Chem. J. Chinese Universities ›› 2014, Vol. 35 ›› Issue (9): 1926.doi: 10.7503/cjcu20140426
• Physical Chemistry • Previous Articles Next Articles
ZHENG Huayan, ZHANG Riguang*(), LI Zhong
Received:
2014-05-08
Online:
2014-09-10
Published:
2014-07-14
Contact:
ZHANG Riguang
E-mail:zhangriguang@tyut.edu.cn
Supported by:
CLC Number:
TrendMD:
ZHENG Huayan, ZHANG Riguang, LI Zhong. Theoretical Studies on the Interaction of CO and CH3O on CuCl(111) Surface for Methanol Oxidative Carbonylation†[J]. Chem. J. Chinese Universities, 2014, 35(9): 1926.
Method | R(C—O)/nm | BDE/(kJ·mol-1) | v(C—O)/cm-1 |
---|---|---|---|
GGA-BLYP | 0.1143 | 1091.24 | 2128 |
Expt. | 0.1128[ | 1076.38±0.67 [ | 2138[ |
Table 1 Bond length(R), stretching frequency(ν) and bond dissociation energy(BDE) for free CO molecule
Method | R(C—O)/nm | BDE/(kJ·mol-1) | v(C—O)/cm-1 |
---|---|---|---|
GGA-BLYP | 0.1143 | 1091.24 | 2128 |
Expt. | 0.1128[ | 1076.38±0.67 [ | 2138[ |
Mode | Site | R(C—O)/ nm | R(Cu—C)/ nm | R(Cu—O)/ nm | ∠C—O—Cl(Cu)/ (°) | ∠O—C—Cu(Cl)/ (°) | q(CO) | Eads/ (kJ·mol-1) |
---|---|---|---|---|---|---|---|---|
CO(O-down) | Top | 0.1145 | 0.3905 | 179.72 | -0.005 | 11.23 | ||
Cl-site | 0.1145 | 0.4383 | 179.52 | -0.005 | 10.90 | |||
Hollow | 0.1146 | 0.4135 | 179.82 | -0.005 | 11.14 | |||
Bridge | 0.1145 | 0.4152 | 174.94 | -0.004 | 11.12 | |||
CO(C-down) | Top | 0.1153 | 0.1905 | 172.50 | 0.079 | 84.47 | ||
Hollow | 0.1158 | 0.2816 | 179.95 | -0.093 | 18.97 |
Table 2 Predicted geometrical parameter, adsorption energies and Mulliken charge at four selected sites
Mode | Site | R(C—O)/ nm | R(Cu—C)/ nm | R(Cu—O)/ nm | ∠C—O—Cl(Cu)/ (°) | ∠O—C—Cu(Cl)/ (°) | q(CO) | Eads/ (kJ·mol-1) |
---|---|---|---|---|---|---|---|---|
CO(O-down) | Top | 0.1145 | 0.3905 | 179.72 | -0.005 | 11.23 | ||
Cl-site | 0.1145 | 0.4383 | 179.52 | -0.005 | 10.90 | |||
Hollow | 0.1146 | 0.4135 | 179.82 | -0.005 | 11.14 | |||
Bridge | 0.1145 | 0.4152 | 174.94 | -0.004 | 11.12 | |||
CO(C-down) | Top | 0.1153 | 0.1905 | 172.50 | 0.079 | 84.47 | ||
Hollow | 0.1158 | 0.2816 | 179.95 | -0.093 | 18.97 |
Fig.2 Optimized structure of CO, CH3O and CH3OCO at the top site of CuCl(111) surface (A) CO; (B) CH3O; (C) CH3OCO. Green balls represent Cl atoms, orange balls represent Cu atoms, grey balls represent C atoms, white balls represent H atom, red balls represent O atoms.
Site | R(C—O)/nm | R(Cu—O)/nm | ∠C—O—Cu/(°) | ∠O—C—Cl/(°) | Eads/(kJ·mol-1) | |
---|---|---|---|---|---|---|
Hollow | 0.1431 | 0.2508 | 179.723 | -0.423 | 218.02 | |
Top | 0.1390 | 0.1930 | 175.751 | -0.380 | 184.12 |
Table 3 Predicted geometrical parameter, adsorption energies and Mulliken charge of CH3O
Site | R(C—O)/nm | R(Cu—O)/nm | ∠C—O—Cu/(°) | ∠O—C—Cl/(°) | Eads/(kJ·mol-1) | |
---|---|---|---|---|---|---|
Hollow | 0.1431 | 0.2508 | 179.723 | -0.423 | 218.02 | |
Top | 0.1390 | 0.1930 | 175.751 | -0.380 | 184.12 |
Site | R(C nm | R(C—O)/ nm | R( nm | R[Cu—C (nearest)]/nm | ∠O—C—O/ (°) | ∠C—O—C/ (°) | q(CH3OCO) | Eads/ (kJ·mol-1) |
---|---|---|---|---|---|---|---|---|
Top | 0.1258 | 0.1481 | 0.1367 | 0.2046 | 118.350 | 117.837 | 0.171 | 219.59 |
Bridge | 0.1259 | 0.1480 | 0.1368 | 0.2045 | 118.164 | 117.846 | 0.170 | 219.54 |
Cl-site | 0.1257 | 0.1480 | 0.1368 | 0.2052 | 118.517 | 117.887 | 0.171 | 219.27 |
Hollow | 0.1260 | 0.1482 | 0.1369 | 0.2055 | 117.773 | 117.611 | 0.171 | 218.72 |
Table 4 Predicted geometrical parameter, Mulliken charge and adsorption energy of CH3OCO at different adsorption sites
Site | R(C nm | R(C—O)/ nm | R( nm | R[Cu—C (nearest)]/nm | ∠O—C—O/ (°) | ∠C—O—C/ (°) | q(CH3OCO) | Eads/ (kJ·mol-1) |
---|---|---|---|---|---|---|---|---|
Top | 0.1258 | 0.1481 | 0.1367 | 0.2046 | 118.350 | 117.837 | 0.171 | 219.59 |
Bridge | 0.1259 | 0.1480 | 0.1368 | 0.2045 | 118.164 | 117.846 | 0.170 | 219.54 |
Cl-site | 0.1257 | 0.1480 | 0.1368 | 0.2052 | 118.517 | 117.887 | 0.171 | 219.27 |
Hollow | 0.1260 | 0.1482 | 0.1369 | 0.2055 | 117.773 | 117.611 | 0.171 | 218.72 |
Fig.3 Optimized co-adsorbed structure of CO+CH3O and the corresponding transition state for CO interaction with CH3O to CH3OCO over CuCl(111) surface (A) CO+CH3O; (B) TS1. Bond lengths are in nm.
Absorption | Molecule | R(C—O)/ nm | R(Cu—C)/ nm | R(Cu—O)/ nm | ∠C—O—Cl/ (°) | ∠O—C—Cu/ (°) | q(X) | Eads/ (kJ·mol-1) | Ecads/ (kJ·mol-1) | Eint/ (kJ·mol-1) |
---|---|---|---|---|---|---|---|---|---|---|
Co-adsorption | CO | 0.1152 | 0.1918 | 174.247 | 0.212 | 89.74 | 294.92 | 2.89 | ||
CH3O | 0.1425 | 0.2443 | 164.351 | -0.410 | 208.07 | |||||
Single adsorption | CO | 0.1153 | 0.1905 | 175.502 | 0.186 | 84.47 | | | ||
CH3O | 0.1431 | 0.2508 | 179.723 | -0.423 | 218.02 | | |
Table 5 Comparisons of theoretical calculation results between(CO+CH3O)/CuCl(111) co-adsorption and CO/CuCl(111) as well as CH3O/CuCl(111) single adsorption
Absorption | Molecule | R(C—O)/ nm | R(Cu—C)/ nm | R(Cu—O)/ nm | ∠C—O—Cl/ (°) | ∠O—C—Cu/ (°) | q(X) | Eads/ (kJ·mol-1) | Ecads/ (kJ·mol-1) | Eint/ (kJ·mol-1) |
---|---|---|---|---|---|---|---|---|---|---|
Co-adsorption | CO | 0.1152 | 0.1918 | 174.247 | 0.212 | 89.74 | 294.92 | 2.89 | ||
CH3O | 0.1425 | 0.2443 | 164.351 | -0.410 | 208.07 | |||||
Single adsorption | CO | 0.1153 | 0.1905 | 175.502 | 0.186 | 84.47 | | | ||
CH3O | 0.1431 | 0.2508 | 179.723 | -0.423 | 218.02 | | |
Fig.4 Optimized co-adsorbed structure of CH3OCO and CH3O and the corresponding transition state for CH3OCO interaction with CH3O to DMC over CuCl(111) surface (A) CH3OCO+CH3O; (B) TS2; (C) DMC. Bond lengths are in nm.
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