Fourier transform infrared evidence of proton uptake by glutamate L212 upon reduction of the secondary quinone QB in the photosynthetic reaction center from Rhodobacter capsulatus

The photoreduction of the secondary quinone Q(B) in native reaction centers (RCs) of Rhodobacter capsulatus and in RCs from the GluL212 --> Gln and GluL212 --> Ala mutants has been investigated at pH 7 in (1)H(2)O and (2)H(2)O by light-induced Fourier transform infrared (FTIR) difference spectroscopy. The Q(B)(-)/Q(B) FTIR difference spectra reflect changes of quinone-protein interactions and of protonation state of carboxylic acid groups as well as reorganization of the protein upon electron transfer. Comparison of Q(B)(-)/Q(B) spectra of native and mutant RCs indicates that the interactions between Q(B) or Q(B)(-) and the protein are similar in all RCs. A differential signal at approximately 1650/1640 cm(-1), which is common to all the spectra, is associated with a movement of a peptide carbonyl or a side chain following Q(B) reduction. On the other hand, Q(B)(-)/Q(B) spectra of native and mutant RCs display several differences, notably between 1700 and 1650 cm(-1) (amide I and side chains), between 1570 and 1530 cm(-1) (amide II), and at 1728-1730 cm(-1) (protonated carboxylic acid groups). In particular, the latter region in native RCs is characterized by a main positive band at 1728 cm(-1) and a negative signal at 1739 cm(-1). In the L212 mutants, the amplitude of the positive band is strongly decreased leading to a differential signal at 1739/1730 cm(-1) that is insensitive to (1)H/(2)H isotopic exchange. In native RCs, only the 1728 cm(-1) band is affected in (2)H(2)O while the 1739 cm(-1) signal is not. The effects of the mutations and of (1)H/(2)H exchange on the Q(B)(-)/Q(B) spectra concur in the attribution of the 1728 cm(-1) band in native RCs to (partial) proton uptake by GluL212 upon the first electron transfer to Q(B), as previously observed in Rhodobacter sphaeroides RCs [Nabedryk, E., Breton, J., Hienerwadel, R., Fogel, C., M?ntele, W., Paddock, M. L., and Okamura, M. Y. (1995) Biochemistry 34, 14722-14732]. More generally, strong homologies of the Q(B) to Q(B)(-) transition in the RCs from Rb. sphaeroides and Rb. capsulatus are detected by differential FTIR spectroscopy. The FTIR data are discussed in relation with the results from global proton uptake measurements and electrogenic events concomitant with the reduction of Q(B) and with a model of the Q(B) turnover in Rb. sphaeroides RCs [Mulkidjanian, A. Y. (1999) FEBS Lett. 463, 199-204].     

Conformational study of globulin from rice (Oryza sativa) seeds by Fourier-transform infrared spectroscopy

The conformation of rice globulin (10%, w/v, in deuterated phosphate buffer, pD 7.4) under the influence of pH, chaotropic salts, several protein structure perturbants and heat treatments was studied by Fourier-transform infrared (FTIR) spectroscopy. Rice globulin exhibited seven major bands in the region of 1700-1600 cm-1 and the spectrum suggests high alpha-helical content with large quantities of beta-sheet and beta-turn structures. Highly acidic and alkaline pH conditions induced changes in band intensity attributed to intermolecular beta-sheet structure (1681 and 1619 cm-1). Addition of chaotropic salts led to progressive changes in band intensity, following the lyotropic series of anions, whereas several protein structure perturbants caused shifts in band positions. Heating at increasing temperature led to progressive decreases in alpha-helical content and increases in random coil structures, suggesting protein denaturation. This was accompanied by intensity increases in the intermolecular beta-sheet transitions.     

The role of Val-265 for flavin adenine dinucleotide (FAD) binding in pyruvate oxidase: FTIR, kinetic, and crystallographic studies on the enzyme variant V265A

In pyruvate oxidase (POX) from Lactobacillus plantarum, valine 265 participates in binding the cofactor FAD and is responsible for the strained conformation of its isoalloxazine moiety that is visible in the crystal structure of POX. The contrasting effects of the conservative amino acid exchange V265A on the enzyme's catalytic properties, cofactor affinity, and protein structure were investigated. The most prominent effect of the exchange was observed in the 2.2 A crystal structure of the mutant POX. While the overall structures of the wild-type and the variant are similar, flavin binding in particular is clearly different. Local disorder at the isoalloxazine binding site prevents modeling of the complete FAD cofactor and two protein loops of the binding site. Only the ADP moiety shows well-defined electron density, indicating an "anchor" function for this part of the molecule. This notion is corroborated by competition experiments where ADP was used to displace FAD from the variant enzyme. Despite the fact that the affinity of FAD binding in the variant is reduced, the catalytic properties are very similar to the wild-type, and the redox potential of the bound flavin is the same for both proteins. The rate of electron transfer toward the flavin during turnover is reduced to one-third compared to the wild-type, but k(cat) remains unchanged. Redox-triggered FTIR difference spectroscopy of free FAD shows the nu(C(10a)=N(1)) band at 1548 cm(-)(1). In POX-V265A, this band is found at 1538 cm(-)(1) and thus shifted less strongly than in wild-type POX where it is found at 1534 cm(-)(1). Taking these observations together, the conservative exchange V265A in POX has a surprisingly small effect on the catalytic properties of the enzyme, whereas the effect on the three-dimensional structure is rather big.     

Changes in secondary structure and salt links of cytochrome P-450cam induced by photoreduction: a Fourier transform infrared spectroscopic study

Tris(2,2'-bipyridyl)ruthenium(II) was used as a light-induced artificial electron donor for the transfer of the first electron to cytochrome P-450(cam) bound with (1R)-camphor and camphane substrates, and in the substrate-free form. Fourier transform infrared spectroscopy was used to detect changes of the amide I' band and the CO ligand stretch vibration of heme-bound carbon monoxide associated with the heme redox transition. The reduced-minus-oxidized difference spectra show that not only the heme group but also the protein backbone and individual amino acid side chains were affected by the redox transition. Observed secondary structure changes were almost identical for (1R)-camphor-bound and camphane-bound cytochrome P-450(cam), with a remarkable negative signal at 1724.3 cm(-)(1) and a positive signal at 1716.0 cm(-)(1). These signals were not observed in substrate-free P-450(cam). On the basis of known crystallographic data, we assign these signals to a change of hydrogen bonds of a salt link between Arg112, His355, and the heme 6-propionic group.     

Nuclear wavepacket motion between P and P(+)B(A)(-) potential surfaces with subsequent electron transfer to H(A) in bacterial reaction centers. 1. Room temperature

Formation and coherent propagation of nuclear wavepackets on potential energy surfaces of the excited state of the primary electron donor P and of the charge transfer states P(+)B(A)(-) and P(+)H(A)(-) were studied in native and pheophytin-modified Rhodobacter sphaeroides R-26 reaction centers (RCs) induced by 25 fs excitation (where B(A) and H(A) are the primary and secondary electron acceptors, respectively). The processes were monitored by measuring coherent oscillations in kinetics of the time evolution of the stimulated emission band of P at 935 nm, of the absorption band of B(A)(-) at 1020 nm, and of the bleaching band of H(A) at 760 nm. It was found that the nuclear wavepacket motion on the 130-140 cm(-1) surface of P is directly induced by light absorption in P. When the wavepacket approaches the intersection between P and P(+)B(A)(-) surfaces at 120 and 380 fs delays, the formation of intermediate mixed-state emitting light at 935 nm (P) and absorbing light at 1020 nm (P(+)B(A)(-)) takes place. At the latter time, the wavepacket is transferred to the 32 cm(-1) mode which can belong to the P hypersurface effectively transferring the wavepacket to the P(+)B(A)(-) surface or can represent a diabatic surface which is formed by the states P and P(+)B(A)(-). The wavepacket motion on the P(+)B(A)(-) surface or on the P(+)B(A)(-) part of the mixing surface is accompanied by irreversible electron transfer to H(A). This process is monitored by the kinetics of 1020 nm band development and 760 nm band bleaching (delayed with respect to 1020 nm band development) which both have the enhanced 32 cm(-1) mode in Fourier transform (FT) spectra. The mechanism of wavepacket transfer from the 130-140 cm(-1) to the 32 cm(-1) mode is discussed.     

Histidine is involved in coupling proton uptake to electron transfer in photosynthetic proteins

In photosynthesis, the central step in transforming light energy into chemical energy is the coupling of light-induced electron transfer to proton uptake and release. Despite intense investigations of different photosynthetic protein complexes, including the photosystem II (PS II) in plants and the reaction center (RC) in bacteria, the molecular details of this fundamental process remain incompletely understood. In the RC of Rhodobacter (Rb.) sphaeroides, fast formation of the charge separated state, P(+)Q(A)(-), is followed by a slower electron transfer from the primary acceptor, Q(A), to the secondary acceptor, Q(B), and the uptake of a proton from the cytoplasm. The proton transfer to Q(B) takes place via a protonated water chain. Mutation of the amino acid AspL210 to Asn (L210DN mutant) near the entry of the proton pathway can disturb this water chain and consequently slow down proton uptake. Time-resolved step-scan Fourier transform infrared (FTIR) measurements revealed an intermediate X in the Q(A)(-)Q(B) to Q(A)Q(B)(-) transition. The nature of this transition remains a matter of debate. In this study, we investigated the role of the iron-histidine complex located between Q(A) and Q(B). We used time-resolved fast-scan FTIR spectroscopy to characterize the Rb. sphaeroides L210DN RC mutant marked with isotopically labeled histidine. FTIR marker bands of the intermediate X between 1120 cm(-1) and 1050 cm(-1) are assigned to histidine vibrations and indicate the protonation of a histidine, most likely HisL190, during the disappearance of the intermediate. Based on these results we propose a novel mechanism of the coupling of electron and proton transfer in photosynthesis.     

Characterization of the bonding interactions of Q(B) upon photoreduction via A-branch or B-branch electron transfer in mutant reaction centers from Rhodobacter sphaeroides

In Rhodobacter sphaeroides reaction centers (RCs) containing the mutation Ala M260 to Trp (AM260W), transmembrane electron transfer along the full-length of the A-branch of cofactors is prevented by the loss of the Q(A) ubiquinone, but it is possible to generate the radical pair P(+)H(A)(-) by A-branch electron transfer or the radical pair P(+)Q(B)(-) by B-branch electron transfer. In the present study, FTIR spectroscopy was used to provide direct evidence for the complete absence of the Q(A) ubiquinone in mutant RCs with the AM260W mutation. Light-induced FTIR difference spectroscopy of isolated RCs was also used to probe the neutral Q(B) and the semiquinone Q(B)(-) states in two B-branch active mutants, a double AM260W-LM214H mutant, denoted WH, and a quadruple mutant, denoted WAAH, in which the AM260W, LM214H, and EL212A-DL213A mutations were combined. The data were compared to those obtained with wild-type (Wt) RCs and the double EL212A-DL213A (denoted AA) mutant which exhibit the usual A-branch electron transfer to Q(B). The Q(B)(-)/Q(B) spectrum of the WH mutant is very close to that of Wt RCs indicating similar bonding interactions of Q(B) and Q(B)(-) with the protein in both RCs. The Q(B)(-)/Q(B) spectra of the AA and WAAH mutants are also closely related to one another, but are very different to that of the Wt complex. Isotope-edited IR fingerprint spectra were obtained for the AA and WAAH mutants reconstituted with site-specific (13)C-labeled ubiquinone. Whilst perturbations of the interactions of the semiquinone Q(B)(-) with the protein are observed in the AA and WAAH mutants, the FTIR data show that the bonding interaction of neutral Q(B) in these two mutants are essentially the same as those for Wt RCs. Therefore, it is concluded that Q(B) occupies the same binding position proximal to the non-heme iron prior to reduction by either A-branch or B-branch electron transfer.     

Low-temperature interquinone electron transfer in photosynthetic reaction centers from Rhodobacter sphaeroides and Blastochloris viridis: characterization of Q(B)- states by high-frequency electron paramagnetic resonance (EPR) and electron-nuclear double resonance (ENDOR)

High-frequency electron paramagnetic resonance (HF EPR) techniques have been employed to look for localized light-induced conformational changes in the protein environments around the reduced secondary quinone acceptor (Q(B)(-)) in Rhodobacter sphaeroides and Blastochloris viridis RCs. The Q(A)(-) and Q(B)(-) radical species in Fe-removed/Zn-replaced protonated RCs substituted with deuterated quinones are distinguishable with pulsed D-band (130 GHz) EPR and provide native probes of both the low-temperature Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron-transfer event and the structure of trapped conformational substates. We report here the first spectroscopic evidence that cryogenically trapped, light-induced changes enable low-temperature Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron transfer in the B. viridis RC and the first observation of an inactive, trapped P(+)Q(B)(-) state in both R. sphaeroides and B. viridis RCs that does not recombine at 20 K. The high resolution and orientational selectivity of HF electron-nuclear double resonance (ENDOR) allows us to directly probe protein environments around Q(B)(-) for distinct P(+)Q(B)(-) kinetic RC states by spectrally selecting specific nuclei in isotopically labeled samples. No structural differences in the protein structure near Q(B)(-) or reorientation (within 5 degrees ) of Q(B)(-) was observed with HF ENDOR spectra of two states of P(+)Q(B)(-): "active" and "inactive" states with regards to low-temperature electron transfer. These results reveal a remarkably enforced local protein environment for Q(B) in its reduced semiquinone state and suggest that the conformational change that controls reactivity resides beyond the Q(B) local environment.     

Vibrational modes of ubiquinone in cytochrome bo(3) from Escherichia coli identified by Fourier transform infrared difference spectroscopy and specific (13)C labeling.

In this study we present the infrared spectroscopic characterization of the bound ubiquinone in cytochrome bo(3) from Escherichia coli. Electrochemically induced Fourier transform infrared (FTIR) difference spectra of DeltaUbiA (an oxidase devoid of bound ubiquinone) and DeltaUbiA reconstituted with ubiquinone 2 and with isotopically labeled ubiquinone 2, where (13)C was introduced either at the 1- or at the 4-position of the ring (C=O groups), have been obtained. The vibrational modes of the quinone bound to the discussed high-affinity binding site (Q(H)) are compared to those from the synthetic quinones in solution, leading to the assignment of the C=O modes to a split signal at 1658/1668 cm(-)(1), with both carbonyls similarly contributing. The FTIR spectra of DeltaUbiA reconstituted with the labeled quinones indicate an essentially symmetrical and weak hydrogen bonding of the two C=O groups from the neutral quinone with the protein and distinct conformations of the 2- and 3-methoxy groups. Perturbations of the vibrational modes of the 5-methyl side groups are discussed for a signal at 1452 cm(-)(1). Only negligible shifts of the aromatic ring modes can be reported for the reduced and the protonated form of the quinone. Alterations of the protein upon quinone binding are reflected in the electrochemically induced FTIR difference spectra. In particular, difference signals at 1640-1633 cm(-)(1) and 1700-1670 cm(-)(1) indicate variations of beta-sheet secondary structure elements and loops, bands at 1706 and 1678 cm(-)(1) are tentatively attributed to individual amino acids, and a difference signal a 1540 cm(-)(1) is discussed to reflect an influence on C=C modes of the porphyrin ring or on deprotonated propionate groups of the hemes. Further tentative assignments are presented and discussed. The (13)C labeling experiments allow the assignment of the vibrational modes of a bound ubiquinone 8 in the electrochemically induced FTIR difference spectra of wild-type bo(3).     

Towards developing a protein infrared spectra databank (PISD) for proteomics research

Fourier transform infrared (FTIR) spectroscopy is an attractive tool for proteomics research as it can be used to rapidly characterize protein secondary structure in aqueous solution. Recently, a number of secondary structure prediction methods based on reference sets of FTIR spectra from proteins with known structure from X-ray crystallography have been suggested. These prediction methods, often referred to as pattern recognition based approaches, demonstrated good prediction accuracy using some error measure, e.g., the standard error of prediction (SEP). However, to avoid possible adverse effects from differences in recording, the analysis has been mostly based on reference sets of FTIR spectra from proteins recorded in one laboratory only. As a result, these studies were based on reference sets of FTIR spectra from a limited number of proteins. Pattern recognition based approaches, however, rely on reference sets of FTIR spectra from as many proteins as possible representing all possible band shape variation to be related to the diversity of protein structural classes. Hence, if we want to build reliable pattern recognition based systems to support proteomics research, which are capable of making good predictions from spectral data of any unknown protein, one common goal should be to build a comprehensive protein infrared spectra databank (PISD) containing FTIR spectra of proteins of known structure. We have started the process of developing a comprehensive PISD composed of spectra recorded in different laboratories. As part of this work, here we investigate possible effects on prediction accuracy achieved by a neural network analysis when using reference sets composed of FTIR spectra from different laboratories. Surprisingly low magnitude of difference in SEPs throughout all our experiments suggests that FTIR spectra recorded in different laboratories may be safely combined into one reference set with only minor deterioration of prediction accuracy in the worst case.     

Transducin-dependent protonation of glutamic acid 134 in rhodopsin

A highly conserved carboxylic acid residue in rhodopsin, Glu(134), modulates transducin (G(t)) interaction. It has been postulated that Glu(134) becomes protonated upon receptor activation. We studied the interaction between rhodopsin and G(t) using Fourier transform infrared (FTIR) difference spectroscopy combined with attenuated total reflection (ATR). Formation of the complex between G(t) and photoactivated rhodopsin reconstituted into phosphatidylcholine vesicles caused prominent infrared absorption increases at 1641, 1550, and 1517 cm(-)(1). The rhodopsin mutant E134Q was also studied. When measured in the presence of G(t), replacement of Glu(134) by glutamine abolished the low-frequency part of a broad absorption band at 1735 cm(-)(1) that is normally superimposed on the light-induced absorption changes of Asp(83) and Glu(122) of rhodopsin. In addition, a negative absorption band at 1400 cm(-)(1) that is evoked by interaction of native metarhodopsin II (MII) with G(t) was not observed in the difference spectrum of the E134Q mutant. Thus, Glu(134) is ionized in the dark and exhibits a symmetrical COO(-) stretching vibration at 1400 cm(-)(1). Glu(134) becomes protonated in the G(t)-MII complex and displays a C=O stretching mode near 1730 cm(-)(1). The E134Q mutation also affects absorption changes attributable to lipids, suggesting that the protonation of Glu(134) is linked to transfer of the carboxylic acid side chain from a polar to a nonpolar environment by becoming exposed to the lipid phase when G(t) binds. These results show directly that Glu(134) becomes protonated in MII upon G(t) binding and suggest that changes in receptor conformation affect lipid-protein interactions.     

Blue-light-induced changes in Arabidopsis cryptochrome 1 probed by FTIR difference spectroscopy

Cryptochromes are blue-light photoreceptors that regulate a variety of responses in animals and plants, including circadian entrainment in Drosophila and photomorphogenesis in Arabidopsis. They comprise a photolyase homology region (PHR) of about 500 amino acids and a C-terminal extension of varying length. In the PHR domain, flavin adenine dinucleotide (FAD) is noncovalently bound. The presence of a second chromophore, such as methenyltetrahydrofolate, in animal and plant cryptochromes is still under debate. Arabidopsis cryptochrome 1 (CRY1) has been intensively studied with regard to function and interaction of the protein in vivo and in vitro. However, little is known about the pathway from light absorption to signal transduction on the molecular level. We investigated the full-length CRY1 protein by Fourier transform infrared (FTIR) and UV/vis difference spectroscopy. Starting from the fully oxidized state of the chromophore FAD, a neutral flavoprotein radical is formed upon illumination in the absence of any exogenous electron donor. A preliminary assignment of the chromophore bands is presented. The FTIR difference spectrum reveals only moderate changes in secondary structure of the apoprotein in response to the photoreduction of the chromophore. Deprotonation of an aspartic or glutamic acid, probably D396, accompanies radical formation, as is deduced from the negative band at 1734 cm(-)(1) in D(2)O. The main positive band at 1524 cm(-)(1) in the FTIR spectrum shows a strong shift to lower frequencies as compared to other flavoproteins. Together with the unusual blue-shift of the absorption in the visible range to 595 nm, this clearly distinguishes the radical form of CRY1 from those of structurally highly homologous DNA photolyases. As a consequence, the direct comparison of cryptochrome to photolyase in terms of photoreactivity and mechanism has to be made with caution.     

Fourier-transform infrared study of the photoactivation process of Xenopus (6-4) photolyase

Photolyases (PHRs) are blue light-activated DNA repair enzymes that maintain genetic integrity by reverting UV-induced photoproducts into normal bases. The flavin adenine dinucleotide (FAD) chromophore of PHRs has four different redox states: oxidized (FAD(ox)), anion radical (FAD(?-)), neutral radical (FADH(?)), and fully reduced (FADH(-)). We combined difference Fourier-transform infrared (FTIR) spectroscopy with UV-visible spectroscopy to study the detailed photoactivation process of Xenopus (6-4) PHR. Two photons produce the enzymatically active, fully reduced PHR from oxidized FAD: FAD(ox) is converted to semiquinone via light-induced one-electron and one-proton transfers and then to FADH(-) by light-induced one-electron transfer. We successfully trapped FAD(?-) at 200 K, where electron transfer occurs but proton transfer does not. UV-visible spectroscopy following 450 nm illumination of FAD(ox) at 277 K defined the FADH(?)/FADH(-) mixture and allowed calculation of difference FTIR spectra among the four redox states. The absence of a characteristic C=O stretching vibration indicated that the proton donor is not a protonated carboxylic acid. Structural changes in Trp and Tyr are suggested by UV-visible and FTIR analysis of FAD(?-) at 200 K. Spectral analysis of amide I vibrations revealed structural perturbation of the protein's β-sheet during initial electron transfer (FAD(?-) formation), a transient increase in α-helicity during proton transfer (FADH(?) formation), and reversion to the initial amide I signal following subsequent electron transfer (FADH(-) formation). Consequently, in (6-4) PHR, unlike cryptochrome-DASH, formation of enzymatically active FADH(-) did not perturb α-helicity. Protein structural changes in the photoactivation of (6-4) PHR are discussed on the basis of these FTIR observations.     

Rapid-scan Fourier transform infrared spectroscopy shows coupling of GLu-L212 protonation and electron transfer to Q(B) in Rhodobacter sphaeroides reaction centers

Rapid-scan Fourier transform infrared (FTIR) difference spectroscopy was used to investigate the electron transfer reaction Q(A-)Q(B)-->Q(A)Q(B-) (k(AB)(1)) in mutant reaction centers of Rhodobacter sphaeroides, where Asp-L210 and/or Asp-M17 have been replaced with Asn. Mutation of both residues decreases drastically k(AB)(1)), attributed to slow proton transfer to Glu-L212, which becomes rate limiting for electron transfer to Q(B) [M.L. Paddock et al., Biochemistry 40 (2001) 6893]. In the double mutant, the FTIR difference spectrum recorded during the time window 4-29 ms following a flash showed peaks at 1670 (-), 1601 (-) and 1467 (+) cm(-1), characteristic of Q(A) reduction. The time evolution of the spectra shows reoxidation of Q(A-) and concomitant reduction of Q(B) with a kinetics of about 40 ms. In native reaction centers and in both single mutants, formation of Q(B-) occurs much faster than in the double mutant. Within the time resolution of the technique, protonation of Glu-L212, as characterized by an absorption increase at 1728 cm(-1) [E. Nabedryk et al., Biochemistry 34 (1995) 14722], was found to proceed with the same kinetics as reduction of Q(B) in all samples. These rapid-scan FTIR results support the model of proton uptake being rate limiting for the first electron transfer from Q(A-) to Q(B) and the identification of Glu-L212 as the main proton acceptor in the state Q(A)Q(B-).     

Water structural changes involved in the activation process of photoactive yellow protein

Fourier transform infrared (FTIR) spectroscopy was applied to the blue-light photoreceptor photoactive yellow protein (PYP) to investigate water structural changes possibly involved in the photocycle of PYP. Photointermediates were stabilized at low temperature, and difference IR spectra were obtained between intermediate states and the original state of PYP (pG). Water structural changes were never observed in the >3570 cm(-)(1) region for the intermediates stabilized at 77-250 K, such as the red-shifted pR and blue-shifted pB intermediates. In contrast, a negative band was observed at 3658 cm(-)(1) in the pB minus pG spectrum at 295 K, which shifts to 3648 cm(-)(1) upon hydration with H(2)(18)O. The high frequency of the O-H stretch of water indicates that the water O-H group does not form hydrogen bonds in pG, and newly forms these upon pB formation at 295 K, but not at 250 K. Among 92 water molecules in the crystal structure of PYP, only 1 water molecule, water-200, is present in a hydrophobic core inside the protein. The amide N-H of Gly-7 and the imidazole nitrogen atom of His-108 are its possible hydrogen-bonding partners, indicating that one O-H group of water-200 is free to form an additional hydrogen bond. The water band at 3658 cm(-)(1) was indeed diminished in the H108F protein, which strongly suggests that the water band originates from water-200. Structural changes of amide bands in pB were much greater in the wild-type protein at 295 K than at 250 K or in the H108F protein at 295 K. The position of water-200 is >15 A remote from the chromophore. Virtually no structural changes were reported for regions larger than a few angstroms away from the chromophore, in the time-resolved X-ray crystallography experiments on pB. On the basis of the present results, as well as other spectroscopic observations, we conclude that water-200 (buried in a hydrophobic core in pG) is exposed to the aqueous phase upon formation of pB in solution. In neither crystalline PYP nor at low temperature is this structural transition observed, presumably because of the restrictions on global structural changes in the protein under these conditions.     

Structural intermediate in the photocycle of a BLUF (sensor of blue light using FAD) protein Slr1694 in a Cyanobacterium Synechocystis sp. PCC6803

Slr1694 in Synechocystis sp. PCC6803 is a family of blue-light photoreceptors based on flavin adenine dinucleotide (FAD) called BLUF (sensor of blue light using FAD) proteins, which include AppA from Rhodobacter sphaeroides and PAC from Euglena gracilis. Illumination of dark-state Slr1694 at 15 degrees C reversibly induced a signaling light state characterized by the red shift in the UV-visible spectrum and by the light-induced Fourier transform infrared (FTIR) difference spectrum for structural changes of a bound flavin and apo protein. Illumination at the medium-low temperature (-35 degrees C) led to the red shift in the UV-visible spectrum despite some small difference in the light-induced changes. In contrast, the -35 degrees C illumination resulted in a completely different light-induced FTIR spectrum, in which almost all of the bands were suppressed with the exception of the bands for the change of C4=O bonding of the FAD isoalloxazine ring. The C4=O bands were induced at -35 degrees C with almost the same intensity, but the band frequency for the light state was upshifted by 6 cm(-)(1). The changes in frequency of the light-state C4=O band and in amplitude of other bands showed the same temperature dependence with a half-change temperature at approximately -20 degrees C. It was indicated that the light-induced structural changes of apo protein and FAD were inhibited at low temperature with the exception of the change in hydrogen bonding to the C4=O group. The light-induced formation of the FTIR bands was similarly inhibited by sample dehydration. We discussed the possibility that this constrained light state is a trapped intermediate state in the photocycle of Slr1694.     

Assembly of electroactive layer-by-layer films of hemoglobin and polycationic poly(diallyldimethylammonium)

Layer-by-layer (PDDA/Hb)(n) films were assembled by alternate adsorption of positively charged poly(diallyldimethylammonium) (PDDA) and negatively charged hemoglobin (Hb) at pH 9.2 from their aqueous solutions on pyrolytic graphite electrodes and other substrates. The assembly process was monitored and confirmed by quartz crystal microbalance (QCM), UV-vis spectroscopy, and cyclic voltammetry (CV). CVs of (PDDA/Hb)(n) films showed a pair of well-defined, nearly reversible peaks at about -0.34 V vs SCE at pH 7.0, characteristic of Hb heme Fe(III)/Fe(II) redox couple. Positions of Soret absorption band and infrared amide II band of Hb in (PDDA/Hb)(8) films suggest that Hb in the films keeps its secondary structure similar to its native state. The electrochemical parameters of (PDDA/Hb)(8) films were estimated by square wave voltammetry, and the thickness of the PDDA/Hb bilayer was estimated by QCM and scanning electron microscopy. Trichloroacetic acid and nitrite (NO(2)(-)) were catalytically reduced at (PDDA/Hb)(8) film electrodes. The electrochemical catalytic reactions of O(2) and H(2)O(2) on (PDDA/Hb)(8) films were also studied.     

Application of multivariate curve resolution-alternating least squares (MCR-ALS) for secondary structure resolving of proteins

Fourier transform infrared (FTIR) spectroscopy is the most common spectroscopic technique used for study of protein structure. Initially, band deconvolution techniques were applied to determine the secondary structure of proteins. Recently, several multivariate regression methods have been used to predict the secondary structure of proteins as an alternative to the previous methods. Multivariate curve resolution-alternating least squares (MCR-ALS) was applied on the FTIR spectra of proteins to resolve the fraction and spectral profiles of different structural motifs. Initial estimates of spectral profiles of different protein motifs were built using orthogonal projection approach (OPA). Predicted fractions of α-helix and β-sheet obtained by MCR-ALS technique were compared with those from partial least squares (PLS) modeling which revealed superiority of the former. If we consider the possibility of pure spectra prediction in addition to the prediction of secondary structure from the data set, MCR-ALS can be proposed as a very valuable alternative for qualitative and quantitative study of protein structures.     

Residual water modulates QA- -to-QB electron transfer in bacterial reaction centers embedded in trehalose amorphous matrices

The role of protein dynamics in the electron transfer from the reduced primary quinone, Q(A)(-), to the secondary quinone, Q(B), was studied at room temperature in isolated reaction centers (RC) from the photosynthetic bacterium Rhodobacter sphaeroides by incorporating the protein in trehalose water systems of different trehalose/water ratios. The effects of dehydration on the reaction kinetics were examined by analyzing charge recombination after different regimes of RC photoexcitation (single laser pulse, double flash, and continuous light) as well as by monitoring flash-induced electrochromic effects in the near infrared spectral region. Independent approaches show that dehydration of RC-containing matrices causes reversible, inhomogeneous inhibition of Q(A)(-)-to-Q(B) electron transfer, involving two subpopulations of RCs. In one of these populations (i.e., active), the electron transfer to Q(B) is slowed but still successfully competing with P(+)Q(A)(-) recombination, even in the driest samples; in the other (i.e., inactive), electron transfer to Q(B) after a laser pulse is hindered, inasmuch as only recombination of the P(+)Q(A)(-) state is observed. Small residual water variations ( approximately 7 wt %) modulate fully the relative fraction of the two populations, with the active one decreasing to zero in the driest samples. Analysis of charge recombination after continuous illumination indicates that, in the inactive subpopulation, the conformational changes that rate-limit electron transfer can be slowed by >4 orders of magnitude. The reported effects are consistent with conformational gating of the reaction and demonstrate that the conformational dynamics controlling electron transfer to Q(B) is strongly enslaved to the structure and dynamics of the surrounding medium. Comparing the effects of dehydration on P(+)Q(A)(-)-->PQ(A) recombination and Q(A)(-)Q(B)-->Q(A)Q(B)(-) electron transfer suggests that conformational changes gating the latter process are distinct from those stabilizing the primary charge-separated state.