Uncertainties in Calibration of an Optical Spectrometer for Measuring Isotope Ratios in Methane

The stable isotope ratios of carbon (δ13C(CH4)) and hydrogen (δ2H(CH4)) in methane (CH4) from atmospheric air samples provide a tracer that can help distinguish the relative contribution of emission sources. These can be continuously measured at atmospheric monitoring stations by optical isotope ratio spectrometer (OIRS) instruments, providing data that is complementary to isotope ratio mass spectrometry (IRMS) measurements. OIRS instruments directly measure the amount fraction of the 12CH4, 13CH4, and 12CH32H isotopologues, in contrast to the IRMS method of conversion to CO2 and H2, so they have different calibration needs related to reference materials (RMs) and analysis protocol. We use a single high-purity source of CH4, which has been isotopically characterized by IRMS, to produce two calibration RMs that bracket the sample in amount fraction. The isotope ratio measurement is calibrated via the isotopologue amount fraction, which is used to derive analytical expressions for the combined uncertainty. We test this approach using a 550 μmol mol–1 sample (representative of the amount fraction produced from air sampled by the NPL preconcentrator) prepared from a separate CH4 source. The combined standard uncertainty for the isotope ratio of this sample is 0.19 ‰ for δ13C(CH4) and 1.1 ‰ for δ2H(CH4), including uncertainty contributions from the isotopic assignment of the CH4 used for the RMs, their gravimetric preparation, and the spectrometer noise. The dominant contribution to this is from the uncertainty in isotopic assignment of the CH4 used in RM preparation. The next largest contribution to the uncertainty budget is the measurement noise, estimated from the Allan-Werle deviation, and the smallest contribution is from the preparation uncertainty in the total CH4 amount fraction in the RMs. We demonstrate that preparing the bracketing RMs from a common CH4 source results in correlations between isotopologue amount fractions and that neglecting this leads to an overestimation of the isotope ratio uncertainty.

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Publication Details

Journal
ACS Measurement Science Au
Published
2026-02-10
DOI
https://doi.org/10.1021/acsmeasuresciau.5c00094
Primary Topic
Spectroscopy and Laser Applications
Type
article
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article

Uncertainties in Calibration of an Optical Spectrometer for Measuring Isotope Ratios in Methane

Chris Rennick, Aimee Hillier, Emily Hopkinson, Tim Arnold et al.
ACS Measurement Science Au
Spectroscopy and Laser Applications
article

Uncertainties in Calibration of an Optical Spectrometer for Measuring Isotope Ratios in Methane

Chris Rennick, Aimee Hillier, Emily Hopkinson, Tim Arnold, Emmal Safi, Ruth E. Hill-Pearce
article en

Abstract

The stable isotope ratios of carbon (δ13C(CH4)) and hydrogen (δ2H(CH4)) in methane (CH4) from atmospheric air samples provide a tracer that can help distinguish the relative contribution of emission sources. These can be continuously measured at atmospheric monitoring stations by optical isotope ratio spectrometer (OIRS) instruments, providing data that is complementary to isotope ratio mass spectrometry (IRMS) measurements. OIRS instruments directly measure the amount fraction of the 12CH4, 13CH4, and 12CH32H isotopologues, in contrast to the IRMS method of conversion to CO2 and H2, so they have different calibration needs related to reference materials (RMs) and analysis protocol. We use a single high-purity source of CH4, which has been isotopically characterized by IRMS, to produce two calibration RMs that bracket the sample in amount fraction. The isotope ratio measurement is calibrated via the isotopologue amount fraction, which is used to derive analytical expressions for the combined uncertainty. We test this approach using a 550 μmol mol–1 sample (representative of the amount fraction produced from air sampled by the NPL preconcentrator) prepared from a separate CH4 source. The combined standard uncertainty for the isotope ratio of this sample is 0.19 ‰ for δ13C(CH4) and 1.1 ‰ for δ2H(CH4), including uncertainty contributions from the isotopic assignment of the CH4 used for the RMs, their gravimetric preparation, and the spectrometer noise. The dominant contribution to this is from the uncertainty in isotopic assignment of the CH4 used in RM preparation. The next largest contribution to the uncertainty budget is the measurement noise, estimated from the Allan-Werle deviation, and the smallest contribution is from the preparation uncertainty in the total CH4 amount fraction in the RMs. We demonstrate that preparing the bracketing RMs from a common CH4 source results in correlations between isotopologue amount fractions and that neglecting this leads to an overestimation of the isotope ratio uncertainty.

ACS Measurement Science Au
National Physical Laboratory (GB), Lund University (SE), University of Edinburgh (GB)
Affordable and clean energy
Openalex Percentile: Top 63%
Spectroscopy and Laser Applications
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