Abstract
A study was made ofX—H...F—C interactions (X= N or O) in small-molecule crystal structures. It was primarily based on 6728 structures containingX—H and C—F and no atom heavier than chlorine. Of the 28 451 C—F moieties in these structures, 1051 interact withX—H groups. However, over three-quarters of these interactions are either the weaker components of bifurcated hydrogen bonds (so likely to be incidental contacts) or occur in structures where there is a clear insufficiency of good hydrogen-bond acceptors such as oxygen, nitrogen or halide. In structures where good acceptors are entirely absent, there is about a 2 in 3 chance that a givenX—H group will donate to fluorine. Viable alternatives areX—H...π hydrogen bonds (especially to electron-rich aromatics) and dihydrogen bonds. The average H...F distances ofX—H...F—C interactions are significantly shorter for CR3F (R= C or H) and Csp2—F acceptors than for CRF3. TheX—H...F angle distribution is consistent with a weak energetic preference for linearity, but that of H...F—C suggests a flat energy profile in the range 100–180°.X—H...F—C interactions are more likely when the acceptor is Csp2—F or CR3F, and when the donor is C—NH2. They also occur significantly more often in structures containing tertiary alcohols or solvent molecules, or withZ′ > 1,i.e.when there may be unusual packing problems. It is extremely rare to findX—H...F—C interactions in structures where there are several unused good acceptors. When it does happen, there is often a clear reason,e.g.awkwardly shaped molecules whose packing isolates a donor group from the good acceptors.
Publisher
International Union of Crystallography (IUCr)
Subject
Materials Chemistry,Metals and Alloys,Atomic and Molecular Physics, and Optics,Electronic, Optical and Magnetic Materials
Cited by
51 articles.
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