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As part of the preparation for this project, a Category III Quality Assurance Project Plan (QAPP)<br />

was prepared and approved for the field campaigns. In addition, standard operating procedures<br />

were in place during the field campaigns.<br />

5.2 Assessment of DQI Goals<br />

The critical measurements associated with this project and the established data quality indicator<br />

(DQI) goals in terms of accuracy, precision, and completeness are listed in Table 5-2.<br />

Table 5-2. DQI Goals for Instrumentation<br />

Measurement<br />

Parameter<br />

Analysis Method Accuracy Precision<br />

Acceptance Criterion<br />

(%Bias/Recovery)<br />

Completeness<br />

(%)<br />

Methane PIC OP-TDLAS ±20% ±20% Not applicable 90<br />

Analyte PIC OP-FTIR: Nitrous Oxide<br />

Concentrations<br />

Ambient Wind<br />

Speed<br />

Ambient Wind<br />

Direction<br />

Distance<br />

Measurement<br />

R.M. Young Met heads postdeployment<br />

calibration in EPA<br />

Metrology Lab<br />

R.M. Young Met heads postdeployment<br />

calibration in EPA<br />

Metrology Lab<br />

±25%, ±15%, 10%* ±10% Not applicable 90<br />

±1 m/s ±1 m/s Not applicable 90<br />

±10º ±10º Not applicable 90<br />

Theodolite- Topcon ±1m ±1m Not applicable 100<br />

Beam angle Theodolite- Topcon ±0.1º ±0.1º Not applicable 100<br />

Mercury<br />

concentrations<br />

Lumex Mercury Analyzer ±25% ±25% Not applicable 90<br />

Total Mercury Frontier Geosciences Not applicable ±20% 50-150 90<br />

Organo- Mercury Frontier Geosciences Not applicable ±20% 50-150 90<br />

VOCs EPA Method TO-15 Not applicable ±20% 50-150 90<br />

* The accuracy acceptance criterion of ±25% is for pathlengths of less than 50m, ±15% is for pathlengths between 50 and<br />

100m, and ±10% is for pathlengths greater than 100m.<br />

5.2.1 DQI Check for Methane PIC Measurement with OP-TDLAS<br />

The Boreal <strong>Gas</strong>Finder 2.0 OP-TDLAS provides an R 2 value for each concentration<br />

measurement. The R 2 value is calculated by the internal software of the instrument, and is an<br />

indication of the similarity between the waveform of the sample gas and the reference cell gas.<br />

When the instrument detector receives the returning laser signal after it has passed through the<br />

sample beam path, it converts the signal to the shape of a specific waveform (sample waveform).<br />

The instrument also receives a similar laser signal after the laser has passed through the reference<br />

cell in the instrument (reference waveform). The two waveforms are then digitized and compared<br />

as two numeric arrays. The instrument software then performs a Linear Least Squares Regression<br />

for each measurement, to evaluate the similarity (R 2 ) between the sample and reference<br />

waveforms.<br />

5-2

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