3.1. Climatic Effects Due to Increased CO2 Levels
In this section, this paper study the changes in different climatic variables due to rising CO2 levels. The obtained results provide the physical explanations to the evolution of anthropogenic and natural aerosols in the future climate, as shown in the following sections. The changes in these climatic variables are evaluated with a statistical significance of 90%. As mentioned in the experimental design, the CO2 mass-mixing ratios were set to 389, 778, and 1556 ppm, respectively, in the three tests. However, it was found that changes in these climatic variables, including surface temperature, cloud, precipitation, horizontal wind, and divergence, due to 2 × CO2, have similar patterns to those caused by 4 × CO2. Therefore, the variations of climatic factors under 4 × CO2-induced global warming, will be discussed in detail. Also, this paper will pay attention to seasonal variation by addressing the results of the two seasons of JJA and DJF.
Figure 1 shows the geographic distributions of changes in the surface air temperature (SAT) between 1 × CO
2- and 4 × CO
2- induced climatic status in JJA and DJF, with the solid lines representing the SAT under the 1 × CO
2 climate. The global annual mean SAT increases by 6.29 K in JJA and 6.66 K in DJF between the experiments of 4 × CO
2 and 1 × CO
2, which is almost double the related values between the experiments of 2 × CO
2 and 1 × CO
2 (3.09 K in JJA and 3.29 K in DJF). The growth rates of SAT to CO
2 concentrations are 0.008 K/ppm for both JJA and DJF under 2 × CO
2-induced warming, which are slightly higher than the corresponding values from 4 × CO
2 (0.005 K/ppm in JJA, and 0.006 K/ppm in DJF), due to the CO
2 effect. Since the patterns of climate change are similar for 2 × CO
2 and 4 × CO
2, here, only the results of 4 × CO
2 are discussed in this paper because of the stronger signals. From
Figure 1a,b, although the global warming induced by rising CO
2 levels is found in both JJA and DJF, the geographic distributions of changes in SAT are very different.
In JJA, the apparent surface warming induced by rising CO
2 is found over the high-latitude regions in the southern hemisphere (SH), and mid-latitudes over North America and North Asia in the northern hemisphere (NH). The largest increase of SAT occurs over the high latitudes in the SH, reaching up to 18.0 K. However, in DJF, SAT increases more over the high latitude continental regions in the NH than in other areas. The most significant changes in SAT are also found over high latitudes in the NH, with the local maximum of SAT exceeding 18.0 K. Slight warming occurs over high latitudes in the SH, with SAT increasing up to 8.0 K over most of this area. Larger increases of SAT are often at high latitudes in the NH (DJF) and SH (JJA), whereas changes over the tropics are considerably smaller. Warming near the surface could be enhanced over the polar areas because of the strong ice and snow albedo feedback [
15]. In addition, surface warming occurs much stronger over continental areas than oceanic regions, which is caused by the weaker heat capacity as well as less efficient evaporative cooling.
Different results of changes in surface temperature in JJA and DJF induced by rising CO
2 concentrations, as shown in
Figure 1, can produce differences in atmospheric circulation since the surface heat source is one of the key factors driving air movement. Changes in large-scale circulations result in variations of wind speed.
Figure 2 shows seasonal changes in the surface wind vector (U, V) under 4 × CO
2-induced global warming, where U and V are the zonal and meridional wind speeds. Furthermore, changes in the convergence and divergence (∂U/∂x + ∂V/∂y) of wind near surface are presented.
In JJA, apparent changes in the surface wind vector occur over the Atlantic Ocean in the NH, whereas slight and messy changes in surface wind are seen over the Pacific Ocean. Over central Africa, an increase in the wind speed causes a significant convergence of surface wind over northern Africa. Changes in the wind vector are found in vortex forms over tropical regions, leading to a large account of convergence and divergence over this region (
Figure 2a,c). The divergence/convergence of wind could cause a decrease/increase in local aerosol distributions when it overlaps with the source of aerosol particles. In addition, the eastward horizontal zonal wind is slightly strengthened over oceans at 50° S (
Figure 2a). Horizontal divergence of surface wind at 50° S is minimal due to the parallel surface air flows. In DJF, the largest wind speed occurs over the Pacific Ocean in the NH, whereas the wind speed over the Atlantic Ocean is lower. Similar to changes in JJA, the convergence and divergence are also located over tropical areas in DJF (
Figure 2b,d). Enhanced westerlies over oceanic regions at 50° S are much larger than those during JJA (
Figure 2b). Changes in the surface wind vector and the resulting convergence and divergence may have impacts on variations of particles over the corresponding regions.
Changes in the zonal mean stream function of vertical atmospheric circulation under 4 × CO
2-induced global warming (color contours), as well as the stream function at the 1 × CO
2 level (solid and dashed lines), are also shown in
Figure 2. In JJA, the Hadley cell in the NH is much weaker than that in the SH in the 1 × CO
2 experiment. In 4 × CO
2, the Hadley circulation in the SH is enhanced and moves northwards, whereas the Hadley in the NH becomes much weaker (
Figure 2e). Changes in the Hadley circulation would lead to a northward shift of the intertropical convergence zone (ITCZ). Moreover, the Ferrel cell in the SH is slightly strengthened due to rising CO
2 levels, which could be the reason for small increases in the surface wind speed over the oceanic regions at 50° S (
Figure 2e) due to the Coriolis force. However, in DJF, the situation is totally different from that in JJA. The Hadley is more robust in the NH than in the SH in the 1 × CO
2 experiment (
Figure 2f). Under 4 × CO
2-induced warming, the Hadley and Ferrel cells in the NH are slightly intensified, with the ascending branches of Hadley circulations moving southward. A strengthened Hadley circulation in the NH is likely to lead to a southward shift of ITCZ. In the SH, although a weakened trend is found in the Hadley circulation, the Ferrel cell is strengthened in DJF due to 4 × CO
2-induced warming. The enhanced Ferrel cell contributes to the increase in the wind speed over oceanic regions in the SH.
Figure 3 shows the geographic distributions of changes in total cloud cover (TCC, the sum of low, middle, and high cloud fractions) and precipitation during JJA and DJF, respectively, under 4 × CO
2-induced global warming. The simulated global annual mean TCC decreases by approximately 2.73% in JJA and increases by 0.75% in DJF. In JJA, the TCC decreases over most continental regions with the rising CO
2 levels. The relatively large decreases of TCC are over Europe, North America, eastern South America, and southern Africa. The reductions over the regions mentioned above are mainly due to dry descending air branches of the Hadley and Ferrel cells caused by CO
2-induced warming, as shown in
Figure 2. The reductions in cloud over regions in the subtropics and mid-latitude under global warming have also been shown in climatic models and observations [
16,
17]. Increases of TCC caused by rising CO
2 levels are located over the high latitudes of the two hemispheres, such as oceanic regions at latitudes between 80° N to 90° N in the NH, and regions at 70° S in the SH. Increases of TCC at 70° S are mainly due to the amplified Ferrel cell in the SH during JJA. At high latitudes, the maximum increases of TCC reach up to 49% in the NH and 40% in the SH. In addition, some slight increases in TCC caused by rising CO
2 concentrations are over regions at 10° N during JJA, such as western North America, South Asia, and the oceans west of northern Africa. Increases in TCC over these regions above are mainly due to the shift of the ascending branch of the Hadley circulation (
Figure 2e). In DJF, the increases in TCC in the NH shift to the regions with latitudes ranging from 50° N to 80° N. The most apparent increases are over the northwestern part of North America and northern Asia, with the maximum increase reaching up to 54%. Apparent decreases in TCC are still found over lower and mid-latitudes, which are similar to changes in TCC during JJA.
Global averaged precipitation increases by 0.37 mm day
−1 in JJA and 0.41 mm day
−1 in DJF. Apparent increases occur over the tropical regions during both seasons (
Figure 3c,d). In JJA, increases in precipitation are located in the tropical regions of the NH, especially over oceanic regions at 10° N, such as the central Pacific Ocean, South Asia, and their neighboring oceanic regions (
Figure 3c). The maximum increase over these regions above reaches up to 8.18 mm day
−1. Increases in precipitation at 10ºN are mainly caused by the northward shift of ITCZ under 4 × CO
2-induced warming, as shown in
Figure 2. In DJF, the ITCZ is shifted to the regions at 10° S; thus, the changes in the distribution of precipitation become different from those of JJA. For the central Pacific Ocean, increases of precipitation in the NH are weakened, with significant increases occurring over areas at 10ºS over the eastern Pacific Ocean (
Figure 3d). For South Asia, increases in precipitation shift to the central Indian Ocean in DJF. In addition, there are slight increases over mid- and high latitudes in both the NH and SH during the two seasons (
Figure 3c,d). The distributions of changes in precipitation are mainly caused by the strengthened Hadley circulation in the NH under 4 × CO
2-induced global warming.
Furthermore, increases in precipitation are at mid- and high latitudes in both the NH and SH in both seasons. Over mid- and high-latitude regions, increases in precipitation during DJF are much larger than those in JJA, which is caused by different changes in particles in the two seasons. Strengthened ascending branches of the Ferrel cell, along with the amount of moisture from the ocean, are the main leading factors of increases in precipitation. Changes in TCC and precipitation may play roles in variations of anthropogenic and natural particulate matter in JJA and DJF, under CO2-induced global warming.
3.2. Variations in Anthropogenic Particulate Matters
This section presents the differences in anthropogenic aerosol column concentrations between the experiments of 4 × CO
2 and 1 × CO
2.
Figure 4 shows the JJA seasonal mean of geographic distributions of changes in column concentrations of anthropogenic PM
2.5 and CPM. Global mean column concentrations of PM
2.5 decrease by approximately 0.19 mg m
−2, and those of CPM increase by 0.005 mg m
−2. Changes in fine particles are about two or more orders of magnitude larger than those of particulate matter of coarse mode. Variations of corresponding SO
4, BC, and OC particles of fine and coarse modes in JJA are also shown in
Figure 4. Decreases in global mean column concentrations of SO
4 (PM
2.5), BC (PM
2.5), and OC (PM
2.5) are 0.07, 0.01, and 0.11 mg m
−2, respectively, contributing about 37%, 5%, and 58% to the total reduction of PM
2.5. The global mean SO
4 (CPM) burden increases by 0.005 mg m
−2, accounting for almost of the total increase in CPM. Changes in BC (CPM) and OC (CPM) particles are very small. For fine anthropogenic particles, the PM
2.5 burden decreases sharply over the mid- and high-latitude regions, especially in the NH, whereas it increases over the continental areas at lower latitudes in the two hemispheres during summer (
Figure 4a). In addition, it is found that changes in column concentrations of the three individual species (SO
4 (PM
2.5), BC (PM
2.5), and OC (PM
2.5)) are similar to those of PM
2.5 from the perspective of global distributions (
Figure 4b–d). The largest reduction in the anthropogenic PM
2.5 burden occurs over North America and North Asia. Over mid- and high-latitude regions (regions with latitudes > 40° N), regional mean burdens of PM
2.5, SO
4 (PM
2.5), BC (PM
2.5), and OC (PM
2.5) particles decrease by approximately 2.41, 1.49, 0.07, and 0.85 mg m
−2, with three individual species (SO
4 (PM
2.5), BC (PM
2.5), and OC (PM
2.5)) contributing about 62%, 3%, and 35%, respectively, to the reduction of total fine anthropogenic particles. The most apparent increases in PM
2.5, SO
4 (PM
2.5), BC (PM
2.5), and OC (PM
2.5) column concentrations are located over the Arabian Peninsula and Africa, with the regional mean increases reaching up to 2.79 and 3.35 mg m
−2. Also, changes in anthropogenic PM
2.5 particles over the Arabian Peninsula are mainly caused by increases of the SO
4 (PM
2.5) burden (about 2.44 mg m
−2), contributing about 87% to the total changes. Over Africa, the SO
4 (PM
2.5), BC (PM
2.5), and OC (PM
2.5) column concentrations increase by 2.28, 0.14, and 0.93 mg m
−2, accounting for about 68%, 4%, and 28% of the total increase of anthropogenic PM
2.5. Slight increases occur over southern North America, South America, East Asia, and Southeast Asia, with the largest regional mean increases of total fine particles reaching up to 0.72 mg m
−2.
Different from changes in fine anthropogenic particulate matter, the column concentrations of coarse particles apparently increase over the Arabian Peninsula, with regional mean burdens increasing by 0.109 mg m
−2. Over these growing areas, the regional mean column concentrations of SO
4 (CPM) increase by approximately 0.108 mg m
−2, accounting for about 99% of the total anthropogenic CPM changes. Changes in BC (CPM) and OC (CPM) particles are much smaller than those in SO
4 (CPM). A slight increase of 0.04 mg m
−2 is also found over central Africa. Changes in CPM over the rest of the areas are very small (
Figure 4e) since changes in BC (CPM) and OC (CPM) column concentrations are about two orders of magnitude smaller than the corresponding concentrations of fine particles in JJA. Therefore, the paper does not pay more attention to changes in carbon particles in JJA. Increases in anthropogenic CPM over central Africa are consistent with those of fine particulate matters, which could be put together in the discussion of the climatic factors, as in the following sections.
Figure 5 shows the corresponding changes in fine and coarse anthropogenic particles during DJF. It is interesting to find, to some extent, that the geographic distributions of changes in anthropogenic PM
2.5 in DJF are similar to those in JJA, but the magnitudes of maximum regional changes are much smaller than those in JJA (
Figure 4a and
Figure 5a). Similar to JJA, the burden of anthropogenic PM
2.5 decreases in mid- and high latitudes in the NH, with the maximum decrease occurring over East Asia, and increases over some regions in the tropics and over central Africa. Over mid- and high-latitude regions, decreases in anthropogenic PM
2.5 during DJF are much smaller than those during JJA. The main reason is the lower column concentration of anthropogenic PM
2.5 in DJF than in JJA. Although changes in rainfall are more conducive to a decreased PM
2.5 burden during DJF, the decreasing regions of anthropogenic PM
2.5 over Asia are broader to the south. Furthermore, the growing regions are narrowed down sharply, especially over northern and central Africa. Over the Arabian Peninsula, the trend of changes in anthropogenic PM
2.5 shifts from a noticeable increase in JJA to a small decrease in DJF. The same as in JJA, changes in particles of coarse mode are much lower than those of fine particles in DJF.
Under 4 × CO
2-induced warming, changes in anthropogenic fine and coarse particulate matter can be analyzed and understood from changes in surface wind and precipitation caused by rising CO
2 concentrations, as shown in
Section 3. In both JJA and DJF, the burden of the anthropogenic particle decreases over mid- and high latitudes and increases over some land regions in the tropics. Based on the results of precipitation, it is found that large-scale precipitation over mid- and high-latitude regions in the NH increases, which leads to enhanced wet deposition over these regions during both JJA and DJF. Changes in the surface wind are minimal and messy at mid- and high latitudes, and contribute little to decreases over these regions (
Figure 2). Although convergences occur over eastern Greenland and the northern part of North Asia, the anthropogenic particles are still exposed to a decrease because there is no particle source over these regions. Over Europe and central Asia, the precipitation falls slightly during JJA, but increases during DJF, which supports the broadened decrease over Asia and Europe in DJF. Although the anthropogenic particle burden increases over regions in the tropics in both JJA and DJF, some differences still can be found over some regions caused by variations in some climatic factors. For example, over the Arabian Peninsula, the anthropogenic particle burden decreases in JJA but increases in DJF, which is opposite to the trends of precipitation in JJA and DJF.
In the mode of high CO
2 concentrations, the column concentrations of PM
2.5 may be larger [
18,
19]. The wet deposition caused by the rising CO
2 concentrations is the most important factor in changes in the column concentrations of anthropogenic particulate matter.
3.3. Variations in Natural Particulate Matters
Figure 6 shows the geographic distributions of changes in column concentrations of natural PM
2.5 and CPM, as well as in the corresponding species of fine and coarse particles in JJA under 4 × CO
2-induced global warming. Different from the anthropogenic particles, the column concentrations of natural particulate matter in both modes increase significantly over northern Africa and the Arabian Peninsula. Global mean burden increases of natural PM
2.5 and CPM are 7.00 and 3.60 mg m
−2; much more substantial than the corresponding results of anthropogenic particles. Increases in fine particles are more apparent than those of coarse particles in JJA, and contribute approximately 66% to the total increase of natural aerosols. Changes in SD particles mainly cause increases in PM
2.5 and CPM over northern Africa and the Arabian Peninsula. From
Figure 6b,e, it can be seen that the distributions of changes in SD (PM
2.5) and SD (CPM) are highly consistent with those of corresponding natural PM
2.5 and CPM particles, respectively, occurring over central Africa and the Arabian Peninsula. The global mean burden of SD (PM
2.5) and SD (CPM) increases by 6.45 and 2.63 mg m
−2, and contributes 92% and 73% to PM
2.5 and CPM particles in JJA due to 4 × CO
2-induced climate change. Similar to the changes in total fine and coarse particulate matter, the increases in SD (PM
2.5) in JJA also are more severe than changes in SD (CPM) over these significant areas mentioned above. In addition, slight increases in PM
2.5 and CPM column concentrations are shown over the oceanic regions near 50°S in JJA under 4 × CO
2-induced warming, which is mainly due to changes in SS. From
Figure 6c,f, it can be seen that significant increases in SS (PM
2.5) and SS (CPM) are shaped as a band over oceans at 50° S. Opposite to the results of total natural particles and SD, the increase in coarse SS particles is much higher than that of fine mode. Over the jet stream regions from 40° S to 60° S, the maximum increases of SS (PM
2.5) and SS (CPM) reach up to 7.00 and 19.02 mg m
−2, respectively.
Figure 7 is the same as
Figure 6, but for the season of DJF. Different from the result of JJA, the decrease in changes in natural particles becomes the dominant tendency over the continental regions, especially the fine natural particles over land areas in the NH. Except for a few areas in East Asia, the column concentrations of natural PM
2.5 in DJF decrease over the regions with latitudes 30° N, especially over northern Africa, the northern part of the Arabian Peninsula, central Asia, North Asia, and North America. The most substantial decrease in fine natural particles reaches up to 206.86 mg m
−2. On the other hand, the reductions in coarse natural particles are much smaller than those of fine natural particulate matter, with apparent reductions occurring over northern Africa and central Asia. Slight increases in the natural PM
2.5 and CPM burden are also found in some land regions, such as western North Africa, East Asia, and Western Australia, which is also due to increases in SD particles of both fine and coarse modes. Compared with the distributions of changes in SD particles (
Figure 7b,e), changes in PM
2.5 and CPM over most land regions are mainly dominated by changes in SD particles. For SS particles, both SS (PM
2.5) and SS (CPM) increase over oceanic regions near 50° N and 50° S during DJF. Increases in the column concentrations of SS (PM
2.5) particles are much smaller than those of SS (CPM). Increases in the SS (PM
2.5) burden are often offset by the decreases in SD (PM
2.5), especially over the oceanic regions near 50° N (
Figure 7a–c). Increases in the SS (CPM) burden are much larger, with maximum increases of 18.58 and 15.10 mg m
−2 over the oceanic regions (near 50° N) in the NH and SH. The rising SS (CPM) burden in the NH will lead to slight increases in natural particles of the coarse mode over the oceans in the mid-latitudes in the NH (
Figure 7d,f).
The results in
Figure 6 and
Figure 7 show that the fine and coarse models have the same trends of changes. Climate change, as well as land-use change, might be the most important factors affecting the variations of natural particle burden in the atmosphere [
20].
In JJA, the column concentrations of natural PM
2.5 and CPM increase over northern Africa and the Arabian Peninsula, which is associated with the large sand source region of the Sahara Desert. Changes in the distributions of natural particles can be found when the divergence/convergence of surface wind overlaps with the source regions. As discussed above, the Hadley circulation in the SH is strengthened and moves northward during JJA, with the ascending branch of the Hadley circulation extending around 10° N. The enhanced northward surface wind of the Hadley circulation and the weakened southward surface wind lead to a horizontal convergence over regions at 10° N. The convergence occurs over the desert region, which could contribute to the increases in natural particles over northern Africa and the Arabian Peninsula. In JJA, the precipitation and TCC over North Africa and the Arabian Peninsula decrease slightly under 4 × CO
2 (
Figure 3), and are conducive to the increases in natural particles due to a weaker wet deposition over these regions. These decreases in the precipitation and TCC over North Africa and the Arabian Peninsula rely on the changes in the atmospheric circulation. For SS particles, from the comparisons of the changes in the SS burden and the surface wind speed shown in
Figure 2 and
Figure 6, we can conclude that the rising column concentrations of SS particles are mainly caused by the enhanced eastward wind speed over oceanic regions, especially in the polar jet stream regions. As discussed above, the accelerated wind speed over oceanic regions at 50° N and 50° S are mainly caused by the strengthened Ferrel cell in the two hemispheres (
Figure 2).
In DJF, the column concentrations of natural particles of both fine and coarse modes decrease over most continental regions in the NH, except for the west coast of North America, Australia, North Africa and the eastern and northern regions of East Asia. The result of DJF is very different from that of JJA, particularly for SD in both fine and coarse modes. In DJF, Hadley and Ferrel cells in the NH are strengthened due to 4 × CO
2-induced warming (
Figure 3). The descending branches of Hadley and Ferrel cells are located over the lower-latitude regions (<30° N), leading to decreases in aerosol column loading over these regions; whereas the robust ascending branches of the enhanced Ferrel cell in the NH result in increases in precipitation over the mid- and high latitudes (>30° N). Over mid- and high latitudes, the rising precipitation could cause the apparent reductions in natural particles during DJF. The same as in JJA, the change in SS particle column loading is mostly associated with the surface wind speed. In summary, the divergence/convergence of surface wind, near-surface wind speed, and decreasing precipitation caused by the rising CO
2 concentrations contribute most to changes in natural particle concentrations.