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NH and NCl homolytic bond dissociation energies and radical stabilization energies: An assessment of theoretical procedures through comparison with benchmark-quality W2w data

✍ Scribed by Robert J. O'reilly; Amir Karton; Leo Radom


Book ID
104577298
Publisher
John Wiley and Sons
Year
2011
Tongue
English
Weight
814 KB
Volume
112
Category
Article
ISSN
0020-7608

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✦ Synopsis


Abstract

The performance of a large variety of contemporary density functional theory (DFT), double‐hybrid DFT, and high‐level Gaussian‐n (G__n__) procedures has been evaluated for the calculation of bond dissociation energies (BDEs) and radical stabilization energies (RSEs) associated with NX bonds (X = H, Cl). The chosen set of 62 NX systems (31 NH and 31 NCl) span a wide range of biologically relevant species. As reference values, we used benchmark‐quality W2w data that we recently obtained as part of a systematic thermochemical study of substituent effects in these systems. Of the G__n__ schemes, the modified G4 procedures (G4‐5H and G4(MP2)‐6X) perform somewhat better than the corresponding standard G4 procedures for the NX BDEs of these systems. For the NH RSEs, G3X, G3X(MP2), G3X(MP2)‐RAD, G4‐5H, and G4(MP2)‐6X emerge as excellent performers, with mean absolute deviations (MADs) from the benchmark W2w values of 0.9–1.4 kJ mol^–1^. However, for the NCl RSEs, G4 is the best performer, with an MAD of 1.7 kJ mol^–1^. The BDEs of both NH and NCl bonds represent a challenge for DFT procedures. In particular, only a handful of functionals (namely, B3P86, M05‐2X, M06‐2X, and ROB2‐PLYP) perform well, with MADs ≤ 4.5 kJ mol^−1^ for both bond types. Nearly all of the considered DFT procedures perform significantly better for the computation of RSEs, due to a significantly larger degree of error cancelation compared with the BDEs. For the RSEs, BH&HLYP, M05‐2X, M06, M06‐2X, BMK, PBE0, B2‐PLYP, B2GP‐PLYP, B2T‐PLYP, and ROB2‐PLYP are the best performers, with MADs ≤ 4.2 kJ mol^−1^. Reliable values of NH and NCl BDEs may be obtained by using the RSEs calculated by these functionals in conjunction with a thermochemical cycle involving an experimental (or high‐level theoretical) BDE for the H~2~NH or H~2~NCl bond. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2011


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