Evaluating the feasibility of using downwind methods to quantify point source oil and gas emissions using continuous monitoring fence-line sensors
Data files
Jul 01, 2025 version files 8.16 GB
-
AERIES-2m.csv
615.48 MB
-
AERIES-4m.csv
255.82 MB
-
CH4_MGGA_8hz.csv
93.47 MB
-
CH4_MGGA.csv
852.59 MB
-
met.csv
6.34 GB
-
README.md
2.47 KB
-
Releases_Information.csv
80.61 KB
Abstract
The accurate reporting of methane (CH4) emissions from point sources, such as fugitive leaks from oil and gas infrastructure, is important for evaluating climate change impacts, assessing CH4 fees for regulatory programs, and validating methane intensity in differentiated gas programs. Currently, there are disagreements between emissions reported by different quantification techniques for the same sources. It has been suggested that downwind CH4 quantification methods using CH4 measurements on the fence-line of production facilities could be used to generate emission estimates from oil and gas operations at the site level, but it is currently unclear how accurate the quantified emissions are. To investigate model accuracy, this study uses fence-line simulated data collected during controlled release experiments as input for eddy covariance, aerodynamic flux gradient, backward Lagrangian stochastic model, and the Gaussian plume inverse methods in a range of atmospheric conditions. Eddy covariance’s data failed the quality test based on Mauder and Foken (2004) (0-1-2 system) quality test and could not be used for quantification. The aerodynamic flux gradient method quantified within a relative factor (estimated emission/actual emission) of 0.4 to 0.85 for a single release single emission, and at between 2.51 and 4.21 for multiple releases single emissions. The backward Lagrangian stochastic model for point sources using WindTrax performed well for single release single emissions, relative factor of between 0.82 to 1.07, but largely overestimated emissions for multiple releases single emissions, relative factor of 418.8, 2156.7, and 3.91 at 5, 10, and 15-minute averaging. Similar to the backward Lagrangian stochastic model, the Gaussian plume inverse model performed well for single point sources, average relative factor of 3. However, the model largely overestimated emissions when multiple releases were happening, relative factor between 20 and 30. As continuous monitoring of oil and gas sites involves complex emissions where plumes are not defined due to multiple sources, this study shows that the common downwind point source dispersion models could largely overestimate emissions. Aerodynamic flux gradient provided promising results for multiple releases quantification, and this study recommends more testing of flux quantification models for oil and gas continuous monitoring quantification.
https://doi.org/10.5061/dryad.hhmgqnkss
Description of the data and file structure
File list:
- Releases_Information.csv: This is the METEC releases information, location, height, duration, and emission rate
- AERIS-2m.csv: Methane concentration data at location [40.59612017,-105.14032567], 2 m height
- AERIS-4m.csv: Methane concentration data at location [40.59612017,-105.14032567], 4 m height
- CH4 MGGA: Methane concentration data at location [40.59603590,-105.14032186], 3 m height
- CH4_MGGA*_*8hz: Dry methane concentration at location [40.59603590,-105.14032186], 3 m height
- met.csv: Meteorological data from the sonic anemometer collocated with the MGGA, 3 m height
Files and variables
File: AERIES-2m.csv
Variables:
- TimeStamp: Mountain Time in the format mm/dd/yyyy hh:mm:ss
- CH4_ppm_: Methane concentration in ppm
File: AERIES-4m.csv
Variables:
- TimeStamp: Mountain Time in the format mm/dd/yyyy hh:mm:ss
- CH4_ppm_: Methane concentration in ppm
File: met.csv
Variables:
- Time: Mountain Time in the format mm/dd/yyyy hh:mm:ss
- timestamp: UTC Time
- AT: Air temperature (°C)
- BP: Barometric Pressure (hPa)
- RH: Relative Humidity (%)
- U: u wind vector (m/s)
- V: v wind vector (m/s)
- W: w wind vector (m/s)
- WS: wind speed (m/s)
- WD: wind direction (m/s)
File: CH4_MGGA.csv
Variables:
- Time:Mountain Time in the format mm/dd/yyyy hh:mm:ss
- x_CH4__ppm:Methane concentration in ppm
File: CH4_MGGA_8Hz.csv
Variables:
- Time:Mountain Time in the format mm/dd/yyyy hh:mm:ss
- x_CH4__ppm:Methane concentration in ppm
- x_CH4_d_ppm:Dry methane concentration in ppm
- GasP_torr: Gas pressure
- GasT_C: Gas temperature (°C)
File: Releases_Information.csv
Variables:
- EmissionPoint: Identifier for the release point
- Lat: Emission point latitude
- Lon: Emission point longitude
- hs: Emission point height (m)
- EventID: identifier for the release
- UTCStart: Emission start time in UTC
- UTCEnd: Emission end time in UTC
- Duration_HMS: Release duration in hh:mm:ss
- C1FlowAvg_slpm: Methane release rate in slpm
- Actual_Emission_kg_h: Methane release rate in kg/h
Code/software
All files are available in .csv format and can be opened in excel
Methane concentration data for eddy covariance, Gaussian plume inverse method, and the backward Lagrangian stochastic model were collected through an inlet tubing (3.275 inner diameter) at 3 m height, connected to the ABB (Zurich, Switzerland) GLA131 Series Microportable Greenhouse Gas Analyzer (MGGA) set to sample at 10 Hz. The MGGA is a closed-path greenhouse gas analyzer with a ~3.2 lpm pump flowrate, 10 cm cell length, 1 inch cell diameter (~0.23 standard cubic centimeters per minute (sccm) effective volume), and 0.4 s gas flow response time. The inlet tubing was collocated with an R. M. Young (Traverse City, MI, USA) 81000 sonic anemometer (R.M. Young Company, 2023), which measured micrometeorology at 10 Hz. The northward, eastward, and vertical separation of the inlet tubing from the sonic anemometer was 0, 0, -10 cm, respectively. For aerodynamic flux gradient, CH4 concentration data were collected at 2 and 4 m using two Aeris (Hayward, CA, USA) MIRA Ultra Series analyzers connected to tubing with a 3.275 inner diameter. As we had only one sonic anemometer, data from the sonic anemometer collocated with the MGGA were used for the aerodynamic flux gradient quantification.
