Sulfuric Acid Decomposition Chemistry Above Junge Layer in Earth's Atmosphere Concerning Ozone Depletion and Healing

Sulfuric Acid Decomposition Chemistry Above Junge Layer in Earth's Atmosphere Concerning Ozone Depletion and Healing

ARTICLE https://doi.org/10.1038/s42004-019-0178-4 OPEN Sulfuric acid decomposition chemistry above Junge layer in Earth's atmosphere concerning ozone depletion and healing Montu K. Hazra 1, Sourav Ghoshal1, Prabhash Mahata2 & Biswajit Maiti2 1234567890():,; Sulfuric acid (H2SO4) is the seed molecule for formation of stratospheric sulfate aerosol layer that assists ozone depletion by activation of halogen species. The impact of increased stratospheric sulfate aerosols due to large volcanic eruptions and possible side effect claimed in the geoengineering scheme of global climate using man-made injected stratospheric sul- fate aerosols is ozone depletion. Given that both volcanic eruptions and geoengineering scheme are ultimately connected with increased upper stratospheric concentrations of 1 H2SO4, here we show by theoretical approach that the pressure-independent H2SO4 + O( D) insertion/addition reactions via barrierless formation of peroxysulfuric acid (H2SO5) or HSO4 + OH radicals or sulfur trioxide (SO3) + hydrogen peroxide (H2O2) molecules are the potential routes towards H2SO4 loss above the stratospheric sulfate aerosol layer, and for the regeneration or transportation of consumed lower-middle stratospheric OH radical in the upper stratosphere at the cost of O(1D)/ozone. 1 Chemical Sciences Division, Saha Institute of Nuclear Physics, Homi Bhabha National Institute, 1/AF Bidhannagar, Kolkata 700 064, India. 2 Department of Chemistry, Institute of Science, Banaras Hindu University, Varanasi 221 005, India. Correspondence and requests for materials should be addressed to M.K.H. (email: [email protected]) COMMUNICATIONS CHEMISTRY | (2019) 2:75 | https://doi.org/10.1038/s42004-019-0178-4 | www.nature.com/commschem 1 ARTICLE COMMUNICATIONS CHEMISTRY | https://doi.org/10.1038/s42004-019-0178-4 he highly dispersed microscopic particles in strato- Results spheric aerosol layer play an important role in the Potential energy diagrams. The detailed theoretical methodolo- T ’ stratospheric ozone depletion, and affect the Earth s gies for geometries, energetics, kinetics and direct dynamics of the 1–7 + 1 climate by absorbing and scattering the solar-radiation .Itis H2SO4 O( D) insertion/addition reactions in the ground believed that this layer (Junge layer) is composed of mainly the potential energy surface have been given below (Methods Sec- sulfuric acid (H2SO4)andwater(H2O) molecules to form the tion). In H2SO4, there are six chemical bonds wherein the sulfate aerosols or droplets. Similarly, the sulfate aerosols and insertions or additions of the O(1D) are possible. However, other atmospheric aerosols resulting from various inorganic among these six bonds, two equivalent O−H, S=O and S−O and organic species in troposphere also play an important role bonds are there. Therefore, the study of insertion/addition reac- in degrading visibility, promoting heterogeneous chemistry tions of O(1D) into the O−H, S=O and S−O bonds are effec- through atmospheric chemical reactions, as well as negatively tively important, and each reaction pathway can be considered impacting human health8–12. It is seen from the chemical with reaction degeneracy (σ) = 231. To keep our presentation composition of aerosol particles in the Earth's atmosphere that simple, we label the insertions or additions of O(1D) into the O − = − the H2SO4 among various species is the most important pre- H, S O and S O bonds as the Channel-I, Channel-II and cursor for the formation of aerosol particles at a wide range of Channel-III, respectively. altitudes including both the troposphere and stratosphere1,8–12. It is seen from our calculations that the insertions/additions of Indeed, the nucleated aerosol particles from trace atmospheric O(1D) through Channel-I to III produce directly either the adduct − 1 ≡ fi vapors are expected to provide ~45% or more of global cloud intermediates (H2SO4 O( D) Ad) or H2SO5 in the rst step. 11–13 condensation nuclei (CCN) . Consequently, the H2SO4 Moreover, the reactions are highly exothermic, and because of the fi molecule becomes of major importance in atmospheric chem- large exothermicities, the adducts or H2SO5 formed in the rst istry−which has led to many studies investigating its formation, steps of Channel-I to III are expected to undergo further decomposition and its crucial role as a nucleating species for unimolecular isomerizations or decompositions followed by aerosols and cloud formation8–22. isomerizations to form various other product molecules. It is The most abundant sulfur molecules in the Earth's atmo- also seen from our calculations that the H2SO5 is the most stable + sphere at altitudes above 35 km or above the stratospheric product molecule and the formations of H2SO5 or SO3 H2O2 sulfate aerosol layer or ozone layer are H2SO4 and sulfur are energetically the most favorable pathways. 23–25 dioxide (SO2) . Moreover, the seed molecule for the for- In Fig. 1, we present the CCSD(T)/aug-cc-pVTZ level predicted mation of stratospheric sulfate aerosols, which assist ozone potential energy diagrams of energetically the most favorable + depletion through activation of halogen species, especially after paths of three channels that produce either the H2SO5 or SO3 26–29 volcanic eruptions, is H2SO4 .TheH2SO4 above 35 km H2O2 molecules, especially, to understand the potential atmo- + 1 altitude is formed from the surface of stratospheric sulfate spheric impact of H2SO4 O( D) insertion/addition reactions aerosol layer via evaporation1,4,23–25. Hence, the decomposition with respect to visible solar radiation pumping photolysis of mechanisms of H2SO4 in upper stratosphere or above 35 H2SO4. The M06-2X/aug-cc-pVTZ level optimized geometries of km altitude are the potential routes towards the degradation various species, especially the adducts, transition states (TSs) and of enhanced stratospheric sulfate aerosols that assist ozone product molecules, involved in the potential energy diagrams depletion after volcanic eruptions. have also been shown in the Fig. 1. The potential energy diagrams In the quest for an answer to the question about the with various interconnectivities between the above-mentioned decomposition of H2SO4 molecule in the Earth's upper strato- insertion/addition reactions via the Channel-I to III and the sphere, the visible solar radiation (hν) pumping photolysis of optimized geometries of the species involved in potential energy H2SO4 vapor (H2SO4 + hν → SO3 + H2O) is the potential diagrams have been shown in the Supplementary Figs. 1 and 2. mechanism. This mechanism has been proposed by Vaida Importantly, it is worth noting here that our main focus is on the 17 et al. in 2003, and absorption of visible sunlight by the H2SO4 upper stratospheric loss of H2SO4 molecule through its decom- molecule is the prerequisite step for the occurrence of its position into all possible products, while H2SO4 is the perpetrator unimolecular decomposition17–19. This visible photolysis for the formation stratospheric sulfate aerosol layer involved in mechanism via direct formation of sulfur trioxide (SO3), an ozone loss. From Fig. 1, it is seen that the formation of H2SO5 and important molecule in atmospheric sulfur cycle, explains not SO3 + H2O2 in Channel-I occurs through the formation of a only the decomposition of H2SO4 in the upper stratosphere; but common adduct intermediate (Ad-I). Moreover, energetically the also satisfy model requirements that explains the field obser- most favorable path is the formation of SO3 + H2O2 via TS-IA, as fi 19 → − vations of the SO2 vertical pro les at higher altitudes . Simi- the barrier heights for the unimolecular Ad-I H2SO5 I and larly, the dominant photo-dissociation mechanism of H2SO4 Ad-I → SO3 + H2O2 conversion steps via TS-I and TS-IA are −α −1 above 70 km altitude is the absorption of Lyman radiation only ~3.2 and ~1.0 kcal mol , respectively. It is seen from the T1 by high energy Rydberg excited states30. Hence, these two diagnostic calculations at the CCSD(T)/aug-cc-pVTZ level that mechanisms are two important pathways towards the upper the TS-I might have slight multi-reference character (Supple- atmospheric loss of H2SO4 molecule. mentary Note-1 and Supplementary Table 3). Because of this + 1 Here we show that the barrierless fast H2SO4 O( D) prediction, we further perform the CASPT2//CASSCF calcula- insertion/addition reactions are the potential mechanism that tions (Supplementary Note-1), and the predicted unimolecular → − also interprets the upper stratospheric loss of H2SO4 molecule barrier heights for the Ad-I H2SO5 I conversion at the via formation of, especially, the peroxysulfuric acid (H2SO5)or CASPT2(12,12)/aug-cc-pVDZ and CASPT2(12,12)/aug-cc-pVTZ + + −1 HSO4 OH radicals or SO3 H2O2 (hydrogen peroxide) levels are respectively ~2.7 and ~2.1 kcal mol (Supplementary fi + 1 molecules. We also nd that the H2SO4 O( D) insertion/ Fig. 3 and Supplementary Table 4). Therefore, when we consider addition reactions are involved in affecting the upper strato- both the CCSD(T) and CASPT2 levels of calculations, energeti- spheric ozone chemistry. In addition, this mechanism via direct cally the most favorable path in the Channel-I is the formation of 1 + involvement of O( D) provides physical insight towards the SO3 H2O2 via TS-IA, as mentioned above. claim or sensitivity of the ozone depletion in geoengineering Similarly, we also note that while the formation of H2SO5 in scheme of climate using injected stratospheric sulfate aero- Channel-II occurs via the formation of another adduct inter- 2–7 sols . mediate (Ad-II), the formation of H2SO5 in Channel-III occurs 2 COMMUNICATIONS CHEMISTRY | (2019) 2:75 | https://doi.org/10.1038/s42004-019-0178-4 | www.nature.com/commschem COMMUNICATIONS CHEMISTRY | https://doi.org/10.1038/s42004-019-0178-4 ARTICLE a 0 1 In contrast, as mentioned above that the formation of H SO + O( D) 2 4 − − Channel -I H2SO5 II in the Channel-III is a direct process, and H2SO5 II TS-I TS-IA −1 + 1 –22.33 –24.51 is ~ 82.6 kcal mol more stable than the isolated H2SO4 O( D) reactants.

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