R. D. Guiles

Pseudocontact shifts used in the restraint of the solution structures of electron transfer complexes.

The geometry of the ferricytochrome b5-ferricytochrome c complex has been analysed using long-range interprotein paramagnetic dipolar shifts. Heteronuclear filtered NMR spectra of samples containing 15N-labelled cytochrome b5 in complex with unlabelled cytochrome c allowed unambiguous assessment of pseudocontact shifts relative to diamagnetic reference states. Because pseudocontact shifts can be observed for protons as much as 20 Å from the paramagnetic centre, this approach allows study of electron transfer proteins in fast exchange. Our findings provide the first physical evidence confirming hypotheses presented in previous theoretical studies. The absence of certain predicted shifts that are expected based on the best fit to a static model of the complex suggests that cytochrome b5 is more dynamic in solution than in the crystal, in agreement with molecular dynamics simulations.

NMR studies of the structure and dynamics of peptide E, an endogenous opioid peptide that binds with high affinity to multiple opioid receptor subtypes.

Structural and dynamic properties of opioid peptide E have been examined in an sodium dodecyl sulfate (SDS) micelle. Structural and dynamic studies both indicate that this peptide exhibits greater segmental mobility than typical structured proteins. An nmr structural analysis of adrenal peptide E in SDS micelles indicated the presence of two well-defined beta-turns, one at the N-terminus encompassing residues 3 to 6, and the second in the region between residues 15 and 18. Certain side chain dihedral angles were also remarkably well defined, such as the chi 1 angle of F4, which exhibited a trans configuration. These calculated structures were based on a set of 9.5 restraints per residue. The backbone dynamics of peptide E in SDS micelles were examined through an analysis of 15N-relaxation parameters. An extended model-free analysis was used to interpret the relaxation data. The overall rotational correlation time is 19.7 ns. the average order parameter S2 is 0.66 +/- 0.15. The N-terminal loop region residues including G3 to R6 have an average order parameter of 0.70 +/- 0.23. The average order parameter lies somewhere between that observed for a random coil (e.g., S2 = 0.3) and that of a well-defined tertiary fold (e.g., S2 = 0.86). This suggests that peptide E in SDS micelles adopts a restricted range of conformations rather than a random coil. Based on the helical structure recently obtained for the highly homologous kappa-agonist dynorphin-A(1-17) and the beta-turn in the same region of peptide E, it is reasonable to assume that these two elements of secondary structure reflect different receptor subtype binding geometries. The intermediate order parameters observed for peptide E in an SDS micelle suggest a degree of dynamic mobility that may enable facile interconversion between helical and beta-turn geometries in the N-terminal agonist domain.

1H, 13C and 15N NMR assignments and secondary structure of the paramagnetic form of rat cytochrome b5

SummaryModern multidimensional double- and triple-resonance NMR methods have been applied to assign the backbone and side-chain 13C resonances for both equilibrium conformers of the paramagnetic form of rat liver microsomal cytochrome b5. The assignment of backbone 13C resonances was used to confirm previous 1H and 15N resonance assignments [Guiles, R.D. et al. (1993) Biochemistry, 32, 8329–8340]. On the basis of short- and medium-range NOEs and backbone 13C chemical shifts, the solution secondary structure of rat cytochrome b5 has been determined. The striking similarity of backbone 13C resonances for both equilibrium forms strongly suggests that the secondary structures of the two isomers are virtually identical. It has been found that the 13C chemical shifts of both backbone and side-chain atoms are relatively insensitive to paramagnetic effects. The reliability of such methods in anisotropic paramagnetic systems, where large pseudocontact shifts can be observed, is evaluated through calculations of the magnitude of such shifts.