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Advances in Meteorology
Volume 2012 (2012), Article ID 140932, 18 pages
Examining the Impact of Nitrous Acid Chemistry on Ozone and PM over the Pearl River Delta Region
1Department of Mathematics, The Hong Kong University of Science & Technology, Clear Water Bay, Kowloon, Hong Kong
2Atmospheric Modeling and Analysis Division, National Exposure Research Laboratory, Office of Research and Development, US Environmental Protection Agency, RTP, NC 27711, USA
3Division of Environment, The Hong Kong University of Science & Technology, Clear Water Bay, Kowloon, Hong Kong
4College of Environmental Sciences and Engineering, Peking University, Beijing 100871, China
Received 16 February 2012; Accepted 3 April 2012
Academic Editor: Tareq Hussein
Copyright © 2012 Rui Zhang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
The impact of nitrous acid (HONO) chemistry on regional ozone and particulate matter in Pearl River Delta region was investigated using the community multiscale air quality (CMAQ) modeling system and the CB05 mechanism. Model simulations were conducted for a ten-day period in October 2004. Compared with available observed data, the model performance for NOx, SO2, PM10, and sulfate is reasonably good; however, predictions of HONO are an order of magnitude lower than observed data. The CB05 mechanism contains several homogenous reactions related to HONO. To improve the model performance for HONO, direct emissions, two heterogeneous reactions, and two surface photolysis reactions were incorporated into the model. The inclusion of the additional formation pathways significantly improved simulated HONO compared with observed data. The addition of HONO sources enhances daily maximum 8-hour ozone by up to 6 ppbV (8%) and daily mean PM2.5 by up to 17 ug/m3 (12%). They also affected ozone control strategy in Pearl River Delta region.
The importance of nitrous acid (HONO) to tropospheric chemistry is well recognized due to its contribution to HOx (OH + HO2) budget, which may lead to the enhancement of overall oxidation capacity of the atmosphere [1–10]. Accumulated HONO at night would undergo photolysis after sunrise to become an important source of hydroxyl radical (OH). It is especially important in the early morning when other major OH sources are still small.
Analysis of measured HONO in urban area of Europe suggested that reaction contributes more than 30% of the integrated photolytic HOx formation [6, 7]. Some recent studies even suggested its significance through the entire day especially over the remote environment [9, 11–13]. Box model studies by considering the importance of HONO photolysis to HOx budget also demonstrated its impact on O3 buildup [1, 2].
Despite the importance of HONO to tropospheric chemistry, the detail formation mechanisms, especially during daytime, have not been well established yet and incorporated into air quality models. There exist some review papers [14–16] to summarize the current knowledge on HONO formation mechanisms. Normally, four groups of HONO formation pathways were indentified: direct emission, homogeneous reactions, heterogeneous reactions, and surface photolysis reactions.
HONO can be directly emitted into the atmosphere via combustion process (e.g., vehicle exhaust) when temperature of produced NO (from nitrogen thermal fixation) is decreased . Measurements of HONO emission from combustion system are mainly focused on motor vehicles, especially diesel vehicles. HONO/NOx emission ratio from different engines was reported on average to be 0.3~0.8% [19–21]. Direct HONO emission source can possibly play an important role over heavily polluted areas with high traffic volume.
The most important homogeneous reaction that produces HONO is the reverse reaction of : This reaction has a greater role during daytime when the mixing ratios of OH and NO are high, and little contribution to the HONO was built up at night. The excited NO2 (NO2E) chemistry is another homogenous reaction that can produce HONO in urban areas [22–26]: Also, carbon bond 2005 (CB05) chemical mechanism  contains the following homogenous reactions which are considered small impacts to HONO formation: Recently, the photolysis of aromatic compounds containing the ortho-nitrophenol was proposed as a new gas-phase source of HONO, which would partially help to explain the high contribution of HONO to oxidation capacity in urban atmosphere environment .
Most chamber studies indicated the importance of HONO production through the heterogeneous conversion of NO2 absorbed on the available surfaces in the presence of water vapor [14, 29]: The heterogeneous nature of those reactions was shown by the enhanced conversion frequency with the increase of S/V ratio and the strong dependence on surface properties [30–32]. HONO heterogeneous production can also appear either on soot or on semiorganic surface [33, 34]: However, the surface deactivation occurs on soot within a few minutes, and consequently, it is not an important pathway for HONO [35, 36]. In regards to the reaction on semiorganic surface, even though the potential to HONO production is relatively high , the parameterization method is still open to discuss. Besides those, the renoxification of HNO3 on surfaces was also believed to be important for HONO formation within the boundary layer of polluted atmosphere [37, 38]:
With the involvement of solar radiation, two surface photolysis reactions are believed to be important for daytime HONO formation. One is the photosensitized reduction of NO2 on organic surface [39, 40]: where is the reduced photosensitizer in aromatic hydrocarbons or humid acids. The other one is the photolysis of absorbed nitric acid (HNO3) deposited on the ground [41, 42]: Recently, the enhancement of NO2 to HONO conversion on soot particles with the presence of artificial solar radiation was also proposed as a potential pathway for HONO formation .
There are already some modeling attempts to test the impact of different HONO formation pathways to photochemistry using either box model [17, 44] or 3D air quality model [18, 45–47]. For example, Aumont et al.  demonstrated the importance of direct emission and heterogeneous reactions to HONO enhancement under polluted condition using two-layer box model. Vogel et al.  suggested that reaction and emission were the most important sources of night time HONO production using a one-dimensional air quality model. Lei et al.  reported that reaction enhanced daytime OH and subsequently increased daytime O3 by 4–12 ppbV by using a 3D chemical transport model in Houston. Sarwar et al.  incorporated reaction , , and direct HONO emission into CMAQ model and reproduced 60% observed HONO value at eastern US. Li et al.  pointed out that reaction and can significantly improve HOx simulations during daytime and the partition of NO/NO2 in the morning in Mexico using WRF-CHEM model. Gonçalves et al.  applied the WRF-CMAQ modeling system to quantify the contribution of HONO direct emission and reaction on predicted O3 and PM2.5 value. However, most of the studies were carried out over relatively clean area with moderate photochemical precursor level. Evaluating the impact of additional HONO sources to air quality over heavy-polluted areas such as Pearl River Delta region, China has important practical significance.
Measurements in PRD region indicate the presence of elevated ambient HONO levels not only in urban but also in rural areas. For example, early-morning HONO mixing ratio of up to 12 ppbV was measured at Guangzhou (GZ) in June 2000 . Mean noon value of about 4 ppbV at GZ was measured during the first Program of Regional Integrated Experiments on air quality over the PRD in October, 2004 (PRIDE-PRD2004 ). A nocturnal peak HONO mixing ratio of over 8 ppbV was reported in PRIDE-PRD2006 campaign [50, 51]. High nighttime HONO levels of up to 4 ppbV  occurred even at the rural site Xinken (XK), which is located at the western coast of Pearl River Estuary (PRE) (see Figure 1).
Observation based-model (OBM) also supported the importance of HONO chemistry to the PRD region especially during the episode days. Zhang et al.  used the observed HONO data at XK as input to GIT-OBM model and compared simulation results to those obtained with gas-phase HONO chemistry only. Two-to-four times increase of OH and ozone production rate were found both at GZ or XK site, which may suggest the importance of heterogeneous reactions of HONO to regional photochemical process. Lu et al.  employed the same model to investigate the importance of HONO during the PRIDE_PRD2006 campaign. It was suggested that it is one of the critical species for radical recycling and photochemical O3 production for the urban areas.
Currently, CMAQ model only considers homogeneous formation pathway for HONO; hence, it may underestimate HONO level by order of magnitude . The additional HONO sources can produce more OH and may improve model performance for O3 and PM. In this study, direct HONO emissions and four additional HONO formation pathways were incorporated into CMAQ model, and their effects on predicted HONO, O3, and PM were investigated over PRD region.
2.1. Model Description
CMAQ version 4.6  was used for this study. Modeling domain was shown in Figure 1 and consisted of grid cells with 4.5 kilometer grid spacing. The boundary conditions of the domain of interest were provided by the outer nesting domains and kept consistent for different case run. Twenty vertical layers were constructed in CMAQ with the first layer around 17 m above the ground and 11 vertical layers below 1 km. The CB05 gas-phase chemical mechanism  was used. The calculation of convective cloud mixing in the planetary boundary layer was represented by Asymmetric Convection Model . The aerosol process was represented by fourth-generation CMAQ aerosol module (AERO4), which includes SORGAM  as a secondary organic aerosol model, ISORROPIA  as an inorganic aerosol model, and RPM  as a regional particulate model. Boundary conditions for the model were generated from the CMAQ results of larger domain covering the southern China. Initial conditions for the model were chosen from default mixing ratio profiles and the first 3-day simulation was used as model spin-up.
The meteorological field for the CMAQ model was simulated by the Fifth-Generation National Center of Atmospheric Research/Pennsylvania State University (NCAR/PSU) Mesoscale Model (MM5) version 3.6.3  with updated land use information and four-dimensional data assimilation (FDDA). Detailed descriptions on model configuration and data preprocessing can be found in Yim et al. . Pervious comprehensive model performance evaluations by comparing the modeled pressure, ground temperature, wind speed, wind direction, and RH with available global telecommunication system observations had demonstrated that this set of MM5 simulation can represent the regional flow pattern reasonably well [60–62] and is suitable for driving chemical transport model for regional air quality study [63, 64].
2.2. Emissions for the Model
PRD local emission inventory developed by “bottom-up” methods was allocated into domain grids by Sparse Matrix Operator Kernel Emissions (SMOKE V2.1)  through spatial surrogate file, temporal profiles, and chemical speciation profiles . Due to lack of systematic work on local PM and VOC speciation profiles for different sources in China, the corresponding SPECIATE algorithm  was introduced to apportion VOC to CB05 species. Gridded biogenic emission was generated through SMOKE by using the Biogenic Emission Inventory System, version 2 (BEIS2) with emission factors and the land cover information provided by the Hong Kong Planning Department .
2.3. HONO Formation Pathways
The CB05 gas-phase chemical mechanism in CMAQ model contains known homogeneous reactions involving HONO except the excited NO2 chemistry and the photolysis of ortho-nitrophenols . Reaction is not included in this study since Sarwar et al.  reported that it contributes only a small amount to daytime HONO. CMAQ version 4.6 does not contain any direct HONO emissions from vehicles. In this study, direct HONO emissions are also included. Three groups of additional HONO formation pathways as described earlier were incorporated into CMAQ model. Compared to the similar study of Sarwar et al. , reactions and are the first time to incorporate into a 3D air quality model for quantifying the HONO impact on air quality modeling results.
Direct HONO emission over PRD region is estimated from on-road and off-road vehicle sources as a fraction of NOx vehicle emission; HONO/ NOx emission ratio is set to 0.008 based on the results reported by Kurtenbach et al. . Vehicle NOx emission was initially speciated into NO by 90% and NO2 by 10% (by volume). For this study, we modified the speciation of vehicle NOx emission into NO by 90%, NO2 by 9.2%, and HONO by 0.8%. Su et al.  reported an upper limit of 0.01 for [HONO]/[NOx] ratio in PRD, which is consistent with the value used in this study
Estimates of direct HONO and other emissions were developed using SMOKE . The spatial distribution as well as temporal profile of ground HONO emission rate is demonstrated in Figure 2. The general HONO distribution pattern matches with PRD road network, and the emission rate is scaled by total vehicle volume. Multiple hotspots with the average daily emission rate greater than 0.5 mol s−1 area−1 (area in this study is 4.5 km × 4.5 km) are found at GZ city and its vicinity area, Dongguan, Shenzhen city cluster, and Central in Hong Kong. The emission gradient between eastern and the western parts of PRE is noticeable. The diurnal variation of HONO emission rate closely follows the vehicle use pattern. Emission rates are relatively high during daytime (08:00–19:00 LST), then drop after the midnight (00:00 LST), and increase again around 07:00 LST with the start of morning rush hour.
Two heterogeneous reactions and were added to the CMAQ model. The first-order reaction constant is given as where is dimensionless reactive uptake coefficient. The for reaction is taken as  and for reaction is taken as ; is the mean thermal velocity of a given reactant and is calculated following Pleim and Xiu .
The estimation of S/V for heterogeneous reactions is a challenging task. Total S/V ratio for reaction includes model-resolved aerosol surface area and other available surface area at the first model layer:
Here, S/V for building is taken to represent surface areas provided by buildings, roads, parking lots, and other structures. Unless during heavily polluted days, the S/V ratio for aerosol is much smaller than corresponding S/V values for available surface on the ground . S/V ratio for vegetation can be represented by leaf area index (LAI) in the first model layer . The LAI values were multiplied by two to account for both sides of leaves into total reaction interface . The S/V ratio for soil is set to 0.1 m−1. Svensson et al.  studied the kinetics of the reaction involving NO2 and H2O and suggested an S/V value of 0.2 m−1 for typical urban environment. However, Cai  used a value of 1.0 m−1 to represent the high urban density environment in New York. In this study, the estimated S/V ratio for building at each grid is taken as proportional to the model-resolved urban fraction (PURB, with the range 10% to 100%, see Figure 1) and capped with an empirical upper limit . Over the very low urban density place with PURB less than 10%, S/V for building is a fixed value as 10% of : where is used for the base case following Sarwar et al. . Sensitivity study is also conducted to investigate the impact of alternative value of on predicted HONO. Values of S/V for building over water were set to zero. In the model, reaction can produce HONO on aerosol surfaces at all vertical levels, while it can only produce HONO in the first layer on ground surfaces.
Two surface photolysis pathways (reactions and ) for HONO formation are added into CMAQ to investigate the production of HONO during daytime. As regards to the photosensitized reduction of NO2 on humic acid coated aerosol (reaction ), HONO production is not linearly increased with the integrated actinic flux (photons·m−2 s−1, 300–750 nm) due to the quick deactivation process by reaction with photo-oxidants which are formed simultaneously during the irradiation of humic acid surfaces . In this study, the empirical first-order HONO formation model suggested by Stemmler et al.  is parameterized into CMAQ with the uptake coefficient : where mixing ratios of NO2 is in ppbV. Only the S/V ratio for soil is considered for reaction . In the model, HONO production from reaction is released in the first layer only.
HONO formation through photolysis of absorbed HNO3 on surfaces (reaction ) was incorporated into the model upon the empirical relationship derived from laboratory measurements  where is the fraction of deposited HNO3 exposure to full noontime sunlight with the photolysis rate . In this study, is set as 0.5. is dry deposition velocity of HNO3, [HNO3] is the mixing ratio in the first model layer, is accumulated time since the last precipitation event, and is the first layer model height (17 m) in CMAQ configuration. The model assumes that the wet deposition removes all absorbed HNO3 on the ground and resets it to zero for subsequent simulation. The photolysis rate of adsorbed HNO3 reported by Zhou et al.  is 24 times greater than the photolysis rate of gaseous HNO3; thus, it was taken as in the model, and HONO production from reaction is released in the first layer only.
2.4. General Synoptic Condition and Case Selection
The time period for HONO simulation over PRD region is chosen from 23 October, 2004 to 2 November, 2004, when the PRIDE-PRD2004 campaign was carried out. HONO measurements were conducted using rotated wet effluent diffusion denuder (WEDD) methods at two supersites: one at an urban area (GZ : 23.13°N, 113.26°E) and one at a rural area (XK : 22.61°N, 113.59°E) (Figure 1) . During the PRIDE-PRD2004 campaign period, the persistent surface high-pressure system (anticyclone), descent motion outside of hurricane, and frequent sea breeze result in high-level ground mixing ratio for gaseous and particulate pollutants . For instance, at XK supersite, at least two severe episodes were observed on October 25 and October 29 with measured daily peak O3 mixing ratio reaching over 150 ppbV and PM2.5 peak mixing ratio near or greater than 200 μg/m3 . Observed maximum HONO mixing ratio in XK was reported to be more than 4 ppbV in the nighttime and about 1 ppbV during the daytime .
A total of eleven simulation cases were performed to investigate the impact of additional HONO formation pathways on air quality modeling results over PRD region. Sensitivity runs were designed to understand the impacts of uncertainties of selected parameters on air quality. Selected significance test on HONO prediction using the previous proposed parameterization methods was carried out to discuss their robustness over PRD region simulation. The impact of HONO chemistry on O3 control strategy due to the VOC emission reduction was also evaluated. The case ID, case description, and designed purpose are summarized in Table 1.
3. Results and Discussion
3.1. Model Performance for Base Case CB05
Time series of predicted SO2, NOx, O3, and PM2.5, as well as aerosol sulfate and aerosol nitrate (case CB05, see Table 1) are compared to the measurements obtained from the Hong Kong Environmental Protection Department (HKEPD) for Yuen Long (YL) monitoring station (Figure 3). Model performance statistics for other locations (CW, TM, TW, TC, and YL) (see Figure 1) are summarized in Table 2. Generally, CMAQ model has skill to reproduce air pollutant mixing ratios, their trends, spatial gradient, and relative abundance. Relatively high indexes of agreement (IOA, ) were obtained for all species except aerosol nitrate (ANO3). Mean normalized bias (MNB) for SO2, NOx, O3, and aerosol sulfate (ASO4) are less than ±30%, which is taken as the acceptable level for model performance .
Predicted O3 mixing ratios agree reasonably well with observed data in terms of diurnal variation however, it sometimes cannot reproduce high observed afternoon O3 peaks due to the uncertainty of emission precursor (NOx and VOC) ratio estimation and UV calculation for photochemical reaction (Figure 3). Model tends to underestimate PM2.5 mass mixing ratios uniformly by 40~50%. This may be due to the underestimation of related PM emission rates and missrepresentation of particulate species in the model. Current CMAQ aerosol module  allocates all unspecified aerosol components into the category “PM_OTHER” and represents them as chemical inert. The modeled PM2.5 component has a large portion (25%~40%) of “PM_OTHER,” which may cause the underestimation of specific aerosol component. Modeling results are consistent with the work reported by Kwok et al. .
However, the CMAQ model has certain skill to represent sulfate formation pathways via gaseous-phase and aqueous-phase chemical reactions. The second pathway is especially important over PRD region due to high ambient RH and large fraction of cloud cover generally present throughout the year . Simulated ASO4 is reasonably good with IOA around 0.6 and MNB less than ±25%. The grossly underestimation of aerosol nitrate performance (IOA below 0.3 and MNB greater than −80%) may be due to the underestimation of nitrogen oxide emissions over PRD region and the lack of coarse-mode ANO3 formation in CMAQ 4.6 either through reaction between HNO3 and calcium carbonate or between gaseous HNO3 and NaCl . Ambient observed O3 and PM2.5 outside Hong Kong are not publicly available; thus, predicted mixing ratios cannot be compared with observed data. In summary, model performance statistics simulation is reasonably well, and the model is suitable for evaluating the impact of HONO chemistry over PRD region.
3.2. Model Evaluation at Xinken (XK) and Guangzhou (GZ)
During the PRIDE_PRD2004 campaign, HONO was measured at XK and GZ . XK measurement site is located at a rural area, while GZ measurements site is located at an urban area (Figure 1). The model evaluation after incorporation of different HONO chemistry at XK (first column) and GZ (second column) site for NO2, O3 and HONO is presented in Figure 4. Daytime (07:00–18:00 LST) as well as nighttime (19:00–06:00 LST) model average values were compared with corresponding observations. The modeled NO2 mixing ratios for different simulation cases (Table 1) during daytime are underestimated by 26% ~28% at XK while during nighttime were overestimated at XK by 21% ~26% (no observation for NO2 available at GZ). On the contrary, the modeled O3 mixing ratios are consistently underestimated at two sites, and the degree of underestimation was more severe during daytime (−34% at XK and −40% at GZ) than that during nighttime (−28% at XK and −10% at GZ). The reason for the underestimation of O3 peaks may be associated with the overestimation of NOx and missing of HONO chemistry in base case CMAQ run. However, the HONO chemistry does not have obvious improvement on the NO2 and O3 model performance at XK and GZ sites (pin-pointed with grid area 4.5 km × 4.5 km) during the campaign. However, in other places over PRD region, the HONO chemistry does have potential to enhance the simulated O3 peak value, which will be discussed in Section 3.6.
The modeled HONO mixing ratio increases by an order of magnitude after considering different HONO sources from direct emission, heterogeneous reactions and surface photolysis reactions. The simulation case CB05+EM+HT+SP can predict 40% and 36% of the observation values in XK (1.1 ppbV) and GZ (4.2 ppbV) site, while the values for base case CB05 are only 4% and 2%, respectively. Normalized mean bias (NMB) at XK is lower during nighttime (NMB%) than that during daytime (NMB), while at GZ site, the result is opposite (NMB% during nighttime and (NMB% during daytime). Verification for hourly HONO observations at XK site  shows that case CB05+EM+HT+SP can improve the model performance with the statistic metrics NMB from −95% to −54% and IOA from 0.35 to 0.56 compared with case CB05.
Predicted daytime average OH was 2.2 × 106 molec·cm−3 at XK for case CB05 (homogeneous reactions only) which increased to 2.3 × 106 molec·cm−3, molec·cm−3, molec·cm−3 for case CB05+EM, CB05+EM+HT, and case CB05+EM+HT+SP, respectively. Predicted daytime average OH was molec·cm−3 at GZ for case CB05 (homogeneous reactions only) which increased to 1.7 × 106 molec·cm−3, 1.8 × 106 molec·cm−3, 1.9 × 106 molec·cm−3 for case CB05+EM, CB05+EM+HT, and CB05+EM+HT+SP, respectively. Thus, the additional HONO sources increased daytime OH by 13.6% and 26.7% at XK and GZ, respectively. OH concentration was measured during PRD-PRIDE 2006 campaign at the upper wind of Guangzhou city ; the typical average daytime OH concentration in the similar is above molec·cm−3, which is a factor of two higher than the simulated OH value here in GZ. It may suggest that current MM5-CMAQ modeling system tends to underestimate overall oxidization capacity due to the large uncertainty in VOC emission estimation over PRD region .
3.3. Spatial Pattern of HONO Simulation
Spatial patterns of simulated HONO distributions during daytime (Figures 5(a)–5(d)) and nighttime (Figures 5(e)–5(h)) are presented in Figure 5 separately. The HONO fields for different cases in Figure 5 are the daily average of October 28 with the maximum ozone enhancement during the simulation period. The distribution patterns of simulated HONO for daytime and nighttime are generally consistent with the NOx emission pattern, which is due to the fact that HONO formation pathways are related to NO2. Remarkable contrast for predicted daytime and nighttime HONO mixing ratio exists in different simulation cases. Mean nighttime HONO mixing ratio is about twice that of daytime value. For case CB05+EM+HT, this night-to-day contrast is more pronounced. Over the GZ area, the mean daytime HONO mixing ratio is around 2 ppbV while the predicted nighttime value is above 5 ppbV.
The simulated HONO level from base case (case CB05) is low with the mean daytime value of less than 500 pptV and nighttime value of 800 pptV. The addition of HONO emission (case CB05+EM) increased predicted HONO by 2~3 times. The heterogeneous reactions (case CB05+EM+HT) and surface photolysis (case CB05+EM+HT+SP) further enhanced the modeled HONO level, which resulted in more than 8~10 times greater than homogenous reaction only. Surface photolysis contributes more to the HONO enhancement during daytime due to the available solar radiation (the difference between Figures 5(c) and 5(d)), whereas heterogeneous reactions play a more important role in HONO formation at nighttime (the difference between Figures 5(g) and 5(f) is as large as 200%). Results are consistent with those reported by Sarwar et al. .
3.4. Relative Contribution to HONO from Different Formation Pathways
The average diurnal relative contribution of the four HONO sources to predicted HONO concentration in XK and GZ site is shown in Figure 6. The relative contribution at each site is counted by subtracting the mean predicted value of different formation pathways (emission, heterogeneous reaction, and photolysis) to corresponding base case one at each hour. It can be found that the predicted nighttime HONO concentration is primarily controlled by heterogeneous reaction both at rural and urban sites (up to 89% in XK and 81% in GZ). During daytime, the contribution of surface photolysis increases with the increase of solar radiation. The maximum contribution can reach up to 64% in XK and 31% in GZ at the late afternoon. The relative contribution of direct HONO emission in rural site is greater at night and nearly negligible during the day due to very low traffic volume. The relative contribution of direct HONO emissions at urban site is relatively high (20–30%) with peak observed during morning and evening rush hour. The relatively high contribution from direct emission at GZ suggests the importance of accurately speciating NOx emission from vehicles (e.g., reaction ).
3.5. Sensitivity Study of Different HONO Simulation Cases
Three additional model simulations were conducted to investigate the sensitivity of different parameters on simulated HONO. The first parameter investigated is the NOx emission (from motor vehicle) speciation. For air quality modeling studies, NOx emissions are typically speciated into NO and NO2 by 90% and 10%, respectively (by volume). Long-term observation of NO2/NO ratio in Hong Kong from vehicle emission suggested that the traditional speciation for NOx emission may not be suitable for PRD area . Higher NO2 emission contribution may be due to the unique condition of mobile fleet composition and engine type usage in Hong Kong. Hence, a sensitivity run (case HONO_NOx) by using alternative NOx emissions speciation is designed. For this study, NOx was speciated into NO, NO2, and HONO by 85%, 13.8%, and 1.2%. In this sensitivity run, the impact of increased direct HONO emission on predicted HONO is investigated. The second parameter for the sensitivity runs is the available surface area for heterogeneous reaction (case HONO_S/V). In case of CB05+EM+HT+SP, [S/V] ratio for soil surface was set at 0.1 m−1, and the [S/V] for building surface in (3) was estimated using an m−1. For PRD region, especially along the PRE area, the urban density and average building height are much higher than that in US condition  and hence may provide more available interface for heterogeneous reaction. For this study, m−1 and [S/V]soil = 0.2 m−1 were used. The third parameter is the HONO deposition velocity (case HONO_DV). An alternative lower deposition velocity taken the value of NO2 was used as the surrogate in the model to increase the chance for surface HONO accumulation.
Figure 7 gives the diurnal pattern of simulated HONO at XK and GZ with different simulation cases. The mean observation diurnal variation with error bars over PRIDE-PRD2004 campaign is from Figure 3 of Zhang et al. . The diurnal variation of different simulation cases is the mean of each local hour HONO mixing ratio over the simulation window. The characteristic of HONO diurnal profile over PRD region with high peak at night and relatively low during morning is consistent with the observation worldwide [9, 11–13]. The adding of direct emission (case CB05+EM) contributed to the HONO morning peak at the rush hour 0700~0800 local standard time (LST). The adding of heterogeneous reaction (case CB05+EM+HT) mainly contributed to the late afternoon (17:00–22:00 LST) buildup of HONO concentration. The simulation case HONO_S/V nearly followed the observed HONO diurnal variation pattern at GZ, but in XK, it shows that the large overestimation occurred after sunset. However, the current implementation cannot repeat observed elevated HONO level late at night (02:00~06:00 LST); the model tends to have the steep jump after the peak near the midnight.
Simulated daytime and nighttime mean HONO mixing ratios at XK and GZ for different simulation cases are presented in Figure 8. Mean observed HONO at GZ at daytime is 4.17 ppbV, which is nearly four times greater than that at XK (1.12 ppbV). GZ site is located at an urban area, and NO2 mixing ratios are much greater than those at the rural XK site. Thus, observed HONO at GZ is much greater than that at XK. Homogenous reactions (case CB05) can only explain 5% or less of the observed HONO, whereas the heterogeneous reactions contribute more than 30% of observed value both in daytime and nighttime.
Compared with simulation case CB05+EM+HT+SP, HONO increases at GZ from sensitivity run HONO_DV, HONO_NOx, and HONO_S/V are 17%, 13%, and 157%, respectively; while at XK, the values are 37%, 9%, and 207%. The improvement at nighttime is better than that in daytime. Predicted HONO for HONO_S/V case agrees well both at GZ and XK at daytime but overestimates 60% during nighttime at XK. Results of sensitivity runs may suggest the importance of [S/V] value for simulating HONO chemistry. While the PRD region has relatively high urban density and greater building height, the value is not currently known. The model with predicts HONO levels closer to the observed data in PRD both in terms of mean and diurnal variation. The details of the HONO chemistry are still unknown. The use of currently known HONO reactions in air quality model does not reproduce observed HONO levels in PRD. Until the details of the HONO chemistry are known, this value can be used in the model for PRD. This is an empirical parameter that produces HONO closer to observed data in PRD and is not intended for other urban areas.
The production of HONO via heterogeneous reaction at ground using procedure described by Aumont et al.  (case HONO_G) was also tested. Consistent with the results reported, Sarwar et al.  predicted nighttime HONO was 30%–67% lower than the values obtained with CB05+EM+HT+SP and 66%–236% lower than the observed data.
The importance of HONO formation from heterogeneous reaction on semivolatile organics was also examined (case HONO_SOA) using the procedure of Li et al. . HONO production from diesel bound NOx emission at ground was parameterized as HONO source using the conversion factor of 0.023. The predicted daytime and nighttime mean HONO mixing ratios are 18%–33% higher than that of case CB05+EM+HT+SP but with larger variations (see Figure 8). However, the results were still 43%–57% and 19%–54% lower than corresponding observed data at nighttime and daytime, which suggests that the contribution of the semivolatile organics heterogeneous reaction to HONO formation may subject to high uncertainty and need to parameterize carefully in future.
3.6. Impact of HONO Chemistry on Ozone and PM
The spatial distribution of the largest enhancements of daily maximum 8-hour O3 and daily mean PM2.5 due to the additional HONO sources is presented in Figure 9. The largest enhancement occurred on October 28th with northeasterly moderate synoptic wind and relatively steady atmosphere . Daily maximum 8-hour O3 increased by up to 6 ppbV near the downwind of GZ city with simulated O3 level of 90 ppbV in base case run (case CB05). The impact on daily mean PM2.5 is relatively significant with the largest increase of nearly 17 g/m3 or 12% at GZ, the downwind of GZ, Shenzhen area, and northwest of Hong Kong. The impact of additional HONO sources on aerosol sulfate and secondary organic aerosols was small; however, the impact on ammonium and nitrate was relatively large (3.6 and 12.0 g/m3, resp.) which subsequently enhanced PM2.5. The additional OH from the photolysis of enhanced HONO reacts with NO2 and produces additional HNO3 which subsequently generates greater aerosol nitrate and ammonium.
The largest enhancement in morning O3 (8 am noon), daily maximum 8-hour O3, and daily mean PM2.5 in the modeling domain for each day is shown in Table 3. The largest enhancement in daily maximum 8-hour O3 ranged between 3 and 7 ppbV, while the largest enhancement in morning O3 ranged between 3 and 9 ppbV. Levels of the morning O3 increases are generally similar to those of daily maximum 8-hour O3. The accumulated HONO at night undergoes photolysis during the day and produces OH which drives the photochemistry and enhances O3. The largest enhancement in daily mean PM2.5 ranged between 4 and 17 g/m3. As mentioned earlier, ambient observed O3 and PM2.5 data in PRD region outside Hong Kong are not publicly available, and thus, increases in predicted mixing ratios cannot be compared with observed data.
The impact of additional HONO sources on O3 control strategy is also investigated. Urban areas of PRD are mostly VOC limited for O3 production ; thus, only response of 25% VOC emission reduction was investigated (cases 0.75 VOC and 0.75 VOC w/HONO). The relative response factor (RRF) is calculated to quantify the response of O3 under different chemical mechanisms. RRF is the average ratio of simulated O3 mixing ratio with and without reduced emissions. RRF at several cities over PRD with and without additional HONO sources is presented in Figure 10. Relatively high response was obtained in cities where intensive NOx and VOC emissions are present. The use of additional sources affected the RRF for many cities as shown in the figure. For example, predicted RRF without the additional HONO sources at FS was 0.87 (13% O3 decrease) due to the 25% VOC emission reduction. The inclusion of additional HONO sources changed the RRF to 0.85 or 15% O3 decrease due to the same VOC emission reduction (2% increase in O3 response). Impact on RRF at other cities was also similar. Thus, the use of additional HONO sources in the model affects the O3 control strategy.
This study investigated the contribution of HONO sources to the photochemistry over PRD using the MM5-SMOKE-CMAQ model system. In addition to the gas-phase reactions, additional heterogeneous and surface photolysis HONO formation pathways and direct emissions were incorporated into the model. 10-day ozone episode in October 2004 was chosen to simulate impact of different HONO sources to HONO formation and ozone and PM2.5 yields. The inclusion of additional sources improved HONO predictions significantly with HONO enhancement 8–10 times greater than homogenous reaction. The simulated HONO mean diurnal profiles were compared with observations at rural site XK and urban site GZ. The model can generally produce the daytime variation but cannot maintain the observed elevated HONO late at night. In terms of the relative contribution of different pathway to HONO formation, the weighting from homogenous reaction is no more than 10% both at urban and rural site, while the heterogeneous and daytime surface photolysis reactions can dominate 69%~83% contributions with comparable weightings. Direct emission contribution is more important at urban site than that in rural site. The inclusion of additional HONO sources enhanced daily maximum 8-hour O3 by up to 7 ppbV (8%) and daily average PM2.5 up to 17 g/m3 (12%) over the downwind area of GZ. The use of additional HONO sources also affected the O3 control strategy.
Results of sensitivity studies suggest that the parameterization of surface area for heterogeneous reactions is an important factor that can affect simulated HONO. However, surface area estimates needed for these heterogeneous reactions are not currently available; hence, implementations of these reactions in air quality models require simplifying assumptions. Thus, the details of these reactions (e.g., their dependence on types of surface, relative humidity, etc.) along with the estimates of available surface areas should be investigated in the future. The atmospheric chemistry community is actively investigating possible HONO sources and it is likely that additional HONO sources, will be identified in the future. When these additional HONO sources are known, the impact of HONO chemistry on air quality in PRD can be reevaluated.
This project was supported by HKUST Oversea Research Grant for PhD student, Grants from the Research Grant Council of Hong Kong (RGC612807, RGC615406), and NSFC/RGC Joint Research Scheme (N_HKUST630/04, N_HKUST631/05). Although this paper has been reviewed by EPA and approved for publication, it does not necessarily reflect EPA’s polices or views.
- G. W. Harris, W. P. L. Cater, A. M. Winer, J. N. Pitts, U. Platt, and D. Perner, “Observations of nitrous acid in the Los Angeles atmosphere and implications for predictions of ozone-precursor relationships,” Environmental Science Technology, vol. 16, no. 7, pp. 414–419, 1982.
- M. E. Jenkin, R. A. Cox, and D. J. Williams, “Laboratory studies of the kinetics of formation of nitrous acid from the thermal reaction of nitrogen dioxide and water vapour,” Atmospheric Environment, vol. 22, no. 3, pp. 487–498, 1988.
- A. M. Winer and H. W. Biermann, “Long pathlength differential optical absorption spectroscopy (Doas) measurements of gaseous HONO, NO2 and HCNO in the California South Coast Air Basin,” Research on Chemical Intermediates, vol. 20, no. 3–5, pp. 423–445, 1994.
- T. Staffelbach, A. Neftel, and L. W. Horowitz, “Photochemical oxidant formation over Southern Switzerland 2. Model results,” Journal of Geophysical Research D, vol. 102, no. 19, pp. 23363–23373, 1997.
- B. Alicke, U. Platt, and J. Stutz, “Impact of nitrous acid photolysis on the total hydroxyl radical budget during the Limitation of Oxidant Production/Pianura Padana Produzione di Ozono study in Milan,” Journal of Geophysical Research D, vol. 107, no. 22, article 8196, 2002.
- B. Alicke, A. Geyer, A. Hofzumahaus et al., “OH formation by HONO photolysis during the BERLIOZ experiment,” Journal of Geophysical Research D, vol. 108, article 8247, 17 pages, 2003.
- K. Acker, D. Möller, W. Wieprecht et al., “Strong daytime production of OH from HNO2 at a rural mountain site,” Geophysical Research Letters, vol. 33, Article ID L02809, 2006.
- Y. H. Zhang, H. Su, L. J. Zhong et al., “Regional ozone pollution and observation-based approach for analyzing ozone-precursor relationship during the PRIDE-PRD2004 campaign,” Atmospheric Environment, vol. 42, no. 25, pp. 6203–6218, 2008.
- Y. F. Elshorbany, R. Kurtenbach, P. Wiesen et al., “Oxidation capacity of the city air of Santiago, Chile,” Atmospheric Chemistry and Physics, vol. 9, no. 6, pp. 2257–2273, 2009.
- K. D. Lu, Y. H. Zhang, H. Su et al., “Regional ozone pollution and key controlling factors of photochemical ozone production in Pearl River Delta during summer time,” Science China Chemistry, vol. 53, no. 3, pp. 651–663, 2010.
- J. Kleffmann, T. Gavriloaiei, A. Hofzumahaus et al., “Daytime formation of nitrous acid: a major source of OH radicals in a forest,” Geophysical Research Letters, vol. 32, Article ID L05818, 4 pages, 2005.
- X. Ren, W. H. Brune, A. Oliger et al., “OH, HO2, and OH reactivity during the PMTACS-NY Whiteface Mountain 2002 campaign: obervations and model comparison,” Journal of Geophysical Research D, vol. 111, Article ID D10S03, 2006.
- J. Mao, X. Ren, S. Chen et al., “Atmospheric oxidation capacity in the summer of Houston 2006: comparison with summer measurements in other metropolitan studies,” Atmospheric Environment, vol. 44, no. 33, pp. 4107–4115, 2010.
- J. G. Calvert, G. Yarwood, and A. M. Dunker, “An evaluation of the mechanism of nitrous acid formation in the urban atmosphere,” Research on Chemical Intermediates, vol. 20, no. 3–5, pp. 463–502, 1994.
- G. Lammel and J. N. Cape, “Nitrous acid and nitrate in the atmosphere,” Chemical Society Reviews, vol. 25, pp. 361–369, 1996.
- J. Kleffmann, “Daytime sources of nitrous acid (HONO) in the atmospheric boundary layer,” ChemPhysChem, vol. 8, no. 8, pp. 1137–1144, 2007.
- B. Aumont, F. Chervier, and S. Laval, “Contribution of HONO sources to the NOx/HOx/O3 chemistry in the polluted boundary layer,” Atmospheric Environment, vol. 37, no. 4, pp. 487–498, 2003.
- G. Li, W. Lei, M. Zavala et al., “Impacts of HONO sources on the photochemistry in Mexico City during the MCMA-2006/MILAGO Campaign,” Atmospheric Chemistry and Physics, vol. 10, no. 14, pp. 6551–6567, 2010.
- C. Kessler and U. Platt, “Nitrous acid in polluted air masses-sources and formation pathways,” in Physico-Chemical Behaviour of Atmospheric Pollutants (Proceedings), B. Versino and G. Angeletti, Eds., pp. 412–422, Reidel, Dordrecht, The Netherlands, 1984.
- R. Kurtenbach, K. H. Becker, J. A. G. Gomes et al., “Investigations of emissions and heterogeneous formation of HONO in a road traffic tunnel,” Atmospheric Environment, vol. 35, no. 20, pp. 3385–3394, 2001.
- T. W. Kirchstetter, R. A. Harley, and D. Littlejohn, “Measurement of nitrous acid in motor vehicle exhaust,” Environmental Science & Technology, vol. 30, no. 9, pp. 2843–2849, 1996.
- S. Li, J. Matthews, and A. Sinha, “Atmospheric hydroxyl radical production from electronically excited NO2 and H2O,” Science, vol. 319, no. 5870, pp. 1657–1660, 2008.
- G. Sarwar, R. W. Pinder, K. W. Appel, R. Mathur, and A. G. Carlton, “Examination of the impact of photoexcited NO2 chemistry on regional air quality,” Atmospheric Environment, vol. 43, no. 40, pp. 6383–6387, 2009.
- J. N. Crowley and S. Carl, “OH formation in the photoexcitation of NO2 beyond the dissociation threshold in the presence of water vapor,” Journal of Physical Chemistry A, vol. 101, no. 23, pp. 4178–4184, 1997.
- S. Carr, D. E. Heard, and M. A. Blitz, “Comment on “atmospheric hydroxyl radical production from electronically excited NO2 and H2O”,” Science, vol. 324, no. 5925, p. 336, 2009.
- S. Li, J. Matthews, and A. Sinha, “Response to comment on ‘atmospheric hydroxyl radical production from electronically excited NO2 and H2O’,” Science, vol. 324, no. 5925, p. 336, 2009.
- G. Yarwood, S. Rao, M. Yocke, and G. Whitten, “Updates to the carbon bond chemical mechanism: CB05, final report to the U.S. EPA, RT-0400675,” 2005, http://www.camx.com/.
- I. Bejan, Y. Abd El Aal, I. Barnes et al., “The photolysis of ortho-nitrophenols: a new gas phase source of HONO,” Physical Chemistry Chemical Physics, vol. 8, no. 17, pp. 2028–2035, 2006.
- R. Svensson, E. Ljungstrom, and O. Lindqvist, “Kinetics of the reaction between nitrogen dioxide and water vapour,” Atmospheric Environment, vol. 21, no. 7, pp. 1529–1539, 1987.
- R. F. Graham and B. J. Tyler, “Formation of nitrous acid in a gas-phase stirred flow reactor,” Journal of the Chemical Society, Faraday Transactions 1, vol. 68, pp. 683–688, 1972.
- J. Kleffmann, K. H. Becker, and P. Wiesen, “Heterogeneous NO2 conversion processes on acid surfaces: possible atmospheric implications,” Atmospheric Environment, vol. 32, no. 16, pp. 2721–2729, 1998.
- B. J. Finlayson-Pitts, L. M. Wingen, A. L. Sumner, D. Syomin, and K. A. Ramazan, “The heterogeneous hydrolysis of NO2 in laboratory systems and in outdoor and indoor atmospheres: an integrated mechanism,” Physical Chemistry Chemical Physics, vol. 5, no. 2, pp. 223–242, 2003.
- M. Ammann, M. Kalberer, D. T. Jost et al., “Heterogeneous production of nitrous acid on soot in polluted air masses,” Nature, vol. 395, no. 6698, pp. 157–160, 1998.
- L. Gutzwiller, F. Arens, U. Baltensperger, H. W. Gäggeler, and M. Ammann, “Significance of semivolatile diesel exhaust organics for secondary HONO formation,” Environmental Science & Technology, vol. 36, no. 4, pp. 677–682, 2002.
- J. Kleffmann, K. H. Becker, M. Lackhoff, and P. Wiesen, “Heterogeneous conversion of NO2 on carbonaceous surfaces,” Physical Chemistry Chemical Physics, vol. 1, no. 24, pp. 5443–5450, 1999.
- F. Arens, L. Gutzwiller, U. Baltensperger, H. W. Gäggeler, and M. Ammann, “Heterogeneous reaction of NO2 on diesel soot particles,” Environmental Science & Technology, vol. 35, no. 11, pp. 2191–2199, 2001.
- A. M. Rivera-Figueroa, A. L. Sumner, and B. J. Finlayson-Pitts, “Laboratory studies of potential mechanisms of renoxification of tropospheric nitric acid,” Environmental Science & Technology, vol. 37, no. 3, pp. 548–554, 2003.
- E. M. Knipping and D. Dabdub, “Modeling surface-mediated renoxification of the atmosphere via reaction of gaseous nitric oxide with deposited nitric acid,” Atmospheric Environment, vol. 36, no. 36-37, pp. 5741–5748, 2002.
- K. Stemmler, M. Ammann, C. Donders, J. Kleffmann, and C. George, “Photosensitized reduction of nitrogen dioxide on humic acid as a source of nitrous acid,” Nature, vol. 440, no. 7081, pp. 195–198, 2006.
- K. Stemmler, M. Ndour, Y. Elshorbany et al., “Light induced conversion of nitrogen dioxide into nitrous acid on submicron humic acid aerosol,” Atmospheric Chemistry and Physics, vol. 7, no. 16, pp. 4237–4248, 2007.
- X. Zhou, K. Civerolo, H. Dai, G. Huang, J. J. Schwab, and K. L. Demerjian, “Summertime nitrous acid chemistry in the atmospheric boundary layer at a rural site in New York State,” Journal of Geophysical Research D, vol. 107, no. 21, article 4590, 2002.
- K. A. Ramazan, D. Syomin, and B. J. Finlayson-Pitts, “The photochemical production of HONO during the heterogeneous hydrolysis of NO2,” Physical Chemistry Chemical Physics, vol. 6, no. 14, pp. 3836–3843, 2004.
- M. E. Monge, B. D'Anna, L. Mazri et al., “Light changes the atmospheric reactivity of soot,” Proceedings of the National Academy of Sciences of the United States of America, vol. 107, no. 15, pp. 6605–6609, 2010.
- B. Vogel, H. Vogel, J. Kleffmann, and R. Kurtenbach, “Measured and simulated vertical profiles of nitrous acid—Part II. Model simulations and indications for a photolytic source,” Atmospheric Environment, vol. 37, no. 21, pp. 2957–2966, 2003.
- W. Lei, R. Zhang, X. Tie, and P. Hess, “Chemical characterization of ozone formation in the Houston-Galveston area: a chemical transport model study,” Journal of Geophysical Research D, vol. 109, Article ID D12301, 15 pages, 2004.
- G. Sarwar, S. J. Roselle, R. Mathur, W. Appel, R. L. Dennis, and B. Vogel, “A comparison of CMAQ HONO predictions with observations from the Northeast Oxidant and Particle Study,” Atmospheric Environment, vol. 42, no. 23, pp. 5760–5770, 2008.
- M. Gonçalves, D. Dabdub, W. L. Chang, F. Saiz, O. Jorba, and J. M. Baldasano, “The impact of different nitrous acid sources in the air quality levels of the lberian Peninsula,” Atmospheric Chemistry and Physics Discussion, vol. 10, pp. 28183–28230, 2010.
- M. Hu, F. M. Zhou, K. S. Shao, Y. H. Zhang, X. Y. Tang, and J. Slanina, “Diurnal variations of aerosol chemical compositions and related gaseous pollutants in Beijing and Guangzhou,” Journal of Environmental Science and Health A, vol. 37, no. 4, pp. 479–488, 2002.
- Y. H. Zhang, M. Hu, L. J. Zhong et al., “Regional integrated experiments on air quality over Pearl River Delta 2004 (PRIDE-PRD2004): overview,” Atmospheric Environment, vol. 42, no. 25, pp. 6157–6173, 2008.
- M. Qin, P. H. Xie, H. Su et al., “An observational study of the HONO-NO2 coupling at an urban site in Guangzhou City, South China,” Atmospheric Environment, vol. 43, no. 36, pp. 5731–5742, 2009.
- A. Hofzumahaus, F. Rohrer, K. Lu et al., “Amplified trace gas removal in the troposphere,” Science, vol. 324, no. 5935, pp. 1702–1704, 2009.
- H. Su, Y. F. Cheng, P. Cheng et al., “Observation of nighttime nitrous acid (HONO) formation at a non-urban site during PRIDE-PRD2004 in China,” Atmospheric Environment, vol. 42, no. 25, pp. 6219–6232, 2008.
- K. D. Lu, Y. H. Zhang, H. Su et al., “Oxidant (O3+ NO2) production processes and formation regimes in Beijing,” Journal of Geophysical Research D, vol. 115, Article ID D07303, 18 pages, 2010.
- D. Byun and K. L. Schere, “Review of the governing equations, computational algorithms, and other components of the models-3 Community Multiscale Air Quality (CMAQ) modeling system,” Applied Mechanics Reviews, vol. 59, no. 1–6, pp. 51–76, 2006.
- J. E. Pleim and J. S. Chang, “A non-local closure model for vertical mixing in the convective boundary layer,” Atmospheric Environment A, vol. 26, no. 6, pp. 965–981, 1992.
- B. Schell, I. J. Ackermann, H. Hass, F. S. Binkowski, and A. Ebel, “Modeling the formation of secondary organic aerosol within a comprehensive air quality model system,” Journal of Geophysical Research D, vol. 106, no. 22, pp. 28275–28293, 2001.
- A. Nenes, C. Pilinis, and S. N. Pandis, “ISORROPIA: a new thermodynamic equilibrium model for multiphase multicomponent inorganic aerosols,” Aquatic Geochemistry, vol. 4, no. 1, pp. 123–152, 1998.
- F. S. Binkowski and S. J. Roselle, “Models-3 Community Multiscale Air Quality (CMAQ) model aerosol component 1. Model description,” Journal of Geophysical Research D, vol. 108, no. 4183, 18 pages, 2003.
- G. A. Grell, J. Dudhia, and D. R. Stauffer, “A description of the fifth-generation Penn State/NCAR mesoscale model (MM5),” NCAR Technical Note NCAR/TN-398+STR, National Center for Atmospheric Research, Boulder, Colo, USA, 1994.
- S. H. L. Yim, J. C. H. Fung, A. K. H. Lau, and S. C. Kot, “Developing a high-resolution wind map for a complex terrain with a coupled MM5/CALMET system,” Journal of Geophysical Research D, vol. 112, no. 5, Article ID D05106, 2007.
- J. C. F. Lo, A. K. H. Lau, J. C. H. Fung, and F. Chen, “Investigation of enhanced cross-city transport and trapping of air pollutants by costal and urban land-sea breeze circulations,” Journal of Geophysical Research, vol. 111, Article ID D14104, 2006.
- X. Lu, K. C. Chow, T. Yao, J. C. H. Fung, and A. K. H. Lau, “Seasonal variation of the land-sea breeze circulation in the Pearl River Delta region,” Journal of Geophysical Research D, vol. 114, no. 17, Article ID D17112, 2009.
- J. P. Huang, J. C. H. Fung, and A. K. H. Lau, “Integrated processes analysis and systematic meteorological classification of ozone episodes in Hong Kong,” Journal of Geophysical Research D, vol. 111, Article ID D20309, 14 pages, 2006.
- R. H. F. Kwok, J. C. H. Fung, A. K. H. Lau, and J. S. Fu, “Numerical study on seasonal variations of gaseous pollutants and particulate matters in Hong Kong and Pearl River Delta region,” Journal of Geophysical Research D, vol. 115, Article ID D16308, 2010.
- M. R. Houyoux, J. M. Vukovich, C. J. Coats Jr., N. M. Wheeler, and P. S. Kasibhatla, “Emission inventory development and processing for the seasonal model for regional air quality (SMRAQ) project,” Journal of Geophysical Research D, vol. 105, no. 7, pp. 9079–9090, 2000.
- CH2M HILL (China) Limited, “Study of air quality in the Pearl River Delta region, technique report (Agreement No. CE 106/98) prepared for the Hong Kong Environmental Protection Department,” Hong Kong Administrative Region Government, 2011, http://www.epd.gov.hk/epd/english/environmentinhk/air/studyrpts/study_pearl.html.
- USEPA, “SPECIATE data base V3.1,” Research Triangle Park, NC, US, 2000, http://www.epa.gov/ttn/chief/software/speciate/speciate32.html.
- J. E. Pleim and A. Xiu, “Development and testing of a surface flux and planetary boundary layer model for application in mesoscale models,” Journal of Applied Meteorology, vol. 34, no. 1, pp. 16–32, 1995.
- M. R. Jones, Ammonia deposition to semi-natural vegetation [Ph.D. dissertation], University of Dundee, Scotland, UK, 2006.
- C. X. Cai, Implementation and performance evaluation on an air quality forecast modeling system (AQFMS) for northeastern USA [Ph.D. dissertation], Department of Earth and Atmospheric Science, University at Albany, State University of New York, Albany, NY, USA, 2005.
- X. L. Zhou, H. L. Gao, Y. He et al., “Nitric acid photolysis on surfaces in low-NOx environments: significant atmospheric implications,” Geophysical Research Letters, vol. 30, no. 2217, 4 pages, 2003.
- S. J. Fan, B. M. Wang, M. Tesche et al., “Meteorological conditions and structures of atmospheric boundary layer in October 2004 over Pearl River Delta area,” Atmospheric Environment, vol. 42, no. 25, pp. 6174–6186, 2008.
- C. J. Willmott, “On the validation of models,” Physical Geography, vol. 2, no. 2, pp. 184–194, 1981.
- USEPA, “Guidance on the use of models and other analyses in attainment demonstrations for the 8-hour ozone NAAQS,” EPA-454/R-99-004, U.S. Environmental Protection Agency, Research Triangle Park, NC, US, 1999.
- J. Z. Yu, X. F. Huang, J. Xu, and M. Hu, “When aerosol sulfate goes up, so does oxalate: implication for the formation mechanisms of oxalate,” Environmental Science & Technology, vol. 39, no. 1, pp. 128–133, 2005.
- J. Zheng, L. Zhang, W. Che, Z. Zheng, and S. Yin, “A highly resolved temporal and spatial air pollutant emission inventory for the Pearl River Delta region, China and its uncertainty assessment,” Atmospheric Environment, vol. 43, no. 32, pp. 5112–5122, 2009.
- HKEPD (Hong Kong Environmental Protection Department), “Guideline on modeling vehicle emissions,” July 2005, http://www.epd.gov.hk/epd/english/environmentinhk/air/guide_ref/files/EMFAC_HK_Guidelines_on_Modelling_Vehicle_Emissions_July2005.pdf.
- HKPD (Hong Kong Planning Department), “Hong Kong 2030: planning vision and strategy consultancy study to analyze broad land use pattern of the Pearl River Delta Region,” 2003, http://www.pland.gov.hk/pland_en/p_study/comp_s/hk2030/eng/consultants/pdf/Tpaper5.pdf.