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Author(s):
Sheng, L.; Li, Z.-S.; Liu, J.-Y.; Xiao, J.-F.; Sun, C.-C.
Title:
Ab initio direct dynamics studies on the reactions of H atoms with CCl4 and CHCl3
Journal:
J. Phys. Chem. A
Volume:
106
Page(s):
12292 - 12298
Year:
2002
Reference type:
Journal article
Squib:
2002SHE/LI12292-12298
Reaction:
CHCl3 + H· → Products
Reaction order:
2
Temperature:
200 - 5000
K
Rate expression:
2.76x10-13 [cm3/molecule s] (T/298 K)2.77 e-10327 [J/mole]/RT
Category: Theory
Data type:
Ab initio
Comments:
Used density functional theory (DFT) and ab initio quantum calculations to determine reaction pathways for reactions of H atoms with CCl4 and CHCl3. Employed BH&HLYP/6-311G(d,p) geometries/frequencies and PM4/6-311+G(3df,2p) energies. Rate expressions calculated using Truhlars Polyrate program employing CVT/SCT tunneling correction. The calculated barrier for CCl4+H = CCl3+HCl was about 6.5 kcal/mol. For reaction with CHCl3, there are two reaction channels, abstraction of H atom with a barrier of about 6.8 kcal/mol and abstraction of Cl with a barrier of about 8.0 kcal/mol. The H atom abstraction channel dominates at low temperature, at about 670 K the two channels are about equal, and at high temperatures (2000 K) the Cl atom abstraction is about 65% of the total rate. For CCl4+H, the calculated rate expression is about 2-3 lower than experimental rate constants (2001 Bryukov, Slagle, and Knyazev) and for CHCl3, the calculated total rate expression is only about 10-30% lower than the experimental values (same reference).
View full bibliographic record.
Rate constant values calculated from the Arrhenius expression:
| T (K) | k(T) [cm3/molecule s] |
| 200 |
1.84E-16 |
| 300 |
4.48E-15 |
| 400 |
2.80E-14 |
| 500 |
9.66E-14 |
| 600 |
2.42E-13 |
| 700 |
4.99E-13 |
| 800 |
9.02E-13 |
| 900 |
1.48E-12 |
| 1000 |
2.28E-12 |
| 1100 |
3.33E-12 |
| 1200 |
4.65E-12 |
| 1300 |
6.29E-12 |
| 1400 |
8.26E-12 |
| 1500 |
1.06E-11 |
| 1600 |
1.34E-11 |
| 1700 |
1.65E-11 |
| 1800 |
2.02E-11 |
| 1900 |
2.43E-11 |
| 2000 |
2.90E-11 |
| 2100 |
3.42E-11 |
| 2200 |
3.99E-11 |
| 2300 |
4.63E-11 |
| 2400 |
5.32E-11 |
| 2500 |
6.08E-11 |
| 2600 |
6.91E-11 |
| 2700 |
7.81E-11 |
| 2800 |
8.78E-11 |
| 2900 |
9.83E-11 |
| 3000 |
1.10E-10 |
| 3100 |
1.22E-10 |
| 3200 |
1.34E-10 |
| 3300 |
1.48E-10 |
| 3400 |
1.63E-10 |
| 3500 |
1.78E-10 |
| 3600 |
1.94E-10 |
| 3700 |
2.12E-10 |
| 3800 |
2.30E-10 |
| 3900 |
2.49E-10 |
| 4000 |
2.70E-10 |
| 4100 |
2.91E-10 |
| 4200 |
3.13E-10 |
| 4300 |
3.36E-10 |
| 4400 |
3.61E-10 |
| 4500 |
3.87E-10 |
| 4600 |
4.13E-10 |
| 4700 |
4.41E-10 |
| 4800 |
4.70E-10 |
| 4900 |
5.01E-10 |
| 5000 |
5.32E-10 |
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