N-1, F-19, AND C-13 NUCLEAR-MAGNETIC-RESONANCE APPROACHES TO THE BARRIER TO ROTATION ABOUT THE CSP(2)-CSP(3) BOND IN 1,1,1-TRIFLUORO-2-PHENYLETHANE - PROXIMATE COUPLING-CONSTANTS AND MOLECULAR-ORBITAL COMPUTATIONS
T. Schaefer et al., N-1, F-19, AND C-13 NUCLEAR-MAGNETIC-RESONANCE APPROACHES TO THE BARRIER TO ROTATION ABOUT THE CSP(2)-CSP(3) BOND IN 1,1,1-TRIFLUORO-2-PHENYLETHANE - PROXIMATE COUPLING-CONSTANTS AND MOLECULAR-ORBITAL COMPUTATIONS, Canadian journal of chemistry, 73(9), 1995, pp. 1387-1394
The H-1, 'F-19 and C-13{H-1} nuclear magnetic resonance spectra of 1,1
,1-trifluoro-2-phenylethane, 1, in CS2-C6D12, acetone-d(6), and benzen
e-d(6) solutions, on analysis, yield long-range coupling constants fro
m which are derived the apparent twofold barriers to rotation about th
e Csp(2)-Csp(3) bonds. The twofold barrier is 9.0(2) kJ/mol, independe
nt of solvent, 4.0 kJ/mol larger than that of ethylbenzene, also indep
endent of solvent. The theoretical barrier heights for the free molecu
les at the post-Hartree-Fock level of molecular orbital theory (frozen
-core MP2/6-31G) also differ by 4 kJ/mol, but are about 1 kJ/mol high
er than the experimental estimates. The,perpendicular conformer is the
most stable for both molecules. Comparisons are made with the benzyl
halides, in which the internal barriers are remarkably sensitive to so
lvent. A spin-spin coupling constant over five formal bonds, (5)J(H, F
) involving the ortho protons in 1, is +0.74(2) Hz and is discussed in
some detail in terms of its dependence on internuclear distances (pos
sible through-space interactions). The solvent perturbations of (3)J(H
, F) and of (2)J(C, F) are of opposite sign. Other long-range coupling
constants or their absence are also pointed out. For example, those b
etween F-19 and C-13 nuclei or protons at the meta position are effect
ively zero; at the para position they are significant.