3.1. CH4 Observations
 Globally-averaged surface CH4 mole fractions (solid line) and deseasonalized trend (dashed line) at weekly resolution are plotted in Figure 1a for 1983 to 2008. From 1999 to 2006, CH4 remained nearly constant except for a small increase in 2002 to 2003. Based on measurements of CO abundance in the same samples, a potential contributor to this increase was biomass burning in Boreal regions of Asia and N. America [van der Werf et al., 2006]. In Figure 1b, the derivative with respect to time of the trend is plotted as a solid line, and annual increases (from 1 January in one year to 1 January in the next) are plotted as circles. Uncertainties (1 s.d.) are calculated with a Monte Carlo method [Steele et al., 1992] and only account for the sampling uncertainty resulting from the distribution of our network. Though the average annual increase from 2000 to 2006 was 0.4 ppb yr−1 (s.d. = 3.1 ppb yr−1), the global CH4 burden decreased during 3 of these years. In 2007, the global increase was 8.3 ± 0.6 ppb, in good agreement with Rigby et al. , corresponding to an imbalance between emissions and sinks of ∼23 Tg CH4. Except for 1998, this is the largest observed increase since the early 1990s. The largest zonally averaged CH4 increase in 2007 was observed at polar northern latitudes, 13.7 ± 1.3 ppb. Despite this large increase at Arctic latitudes, the increase during 2007 in the zonally averaged Southern Hemisphere (9.2 ± 0.3 ppb) was larger than the increase in the zonally averaged Northern Hemisphere (7.3 ± 1.3 ppb). In 2008, the global increase was 4.4 ± 0.6 ppb yr−1, with the largest increase, 8.1 ± 1.6 ppb, observed at low northern latitudes. Northern polar regions resumed their low growth in 2008, with near-zero increase (0.5 ± 0.8 ppb).
Figure 1. (a) Solid line shows globally averaged CH4 dry air mole fractions; dashed line is a deseasonalized trend curve fitted to the global averages. (b) Instantaneous growth rate for globally averaged atmospheric CH4 (solid line; dashed lines are ±1σ [Steele et al., 1992]). The growth rate is the time-derivative of the dashed line in Figure 1a. Circles are annual increases, calculated from the trend line in Figure 1a as the increase from January 1 in one year to January 1 in the next. (c) Residuals from a function fitted to zonal averages for CH4 (solid line), CO (dotted line), and MOPITT CO (circles) for polar northern latitudes (53.1°N to 90°N). (d) Same as Figure 1c, but for the tropics (17.5°S to 17.5°N).
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 Methane mole fractions (Figure 2a) and δ13C (Figure 2b) are plotted for Alert, Canada. Data were smoothed (lines) as discussed above. Minimum CH4 values during summer occur primarily because there is a seasonal maximum in OH concentrations in the Northern Hemisphere, despite summer being the time of maximum CH4 emissions from wetlands. During summer 2007, CH4 at ALT was ∼12 ppb greater than during the previous few summers; this anomaly continued through the winter and persisted into 2008. In late-summer 2007, we also observed that δ13C in CH4 was the lowest during our period of record. The changes in δ13C and CH4 mole fraction from 2006 to 2007 during summer suggest increased emissions from a source with δ13C ≈ −66‰, while typical δ13C from wetlands is −60‰ or lighter. Reaction of CH4 with OH enriches 13C, but only one third as much per mole. A decrease in [OH] would shift observed δ13C in the same direction as increased emissions from 13C-depleted source, but the observed change in δ13C (∼−0.1‰ from 2006 to 2007) is too large to be consistent with potential changes in [OH]. Decreased [OH] would also affect other species such as CO, but significant anomalies were not observed for CO at high northern latitudes in 2007. Emissions from biomass burning, with δ13C values of ∼−25‰, would have resulted in more positive δ13C in CH4.
Figure 2. (a) Circles are CH4 dry air mole fractions from weekly discrete samples collected at Alert, Canada. Lines are a smooth curve fitted to weekly samples and trend, as in Figure 1a. Smoothing of weekly samples eliminates variability with periods on order of one month or less. (b) Circles are δ13C in CH4 (‰) measured in same samples used for CH4 analysis. Lines are same as in Figure 2a.
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3.2. Potential Contributions to the 2007 and 2008 Increases
 Emission rates of CH4 from most anthropogenic sources change gradually, so the drivers of interannual variability in CH4 growth rate are typically changes in emissions from biomass burning and wetlands, and changes in CH4 sink rate, through changes in [OH] [Dlugokencky et al., 1996]. The large increase in CH4 at polar northern latitudes during 2007 compared to other latitude zones was coincident with anomalously high temperature (warmest year during our measurement period for northern wetland regions). Lighter than average δ13C in CH4 during late-summer 2007 is consistent with a wetland source. A change in [OH] at high northern latitudes is not a potentially important contributor to the CH4 budget there, because [OH] is low relative to the tropics and there is a limited seasonal period when the reaction occurs. The effects of changes in [OH] at low latitudes would be transported to high latitudes. Observations of 1,1,1-trichloroethane (update of Montzka et al. ) also suggest no significant contribution to the ∼4% CH4 anomaly in 2007 from decreased [OH] (inferred [OH] changes were in the range −2% to +1%, depending on assumptions made about 1,1,1-trichloroethane emissions). This result is consistent with the change in [OH] estimated by Rigby et al.  because of their large uncertainty range (−4 ± 14%).
 To assess the potential for increased emissions of CH4 from biomass burning at high northern latitudes, we studied surface CO measured in the same samples that were analyzed for CH4. Figure 1c shows residuals from a function (2nd-order polynomial and 4 annual harmonics) fitted to zonally averaged CH4 and CO for northern polar latitudes (53° to 90°N). Significant elevations from the noise are seen for CH4 residuals (solid line) in 1997/98, 2002/03, and 2007/08. CO, with an emission molar ratio relative to CH4 for biomass burning in the range 10 to 20 [Christian et al., 2003], has large residuals (dotted line) only during the first two periods, when anomalies in Boreal biomass burning are known to have occurred. This also suggests the Arctic CH4 anomaly in 2007 is related to sources other than biomass burning, or to a larger change in [OH] than is consistent with methyl chloroform observations.
 In the tropics, our CO measurements may be a less-reliable indicator of biomass burning emissions, because emissions are injected into the mid-troposphere, away from our surface sampling sites. Despite this, CO anomalies in the tropics were clearly seen in late-1997 and 1998 when biomass burning was wide-spread in Indonesia (Figure 1d). During 2006, 2007, and 2008, the surface CO signal was small, typical of background variability. However, in the middle troposphere, from October, 2006 through March, 2007, evidence of biomass burning comes from monthly averaged CO centered at 700 hPa detected by MOPITT (Measurements of Pollution in the Troposphere), a gas filter radiometer on board the Terra satellite from which CO vertical profiles are obtained [see, e.g., Edwards et al., 2006] (http://www.acd.ucar.edu/mopitt/MOPITT/data/plots4/mapsv4_mon.html). CO anomalies up to 90 ppb were detected over the Indian Ocean. Zonally averaged monthly CO anomalies for polar northern (Figure 1c) and tropical latitudes (Figure 1d) are plotted as circles. Further evidence that some of the CH4 anomaly was caused by biomass burning comes from changes in global ethane abundance observed during 2007 [Simpson et al., 2006; I. Simpson, personal communication, 2008] and CH3Cl (lifetime ∼1.5 yr), which increased along with CH4 in early-2007 at Samoa. Based on an emission ratio of 15 ppt CH3Cl to 1 ppb CH4 for biomass burning [Christian et al., 2003] and anomalies in CH3Cl of ∼20 ppt at Mauna Loa and Samoa in 2007, the relative contribution of biomass burning to the CH4 anomaly in the tropics during 2007 was small.
 A source other than biomass burning must have made significant contributions to the CH4 enhancements in the tropics and extra-tropical Southern Hemisphere. Based on our analysis of gridded precipitation fields [Schneider et al., 2008] (http://gcmd.nasa.gov/records/GCMD_DWD-GPCC_VASClimO.html), 2007 had the 3rd-largest and 2008 the largest positive precipitation anomalies from 1986 to 2008 for all wetland grid cells between 17.5°S and 17.5°N. In the tropics, precipitation is the dominant driver of wetland CH4 emissions. Above-normal precipitation is common in some tropical regions during La Niña events; La Niña conditions started in mid-2007, waned toward the end of the year, and intensified during the first half of 2008. Vertical profiles of air samples collected near Santerém and Manaus in eastern and central Amazônia are typically enhanced in CH4 relative to Atlantic background sites in the NOAA air sampling network. Miller et al.  used these observations to infer CH4 fluxes averaged over large areas (∼105 km2). Extension of their analysis to include 2007 and 2008 shows that, during these La Niña years (2007 and 2008), CH4 emissions estimated from the profiles averaged over all seasons were ∼50% greater than the average emissions calculated for 2000 to 2006. While many sources contribute to these estimated fluxes, wetlands are likely the dominant source.
 ENSO can affect observed CH4 hemispheric averages in another way. During cold phases, interhemispheric transport may be enhanced as westerly winds at ∼200 hPa in the tropics allow large scale waves to propagate through the topics into the other hemisphere. These conditions can enhance the rate of interhemispheric exchange [Prinn et al., 1992], which may be in part responsible for the increased growth rate of CH4 at mid- to high southern latitudes during 2007. Our measurements of the SF6 latitude gradient over time are consistent with an increase of ∼15% in the rate of interhemispheric exchange. We last saw such an event for CH4 during the La Niña of 1988/1989 when the CH4 growth rate in the SH increased while the growth rate in the NH decreased by a comparable magnitude. Changes in growth rate were accompanied by a decrease of ∼5 ppb in the difference between NH and SH annual means in 1989. These changes are consistent with a temporary increase in interhemispheric exchange rate of ∼10% [Steele et al., 1992].