the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.

The impact of sea spray aerosol on photochemical ozone formation over eastern China: heterogeneous reaction of chlorine particles and radiative effect
Yingying Hong
Yuqi Zhu
Yuxuan Huang
Chuqi Xiong
Qi Fan
Eastern China has suffered from severe photochemical O3 (ozone) pollution in recent years. In this coastal region, the atmospheric environment can be influenced by sea spray aerosols (SSAs) from marine emissions. However, the extent and mechanisms by which SSA affects O3 formation remain incompletely understood. Here, using the WRF-CMAQ model, this study investigates the comprehensive effect of SSA on radical chemistry and O3 formation in the lower troposphere across four seasons. SSA (over 50 % of which is particulate chlorine) can reach further inland through an atmospheric “bridge” aloft, interacting with the nitrogen-containing gases from continental anthropogenic emissions to reduce NOx levels and release Cl radicals. The NOx reduction increases O3 in volatile organic compound (VOC)-limited regions while decreasing it in NOx-limited zones. Elevated Cl radicals enhance VOC degradation and O3 formation during morning hours. Meanwhile, the scattering properties of SSA reduce daytime O3 formation by diminishing photolysis rates. Due to the contrasting effect of SSA via different mechanisms, the response of O3 varies seasonally and geographically. In winter, SSA increases O3 in eastern China due to the dominant effect of NOx reduction in VOC-limited regions. In spring and autumn, similar effects occur in the North China Plain, whereas southern China sees a decrease due to NOx reduction in the NOx-limited region and reduced photolysis rates. In summer, O3 increases are observed only around Bohai, with reductions elsewhere driven by NOx reductions in NOx-limited regions and decreased photolysis. This study highlights the important, varying, but previously unreported role of SSAs in shaping tropospheric photochemistry over eastern China.
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In recent years, eastern China has grappled with severe photochemical O3 (ozone) pollution, eliciting widespread concern from governmental and academic sectors (Wang et al., 2022; Lu et al., 2018; Wang et al., 2017). Elevated O3 concentrations pose serious threats to public health and have detrimental effects on vegetation growth and crop yields (Fleming et al., 2018; Lefohn et al., 2018; Liu et al., 2018a; Feng et al., 2022). Traditionally perceived as a warm-season issue (Lu et al., 2020), O3 pollution has recently been documented during winter and spring, driven by substantial reductions in NOx emissions juxtaposed against relatively stable VOC (volatile organic compound) emissions in China since 2013 (Li et al., 2021). The escalation of O3 levels following the Clean Air Action in 2013 underscores the need for a nuanced understanding of its formation mechanisms throughout the year (Liu and Wang, 2020a, b; Wei et al., 2022).
Sea spray aerosols (SSAs) are a major natural particulate source in the atmosphere (Weis and Ewing, 1999; Roth and Okada, 1998), generated from oceanic surfaces through wave-breaking and bubble-bursting processes (Lewis and Schwartz, 2004). According to IPCC reports, an estimated 3300 Tg of SSA annually enters the atmospheric boundary layer, driven by wind stress on ocean surfaces and contributing to complex atmospheric chemical interactions. The rapid economic growth in coastal areas, coupled with unique challenges of complex atmospheric pollution, particularly in eastern China, has highlighted the role of SSA in atmospheric oxidation processes. While previous studies have indicated the potential impact of SSA on coastal O3 levels (Dai et al., 2020; Knipping and Dabdub, 2003), a comprehensive and systematic investigation into the mechanisms of these effects is lacking.
Sea spray aerosols influence near-ground O3 formation through multiple mechanisms. SSA can significantly scatter incoming solar radiation that reaches the ground, thereby diminishing the actinic flux within the troposphere (Lohmann and Feichter, 2005; Hatzianastassiou et al., 2007). This reduction in solar energy lowers the rate of photochemical reactions crucial for O3 generation. Near-ground O3 primarily forms through photochemical reactions between NOx and VOCs under sunlight, with its production heavily dependent on the amount of solar radiation penetrating to the surface. As a prominent source of atmospheric aerosols, SSA can attenuate this solar radiation, leading to decreased photolysis rates of NO2 and, consequently, reduced O3 formation (Li et al., 2011; Xing et al., 2017). Currently, this mechanism – the impact of SSA on ground-level ozone through the modulation of photolysis rates – is often overlooked in previous studies on the influence of SSA on O3 concentrations.
Particulate chlorine in SSA engages in heterogeneous chemical reactions with nitrogen-containing gases, releasing Cl radicals that enhance atmospheric oxidation and affect photochemical O3 formation. While the traditional pathway for urban O3 formation involves the reaction of VOCs with hydroxyl radicals (OH), recent research underscores the significant role of Cl radicals in similar processes (Faxon and Allen, 2013; Qiu et al., 2019; Young et al., 2014). Chlorine radicals react with VOCs more rapidly than OH radicals, despite their lower atmospheric concentrations, making their oxidation potential comparably significant (Aschmann and Atkinson, 1995; Nelson et al., 1990; Wingenter et al., 1999).
Particulate chlorine reacts with N2O5 to form nitroxyl chloride (ClNO2), which releases chlorine radicals upon photolysis, contributing significantly to atmospheric Cl levels (Thornton et al., 2010; Bertram and Thornton, 2009; Roberts et al., 2009). These reactions are outlined in Reactions (R1) and (R2) (where g and cd represent the gas and condensed phases, respectively). Observations of ClNO2 have shown high concentrations in eastern China, indicating active chlorine chemistry (Tham et al., 2016; Yun et al., 2018; Wang et al., 2016).
Particulate chlorine can also react with NO2 to produce nitrosyl chloride (ClNO), which, like ClNO2, can release Cl radicals (Reactions R3 and R4) under photolysis (Finlayson-Pitts, 2003; Faxon and Allen, 2013).
Furthermore, particulate chlorine can also directly react with NO3 to release Cl radicals (Reaction R5), which is a potentially important nighttime source of Cl radicals (Gershenzon et al., 1999; Seisel et al., 1999).
Most chemical transport models only considered the reaction between particulate chlorine and N2O5, neglecting other significant chlorine-related heterogeneous chemical processes. To accurately assess the effect of SSA on O3 concentration, it is essential to integrate recent findings on the heterogeneous chemistry of chlorine and update chemical models accordingly. This integration will provide a more comprehensive understanding of SSA's role in photochemical O3 generation, addressing a critical gap in current atmospheric chemistry research.
Heterogeneous chemical reactions of SSA with NOx can alter NOx concentrations, thereby affecting O3 production. As illustrated by Reactions (R1)–(R5), nitrogen oxides undergo heterogeneous chemical reactions with particulate chlorine at night, leading to reduced NOx concentrations. By morning, the photolysis of ClNO and ClNO2 results in the release and subsequent increase NOx concentrations. The relationship between O3 and its precursors is highly nonlinear and varies by region and time due to the differences in the O3 formation regime. In VOC-limited urban and suburban areas, decreases in NOx levels can paradoxically lead to an increase in O3 concentration. Conversely, in NOx-limited rural areas, a reduction in NOx levels typically leads to a decrease in O3 production, highlighting the complex dynamics of atmospheric chemistry (Wang et al., 2017).
In terms of model-based studies, Knipping and Dabdub (2003) incorporated SSA emissions into their model, finding that O3 concentration in the coastal areas of California in the United States increased by 12 ppb in the morning and 4 ppb at noon. Similarly, Sarwar and Bhave (2007) utilized the Community Multiscale Air Quality Modeling System (CMAQ) model to explore the impact of SSA emissions on O3 across the eastern United States, revealing that the associated chlorine chemical processes increased the oxidation of VOCs, thereby enhancing O3 production. This resulted in increases of up to 12 and 6 ppb in the maximum hourly O3 concentrations in the Houston and New York–New Jersey regions, respectively; daily maximum 8 h average O3 concentrations rose by 8 and 4 ppb. Dai et al. (2020) investigated the impact of ClNO2 from sea-salt chloride on O3 in the Pearl River Delta (PRD), China, and found an increase of up to 2.0 ppb over the inland areas during marine winds and up to 3.8 and 6.5 ppb over the South China Sea. However, these studies did not fully account for the tripartite influence of SSA on O3 concentration, nor did they integrate the complete heterogeneous chemistry of chlorine particulates, leading to potential uncertainties in assessing the impact of SSA.
In this study, we employed the WRF-CMAQ model to evaluate the impact of SSA on the tropospheric chemistry in eastern China during different seasons. The responses of HO2, OH radicals, and O3 caused by SSA were quantified. Section 2 demonstrates the modeling settings, SSA emission calculation, and experiment designs. Section 3 discusses the impact of SSA on the tropospheric chemistry. We conclude with a summary of our findings and discussions in Sect. 4.
2.1 Model settings
Here we used the WRF-CMAQ model to perform air quality simulations in this study. The CMAQ (version 5.1) model is a regional chemical transport model developed by the United States Environmental Protection Agency (Appel et al., 2017). It has been widely used to explore the mechanism of multiple air quality issues, including tropospheric ozone, fine particles, acid deposition, and visibility degradation (Zhu et al., 2024; Kitagawa et al., 2021; Onwukwe and Jackson, 2021). The meteorological inputs of the CMAQ model (version 5.1) were provided by the Weather Research and Forecasting (WRF) model. The configuration and emission inputs of WRF-CMAQ were consistent with those used by Hong et al. (2020). Specifically, the simulation environment was structured into two nested domains within the WRF and CMAQ models, featuring horizontal resolutions of 81 and 27 km, respectively (Fig. S1 in the Supplement). These domains included 23 vertical layers extending up to 50 hPa. The inner domain focused on eastern China, where the detailed analysis was conducted, while the outer domain encompassed a broader area, including the land regions of East Asia and the Western Pacific. This broader scope allowed for a comprehensive consideration of SSA emission transport into the region of interest. Meteorological initial and boundary conditions for the WRF model were derived from the NCEP/NCAR final (FNL) reanalysis gridded data, which have a horizontal resolution of 1° × 1°. Chemical boundary conditions for the CMAQ model were sourced from the Model for Ozone and Related Chemical Tracers, version 4 (MOZART-4) results.
The calculation of photolysis rates in CMAQ uses an in-line approach for calculating actinic fluxes by solving a two-stream approximation of the radiative transfer equation (Binkowski et al., 2007; Toon et al., 1989) over wavebands based on the FAST-J photolysis model (Wild et al., 2000). Each layer includes scattering and extinction using simulated air density, cloud condensates, aerosols, and trace gases such as O3 and NO2 (Appel et al., 2017). This approach has been verified or evaluated in previous studies. Based on the aircraft measurement, Baker et al. (2018) found that the CMAQ model can well capture the observed NO2 photolysis rates at ∼ 2 km height. Using this approach, Fu et al. (2014) concluded that the NO2 and O3 photolysis rates reduced by up to 2.4 % and 1.9 %, respectively, due to the impact of dust aerosol during a heavy dust event. Fan and Li (2022) also found that the O3 photolysis rates decreased by 1 %–4 % due to the extinction effect of SSA. These references provide robustness of the CMAQ model's ability to calculate photolysis rates. It enables us to assess the effect of aerosols (e.g., SSA) on photochemical processes by adjusting photolysis rates accordingly.
In the CMAQ simulation, we utilized the SAPRC07TIC (Carter, 2010; Hutzell et al., 2012; Xie et al., 2013) and AERO6i (Lin et al., 2013; Pye et al., 2015) mechanisms to represent gas-phase chemical and aerosol processes, respectively. The AERO6i aerosol module employed ISORROPIA (Binkowski and Roselle, 2003; Fountoukis and Nenes, 2007; Kelly et al., 2010) to uniformly simulate inorganic aerosol thermodynamics. The chlorine depletion of SSA through its equilibrium reactions with H2SO4 and HNO3 was considered in the model (Liu et al., 2015). As for the heterogeneous reaction, the original model was configured to only account for the heterogeneous reaction of particulate chlorine with N2O5 (Reaction R1) (Sarwar et al., 2012, 2014). To provide a more comprehensive evaluation of SSA's impact on photochemistry, we expanded the model's capability to include heterogeneous reactions of particulate chlorine with NO2 (Reaction R3) and NO3 (Reaction R5). We developed a linear segmentation function to parametrize the uptake coefficients of NO2 and NO3 on aerosol surfaces, reflecting their strong positive correlation with relative humidity (Dentener et al., 1996; Stutz et al., 2004). This parameterization was identical across different aerosol modes (Aitken, accumulation, and coarse). The selection of maximum and minimum uptake coefficients for NO2 and NO3 was based on laboratory findings, aligning with methodologies from previous modeling studies by Wang et al. (2012) and Zheng et al. (2015). A detailed exposition of these modifications and their implications for the model's chemistry of heterogeneous reactions is documented by Hong et al. (2020).
Both anthropogenic and natural emissions were incorporated in the simulation to ensure comprehensive atmospheric modeling. Anthropogenic sources included routine pollutant emissions from the MIX emission inventory (http://www.meicmodel.org, last access: 30 August 2025) (Li et al., 2017), international shipping emissions from HTAP (Hemispheric Transport Atmospheric Pollution) emissions version 2.0 dataset (Janssens-Maenhout et al., 2015), and chlorine emissions (HCl and Cl2) from the 2014 ACEIC (Anthropogenic Chlorine Emission Inventory for China) (Hong et al., 2020; Liu et al., 2018b). For natural sources, biogenic emissions were calculated using the Model of Emissions of Gas and Aerosols from Nature (MEGAN) (Guenther et al., 2012), which utilized meteorological inputs from the WRF simulation. Sea spray aerosol emissions were calculated inline in the CMAQ model (see Sect. 2.2).
We utilized the process analysis module within the CMAQ model to quantify the production and loss of model species. This diagnostic tool employs both integrated process rate (IPR) and integrated reaction rate (IRR) methods. The IPR method assesses the contributions of various physical and chemical processes to pollutant concentrations, while the IRR method determines the contributions from specific chemical reactions. Process analysis has been extensively used in prior research to elucidate the chemical mechanism underlying O3 formation (Wang et al., 2015; Chen et al., 2018; Liu et al., 2021).
2.2 SSA emission calculation
The SSA emission was calculated on line in the CMAQ model, utilizing a source function developed by Gantt et al. (2015), which builds upon the foundational source function established by Gong (2003). Gantt et al. (2015) introduced two main modifications to enhance the model's accuracy. Firstly, a sea surface temperature (SST) correction function was incorporated, based on the findings of Ovadnevaite et al. (2014), to account for the substantial impact of SST on SSA fluxes. This correction function linearly adjusts to SST variations, reflecting its influence on emission rates (e.g., Barthel et al., 2019; Liu et al., 2021). Secondly, the shape factor of the source function was adjusted to increase the emission of submicron SSA particles, altering the flux distribution to better reflect observed atmospheric conditions (see Fig. S1 in Gantt et al., 2015). Additionally, surf-enhanced emissions were reduced by narrowing the defined surf zone from 50 to 25 m from the coast, aligning with the modifications in Gantt et al. (2015). The estimated diameters of SSA range from ∼ 0.02 to 20 µm in the model. The composition of dry SSA in different aerosol modes remains consistent with that of seawater, containing Cl− (55.4 %), Na+ (30.8 %), SO (7.7 %), Mg2+ (3.8 %), Ca2+ (1.2 %), and K+ (1.1 %).
2.3 Experiment setting
We conducted simulations for January, April, July, and October of 2015 to represent the typical atmospheric conditions for each season in eastern China. A 10 d spin-up period preceded the actual modeling to stabilize initial conditions. The simulations incorporating all emissions were designated as the baseline scenario (BASE). Additionally, a sensitivity experiment (NOSA), which excluded SSA emissions, was performed to discern the specific contributions of SSA to surface O3 levels. The seasonal impacts of SSA emissions were assessed by comparing the differences in simulated pollutant concentrations between the BASE and NOSA experiments.
Model validation was rigorously carried out against observational data from eastern China for the corresponding periods (Hong et al., 2020). The validation confirmed that the WRF-CMAQ model capably simulated key meteorological factors (temperature, relative humidity, and wind speed) and routine pollutant concentrations (O3, NO2, CO, PM2.5, PM10, and SO2), along with particulate chlorine concentrations. This validation provides a solid foundation for our confidence in further exploring the impact of SSA on tropospheric photochemistry using these modeling results. Detailed validation results were described by Hong et al. (2020).
3.1 SSA transport
We used particulate Na+ as a proxy for SSA, due to its major presence and relatively inactivity in the atmosphere (Neumann et al., 2016). Our analysis distinguished regions significantly affected by SSA by comparing Na+ concentrations from BASE and NOSA experiments (Fig. 1). Near the ocean, areas exhibiting elevated Na+ align with high SSA emissions zones (Fig. S2). In eastern China, increased Na+ concentrations are notably due to SSA transport from the ocean, diminishing progressively with distance from the coast. Cities such as Shanghai and Guangzhou, located along the coastline of eastern China, displayed significant Na+ increases (> 1 µg m−3), indicating marked influence of SSA. Smaller yet notable increases (> 0.1 µg m−3) extend into broader inland areas spanning several provinces including Liaoning, Tianjin, and Guangxi. More than 80 % of the inland region's Na+ within ∼ 100 km of the coast (e.g., Shanghai, Zhejiang, Fujian, Guangdong, and Guangxi) is attributable to SSA, decreasing to 10 %–60 % towards central regions like Hubei. The terrain influences regional SSA impacts distinctly. In northern China, the Taihang Mountains impede westward SSA transport, confining its influence to the North China Plain. Conversely, lower terrain elevations in southern China facilitate broader inland SSA dispersal. Seasonally, the inland reach of SSA is most extensive in July, propelled further by the southerly summer monsoon.

Figure 1Changes in simulated monthly mean concentrations of particulate Na+ induced by SSA (BASE minus NOSA) during January, April, July, and October 2015. Panels (a) and (b) present the spatial distribution of changes and percentage changes, respectively. Panels (c)–(e) display the vertical diurnal variations of changes in Beijing, Shanghai, and Guangzhou, respectively. The black line in panels (c)–(e) is the simulated planetary boundary layer height.
SSA transport also occurs via an “aloft bridge” over the planetary boundary layer, enhancing its penetration inland. Figure 1c, d, and e illustrate vertical diurnal variations of SSA-induced Na+ concentration in Beijing, Shanghai, and Guangzhou, which is pinpointed in Fig. 1a. These profiles reveal that while coastal cities like Shanghai show higher surface-level concentrations, more inland cities such as Guangzhou and Beijing exhibit elevated concentrations aloft, especially in October. This pattern suggests that SSA is not only transported horizontally near the surface but also vertically mixed upward from the coast before descending inland, influenced by varying thermodynamic properties and boundary layer structures between continental and marine areas. Similar transport features were observed in northwestern Europe, where SSA influences extend approximately 400 km inland (Chen et al., 2016).
Additionally, the simulated changes in particulate Cl− concentrations due to SSA (BASE minus NOSA) are shown in Figs. S3 and S4. The spatial distributions of SSA-induced Cl− near the surface mirrors that of Na+ (Fig. 1). However, due to the higher composition of particulate Cl− than Na+ in SSA emissions, regions experiencing > 80 % change in Cl− are more extensive, underlining its substantial regional impact. Notably, in cities like Beijing and Guangzhou, Cl− concentrations are higher aloft than at the surface, a distinction more pronounced than for Na+. This is likely due to the higher reactivity of particulate Cl−. In a polluted lower atmosphere, particulate Cl− in SSA can be chemically depleted through thermodynamic equilibrium processes and heterogeneous reactions, which will be discussed in the following section.
3.2 Heterogeneous reactions of particulate Cl− with nitrogen-containing gases
Particulate Cl−, a chemically active and abundant component of SSA, undergoes heterogeneous reactions with NO2, NO3, and N2O5, releasing Cl radicals in the process. Figure 2 shows the influence of these reactions on particulate Cl− concentrations, revealing significant negative impacts along coastal regions. This suggests that SSA from the ocean mixes with nitrogen-containing gases from continental sources, leading to enhanced chlorine depletion in these areas. Seasonally, the greatest depletion occurs in January, followed by October, April, and July, likely due to variations in NO2 levels. In January, a notable depletion along the eastern Chinese coastline is observed, with significant reductions in Bohai Bay, the Yangtze River Delta (YRD) region, and the PRD region during April and October. In July, pronounced depletion is evident in Bohai Bay and YRD, while the PRD region shows less impact. Depletion diminishes progressively inland, with coastal areas experiencing the most significant effects.

Figure 2Changes in the contributions of heterogeneous reactions to the simulated monthly mean concentrations of particulate Cl− near the surface caused by SSA (BASE minus NOSA) during (a) January, (b) April, (c) July, and (d) October 2015. Heterogeneous reactions include reactions of particulate Cl− with NO2, NO3, and N2O5.
Alongside the depletion of Cl−, NOx concentration decreases due to the heterogeneous reaction between Cl− and NO2, NO3, and N2O5 across eastern China. Figure 3 presents the seasonal changes in NOx mixing ratios caused by SSA, showing a substantial reduction, particularly in the coastal regions of eastern China, with the most significant decreases occurring in January and the least in July. The incorporation of SSA into the model results in a decrease in NOx mixing ratios by up to 3–5 ppbv (5 %–10 %) across different months. Given the critical role of NOx as an O3 precursor, these reductions could significantly influence O3 level, a topic that we will explore in detail in Sect. 3.5.

Figure 3Changes in simulated monthly mean NOx mixing ratios near the surface caused by SSA (BASE minus NOSA) during January, April, July, and October 2015. Panels (a) and (b) present the spatial distribution of changes and percentage changes, respectively.
The reactions of particulate Cl− with NO2 and N2O5 result in the production of ClNO and ClNO2, respectively, which are crucial precursors to Cl radicals. Figure 4a and b display the spatial variations in their mixing ratios induced by SSA, specifically analyzed at 05:00 LST due to the nocturnal accumulation of these compounds. The figures demonstrate that SSA significantly increases ClNO and ClNO2 levels across eastern China, particularly in coastal regions. The spatial and seasonal patterns of these increases align closely with reductions in Cl− (Fig. 2) and NOx (Fig. 3), highlighting the important impact of SSA on these heterogeneous reactions. The most substantial effects of SSA are observed in January, followed by October, April, and July. In January, pronounced increases in ClNO and ClNO2 levels are noted in southeastern coastal regions of eastern China. In April and October, significant increases are localized to Bohai Bay, YRD, and PRD. In July, increases remain high in Bohai Bay and YRD. The transport of SSA inland results in diminishing increases of ClNO and ClNO2 from the coastline inward. Quantitatively, ClNO mixing ratios increase by up to 1.0, 1.1, 1.1, 1.3 ppbv in January, April, July, and October, respectively. Over 80 % of the ClNO in coastal areas is sourced from SSA emissions, with some areas nearing 100 % contribution (Fig. S5a). For ClNO2, the maximum increases are 1.0, 0.8, 0.5, 0.8 ppbv in respective months, with a broader regional impact compared to ClNO (Fig. S5b). Southern China experiences a more pronounced impact from SSA compared to the northern part, with the influence markedly tapering off towards inland regions like Hubei, Chongqing, and Guizhou where contributions decrease to around 10 %.

Figure 4Spatial distribution of changes in simulated monthly mean concentrations of (a) ClNO and (b) ClNO2 at 05:00 LST, and (c) daily mean Cl radicals near the surface caused by SSA (BASE minus NOSA) during January, April, July, and October 2015.
The heterogeneous reactions between SSA and nitrogen-containing gases release Cl radicals as a result. Figure 4c shows the spatial distribution of SSA-induced Cl radical concentrations in different seasons. The increases in precursor compounds ClNO and ClNO2 during the nighttime enhance their photolysis after sunrise, which significantly boosts Cl radical concentrations. High increases are evident in January in the Taiwan Strait, reaching up to 2.9 × 104 molec. cm−3. The concentrations peak in April and July in the Bohai Sea, the Yellow Sea, and the Taiwan Strait, with the highest increase of 4.0 × 104 and 8.1 × 104 molec. cm−3, respectively. October also shows substantial increases in the Taiwan Strait and Bohai Bay. The coastal regions see Cl radical concentrations boosted by 0.2–2 × 104 molec. cm−3, indicating a strong link between coastal SSA emissions and increased Cl radicals. These regions experiencing elevated Cl radical levels correspond with areas showing increases in ClNO and ClNO2 mixing ratios (Fig. 4a and b). Notably, nearly 100 % of the Cl radicals in oceanic regions stem from SSA emissions, with over 40 % in eastern China attributed to the same source (Fig. S5c). The IRR process analysis module helps trace the main pathways driving this increase (Fig. S6), including ClNO photolysis, ClNO2 photolysis, reaction of ClO and NO, heterogeneous reaction of particulate Cl− with NO3, and other processes (including Cl2 photolysis, reaction of HCl and OH, and etc.). Daytime increases in Cl radicals are predominantly due to the photolysis of ClNO and ClNO2 following sunrise.
Furthermore, the impact of SSA on Cl radicals is observed not only at the surface but also vertically through the atmosphere. Figure 5 examines the vertical diurnal variations in SSA-induced Cl radical concentrations in Beijing, Shanghai, and Guangzhou. This analysis shows that SSA emissions significantly elevate Cl radical concentrations after sunrise, especially during the morning hours. These increases are more pronounced near the top of the planetary boundary layer shortly after sunrise, suggesting the impact of SSA on Cl radicals is more significant in upper levels than near the surface.

Figure 5Vertical diurnal variations of changes in simulated monthly mean concentrations of Cl radicals caused by SSA (BASE minus NOSA) in (a) Beijing, (b) Shanghai, and (c) Guangzhou during January, April, July, and October 2015. The black line is the simulated planetary boundary layer height.
It should be noted that besides heterogenous reactions with nitrogen-containing species, particulate Cl− in SSA can react with H2SO4 and HNO3 through thermodynamic equilibrium reactions, releasing gaseous HCl (Chi et al., 2015). HCl is another precursor of Cl radicals via its reaction with OH radicals, which generally occurs during daytime (Finlayson-Pitts, 2003). However, as shown in Fig. S6, the contribution of HCl to Cl radicals is much lower than the photolysis of ClNO and ClNO2. Such small contributions of HCl were also reported in a box-model study of the North China Plain (Liu et al., 2017). It suggests the limited role of these thermodynamic equilibrium reactions in the Cl radicals and the following O3 formation.
3.3 Radiative effect of SSA
SSA plays a significant role in modulating incoming solar radiation through scattering, which influences the photolysis rates of various photochemical species. As O3 formation is closely linked to the photolysis of NO2 (J(NO2)), examining the impact of SSA on this process is crucial. Figure 6 highlights that the J(NO2) decreases by up to 15.1 %, 5.7 %, 6.0 %, and 11.8 % in January, April, July, and October, respectively, particularly in oceanic and coastal areas. This reduction in J(NO2) correlates well with the spatial distributions of SSA emission (Fig. S2) and SSA-induced Na+ concentration, underscoring the significant radiative effect of SSA. Despite relatively modest reductions in coastal regions (1 %–5 %), such changes are significant enough to influence O3 formation considerably. According to a study by Fan and Li (2022), similar decreases in photolysis rate (1 %–4 %) caused by SSA led to reductions in O3 mixing ratios by up to 1 %–2 % in eastern China during July.

Figure 6Changes in simulated monthly mean photolysis rate of NO2 (J(NO2)) induced by SSA (BASE minus NOSA) during January, April, July, and October 2015. Panels (a) and (b) present the spatial distribution of changes and percentage changes at 12:00 LST, respectively. Panels (c)–(e) display the vertical diurnal variations of changes in Beijing, Shanghai, and Guangzhou, respectively. The black line in panels (c)–(e) is the simulated planetary boundary layer height.
Additionally, the photolysis rates of photochemical gases generally increase with altitude due to the rising actinic flux (Gao et al., 2020). Figure 6 also presents the vertical diurnal variations in J(NO2) changes caused by SSA in Beijing, Shanghai, and Guangzhou. The influence of SSA on J(NO2) is notably lesser in Beijing compared to the other two cities. A significant reduction in J(NO2) is observed around noon (12:00 LST), coinciding with the daily peak in actinic flux. We note that the extinction effect of SSA can extend into the upper levels (2–3 km), where the decrease in J(NO2) can be the same degree as those observed near the surface. This is because the aerosol extinction effect depends on particle size distribution. Fine particles have a higher extinction effect than coarse ones (Molnár and Mészáros, 2001), and they can be transported to higher levels.
The reduction in radiation due to SSA not only impacts J(NO2) but also affects the photolysis rate of other photochemical species, including J(O3) (Figs. S7 and S8), which is crucial for OH radical production in the atmosphere. The spatial and seasonal distribution patterns of J(O3) reductions mirror those of J(NO2), highlighting a consistent influence across photochemical species. These changes are poised to affect the photochemical formation of OH and O3, the implications of which will be explored in subsequent sections.
3.4 Impacts of SSA on HOx radical
The Cl radicals released from SSA contribute to atmospheric oxidation similarly to OH radicals, catalyzing the conversion of VOCs into HO2 radicals. Figure 7a and b illustrate the spatial distribution of the SSA-induced increases in HO2 radicals near the ground across eastern China and adjacent oceanic areas, corresponding with the significant rise in Cl radicals. This increase is primarily due to the enhanced VOC degradation by Cl radicals. In remote oceanic regions, where VOC concentration is generally low, a decrease in HO2 can be observed. This decrease is mainly attributed to the reduced photolysis rates due to the extinction effect of SSA, which seems to have countered any increases in HO2 that would be caused by additionally available Cl radicals (Fig. 4c).
Figure 7c, d, and e present the vertical diurnal variations of SSA-induced HO2 concentrations in different months. Notably, HO2 concentrations significantly increase after sunrise, driven by Cl radicals generated from the photolysis of ClNO and ClNO2. However, a reduction in HO2 is observed around noon, particularly at altitudes above the boundary layer, attributed to the pronounced radiative effect of SSA. In October, unlike other months, there is an increase in HO2 concentration over the boundary layer in Beijing, suggesting a reduced radiative effect of SSA during this period in northern inland regions. Moreover, a more substantial chemical contribution from Cl radicals in October leads to a sustained increase in HO2 levels over the boundary layer.
In the presence of NO, HO2 converts into OH radicals, forming a critical HOx chemical cycle. Figure 8a and b show the spatial distribution of SSA-induced OH radicals near the ground, showing similar spatial and seasonal patterns to those of HO2, which is especially prominent in the North China Plain, Bohai Bay, and the YRD. However, in southern China, the area showing a decrease in OH is more extensive than that for HO2, stretching from oceanic regions to inland areas.
Figure 8 also shows the vertical diurnal variations of SSA-induced OH concentrations in different months. The radiation effect distinctly influences OH concentrations, particularly in southern coastal cities. For instance, in July, the increase in OH concentration during the early morning is significantly offset by a noon decrease due to the radiation effect of SSA, resulting in an overall reduction in OH levels.
We employed the IRR process analysis module to elucidate the primary mechanisms driving the increase in OH radicals caused by SSA (Fig. 9). The production of OH is facilitated by several processes, including HO2 conversion, O3 photolysis, HONO photolysis, ozonolysis of some VOCs, and others such as H2O2 photolysis. Among these, HO2 conversion accounts for over 70 % of total OH generation, followed by O3 and HONO photolysis. In Guangzhou, a southern coastal city, the contribution from O3 photolysis to OH production is notably higher than that in other regions, likely due to the lower latitude with higher radiation levels. During the morning, the increase in OH is driven by enhanced HO2 conversion caused by SSA. While in Guangzhou, the afternoon sees a decrease in HO2 conversions, which can be attributed to the decreased HO2 concentrations (Fig. 7e). Additionally, the reduced O3 photolysis, exacerbated by SSA's enhanced radiative effects and an overall reduction in O3 concentrations due to decreased NOx levels in a NOx-limited regime (see Sect. 3.5), further decreases OH production.

Figure 9Contribution of different pathways to the OH production near the surface and its changes caused by SSA (BASE minus NOSA) in (a) Beijing, (b) Shanghai, and (c) Guangzhou during January, April, July, and October 2015. These pathways include HO2 conversion (HO2), O3 photolysis (O1D), HONO photolysis (HONO), ozonolysis of some VOCs (OZLY), and others (OTHR, including H2O2 photolysis, etc.).
3.5 Impacts of SSA on O3
Figure 10 illustrates the spatial distribution of changes in the maximum daily average 8 h (MDA8) O3 mixing ratio near the ground after incorporating SSA emissions into the model. In January, there is a notable increase in O3 mixing ratios across eastern China and surrounding oceanic areas, peaking at 6.3 ppbv. In April, the North China Plain, Bohai Bay, and the Yellow Sea see increases up to 3.6 ppbv, while decreases up to 2.2 ppbv in southern China, South China Sea, and East China Sea. By July, increased O3 levels are confined to smaller areas like Bohai Bay and the Yellow Sea, with a maximum rise of 3.6 ppbv, whereas decreases up to 1.8 ppbv are observed in the eastern coastal and oceanic regions of China. The variations of O3 mixing ratios in October range from decreases of 2.8 ppbv to increases of 3.7 ppbv, showing similar patterns to April. We hypothesize that the regional and seasonal variations in O3 largely depend on O3 formation regime.

Figure 10Changes in the simulated monthly mean mixing ratio of MDA8 O3 induced by SSA (BASE minus NOSA) and daytime O3 formation regime during January, April, July, and October 2015. Panels (a) and (b) present the spatial distribution of changes and percentage changes, respectively. Panels (c) display the spatial distribution of the daytime (08:00–20:00 LST) O3 formation regime. The regime is estimated by the ratio of the production rates of H2O2 to HNO3 (). VOC-limited region: < 0.06; NOx-limited region: ≥ 0.2, and transition zone: 0.06 ≤ < 0.2. The production rates of H2O2 and HNO3 are calculated using the integrated reaction rate (IRR) diagnose tool in the CMAQ model.
To determine the O3 formation regime, we analyzed the ratio of production rates between hydrogen peroxide (H2O2) and HNO3 (Fig. 10c), using thresholds established in previous studies (Tonnesen and Dennis, 2000; Gaubert et al., 2021; Liu et al., 2021). A ratio below 0.06 indicates a VOC-limited region; ratios of 0.06 to less than 0.2 signify a transition zone; and ratios of 0.2 or higher indicate a NOx-limited region. Our results indicate that areas exhibiting increased MDA8 O3 are primarily within VOC-limited regions, while decreases predominantly occur in NOx-limited regions. In high NOx environments, the reaction between particulate Cl− from SSA and NOx leads to the formation of more Cl radicals, which can either reduce NO titration to O3 or enhance O3 production through interactions with VOCs. In contrast, in low NOx conditions, the reactions between particulate Cl− and NOx consume NOx, resulting in lower O3 levels. However, deviations from these patterns occur. For example, significant decreases in O3 are observed in the PRD region during April, July, and October, and in most of the regions in continental eastern China during summer, which are typically characterized as VOCs-limited. This phenomenon is likely due to SSA-induced reductions in NO2 photolysis rates overshadowing potential increases in O3 levels.
Figure 11 shows the vertical diurnal variations in SSA-induced O3 concentrations in Beijing, Shanghai, and Guangzhou. Morning increases within the planetary boundary layer across these cities are attributed to enhanced VOCs oxidation by SSA-induced Cl radicals, promoting the formation of RO2 and HO2 radicals that react with NO to generate NO2, thereby increasing O3 production. Moreover, the variations in other time frames largely reflect the interplay between heterogeneous reactions and radiative effects. In January, the prevailing reduction in NOx within VOCs-limited areas elevates OH and O3 levels in all three cities. April and October show similar patterns in Beijing and Shanghai, while Guangzhou exhibits declines due to the NOx reduction in a NOx-limited environment coupled with decreased photolysis rates. In July, only in Beijing do O3 levels rise during the morning hours, with reductions noted elsewhere, driven by NOx decreases in NOx-limited conditions and reduced photolysis.

Figure 11Vertical diurnal variations of changes in simulated monthly mean O3 mixing ratios caused by SSA (BASE minus NOSA) in (a) Beijing, (b) Shanghai, and (c) Guangzhou during January, April, July, and October 2015. The black line is the simulated planetary boundary layer height.
We also find significant decreases in SSA-induced O3 concentrations over oceanic regions (Fig. 10) and in the upper levels (Fig. 11). This decline can be explained by two reasons: for one thing, remote oceanic areas (Fig. 10c) and upper levels (Wang et al., 2025; Lin et al., 2022) are generally in NOx-limited conditions due to lower NOx concentrations, and the SSA-induced decrease in NOx (Fig. 3) reduce O3 formation; for another, in these areas with scant VOCs, SSA-induced Cl radicals preferentially react with O3 to form ClO (as depicted in Figs. S9 and S10), which enhances O3 depletions. This behavior mirrors stratospheric conditions where Cl radicals are pivotal in consuming O3.
Our analysis indicates that while SSA can suppress daytime O3 and HOx levels through reduced photolysis rates, it also contributes to their morning production via the release of Cl radicals through heterogeneous reactions. Additionally, the interactions of SSA with nitrogen-containing species modulate NOx levels, affecting O3 variations according to the prevailing formation regime, leading to regional and seasonal discrepancies in O3 responses. The findings of this study contrast with previous modeling studies (Knipping and Dabdub, 2003; Dai et al., 2020; Sarwar and Bhave, 2007), which primarily reported increases in O3 attributable to SSA, highlighting the complex and variable impacts of SSA on coastal atmospheric chemistry.
In this study, we utilized the WRF-CMAQ model to comprehensively investigate the complex interactions between SSA and continental anthropogenic emissions affecting O3 formation in Eastern China. Figure 12 illustrates the mechanisms by which SSA influences radicals and O3 formation in coastal areas. The process begins with the emission of SSA over oceanic areas. In addition to its horizontal transport from the ocean to inland areas near surfaces, SSA is also transported extensively over continental regions through long-range transport above the planetary boundary layer. Once inland, SSA interacts with pollutants from both continental anthropogenic and natural sources. Three primary pathways are identified by which SSA impacts radicals and O3 formations: (1) SSA scatters solar radiation, reducing the photolysis rates of atmospheric chemicals and suppressing the daytime formation of O3 and subsequently OH radicals. (2) Heterogeneous reactions between particulate Cl− in SSA and nitrogen-containing species (NO2 and N2O5) produce ClNO and ClNO2, which are key precursors of Cl radicals. These SSA-induced Cl radicals oxidize VOCs and produce more OH, enhancing atmospheric oxidation capacity and O3 production during morning hours. (3) These reactions also reduce NOx concentrations, an essential O3 precursor. The resultant O3 changes depend on its formation regime, subsequently influencing OH variations.
In summary, the influence of SSA on photochemical O3 formation via the combination of these three pathways is both complex and variable, changing with regions and seasons. In winter, SSA notably increases OH and O3 levels in eastern China due to significant NOx reductions in VOC-limited areas. In contrast, in spring and autumn, while similar increases are found in the North China Plain, southern China experiences decreases due to NOx reductions in NOx-limited areas and reduced photolysis rates. In summer, O3 increases are confined to areas around Bohai Bay, with reductions noted in other regions driven by NOx reductions in NOx-limited areas and decreased photolysis.
This study suggests that as global efforts intensify to control anthropogenic emissions, the natural contributions from sources like SSA are likely to play an increasingly significant role in regional air quality and climate dynamics. This underscores the necessity for atmospheric chemistry models to integrate the diverse and seasonally varying impacts of natural aerosols like SSA to improve predictions of air quality and to devise more effective environmental management strategies. This integration is crucial for accurately assessing future air quality trends and making informed policy decisions in the face of changing global emissions patterns.
The code or data used in this study are available upon request from Yiming Liu (liuym88@mail.sysu.edu.cn) and Yingying Hong (yyhong0809@foxmail.com).
The supplement related to this article is available online at https://doi.org/10.5194/acp-25-11847-2025-supplement.
QF and YML initiated the research. YML and YYH designed the research framework. YML conducted model simulations and drew the figures. YML and YYH analyzed the results and wrote the paper with input from all authors. All authors contributed to the discussion and improvement of the paper.
The contact author has declared that none of the authors has any competing interests.
Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. While Copernicus Publications makes every effort to include appropriate place names, the final responsibility lies with the authors. Regarding the maps used in this paper, please note that Figs. 1–4, 6–8, and 10 contain disputed territories.
The authors would like to thank the MEIC team from Tsinghua University for providing the anthropogenic emissions for this modeling study and acknowledge the computational support from the National Supercomputer Center in Guangzhou (Tianhe-2).
This research has been supported by the National Key Research and Development Program of China (grant no. 2023YFC3710900), Guangdong–Hong Kong–Macao Greater Bay Area Meteorological Technology Collaborative Research Project (project no. GHMA2025Z02), the Key Innovation Team of Guangdong Meteorological Bureau (grant no. GRMCTD202506-ZD06), the National Natural Science Foundation of China (grant nos. 42105097, 42375182, 91544102), the Science and Technology Program of Guangdong Province (Science and Technology Innovation Platform Category) (grant no. 2019B121201002), the Guangdong Basic and Applied Basic Research Foundation (grant no. 2023A1515010162), and the Guangdong Meteorological Bureau project (project no. GRMC2024M07).
This paper was edited by Armin Sorooshian and reviewed by two anonymous referees.
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