| Literature DB >> 34565227 |
Euan G Nisbet1,2, Edward J Dlugokencky3, Rebecca E Fisher1, James L France1,4, David Lowry1, Martin R Manning5, Sylvia E Michel6, Nicola J Warwick2.
Abstract
The causes of methane's renewed rise since 2007, accelerated growth from 2014 and record rise in 2020, concurrent with an isotopic shift to values more depleted in 13C, remain poorly understood. This rise is the dominant departure from greenhouse gas scenarios that limit global heating to less than 2°C. Thus a comprehensive understanding of methane sources and sinks, their trends and inter-annual variations are becoming more urgent. Efforts to quantify both sources and sinks and understand latitudinal and seasonal variations will improve our understanding of the methane cycle and its anthropogenic component. Nationally declared emissions inventories under the UN Framework Convention on Climate Change (UNFCCC) and promised contributions to emissions reductions under the UNFCCC Paris Agreement need to be verified independently by top-down observation. Furthermore, indirect effects on natural emissions, such as changes in aquatic ecosystems, also need to be quantified. Nitrous oxide is even more poorly understood. Despite this, options for mitigating methane and nitrous oxide emissions are improving rapidly, both in cutting emissions from gas, oil and coal extraction and use, and also from agricultural and waste sources. Reductions in methane and nitrous oxide emission are arguably among the most attractive immediate options for climate action. This article is part of a discussion meeting issue 'Rising methane: is warming feeding warming? (part 1)'.Entities:
Keywords: atmospheric methane growth; nitrous oxide growth
Year: 2021 PMID: 34565227 PMCID: PMC8473950 DOI: 10.1098/rsta.2020.0457
Source DB: PubMed Journal: Philos Trans A Math Phys Eng Sci ISSN: 1364-503X Impact factor: 4.226
Figure 1Record of zonally averaged methane in the marine boundary layer, 2008–2019, from NOAA's Cooperative Global Air Sampling Network. Surface shows atmospheric methane as a function of latitude (10° spacing) and time (48 steps per year). Rear of plot: North Pole. Front of plot: South Pole. Note renewed growth from 2008, increasing in 2014. E. Dlugokencky, NOAA. (Online version in colour.)
Figure 2Upper panel: Global monthly mean methane record from the NOAA collaborative global network. Lower panel: Annual growth rates in global methane: note strong growth in the 1980s, reduced growth in many years in the 1990s, stabilization 1999–2006 and renewed growth from 2007. Plots show data to 1 January 2020; more recent data show very strong growth. (Online version in colour.)
Figure 3Coincidence of start of onset of global growth in the methane burden with the sustained shift towards more negative δ13CCH4. Red symbols show weekly global means; blue lines show deseasonalized trends. (a) Global mean atmospheric methane (as in figure 2). (b) δ13C isotopic ratio in atmospheric methane: note synchroneity of negative shift with start of 2007 rise in the upper panel. University of Colorado, INSTAAR and NOAA data. E. Dlugokencky. (Online version in colour.)
Approximate isotopic source signatures of the major inputs to the global budget, and the fractionations imposed by the major sinks. Note the caveat that the variability in each source is likely greater than the s.d. shown here.
| source | flux (Tg yr−1)b | ||
|---|---|---|---|
| microbial | −62 (±12) | −317 (±66) | 516 (360–463) |
| fossil | −45 (±21) | −197 (±102) | 155 (112–194) |
| biomass burning | −26 (±10) | −211 (±30) | 31 (26–46) |
| sink | 13C | D | |
| [OH] | −3.9c, −5.4d | −145e, −200f, −227c −237g | 553 (476–677) |
| soil uptake | −16 to −26h,i,j,k | −90k, −62k | 30 (11–49) |
| tropospheric [Cl] | −62l,m | −337n | 11 (1–35) |
| stratosphere | −3o | — | 31 (12–37) |
Source signatures and fluxes (with ranges).
aSherwood et al. [64].
bSaunois et al. [29]. Sink fluxes (with ranges) and isotopic fractionation factors (where ε is defined as the ratio of the reaction rate constants minus 1, with the rate constant for the more abundant isotopologue as the denominator).
cSaueressig et al. [65] (296 K).
dCantrell et al. [66] (273–353 K).
eDeMore [67] (298 K).
fGierczak et al. [68] (298 K).
gJoelsson et al. [69] (298 K).
hKing et al. [70].
iTyler et al. [71].
jReeburgh et al. [72].
kSnover et al. [73].
lSaueressig et al. [74] (297 K).
mCrowley et al. [75] (298 K).
nSaueressig et al. [76] (296 K).
oLassey et al. [77].
Figure 4δ13CCH4 record from weekly air samples collected at Mauna Loa Observatory, 1998–2017. Note sustained shift to more negative values since 2007. Later data are as yet unvalidated. S.E. Michel. (Online version in colour.)
Figure 5Zonally averaged δ13CCH4 and its uncertainty range for high latitude Northern Hemisphere (HNH), low latitude Northern Hemisphere (LNH), low latitude Southern Hemisphere (LSH) and high latitude Southern Hemisphere (HSH). These are semi-hemispheres: equator-30° = LNH/LSH and 30–90° = HNH/HSH. For practical purposes, they represent equal volumes of atmosphere, approximately 25% of the global total, each. Uncertainty estimates consider atmospheric variability, analytical uncertainty and the uncertainty of the sampling network. S.E. Michel. (Online version in colour.)
Figure 6Top panel shows the evolution of methane's mean global atmospheric mixing ratio (green open circles) compared to Representative Concentration Pathways RCP2.6 and RCP8.5 [123] and shared socio-economic pathways (SSP) from [124]. RCP2.6 scenario, which is consistent with the Paris Agreement, peaks in 2012, whereas SSPs peak in the early 2020s, and RCP 8.5 (dotted) continues to rise throughout the twenty-first century. Lower panel shows similar evolution scenarios for CO2. Radiative forcing used here is from Etminan et al. [11] and the figure is updated from that in [4] using NOAA/GML mole fraction data to January 2021. M. Manning. (Online version in colour.)
Figure 7Globally averaged N2O, 2001-present. Note sustained growth at increasing rates. NOAA data: E. Dlugokencky. (Online version in colour.)