GCAP 2.0: a global 3-D chemical-transport model framework for past, present, and future climate scenarios
This paper describes version 2.0 of the Global Change and Air Pollution (GCAP 2.0) model framework, a one-way offline coupling between version E2.1 of the NASA Goddard Institute for Space Studies (GISS) general circulation model (GCM) and the GEOS-Chem global 3-D chemical-transport model (CTM). Meteorology for driving GEOS-Chem has been archived from the E2.1 contributions to phase 6 of the Coupled Model Intercomparison Project (CMIP6) for the pre-industrial era and the recent past. In addition, meteorology is available for the near future and end of the century for seven future scenarios ranging from extreme mitigation to extreme warming. Emissions and boundary conditions have been prepared for input to GEOS-Chem that are consistent with the CMIP6 experimental design. The model meteorology, emissions, transport, and chemistry are evaluated in the recent past and found to be largely consistent with GEOS-Chem driven by the Modern-Era Retrospective analysis for Research and Applications version 2 (MERRA-2) product and with observational constraints.
How atmospheric composition and chemistry has changed in the past and will change in the future is of tremendous societal importance. Surface air pollution is the leading cause of preventable death worldwide (GBD 2019 Risk Factor Collaborators, 2020) and threatens global food security and ecosystem health (e.g., Tai et al., 2021). Short-lived climate forcers like methane, tropospheric ozone, and aerosol particles influence global and regional climate (e.g., Fiore et al., 2015). The emission of ozone-depleting substances and climate change threatens the overlying stratospheric ozone layer (WMO, 2018). And solar radiation modification through the purposeful injection of chemical species into the atmosphere is seriously being considered to combat anthropogenic climate change. Yet, it remains highly uncertain in its efficacy or risks (e.g., Eastham et al., 2021).
To study and address these issues, scientists, regulators, and policymakers frequently use 3-D chemical-transport models (CTMs). CTMs use archived meteorology to drive the spatial and temporal evolution of trace gases and particles in the atmosphere. By not needing to resolve all the equations of motion, as in a general circulation model (GCM), CTMs can expend additional computational power to resolve more complex chemistry or perform additional simulations. Furthermore, the chain of cause and effect between meteorology and composition is much easier to establish in a CTM than a fully coupled chemistry–climate model (CCM) or Earth system model (ESM) running online chemistry. And because meteorological reanalyses usually drive CTMs, they may easily be matched in space and time to observations, unlike CCMs or ESMs that generate their own winds. However, the reliance of CTMs on existing driving meteorology means that CTMs have traditionally been largely excluded from international assessments aimed at forecasting future or past changes, such as those of the ongoing phase (phase 6) of the Coupled Model Intercomparison Project (CMIP6, Eyring et al., 2016) that is set to inform the upcoming Intergovernmental Panel on Climate Change (IPCC) Sixth Assessment Report.
Here, we introduce, describe, and evaluate version 2.0 of the Global Change and Air Pollution (hereafter, “GCAP 2.0”) chemical-transport model framework. GCAP 2.0 represents a major update and expansion of the original GCAP described by Wu et al. (2007) and Murray et al. (2014). Meteorology necessary for driving the grassroots-community GEOS-Chem 3-D chemical-transport model (http://www.geos-chem.org, last access: 9 September 2021) has been archived for the pre-industrial, recent past, and several future scenarios of the CMIP6 experiment using version E2.1 of the NASA Goddard Institute for Space Studies (GISS) GCM (Kelley et al., 2020; Miller et al., 2021). In addition, the CMIP6 emissions and surface boundary conditions have been processed for use within GEOS-Chem for consistency with the driving meteorology and to enable GEOS-Chem to perform and contribute to the CMIP6 experiments.
Section 2 summarizes the history of the GCAP framework. Section 3 describes the climate and chemistry models used and their interface. Section 4 summarizes and evaluates the meteorology products in the recent past versus reanalyses. Section 5 describes the emissions and boundary conditions and evaluates the climate-sensitive emissions. Section 6 evaluates the model in the recent past by comparing it to observations. We conclude with a summary section.
The GISS GCM and GEOS-Chem CTM have a long history of collaborative development. The immediate predecessor to GEOS-Chem was a gas-phase CTM of tropospheric ozone–NOx–CO–hydrocarbon chemistry (Wang et al., 1998a, b, c; Wang and Jacob, 1998) driven by present-day meteorology archived from version II' of the GISS GCM at 4∘ latitude by 5∘ longitude horizontal resolution with seven vertical layers extending from the surface to 150 hPa (Hansen et al., 1983; Rind and Lerner, 1996). GEOS-Chem was born when Bey et al. (2001) updated this model to include the tropospheric non-methane hydrocarbon oxidation mechanism of Horowitz et al. (1998) and allowed it to be driven instead by the Goddard Earth Observing System (GEOS) assimilated meteorological reanalyses produced by the NASA Global Modeling and Assimilation Office (GMAO) (Schubert et al., 1993). This early version of GEOS-Chem incorporated the GEOS dynamical core (Lin and Rood, 1996). Shortly afterward, a bulk sulfur–nitrate–ammonium aerosol mechanism was included by Park et al. (2004).
Since these origins, GEOS-Chem has developed a large user and active developer base of hundreds of individuals at more than 150 institutions in over 30 countries (http://www.geos-chem.org, last access: 9 September 2021). The model is extensively versioned, documented, and benchmarked. Other subsequent major developments include the development of one- and two-way coupled nested regional simulations (Wang et al., 2004; Yan et al., 2016; Bindle et al., 2020), an adjoint for inverse model applications (Henze et al., 2007; Kopacz et al., 2009), a unified chemical mechanism from the surface to the mesopause (Eastham et al., 2014), a flexible emissions pre-processor (Keller et al., 2014), and a massively parallel distributed computing framework enabling global simulations down to resolutions of 0.25∘ latitude by 0.3125∘ longitude with 72 vertical layers extending to 0.01 hPa (Eastham et al., 2018).
The Global Change and Air Pollution (GCAP) framework developed by Wu et al. (2007) re-enabled version 7-02-04 of GEOS-Chem to be driven by GISS meteorology in order to explore how changes in future climate and precursor emissions may influence surface air quality (e.g., Wu et al., 2008a, b; Pye et al., 2009; Pye and Seinfeld, 2010; Selin et al., 2009; Hui and Hong, 2013; Zhu et al., 2017). GCAP utilized meteorology archived from version III of the GCM (Rind et al., 2007) at 4∘ latitude by 5∘ longitude resolution with 23 vertical layers extending to 0.002 hPa for the present-day and the Intergovernmental Panel on Climate Change (IPCC) Special Report on Emissions Scenarios (SRES) “A1B” scenario for 2050 CE (Nakicenovic and Swart, 2000).
In the subsequent ICE age Chemistry And Proxies (ICECAP) project, Murray et al. (2014) updated the GCAP implementation to enable version 9-01-03 of GEOS-Chem to be driven by paleometeorology archived from version E of the GISS GCM (Schmidt et al., 2006) and consistent land cover simulated using terrestrial vegetation models (Kaplan et al., 2006; Pfeiffer et al., 2013) to explore chemistry–climate changes at and since the Last Glacial Maximum (LGM; ∼ 21 kyr before present; Murray et al., 2014; Achakulwisut et al., 2015; Geng et al., 2015, 2017).
However, the original GISS-driven variants of GEOS-Chem suffered from several issues. Most notably, the stratosphere-to-troposphere mass flux was always too large, complicating the tropospheric ozone budget and the interpretation of polar ice-core records once GEOS-Chem developed online interactive stratospheric chemistry. The use of the more accurate, but computationally expensive, GISS dynamical core within GEOS-Chem to improve transport yielded severe performance issues in the CTM. At the time, both GEOS-Chem and the GISS GCM used their own in-house binary formats for file input and output that required translation (versus the standard NetCDF file format used today by both models). Lastly, the different horizontal and vertical resolutions required extensive offline processing of input fields. GCAP was eventually deprecated and removed from the GEOS-Chem codebase in version 11-02d.
However, subsequent developments to both models increased flexibility and capabilities, motivating the development of GCAP 2.0, as described in the subsequent section.
GCAP 2.0 is the second generation of a one-way offline coupling between the NASA GISS GCM and the GEOS-Chem CTM. Meteorology archived from version E2.1 of the GCM for any period of Earth history or its future may be used to drive the GEOS-Chem CTM. The following subsections describe the salient components and edits to the GCM and CTM relevant for GCAP 2.0 simulations.
3.1 NASA GISS ModelE2.1
The version of the GISS GCM frozen and applied to the initial CMIP6 experiments (ModelE2.1, hereafter “E2.1”) is described in detail by Kelley et al. (2020) and Miller et al. (2021). In brief, the standard E2.1 configuration resolves the equations of mass, momentum, and energy in Earth's atmosphere at a horizontal resolution of 2∘ latitude by 2.5∘ longitude and with 40 vertical layers extending from the surface to 0.1 hPa (∼ 28 in the tropical troposphere; see Fig. 1). The model employs a quadratic-upstream scheme for advection that yields finer effective spatial resolutions by transporting higher-order moments of the subgrid distributions (Prather, 1986). Gravity-wave momentum fluxes resulting from flow over topography and fronts are parameterized as stratospheric drag processes (Rind et al., 1988). Moist convection underwent substantial updates relative to E2.1's predecessor version, E2 (Kim et al., 2012; Del Genio et al., 2012, 2015). Radiation physics includes calculations for major shortwave and longwave absorbers (water vapor, carbon dioxide, ozone, methane, nitrous oxide, chlorofluorocarbons) and aerosol particles (Hansen et al., 1983), any of which may be either prescribed or calculated online as a function of emissions, chemistry, and physical losses. The influence of aerosol particles on cloud microphysics and albedo may be explicitly represented or parameterized (Bauer et al., 2020). The model may be coupled to a fully interactive ocean model or be applied in atmosphere-only mode through prescribed sea-surface temperatures.
GISS contributed several configurations of E2.1 to CMIP6. Here, we use the atmosphere-only configuration with composition prescribed from earlier runs using online and interactive chemistry for computational expediency. At the time of publication, GISS also contributed up to 11 ensemble members per historical and future emission scenario initialized from different moments of the pre-industrial control simulation. We focus on the atmosphere-only ensemble member that contributed to the largest number of Tier 1 and Tier 2 scenarios of the CMIP and Scenario Model Intercomparison Project (ScenarioMIP) experiments, corresponding to variant label “r1i1p1f2” in the CMIP6 data repository (https://esgf-node.llnl.gov/projects/cmip6/, last access: 9 December 2020).
On top of the E2.1 codebase used for the CMIP6 simulations, we implemented new subdaily diagnostics that archive the same fields used to drive GEOS-Chem as generated by the Modern-Era Retrospective analysis for Research and Applications version 2 (MERRA-2) meteorological reanalysis (Gelaro et al., 2017). We then re-performed the “r1i1p1f2” variant of the E2.1 contributions to the CMIP and ScenarioMIP experiments using initial and intermediate restart files archived during the original simulations and archiving the subdaily diagnostics necessary for driving GEOS-Chem. We discuss and evaluate the meteorology in Sect. 4. Three-dimensional fields were archived at 3 h temporal resolution and two-dimensional fields were archived at hourly temporal resolution, consistent with the MERRA-2 product. In addition, we archived hourly lightning flash densities and convective cloud depths. The only difference in the repeat simulation configurations with respect to their original runs was a need to call the radiation code every dynamic time step instead of every five to obtain the hourly radiation fields necessary for driving GEOS-Chem; the consequences of this are discussed in Sect. 4.
All meteorology fields available at 2∘ latitude by 2.5∘ longitude with 40 vertical layers from the surface to 0.1 hPa. Two-dimensional fields are archived at hourly temporal resolution. Three-dimensional fields are archived at 3 h temporal resolution.
Table 1 summarizes the 178 years of GCAP 2.0 meteorology archived and publicly available at publication time. For comparison, MERRA-2 presently has 41 years of complete meteorology available. The data are publicly served from the new GCAP data server hosted by the University of Rochester Atmospheric Chemistry and Climate Group at http://atmos.earth.rochester.edu/input/gc/ExtData (last access: 9 September 2021). Users can point to this repository analogously to the existing GEOS-Chem data servers hosted by Harvard University (http://ftp.as.harvard.edu/gcgrid/data/ExtData/, last access: 9 September 2021) or Compute Canada (http://geoschemdata.computecanada.ca/ExtData/, last access: 9 September 2021). Historical meteorology has been archived for the pre-industrial era (1851–1860 CE) and recent past (2001–2014 CE). In addition, we archive near-future (2040–2049 CE) and end-of-the-century (2090–2099 CE) meteorology for seven future scenarios ranging from extreme mitigation to extreme warming (see Sect. 5 for a description of the emission scenarios). In addition, to facilitate comparison of GCAP 2.0 meteorology and composition with observations and traditional GEOS-Chem, we have also performed a recent past simulation in which the E2.1 horizontal winds of the r1i1p1f2 variant were “nudged” to match those of the MERRA-2 reanalysis for 2001–2014 CE (Menon et al., 2008). Note that we only nudge the winds and not temperature, humidity, or surface pressure as may be done in other models. We urge users to be aware of the challenges involved when interpreting the impact of nudged meteorology on atmospheric composition, especially in the stratosphere (e.g., see Orbe et al., 2020a).
GEOS-Chem (http://www.geos-chem.org, last access: 9 September 2021) is a global or regional 3-D chemical transport model traditionally driven by assimilated meteorology products produced by the NASA Global Modeling and Assimilation Office (GMAO) Goddard Earth Observing System Data Assimilation System (GEOS-DAS). These include the MERRA-2 science product, which is generated at 0.5∘ latitude by 0.625∘ longitude and 72 vertical layers extending from the surface to 0.01 hPa (∼ 38 layers in the tropical troposphere) and available from 1980 CE to the present (Gelaro et al., 2017). There is also a near-real-time product (GEOS-FP) available at 0.25∘ latitude by 0.3125∘ longitude horizontal resolution and available from 2012 CE, although with periodic changes to the underlying code. Both products are provided at hourly temporal resolution for two-dimensional fields and at 3 h resolution for three-dimensional fields1. Most GEOS-Chem users make use of these fields that have been pre-processed to coarser horizontal resolutions (4∘ latitude by 5∘ longitude or 2∘ latitude by 2.5∘ longitude)2 for computational expediency and to minimize storage requirements. Users may also select to run with reduced vertical resolution in the stratosphere (see Fig. 1).
Emissions are the subject of Sect. 5. The original description of the tropospheric chemical mechanism is by Bey et al. (2001), which was expanded to include a stratospheric mechanism by Eastham et al. (2014), the latter of which did not exist in the earlier versions of GCAP. The coupled sulfur–nitrate–ammonium aerosol simulation is described by Park et al. (2004) with aerosol thermodynamics computed via the ISORROPIA II model (Fountoukis and Nenes, 2007). Advection is handled by a flux-form and partially semi-Lagrangian transport scheme (Lin and Rood, 1996). Convective transport is parameterized as a single plume acting under the mean upward convective, entrainment, and detrainment mass fluxes for each level of a model column as archived from the GCM.
GEOS-Chem developed the capability to be driven by any horizontal resolution beginning with the “FlexGrid” update in version 12.4.0 (https://doi.org/10.5281/zenodo.3360635, The International GEOS-Chem User Community, 2019). The model can now define any horizontal resolution at initialization and automatically regrid input meteorology upon file read from its archived resolution to the runtime resolution. Because our strategy was to archive from E2.1 the same fields as in the MERRA-2 reanalysis, very few modifications were necessary to the GEOS-Chem source code to allow GEOS-Chem to use E2.1 output as a meteorological driver. The primary additional code required is the inclusion of the specification of the E2.1 vertical resolution. Otherwise, the only other GEOS-Chem changes were removing some hard-coded limitations, e.g., those that prevented the model from running on dates before 1 January 1900. These updates entered the standard GEOS-Chem code in version 13.1.0 (https://doi.org/10.5281/zenodo.4984436, The International GEOS-Chem User Community, 2021a). Version 13.0.0 of GEOS-Chem (https://doi.org/10.5281/zenodo.4618180, The International GEOS-Chem User Community, 2021c) introduced the ability of the source code to generate run directories, and version 13.1.0 has been updated to do so for GCAP 2.0. We have regridded all restart files to the new 40-layer vertical resolution.
Because of the relatively few required changes, GCAP 2.0 meteorology is easily compatible with any existing GEOS-Chem capability. There are three primary methods by which GEOS-Chem may be used. The first and most common method due to its ease of installation and application is GEOS-Chem Classic or “GCClassic”. Therefore, we have guaranteed that all GCClassic configurations work with GCAP 2.0 by including run directories and regridding all input files that have a vertical dimension. In addition to full-chemistry simulations, these include the speciality simulations (e.g., offline aerosol, methane, carbon dioxide, tagged CO, tagged methane, tagged ozone). Only the existing GCClassic mercury simulation will require some modifications; in the interest of storage, we did not archive the 10 extra sea-ice fields only used by that simulation since they may be determined online from the fraction of sea-ice field that was archived. FlexGrid also enables one to perform a global simulation at a relatively coarse resolution to archive boundary conditions for driving nested regional simulations at higher spatial resolution. Although the underlying meteorology would still be the 2∘ latitude by 2.5∘ longitude of the GCAP 2.0 meteorology, one can benefit from the finer spatial resolution of the emission inventories.
The second method of running GEOS-Chem is the Message Passing Interface (MPI) parallelized variant utilizing a cubed-sphere dynamical core known as GEOS-Chem High-Performance (GCHP, Eastham et al., 2018). GCAP 2.0 meteorology is fully compatible with GCHP, although we refer the reader to Sect. 5.2 about the necessary pre-processing of emissions for GCAP 2.0 runs using GCHP.
Lastly, there exists an adjoint of GCClassic used for inverse modeling and sensitivity applications (Henze et al., 2007). Since the adjoint presently works with MERRA-2 meteorology, the GCAP 2.0 meteorology is also compatible with the adjoint code once the vertical resolution is added, allowing for inverse modeling applications in past and future climates.
This section evaluates the GCAP 2.0 meteorology by comparing it to its original CMIP6 simulation, the CMIP6 E2.1 ensemble, and the MERRA-2 reanalysis. Model output contributed to the CMIP6 experiment is archived by an international distributed data repository powered by the Earth System Grid Federation (ESGF) and available online at https://esgf-node.llnl.gov/projects/cmip6 (last access: 9 September 2021).
Figure 2 shows the temporal evolution of annual mean surface air temperature. The black line shows the E2.1 r1i1pif2 variant and the gray shading shows the mean and 2σ spread of the submitted E2.1 ensemble from ESGF (ranging from 11 members in the historical to 1 member in some future scenarios). Our repeat simulations of the r1i1p1f2 variant from its archived restart files are shown in red and the same variant nudged to MERRA-2 is shown in blue. The MERRA-2 historical record is shown in orange.
First, we note that the repeat simulations have slightly warmer surface air temperatures than the original simulations. A small portion of this difference results from numerical noise associated with the original and repeat simulations' different computer architectures (NASA Center for Climate Simulations versus the University of Rochester Center for Integrated Research Computing). However, tests revealed that the increased frequency in calls to the radiation code necessary to archive hourly radiation fluxes for driving GEOS-Chem explains most of the difference in surface temperature. Although almost no locations show significant changes with respect to local interannual variability (see Fig. S1 in the Supplement), this does lead to a weakly but statistically different annual mean temperature with respect to the original simulation (+0.6 ∘C for 2001–2014 CE, p value = 0.002). However, the change is largely a linear offset, with temporal correlation remaining high (R=0.87 for 2001–2014 CE), providing confidence in the ability of GCAP 2.0 to produce changes in composition associated with changes in climate accurately. Nudging the winds to MERRA-2 reduces this offset by influencing the rate of mixing of air between the high latitudes and midlatitudes, and the warmer Arctic surface temperatures in our repeat free-running E2.1 simulations are in greater agreement with MERRA-2.
Second, we note that for researchers interested in studying a “Paris Agreement”-like future world, in which future warming is limited to 2 ∘C over pre-industrial levels, one may use the SSP1-1.9, SSP1-2.6, or SSP4-3.4 scenarios. However, if one wishes to study a future world with the more aggressive goal of limiting warming to 1.5 ∘C over pre-industrial levels, then the only scenario that may be used is SSP1-1.9.
Figure 3 shows the temporal evolution of the global annual mean precipitation rate in the simulations. Global precipitation rates are forecast to increase in the coming century due to the temperature-driven increase in surface evaporation and saturation vapor pressures. Unlike surface air temperature, the repeat simulations closely follow the original values and are statistically identical except in the recent past historical simulation, where they are globally higher by 0.9 %. The MERRA-2 reanalysis shows substantially more interannual variability in its global precipitation rates. Nudging E2.1 decreases the global precipitation rate.
Figures S2 to S51 of the Supplement include detailed comparisons of the seasonal climatologies for all fields in the three meteorology products that may be used to drive GEOS-Chem for 2005–2014 CE (MERRA-2, E2.1 nudged to MERRA-2, and the free-running E2.1). In general, most fields show excellent agreement with high pattern (i.e., spatial) correlation and small mean difference. However, a few fields differ between E2.1 and MERRA-2 that are of interest for chemical-transport modeling, which we now summarize. The primary difference between MERRA-2 and E2.1 is the relative importance of stratiform versus convective precipitation. Whereas both models agree on the total precipitation flux to the surface (Fig. S16), MERRA-2 has a higher rate of stratiform condensation (Fig. S33) balanced by a higher rate of stratiform re-evaporation (Fig. S45). In contrast, E2.1 has a higher rate of convective condensation (Fig. S34) balanced by a higher rate of convective re-evaporation (Fig. S44). Furthermore, E2.1 has consistently smaller surface roughness heights over the ocean and vegetated regions than MERRA-2; in contrast, MERRA-2 does not appear to include an orographic component in its surface roughness calculation and therefore has lower surface roughness heights over non-vegetated land surfaces (Fig. S29). Consequently, the E2.1 simulations have lower planetary boundary layer heights over oceans and heavily vegetated regions (globally ∼ 200 m lower; Fig. S12) relative to MERRA-2. The E2.1 simulations also have a lower tropopause pressure by approximately 40 hPa (Fig. S23); this has been corrected in version E2.2 of the GCM by moving to a higher vertical resolution (Orbe et al., 2020b). Lastly, E2.1 has a higher fraction of photosynthetically active radiation (PAR) present as diffuse (Fig. S10) rather than direct (Fig. S11) radiation, which will promote higher levels of biogenic emissions (see Sect. 5.2). Note also that MERRA-2 sets PAR fluxes to zero over water. Therefore, coastal and island cells will underestimate the radiation flux in MERRA-2-driven GEOS-Chem simulations, again with consequences for biogenic emissions.
Figure 4 compares the spatial distribution of key surface meteorological variables generated for GCAP 2.0 with their MERRA-2 counterparts. Surface air temperature shows near-perfect agreement in spatial distribution between the E2.1 products and MERRA-2. The E2.1 temperatures are slightly higher than MERRA-2, especially over the Northern Hemisphere's oceans; nudging reduces this difference as previously discussed. Total precipitation in the E2.1 fields has a weaker pattern correlation with MERRA-2 since the free-running model produces a split Intertropical Convergence Zone (ITCZ) in the eastern Pacific (a common issue in free-running GCMs; e.g., see Samanta et al., 2019); nudging the winds corrects the spatial patterns but brings the total precipitation rate out of agreement. The surface zonal wind component shows excellent agreement in their spatial patterns, although the magnitudes are greater in the E2.1 simulations relative to MERRA-2. The free-running GCM underestimates the extent of flow towards the Equator over the eastern ocean basins, which is corrected in the nudging simulation (and may be responsible for the improved ITCZ). The E2.1 simulations also lack the relatively large spatial heterogeneity seen in surface winds over the land ice sheets.
Figure 5 compares key zonal mean meteorological variables generated for GCAP 2.0 with their MERRA-2 counterparts. Lower- and free-tropospheric air temperatures are in agreement between E2.1 and MERRA-2, but the higher tropopause leads to colder temperatures in the upper troposphere with respect to MERRA-2. Nudging the winds removes some of the temperature difference in the extratropical upper troposphere but introduces differences in the free troposphere. Specific humidity agrees between E2.1 and MERRA-2 except for a drier polar free troposphere and northern extratropical surface; nudging leads to an additional drying of the stratosphere. The zonal winds agree well between all simulations, particularly between the MERRA-2 reanalysis and the nudged simulation as to be expected.
This section describes the anthropogenic emission inventories and surface boundary conditions from the CMIP6 experiment that have been processed for use by GEOS-Chem, either driven by E2.1 or MERRA-2 meteorology (Sect. 5.1). It then evaluates and compares the emission fluxes that are sensitive to meteorology between MERRA-2 and E2.1-driven GEOS-Chem simulations in the recent past (Sect. 5.2).
5.1 Anthropogenic emissions and surface boundary conditions
Figure 6 shows the time series of annual mean anthropogenic emissions and Fig. 7 shows the time series of annual mean surface boundary conditions developed for the CMIP6 experiments and processed for use in GEOS-Chem. Emissions are used for short-lived climate forcers and air pollution precursors. Surface boundary conditions are used to prescribe long-lived species like chlorofluorocarbons that are well mixed in the troposphere but may advect to and react within the stratosphere. The emissions and boundary conditions developed for the CMIP6 experiments include a historical reconstruction and several future scenarios with different target radiative forcings for the end of this century. They are hosted on ESGF under the input data sets for Model Intercomparison Projects (input4MIPs) project. They are available from https://esgf-node.llnl.gov/projects/input4mips (last access: 30 September 2020). These emissions and boundary conditions have been processed for input to GEOS-Chem/GCAP 2.0. They are consistent with those that influenced the climate of the E2.1 simulations used to generate the respective GCAP 2.0 meteorology. When users generate a GCAP 2.0 run directory, the respective CMIP6 emissions and boundary conditions for a historical or future scenario are enabled by default. However, users may always modify the Harmonized EMissions COmponent (HEMCO, Keller et al., 2014) configuration to use any emissions they desire (e.g., to use the alternative inventories, regional overwrites and/or scaling factors from the default GEOS-Chem configuration).
Historical anthropogenic emissions in CMIP6 are from the Community Emissions Data System (CEDS, Hoesly et al., 2018). For surface emissions, we processed version 2017-05-18 of the CEDS inventory available at monthly temporal and 0.5∘ spatial resolution for the eight surface sectors listed in Table 2 and the 1850–2014 CE period. CEDS is presently the default global surface anthropogenic emissions inventory used by GEOS-Chem, although only species for the full-chemistry simulation have been processed, and these emissions are overwritten for many locations by regional inventories. Here, we additionally processed the methane and CO2 fluxes for those GEOS-Chem specialty simulations. All surface emissions increased exponentially over the historical period except for sulfur dioxide (SO2), whose emissions peaked in the 1980s (Fig. S52). We also processed the three-dimensional CEDS aircraft emissions for input into GEOS-Chem as a CMIP6-compliant alternative to the Aviation Emissions Inventory Code (AEIC, Stettler et al., 2011) source that is the default in GEOS-Chem. We processed version 2017-08-30 of the CEDS aircraft inventory, available for NO, CO, black and organic carbon, SO2, and ammonia (NH3) at monthly temporal and 0.5∘ spatial resolution and 25 vertical levels of equal thickness from the surface to 15 km. We have vertically regridded to the native 40-level E2.1 resolution and the reduced stratospheric 47-level MERRA-2 resolution. Global aircraft emissions increased mostly linearly across the historical period beginning in approximately 1950 CE (Fig. S53).
In addition, we processed the biomass burning emissions from version 1.2 of the Biomass Burning for Model Intercomparison Projects (BB4MIPs) inventory (van Marle et al., 2017). The BB4MIPs reconstruction combines version 4 of the satellite-based Global Fire Emissions Database (GFED4; van der Werf et al., 2017, the default biomass burning inventory in GEOS-Chem and available since 1997 CE) with observational proxies and model simulations from the Fire Model Intercomparison Project (FireMIP) for earlier periods. BB4MIPs provides the total mass flux per species at monthly temporal and 0.25∘ spatial resolution. We have regridded to 0.5∘ spatial resolution and speciated for input to GEOS-Chem using a consistent hydrocarbon speciation scheme with CEDS. Fire emissions from BB4MIPs increase slightly across the historical period. However, interannual variability greatly increases in the second half of the 20th century (Fig. S54), driving the large interannual variability observed in the total emissions during this period (e.g., Fig. 6b).
We have prepared version 1.2.0 of the CMIP6 surface boundary conditions derived from historical observations (Meinshausen et al., 2017) and available at monthly temporal resolution and as 0.5∘ latitude bands. These have been regridded to 0.5∘ global spatial resolution for input into GEOS-Chem. Carbon dioxide, methane, and nitrous oxide have monotonically increased since the pre-industrial era due to anthropogenic activity, whereas shorter-lived stratospheric ozone-depleting substances peaked around the turn of the last century following their ban under the Montreal Protocol (Fig. 7).
5.1.2 Future scenarios
The future anthropogenic emissions and boundary conditions used by CMIP6 and processed here for GCAP 2.0 are summarized by Riahi et al. (2017). In brief, the so-named Shared Socioeconomic Pathways (SSPs) are determined from integrated assessment modeling (IAM) of five future societal narratives that may be followed to limit future warming to a target radiative forcing. The nomenclature for characterizing the SSP scenarios is SSPx-y.z (or SSPxyz), where x is the number of the future narrative (1 to 5; Table 3), and y.z represents the target radiative forcing in W m−2 at the end of the 21st century ranging from 1.9 (extreme mitigation; low warming) to 8.5 (low mitigation; extreme warming). The names of the five narratives are listed in Table 3, and each employs different assumptions about how global society would achieve the target radiative forcing. SSP1 assumes low challenges to mitigation and adaptation (van Vuuren et al., 2017), SSP2 assumes medium challenges to mitigation and adaptation (Fricko et al., 2017), SSP3 assumes high challenges to mitigation and adaptation (Fujimori et al., 2017), SSP4 assumes low challenges to mitigation and high challenges to adaptation (Calvin et al., 2017), and SSP5 assumes high challenges to mitigation and low challenges to adaptation (Kriegler et al., 2017).
For GCAP 2.0, we focus on seven scenarios corresponding to Tiers 1 and 2 of the ScenarioMIP experiment: SSP1-1.9, SSP1-2.6, SSP4-3.4, SSP2-4.5, SSP4-6.0, SSP3-7.0, and SSP5-8.5 (O'Neill et al., 2016). Assumptions about future population growth, urbanization, gross domestic production (GDP), energy, land use, and air pollution trends of the SSP IAM scenarios are described in a series of papers (Crespo Cuaresma, 2017; Dellink et al., 2017; Jiang and O'Neill, 2017; Leimbach et al., 2017; Samir and Lutz, 2017; Bauer et al., 2017; Popp et al., 2017; Rao et al., 2017). Version 1.1 of these scenarios (Gidden et al., 2019) was obtained from input4MIPs on ESGF and available at 0.5∘ spatial and monthly resolution for 2015 CE and then every 10 years beginning with 2020 CE and ending with 2100 CE. These future emissions were processed for input to GEOS-Chem in the same way as the historical emissions and boundary conditions. Linear interpolation was used to develop individual yearly emissions between the available decadal values. In addition to the sectors of Table 2, future CO2 emissions include a “neg” sector that considers negative emission (i.e., carbon capture).
From the perspective of the simulated climate, the forcing that dominates the end-of-the-century response is the CO2 abundance. Therefore, CO2 is the only gas that monotonically increases with future forcing target values (Fig. 7a). The trajectories of the remainder of the well-mixed greenhouse gases, stratospheric ozone-depleting substances, short-lived climate forcers, and air-pollution precursors vary between the SSP scenarios and target forcings (Figs. 6 and 7b–l). For example, methane in 2100 CE is highest in the SSP3-7.0 scenario, not SSP5-8.5 (Fig. 7b). Because ammonia is primarily produced from agriculture and the world population will continue to grow, it is the only emission expected to remain constant or grow into the future. Otherwise, the narrative assumptions strongly influence the global and regional emission changes. Furthermore, we note that the historical emissions inventories have large amounts of interannual variability (primarily due to biomass burning), whereas the SSP scenarios have very low interannual variability. This highlights the necessity for CTM studies such as those that may be accomplished by GCAP 2.0 that can explore the impact of a wider range of future emission trajectories on air quality, short-lived climate forces, and stratospheric ozone in future warmer climates whose meteorology is primarily driven by changes in CO2. It also highlights the necessity for performing simulations long enough to establish robust statistics for chemistry–climate interactions (e.g., Garcia-Menendez et al., 2017).
5.2 Natural emissions
Figure 8 shows the climatological mean emission fluxes for key species whose emissions are sensitive to meteorology. Figures S55–S60 in the Supplement provide seasonal details for each species.
Emission fluxes sensitive to meteorology and thereby grid resolution began to be pre-processed offline at high spatial resolution in version 12.4.0 of GEOS-Chem. This was to facilitate the calculation of consistent emissions between the various cubed-sphere geometries of the GCHP variant of the model (Eastham et al., 2018, see Sect. 3.2), although the option to calculate these emissions online was maintained through online extensions in the HEMCO processing code (Keller et al., 2014). The default behavior for GCAP 2.0 is to use online calculations to respond to the underlying climate. Users who wish to run GCHP with GCAP 2.0 may quickly pre-process offline natural emission fluxes using the “standalone” version of HEMCO with a HEMCO_Config.rc file from a GCClassic version of GCAP 2.0. Here, we compare the online emission fluxes in our MERRA-2-driven simulation to those of our E2.1-driven simulations.
Panels a–c of Fig. 8 show the spatial distribution of isoprene from terrestrial plants. Emissions of non-methane hydrocarbons (NMHCs) from terrestrial plants follow version 2.1 of the Model of Emissions from Gases and Aerosols from Nature (MEGAN), which responds positively to changes in diffuse photosynthetically active radiation (PAR), recent surface air temperature, and soil root wetness (Guenther et al., 2012). There is an option for emissions to respond to CO2 abundance as well (Tai et al., 2013). Because E2.1 has a greater proportion of PAR present as diffuse radiation, isoprene emissions in E2.1-driven simulations are about 40 % higher than in the MERRA-2-driven simulation.
Panels d–f of Fig. 8 show a very tight agreement in the spatial pattern and magnitude of the flux of dimethylsulfide (DMS; (CH3)2S) produced by marine phytoplankton. Emissions of NMHCs from marine environments are represented as the product of prescribed seawater concentration distributions and sea-to-air transfer velocities calculated via the parameterization of Nightingale et al. (2000a, b). The latter respond to sea-surface temperatures and surface wind velocities.
Panels g–i of Fig. 8 compare the source of mineral dust between the simulations. We use the Dust Entrainment and Deposition (DEAD) scheme for mineral dust evasion (Zender et al., 2003), which responds to changes in surface friction velocity (u*), roughness height, snow/ice cover and depth, soil wetness, pressure, specific humidity, and temperature. Dust mobilization was found in our tests to be extremely sensitive to the meteorology product used, with poor spatial correlation (R≤0.26) and with each meteorology product yielding a different order of magnitude in its global total. Therefore, we have determined respective scaling factors for the E2.1 simulations that bring the present-day global total into agreement with the MERRA-2-driven value. These are included by default in the GCAP 2.0 run directories for the DEAD dust scheme.
Panels j–l of Fig. 8 show the source of sea-salt aerosol. The sea-salt mobilization scheme is described by Jaeglé et al. (2011) and responds to sea-surface temperature, surface wind velocity, and the fraction of sea-ice coverage. There is an excellent agreement between each source's spatial distributions, although the stronger surface winds in E2.1 lead to 15 %–20 % higher emissions in the E2.1 simulations, especially over the Southern Ocean.
Panels m–o of Fig. 8 show the column-integrated source of NO from lightning. In MERRA-2, lightning flash densities (flashes km−2 s−1) are pre-calculated offline from MERRA-2 convective cloud depths at 0.5∘ latitude by 0.625∘ longitude spatial and 3 h temporal resolution. These densities are then input as a meteorological parameter to GEOS-Chem, from which vertical profiles of NO production are determined following Murray et al. (2012). For the GCAP 2.0 meteorology, flash rates are calculated online in the E2.1 moist convection code following the description in Kelley et al. (2020) and archived at E2.1 native spatial and hourly temporal resolution for input as a meteorological parameter to GEOS-Chem (see Sect. 4). Both lightning flash density calculations are ultimately based on the same cloud-top height scheme of Price and Rind (1992) and global mean lightning flash rates are tuned to climatology in the recent past (Cecil et al., 2014). However, because the spatial and seasonal climatology in the MERRA-2-driven simulations is constrained by satellite observations (Murray et al., 2012), which is not appropriate for a free-running GCM, the spatial patterns differ between the simulations. Therefore, E2.1 overestimates the fraction of lightning in the tropics with respect to the extratropics and puts too much lightning over South America and Oceania and not enough over Africa. It is also worth emphasizing that we do not know how lightning has changed since the pre-industrial era or will change in a warming world (e.g., Williams, 2005; Price, 2013; Murray, 2016, 2018; Finney et al., 2018).
Panels p–r of Fig. 8 show the source of NO from soil microbial activity. The parameterization is described by Hudman et al. (2012) and responds to surface air temperature, wind speed, soil wetness, cloud fraction, downwelling shortwave radiation, and snow/ice cover. To a lesser degree, lightning can also influence the soil NO source through its impact on nitrate deposition to the soils. The spatial correlation is excellent between the different sources, although the E2.1 magnitude is higher by about 40 %.
Lastly, we note the important and variable geologic source of SO2. Volcanic emissions of SO2 in GEOS-Chem are normally prescribed from the Aerosol Comparisons between Observations and Models (AeroCom) point-source inventory (Carn et al., 2015), with data available since 1978 CE. The CMIP6 experiment did not provide historical or future emission fluxes for volcanism. Instead, input4MIPs provided time series of stratospheric aerosol surface area densities and effective radii with which to force the GCMs. Therefore, when users generate a GCAP 2.0 run directory, they are given the option to select a fixed historical AeroCom year from which to prescribe their volcanic emissions.
This section evaluates the performance of GCAP 2.0 driven by E.21 versus MERRA-2 meteorology for the recent past through comparison with observations. We first evaluate model physics and transport using the “TransportTracers” variant of GEOS-Chem (Sect. 6.1). We then evaluate the standard full-chemistry mechanism (Sect. 6.2).
All simulations were performed at 4∘ latitude by 5∘ longitude horizontal resolution for the period 2001–2014 CE, with meteorology respectively prescribed from MERRA-2, E2.1 nudged to MERRA-2, and the free-running E2.1 simulation. All simulations used version 12.9.3 of GEOS-Chem (https://doi.org/10.5281/zenodo.3974569, The International GEOS-Chem User Community, 2020) with modifications as described throughout the paper. The E2.1 meteorology fields were regridded from their native resolution upon input to GEOS-Chem by FlexGrid. The E2.1 simulations used the native 40-layer resolution and the MERRA-2 simulations used the 47-layer reduced-stratospheric resolution (see Fig. 1). Identical initial conditions were regridded to each model's respective vertical resolution. The first 4 years of each simulation were discarded as initialization, with the remaining 10 years used for evaluation and statistics. All prescribed emissions were identical between each simulation.
Model transport and physical processes may be evaluated against observations using the “TransportTracers” variant of GEOS-Chem. We focus on four tracers of particular utility: sulfur hexafluoride (SF6), radon-222 (222Rn), lead-210 (210Pb), and beryllium-7 (7Be).
Sulfur hexafluoride is a trace gas of anthropogenic origin that is chemically and physically inert on human timescales (lifetime of 3200 years). It is primarily emitted at the surface in the Northern Hemisphere (Maiss and Brenninkmeijer, 1998). Its meridional gradient may be used to test the rate of interhemispheric mixing (Rigby et al., 2010; Hall et al., 2011) and its vertical gradients may be used to infer the age of air in the stratosphere (Waugh and Hall, 2002; Waugh, 2009). Its meridional gradients may also be used to infer the tropospheric age of air (Waugh et al., 2013). Here, we use emissions from version 4.2 of the Emissions Database for Global Atmospheric Research (EDGAR), available at 0.1∘ global resolution for 1970–2008.
Terrigenic 222Rn is an inert, insoluble, short-lived (half-life of 3.8 d) noble gas produced from the slow decay of 226Ra (half-life of 1600 years) found in uranium ores. Its evasion from surface soils is relatively uniform and constant and is as described by Jacob et al. (1997). Its insolubility and timescale of decay make it a useful tracer for diagnosing quick vertical mixing within atmospheric models from boundary layer processes and moist convection (e.g., Allen et al., 1996; Brost and Chatfield, 1989; Considine et al., 2005; Feichter and Crutzen, 1990; Hauglustaine et al., 2004; Jacob and Prather, 1990; Jacob et al., 1997; Lambert et al., 1982; Mahowald et al., 1995; Stockwell et al., 1998).
Radiogenic 210Pb is the chemically inert decay product of 222Rn. It is readily taken up by submicron aerosol particles and subsequently removed from the atmosphere by deposition or decay (Bondietti et al., 1988; Maenhaut et al., 1979; Preiss et al., 1996; Sanak et al., 1981). Because of its relatively long lifetime (half-life of 22.2 years), nearly all 210Pb is removed via deposition. As its source from 222Rn is relatively well known, and there is a global and long-term surface deposition flux inventory (Preiss et al., 1996), it is the standard test for model deposition.
Cosmogenic 7Be is produced by cosmic-ray spallation of N2 and O2, predominantly in the polar upper troposphere and lower stratosphere (Lal et al., 1958). The source of 7Be is updated for this work to use the parameterization of Usoskin and Kovaltsov (2008). Mean solar activity is assumed (solar modulation potential Φ = 670 MV), leading to an average production rate of 0.065 atoms cm−2 s−1; about 60 % in the stratosphere and 40 % in the troposphere. Like 210Pb, 7Be is rapidly taken up by submicron aerosol particles (Bondietti et al., 1988; Maenhaut et al., 1979; Papastefanou, 2009; Papastefanou and Ioannidou, 1996; Sanak et al., 1981). It is subsequently transported until removal by deposition or radioactive decay (half-life of 53.3 d). 7Be has been used to constrain vertical transport, wet deposition fluxes, and stratosphere–troposphere exchange in models (e.g., Allen et al., 2003; Brost et al., 1991; Koch et al., 1996; Liu et al., 2001, 2016; Barrett et al., 2012).
Table 4 gives the atmospheric budget of the three radionuclides driven by the three meteorological products.
6.1.1 Horizontal mixing
Figure 9 shows observed meridional and vertical gradients of SF6 with respect to Cape Matatula, American Samoa (SMO), in the remote tropical southern Pacific. The observations are version 2.1.1 of the NOAA Carbon Cycle Group SF6 ObsPack (https://doi.org/10.25925/20180817, NOAA Carbon Cycle Group ObsPack Team, 2018) and represent a mixture of surface in situ, flask, tower, and aircraft sources from 2005–2014 CE. Observations were aggregated at model spatial and monthly temporal resolution, compared to that month's SMO value, from which zonal climatologies were determined. Also shown is the value of each simulation sampled and processed as in the observations. In all simulations, GEOS-Chem underestimates the cross-equatorial meridional gradient by 17 %–26 %, an improvement over GEOS-Chem driven by earlier meteorology products (see Supplement of Murray et al., 2014). However, this suggests that the interhemispheric mixing rate in the model is too fast and/or that the EDGAR inventory underestimates the emission growth rate in the Northern Hemisphere relative to the Southern Hemisphere. Meanwhile, meridional mixing rates in the Southern Hemisphere are consistent with the observations in all simulations. The E2.1 simulation slightly better matches the cross-equatorial gradient than the MERRA-2 and nudged simulations, but E2.1 greatly underestimates the lower stratospheric gradient (see Sect. 6.1.3).
6.1.2 Vertical mixing – troposphere
We assess vertical mixing within the troposphere using vertical profiles of 222Rn and the ratio of 7Be to 210Pb in surface air.
Figure 10 shows simulated climatological 222Rn profiles sampled at the month and location of the available observations, also plotted. Observations are scarce and available only at northern extratropical continental locations (Bradley and Pearson, 1970; Nazarov et al., 1970; Wilkening, 1970; Moore et al., 1973; Kritz et al., 1998). In an overly convective atmosphere, the vertical gradient of 222Rn would disappear. There is a slight overestimate of 222Rn abundance within the boundary layer and underestimate above in all of our simulations, implying a small underestimate in boundary layer ventilation. Our results are comparable to or better than other atmospheric models (e.g., see Fig. 5 of Considine et al., 2005).
Figure 11 shows the annual mean surface mixing ratios of 7Be, 210Pb and their ratio in our simulations. Since 7Be is produced in the upper troposphere/lower stratosphere and 210Pb is produced near the surface, and because the ratio of 7Be to 210Pb is unaffected by deposition, the ratio serves as a useful measure for tropospheric vertical mixing (Koch et al., 1996). A persistent high bias would indicate excessive downward transport and/or insufficient upward transport, assuming no bias in either source. The left column shows the climatological long-term data from the surface monitoring stations of the DOE Environmental Measurements Laboratory (EML) Surface Air Sampling Program (SASP) (obtained from https://www.wipp.energy.gov/namp/emllegacy/databases.htm, last access: 15 January 2021). SASP recorded the spatial and temporal distribution of various radionuclides in surface ambient air from 1957 until 1999 CE, including 7Be and 210Pb. For comparison with our simulations, we select data from periods of average solar activity (solar modulation potential Φ = 670 ± 50 MV from the Usoskin et al., 2005 reconstruction). All simulations show only minor biases in surface abundance in either 7Be and 210Pb. The 7Be to 210Pb ratio shows tight agreement between the different model simulations, with the E2.1 simulation slightly outperforming the MERRA-2-driven simulation relative to the observations.
6.1.3 Vertical mixing – stratosphere
Figure 12 shows the simulated zonal climatology of the age of air in the stratosphere, which is defined as the mean time since an air mass at a given location was last in the troposphere (Hall and Waugh, 2000). Age of air increases away from the equatorial tropopause where most tropospheric air enters the stratosphere (Holton et al., 1995). We determine age of air by using SF6 as a chronological tracer (e.g., Waugh and Hall, 2002) to determine the average temporal lag between a mixing ratio at a given location in the stratosphere relative to the tropical tropopause for the period 2005–2014 CE.
Models traditionally underestimate the stratospheric age of air implied by observations, which increases up to 7 years by 35 km in the poles (Waugh and Hall, 2002). All three of our simulations, including the MERRA-2 reanalysis, underestimate the age of air. E2.1 has the youngest air, with values consistent with those determined online within the GCM and reported by Orbe et al. (2020b). E2.1 nudged to MERRA-2 has the oldest air but is still only about two-thirds of what observational constraints suggest they should be and remain difficult to interpret given the challenges of nudged simulations (e.g., Orbe et al., 2020a). The young age in E2.1 results from too strong an ascent in the tropical pipe and a relatively leaky lower branch of the Brewer–Dobson circulation (e.g., Ray et al., 2010); updates to version E2.2 of the GISS GCM greatly improve the stratospheric circulation (Orbe et al., 2020b) and will be included in future GCAP 2.0 meteorology products and scenarios.
6.1.4 Stratosphere–troposphere exchange
Beryllium-7 has often been used as a tracer of downward transport from the stratosphere (Dibb et al., 1992, 1994; Husain et al., 1977; Rehfeld and Heimann, 1995; Sanak et al., 1985; Viezee and Singh, 1980) and as an indicator of stratosphere–troposphere exchange (STE) performance within global atmospheric models (Allen et al., 2003; Liu et al., 2001, 2016; Barrett et al., 2012; Murray et al., 2014).
Figure 13 shows the annual zonal fraction of 7Be of stratospheric origin in each simulation. Using E2.1 (MERRA-2) meteorology, we find that 23 % (30 %) of annual average surface 7Be abundance from 38–51∘ N is of stratospheric origin, slightly lower (higher) than the observational constraint of 25 % reported by Dutkiewicz and Husain (1985). This is a dramatic improvement over the earlier GCAP/ICECAP studies in which the stratospheric downwelling source in the E2.1-driven simulations was greatly overestimated (Murray et al., 2014) and was also seen in the NASA Global Modeling Initiative (GMI) CTM driven by GISS Model II' meteorology (Liu et al., 2016). This possibly reflects improvements in downward mass flux in the GCM associated with the increase in vertical resolution (Fig. 1) and updates to the GEOS-Chem dynamical core code that occurred since the original GCAP/ICECAP.
Figure 14 (top row) compares the simulated wet deposition flux of 210Pb in each simulation to the observational values reported by Preiss et al. (1996) aggregated to model resolution. Wet deposition of 210Pb in all simulations is biased low by ∼ 20 % in all simulations, consistent with earlier versions of GEOS-Chem (Murray et al., 2014). These results imply a low bias in the 210Pb source (and therefore 222Rn emission) or a high bias in the dry deposition flux in all simulations.
Figure 14 (bottom row) compares the simulated wet deposition fluxes of 7Be to the few observations that exist (Baskaran et al., 1993; Bleichrodt, 1978; Brown et al., 1989; Dibb, 1989; Du et al., 2008; Harvey and Matthews, 1989; Hasebe et al., 1981; Hirose et al., 2004; Igarashi et al., 1998; Narazaki and Fujitaka, 2010; Nijampurkar and Rao, 1993; Olsen et al., 1985; Papastefanou et al., 1995; Schuler et al., 1991; Turekian et al., 1983; Wallbrink and Murray, 1994, and references therein). The wet deposition flux is increased in the E2.1 simulation with respect to the MERRA-2 simulation, particularly over the midlatitude oceans, and is the closest simulation to matching the observations.
We find a tropospheric residence time for 210Pb-containing aerosols against deposition of 8.3 d in MERRA-2 versus 8.8 d in the E2.1 simulations (Table 4), an improvement in consistency with respect to GCAP/ICECAP, and within the range of previous estimates of 6.5–12.5 d (Turekian et al., 1977; Lambert et al., 1982; Balkanski et al., 1993; Koch et al., 1996; Guelle et al., 1998b, a; Liu et al., 2001). We find a similar relative increase in the lifetime of 7Be-containing aerosols of 19.7 d versus 21.7 d, also consistent with earlier findings of 23 d (Koch et al., 1996) and 21 d (Liu et al., 2001). Whereas wet deposition in MERRA-2-driven simulations is primarily due to stratiform clouds, it is primarily due to convective clouds in E2.1-driven simulations, consistent with the meteorological fields (see Sect. 4) and leading to the longer residence times in the E2.1 simulations.
Next, we evaluate the “standard” full-chemistry simulation of version 12.9.3 of GEOS-Chem driven by the three meteorology products for 2005–2014 CE. The standard mechanism contains a unified chemical mechanism of ozone–NOx–hydrocarbon–halogen–aerosol chemistry from the surface to the mesopause (Bey et al., 2001; Park et al., 2004; Eastham et al., 2014; Wang et al., 2019). As of version 12.9.3, this includes 255 interactive species, 597 gas-phase reactions, 101 heterogeneous reactions, and 153 photolysis reactions. All our simulations use identical prescribed emissions from the CMIP6 experiments as described in Sect. 5.1 (as opposed to the default GEOS-Chem anthropogenic inventories) and natural emissions vary with each model meteorology as described in Sect. 5.2. Volcanic emissions of SO2 from 2005 were used in all simulation years.
6.2.1 Hydroxyl radical
Table 5 assesses hydroxyl radical (OH) concentrations in the model by comparing the simulated lifetime of relatively long-lived molecules whose main sink is tropospheric OH with observational constraints. It is common for atmospheric models to be biased high with respect to OH in these observational constraints (i.e., low with respect to lifetime, e.g., Naik et al., 2013; Voulgarakis et al., 2013), which is true as well in our three simulations. However, the lifetime of methyl chloroform (CH3CCl3) and methane in the E2.1 simulations is statistically consistent with the low end of the observed constraint of years and years from Prinn et al. (2005), respectively. All simulations fall within the multi-model estimates of a tropospheric methane lifetime of 10.2 ± 1.7 years (Fiore et al., 2009) and 9.8 ± 1.6 years (Voulgarakis et al., 2013) but fall short of the observationally derived estimates of 11.2 ± 1.3 years from Prather et al. (2012). In all simulations, the E2.1 simulations better match the observational constraints. The E2.1-driven simulations in the tropics have thinner overhead ozone columns (see Sect. 6.2.4), greater free-tropospheric water vapor abundances, and greater lightning NO emissions (see Fig. 8), all of which promote increased OH (e.g., Murray et al., 2014), so their lower OH may reflect their higher biogenic NMHC emissions (Fig. 8).
a Prinn et al. (2005) for CH3CCl3 and Prather et al. (2012) for CH4. b 2005–2014 CE annual mean and standard deviation.
6.2.2 Oxidized nitrogen
Table 6 gives the tropospheric budget for total reactive nitrogen (NOy) in all three simulations, which includes NOx (≡ NO + NO2) and its longer-lived reservoir species such as nitric acid (HONO2) and peroxyacetyl nitrate (CH3C(O)OONO2; PAN). The E2.1 simulations have greater total sources of NOy because of the larger natural sources from lightning and soils (see Sect. 5.2) and a greater flux of NOy transported from the stratosphere from the products of nitrous oxide (N2O) oxidation. The NOy speciation between family members is largely consistent between the simulations. The lifetime of NOy in the nudged E2.1 simulation is longer than in the free-running E2.1 simulation, reflecting the reduction in that simulation's global mean precipitation flux.
a NOy ≡ .
b RONO2 ≡ .
Panels a–d of Fig. 15 compare the spatial distribution of tropospheric columns of nitrogen dioxide (NO2) for 2005–2014 CE from version 3 of the OMNO2d product from the Ozone Monitoring Instrument (OMI) on the Aura satellite (https://doi.org/10.5067/Aura/OMI/DATA3007, Krotkov et al., 2019, 2017) to the three simulations. Figure S61 in the Supplement provides seasonal details. The simulations have been sampled at the satellite's overpass time and the tropopause was determined online within the model following the thermal definition is used to calculate the partial columns. All simulations well reproduce the spatial distribution of tropospheric NO2 (all R≥0.94) and have small global mean low biases but statistically disagree with the satellite product in the subtropical latitudes. The subtropical disagreement is potentially due to uncertainties in the tropopause height between the various products. Tropospheric columns match over East Asia during this period but are underestimated over North America and Europe.
6.2.3 Reduced carbon
Table 7 gives the tropospheric emissions and lifetimes for key reduced carbon species in all three simulations. Species primarily emitted from terrestrial plants such as isoprene and monoterpenes have higher emission rates in E2.1 due to the higher diffuse radiation fluxes than in MERRA-2 (see Sects. 4 and 5.2). Species that are primarily lost via oxidation by OH, such as isoprene, have shorter lifetimes in E2.1 due to the higher OH abundances (see Table 5). In contrast, soluble species such as methanol have longer atmospheric lifetimes in E2.1 due to the lower large-scale stratiform precipitation rates in E2.1 relative to MERRA-2.
Annual mean and standard deviation. The percentage of total emission is given per biogenic source.
Panels e–h of Fig. 15 compare total columns of formaldehyde (HCHO) from version 3 of the OMHCHOd product from OMI on the Aura satellite (https://doi.org/10.5067/Aura/OMI/DATA3010, Chance, 2019; González Abad et al., 2015) to the three simulations for 2005–2014 CE. Figure S62 in the Supplement provides seasonal details. The simulations have been sampled at the overpass time of the satellite. Formaldehyde is a common product of hydrocarbon oxidation. Despite higher mean values over the continents, all three simulations are statistically consistent with respect to the large amount of interannual variability in the simulated and observed HCHO columns. There is strong spatial correlation between the simulations and the satellite product (all R≥0.8). Terrestrial columns simulated by the E2.1 simulations are higher than the MERRA-2 simulations, reflecting the higher biogenic emissions. All simulations underestimate HCHO columns over the remote ocean aside from the continental outflows of North America and Asia and over the Arctic.
Annual mean and standard deviation. The percentage of the total is given per source and sink.
Table 8 gives the tropospheric budget for carbon monoxide (CO) in all three simulations. The direct emissions of CO from anthropogenic and biomass burning sources between the three simulations are identical by experimental design. However, the chemical source of CO from methane and non-methane hydrocarbon oxidation is higher in the E2.1 simulations due to the higher OH abundances (Table 5). This is balanced by the increased chemical loss of CO by OH. The influence of OH on CO production from short-lived non-methane hydrocarbon species seems to outweigh the influence on CO loss, and consequently there are slightly longer CO tropospheric lifetimes in the E2.1 simulations.
Panels i–l of Fig. 15 compare CO mixing ratios at 500 hPa from version 7 of the AIRX3STD product from the Atmospheric Infrared Sounder (AIRS) on the Aqua satellite (https://doi.org/10.5067/8XB4RU470FJV, AIRS project, 2019; Tian et al., 2020) to the three simulations for 2005–2014 CE. Figure S63 in the Supplement provides seasonal details. The simulations have been sampled at the overpass time of the satellite. All simulations have strong spatial correlation with the observations (R=0.93). CO in the free troposphere is higher in the E2.1 simulations, consistent with its longer lifetime (Table 8). The E2.1 simulations are globally biased high by 15 % compared to the AIRS values. However, they are statistically consistent almost everywhere with respect to the large amount of interannual variability in the observations and simulations. In contrast, the MERRA-2 simulations are globally biased low by 5 % and significantly so throughout the tropics and Southern Hemisphere. All models underestimate the curious enhancement of CO seen in the AIRS climatology over Antarctica.
Table 9 gives the tropospheric budget for the odd-oxygen family (Ox ≡ O3 + rapid cycling species) for all three simulations. The individual budget terms are all are consistent with the range of reported values from the Tropospheric Ozone Assessment Report (TOAR) multi-model assessment (see Fig. 3 of Young et al., 2018), the CMIP6 models that performed interactive tropospheric chemistry (Griffiths et al., 2021), as well as the last extensive tropospheric ozone budget evaluation within the standard GEOS-Chem model (Hu et al., 2017). The E2.1 simulations are on the high end of the previously reported values due to the higher tropopause height in those simulations; the upper troposphere and lower stratosphere regions contribute strongly to each Ox budget term due to the rapidly increasing abundances of ozone with altitude there. We point out that the stratosphere-to-troposphere flux calculated using the “residual method” of the other budget terms yields consistent results when we track the mass flux of ozone across the dynamic tropopause in the model. Relative to the earlier GCAP and ICECAP simulations (Murray et al., 2014), the transport of ozone from the stratosphere is dramatically improved.
∗ Ox ≡ .
A molar mass of 48 g is assumed for Ox.
Figure 16 evaluates the zonal and seasonal distribution of ozone versus in situ measurements. We use the ozonesonde measurements archived by the World Ozone and Ultraviolet Radiation Data Centre (WOUDC) of the World Meteorological Organization/Global Atmosphere Watch Program (WMO/GAW). The data were accessed on 4 November 2019 from https://doi.org/10.14287/10000001 (WMO/GAW, 2019). All models fall within the variability of the measurements, except the free troposphere of the northern extratropics, where the simulations are biased low, especially during the summer months. The MERRA-2 simulations better reproduce the seasonality of ozone in the tropical free and upper troposphere, likely reflecting the climatologically constrained lightning NO source in that version (see Sect. 5.2).
Figure 17 evaluates spatial distributions of ozone in the three simulations against surface in situ and satellite observations. The top row shows the annual average surface ozone mixing ratio in ppbv (≡ nmol mol−1) from our simulations versus the gridded mean non-urban surface ozone product from the Tropospheric Ozone Assessment Report (TOAR) (https://doi.org/10.1594/PANGAEA.876108, Schultz et al., 2017b, a). The middle row shows tropospheric columns of ozone (TCO; in Dobson units) versus the joint Ozone Monitoring Instrument (OMI) and Microwave Limb Sounder (MLS) product from the Aura satellite (Ziemke et al., 2006). The bottom row shows total ozone columns (TOCs; in Dobson units) versus the OMDOAO3e product from OMI (https://doi.org/10.5067/Aura/OMI/DATA3005, Veefkind, 2012; Dobber et al., 2006). All observational products have been aggregated to model resolution for comparison. In the case of the satellite products, we sampled the model at the overpasses' time and location. We use the online thermal lapse rate tropopause to calculate TCO. Seasonal details are given in Figs. S64–S66 of the Supplement.
All simulations are biased high by 15 %–17 % with respect to surface ozone, mostly driven by the eastern North American data. The E2.1 simulations are especially higher over the Amazon than either MERRA-2 or the observations. Comparisons of TCO to OMI/MLS are sensitive to uncertainties in the tropopause location in the satellite product versus the models (Griffiths et al., 2021). The E2.1 TCOs are globally higher than the OMI/MLS product by 12 %, reflecting the lower tropopause pressures. However, the only locations in which it is statistically different regarding interannual variability are over the tropical oceans, where it is biased low. This likely reflects the more vigorous convection in E2.1 that leads to ozone destruction (e.g., Murray et al., 2013). Tropospheric columns in MERRA-2 match the global mean from OMI/MLS but also underestimate the western Pacific and additionally underestimate northern extratropical ozone. All simulations underestimate tropospheric columns in the southern extratropics with respect to OMI/MLS. The models all show excellent agreement with respect to total ozone columns with small positive mean global biases of 4 % and high pattern correlation (all R≥0.96). Total ozone in the tropics is higher in MERRA-2 than E2.1, consistent with differences in the rate of vertical ascent in the tropical pipe implied by the stratospheric age of air comparison (see Sect. 6.1.3). The E2.1 simulation overestimates Antarctic ozone relative to MERRA-2 or the nudged simulation, although not significantly compared to interannual variability.
6.2.5 Particulate matter
Figure 18 evaluates the spatial distribution of particulate matter in the three simulations against satellite observations. The top row shows the simulated concentration of fine particulate matter under 2.5 µm (PM2.5) in µg m−3 versus the historical reconstruction from Hammer et al. (2020). The middle row shows the total aerosol optical thickness (AOT) at 550 nm (unitless) in the simulations versus the combined Dark Target and Deep Blue AOT at 0.55 µm from Collection 6.1 of the MODerate resolution Imaging Spectroradiometer (MODIS) MYD08 product from the Aqua satellite (https://doi.org/10.5067/MODIS/MYD08_M3.061, Platnick et al., 2015). The bottom row shows the total column of sulfur dioxide (SO2) in Dobson units in the simulations versus the second public release of version 3 of the OMSO2e product from OMI on the Aura satellite (https://doi.org/10.5067/Aura/OMI/DATA3008, Li et al., 2020b, a). The model has been sampled at the time of the Aura and Aqua overpasses for comparison to the satellite products. Figures S67–S68 of the Supplement provide seasonal details for AOT and the SO2 columns.
Surface PM2.5 agrees between the simulations and Hammer et al. (2020) over heavily industrialized regions. However, we note that the Hammer et al. (2020) product used ratios of surface PM2.5 to AOT from GEOS-Chem to generate their proxy reconstruction from satellite AOT measurements, so it is not an entirely independent comparison. Surface concentrations are underestimated almost everywhere else in all simulations, especially in regions heavily influenced by mineral dust and biomass burning. The same story is reflected in the MODIS AOT, except the stronger sea-salt aerosol emission in the E2.1 simulations yielding better comparison in the Southern Ocean and portions of the Pacific. Simulated total columns of sulfur dioxide are underestimated everywhere in all simulations except over East Asia and the locations of the major volcanic eruptions of 2005 (Sierra Negra in the Galápagos and Anatahan of the Northern Mariana Islands).
This paper described and evaluated version 2.0 of the Global Change and Air Pollution (GCAP) chemical-transport model framework.
GCAP 2.0 is a one-way offline coupling between the E2.1 version of the NASA GISS GCM frozen for the CMIP6 experiments (Kelley et al., 2020; Miller et al., 2021) and the GEOS-Chem 3-D chemical-transport model (http://www.geos-chem.org, last access: 9 September 2021; Bey et al., 2001). Additional subdaily diagnostics were added to E2.1 to archive the same fields as the MERRA-2 reanalysis product (Gelaro et al., 2017) that is normally used to drive GEOS-Chem. We then re-performed one of the atmosphere-only members of the E2.1 contributions to the CMIP6 ensemble, archiving the meteorology necessary for driving GEOS-Chem. The E2.1 meteorology is available at 2∘ latitude by 2.5∘ longitude and for 40 vertical layers ranging from the surface to 0.1 hPa. At publication time, meteorology is available for the pre-industrial era (1851–1860 CE) and recent past (2001–2014 CE), including a recent-past simulation nudged to MERRA-2 to assist users in comparing with observations. Also available is meteorology for the near future (2040–2049 CE) and the end of the century (2090–2099 CE) for seven future SSP scenarios ranging from extreme mitigation (SSP1-1.9) to extreme warming (SSP5-8.5). In addition, the CMIP6 emissions and surface boundary conditions (Hoesly et al., 2018; van Marle et al., 2017; Riahi et al., 2017; Meinshausen et al., 2017; Gidden et al., 2019) have been processed for input into GEOS-Chem. GCAP 2.0 is operational in all current variants of the GEOS-Chem model, with all GCClassic run directories and input files provided. All GCAP 2.0 input data are publicly served at http://atmos.earth.rochester.edu/input/gc/ExtData/ (last access: 9 September 2021).
The meteorology was evaluated by comparing to both the original simulation and the MERRA-2 reanalysis for the recent past. Surface air in the repeat simulation is slightly warmer than the original run due to increased calls to the radiation code necessary for archiving shortwave fluxes for input to GEOS-Chem. The E2.1 climatology in the recent past largely agrees with the MERRA-2 climatology for that period, with the primary difference being in the relative amount of precipitation in stratiform versus convective clouds as well as a higher tropopause height in E2.1. Emissions that respond to meteorology in GEOS-Chem are slightly higher in the E2.1-driven simulations, including biogenic emissions from terrestrial plants, the lightning and soil microbial sources of reactive nitrogen, and sea-salt evasion. The dust mobilization parameterization was found to be extremely sensitive to resolution and meteorology, and scaling factors have been determined to constrain the global source.
Model physics and transport were evaluated using simulations and observations of sulfur hexafluoride and radionuclides. In all cases, transport is substantially improved over the original GCAP, and the E2.1-driven simulations perform comparably to the MERRA-2-driven simulations. Most importantly, whereas age of air remains too young in both E2.1 and MERRA-2, the stratosphere-to-troposphere mass flux now yields comparable values, with consistent stratosphere-to-troposphere fluxes of ozone with multi-model means. This is a major improvement over the previous versions of GCAP (Wu et al., 2007; Murray et al., 2014). However, we urge users to be cautious when using these fields for stratospheric chemistry–climate applications. Future simulations will provide CMIP6 meteorology from the 102-layer version of the GISS GCM (E2.2, Rind et al., 2020), which will be better suited for studies of the middle atmosphere; E2.2 includes an interactive quasi-biennial oscillation and improved polar vortex variability including sudden warmings, which could contribute additional dynamical variability that GEOS-Chem may otherwise not see (Orbe et al., 2020b).
Lastly, the chemistry of the model using the CMIP6 emissions and the different meteorology was evaluated against a suite of satellite products and in situ observations. The E2.1-driven simulations have lower OH and therefore more accurate methyl chloroform and methane lifetimes. Greater biogenic fluxes yield greater abundances of oxidation products (e.g., CO) in the E2.1-driven simulations, improving comparison with observations in the Southern Hemisphere. However, the MERRA-2-driven simulations have a superior representation of free-tropospheric ozone, likely due to the constrained lightning seasonality and distribution as well as the more realistic tropopause pressure in those simulations. All simulations underestimate particulate matter abundances outside of industrialized areas and AOT in most places. Otherwise, model performance was very similar in all simulations.
GCAP 2.0 entered the public GEOS-Chem repository in version 13.1.0 (https://doi.org/10.5281/zenodo.4984436, The International GEOS-Chem User Community, 2021a; https://doi.org/10.5281/zenodo.4984639, The International GEOS-Chem User Community, 2021b; https://doi.org/10.5281/zenodo.4984437, Lundgren et al., 2021). Source code for generating E2.1 output to drive GEOS-Chem is available at https://doi.org/10.5281/zenodo.4783672 (Murray et al., 2021). Archived meteorology, emissions, and boundary conditions for GCAP 2.0 are hosted online at http://atmos.earth.rochester.edu/input/gc/ExtData/ (last access: 9 September 2021, Murray, 2021). LTM can generate additional CMIP6 scenarios and time periods upon request.
The supplement related to this article is available online at: https://doi.org/10.5194/gmd-14-5789-2021-supplement.
LTM conceived the project, performed the model development, simulation, and evaluation of the E2.1 and GEOS-Chem interface, and wrote the manuscript. EML and LJM provided code edits from ModelE that were updated to E2.1 by LTM. CO provided feedback on the implementation of the new subdaily diagnostics. MS was a developer of the FlexGrid code in GEOS-Chem. All authors contributed feedback to the manuscript.
The contact author has declared that neither they nor their co-authors have any competing interests.
Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
We thank the entire GISS and GEOS-Chem developer and user communities.
This research has been supported by the National Science Foundation (grant nos. AGS-1702106 and AGS-2002414 to Lee T. Murray) and the National Aeronautics and Space Administration, Earth Sciences Division (grant no. NNX13AO08G to Loretta J. Mickley).
This paper was edited by Fiona O'Connor and reviewed by two anonymous referees.
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Like many free-running climate models, E2.1 uses a 365 d calendar, whereas GEOS-Chem includes leap days; the default behavior of GCAP 2.0 is to repeat 28 February meteorology on 29 February. Users alternatively may stop the model at the end of 28 February and apply the restart file to 1 March for leap years to avoid meteorological discontinuities.
Note that the native horizontal grid of E2.1 is offset from that traditionally used by GEOS-Chem at comparable resolutions. The former has the International Date Line as a cell edge, whereas the latter has it as a cell midpoint. In addition, E2.1 does not make use of half-polar cells as does GEOS-DAS or GEOS-Chem, making the total number of latitude bands one fewer in E2.1 as opposed to GEOS-Chem.