Reaction centers of wild-type Rhodobacter sphaeroides were selectively (13)C-isotope labeled in bacteriochlorophyll and bacteriopheophytin. (13)C solid-state CP/MAS NMR and photo-CIDNP were used to provide insight into the electronic structure of the primary electron donor and acceptor on the atomic scale. The first 2-dimensional photochemically induced dynamic nuclear polarization (photo-CIDNP) (13)C-(13)C solid-state MAS NMR spectra reveal that negative charging of the two BChl rings of the primary donor is involved in ground-state tuning of the oxidation potential of these cofactors in the protein via local electrostatic interactions. In particular, the (13)C shifts show moderate differences in the electronic structure between the two BChl molecules of the special pair in the electronic ground state, which can be attributed to hydrogen bonding of one of the BChl molecules. The major fraction of the electron spin density is strongly delocalized over the two BChl molecules of the special pair and the photochemically active BPhe. A small fraction of the pi-spin density is distributed over a fourth component, which is assigned to the accessory BChl. Comparison of the photo-CIDNP data with "dark" NMR spectra obtained in ultra high field indicates a rigid special pair environment upon photoreaction and suggests that structural changes of the aromatic macrocycles of the two BChl molecules of the special pair do not significantly contribute to the reorganization energy associated with the charge-transfer process.
Selective 2H-, 13C-, and 17O-isotope labeling of the tyrosine amino acid has been used to map the unpaired π-electron spin-density distribution of the UV-generated neutral l-tyrosine phenoxy radical in alkaline frozen solution. The use of 13C and 17O labels allowed accurate determination of the full spin-density distribution and provided more insight in the geometrical structure of the neutral tyrosine radical in vitro. Simulations of the X-band (9.2 GHz) and Q-band (34.8 GHz) EPR powder spectra yielded the principal components of the 1H-, 13C-, and 17O-hyperfine tensors. For the two β-methylene hydrogens, a static conformational distribution of the dihedral angles (90° < θ1 < 60° and 60° < θ2 < 30°) was taken into account. The major proton hyperfine interactions and the principal g values for the neutral tyrosine radical, obtained from selectively deuterated samples, are consistent with literature values. The spin density at the specifically labeled postitions (C1‘, C2‘, C3‘, C4‘, C5‘, O4‘) was evaluated from the anisotropy of the 13C- and 17O-hyperfine tensors. A quantitative analysis of the positions C3‘ and C5‘ provided evidence for a planar distortion of the aromatic ring at these positions. 17O enrichment of the phenol oxygen O4‘ of the tyrosine radical unambiguously showed that the spin density at this oxygen is 0.26 ± 0.01. From the relatively large delocalization of the spin density over the carbonyl group of the tyrosine aromatic ring system, it is concluded that the C4‘−O4‘ bond has a double-bond character. The experimentally determined spin-density distribution is compared with several computational calculated spin-density distributions found in the literature. The isotropic 13C-hyperfine interactions are discussed in the framework of the Karplus−Fraenkel theory. This theory proved to be accurate for the determination of sign and magnitude of the isotropic 13C- and 17O-hyperfine interactions.
Ampullosporin A and alamethicin are two members of the peptaibol family of antimicrobial peptides. These compounds are produced by fungi and are characterized by a high content of hydrophobic amino acids, and in particular the alpha-tetrasubstituted amino acid residue ?-aminoisobutyric acid. Here ampullosporin A and alamethicin were uniformly labeled with (15)N, purified and reconstituted into oriented phophatidylcholine lipid bilayers and investigated by proton-decoupled (15)N and (31)P solid-state NMR spectroscopy. Whereas alamethicin (20 amino acid residues) adopts transmembrane alignments in 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) or 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) membranes the much shorter ampullosporin A (15 residues) exhibits comparable configurations only in thin membranes. In contrast the latter compound is oriented parallel to the membrane surface in 1,2-dimyristoleoyl-sn-glycero-3-phosphocholine and POPC bilayers indicating that hydrophobic mismatch has a decisive effect on the membrane topology of these peptides. Two-dimensional (15)N chemical shift -(1)H-(15)N dipolar coupling solid-state NMR correlation spectroscopy suggests that in their transmembrane configuration both peptides adopt mixed alpha-/3(10)-helical structures which can be explained by the restraints imposed by the membranes and the bulky alpha-aminoisobutyric acid residues. The (15)N solid-state NMR spectra also provide detailed information on the helical tilt angles. The results are discussed with regard to the antimicrobial activities of the peptides.
The all-trans to 13-cis photoisomerization of the retinal chromophore of bacteriorhodopsin occurs selectively, efficiently, and on an ultrafast time scale. The reaction is facilitated by the surrounding protein matrix which undergoes further structural changes during the proton-transporting reaction cycle. Low-temperature polarized Fourier transform infrared difference spectra between bacteriorhodopsin and the K intermediate provide the possibility to investigate such structural changes, by probing O-H and N-H stretching vibrations [Kandori, Kinoshita, Shichida, and Maeda (1998) J. Phys. Chem. B 102, 7899-7905]. The measurements of [3-18O]threonine-labeled bacteriorhodopsin revealed that one of the D2O-sensitive bands (2506 cm(-1) in bacteriorhodopsin and 2466 cm(-1) in the K intermediate, in D2O exhibited 18(O)-induced isotope shift. The O-H stretching vibrations of the threonine side chain correspond to 3378 cm(-1) in bacteriorhodopsin and to 3317 cm(-1) in the K intermediate, indicating that hydrogen bonding becomes stronger after the photoisomerization. The O-H stretch frequency of neat secondary alcohol is 3340-3355 cm(-1). The O-H stretch bands are preserved in the T46V, T90V, T142N, T178N, and T205V mutant proteins, but diminished in T89A and T89C, and slightly shifted in T89S. Thus, the observed O-H stretching vibration originates from Thr89. This is consistent with the atomic structure of this region, and the change of the S-H stretching vibration of the T89C mutant in the K intermediate [Kandori, Kinoshita, Shichida, Maeda, Needleman, and Lanyi (1998) J. Am. Chem. Soc. 120, 5828-5829]. We conclude that all-trans to 13-cis isomerization causes shortening of the hydrogen bond between the OH group of Thr89 and a carboxyl oxygen atom of Asp85.
A new technique is described that is suitable to determine the formation of aggregates from monomeric biomolecules. This technique has been tested in the study of the self-assembling properties of the antibiotic trichogin GA IV which belongs to the class of peptaibols. We have investigated the self-assembling properties of three trichogin analogues by pulsed double resonance in electron spin−echo (PELDOR) spectroscopy combined with conventional continuous wave ESR spectroscopy. In the peptides examined Aib has been substituted by its spin-labeled analogue TOAC at three specific positions of the sequence. More specifically, the magnetic dipole−dipole relaxation of the spin-labeled peptides is measured in glassy polar and apolar solvents at 77 K. Specific assemblies of trichogin molecules are formed in an apolar solvent but addition of a more polar solvent leads to dissociation of the aggregates. The estimates based on experimental data show that each aggregate cluster contains four peptide molecules. Some of the distances between spin labels in the cluster have been determined. In addition, CW-ESR data suggest the occurrence of aggregated species in the same solutions at room temperature. The experimental results are consistent with a model wherein four amphiphilic helical peptide molecules form a vesicular system with the polar amino acid side chains pointing to the interior and the apolar side chains to the exterior of the cluster.
Solid-state 13C magic angle spinning (MAS) NMR has been used to investigate detergent-solubilized photosynthetic reaction centers of Rhodobacter sphaeroides R26, selectively enriched in [4-13C]-tyrosine. The reaction centers were frozen, in the dark and while subject to intense illumination, and studied at temperatures between approximately 215 and approximately 260 K. The signal consists of at least seven narrow lines superimposed on a broad doublet. The chemical shift anisotropy is similar to that for crystalline tyrosine. The two narrowest resonances, corresponding to signals from individual tyrosines, are 28 +/- 5 Hz wide, comparable to what is observed for quaternary carbons in linearly elastic organic solids. The line width as well as the chemical shift of these signals is essentially independent of temperature. This provides strong evidence for an unusually ordered, well-shielded, and structurally, electrostatically, and thermodynamically stable interior of the protein complex without structural heterogeneities. As the temperature is lowered, additional signal from the labels develops and the natural abundance resonances from the detergent broaden, providing evidence for considerable flexibility at the exterior of the protein complex and in the detergent belt at the higher temperatures. In addition, the NMR provides evidence for an electrostatically uniform and neutral complex, since the total dispersion in isotropic shifts for the labels is < 5 ppm and corresponds to electron density variations of less than 0.03 electronic equivalents with respect to tyrosine in the solid state or in solution. When the sample is frozen while subject to intense illumination, a substantial part of the protein is brought into the charge-separated state P.+QA.-. At least three sharp resonances, including the narrowest lines, are substantially reduced in intensity. It is argued that this effect is caused by the electronic spin density associated with the oxidized primary donor P.+. These results strongly suggest that the environment of the special pair is extremely rigid and question the role of protein conformational distortions during the primary photoprocess.
Fourier transform infrared spectra of the L intermediate of light-adapted bacteriorhodopsin were examined for recombinant proteins with amino acid substitutions at Thr46 and Asp96. Two O-H stretching vibrational bands of water, at 3607 and 3577 cm-1, change into stronger H-bonding states in L of the wild type. Thr46-->Val substitution abolished these bands in spite of the fact that [3-18O]threonine-labeling did not shift them, indicating that they correspond to coordination of the water with Thr46. The two water bands were restored, although with changed frequencies, by an additional Asp96-->Asn substitution in Thr46-->Val/Asp96-->Asn. A single Asp96-->Asn substitution abolished the 3607 cm-1 band. Thus, Asp96 also takes part in structural changes in water. The perturbations of these water molecules in the L intermediate displayed a weak correlation with the ratio of intensity change in the two vibrational bands of the Schiff base mode at 1312 and 1301 cm-1 and the rate for the deprotonation of the Schiff base at the L-to-M reaction of the photocycle. We find, therefore, that the water molecules in the cytoplasmic Asp96-Thr46 domain, which comprises the site of proton uptake after formation of the M intermediate, undergo structural changes in the L intermediate already. These changes are transmitted to the extracellular domain and affect interaction of the Schiff base with Asp85, that is far removed from this region.
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