1), (3.7)<br />

M=1<br />

R M ≡ I N 2<br />

I M<br />

. (3.8)<br />

91

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