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Absolute configuration

Chemical notation for the handedness of a chiral molecule or group

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R and S configuration of chiral centre of enantiomers.
Polimerek · Public domain

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Enantiomers can differ in their chemical properties, but are identical in their physical properties, which can make distinguishing them challenging. Absolute configurations for a chiral molecule (in pure form) are most often obtained by X-ray crystallography, although with some important limitations. All enantiomerically pure chiral molecules crystallise in one of the 65 Sohncke groups (chiral space groups). Alternative techniques include optical rotatory dispersion, vibrational circular dichroism, ultraviolet-visible spectroscopy, the use of chiral shift reagents in proton NMR and Coulomb explosion imaging.

History

Until 1951, it was not possible to obtain the absolute configuration of chiral compounds. It was at some time arbitrarily decided that (+)-glyceraldehyde was the D-enantiomer. The configuration of other chiral compounds was then related to that of (+)-glyceraldehyde by sequences of chemical reactions. For example, oxidation of (+)-glyceraldehyde (1) with mercury oxide gives (−)-glyceric acid (2), a reaction that does not alter the stereocenter. Thus the absolute configuration of (−)-glyceric acid must be the same as that of (+)-glyceraldehyde. Oxidation of (+)-isoserine (3) by nitrous acid gives (−)-glyceric acid, establishing that (+)-isoserine also has the same absolute configuration. (+)-Isoserine can be converted by a two-stage process of bromination to (−)-3-bromo-2-hydroxy-propanoic acid (4) and zinc reduction to give (−)-lactic acid (5), therefore (−)-lactic acid also has the same absolute configuration. If a reaction gave the enantiomer of a known configuration, as indicated by the opposite sign of optical rotation, it would indicate that the absolute configuration is inverted.

In 1951, Johannes Martin Bijvoet for the first time used in X-ray crystallography the effect of anomalous dispersion, which is now referred to as resonant scattering, to determine absolute configuration. The compound investigated was (+)-sodium rubidium tartrate and from its configuration (R,R) it was deduced that the original guess for (+)-glyceraldehyde was correct.

Despite the tremendous and unique impact on access to molecular structures, X-ray crystallography poses some challenges. The process of crystallization of the target molecules is time- and resource-intensive, and can not be applied to relevant systems of interest such as many biomolecules (some proteins are an exception) and in situ catalysts. Another important limitation is that the molecule must contain "heavy" atoms (for example, bromine) to enhance the scattering. Furthermore, crucial distortions of the signal arise from the influence of the nearest neighbors in any crystal structure and of solvents used during the crystallization process.

Just recently, novel techniques have been introduced to directly investigate the absolute configuration of single molecules in gas-phase, usually in combination with ab initio quantum mechanical theoretical calculations, therefore overcoming some of the limitations of the X-ray crystallography.

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