Reactivity Trends in the Gas-Phase Addition of Acetylene to the N-Protonated Aryl Radical Cations of Pyridine, Aniline, and Benzonitrile

Shiels, Oisin J., Kelly, P. D., Bright, Cameron C., , , Da Silva, Gabriel, & Trevitt, Adam J. (2021) Reactivity Trends in the Gas-Phase Addition of Acetylene to the N-Protonated Aryl Radical Cations of Pyridine, Aniline, and Benzonitrile. Journal of the American Society for Mass Spectrometry, 32(2), pp. 537-547.

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Description

A key step in gas-phase polycyclic aromatic hydrocarbon (PAH) formation involves the addition of acetylene (or other alkyne) to σ-type aromatic radicals, with successive additions yielding more complex PAHs. A similar process can happen for N-containing aromatics. In cold diffuse environments, such as the interstellar medium, rates of radical addition may be enhanced when the σ-type radical is charged. This paper investigates the gas-phase ion-molecule reactions of acetylene with nine aromatic distonic σ-type radical cations derived from pyridinium (Pyr), anilinium (Anl), and benzonitrilium (Bzn) ions. Three isomers are studied in each case (radical sites at the ortho, meta, and para positions). Using a room temperature ion trap, second-order rate coefficients, product branching ratios, and reaction efficiencies are measured. The rate coefficients increase from para to ortho positions. The second-order rate coefficients can be sorted into three groups: low, between 1 and 3 × 10-12 cm3 molecule-1 s-1 (3Anl and 4Anl); intermediate, between 5 and 15 × 10-12 cm3 molecule-1 s-1 (2Bzn, 3Bzn, and 4Bzn); and high, between 8 and 31 × 10-11 cm3 molecule-1 s-1 (2Anl, 2Pyr, 3Pyr, and 4Pyr); and 2Anl is the only radical cation with a rate coefficient distinctly different from its isomers. Quantum chemical calculations, using M06-2X-D3(0)/6-31++G(2df,p) geometries and DSD-PBEP86-NL/aug-cc-pVQZ energies, are deployed to rationalize reactivity trends based on the stability of prereactive complexes. The G3X-K method guides the assignment of product ions following adduct formation. The rate coefficient trend can be rationalized by a simple model based on the prereactive complex forward barrier height.

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20 citations in Web of Science®
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ID Code: 209973
Item Type: Contribution to Journal (Journal Article)
Refereed: Yes
ORCID iD:
Poad, Berwyck L.J.orcid.org/0000-0002-0420-6116
Blanksby, Stephen J.orcid.org/0000-0002-8560-756X
Additional Information: Funding Information: A.J.T., S.J.B., and G.d.S. acknowledge project funding from the Australian Research Council Discovery Program (DP170101596). This work was supported by computational resources provided by the Australian Government through the National Computation Infrastructure under the National Computational Merit Allocation Scheme. The authors also acknowledge the generous allocation of computing resources by the National Computational Infrastructure National Facility (Canberra, ACT, Australia) under the Merit Allocation Scheme. P.D.K. and O.J.S. acknowledge receipt of an Australian Government Research Training Program Scholarship. We are also grateful for the assistance of A. J. Turner and B. R. Burns in aspects of the experiment.
Measurements or Duration: 11 pages
Keywords: computational chemistry, distonic, gas-phase, ion-trap mass spectrometry, kinetics, laser photolysis, PAH formation, radical cation
DOI: 10.1021/jasms.0c00386
ISSN: 1044-0305
Pure ID: 82805997
Divisions: Current > Research Centres > Centre for Materials Science
Current > QUT Faculties and Divisions > Faculty of Science
Current > Schools > School of Chemistry & Physics
Funding Information: A.J.T., S.J.B. and G.d.S. acknowledge project funding from the Australian Research Council Discovery Program (DP170101596). This work was supported by computational resources provided by the Australian Government through the National Computation Infrastructure under the National Computational Merit Allocation Scheme. The authors also acknowledge the generous allocation of computing resources by the National Computational Infrastructure National Facility (Canberra, ACT, Australia) under the Merit Allocation Scheme. P.D.K. and O.J.S. acknowledge receipt of an Australian Government Research Training Program Scholarship. We are also grateful for the assistance of A. J. Turner and B. R. Burns in aspects of the experiment. A.J.T., S.J.B., and G.d.S. acknowledge project funding from the Australian Research Council Discovery Program (DP170101596). This work was supported by computational resources provided by the Australian Government through the National Computation Infrastructure under the National Computational Merit Allocation Scheme. The authors also acknowledge the generous allocation of computing resources by the National Computational Infrastructure National Facility (Canberra, ACT, Australia) under the Merit Allocation Scheme. P.D.K. and O.J.S. acknowledge receipt of an Australian Government Research Training Program Scholarship. We are also grateful for the assistance of A. J. Turner and B. R. Burns in aspects of the experiment.
Funding:
Copyright Owner: 2021 American Society for Mass Spectrometry
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Deposited On: 27 Apr 2021 04:10
Last Modified: 05 Mar 2025 09:27