C-terminal side of alpha-helix is more stable than N-terminal side

Supramolecular assembly and small molecule recognition by genetically engineered protein block polymers composed of two SADs

Genetically engineered protein block polymers are an important class of biomaterials that have gained significant attention in recent years due to their potential applications in biotechnology, electronics and medicine. The majority of the protein materials have been composed of at least a single self-assembling domain (SAD), enabling the formation of supramolecular structures. Recently, we developed block polymers consisting of two distinct SADs derived from an elastin-mimetic polypeptide (E) and the alpha-helical COMPcc (C). These protein polymers, synthesized as the block sequences--EC, CE, and ECE--were assessed for overall conformation and macroscopic thermoresponsive behavior. Here, we investigate the supramolecular assembly as well as the small molecule binding and release profile of these block polymers. Our results demonstrate that the protein polymers assemble into particles as well as fully or partially networked structures in a concentration dependent manner that is distinct from the individual E and C homopolymers and the E+C non-covalent mixture. In contrast to synthetic block polymers, the structured assembly, binding and release abilities are highly dependent on the composition and orientation of the blocks. These results reveal the promise for these block polymers for therapeutic delivery and biomedical scaffolds.

Alpha-helix to random-coil transitions of two-chain coiled coils: the use of physical models in treating thermal denaturation equilibria of isolated subsequences of alpha alpha-tropomyosin

Two extant models of thermal folding/unfolding equilibria in two-chain, alpha-helical coiled coils are tested by comparison with experimental results on excised, isolated subsequences of rabbit alpha alpha-tropomyosin (Tm). These substances are designated iTmj where i and j are, respectively, the residue numbers (in the 284-residue parent chain) of the N- and C-terminal residues of the subsequence. One model postulates that a coiled coil consists of segments, each denaturing in an all-or-none manner, like small globular proteins. Thus this model yields a small number of populated molecular species. In an extant calorimetry study of 11Tm127 and of 190Tm284, each required only two all-or-none-segments, and their enthalpies and transition temperatures were assigned. These assignments are shown here to yield the concentration of all molecular species, and therefore the helix content, as a function of temperature. Such calculations for 190Tm284 are in tolerable agreement with CD experiments, but those for 11Tm127 are in gross disagreement. Thus, either the model itself or the calorimetric assignment is faculty. In the second model, all conformational states are counted and weighted, as in the Zimm-Bragg theory for single-chain polypeptides. This theory has been extended (by Skolnick) to two-chain coiled coils and is here used to fit CD data for 11Tm127, 142Tm281, and 190Tm284. The fit is tolerable for 11Tm127, good for 142Tm281, and quantitative for 190Tm284. Thus this comparison does not falsify this second model. The helix-helix interaction free energy, obtainable from the fit, shows nonadditivity when isolated subsequences are compared with the parent. This suggests that removal of a region from a long coiled coil allows energetically substantial adjustments in side-chain packing in the helix-helix interface. Thus, the helix-helix interaction in long coiled coils is characteristic of a global free energy minimum and not just of the regional constellation of side chains.

Comparison of alpha-helix stability in peptides having a negatively or positively charged residue block attached either to the N- or C-terminus of an alpha-helix: the electrostatic contribution and anisotropic stability of the alpha-helix

An estimation of the thermodynamic effects of a charged random coil, which is attached either to the N- or C-terminus of polyalanine, upon alpha-helix stability is attempted. A temperature-induced helix-coil transition of Ala20Lys20Phe and Lys20Ala20Phe was studied under various conditions of salt concentration and pH. By combining the results with previous ones for Ala20Glu20Phe and Glu20Ala20Phe, which have opposite electric charges to the present system [S. Ihara et al. (1982) Biopolymers 21, 131-145], the free energy of the coil to helix transition of the polyalanine block could be separated into two terms--one term for the electrostatic interaction of electric charges in the random-coil block with the alpha-helix dipole, and a second term for the intrinsic stability of the helix. The first term indicates the significance of the helix dipole-charge interactions, which affects the helix stability depending on the attaching side of the charged block and on the sign of the charges. This clearly shows the anisotropic stability of the alpha-helix. Furthermore, analysis of the dependence of these thermodynamic quantities on salt concentrations showed, assuming that the effect of the attached electric charges was symmetric (in other words, the absolute values of the electrostatic interaction terms were independent of the sign of electric charges), that the intrinsic stability of the alpha-helix was dependent on which side of the helix was attached to the random coil: a random coil attached to the N-terminus of the alpha-helix had little effect while that attached to a C-terminal significantly destabilized the helix.

Amino acid distribution in protein secondary structures

The compositional distribution of the twenty amino acids was examined for particular positions within secondary structures (alpha-helices, beta-strands, and turns) taken from a 44-protein sample. Correlation coefficients calculated between positional composition of the amino acids and various of their physico-chemical characteristics indicated considerable asymmetry in the properties of the residues comprising regions within and adjacent to secondary structures, modes of helix formation, physical parameters most sensitive to the buriedness of residues in beta-strands, and possible improvements in the accuracy of secondary structure prediction methodologies.