A protein conformational change associated with the photoreduction of the primary and secondary quinones in the bacterial reaction center

Probing the primary donor environment in the histidineM200-->leucine and histidineL173-->leucine heterodimer mutants of Rhodobacter capsulatus by light-induced Fourier transform infrared difference spectroscopy

Light-induced P+QB-/PQB FTIR difference spectra of reaction centers (RCs) have been obtained from chromatophores lacking light-harvesting B800-850 antenna for Rhodobacter capsulatus wild type (WT) and for the two mutants HisM200-->Leu and HisL173-->Leu. The primary donor (P) in both mutants consists of a bacteriochlorophyll-bacteriopheophytin heterodimer. The most prominent difference between the WT and the mutant spectra is in the 1600-1200-cm-1 region. The WT spectrum displays large positive bands at approximately 1290, 1500-1430, and 1580-1530 cm-1. These three bands are either small or altogether absent in the heterodimer spectra. In addition, both heterodimer spectra compare well with the electrochemically generated BChla+/BChla spectrum [Mäntele, W.G., Wollenweber, A. M., Nabedryk, E., & Breton, J. (1988) Proc. Natl. Acad. Sci. U.S.A. 85, 8468-8472]. These observations indicate that the positive charge is localized on the monomeric BChl in the heterodimers. The overall shape of the ester and keto C = O signals in the BChla+/BChla spectrum is maintained in the in situ spectra although significant differences are observed in the frequency, width, and splitting of the bands. The shape of the signal at 1757/1744 cm-1 in HisL173-->Leu is comparable to the 1751/1737-cm-1 signal of BChla+/BChla in tetrahydrofuran, indicating a free 10a ester C = O of PM in HisL173-->Leu. The reduced amplitude of the negative 1740-cm-1 feature in both HisM200-->Leu and WT spectra suggests a hydrogen-bonded 10a ester C = O for PL.(ABSTRACT TRUNCATED AT 250 WORDS)

A new infrared electronic transition of the oxidized primary electron donor in bacterial reaction centers: a way to assess resonance interactions between the bacteriochlorophylls

The primary electron donor in the reaction center of purple photosynthetic bacteria consists of a pair of bacteriochlorophylls (PL and PM). The oxidized dimer (P+) is expected to have an absorption band in the mid-IR, whose energy and dipole strength depend in part on the resonance interactions between the two bacteriochlorophylls. A broad absorption band with the predicted properties was found in a previously unexplored region of the spectrum, centered near 2600 cm-1 in reaction centers of Rhodobacter sphaeroides and several other species of bacteria that contain bacteriochlorophyll a, and near 2750 cm-1 in Rhodopseudomonas viridis. The band is not seen in the absorption spectrum of the monomeric bacteriochlorophyll cation in solution, and it is missing or much diminished in the reaction centers of bacterial mutants that have a bacteriopheophytin in place of either PL or PM. With the aid of a relatively simple quantum mechanical model, the measured transition energy and dipole strength of the band can be used to solve for the resonance interaction matrix element that causes an electron to move back and forth between PL and PM, and also for the energy difference between states in which a positive charge is localized on either PL or PM. (The absorption band can be viewed as representing a transition between supermolecular eigenstates that are obtained by mixing these basis states.) The values of the matrix element obtained in this way agree reasonably well with values calculated by using semiempirical atomic resonance integrals and the reaction center crystal structures.(ABSTRACT TRUNCATED AT 250 WORDS)

Time-resolved infrared spectroscopy of electron transfer in bacterial photosynthetic reaction centers: dynamics of binding and interaction upon QA and QB reduction

Light-induced forward electron transfer in the bacterial photosynthetic reaction center from Rhodobacter sphaeroides was investigated by time-resolved infrared spectroscopy. Using a highly sensitive kinetic photometer based on a tunable IR diode laser source [Mäntele, W., Hienerwadel, R., Lenz, F., Riedel, W. J., Grisar, R., & Tacke, M. (1990a) Spectrosc. Int. 2, 29-35], molecular processes concomitant with electron-transfer reactions were studied in the microsecond-to-second time scale. Infrared (IR) signals in the 1780-1430-cm-1 spectral region, appearing within the instrument time resolution of about 0.5 microseconds, could be assigned to molecular changes of the primary electron donor upon formation of a radical cation and to modes of the primary quinone electron acceptor QA and its environment upon formation of QA-. These IR signals are consistent with steady-state FTIR difference spectra of the P+Q- formation [Mäntele, W., Nabedryk, E., Tavitian, B. A., Kreutz, W., & Breton, J. (1985) FEBS Lett. 187, 227-232; Mäntele, W., Wollenweber, A., Nabedryk, E., & Breton, J. (1988) Proc. Natl. Acad. Sci. U.S.A. 85, 8468-8472; Nabedryk, E., Bagley, K. A., Thibodeau, D. L., Bauscher, M., Mäntele, W., & Breton, J. (1990) FEBS Lett. 266, 59-62] and with time-resolved FTIR studies [Thibodeau, D. L., Nabedryk, E., Hienerwadel, R., Lenz, F., Mäntele, W., & Breton, J. (1990) Biochim. Biophys. Acta 1020, 253-259]. At given wavenumbers, kinetic components with a half-time of approximately 120 microseconds were observed and attributed to QA----QB electron transfer. The time-resolved IR signals, in contrast to steady-state experiments where full protein relaxation after electron transfer can occur, allow us to follow directly the modes of QA and QB and their protein environment under conditions of forward electron transfer. Apart from signals attributed to the primary electron donor, signals are proposed to arise not only from the C = O and C = C vibrational modes of the neutral quinones and from the C-O and C-C vibrations of their semiquinone anion form but also from amino acid groups forming their binding sites. Some of the signals appearing with the instrument rise time as well as the transient 120-microseconds signals are interpreted in terms of binding and interaction of the primary and secondary quinone electron acceptor in the Rb. sphaeroides reaction center and of the conformational changes in their binding site.(ABSTRACT TRUNCATED AT 400 WORDS)

FTIR difference spectroscopy of bacteriorhodopsin: toward a molecular model

Bacteriorhodopsin (bR) is a light-driven proton pump whose function includes two key membrane-based processes, active transport and energy transduction. Despite extensive research on bR and other membrane proteins, these processes are not fully understood on the molecular level. In the past ten years, the introduction of Fourier transform infrared (FTIR) difference spectroscopy along with related techniques including time-resolved FTIR difference spectroscopy, polarized FTIR, and attenuated total reflection FTIR has provided a new approach for studying these processes. A key step has been the utilization of site-directed mutagenesis to assign bands in the FTIR difference spectrum to the vibrations of individual amino acid residues. On this basis, detailed information has been obtained about structural changes involving the retinylidene chromophore and protein during the bR photocycle. This includes a determination of the protonation state of the four membrane-embedded Asp residues, identification of specific structurally active amino acid residues, and the detection of protein secondary structural changes. This information is being used to develop an increasingly detailed picture of the bR proton pump mechanism.

Light-induced charge separation in Rhodopseudomonas viridis reaction centers monitored by Fourier-transform infrared difference spectroscopy: the quinone vibrations

Static FTIR light-induced difference spectra have been recorded for reaction centers from Rhodopseudomonas viridis in the following charge-separated states: P+QA(-)-PQA, P+QB(-)-PQB, I(-)-I, I-QA(-)-IQA, and I-QA(2-)-IQA. A comparison of the I(-)-I difference spectra with the I-QA(-)-IQA difference spectra reveals new bands which can be assigned to QA- vibrations; these vibrations are also observed in the P+QA(-)-PQA and P+QB(-)-PQB difference spectra. Through an analysis of all of the static difference spectra, the electron-transfer pathway can be monitored in the infrared from the primary donor, P, to the secondary acceptor, QB, via the intermediate acceptor, I, and the primary acceptor, QA. The difference spectra are dominated by absorbance changes of prosthetic groups, with very few identifiable contributions from amino acids and little overall structural change in the protein backbone, involving only one or two residues for the various charge-separated states. Oxidation of the primary donor in the reaction center shows the characteristic absorbance changes of the 9-keto and 10-ester carbonyl groups observed upon oxidation of bacteriochlorophyll b in a non-hydrogen-bonded environment [Ballschmiter, K. H., & Katz, J. J. (1969) J. Am. Chem. Soc. 91, 2661-2677]. Reduction of the quinones in the reaction center yields absorbance changes of the carbonyls observed during reduction of quinones in a hydrogen-bonded environment [Bauscher, M., Nabedryk, E., Bagley, K., Breton, J., & Mäntele, W. (1990) FEBS Lett. 261, 191-195].(ABSTRACT TRUNCATED AT 250 WORDS)

Photooxidation of high-potential (c559, c556) and low-potential (c552) hemes in the cytochrome subunit of Rhodopseudomonas viridis reaction center. Characterization by FTIR spectroscopy

The photooxidation of c559, c556 and c552 hemes in Rhodopseudomonas viridis cytochrome has been characterized by light-induced FTIR difference spectroscopy. Apart from the common features at 1659 cm-1 and 1561/1551 cm-1 which could arise from one (or possibly two) peptide bond(s), no evidence for major structural rearrangement of the polypeptide backbone was observed. A significant difference with respect to redox-induced FTIR spectra of cytochrome c is the absence of the Tyr marker at 1514/1518 cm-1 in Rps. viridis cytochrome, indicating that the localized shift of a Tyr side chain observed between ferro- and ferri-cytochrome c does not occur in Rps. viridis cytochrome.

Probing the secondary quinone (QB) environment in photosynthetic bacterial reaction centers by light-induced FTIR difference spectroscopy

The photoreduction of the secondary electron acceptor, QB, has been characterized by light-induced Fourier transform infrared difference spectroscopy of Rb. sphaeroides and Rp. viridis reaction centers. The reaction centers were supplemented with ubiquinone (UQ10 or UQ0). The QB- state was generated either by continuous illumination at very low intensity or by single flash in the presence of redox compounds which rapidly reduce the photooxidized primary electron donor P+. This approach yields spectra free from P and P+ contributions making possible the study of the microenvironment of QB and QB-. Assignments are proposed for the C...O vibration of QB- and tentatively for the C = O and C = C vibrations of QB.

Probing the primary quinone environment in photosynthetic bacterial reaction centers by light-induced FTIR difference spectroscopy

The photoreduction of the primary electron acceptor, QA, has been characterized by light-induced Fourier transform infrared difference spectroscopy for Rb. sphaeroides reaction centers and for Rsp. rubrum and Rp. viridis chromatophores. The samples were treated both with redox compounds, which rapidly reduce the photooxidized primary electron P+, and with inhibitors of electron transfer from QA- to the secondary quinone QB. This approach yields spectra free from P and P+ contributions which makes possible the study of the microenvironment of QA and QA-.