The synthesis of a ruthenium(II) tris(bipyridyl) amino acid is described along with its incorporation into a helix-forming peptide using standard solid-phase peptide synthesis methods. The physical properties of the metalloamino acid separately and in the context of the peptide are reported. The electrochemical potential, absorption spectrum, emission and excitation spectra, and emission lifetime data for the ruthenium(II) tris(bipyridyl) amino acid are similar to those of ruthenium(II) tris(bipyridine), indicating that the amino acid functionality introduced on one of the bipyridine rings does not strongly perturb the properties of the metal complex. The ruthenium(II) tris(bipyridyl) amino acid is amenable to direct incorporation into a synthetic peptide using solid-phase methods and BOC/benzyl chemistry. The 22 amino acid alanine-based peptide produced is 67% helical at 0 degrees C in aqueous buffer, as measured by circular dichroism spectroscopy. The 2,2,2-trifluorethanol helix induction curve and the temperature dependence of the helicity are typical for alanine-based peptides. The Lifson-Roig helix propagation parameter, w, derived from circular dichroism and NMR-monitored kinetic hydrogen-deuterium exchange is 0.5 +/- 0.1 at 0 degrees C, indicating a moderate helix propensity for this metalloamino acid.

A short peptide, acetyl-AHAAAHA-carboxamide, has been synthesized and the histidines cross-linked with a cis-tetraammineruthenium(III) moiety. In the absence of the Ru(III) cross-link, the heptapeptide is essentially structureless, as judged by circular dichroism, NMR chemical shift, and NMR-monitored hydrogen deuterium exchange data. The presence of the cis-Ru(III) cross-link is confirmed by mass spectral data and the characteristic pH dependence of the UV-vis spectrum of the cis-(bis-(imidazole))ruthenium(III) unit. Circular dichroism data indicate that the Ru(III) cross-linked heptapeptide is approximately 37% helical at 0 degrees C. The NMR spectrum of the cross-linked peptide has been fully assigned using TOCSY and ROESY experiments. ROE interactions and J-coupling data provide evidence for helical structure. NMR-monitored hydrogen-deuterium exchange data for the Ru(III)-cross-linked peptide, resolved at the level of the individual amides, give larger protection factors at the ends than in the center of the helix. Steric and polarization effects of the Ru(III) cross-link are proposed to cause this unusual apparent protection pattern. A modification to the Lifson-Roig helix-coil model to account for the effect of the i,i+4 Ru(III) cross-link on the helix-coil transition of a peptide is presented. The model provides an excellent fit to the temperature dependence of the circular dichroism spectrum of the Ru(III)-cross-linked peptide. The modified model indicates that the effect of the cross-link on the nucleation parameter, v(2), is modest (about 7-fold) for residues bounded by the cross-link. Significant increases in the propagation parameter, w, occur for residues within the cross-link. The modification to the Lifson-Roig model accounts for the effect of a Ru(III) cross-link on the circular dichroism spectrum of a previously reported 17 residue peptide.

We have synthesized a 22 residue alanine-based peptide with a tris(bipyridyl)ruthenium(II) amino acid near the middle of the peptide which can act as a photoinducible electron donor. Two histidines spaced i, i + 4 near the C-terminus of the peptide were then cross-linked with a tetraammineruthenium(III) moiety to prenucleate the helix and provide an electron acceptor site. Introduction of the cross-link enhances the average helix content from 67% to 84% at 0 degrees C, as judged by circular dichroism spectroscopy. The temperature dependence of the mean molar residue ellipticity at 222 nm, [THETAV;](222), for the bimetalated peptide was fit to a modified Lifson-Roig helix-coil model to permit extraction of the population of helical conformation at each residue separating the electron donor and acceptor. On average, the residues between the donor and acceptor are 92% helical. Photoinduced electron transfer with a driving force of -1.0 eV and an estimated reorganization energy of 0.82 eV was measured by fluorescence quenching methods in H(2)O and D(2)O, yielding rate constants, k(ET), of 7 +/- 3 x 10(6) s(-)(1) and 5 +/- 1 x 10(6) s(-)(1) at 0 degrees C. Calculation of the electronic coupling matrix element, H(ab), with the Marcus equation yields a value of 0.19 +/- 0.4 cm(-)(1). Analysis in terms of the pathway model for electronic coupling indicates that this magnitude of H(ab) is consistent with the participation of hydrogen bonds in electronic coupling for an isolated alpha-helix.

Abstract-We have used fluorescence anisotropy to measure in situ the thermodynamics of binding of alanine-rich mutants of the GCN4 basic region/leucine zipper (bZIP) to short DNA duplexes, in which thymines were replaced with uracils, in order to quantify the contributions of the C5 methyl group on thymines with alanine methyl side chains. We simplified the a-helical GCN4 bZIP by alanine substitution: 4A, 11A, and 18A contain four, 11, and 18 alanine mutations in their DNA-binding basic regions, respectively. Titration of fluorescein-labeled duplexes with increasing amounts of protein yielded dissociation constants in the low-to-mid nanomolar range for all bZIP mutants in complex with the AP-1 target site (5 0 -TGACTCA-3 0 ); binding to the nonspecific control duplex was > 1000-fold weaker. Small changes of <1 kcal/mol in binding free energies were observed for wild-type bZIP and 4A mutant to uracil-containing AP-1, whereas 11A and 18A bound almost equally well to native AP-1 and uracil-containing AP-1. These modest changes in binding affinities may reflect the multivalent nature of protein-DNA interactions, as our highly mutated proteins still exhibit native-like behavior. These protein mutations may compensate for changes in enthalpic and entropic contributions toward DNA-binding in order to maintain binding free energies similar to that of the native protein-DNA complex. #

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