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Diurnal cycle of O 3 at three sites in New England. Dates correspond to selected examples in Figure 4.  

Diurnal cycle of O 3 at three sites in New England. Dates correspond to selected examples in Figure 4.  

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Data obtained from spring 2001 to summer 2003 in New England by the Atmospheric Investigation, Regional Modeling, Analysis and Prediction (AIRMAP) program were used to document the diurnal characteristics of O3, CO2, NO, and during selected intervals hydrocarbon and oxygenated species. The diurnal cycles of O3 and oxygenated species showed a monoto...

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... To further examine the characteristics of the O 3 diurnal cycle across New England, we examined it on four nights at Chicopee, Ware, and Boston, Massachusetts ( Figure 5). All three sites showed similar trends in both O 3 depletion and replenishment which mimicked the fea- tures of the diurnal cycle at TF (Figure 2). ...
Context 2
... three sites showed similar trends in both O 3 depletion and replenishment which mimicked the fea- tures of the diurnal cycle at TF (Figure 2). Using the hourly averaged data presented in Figure 5, the rates of depletion and replenishment were calculated for these four time periods. The results are summarized and compared with results for TF in Table 2. Overall the agreement was reasonable given there are undoubtedly local terrain and other micrometeorological features that cause differences in the actual rates between each location. ...

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... Ground-level ozone (O 3 ) is mainly produced by precursors such as nitrogen oxides (NOx) and volatile organic compounds (VOCs) under light conditions [1][2][3][4][5]. Due to the synthetic effects of photochemical generation, dry depositions, and boundary layer entrainment, the diurnal variation in ozone concentration usually presents a unimodal distribution; that is, the concentration is higher during the daytime and lower at nighttime, which has been confirmed by a large number of field observations [6][7][8][9][10][11]. However, in recent years, many studies have demonstrated that nocturnal ozone concentrations are surging and that a nocturnal ozone peak occurs, which has been widely observed in the United States, Europe, and China [12][13][14][15][16][17][18][19]. ...
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... The decrease in GEM concentration at night may be due to the interaction of pollutants from regional emissions and long-range transport (Fu et al., 2008(Fu et al., , 2010. After sunrise, partial GEM re-emission occurs in the sunlight, along with the mixing effect of the residual boundary layer downward, which may lead to an increase in GEM concentration (Mao and Talbot, 2012;Selin et al., 2007;Weiss-Penzias et al., 2009;Talbot et al., 2005). The height of the boundary layer increases after noon during the daytime, which produces dilution of GEM at the surface and may be the reason for the decrease in GEM concentration in the afternoon. ...
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... The nighttime mixing ratio of hourly O3 drops close to zero in Bode, Paknajol and Pulchowk in the winter season. This is a typical characteristic of many urban areas where reaction with NO at night depletes O3 from the boundary layer (e.g., Talbot et al., 2005). In the pre-monsoon and monsoon months, the titration is not as strong and the hourly O3 falls, but generally remains above 10 ppb. ...
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... This phenomenon abnormalities in comparison with those on 11 May and 13 May, when there was gradual decline in O3 concentration by 00:00 and 06:00 LT. As Talbot et al. (2005) suggested that the second surface O 3 maxima at night were likely due to downward mixing of RL O 3 . Based on this hypothesis, we further observed the vertical distribution of O 3 concentrations during this time (Fig. 5(c)) and found a significant decrease in O 3 concentration at~0.5-1.0 km and an increasing tendency in the lower atmospheric layers. ...
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Aim at the effects of the coastal characteristic on ozone pollution in the Yangtze River Delta (YRD), a campaign was launched at the Ningbo, China in the summer of 2020, which mainly covered the monitoring of the vertical profiles of ozone (O3) concentration, three-dimensional wind field, temperature and humidity profiles and parameters of boundary layer dynamic-thermodynamic structure. At the coastal research station, a sea-land breeze (SLB) circulation accompanied by a concurrent coastal low-level jets (CLLJ) structure was observed and identified during 11-12 May 2020. The sea breeze first formed at 10:00 LT on 11 May, turned to land breeze at night, and returned to sea breeze again at 10:00 LT the next morning, prevailing at altitudes of 0-0.5 km and 0-0.3 km respectively. Land breeze at night carries O3 from the inland to the sea forming high ozone levels over the sea, and the shift of the sea breeze during daytime further blew pollution back to the land. Additionally, the conversion of SLB contributed to the occurrence of CLLJ at the altitudes of ~0.3-0.7 km by 02:00 and 06:00 LT, of which the center of wind speed reached ~13 m s-1. The CLLJ-induced turbulent activity decoupled the residual layer (RL) and stable boundary layer, leading to a reduction of RL-O3 levels and an increase of ~50 μg m-3 in surface-O3 concentration. The YRD's unique coastal characteristics make O3 pollution causes in coastal areas more complicated.
... There was a slight increase in the concentration of acetonitrile during the daytime, and a slow decrease after sunset. This curve was similar to that of acetonitrile concentration data from a rural site in New Hampshire, USA (Jordan et al., 2009), and was likely due to dry deposition (Talbot et al., 2005). The specific and detailed source apportionment for VOCs is discussed in Section 3.4. ...
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... Additional sources include secondary production from the reactions of methylperoxy radicals (CH 3 O 2 ) with CH 3 O 2 and other organic peroxy radicals (Madronich & Calvert, 1990;Tyndall et al., 2001), as well as emissions from oceans (Heikes et al., 2002;Millet et al., 2008), biomass burning (e.g., Akagi et al., 2013;Hornbrook et al., 2011;Wentworth et al., 2018), and anthropogenic sources including solvent use, vehicular exhaust, and industrial processes (Legreid et al., 2007;Olivier et al., 1994;Velasco et al., 2009). Its sinks include reaction with OH (Sander et al., 2006), surface deposition (Karl et al., 2005(Karl et al., , 2004Mao et al., 2006;Talbot et al., 2005), and uptake by the ocean (Yang, Beale et al., 2014;Yang et al., 2013). ...
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... Stability plots generated using NOAAS's HRRR model indicate that during each night of the sampling campaign, atmospheric inversions occurred, creating a moderately stable to extremely stable (Pasquill atmospheric stability class) boundary layer in the valley with a depth of approximately 50 to 100m (Figure 3.5A). These conditions are consistent with the documented trapping of chemical constituents, such as ozone and carbonyl sulfide, within the boundary layer and their depletion by chemical reactions or by vegetation uptake(Talbot et al., 2005;Wehr et al., 2017). Hg 0 is an additional atmospheric constituent that is similarly trapped within the boundary layer resulting in diel variations in THg and Hg isotopic composition(Fu et al., 2016b;Jiskra et al., 2019;Kellerhals et al., 2003;Poissant et al., 2008;. ...
Thesis
Mercury (Hg) is a neurotoxic trace metal that is globally distributed and has important implications for human health. The anthropogenic use of Hg has caused the concentration of Hg in the environment to approximately triple since ~1850. It is therefore imperative to understand the historical deposition trends and modern biogeochemical cycling of Hg to better inform future policy actions regarding the release of Hg to the environment. In this dissertation, measurements of Hg stable isotopes were applied to an environmental record of historical Hg deposition and to remote, low Hg concentration atmospheric samples to answer outstanding questions regarding both historical and modern biogeochemical conditions and processes driving Hg cycling in the environment. To discern past sources of Hg and conditions controlling Hg isotope fractionation in the atmosphere, a sediment core from a remote, high elevation lake near Jackson, Wyoming was collected. Lake sediments were dated to understand temporal changes in the deposition of Hg to the sediments, revealing an approximate 3.8-fold increase in Hg flux from 1850 to the present. Additionally, measurements of Hg stable isotope ratios in the sediments indicated a shift in atmospheric chemical reactions over the same period. Analyses of wet precipitation and snow collected in the lake’s vicinity were utilized to explain the modern Hg isotopic composition observed in the lake sediments and motivated further investigation into Hg isotope fractionation in snow. Measurements of 12-hour atmospheric gaseous Hg samples were collected continuously for one week from two high elevation sites (Mount Bachelor, Oregon and Camp Davis, Wyoming) with contrasting geographic characteristics to understand both the vertical gradient of Hg in the atmosphere and better understand the role of vegetation in Hg isotope fractionation in the atmosphere. Analyses of Hg isotope ratios from samples at Mount Bachelor (mountaintop site) revealed diel variation in the isotopic composition of Hg. Nightly measurements indicated a dominant influence from the free troposphere with a distinct isotopic composition. Near the end of the sampling period, the diel variation dissipated due to a nearby forest fire that came to dominate both daytime and nighttime samples. At Camp Davis (valley site), diel variation in the isotopic composition of Hg was also observed, however, the variation at this site contrasted with observations at Mount Bachelor. Nightly inversions trapping Hg in the valley at Camp Davis and the subsequent uptake of Hg from the atmosphere by vegetation explains the fractionation observed in the residual Hg. Motivated by the analysis of Hg isotopes in snow from Lost Lake, WY, five time series of snow samples (with sampling every 12 hours for 48 hours) were collected at two sites in Michigan (Dexter and Pellston). A time series collected in Dexter during a polar vortex revealed progressively more negative odd-mass independent fractionation (MIF), similar to observations in Arctic snow. In contrast, the fractionation of Hg isotopes in all of the other snow samples progressed towards more positive odd-MIF, indicating a difference in oxidants and binding ligands associated with the Hg in snow. Finally, snow samples indicative of snowmelt were used to estimate the Hg isotopic composition of Hg deposited to mid-latitude ecosystems via snow. As a whole, this dissertation begins to answer outstanding questions concerning processes that control the fractionation and distribution of Hg in the environment and creates a platform for future researchers to expand upon.
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Boundary layer height played an important role in the vertical diffusion of the pollutants .In this research total carbon monoxide column concentration data TCCO, boundary layer height (in meter) (BLH) is consider to study relationship between it. Data taken from (European-Centre for-Medium Range-Weather-Forecasts) (ECMWF) at lat. 33.34 and long. 44.44 (degree) this Situated near the middle of Baghdad city at 8 hours (00,03,06,09,12,15,18,21) from every day for years (2003-2012). The MATLAB program was used to convert data formula from NetCDF (network Common Data Form) nc. File format to excel file. Correlation between boundary layer height (BLH) in (meter) and TCCO concentration column in (Kg/m 2) is accomplished, and consequences display correlation between this column gas and BLH. Two cases were used to find this relationship, First, the daily behaviour, and results show the BLH is low while the CO is high, and gradually decreases to lowest value about (0.67 Kg/m 2) at the hour 12 , when the BLH is at its maximum value (4975 m), then it decreases at night, where TCCO concentration increases. In Second fallouts, monthly and seasonal outlines are consequential and results show that during winter the BLH decrease, the CO concentration reaches its maximum value in February is (1.42 Kg/m 2), and then decrease during March to October until it reaches the lowest value (0.6009 Kg/m 2) during 2012 and increase during October to December, while the BLH is the maximum in May (4991m) in 2008 and gradually decreasing to December. The vital of this revision fundamentally situated in valuation airborne quality of Baghdad city, results show not direct relation between TCCO and BLH, because photochemical reaction in upper atmosphere.
... Moreover, due to less convective activities, the winter season is characterised by shallow boundary layer, which confines the O 3 close to surface thus increasing the concentration level at near surface region. In addition, during winter as the air begins to cool drastically, O 3 rich air grows denser and sinks to lower altitudes, resulting in an increase in lower tropospheric O 3 (Talbot et al., 2005;Seinfeld and Pandis, 2016). This also explains the low O 3 mixing ratio at upper tropospheric region in winter. ...
Article
This paper deals with the temporal changes in the altitude distribution of tropospheric ozone (O3) based on the measurements by balloon-borne O3-sondes during 2011–2014, conducted at the tropical, coastal site Thiruvananthapuram on the south west coast of India. This is the first study from this region addressing the highly dynamic nature of tropospheric O3 profiles (in terms of their vertical structure and short-term changes) and attempting to categorise them based on 121 in-situ measured O3 profiles. The tropospheric O3 profiles could be categorised into four major groups namely (i) those with steady O3 mixing ratio (ii) with increasing mixing ratio, (iii) with mid-tropospheric enhancement and (iv) with multiple layers/laminar nature. The causative mechanisms of these different categories were examined. The observed differences in the tropospheric O3 distribution are attributed to meteorological conditions in particular the synoptic scale systems, long range transport, intrusion from stratosphere and photochemistry, most importantly, the effect of water vapour content. Water vapour and O3 showed complex dependence with positive and negative association depending on the precursor levels and availability of water vapour. The altitudinal changes in O3 also exhibited close association with those of potential temperature and equivalent potential temperature. An analysis of the seasonal characteristics of vertical distribution of tropospheric O3 also carried out along with the altitude-dependent seasonal behaviour. In general, the total column O3 estimated by the integration of O3-sonde retrieved profiles differed by about ±10% with those retrieved by satellite-based measurements. The TCO contributes to about 16% (34 DU) of the total column O3, with minimum of 9% in October and maximum of 27% on March. In general, the OMI retrievals under-estimates the O3-sonde derived TCO by 5–10 DU in all the seasons.