Interaction of Oxalic Acid with Dimethylamine and Its Atmospheric. Implication
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1 Electronic Supplementary Material (ESI) for RSC Advances. This journal is The Royal Society of Chemistry 2017 Interaction of Oxalic Acid with Dimethylamine and Its Atmospheric Implication Jiao Chen, 1,2 Shuai Jiang, 1 Yi-Rong Liu, 1 Teng Huang, 1 Chun-Yu Wang, 1,2 Shou-Kui Miao, 1,2 Zhong-quan Wang, 1,2 Yang Zhang, 1 Wei Huang 1,3,4,5 * 1 Laboratory of Atmospheric Physico- Chemistry, Anhui Institute of Optics & Fine Mechanics, Chinese Academy of Sciences, Hefei, Anhui , China 2 University of Science and Technology of China, Hefei, Anhui , China 3 School of Information Science and Technology, University of Science and Technology of China, Hefei, Anhui , China 4 School of Environmental Science & Optoelectronic Technology, University of Science and Technology of China, Hefei, Anhui , China 5 CAS Center for Excellent in Urban Atmospheric Environment, Xiamen, Fujian , China * huangwei6@ustc.edu.cn Sensitivity analysis of the applied DFT methods and single-point energy calculation based on the DFT methods In order to investigated the sensitivity of the applied DFT methods and singlepoint energy calculation based on the DFT methods, the binding energy ( E), the Gibbs free energy ( G) have been calculated for six typical reactions employing DFT method with G(2d,p) and G(3df,3pd) basis sets. The DFT and DF-LMP2-F12/VDZ-F12//DFT results are compared with a high level calculation of CCSD(T)-F12a/VDZ-F12 as a benchmark of the energies. Table S1 shown the mean absolute error (MAE), mean signed error (MSE) and Maximum error (MaxE) in the DFT binding energies ( E) and single-point energy calculation based on the DFT compared against CCSD(T)-F12a/VDZ-F12 results using both G(2d,p) and G(3df,3pd) basis sets. Our results show that there is a smallest error in the binding energy with 0.71 kcal/mol of MAE and 1.53
2 kcal/mol of MaxE for M06-2X, using the small G(2d,p) basis set. PW91PW91 show the largest MAE, MSE and MaxE of 1.55, 1.37, 2.94 kcal/mol, respectively. The error of MAE is the lowest for ωb97x-d with a value of 0.97 kcal/mol. The value of M06-2X is close to ωb97x-d. Compared the DF-LMP2-F12/VDZ-F12 binding energy with CCSD(T)-F12a/VDZ-F12. The MAE and MSE drop obviously with the value within 0.4 kcal/mol for DF-LMP2-F12/VDZ-F12//DFT. And the maximum errors are also reduced, around 1 kcal/mol. Extending the basis set to G(3df,3pd) improves the results slightly for M06-2X, PW91PW91 andωb97x- D with a difference value of 0.07, 0.40, 0.52 kcal/mol for MAE, and 0.26, 0.29, 0.74 kcal/mol for MaxE, respectively. Table S2 show that changing the basis set from G(2d,p) to G(3df,3pd) obtain a small effect on the Gibbs free energy. There is a very small difference with MAE of 0.6 kacl/mol or less, and the maximum errors are below 0.9 kcal/mol. The MAE difference between the different DFT methods is also very small, below 0.05 kcal/mol. Our comparison results imply that increasing the basis set from G(3df,3pd) to G(2d,p) does not improve the G significantly. The MAE, MSE and MaxE in the CCSD(T)-F12a/VDZ-F12 and DF-LMP2- F12/VDZ-F12 Gibbs free energy can be seen when changing from a G(d,p) to a G(3df,3pd) basis set in Table S3. In all cases there is a minute difference in the CCSD(T)-F12a/VDZ-F12 and DF-LMP2-F12/VDZ-F12 whether the geometries have been optimized with the G(d,p) or G(3df,3pd) basis set. The value of MAE, MSE and MaxE using DF-LMP2-F12/VDZ-F12 almost equal to the
3 CCSD(T)-F12a/VDZ-F12. In conclusion, our results indicate that DF-LMP2- F12/VDZ-F12// M06-2X /6-311+G(2d,p) basis set can be used as a good compromise between accuracy and computational efficient. Table S1 Mean absolute error (MAE), mean signed error (MSE) and Maximum error
4 (MaxE) in the DFT binding energies ( E) and single-point energy calculation based on the DFT of all six reactions a compared against CCSD(T)-F12a/VDZ-F12 results. All energies are in kcal/mol. Method MAE MES MaxE G(2d,p) M06-2x DF-LMP2-F12/VDZ-F12//M06-2x PW91PW DF-LMP2-F12/VDZ-F12//PW91PW ωb97x-d DF-LMP2-F12/VDZ-F12//ωB97X-D G(3df,3pd) M06-2x DF-LMP2-F12/VDZ-F12//M06-2x PW91PW DF-LMP2-F12/VDZ-F12//PW91PW ωb97x-d DF-LMP2-F12/VDZ-F12//ωB97X-D a Reactions are refer to OA + W (OA)(W), (OA)(W) + W (OA)(W) 2, OA + OA (OA) 2, OA + DMA (OA)(DMA), (OA)(DMA) + W (OA)(DMA)(W), OA + (DMA)(OA) (OA) 2 (DMA). Table S2 Mean absolute error (MAE), mean signed error (MSE) and Maximum error
5 (MaxE) in the DFT Gibbs free energy ( G) when changing the basis from G(2d,p) to G(3df,3pd). All energies are in kcal/mol. Method MAE MES MaxE G(2d,p) G(3df,3pd) M06-2x PW91PW ωb97x-d Table S3 Mean absolute error (MAE), mean signed error (MSE) and Maximum error
6 (MaxE) in the CCSD(T)-F12a/VDZ-F12 and DF-LMP2-F12/VDZ-F12 Gibbs free energy ( G) when changing the basis from G(2d,p) to G(3df,3pd). All energies are in kcal/mol. Method MAE MES MaxE G(2d,p) G(3df,3pd) CCSD(T)-F12a/VDZ-F12//M06-2x DF-LMP2-F12/VDZ-F12//M06-2x CCSD(T)-F12a/VDZ-F12//PW91PW DF-LMP2-F12/VDZ-F12// PW91PW CCSD(T)-F12a/VDZ-F12//ωB97X-D DF-LMP2-F12/VDZ-F12//ωB97X-D Figure Caption
7 Figure S1 The local minima for (C 2 H 2 O 4 )(CH 3 NHCH 3 )(H 2 O) n (n = 1-2) optimized at the M06-2x/6-311+G(2d,p) level. Figure S2 The local minima for (C 2 H 2 O 4 )(CH 3 NHCH 3 )(H 2 O) n (n = 3-4) optimized at the M06-2x/6-311+G(2d,p) level. Figure S3 The local minima for (C 2 H 2 O 4 ) 2 (CH 3 NHCH 3 )(H 2 O) n (n = 1-2) optimized at the M06-2x/6-311+G(2d,p) level. Figure S4 The local minima for (C 2 H 2 O 4 ) 2 (CH 3 NHCH 3 )(H 2 O) n (n = 3-4) optimized at the M06-2x/6-311+G(2d,p) level. Figure S1
8 Figure S2
9 Figure S3
10 Figure S4
11 Cartesian Coordinates of optimized Structures
12 OA.1W C C O O O O H H O H H OA.2W C C O O O O H H O H H O H H OA.3W O C O C O O H H O H H O H H
13 O H H OA.4W C C O O O O H H O H H O H H O H H O H H OA C C O O O O H H C C O O O O H H
14 2OA.1W O C O C O O H H O C O C O O H H O H H OA.2W O C O C O O H H O C O C O O H H O H H O H H
15 2OA.3W O C O C O O H H O H H O H H O H H OA.4W O C O C O O H H O C O C O O H H O H H O H H O
16 H H O H H OA.1DMA C N C H H H H H H H O C O C O O H H OA.1DMA.1W-a C N C H H H H H H H O C O C O O H
17 H O H H OA.1DMA.1W-b C N C H H H H H H H O C O C O O H H O H H OA.1DMA.1W-c C N C H H H H H H H O C O C O
18 O H H O H H OA.1DMA.1W-d C N C H H H H H H H O C O C O O H H O H H OA.1DMA.1W-e C N C H H H H H H H O C O
19 C O O H H O H H OA.1DMA.1W-f C N C H H H H H H H O C O C O O H H O H H OA.1DMA.2W-a C N C H H H H H H H O
20 C O C O O H H O H H O H H OA.1DMA.2W-b C N C H H H H H H H O C O C O O H H O H H O H H OA.1DMA.2W-c C N C
21 H H H H H H H O C O C O O H H O H H O H H OA.1DMA.2W-d C N C H H H H H H H O C O C O O H H O H H
22 O H H OA.1DMA.2W-e C N C H H H H H H H O C O C O O H H O H H O H H OA.1DMA.2W-f C N C H H H H H H H O C O
23 C O O H H O H H O H H OA.1DMA.2W-g C N C H H H H H H H O C O C O O H H O H H O H H OA.1DMA.3W-a C N C H H
24 H H H H H O C O C O O H H O H H O H H O H H OA.1DMA.3W-b C N C H H H H H H H O C O C O O H H O H
25 H O H H O H H OA.1DMA.3W-c C N C H H H H H H H O C O C O O H H O H H O H H O H H OA.1DMA.3W-d C N C H H H
26 H H H H O C O C O O H H O H H O H H O H H OA.1DMA.3W-e C N C H H H H H H H O C O C O O H H O H H
27 O H H O H H OA.1DMA.3W-f C N C H H H H H H H O C O C O O H H O H H O H H O H H OA.1DMA.3W-g C N C H H H H
28 H H H O C O C O O H H O H H O H H O H H OA.1DMA.4W-a O C O C O O H H C N C H H H H H H H O H H O
29 H H O H H O H H OA.1DMA.4W-b O C O C O O H H C N C H H H H H H H O H H O H H O H H O H H OA.1DMA.4W-c O C
30 O C O O H H C N C H H H H H H H O H H O H H O H H O H H OA.1DMA.4W-d O C O C O O H H C N C H H H
31 H H H H O H H O H H O H H O H H OA.1DMA.4W-e O C O C O O H H C N C H H H H H H H O H H O H H O H
32 H O H H OA.1DMA.4W-f O C O C O O H H C N C H H H H H H H O H H O H H O H H O H H OA.1DMA.4W-g O C O C O O
33 H H C N C H H H H H H H O H H O H H O H H O H H OA.1DMA.4W-h O C O C O O H H C N C H H H H H H H
34 O H H O H H O H H O H H OA.1DMA C N C H H H H H H H O C O C O O H H O C O C O O H H OA.1DMA.1W-a C N
35 C H H H H H H H O C O C O O H H O C O C O O H H O H H OA.1DMA.1W-b C N C H H H H H H H O C O C O
36 O H H O C O C O O H H O H H OA.1DMA.1W-c C N C H H H H H H H O C O C O O H H O C O C O O H H O H
37 H OA.1DMA.1W-d C N C H H H H H H H O C O C O O H H O C O C O O H H O H H OA.1DMA.1W-e C N C H H H H H H H
38 O C O C O O H H O C O C O O H H O H H OA.1DMA.1W-f C N C H H H H H H H O C O C O O H H O C O C O
39 O H H O H H OA.1DMA.1W-g C N C H H H H H H H O C O C O O H H O C O C O O H H O H H OA.1DMA.2W-a C N C H H
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