| Article ID | Journal | Published Year | Pages | File Type | 
|---|---|---|---|---|
| 1411473 | Journal of Molecular Structure | 2009 | 7 Pages | 
Abstract
												Several models have been used in the gas-phase electron diffraction analysis. The most reliable results are expected to be obtained using a dynamic model where the large amplitude motion is simulated by a harmonic angular motion using a Gaussian distribution about the central CC bond. Only the planar anti-ZZ conformer was used in the final refinements due to the high energy difference to the other conformers. The most important bond distances (ra, Ã
ngstrom) and bond angles (â Î±, degrees) are [GED/MP2(Full)/aug-cc-pVTZ]: rC1C2 = [1.509(15), 1.460], rC2 = N3 = [1.295(6), 1.292], rN3Cl5 = [1.706(5), 1.696], rC2C7 = [1.434(11), 1.421], rC7N9 = [1.165(4), 1.170], â C1C2N3 = [114.5(11), 115.6], â C2N3Cl5 = [115.0(4), 115.0], â C1C2C7 = [118.8(8), 118.5], â C2C7N9 = [178.2(15), 177.4]. The dihedral angle N3C2C7N9 is 0°, i.e. the cyano groups are bended towards the Cl atom. Error estimates from electron diffraction are given as: Ïr = 2.5[Ïlsq2 + (0.001r)2]½ for bond distances and Ïâ Â = 2.5Ïlsq for bond angles.
											Keywords
												
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											Authors
												H. Thomassen, S. Gundersen, S. Samdal, 
											