4.5 Article

A quantitative comparison of methods used to measure smaller methane emissions typically observed from superannuated oil and gas infrastructure

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ATMOSPHERIC MEASUREMENT TECHNIQUES
卷 15, 期 21, 页码 6285-6296

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COPERNICUS GESELLSCHAFT MBH
DOI: 10.5194/amt-15-6285-2022

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  1. METEC Industry Advisory Board (IAB) at Colorado State University

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This study evaluates the methods for measuring methane emissions from point sources between 40 and 200 gCH(4) h(-1). The results show that the static chamber, dynamic chamber, and Bacharach Hi Flow Sampler (BHFS) methods underestimate the emissions, while the backward Lagrangian stochastic (bLs) method generally underestimates and Gaussian plume (GP) method significantly overestimates the emissions. Direct measurement methods have higher accuracy and precision, while far-field methods have lower accuracy.
Recent interest in measuring methane (CH4) emissions from abandoned oil and gas infrastructure has resulted in several methods being continually used to quantify point source emissions less than 200 gCH(4) h(-1). The choice of measurement approach depends on how close observers can come to the source, the instruments available, and the meteorological/micrometeorological conditions. As such, static chambers, dynamic chambers, Bacharach Hi Flow Sampler (BHFS) measurements, Gaussian plume (GP) modeling, and backward Lagrangian stochastic (bLs) models have all been used, but there is no clear understanding of the accuracy or precision of each method. To address this, we copy the experimental design for each of the measurement methods to make single field measurements of a known source, to simulate single measurement field protocol, and then make repeat measurements to generate an understanding of the accuracy and precision of each method. Here, we present estimates for the average percentage difference between the measured emission and the known emission for three repeat measurements, A(r), for emissions of 40 to 200 gCH(4) h(-1). The static chamber data were not presented because of safety concerns during the experiments. Both the dynamic chamber (A(r) = -10 %, -8 %, and -10% at emission rates of 40, 100, and 200 gCH(4) h(-1), respectively) and BHFS (A(r) = -18 %, -16 %, and -18 %) repeatedly underestimate the emissions, but the dynamic chamber had better accuracy. The standard deviation of emissions from these direct measurement methods remained relatively constant for emissions between 40 and 200 gCH(4) h(-1). For the far-field methods, the bLs method generally underestimated emissions (A(r) = +6 %, -6 %, and -7 %) while the GP method significantly overestimated the emissions (A(r)= +86 %, +57 %, and +29 %) despite using the same meteorological and concentration data as input. Variability in wind speed, wind direction, and atmospheric stability over the 20 min averaging period are likely to propagate through to large variability in the emission estimate, making these methods less precise than the direct measurement methods. To our knowledge, this is the first time that methods for measuring CH4 emissions from point sources between 40 and 200 gCH(4) h(-1) have been quantitatively assessed against a known reference source and against each other.

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