Couplage spin-spin : couplage à trois liaisons (couplage vicinal)

Vicinal or three-bond coupling occurs between protons attached to adjacent carbons. Nuclear spin information transfers via electron spin interactions between adjacent C–H bond orbitals, generally favoring antiparallel spin arrangements. This results in positive 3J values and is commonly observed in proton NMR spectra.

The Karplus equation predicts how 3JHH varies with dihedral angle between orbitals. Stereoelectronic interactions are maximized at zero degrees (synperiplanar) and minimized at 90 degrees (orthogonal). Strong coupling also occurs at 180 degrees when sp3 orbital back lobes overlap, creating a characteristic relationship between geometry and coupling strength.

Vicinal coupling magnitude depends on C–C bond length, the two H–C–C angles, electron-withdrawing substituents, and the dihedral angle between involved orbitals. These stereoelectronic factors collectively determine how effectively nuclear spin information transfers through the bonding framework and affects the observed coupling constant.

In cyclohexane derivatives, ring flipping is restricted by bulky substituents, so the vicinal coupling constant reflects a fixed dihedral angle. In acyclic systems, single bonds rotate rapidly, and the observed coupling constant is an average over all conformations, producing different splitting patterns and coupling values.

Nuclear spin information in vicinal coupling transfers primarily via electron spin interactions between adjacent C–H bond orbitals. This mechanism generally favors antiparallel arrangement of spins, explaining why 3J values are typically positive and why coupling is observed across three bonds.

Stereoelectronic interactions are maximized when orbitals are synperiplanar at a dihedral angle of zero degrees, producing strong coupling. Interactions are minimized when orbitals are orthogonal at 90 degrees. This orbital overlap dependency explains why the Karplus equation successfully predicts vicinal coupling constants across different molecular geometries.

In acyclic systems with freely rotating single bonds, the observed coupling constant represents an average over all rapidly interconverting conformations. This dynamic averaging differs from rigid cyclohexane derivatives, where restricted ring flipping produces coupling constants reflecting a single predominant dihedral angle.