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Article

Effects of Emission Variability on Atmospheric CO2 Concentrations in Mainland China

1
Aerospace Information Research Institute, Chinese Academy of Sciences, Beijing 100094, China
2
University of Chinese Academy of Sciences, Beijing 100049, China
3
College of Resources and Environment, University of Chinese Academy of Sciences, Beijing 101408, China
4
Innovation Center for FengYun Meteorological Satellite (FYSIC), Beijing 100081, China
5
Atmospheric Sciences Research Center, University at Albany, State University of New York, Albany, NY 12203, USA
*
Author to whom correspondence should be addressed.
Remote Sens. 2025, 17(5), 814; https://doi.org/10.3390/rs17050814
Submission received: 19 December 2024 / Revised: 13 February 2025 / Accepted: 14 February 2025 / Published: 26 February 2025
(This article belongs to the Section Atmospheric Remote Sensing)

Abstract

:
Accurately assessing the impact of anthropogenic carbon dioxide (CO2) emissions on CO2 concentrations is essential for understanding regional climate change, particularly in high-emission countries like China. This study employed the GEOS-Chem chemical transport model to simulate and compare the spatiotemporal distributions of XCO2 of three anthropogenic CO2 emission inventories in mainland China for the 2018–2020 period and analyzed the effects of emission variations on atmospheric CO2 concentrations. In eastern China, particularly in the Yangtze River Delta (YRD) and Beijing-Tianjin-Hebei (BTH) regions, column-averaged dry air mole fractions of CO2 (XCO2) can exceed 420 ppm during peak periods, with emissions from these areas contributing significantly to the national total. The simulation results were validated by comparing them with OCO-2 satellite observations and ground-based monitoring data, showing that more than 70% of the monitoring stations exhibited a correlation coefficient greater than 0.7 between simulated and observed data. The average bias relative to satellite observations was less than 1 ppm, with the Emissions Database for Global Atmospheric Research (EDGAR) showing the highest degree of agreement with both satellite and ground-based observations. During the study period, anthropogenic CO2 emissions resulted in an increase in XCO2 exceeding 10 ppm, particularly in the North China Plain and the YRD. In scenarios where emissions from either the BTH or YRD regions were reduced by 50%, a corresponding decrease of 1 ppm in XCO2 was observed in the study area and its surrounding regions. These findings underscore the critical role of emission control policies in mitigating the rise in atmospheric CO2 concentrations in densely populated and industrialized areas. This research elucidates the impacts of variations in anthropogenic emissions on the spatiotemporal distribution of atmospheric CO2 and emphasizes the need for improved accuracy of CO2 emission inventories.

1. Introduction

CO2, as one of the most significant greenhouse gases, plays a crucial role in Earth’s radiative balance and contributes to climate change. The global mean CO2 mole fraction reached 417.1 ± 0.1 parts per million (ppm) in 2022 [1]. The rising concentration of CO2 is a major driver of climate change, contributing to global temperature increases [2,3] and exacerbating the frequency and intensity of extreme weather events, including heatwaves, floods, and droughts [4]. Since the Industrial Revolution, the persistent increase in atmospheric CO2 levels has primarily been attributed to human activities such as fossil fuel combustion, industrial production, and land-use changes. The average annual anthropogenic flux of CO2 from fossil fuel emissions between 2013 and 2022 was 9.6 Gt C yr−1, with the total carbon emissions reaching 10.9 Gt C yr−1 [5]. Thus, reducing and controlling CO2 emissions is recognized as a global priority. China accounted for approximately 31% of global fossil fuel CO2 emissions in 2022 [5], establishing its role as a key contributor in global carbon emissions and climate change. Consequently, accurate quantification of China’s carbon emissions is essential to achieve global emission reduction targets and implement effective climate policies.
However, substantial uncertainties remain in carbon emission inventories. These uncertainties primarily stem from discrepancies in energy consumption statistics, emission factor estimates, land-use change data, and spatiotemporal inconsistencies in regional data [6,7,8,9]. Global CO2 emission estimates are accurate to within ±6.5%, while the range of uncertainties for country-level total CO2 emissions is between ±4% and ±35% [10]. Solazzo et al. reported that the uncertainty in anthropogenic emissions of the three main greenhouse gases—carbon dioxide (CO2), methane (CH4), and nitrous oxide (N2O)—in the EDGAR inventory ranged from 15% to 20% in 2015 [11]. Previous studies indicated that average uncertainties are below ±5% in developed countries [9,12], while in developing countries, uncertainties range from ±10% to ±50% [1,12,13,14,15]. As a developing country with a vast territory, China faces significant challenges in emission inventory accuracy due to substantial errors in activity-level statistics and substantial regional disparities in emission factors caused by uneven economic development [16]. These factors contribute to higher levels of uncertainty in emission inventories compared to developed nations. For China, reported anthropogenic emissions vary by over 10% across different statistical sources [16,17,18], primarily due to regional energy-use inconsistencies and the complexity of land-use changes. At sub-national scales, such as provinces, cities, or large point sources, accurately capturing CO2 emissions from fossil fuels and other anthropogenic sources is hindered by factors including economic competition and regional disparities in energy sourcing [19]. Given the scale and uncertainty of China’s carbon emissions, precise quantification of these emissions is crucial for developing effective reduction strategies.
Chemical transport models (CTMs) are essential tools that link emissions and concentrations. CTMs are widely used to improve the accuracy of CO2 flux estimates and refine model simulations by comparing model outputs with observational data. Common CTMs include the Goddard Earth Observing System 3-D chemical transport model (GEOS-Chem), the Weather Research and Forecasting (WRF) model coupled with Chemistry (WRF-Chem), and the Community Multiscale Air Quality (CMAQ) [20]. These models are driven by meteorological fields and incorporate atmospheric chemistry, physical processes, and various emission inventories to simulate the spatial and temporal variations in CO2 concentrations. Satellite observations offer distinct advantages for model evaluation and optimization. Satellites such as the Orbiting Carbon Observatory-2 (OCO-2) [21], Greenhouse Gases Observing Satellite (GOSAT) [22], and the Chinese Carbon Dioxide Observation Satellite (TanSat) [23] provide high spatiotemporal resolution global XCO2 data, helping to address the spatial coverage limitations of ground-based observations. For instance, OCO-2 captures XCO2 with spatial resolution better than 3 km, providing critical data for identifying localized emission hotspots in urban and industrial areas.
Additionally, ground-based observation networks such as the Total Carbon Column Observing Network (TCCON) [24] and Collaborative Carbon Column Observing Network (COCCON) [25] provide high-precision XCO2 measurements using infrared spectrometers, serving as essential benchmarks for validating model simulations. Comparative analyses of simulations and observations frequently reveal systematic biases between simulated and observed data [26,27,28,29]. These discrepancies may arise from inaccuracies in emission inventories, incomplete chemical mechanisms in models, or inaccuracies in atmospheric dynamics. Ma et al. [30] utilized the WRF-STILT atmospheric transport model to simulate CO2 concentrations in the Yangtze River Delta of China and performed Bayesian inversion using tower-based CO2 observations to estimate anthropogenic CO2 fluxes. Numerous studies have explored the impact of changes in prior carbon fluxes on simulated CO2 outcomes, indicating that alterations in oceanic carbon fluxes and biomass burning emission inventories can substantially affect CO2 concentration patterns [8,31,32]. Assimilation techniques, such as four-dimensional variational assimilation (4D-Var) [33] and Ensemble Kalman Filter (EnKF) [34,35], are employed to enhance the accuracy of emission inventories. This approach, which integrates observational data with models, provides critical insights into regional carbon emissions and the global carbon cycle. It also promotes improvements in emission inventories and strengthens the application of atmospheric chemistry models.
This study aims to quantitatively assess the impact of anthropogenic emission inventories and their uncertainties on the forward simulation of atmospheric CO2 concentrations. Anthropogenic CO2 emissions constitute a substantial portion of global carbon sources. This study conducted a consistency analysis between simulation results based on three different anthropogenic CO2 emission inventories and both satellite and ground-based observational data. The findings may serve as a reference for selecting emission inventories in forward simulations and inversions. Additionally, they provide information on the distribution of biases between CO2 simulation results and observational data, which can support the optimization process of these inventories in the inversion framework. To achieve this goal, we conducted nested simulations of CO2 concentrations over East Asia from 2018 to 2020 using the GEOS-Chem and three distinct anthropogenic CO2 emission inventories. Based on these simulations, we designed a series of numerical experiments to evaluate the impact of emission level variations. We evaluated the sensitivity of atmospheric CO2 concentrations to variations in anthropogenic emission fluxes using OCO-2 observations and ground-based measurements. The remainder of this paper is organized as follows: Section 2 details the models, data, and methodologies used in this study; Section 3 provides a comparative analysis of emission inventories and validates simulations against OCO-2, TCCON, and NOAA-ESRL ground observations. The conclusions and significance of this research are summarized in Section 4.

2. Materials and Methods

2.1. Model Description

The Goddard Earth Observing System 3-D chemical transport model (GEOS-Chem) is developed and maintained by the Goddard Earth Observing System (GEOS) of Global Modeling and Assimilation Office (GMAO). GEOS-Chem is capable of simulating atmospheric composition at both global and regional scales. The initial CO2 simulation in GEOS-Chem was introduced by Suntharalingam et al. [36], and significant updates were made later by Nassar et al. [37], particularly in terms of improving the sources of prior carbon fluxes.
A nested simulation of CO2 concentrations over the East Asian region was conducted from 1 January 2018 to 1 January 2021 using the GEOS-Chem model. The initial CO2 concentration fields were obtained from Carbon Tracker (CT2022). First, a global simulation was performed with a horizontal resolution of 2° latitude × 2.5° longitude and 47 vertical layers to simulate the global spatial and temporal distribution of CO2. The results of this global simulation were then used as boundary conditions for a nested simulation over the East Asian region at a finer resolution of 0.5° latitude × 0.625° longitude. The GEOS-Chem model is driven by meteorological data and emission flux data. In this study, the Modern-Era Retrospective analysis for Research and Applications (MERRA-2) was used for the meteorological inputs. The specific input CO2 flux data used in the simulations are detailed as follows, (1) The fossil fuel combustion emission inventories used in this study include three anthropogenic emission inventories: the Open-source Data Inventory for Anthropogenic CO2 (ODIAC) [38], the Multi-resolution Emission Inventory for China (MEIC) [39,40], and the Emissions Database for Global Atmospheric Research (EDGAR) [10]. (2) The biomass burning inventory is derived from the Global Fire Emissions Database, Version 4.1s (GFEDv4.1s) [41], with a spatial resolution of 0.25° × 0.25°. (3) Ocean exchange flux is scaled monthly ocean exchange with interannual variation [42], with a spatial resolution of 4° × 5°. (4) The balanced biosphere exchange flux is represented by the Simple Biosphere Model (SiB3) [43], with a temporal resolution of 3 h. The annual total of the balanced biosphere exchange flux is zero, but it is used to simulate the carbon cycle within a single day. (5) The net terrestrial exchange data are derived from the TransCom climatology dataset [44], representing a fixed terrestrial net ecosystem exchange flux. (6) Shipping and aviation emissions are provided by the Community Emissions Data System (CEDS) [45] and the Aviation Emissions Inventory Code (AEIC) [46,47].
This study focuses on anthropogenic CO2 emission inventories. Therefore, three major emission inventories were selected for the simulations: ODIAC, EDGAR, and MEIC. With all other input data and parameters kept constant, the anthropogenic CO2 emission inventory was substituted with one of the three inventories in each case, resulting in three corresponding CO2 spatiotemporal distribution simulation outcomes (hereafter referred to as sim_ODIAC, sim_EDGAR, and sim_MEIC). It was assumed that any differences in simulation results were solely due to variations in the anthropogenic emission inventories, enabling an analysis of the impact of anthropogenic emissions on simulated atmospheric CO2 concentrations. Additionally, a “no_fossil” experiment was conducted in which fossil fuel emissions were completely turned off in the model setup. The differences between the “no_fossil” experiment and other simulations were attributed exclusively to anthropogenic emissions during the study period [7,48]. Based on this setup, a series of numerical experiments were further conducted by adjusting the initial emission amounts proportionally.

2.2. Emissions

This study utilized three widely used anthropogenic CO2 emission inventories, namely, ODIAC, MEIC, and EDGAR, to investigate their impact on CO2 simulations. These three inventories were consistently adjusted to 1° × 1° monthly emission datasets for use as input data for the model.

2.2.1. ODIAC

ODIAC is a global, high-resolution CO2 emission dataset developed by the National Institute for Environmental Studies (NIES). This study utilized the ODIAC2022 dataset at a 1° × 1° monthly resolution [49]. The ODIAC dataset derives national CO2 emissions for each country based on global combustion statistics from the British Petroleum (BP) Statistical Review of World Energy [50]. The spatial distribution of CO2 emissions is enhanced using point source data from CARMA and nighttime lights observations [38]. Nighttime lights data closely correlate with the distribution of human settlements and land transportation areas. The uncertainties in the ODIAC emission inventory arise from three primary sources: (i) uncertainties in national and regional emission estimates; (ii) incomplete global power plant coverage in Carbon Monitoring and Action (CARMA), leading to emissions inferred from incomplete data [51]; and (iii) the assumption that nighttime lights data directly correspond to CO2 emissions, which is often less reliable in developing countries [52].

2.2.2. MEIC

MEIC is a comprehensive database of anthropogenic pollutant and greenhouse gas emissions developed and managed by Tsinghua University [39,40]. MEIC has been widely used in research fields, including air pollution control and air quality assessments. The activity levels in MEIC are based on provincial statistical data, with emission factors derived from existing measurements within China. Emissions are initially allocated at the county level using statistical indicators such as GDP, population, and agricultural activities. Subsequently, additional gridded data, such as population density and transportation networks, are employed as spatial proxies to further distribute emissions within grid cells. However, limitations in the available underlying data introduce uncertainty into the emission estimates. MEIC currently provides multi-sectoral CO2 emission data at a resolution of 0.25° × 0.25° for the period from 1990 to 2020.

2.2.3. EDGAR

EDGAR is a global anthropogenic emission dataset developed by the European Commission’s Joint Research Centre (JRC) [10]. Emissions in EDGAR are calculated using IPCC accounting methodologies, with activity-level data derived primarily from international datasets such as those provided by the International Energy Agency (IEA) and BP statistical data. The emissions are spatially distributed to a 0.1° × 0.1° grid using spatial proxies including population density, transportation data, power plant locations, and agricultural land use maps [53].

2.3. Satellite Observations

The OCO-2 satellite, launched in 2014, is designed to deliver high-precision atmospheric CO2 observations. The three-channel imaging spectrometer onboard OCO-2 measures solar radiation in the near-infrared and shortwave infrared regions, specifically at 760 nm (O2-A band), 1610 nm (weak CO2 absorption band), and 2060 nm (strong CO2 absorption band). OCO-2 operates in a sun-synchronous orbit at an altitude of 705 km, crossing the equator at approximately 13:36 local time. With a spatial resolution of 1.29 × 2.25 km, OCO-2’s high spatial resolution and accuracy make it particularly suitable for monitoring CO2 concentration variations at regional scales [54,55]. In this study, we utilized the bias-corrected OCO-2_L2_Lite_FP_V10 product [56], which has been rigorously quality-controlled and bias-corrected to exclude unreliable data. To ensure the reliability of the results, only measurements with a Quality Flag of 0 were used.
OCO-2_L2_Lite_FP_V10 product provides XCO2, whereas the GEOS-Chem simulation provides CO2 concentration profiles across 47 layers. To compare the model simulations with satellite data, the simulated results were adjusted using averaging kernels and prior profiles to derive the modeled CO2 concentrations at the corresponding spatiotemporal locations. The specific calculation is given by the following formula [57]:
X C O 2 m = X C O 2 a + j h j a j y m y a j
where X C O 2 a represents the prior XCO2 from OCO-2, j denotes the atmospheric layers, h j is the pressure-weighted function of the j-th layer, a is the column averaging kernel, and y m and y a represent the modeled and prior CO2 vertical profiles, respectively. The parameters such as X C O 2 a , y a , and a j were obtained from the OCO-2_L2_Lite_FP_V10 product.

2.4. Ground-Based CO2 Observations

To validate the reliability of the model simulation results, ground-based observations from the Total Carbon Column Observing Network (TCCON), along with surface CO2 concentration observations provided by the Observation Package (ObsPack) product (obspack_co2_1_GLOBALVIEWplus_v9.1) from the Carbon Cycle and Greenhouse Gases (CCGG) Global Greenhouse Gas Reference Network measurement program, were used. TCCON employs Fourier Transform Infrared Spectrometers (FTIR) to record solar absorption spectra in the near-infrared range, from which column-averaged dry air mole fractions of gases such as CO2, CH4, and N2O are derived [24,58]. The latest TCCON dataset (GGG2020) used in this study achieves high measurement accuracy, with XCO2 errors below 0.6 ppm when the solar zenith angle is less than 82° [59]. Due to its high observational accuracy, TCCON data are extensively used for analyzing greenhouse gas concentration distributions and validating satellite products [54]. For this study, XCO2 observations from four TCCON stations [60,61,62,63] in East Asia were selected for subsequent analysis. Surface CO2 observation data were obtained from ObsPack product distributed by the Global Monitoring Laboratory of Earth System Research Laboratories (NOAA-ESRL) [64]. The ObsPack product is derived from in situ measurements or flask air samples; its reliability has been validated in previous studies [8,29,65]. Accordingly, surface CO2 concentration data from seven locations in China and surrounding East Asian regions were selected to evaluate GEOS-Chem’s simulation of CO2 concentrations.
The Taylor Diagram was utilized in this study to assess the performance of GEOS-Chem in simulating CO2 concentrations. A Taylor Diagram [66] is a polar coordinate plot commonly applied in meteorology and environmental science to evaluate and quantify the similarity between one or more simulated fields and observed data. The Taylor Diagram incorporates three key metrics: the correlation coefficient (R), the centered root mean square error (RMSE-c), and the standard deviations ratio (std_r). It is defined as follows:
R = 1 N i = 1 N [ ( x m i x m ¯ ) ( x o i x o ¯ ) ] / ( σ m σ o )
R M S E c = 1 N i = 1 N [ ( x m i x m ¯ ) ( x o i x o ¯ ) ] 2
s t d _ r = σ m σ o
σ m = 1 N i = 1 N ( x m i x m ¯ ) 2
σ o = 1 N i = 1 N ( x o i x o ¯ ) 2
where x m ¯ and x o ¯ represent the mean values of the model and observation data, respectively; N refers to all the data from a specific site involved in the calculation; and σ m and σ o represent the standard deviations of the simulated and observation data, respectively. These three metrics are represented concurrently within the diagram and are interrelated through a cosine relationship. Specifically, the reference point (REF) on the diagram represents the observed values. The angle between the simulated and observed values represents the correlation coefficient, the distance between the model point and the reference point represents RMSE-c, and the radial distance from the origin to the model point indicates the deviation ratio of the observed and simulated values. A higher R value, a lower RMSE-c, and a standard deviation ratio closer to 1 indicate better model performance. In other words, the closer the simulation point is to the REF point, the more accurate the simulation results.

3. Results and Discussion

3.1. Spatiotemporal Distribution of Emissions and Simulated XCO2

Figure 1 presents the daily mean CO2 emissions from 2018 to 2020 based on the ODIAC, MEIC, and EDGAR emission inventories, with units expressed in gC/m2/day. The resolution of all three emission inventories has been unified to 1° × 1°. The blank areas in the mainland China region of the figure represent areas where emission values are zero in the inventories due to data gaps or sparsely populated regions. Regarding the overall spatial distribution of emissions, all three emission inventories consistently show a pattern of higher emissions in eastern China and lower emissions in the western regions. Low emissions are primarily observed in the economically underdeveloped northwestern regions of China, including Qinghai, Tibet, and southeastern Xinjiang, due to sparse human activity. In contrast, areas with high anthropogenic emissions are predominantly concentrated in the eastern and coastal regions, notably within economically developed urban agglomerations like BTH and YRD. These regions are characterized by high populations densities, rapid economic growth, and substantial fossil fuel consumption, resulting in considerable anthropogenic CO2 emissions. The differences in emissions across the three inventories are primarily observed in the emission hotspots and regional distributions. Compared to the other two inventories, ODIAC shows significantly higher emission levels in Beijing, Shanghai, and surrounding cities. Emissions in these areas reach up to 10 gC/m2/day. The MEIC inventory displays slightly lower emissions in the southern coastal cities compared to the other two inventories. The EDGAR inventory reveals more emission hotspots with CO2 emissions exceeding 8 gC/m2/day. However, the local emission peak in Beijing and its surrounding areas is slightly lower than that in the other two inventories.
All three inventories exhibited noticeable variability in monthly anthropogenic CO2 emissions in mainland China from 2018 to 2020 (Figure 2), with emissions being generally higher in winter and lower in summer. This seasonal trend is likely associated with increased heating demand and the seasonal variations in energy consumption during winter. The three inventories demonstrated strong consistency in their temporal trends, with most monthly CO2 emissions fluctuating between 0.7 and 1.1 Gt. Moreover, a significant decline in CO2 emissions was observed in early 2020 due to the outbreak of the COVID-19 pandemic, which led to a substantial reduction in economic activities. As economic activities gradually resumed, emissions showed a recovery trend across all inventories. Notably, the EDGAR inventory consistently reported higher overall emission levels compared to ODIAC and MEIC, a finding that aligns with previous studies [53]. In terms of fluctuation characteristics, the MEIC inventory exhibited more pronounced variability compared to ODIAC and EDGAR. For instance, emissions of MEIC inventory in February 2020 dropped sharply, amounting to only half of the emissions recorded in the preceding two months. This heightened sensitivity may be attributed to the MEIC inventory’s reliance on detailed local data for statistical inputs and emission factors, making it more responsive to regional emission changes. These differences likely reflect variations in the statistical methodologies and source accounting approaches among the inventories. They collectively reveal the seasonal variations in anthropogenic CO2 emissions in mainland China and underscore the influence of economic activities on emission levels.
The annual distribution of XCO2 across East Asia exhibited a clear spatial pattern, with higher concentrations in the eastern regions and lower concentrations in the western regions, as shown in Figure 3. Higher XCO2 were mainly observed in the southeastern and central regions of China, where the average concentrations during 2018–2020 exceeded 411 ppm. Eastern regions of China, characterized by high population density, advanced industrial activities, and economic development, generated substantial CO2 emissions. In contrast, western and northeastern China displayed lower XCO2 levels due to sparser populations, lower industrial activity, and extensive forest coverage in the northeast, where active vegetation absorption leads to lower XCO2 levels. These findings were consistent with previous CO2 simulations and observations [65,67,68]. In spring (MAM), XCO2 concentrations increased markedly, especially in eastern and northern China, reaching over 413 ppm. During summer (JJA), XCO2 was generally lower, falling below 409 ppm, reflecting the absorption effects of vegetation. In autumn (SON), XCO2 levels rose again across East Asia, particularly along eastern coastal areas of China. XCO2 peaked during winter (DJF), especially in central and eastern China, with values reaching up to 420 ppm. This pattern underscores the significant influence of heating and industrial emissions during this season. Furthermore, significant differences were observed among the simulation results of the ODIAC, MEIC, and EDGAR inventories (Figure 3). The simulation results from the ODIAC inventory showed minimal differences from the mean, with most regions exhibiting slightly lower values than the average for all three inventories. However, in high-emission cities such as Beijing, Shanghai, and Guangzhou, as well as their surrounding areas, the simulated values were slightly higher than the mean. The simulation results from the MEIC inventory were lower than the mean, particularly in the eastern coastal regions of China. The simulated XCO2 of EDGAR was the highest, with significant differences primarily concentrated in southeastern China and adjacent coastal areas, reaching up to 0.4–1 ppm. Moreover, seasonal variations in these differences were more pronounced, with the EDGAR simulation showing greater XCO2 deviations from the mean during the SON and DJF. Overall, the differences among the three inventories were mainly reflected in the spatial distribution and intensity of emissions in high-emission areas.

3.2. Comparisons with Satellite XCO2

To validate the accuracy of simulated XCO2, OCO-2 observations in 2020 were compared with the corresponding simulated XCO2. On an annual scale, the simulations based on the three emission inventories exhibited a correlation coefficient of 0.79 with OCO-2 observations (Figure A1), with biases (XCO2_OCO minus XCO2_Sim) ranging from 0.31 to 1.03 ppm. Among the inventories, the simulations using the EDGAR inventory showed the smallest discrepancy when compared with OCO-2 XCO2 observations (Figure A1). Figure 4 illustrates the bias between OCO-2 XCO2 and GEOS-Chem simulated XCO2 at the corresponding spatiotemporal locations for the year 2020 and across each season. On an annual scale, OCO-2 XCO2 generally exhibited a positive bias (Bias > 0) relative to the GEOS-Chem simulations, with biases primarily ranging from −1 to 4 ppm. The discrepancies were particularly pronounced in western and northern China, where satellite retrievals tended to overestimate XCO2 [29]. This overestimation was mainly attributed to high aerosol concentrations and elevated surface albedo in the northwestern desert regions, which increased retrieval errors and led to localized overestimation. In MAM, the most significant biases were observed in central China. During JJA, the biases of all three inventories were relatively small, ranging mainly from −1 to 1 ppm and showing a more uniform spatial distribution. In some parts of northeastern China, simulated XCO2 exceeded satellite observations, likely due to uncertainties in the terrestrial biosphere effects that caused model overestimation during JJA [7]. In SON, the biases of ODIAC and MEIC were more pronounced, with biases reaching up to 6 ppm, suggesting possible inaccuracies in emission estimates in these areas. In contrast, the EDGAR inventory exhibited lower biases compared to the other two inventories. During DJF, high biases were predominantly concentrated in western China, with EDGAR showing biases within the range of −1 to 1 ppm in other regions.
The deviations between the simulated results from the three emission inventories and satellite-observed XCO2 were analyzed across different seasons (Table 1). Overall, XCO2 over mainland China was lowest in JJA, with an average of 410.73 ppm observed by OCO-2, and higher in DJF and MAM, at 414.50 ppm and 413.04 ppm, respectively. The bias between the model simulations and observations ranged from 0.15 to 1.39 ppm, with RMSE values below 2.15 ppm, indicating the reliability of the simulations. It is noteworthy that the seasonal mean biases (XCO2_OCO minus XCO2_Sim) were generally positive, suggesting that the models tended to underestimate XCO2 to some extent. This underestimation may be largely attributed to uncertainties in other types of carbon fluxes included in the simulation [65].We calculated and analyzed the annual global CO2 flux estimates from the Global Carbon Project (Table A1), as well as the CO2 flux datasets used in this study (Table A2). Our analysis revealed that CO2 simulation biases may arise from the ocean exchange flux and residual annual terrestrial exchange flux, as these fluxes in the simulation datasets were represented by fixed flux from a specific year. The use of these fixed fluxes throughout the simulation period may introduce some bias into the simulated results. In future research, the terrestrial ecosystem and ocean CO2 fluxes from the Global Carbon Project or other sources could be utilized to improve simulation accuracy. Notably, the top 10% of high XCO2 observed by the satellite were higher than the simulated XCO2, while the bottom 10% were lower than the simulations, indicating the model’s limited capability in terms of capturing XCO2 variability. These discrepancies can be attributed to constraints imposed by emission inventories and transport mechanisms on chemical transport models [29]. Satellite observations are more effective in capturing XCO2 variations due to carbon sources and sinks compared to model simulations. The overall correlation between the three inventories and satellite observations was comparable. All models showed the highest correlation in the JJA season (R = 0.83), indicating a good match between simulated and observed data during this period. Among the simulations, Sim_EDGAR consistently outperformed the others across all seasons, demonstrating the lowest bias and RMSE. This performance provides strong support for more accurate simulations and analyses of the spatial and temporal distribution and variation of CO2 concentrations. Comparing the different emission inventories, EDGAR’s biases were generally more concentrated and uniform, i.e., mostly within −1 to 2 ppm. Although some regions still showed underestimation, the overall bias magnitude was smaller than those of the other inventories, underscoring the necessity of refining emission estimates in these regions.

3.3. Validation with Ground-Based Observations

To assess the accuracy and seasonal variability of GEOS-Chem in simulating XCO2 and surface CO2 concentrations, we compared the simulated concentrations with observations from TCCON and NOAA stations across East Asia during the 2018–2020 period (Figure 5). The selected stations are geographically diverse, covering coastal, inland, and plateau environments. For each station, data from 12:00 to 14:00 local time were selected to calculate the mean concentration. The corresponding simulated CO2 concentrations were subsequently filtered and computed. Overall, the model exhibited strong agreement with station observations, demonstrating high accuracy in capturing temporal trends and fluctuations of the observed data. The majority of stations exhibited correlation coefficient above 0.7 (Table 2). The correlations at lln (Lulin) and tap (Tae-ahn Peninsula) stations were approximately 0.5, possibly due to limited observation data and coastal influences, such as atmospheric transport from the ocean. The bias at TCCON stations ranged from −1.009 to −0.063 ppm, indicating strong model performance. Considering that the surface concentration model simulations were influenced by surface fluxes, particularly in large urban areas, differences of approximately 1.5 to 8 ppm from observed values are to be expected [19]. During periods of insufficient atmospheric mixing near the surface, local CO2 concentrations may be unstable and highly variable, leading to greater fluctuations in data from ground-based observation stations. As a result, the model’s bias relative to surface CO2 observations ranged from −3.194 to 3.770 ppm, which is within an acceptable range. At more than 80% of the stations, simulations using the EDGAR inventory demonstrated the smallest bias and highest correlation, indicating superior performance of GEOS-Chem with EDGAR flux data.
To further evaluate the performance of the three anthropogenic emission inventories, a Taylor diagram was constructed (Figure 6) to compare simulations with ground-based measurements for the 2018–2020 period. The distribution of data points on the Taylor diagram clearly visualized the relative performance of each emission inventory. At over 70% of the sites, simulations based on the three inventories demonstrated high correlations (R > 0.7, p < 0.01) with the centered root mean square error (RMSE_c) below 1.0. Simulations at the Xianghe, Saga, uld, and yon stations performed exceptionally well, with a standard deviation ratio (std_r) close to 1, correlation coefficients exceeding 0.8 (p < 0.01), and RMSE_c below 0.5, indicating strong agreement with observational data. Conversely, simulations at the lln and tap stations exhibited lower correlation coefficients and std_r. This may reflect the complex local emission characteristics and topographical influences, limiting the model’s ability to accurately reproduce conditions in these areas. Among the three inventories, the EDGAR inventory showed the best overall agreement, as indicated by the proximity of most station points to the reference point (REF) on the diagram. In summary, the comparison with ground-based observations suggested that GEOS-Chem effectively reproduced CO2 concentrations and their temporal dynamics across most sites. However, there were notable discrepancies between the observed and simulated CO2 concentrations at some sites. These findings highlighted the limitations of current emission inventories in terms of regional adaptability and accuracy, underscoring the need for further adjustments and optimizations tailored to different environmental characteristics.

3.4. The Impact of Emission Variability on XCO2

In this study, we conducted an experiment by turning off the fossil fuel emission option, while keeping all other parameters constant. This experiment is referred to as the “no_fossil” scenario. Figure 7 illustrates the differences between the simulation results of the three emission inventories and the no_fossil scenario, representing discrepancies attributed to anthropogenic fossil fuel emissions. The increase in XCO2 resulting from fossil fuel combustion displays a similar spatial pattern across East Asia for all three inventories. In eastern China, particularly over the North China Plain and the Yangtze River Delta, the difference in XCO2 reached over 10 ppm, as these regions were hotspots for anthropogenic CO2 emissions. In contrast, concentrations were notably lower in the western regions, with XCO2 differences ranging between 6.5 and 9 ppm. The larger increase in eastern China was attributed to its dense population and high levels of industrial activity, whereas the smaller increase in the west was associated with lower industrialization and reduced energy consumption. The XCO2 discrepancy between the sim_EDGAR and no_fossil simulations was the largest, with a broader area showing elevated value. This could be attributed to EDGAR’s higher emission estimates compared to the other two inventories. A previous study indicated that after 2013, EDGAR’s estimates of China’s total CO2 emissions tended to be higher compared to most other inventories [53]. Due to the inherent complexity of the atmospheric transport model, including factors like horizontal atmospheric convection, boundary layer mixing, and variations in the troposphere, the relationship between carbon dioxide emission fluxes and simulated XCO2 concentrations is complex. Spearman’s correlation analysis [69] conducted over mainland China revealed that anthropogenic CO2 emissions show a significant positive correlation (r > 0, p < 0.01) with simulated XCO2 concentrations in most regions (Figure A2). However, our analysis showed that an increase in anthropogenic CO2 flux leads to a corresponding rise in simulated XCO2. Notably, regions with high increases in XCO2 coincided strongly with regions of high emission intensity, indicating that our simulation reasonably reflected the spatial distribution characteristics of the emission inventories and quantifies their impact on CO2 concentration changes.
A series of model experiments were conducted based on the EDGAR emission inventory to explore the impact of emission variability on spatial XCO2. Specifically, the emissions in mainland China were adjusted by ±20%, ±50%, and ±100% relative to the initial EDGAR inventory. The distribution of average XCO2 discrepancy between simulated XCO2 for the adjusted emissions and the baseline experiment (simulated using the initial EDGAR inventory) were then analyzed. Figure 8 indicates that changes in emission levels had a significant impact on XCO2, particularly in central and eastern China, with notable effects in regions with dense industrial activity and urbanization. As emissions increased, XCO2 concentrations rose considerably, with the most pronounced effect observed in the +100% emission scenario (Figure 8, Panel (e)), where the XCO2 difference reached 3.5 ppm, particularly over northern, eastern, and central China. In the +50% and +20% scenarios (Panel (c) and Panel (a)), although the increase was smaller, notable rises of 2 ppm and 1 ppm, respectively, were still observed in these key emission source regions. Conversely, under emission reduction scenarios, XCO2 concentrations decreased to varying degrees. Figure 8, Panel (c) shows that XCO2 concentrations in the eastern seaboard urban agglomeration dropped to −2 ppm in the −50% scenario. In the −50% scenario, the XCO2 concentration was observed to decrease by −2 ppm in the eastern coastal urban clusters. When the emissions in the mainland China region were reduced by 100%, the discrepancy in XCO2 between the adjusted simulation and the baseline experiment in eastern China could reach 2 to 3.5 ppm. This underscores the dominant role of these regions in emissions, where emission reductions have a significant impact on XCO2 concentrations. It is worth noting that even when only the emissions for mainland China were changed, there were still differences observed in regions such as the Bohai Sea, the Yellow Sea, and Southeast Asia, where the emission flux remained unchanged compared to the baseline experiment. This suggests that changes in CO2 emissions in mainland China may have an impact on the CO2 concentrations in neighboring countries and surrounding seas due to atmospheric transport. Overall, the results highlighted a clear spatial heterogeneity in the response of XCO2 concentrations to changes in emission levels, with more pronounced effects in high-emission regions. The nonlinear response across different areas highlighted the critical role of carbon concentrations in high-emission regions in regulating atmospheric XCO2 levels. Targeted emission control in central China, in particular, could not only reduce XCO2 concentrations within the region but also curb the rising trend of CO2 concentrations over a broader spatial scale.
We separately conducted simulation experiments by modifying the emissions in the BTH and YRD regions to analyze the impact of emission changes in these urban clusters on the XCO2 concentrations in the region and its surrounding areas. Compared to nationwide emission adjustments, changes in emissions within the BTH region exhibited a more localized and concentrated influence on XCO2 (Figure 9). This impact was primarily confined to the North China area, although its intensity and magnitude remained significant. In the +100% emissions scenario (BTH, Panel (e)), the increase in XCO2 was most pronounced, with the maximum rise ranging from approximately 1.5 to 2 ppm, concentrated in the industrial and densely populated areas of Beijing, Tianjin, and central Hebei. As emissions were reduced, the extent and intensity of the impact diminished progressively. As shown in BTH, Panel (c), the area of concentration growth became smaller in the +50% scenario, with the intensity diminishing to 0.4–1.5 ppm. The effect remained concentrated in the BTH region, with minor expansion into neighboring provinces. When emissions were increased by 20% (BTH, Panel (a)), the resulting change in XCO2 was minimal, resulting in changes of less than 0.1 ppm. On the other hand, in emissions reduction scenarios, the decline in XCO2 was similarly concentrated in the BTH region. Under the −20% emissions scenario, the XCO2 decrease ranged from −0.2 to −0.4 ppm, with a limited area of influence, mainly covering a small portion of the BTH surroundings. In the −50% and −100% emissions scenarios ((Panel (d) and Panel (f), respectively)), the decrease became more significant, with the largest difference ranging from −1 to −2 ppm. The affected area expanded into the surrounding North China Plain, particularly northern Hebei and Shandong provinces, demonstrating a clear regional impact. This suggested that changes in emissions within the BTH region had a significant localized effect on the spatial distribution of XCO2. Although the scope of influence was smaller compared to national emission adjustments, the impact on atmospheric carbon concentration in the area was substantial, especially under high-emission scenarios.
In the YRD region, increases in emissions predominantly affected XCO2 concentrations in Jiangsu, Shanghai, and Zhejiang, with a maximum increase of 1.5 to 2 ppm in the +100% emissions scenario (YRD, Panel (e)). When emissions were adjusted by 20%, the impact on the YRD and its surrounding areas ranged from −0.4 to 0.4 ppm, with the affected area limited to the YRD and adjacent inland cities (YRD, Panel (a) and Panel (b)). As the magnitude of emission changes increased, the impact gradually extended to parts of Anhui, Jiangxi, and Fujian, with a clear influence on XCO2 levels in the eastern coastal regions of China. This indicated that while emissions were altered only in the YRD, atmospheric circulation and exchange influenced CO2 concentrations in marine areas. Overall, compared to nationwide emission changes, adjustments to emissions in the BTH and YRD regions primarily influenced the local areas and their surroundings, with a more concentrated intensity and relatively smaller spatial extent. However, regional emission changes could significantly alter the XCO2 distribution in these areas. Therefore, carbon reduction policies in the BTH region are essential for regulating atmospheric CO2 concentrations.

4. Conclusions

This study evaluated variations in anthropogenic CO2 emissions across mainland China from 2018 to 2020 and their impact on atmospheric CO2 concentrations. The study conducted a comparative analysis of three commonly utilized emission inventories—ODIAC, MEIC, and EDGAR. Chemical transport models were employed to simulate CO2 concentrations, integrated with both satellite and ground-based observation data. Additionally, numerical experiments to analyze the impacts of emission level variations on the spatiotemporal distribution of CO2 were conducted. The results underscored the vital role of accurate emission inventories, as discrepancies between these datasets significantly affect simulations of atmospheric CO2 concentrations. This research aims to clarify the substantial influence of anthropogenic CO2 emissions on atmospheric CO2 concentrations and their response to emission variations, highlighting the need for improved emission inventories.
The spatial distribution of emissions across the three inventories exhibited consistent patterns. Higher emissions were observed in economically developed coastal regions, such as the North China Plain and the Yangtze River Delta, while lower emissions were found in the western regions. However, differences in spatial resolution and regional emissions were evident between the inventories. The study found that these discrepancies led to notable differences in simulated CO2 concentrations over China and neighboring regions, particularly in areas with high emission values. Additionally, model performance was evaluated against ground-based station and satellite observations, with EDGAR showing the best consistency. The majority of the deviations between EDGAR and satellite observations ranged from −1 to 2 ppm, with an average bias of 0.31 ppm.
Moreover, a series of numerical experiments demonstrated that variations in emission levels significantly influence CO2 concentrations, especially in industrialized and densely populated regions. In the “no_fossil” experiment, where anthropogenic emissions were disabled, the difference in XCO2 between the North China Plain and the Yangtze River Delta regions and the base experiment exceeded 10 ppm, as these areas are hotspots for anthropogenic CO2 emissions. In the scenario where emissions increased by 100%, the XCO2 differences were most pronounced, reaching up to 3.5 ppm, with the pronounced discrepancies concentrated in northern and central China. In high-emission regions like the Yangtze River Delta and BTH areas, this increase in emissions induced significant changes in atmospheric CO2 levels. When emissions were adjusted by ±100% in the BTH and Yangtze River Delta regions, the XCO2 variations reached as high as 2 ppm, and these changes also influenced CO2 concentrations in adjacent regions with unchanged emissions. This finding was particularly important for China, where localized emission reductions in key regions can have profound impacts on national and regional atmospheric CO2 levels.
This study may contribute to understanding the impact of anthropogenic CO2 emissions on atmospheric CO2 concentrations and provide a reference for selecting of anthropogenic emission inventories in forward CO2 simulations. However, there were some uncertainties in this research. The meteorological data used in the model, along with biomass burning emission inventories, land carbon flux data, and other inputs, may have influenced the simulation results. Furthermore, different atmospheric chemistry models employ distinct chemical transport mechanisms. Therefore, future research exploring simulations using a variety of atmospheric chemistry models would be valuable. Additionally, the estimates of fossil fuel emissions are highly uncertain, and the accuracy of emission inventories significantly influences the simulated atmospheric CO2 concentrations. If fossil fuel emissions are not adequately corrected during the inversion process, errors in these emissions will be redistributed to the estimates of other natural biosphere fluxes [70]. Therefore, future research should aim to obtain more reliable fossil fuel emission inventories and enhance the quantification of inventory uncertainties, incorporating the associated uncertainties of fossil fuel emissions into the inversion framework.

Author Contributions

Conceptualization X.L. and W.L.; Methodology, W.L.; Software, W.L.; Formal analysis, W.L.; Investigation Y.G. and W.F.; data curation W.L.; Writing—original draft, W.L.; Writing—review & editing, W.L., X.L., S.L., Y.G. and T.C.; Supervision, X.L. and S.L.; Project administration, X.L. and S.L.; Funding acquisition, X.L. and S.L. All authors have read and agreed to the published version of the manuscript.

Funding

This research was financially supported by the National Key R&D Program of China (2022YFF0606404), and the National Natural Science Foundation of China (Grant No. 42071409).

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.

Acknowledgments

The authors acknowledge the efforts of the GEOS-Chem working groups for developing and managing the model. OCO-2 data used in this research were collected by the OCO-2 Project at the Jet Propulsion Laboratory, California Institute of Technology, and obtained from the OCO-2 data archive maintained at the NASA Goddard Earth Science Data and Information Services Center. CT2022 at three-hourly resolution is publicly available at https://gml.noaa.gov/aftp/products/carbontracker/co2/CT2022/molefractions/co2_total/ (accessed on 1 September 2023). The authors acknowledge the ODIAC team. Also, the authors acknowledge the European Commission, Joint Research Centre (JRC) and the International Energy Agency (IEA) for jointly providing EDGAR Community GHG Database. The Multi-resolution Emission Inventory for China (MEIC) emission data were developed and managed by researchers at Tsinghua University (http://meicmodel.org.cn (accessed on 30 September 2023)). The TCCON (GGG2020) data were obtained from the TCCON Data Archive hosted by CaltechDATA (https://tccondata.org/ (accessed on 30 September 2023)). The authors would like to thank all the research teams that provided surface flask CO2 observations for the global Monitoring Laboratory (GML) of the National Oceanic and Atmospheric Administration (NOAA) (https://gml.noaa.gov/ccgg/obspack/ (accessed on 1 April 2024)). The authors would like to sincerely thank the above organizations and researchers.

Conflicts of Interest

The authors declare no conflict of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript; or in the decision to publish the results.

Appendix A

Figure A1. Scatter plots of the OCO-2 XCO2 and GEOS-Chem simulated XCO2 for the year 2020.
Figure A1. Scatter plots of the OCO-2 XCO2 and GEOS-Chem simulated XCO2 for the year 2020.
Remotesensing 17 00814 g0a1
Figure A2. Heatmap of Spearman’s correlation coefficients between anthropogenic CO2 emissions (using the EDGAR inventory) and simulated XCO2 concentrations for 2018–2020. Blank regions over mainland China indicate areas where the correlation did not meet statistical significance.
Figure A2. Heatmap of Spearman’s correlation coefficients between anthropogenic CO2 emissions (using the EDGAR inventory) and simulated XCO2 concentrations for 2018–2020. Blank regions over mainland China indicate areas where the correlation did not meet statistical significance.
Remotesensing 17 00814 g0a2
Table A1. Global CO2 flux estimated by Global Carbon Project (GCP) for the 2018–2020 period (unit: GtC yr−1) and all uncertainties are reported as ±1δ.
Table A1. Global CO2 flux estimated by Global Carbon Project (GCP) for the 2018–2020 period (unit: GtC yr−1) and all uncertainties are reported as ±1δ.
201820192020
Fossil CO2 emissions10 + 0.59.7 ± 0.59.3 ± 0.5
Land-use change emissions1.5 ± 0.71.8 ± 0.70.9 ± 0.7
Total emissions11.5 ± 0.911.5 ± 0.910.2 ± 0.8
Partitioning
Ocean sink2.6 ± 0.62.6 ± 0.63.0 ± 0.4
Terrestrial sink3.5 ± 0.73.1 ± 1.22.9 ± 1.0
Annual CO2 fluxes5.45.84.3
Reference[71][72][73]
Table A2. Summary of inventories for GEOS-Chem CO2 simulations in this work along with global annual CO2 flux during the study period (2018–2020) (unit: GtC yr−1).
Table A2. Summary of inventories for GEOS-Chem CO2 simulations in this work along with global annual CO2 flux during the study period (2018–2020) (unit: GtC yr−1).
Flux TypeInventory Name/Abbreviation201820192020Reference
Fossil fuel and cement manufactureODIAC10.1110.179.7[49]
EDGAR10.3410.369.82[10,74,75,76]
Biomass burningGFEDv4.1s1.672.061.81[41]
Balanced biosphereSiB3000[43]
Residual annual terrestrial exchangeTransCom climatology
(fixed in 2006)
−5.29−5.29−5.29[44]
Ocean exchangeScaled ocean exchange
(fixed in 2009)
−1.41−1.41−1.41[42]
ShippingCEDS0.2360.230.23[45,77]
AviationAEIC0.160.160.16[37,47]
Chemical sourceGEOS-Chem CO2 Chemical Source1.04–1.061.04–1.061.04–1.06[37]
Total CO2 flux
(chemical source not included)
Using ODIAC as FF flux5.4765.925.2
Using EDGAR as FF flux5.7066.115.32

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Figure 1. Spatial distribution of emissions (gC/m2/d) in mainland China from three inventories in 2018–2020: (a) ODIAC, (b) MEIC and (c) EDGAR, with zoomed-in views of the BTH and YRD regions in the right panel.
Figure 1. Spatial distribution of emissions (gC/m2/d) in mainland China from three inventories in 2018–2020: (a) ODIAC, (b) MEIC and (c) EDGAR, with zoomed-in views of the BTH and YRD regions in the right panel.
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Figure 2. Time series of monthly anthropogenic CO2 emissions over mainland China from 2018 to 2020 based on three emission inventories: ODIAC, MEIC, and EDGAR.
Figure 2. Time series of monthly anthropogenic CO2 emissions over mainland China from 2018 to 2020 based on three emission inventories: ODIAC, MEIC, and EDGAR.
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Figure 3. Distribution of mean XCO2 for three emission inventories (ODIAC, MEIC, and EDGAR) simulations (first column) and discrepancy between each of the three simulations and the mean (second to fourth columns) in 2018–2020 (ANN: annual; MAM: March–April-May; JJA: June–July–August; SON: September–October–November; DJF: December–February).
Figure 3. Distribution of mean XCO2 for three emission inventories (ODIAC, MEIC, and EDGAR) simulations (first column) and discrepancy between each of the three simulations and the mean (second to fourth columns) in 2018–2020 (ANN: annual; MAM: March–April-May; JJA: June–July–August; SON: September–October–November; DJF: December–February).
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Figure 4. Bias (XCO2_OCO minus XCO2_Sim) distributions of satellite XCO2 observations and model simulations for ANN, MAM, JJA, SON and DJF in 2020, with the first, second, and third columns showing the differences between observations and simulations based on the ODIAC, MEIC, and EDGAR inventories ((a) Obs minus Sim_ODIAC, (b) Obs minus Sim_MEIC, and (c) Obs minus Sim_EDGAR).
Figure 4. Bias (XCO2_OCO minus XCO2_Sim) distributions of satellite XCO2 observations and model simulations for ANN, MAM, JJA, SON and DJF in 2020, with the first, second, and third columns showing the differences between observations and simulations based on the ODIAC, MEIC, and EDGAR inventories ((a) Obs minus Sim_ODIAC, (b) Obs minus Sim_MEIC, and (c) Obs minus Sim_EDGAR).
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Figure 5. Geophysical locations of the selected sites.
Figure 5. Geophysical locations of the selected sites.
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Figure 6. The Taylor diagram comparing the XCO2 simulated by the three anthropogenic emission inventories based on GEOS-Chem with the Ground-based CO2 observations in the 2018–2020 period. The radial coordinates represent the standard deviation ratio between the simulated CO2 and the observed CO2 in each stie, while the angular coordinates indicate the correlation coefficient. The gray dashed lines denote the centered root mean square error (RMSE-c).
Figure 6. The Taylor diagram comparing the XCO2 simulated by the three anthropogenic emission inventories based on GEOS-Chem with the Ground-based CO2 observations in the 2018–2020 period. The radial coordinates represent the standard deviation ratio between the simulated CO2 and the observed CO2 in each stie, while the angular coordinates indicate the correlation coefficient. The gray dashed lines denote the centered root mean square error (RMSE-c).
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Figure 7. Spatial distribution of average differences between simulations from inventories and no_fossil simulations ((a) Sim_ODIAC minus Sim_no_fossil, (b) Sim_MEIC minus Sim_no_fossil and (c) Sim_EDGAR minus Sim_no_fossil) in 2018–2020.
Figure 7. Spatial distribution of average differences between simulations from inventories and no_fossil simulations ((a) Sim_ODIAC minus Sim_no_fossil, (b) Sim_MEIC minus Sim_no_fossil and (c) Sim_EDGAR minus Sim_no_fossil) in 2018–2020.
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Figure 8. The distribution of average XCO2 discrepancy between the adjusted emission scenarios ((a) +20%, (b) −20%, (c) +50%, (d) −50%, (e) +100%, and (f) −100% scenarios) and the baseline experiment (Sim_EDGAR) for 2020.
Figure 8. The distribution of average XCO2 discrepancy between the adjusted emission scenarios ((a) +20%, (b) −20%, (c) +50%, (d) −50%, (e) +100%, and (f) −100% scenarios) and the baseline experiment (Sim_EDGAR) for 2020.
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Figure 9. The distribution of XCO2 average discrepancy between the adjusted emission scenarios (solely on the BTH region or YRD region, (a) +20%, (b) −20%, (c) +50%, (d) −50%, (e) +100%, and (f) −100% scenarios) and the baseline experiment (Sim_EDGAR) in 2020.
Figure 9. The distribution of XCO2 average discrepancy between the adjusted emission scenarios (solely on the BTH region or YRD region, (a) +20%, (b) −20%, (c) +50%, (d) −50%, (e) +100%, and (f) −100% scenarios) and the baseline experiment (Sim_EDGAR) in 2020.
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Table 1. Statistical parameters between OCO-2 observations and simulations in 2020.
Table 1. Statistical parameters between OCO-2 observations and simulations in 2020.
Mean of XCO2 (ppm)The Mean of Highest 10% XCO2 (ppm)The Mean of Lowest 10% XCO2 (ppm)Bias
(ppm)
MAE
(ppm)
RMSE
(ppm)
Correlation Coefficient
MAMObs_OCO-2414.50417.51411.51
Sim_ODIAC413.79415.88411.810.721.221.660.52
Sim_EDGAR414.26416.39412.240.241.091.510.52
Sim_MEIC413.61415.67411.650.891.301.740.52
JJAObs_OCO-2410.73415.40404.80
Sim_ODIAC410.06413.73405.290.671.421.860.83
Sim_EDGAR410.59414.26405.820.141.291.740.83
Sim_MEIC409.84413.54405.010.881.511.930.83
SONObs_OCO-2411.45415.18407.88
Sim_ODIAC410.32412.68407.971.131.541.990.60
Sim_EDGAR410.88413.56408.530.561.281.730.60
Sim_MEIC410.06412.35407.701.391.702.150.60
DJFObs_OCO-2413.04416.71410.38
Sim_ODIAC412.32414.86410.380.721.361.820.53
Sim_EDGAR412.80415.58410.740.251.241.680.55
Sim_MEIC412.11414.54410.210.931.451.910.53
Table 2. Statistical parameters and information for each station of ground observation in 2018-2020.
Table 2. Statistical parameters and information for each station of ground observation in 2018-2020.
Sites NameLat (°N)Lon (°E)Alt (m)Emission InventoriesStd_rBias (ppm)Correlation
Coefficient
Xianghe39.80116.96/ODIAC0.98−0.0630.855
EDGAR0.98−0.1500.871
MEIC0.95−0.5770.873
Hefei31.90117.17/ODIAC1.15−0.5550.812
EDGAR1.160.0630.817
MEIC1.14−0.6050.7966
Burgos18.53120.65/ODIAC0.87−0.9890.967
EDGAR0.93−0.7040.968
MEIC0.85−1.0090.9656
Saga33.24130.29/ODIAC0.96−0.6730.937
EDGAR1.00−0.2440.947
MEIC0.95−0.7040.930
gsn33.28126.1578ODIAC0.8802.2090.713
EDGAR0.9211.4980.725
MEIC0.8622.6040.711
lln23.46120.862867ODIAC0.5253.6160.518
EDGAR0.5653.3000.514
MEIC0.5093.7700.519
tap36.73126.1321ODIAC0.7122.6110.513
EDGAR0.7210.9420.518
MEIC0.7132.9360.514
uld37.48130.90231ODIAC1.0502.0160.810
EDGAR1.0811.3790.815
MEIC1.0452.3400.808
uum44.45111.101012ODIAC0.8162.1880.886
EDGAR0.8151.8020.890
MEIC0.8162.3300.886
yon24.47123.0150ODIAC1.1060.9840.801
EDGAR0.9760.3790.804
MEIC0.8771.2680.797
wlg36.27100.923815ODIAC0.920−2.4610.689
EDGAR1.169−3.1940.685
MEIC1.124−2.4230.678
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Lu, W.; Li, X.; Li, S.; Cheng, T.; Guo, Y.; Fang, W. Effects of Emission Variability on Atmospheric CO2 Concentrations in Mainland China. Remote Sens. 2025, 17, 814. https://doi.org/10.3390/rs17050814

AMA Style

Lu W, Li X, Li S, Cheng T, Guo Y, Fang W. Effects of Emission Variability on Atmospheric CO2 Concentrations in Mainland China. Remote Sensing. 2025; 17(5):814. https://doi.org/10.3390/rs17050814

Chicago/Turabian Style

Lu, Wenjing, Xiaoying Li, Shenshen Li, Tianhai Cheng, Yuhang Guo, and Weifang Fang. 2025. "Effects of Emission Variability on Atmospheric CO2 Concentrations in Mainland China" Remote Sensing 17, no. 5: 814. https://doi.org/10.3390/rs17050814

APA Style

Lu, W., Li, X., Li, S., Cheng, T., Guo, Y., & Fang, W. (2025). Effects of Emission Variability on Atmospheric CO2 Concentrations in Mainland China. Remote Sensing, 17(5), 814. https://doi.org/10.3390/rs17050814

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