Solution structures of casein peptides: NMR, FTIR, CD, and molecular modeling studies of alphas1-casein, 1-23.

To determine its potential for interacting with other components of the casein micelle, the N-terminal section of bovine alphas1-casein-B, residues 1-23, was investigated with nuclear magnetic resonance (NMR), Fourier transform infrared (FTIR) and circular dichroism (CD) spectroscopies, and molecular modeling. NMR data were not consistent with conventional alpha-helical or beta-sheet structures, but changes in N-H proton chemical shifts suggested thermostable structures. Both CD and FTIR predicted a range of secondary structures for the peptide (30-40% turns, 25-30% extended) that were highly stable from 5 degrees C to 25 degrees C. Other conformational elements, such as loops and polyproline II helix, were indicated by FTIR only. Molecular dynamics simulation of the peptide predicted 32% turns and 27% extended, in agreement with FTIR and CD predictions and consistent with NMR data. This information is interpreted in accord with recent spectroscopic evidence regarding the nature of unordered conformations, leading to a possible role of alphas1-casein (1-23) in facilitating casein-casein interactions.

Conformational analysis of the hydrophobic peptide alphas1-casein(136-196).

Hydrophobic interactions are important in the self-association of milk proteins, including alphas1-casein. The extent to which casein interaction sites are influenced by local secondary structure is not widely known. Both primary amino acid sequence and local secondary structure are shown to affect the self-association of the hydrophobic peptide alphas1-casein(136-196). The peptide is aggregated at low concentrations (7 microM and above), as determined by 1H nuclear magnetic resonance (NMR) measurements at pH 6.0 in phosphate buffer. Increase in temperature is shown to induce side chain mobility (melting) as indicated by both 1H NMR and near-UV circular dichroism (CD) measurements. As determined by far-UV CD, there is also a loss in the global amount of extended structure with increasing temperature, while beta-turn structures and some aromatic dichroism are conserved at temperatures as high as 70 degrees C. Similar retention of structure occurs at pH 2 and in 6 M guanidine HCl. The observed stability of beta-turns and some side chains in alphas1-casein(136-196) supports previous assumptions that hydrophobic, proline-based turns are important interaction sites in the self-association of alphas1-casein, and possibly in the formation of the calcium transport complexes, the casein micelles. It may be speculated that these areas of the peptide represent a 'molten globule-like', heat stable, core structure for alphas1-casein.

Effect of self-association of alphas1-casein and its cleavage fractions alphas1-casein(136-196) and alphas1-casein(1-197),1 on aromatic circular dichroic spectra: comparison with predicted models.

The self-association of native alphas1-casein is driven by a sum of interactions which are both electrostatic and hydrophobic in nature. The dichroism of aromatic side chains was used to derive regio-specific evidence in relation to potential sites of alphas1-casein polymerization. Near-ultraviolet circular dichroism (CD) revealed that both tyrosine and tryptophan side chains play a role in alphas1-casein associations. Spectral evidence shows these side chains to be in an increasingly nonaqueous environment as both ionic strength and protein concentration lead to increases in the degree of self-association of the protein from dimer to higher oligomers. Near-UV CD investigation of the carboxypeptidase A treated peptide, alphas1-casein(1-197), indicated that the C-terminal residue (Trp199) may be superficial to these interactions, and that the region surrounding Trp164 is more directly involved in an aggregation site. Similar results for the cyanogen bromide cleavage peptide alphas1-casein(136-196) indicated the presence of strongly hydrophobic interactions. Association constants for the peptides of interest were determined by analytical ultracentrifugation, and also were approximated from changes in the near-UV CD curves with protein concentration. Sedimentation equilibrium experiments suggest the peptide to be dimeric at low ionic strength; like the parent protein, the peptide further polymerizes at elevated (0.224 M) ionic strength. The initial site of dimerization is suggested to be the tyrosine-rich area near Pro147, while the hydrophobic region around Pro168, containing Trp164, may be more significant in the formation of higher-order aggregates.

Effects of paramagnetic cations on the nonexponential spin-lattice relaxation of rare spin nuclei in solids.

Nonexponential spin-lattice relaxation is often observed for rare spin nuclei in the solid state. Deviation from single-component decay may be amplified by the coupling of rare spin nuclei to paramagnetic centers. Nonexponential spin-lattice relaxation was observed in derivatized silica gels resins. This phenomenon was localized and enhanced when paramagnetic transition metal cations were bound to surface functional groups. A stretched exponential analysis method was determined to be robust in fitting nonexponential relaxation curves for silica gels both with and without bound paramagnetic ions. Spin-lattice relaxation rates (T1(-1)) for functional group nuclei increased as a function of percent surface coverage with metal ion. The magnitude of the relaxation rate increase was dependent upon internuclear distances from the paramagnetic center. At low surface coverages, a semi-random distribution of paramagnetic centers increased the degree of stretching of spin-lattice relaxation decays, as measured by decreases in the calculated stretching parameter beta. At higher surface coverages, calculated beta values reached a limiting value, indicating that while the spin-diffusion mechanism in metal-exchanged silica gels is restricted, it is not completely diminished.