عنوان البحث(Papers / Research Title)
simulation study of ozone depletion through photolysis mechanism
الناشر \ المحرر \ الكاتب (Author / Editor / Publisher)
عباس عبد علي دريع الصالحي
Citation Information
عباس,عبد,علي,دريع,الصالحي ,simulation study of ozone depletion through photolysis mechanism , Time 15/03/2017 05:24:28 : كلية العلوم
وصف الابستركت (Abstract)
Quantum calculation methods like DFT, Ab-initio, and semiempirical have been used to simulate the mechanism of Ozone depletion by HCFC-124 (1-Chloro-1,2,2,2- tetrafluoroethane).
الوصف الكامل (Full Abstract)
JOURNAL OF MULTIFUNCTIONAL MATERIALS & PHOTOSCIENCE 7(2), December 2016, pp. 99-110 Abbas A-Ali Drea and Roaa A-Hussien Babylon university College of Science Chemistry Department, Hilla – Iraq E-mail: aadreab22@yahoo.com Abstract: Quantum calculation methods like DFT, Ab-initio, and semiempirical have been used to simulate the mechanism of Ozone depletion by HCFC-124 (1-Chloro-1,2,2,2- tetrafluoroethane). Structural properties such as Geometry optimized and single point calculation has been done to understand the configuration interaction singly excited state for all chemical species of the suggested reactions and their transition states. Energetic properties such as total energy, molecular orbital energies, zero point energy, energy gap has been calculated with RHF/6-31G* and Beack88LYP/3-21G(d) methods . Potential energy surface calculation has been determined to evaluate the responsible bond of first initiation cleavage step of photolysis mechanism reaction. They found C-Cl bond is the most responsible in the photolysis mechanism reactions which is produced chlorine radical and other radicals by energy barrier value of 61.305 kCal mol-1 with enthalpy of reaction equal to 78.419 kCal mol-1. The transition state examination of these reactions indicated that chlorine radical is the most probable species than other radicals to depleted ozone by HCFC-124. The depletion reaction is spontaneous and exothermic with enthalpy change of reaction equal to -252.64kCal mol-1 and free energy equal to -291.376 kCal mol-1 . Key words: HCFC-124, Ozone, Depletion, Photolysis mechanism, transition state, Calculation methods, Simulation study. Introduction The earth’s atmosphere is protected from much of the sun’s UV-B and UV-C radiation by a layer of ozone (O3 ) in the stratosphere, which is strongly absorbed in the 230 to 290 nm region1 . Ozone is ubiquitous in the atmosphere but its mainly concentrated in the stratosphere between 19 and 23 km above the surface of the earth2 . Majority of ozone in the stratosphere layer is formed naturally by photolysis of oxygenic molecules under UV-radiation3 . Human activities during the last century involving particularly a new chemical compounds such as chlorofluorocarbons(CFCs), Halons (H), carbontetrachloride (CTC) which leads to the destruction of earth’s protective stratospheric ozone layer.4 *Corresponding author: aadreab22@yahoo.com CFC (chlorofluorocarbon) is a stable compound that is used extensively for air conditioning and refrigeration, Propellants and solvents also for the production of foams. chlorofluorocarbons is the main source of ozone depleting substances in the stratospheric layer, also they contribute to global warming.5 The production of CFC will phase out in beginning of 1995 under the Copenhagen amendment and the Montreal protocol6 . A new chemical compounds have been identified to be a replacement to the CFC compound such as HCFC (hydrochlorofluorocarbons) and hydrofluorocarbons (HFC) that’s have the same physical-chemical properties to the CFC compound with less stratospheric ozone depletion7 . HCFC-124 (1-Chloro-1,2,2,2-tetrafluoroethane) is a replacement to CFC-114 one of the most practical CFC compound as refrigeration and fire extinguishing agents . The HCFC-124 has a molecular weight equal to 136.48, and B.P equal to –12.1C° , also ozone depletion Potential relative to CFC-12 equal to 0.04 8. In the present work quantum calculation methods have been used to estimate the ozone depletion mechanism by HCFC-124, through determining the geometry optimized of the parent compound and for the fragments that’s resulted from the photolysis reaction also the transition state . The structural properties are important to understand the chemical reactivity during the potential energy surface calculations. Theoretical calculations give energetic parameters of short-lived reactive intermediate moieties. The calculation of transition state structures is very sensitive to the level of theory and basis sets that’s be used 9,10 . Computational Details Geometry optimizations were performed at the level of HF/RHF, and density functional theory with an exchange potential Becke 88 and correlation potential LYP that’s proposed by lee-yang-parr with 3-21G(d) basis sets. Then, harmonic vibration frequencies were computed to prove that each of the optimized structures is a local minimum on its potential surface11. Potential energy surface calculation performed by mapping reactants into products to calculate the activation energy.12 Results and Discussion HCFC-124 (1-Chloro-1,2,2,2-tetrafluoroethane) is a polar compound possess one hydrogen atom, the chemical structure represented in figure 1 . Energetic properties of HCFC-124 have been studied using different quantum calculation methods to estimate the chemical reactivity. Table 1 shows the energetic properties of HCFC-124. The total energy calculation by Abinitio method give a value of -583015.8, -585812.9kCal mol-1computed by 3-21G (d), 6-31G* basis set respectively, compared with recent theoretical studies the 6-31G* give nearest value of total energy calculation13. The physical properties of HCFC-124 as a display in figure 2,which is approved that the electrostatic potential give a negative charge density appears on the fluorine atom (red color) while the carbon atom appears with positive charge density, also the Homo &Lumo calculation in 2&3 dimension has been computed. The total charge density gives high density centered on the fluorine atom that connected to carbon atom number two. Table 1 Energetic properties of HCFC-124 computed by different methods* DFT/Becke88 LYP Semiempirical Abinitio Type of calculation PM3 microstate/ 4*4 AM1 3-21G (d) 6-31G* 3-21G (d) Total energy - 53771.57 -59619.32 -583015.8 -585812.85 -584669.69 Binding energy -712.9214 -712.5329 - - - Heat of formation -214.489 -214.101 - - - Molecular HOMO -9.8055 -7.7162 -244.546 -307.31 -164.909 orbital energy LUMO 8.7332 12.2246 121.3469 109.447 57.5026 Eg 18.5387 19.941 365.892 416.757 222.412 Zero point energy 23.05 23.2777 25.4333 25.0256 22.098 Dipole moment D 1.811 1.739 1.4618 1.565 1.383 Energy values in kCal mol-1 unit. Figure 1: Chemical structure of HCFC-124. Figure 2: Physical properties of HCFC-124 computed at Abinitio /6-31G* method The bond parameters such as bond length, bond angle of HCFC-124 have been computed using DFT, Ab-initio method which is given a good agreement between the two methods, the C-C bond length computed by the DFT method give nearest value to the experimental value, as shown in table 2,which is equal to 1.542? and experimental value equal to 1.534?. The C-F bond length gives a value in the range 1.3-1.35? which is reaching the experimental value 1.3 ?. The C-Cl bond length equal to 1.74? calculated by Ab-initio method and the C-H bond length equal to 1.0736 ? which is the same as experimental value14-16. Table 2 Structural properties of HCFC-124 Type of calculation Ab-initio DFT/Becke 88 lyp 3-21G(d) 3-21G(d) C1 -C2 1.5 1.542 C1 -F1 1.3069 1.344 Bond length? C1 -F2 1.31 1.34 C1 -F3 1.3 1.35 C2 -Cl 1.746 1.814 C2 -H 1.0736 1.0972 C2 -F4 1.332 1.3556 C1 -F1 -F2 108.798 109.621 C1 -F1 -F3 109.156 109.082 C1 -F2 -F3 108.897 109.203 Bond angle degree C1 -C2 -F2 108.385 111.472 C1 -C2 -Cl 110.814 109.12 C1 -C2 -F4 107.893 109.757 C2 -Cl-F4 109.724 110.212 C2 -H-Cl 107.936 105.982 C2 -H-F4 111.263 112.471 The vibration calculation of HCFC-124 has been computed by both DFT, Ab-initio method which is given 18 normal modes with one positive value of imaginary frequency these normal modes show in table3 which gives good agreement with recent theoretical studies 13. The potential energy of bond stability has been computed for five types of bonds in HCFC-124 C1 -F1 , C1 -C2 , C2 -H, C2 -F4 , C2 -Cl by using semiempirical- PM3 method as shown in table 4. The C-Cl bond have less value of the dissociation energy with high value of wavelength equal to 407.8643 nm. The C-F bond required less value of wavelength in the range 249.5-250.911 nm, that means high value of energy . Table 3 Vibration calculation of HCFC-124 computed by different methods IR- Frequency* Abinitio DFT/Becke 88 LYP 3-21G(d) 3-21G(d) ?1 73.73 58.3 ?2 199.84 177.14 ?3 242.79 215.07 ?4 345.66 301.06 ?5 414.16 343.79 ?6 488.65 418.62 ?7 588.19 505.78 ?8 642.3 553.24 ?9 773.47 665.97 ?10 892.25 741.23 ?11 996.09 852.09 ?12 1290.79 1136.36 ?13 1368.94 1180.39 ?14 1459.31 1254.87 ?15 1488.47 1275.82 ?16 1527.85 1307.66 ?17 1602 1391.21 ?18 3400.85 3068.54 The C-H bond, and C-C bond needs wavelength equal to 277.326, 348.5226 nm respectively, with an energy value equal to 96.531, 76.8116 kCal mol-1,these values reached the experimental value 17. The examination of potential energy for bond length stability is represented in figure 3. Figure 3: Potential energy search of bonds length & bond angle stability of HCFC-124 computed by semiemprical-PM3 /CI(4*4) microstate. Table 4 Potential energy of bond stability of HCFC-124 computed by semimperical-PM3 /CI (4*4) microstate Type of Equilibrium Equilibrium Breaking Breaking Dissociation ? bond energy bond length ? energy bond length ? energy nm C1 -F1 -702.933 1.247 -595.6659 2.546 107.267 249.569 C1 -C2 -711.835 1.576 -635.023 2.47 76.8116 348.523 C2 -H -711.835 1.147 -614.852 2.55 96.531 277.326 C2 -F4 -703.283 1.25 -596.589 2.54 106.694 250.911 C2 -Cl -699.526 1.57 -633.89 2.67 65.636 407.864 * Energy values in kCal mol-1 unit The suggested photolysis mechanism of HCFC-124 occurs through three proposed transition states as represented in figure 4. TS1 through C-Cl bond which leads to the formation of Cl&C2 F4 H , second proposed transition state TS2 is through C-C bond which gives CF3 &CFHCl, the last proposed transition state is TS3 C-H bond dissociation to give two types of radical H & C2 F4 Cl. The energy barrier & enthalpy of reaction of these proposed transition states given in table 5. Figure 4: The proposed transition state in photolysis of HCFC-124. Table 5 Evaluation compares between the proposed transition state of HCFC-124 photolysis, calculated at semiempirical -PM3quatraic states . Transition States Energy barrier* Enthalpy change* TS1 61.3058 78.419 TS2 141.258 63.585 TS3 65.278 78.6245 *Energy values in kCal mol-1 unit. The calculations of potential energy and energy barrier give up an indication, proof that the reaction of C2 F4 HCl molecule occurs through C-Cl bond scission with higher probability than C-C, C-F ,C-H bonds. The photolysis of HCFC-124 under atmospheric conditions will form the •C2 F4 H and Cl• radicals. The suggested reaction, including •C2 F4 H radical formation, that’s rapidly react with O2 to form a peroxy radical (C2 F4 HO2 ). The radical C2 F4 HO2 will react initially with NO species to produced C2 F4 BrO and NO2 , the energetic values of alkoxy radical shows in table 6 18.The most probable fate of alkoxy radical is a breakdown of C-C bond to form CF3 and CFHO 19. Table 6 Energetic properties of C2 F4 HO radical computed by different methods *Energy values in kCal mol-1 unit. Type of calculation Ab-initio /6-31G* Semiemprical-PM3 Total energy -344438.819 -53204.0208 Binding energy - -741.56 Heat of formation - -211.9988 Dipole D 1.662 1.901 ZPE 25.5937 23.655 HOMO ev -14.798 -7.97 LUMO ev 1.711 -0.1117 Eg ev 16.509 7.858 C1-C2 1.525 1.602 Bond length ? C2-H 1.0834 1.1187 C2-O 1.345 1.3253 C1-F1 1.314 1.344 C2-F4 1.346 1.353 Bond C1-C2-O 110.505 113.036 angle degree C1-C2-H 109.542 111.418 C1-C2-F4 107.643 108.8 C1-C2-F1 111.158 112.304 Imaginary frequency + *Energy values in kCal mol-1 unit. The photolysis mechanism initiated by the reaction of C2 F4 H radical with the ozone molecule to form alkoxy radical with an energy barrier equal to 8.56 kCal mol-1 computed at PM3/CI(4*4)microstate and enthalpy of reaction equal to -73.736 kCal mol-1 also negative value of free energy change(V) which is equal to -71.941 kCal mol-1. The alkoxy radical undergo secondary photolysis through C-C bond at a wavelength equal to 633.53 nm, this reaction occurs with less value for the enthalpy of reaction which equal to -7.22 kCal mol- 1 also the rate constant and “G equal to 9.5*103 s-1, -20.413 kCal mol-1 respectively. The released fragment in photolysis mechanism will react with ozone in different pathways as represented in scheme1. The rate constant of C-C bond scission reached the experimental value 1.5*104 s-1 20 . The CF3 radical react with ozone with enthalpy of reaction equal to - 72.077 kCal mol-1& “G equal to -69.7514kCal mol-1, the reaction of CF3 radical with ozone is most likely to produce the CF3 O and any other product would be thermodynamically unstable or would not contribute to ozone depletion6 . The release radical *CF3 , *F, *CF3 CFH will contribute to ozone depletion through *CF3 O, *FO, *CF3 CFHOcycle respectively, as shown in scheme 2. Scheme 1: The proposed photolysis mechanism of HCFC-124 computed by PM3 method Scheme 2: The *CF3 ,FO*, *CF3 CFH cycle calculated at Semiempirical- PM3 The geometry optimization of the fragment *CF2 ,*CF2 O, *CF3 O, FO*, *CFHO, which resulted in photolysis of HCFC-124 have been computed using PM3 method as represented in table 7. Table 7 Geometry optimization of fragment resulted from photolysis of HCFC-124 calculated at Semiemprical-PM3 method *Energy values in kCal mol-1 unit The vibrational calculation of CFHO (formyl fluoride) has been calculated by the same method which is given six fundamental frequencies two with high intensity one for C=O stretching, which is equal to 1990.43 cm-1 and the other one for C-F stretching which is equal to 1033.8 cm-1 these values reached the experimental value which is equal to 1834 ,1049 cm-1 for C=O,C-F stretching respectively 21. The bond length of CFHO found to be equal to 1.097 ? for C-H bond and 1.34 ? for C-F also 1.202 ? for C=O bond these value reached the experimental value 1.08?,1.4?,1.15? for C-H,C-F,C=O respectively based on electron diffraction data for related molecules22. Conclusion • Depletion of ozone in the stratospheric layer occurs in the presence of HCFC-124 through photolysis of C-Cl bond by energy barrier equal to 61.31 kcal mol-1. • The reactions of the fragment FO, CF3 O, CF3 CFHO with ozone are exothermic with ?Hoverall fall in the range –(48.73 - 48.789) kCal mol-1. • The photolysis net equation of HCFC-124 show that one mole of HCFC-124 deplete six mole of ozone with enthalpy change of reaction equal to -252.64kCal mol-1and free energy change equal to -291.376 kCal mol-1. hv CF3 CFHCl + 6O3 CFHO+CF2 O* +ClO* +FO* +7O2 References [1] Scientific Assessment of Ozone Depletion: 2010, Global Ozone Research and Monitoring Project, Report No. 52, World Meteorological Organization, Geneva, Switzerland, 2011. [2] Jabbar, A.; Munir, A. Ozone Layer Depletion and its Prevention: From Theory to Practice . The Sustainable Development Policy Institute.1993. [3] Müller, R. Stratospheric Ozone Depletion and Climate Change. Royal Society of Chemistry. 2012. 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