Static and time-resolved step-scan Fourier transform infrared investigations of the photoreaction of halorhodopsin from Natronobacterium pharaonis: consequences for models of the anion translocation mechanism.

The molecular changes during the photoreaction of halorhodopsin from Natronobacterium pharaonis have been monitored by low-temperature static and by time-resolved step-scan Fourier transform infrared difference spectroscopy. In the low-temperature L spectrum anions only influence a band around 1650 cm(-1), tentatively assigned to the C=N stretch of the protonated Schiff base of L. The analysis of the time-resolved spectra allows to identify the four states: K, L(1), L(2), and O. Between L(1) and L(2), only the apoprotein undergoes alterations. The O state is characterized by an all-trans chromophore and by rather large amide I spectral changes. Because in our analysis the intermediate containing O is in equilibrium with a state indistinguishable from L(2), we are unable to identify an N-like state. At very high chloride concentrations (>5 M), we observe a branching of the photocycle from L(2) directly back to the dark state, and we provide evidence for direct back-isomerization from L(2). This branching leads to the reported reduction of transport activity at such high chloride concentrations. We interpret the L(1) to L(2) transition as an accessibility change of the anion from the extracellular to the cytosolic side, and the large amide I bands in O as an indication for opening of the cytosolic channel from the Schiff base toward the cytosolic surface and/or as indication for changes of the binding constant of the release site.     

Occupancy of two primary chloride-binding sites in Natronobacterium pharaonis halorhodopsin is a necessary condition for active anion transport

The existence of two primary chloride-binding sites was found on the basis of the study of halorhodopsin spectra at different chloride concentrations. SVD analysis of the spectra revealed two chloride-dependent components at low chloride concentration (0.1-10 mM). Global fitting of SVD components found K _D values of 0.47 mM and 5.2 mM with unitity Hill coefficients. The second K _D coincides with the apparent K _D of the photovoltage response of halorhodopsin.     

FTIR spectroscopy of the O photointermediate in pharaonis phoborhodopsin

pharaonis phoborhodopsin (ppR; also called pharaonis sensory rhodopsin II, psR-II) is a photoreceptor protein for negative phototaxis in Natronobacterium pharaonis. During the photocycle of ppR, the retinal chromophore is thermally isomerized from the 13-cis to all-trans form. We employed FTIR spectroscopy of ppR at 260 K and pH 5 to reveal that this isomerization occurs upon formation of the O intermediate (ppR(O)) by using ppR samples reconstituted with 12,14-D(2)-labeled retinal. In ppR(O), C=O stretching vibrations of protonated carboxylates newly appear at 1757 (+)/1722 (-) cm(-1) in H(2)O and at 1747 (+)/1718 (-) cm(-1) in D(2)O in addition to the 1765 (+) cm(-1) band of Asp75. Amide I vibrations are basically similar between ppR(M) and ppR(O), whereas unique bands of ppR(O) are also observed such as the negative 1656 cm(-1) band in D(2)O and intense bands at 1686 (-)/1674 (+) cm(-1). In addition, O-D stretching vibrations of water molecules in the entire mid-infrared region are assigned for ppR(M) and ppR(O), the latter being unique for ppR, since it can be detected at low temperature (260 K). The ppR(M) minus ppR difference spectra lack the lowest frequency water band (2215 cm(-1)) observed in the ppR(K) minus ppR spectra, which is probably associated with water that interacts with the negative charges in the Schiff base region. It is likely that the proton transfer from the Schiff base to Asp75 in ppR(M) can be explained by a hydration switch of a water from Asp75 to Asp201, as was proposed for the light-driven proton-pump bacteriorhodopsin (hydration switch model) [Tanimoto, T., Furutani, Y., and Kandori, H. (2003) Biochemistry 42, 2300-2306]. In the transition from ppR(M) to ppR(O), a hydrogen-bonding alteration takes place for another water molecule that forms a strong hydrogen bond.     

FTIR spectroscopy of the M photointermediate in pharaonis rhoborhodopsin

pharaonis phoborhodopsin (ppR; also called pharaonis sensory rhodopsin II, psR-II) is a photoreceptor for negative phototaxis in Natronobacterium pharaonis. During the photocycle of ppR, the Schiff base of the retinal chromophore is deprotonated upon formation of the M intermediate (ppR(M)). The present FTIR spectroscopy of ppR(M) revealed that the Schiff base proton is transferred to Asp-75, which corresponds to Asp-85 in a light-driven proton-pump bacteriorhodopsin (BR). In addition, the C==O stretching vibrations of Asn-105 were assigned for ppR and ppR(M). The common hydrogen-bonding alterations in Asn-105 of ppR and Asp-115 of BR were found in the process from photoisomerization (K intermediate) to the primary proton transfer (M intermediate). These results implicate similar protein structural changes between ppR and BR. However, BR(M) decays to BR(N) accompanying a proton transfer from Asp-96 to the Schiff base and largely changed protein structure. In the D96N mutant protein of BR that lacks a proton donor to the Schiff base, the N-like protein structure was observed with the deprotonated Schiff base (called M(N)) at alkaline pH. In ppR, such an N-like (M(N)-like) structure was not observed at alkaline pH, suggesting that the protein structure of the M state activates its transducer protein.     

Anion binding to the chloride pump, halorhodopsin, and its implications for the transport mechanism.

The light-driven chloride pump, halorhodopsin, binds and transports chloride across the membrane, and to a lesser extent nitrate. Binding and transport kinetics, and resonance Raman spectra of the retinal Schiff base, with these anions suggest the existence of two mutually exclusive binding sites. One of these may be the uptake site, and the other the release site during the transport. Plausible locations can be suggested for these sites, because halorhodopsin is a small protein with few buried positively charged residues, and the primary structure of a second pigment with similar function has recently become available for comparison.     

Stopped-flow analysis on anion binding to blue-form halorhodopsin from Natronobacterium pharaonis: comparison with the anion-uptake process during the photocycle

Pharaonis halorhodopsin (phR), the light-driven chloride ion pump from Natronobacterium pharaonis with C-terminal histidine tag, was expressed in Escherichia coli cells. The protein was solubilized with 0.1% n-dodecyl beta-D-maltopyranoside and purified with a nickel column. Removal of Cl- from the medium yields blue phR (phR(blue)) that has lost Cl- near the chromophore. Addition of Cl- converts phR(blue) to a red-shifted Cl--bound form (phR(Cl)). Circular dichroic spectra of phR(blue) and phR(Cl) exhibited a bilobe in the visual region, indicating specific oligomerization of the phR monomers. The order of anion concentration which induced a shift from phR(blue) to phR(X) was Br- < Cl- < NO3- < N3-, which was the same as in the case of phR purified from N. pharaonis membranes. Chloride binding kinetics was measured by time-resolved absorption changes with stopped-flow rapid mixing. Rates of Cl- binding consisted of fast and slow components, and the amplitude of the fast component was about 90% of the total changes. The rate constant of the fast component at 100 mM NaCl at 25 degrees C was 260 s(-1) with an apparent activation energy of 35 kJ/mol. These values are in good agreement with the process of Cl- uptake in the photocycle (O --> hR' reaction) reported previously [Váró et al. (1995) Biochemistry 34, 14500-14507]. In addition, the Cl- concentration dependence on both rates was similar to each other. These observations suggest that the O-intermediate is similar to phR(blue) and that Cl- uptake during the photocycle may be ruled by a passive process.     

On the mechanism of anion uptake by plant roots

Summary The effect of the valence of the associated cation on Cl^–-uptake by excised barley roots grown in CaSO₄ has been studied at 26°, 6° and 2°C. The uptake of Cl^– relative to that of the associated cation was found to increase in the order: trivalent > divalent > monovalent. This was explained on the expected effect of the cation on the negative charge and potential of root surfaces. A lyotropic order was observed in case of monovalent cations, whereas divalent cations showed no such order. The order observed in Cl^–-uptake from chloride solutions of monovalent cations is associated with the ability of the absorbed cation to remove Ca and Mg from the roots. Li⁺ behaved similar to divalent cations in affecting the relative Cl^–-uptake from LiCl.As to the effect of temperature on the uptake of Cl^– and associated cation, it appears that Cl^– is not taken up to any great extent at 2°C whereas cations are still adsorbed at this low temperature. This has been explained on the assumption of the presence of negative adsorption spots on the root surface which can hold cations but not anions. It appears that Cl^–-uptake by roots requires the expenditure of energy to overcome repulsion arising from the negative surface.This work is supported by AEC contract AT (11-1) — 34 project 55.     

Anion transport in rat brain mitochondria: Fumarate uptake via the dicarboxylate carrier

Penetration of fumarate into rat brain mitochondria has been investigated, as required in brain ammoniogenesis. Mitochondria swell in ammonium fumarate and this swelling is increased by both Pi and malate. According to a carrier mediated process, fumarate translocation, which occurs in exchange with intramitochondrial malate or Pi shows saturation characteristics. By photometrically investigating the kinetics of fumarate/malate, fumarate/ Pi and malate/Pi exchanges, different Km values were obtained (10, 22 and 250 M, respectively), whereas no significant difference was found forV _max values (40 nmol NAD(P)⁺ reduced/min×mg protein). This suggests that fumarate and malate share a single carrier to enter mitochondria, namely the dicarboxylate carrier. Both comparison made of theV _max values and inhibiton studies exclude a fumarate translocation via either the tricarboxylate carrier, whose occurrence in brain is here demonstrated, or oxodicarboxylate carrier. Kinetic investigation of the dicarboxylate translocator shows the existence of thiol group/s and metal ion/s at or near the substrate binding sites. The experimental findings are discussed in the light of fumarate uptake in vivo in brain ammoniogenesis.Abbreviations AD.SUCC adenylsuccinate - ASP aspartate - BTA 1,2,3,-benzenetricarboxylate - CITR citrate - D-NAD deamino-NAD - PUM fumarate - GABA -aminobutyrate - GAP glyceraldehyde-3-phosphate - GAP-DH glyceraldheyde-3-phosphate dehydrogenase - GHBA -hydroxybutyrate - HEPES 4-(2-hydroxyethyl)-1-piperazine ethanesulfonic acid - OAA oxaloacetate - OG oxoglutarate - PEP phosphoenolpyruvate - 3-PG glycerate-3-phosphate - 3-PGP glycerate-1,3-diphosphate - PYR pyruvate - RBM rat brain mitochondria - RHM rat heart mitochondria - RKM rat kidney mitochondria - RLM rat liver mitochondria - SSA succinic semialdehyde     

Specific arginine and threonine residues control anion binding and transport in the light-driven chloride pump halorhodopsin.

The light-driven chloride pump halorhodopsin (HR), a halobacterial retinal protein, was studied by comparing wild type with specific mutants. Changes of conserved arginine and threonine residues in the transmembrane regions could be classified in two categories: in the extracellular half of the molecule, mutations influence anion uptake and binding. R108 mutations abolish all anion effects previously attributed to two distinct binding sites and change the characteristic photochemistry. Neutral residues at position 108 completely inactivate the pump. T111 increases the affinity of this anion binding site without being essentially important. In the photochemical cycles of the mutants T111V and Q105E, a red-shifted absorbing intermediate is enriched indicating retarded anion uptake. On the cytoplasmic side, mutations do not change anion binding properties of the unphotolyzed protein, but slow down anion release thereby reducing the chloride transport activity and the photocycling rate. The lowest activity is found for T203V, while R200 mutations have weaker effects. Thus, in the symmetrically arranged pairs R108/T111 and T203/R200, threonine and arginine play different roles, reflecting high affinity anion uptake by the former and effective anion release catalyzed by the latter residues. A model for the anion transport mechanism in HR is suggested comprising the specific functions of channel-lining residues.     

Structural changes in the Schiff base region of squid rhodopsin upon photoisomerization studied by low-temperature FTIR spectroscopy

Low-temperature Fourier transform infrared (FTIR) spectroscopy is used to study squid rhodopsin at 77 K in investigating structural changes in the Schiff base region upon photoisomerization. The analysis of O-D stretching vibrations in D(2)O revealed that there are more internal water molecules near the retinal chromophore in squid rhodopsin than in bovine rhodopsin. Among nine O-D stretching vibrations of water in squid rhodopsin, eight peaks are identical between rhodopsin and 9-cis-rhodopsin (Iso). On the other hand, the isomer-specific O-D stretch of water was observed for rhodopsin (2451 cm(-)(1)) and Iso (2382 cm(-)(1)). Low frequencies of these bands suggest that the water forms a strong hydrogen bond with a negatively charged counterion. In addition, it was suggested that the hydrogen bond of the Schiff base is weaker in squid rhodopsin than in bacteriorhodopsin and bovine rhodopsin, and squid rhodopsin possessed similar hydrogen bonding strength for the Schiff base among rhodopsin, Iso, and bathorhodopsin. Most vibrational bands in the X-D stretch region originate from water O-D or the Schiff base N-D stretches, suggesting that the hydrogen bonding network in the Schiff base region of squid rhodopsin is composed of only water molecules. On the basis of these results, we propose that squid rhodopsin possesses a "bridge" water between the Schiff base and its counterion as well as squid retinochrome [Furutani, Y., Terakita, A., Shichida, Y., and Kandori, H. (2005) Biochemistry 44, 7988-7997], which is absent in vertebrate rhodopsin [Furutani, Y., Shichida, Y., and Kandori, H. (2003) Biochemistry 42, 9619-9625].     

Hydrogen-bonding changes of internal water molecules upon the actions of microbial rhodopsins studied by FTIR spectroscopy

Microbial rhodopsins are classified into type-I rhodopsins, which utilize light energy to perform wide varieties of function, such as proton pumping, ion pumping, light sensing, cation channels, and so on. The crystal structures of several type-I rhodopsins were solved and the molecular mechanisms have been investigated based on the atomic structures. However, the crystal structures of proteins of interest are not always available and the basic architectures are sometimes quite similar, which obscures how the proteins achieve different functions. Stimulus-induced difference FTIR spectroscopy is a powerful tool to detect minute structural changes providing a clue for elucidating the molecular mechanisms. In this review, the studies on type-I rhodopsins from fungi and marine bacteria, whose crystal structures have not been solved yet, were summarized. Neurospora rhodopsin and Leptosphaeria rhodopsin found from Fungi have sequence similarity. The former has no proton pumping function, while the latter has. Proteorhodopsin is another example, whose proton pumping machinery is altered at alkaline and acidic conditions. We described how the structural changes of protein were different and how water molecules were involved in them. We reviewed the results on dynamics of the internal water molecules in pharaonis halorhodopsin as well. This article is part of a Special Issue entitled: Retinal Proteins — You can teach an old dog new tricks.     

Structure of an active water molecule in the water-oxidizing complex of photosystem II as studied by FTIR spectroscopy

The vibrations of a water molecule in the water-oxidizing complex (WOC) of photosystem II were detected for the first time using Fourier transform infrared (FTIR) spectroscopy. In a flash-induced FTIR difference spectrum upon the S(1)-to-S(2) transition, a pair of positive and negative bands was observed at 3618 and 3585 cm(-1), respectively, and both bands exhibited downshifts by 12 cm(-1) upon replacement of H(2)(16)O by H(2)(18)O. Upon D(2)O substitution, the bands largely shifted down to 2681 and 2652 cm(-1). These observations indicate that the bands at 3618 and 3585 cm(-1) arise from the O-H stretching vibrations of a water molecule, probably substrate water, coupled to the Mn cluster in the S(2) and S(1) states, respectively. The band frequencies indicate that the O-H group forms a weak H-bond and this H-bonding becomes weaker upon S(2) formation. Intramolecular coupling with the other O-H vibration of this water molecule was studied by a decoupling experiment using a H(2)O/D(2)O (1:1) mixture. The downshifts by decoupling were estimated to be 4 and 12 cm(-1) for the 3618 (S(2)) and 3585 cm(-1) (S(1)) bands, both of which were much smaller than 52 cm(-1) of water in vapor, indicating that the observed water has a considerably asymmetric structure; i.e., one of the O-H groups is weakly and the other is strongly H-bonded. The smaller coupling in the S(2) than the S(1) state means that this H-bonding asymmetry becomes more prominent upon S(2) formation. Such a structural change may facilitate the proton release reaction that takes place in the later step by lowering the potential barrier. The present study showed that FTIR detection of the O-H vibrations is a useful and promising method to directly monitor the chemical reactions of substrate water and clarify the molecular mechanism of photosynthetic water oxidation.     

Chain-length dependence of alpha-helix to beta-sheet transition in polylysine: model of protein aggregation studied by temperature-tuned FTIR spectroscopy

The chain-length dependence of the alpha-helix to beta-sheet transition in poly(L-lysine) is studied by temperature-tuned FTIR spectroscopy. This study shows that heterogeneous samples of poly(L-lysine), comprising polypeptide chains with various lengths, undergo the alpha-beta transition at an intermediate temperature compared to homogeneous ingredients. This holds true as long as each individual fraction of the polypeptide is capable of adopting an antiparallel beta-sheet structure. The tendency is that the longer chain is, the lower the alpha-beta transition temperature is, which has been linked to the presence of distorted or solvated helices with turns or beta sheets in elongating chains of poly(L-lysine). As such helical structures are apparently conducive to the alpha-beta transition, this draws a comparison to the hypothesis of metastable protein conformational states being a common stage in amyloid-formation pathways. The antiparallel architecture of the beta sheet is likely to reflect the pretransition interhelical interactions in poly(L-lysine). Namely, the chains are arranged in an antiparallel manner because of energetically favored antiparallel pre-assembly of dipolar alpha helices.     

Effects of temperature and water content on the secondary structure of wheat gluten studied by FTIR spectroscopy

The effect of temperature on gluten conditioned at the following water contents, 0%, 13%, and 47% (wet weight basis), was studied by FTIR spectroscopy over the temperature range of 25-85 degrees C. A detailed discussion of the assignment of the amide I band is given. At 0% hydration no changes in the secondary structure with temperature could be detected; spectra were consistent with a tight disordered structure with many protein-protein interactions. At 13% hydration, distinctive changes occurred in the low-frequency region of the amide I band (1,630-1,613 cm(-1)). This was attributed to changes in the beta-sheet structure. On cooling to 25 degrees C, these changes were mainly reversed. It was noted that most of the changes observed occurred above the glass transition temperature. At 47% hydration, more complex changes took place: as the temperature was raised distinct bands at 1,630 and 1,613 cm(-1) merged. However, this process was partially reversed, with recovery of both bands, on cooling. The significance of these results in relation to other changes in gluten proteins in flour and dough with temperature and water content is discussed.     

Structure of the retinal chromophore in the hRL intermediate of halorhodopsin from resonance raman spectroscopy

Time-resolved resonance Raman spectra of the hRL intermediate of halorhodopsin have been obtained. The structurally sensitive fingerprint region of the hRL spectrum is very similar to that of bacteriorhodopsin's L550 intermediate, which is known to have a 13-cis configuration. This indicates that hRL contains a 13-cis chromophore and that an all-trans----13-cis isomerization occurs in the halorhodopsin photocycle. hRL exhibits a Schiff base stretching mode at 1644 cm-1, which shifts to 1620 cm-1 in D2O. This demonstrates that the Schiff base linkage to the protein is protonated. The insensitivity of the C-C stretching mode frequencies to N-deuteriation suggests that the Schiff base configuration is anti. The 24 cm-1 shift of the Schiff base mode in D2O indicates that the Schiff base proton in hRL has a stronger hydrogen-bonding interaction with the protein than does hR578.     

Light-induced structural changes in the LOV2 domain of Adiantum phytochrome3 studied by low-temperature FTIR and UV-visible spectroscopy

Phototropin (Phot) is a blue-light receptor in plants. The molecule has two FMN (flavin mononucleotide) binding domains named LOV (light-, oxygen-, and voltage-sensing), which is a subset of the PAS (Per-Arnt-Sim) superfamily. Illumination of the phot-LOV domains in the dark state (D447) produces a covalent C(4a) flavin-cysteinyl adduct (S390) via a triplet excited state (L660), which reverts to D447 in the dark. In this work, we studied the light-induced structural changes in the LOV2 domain of Adiantum phytochrome3 (phy3), which is a fusion protein of phot containing the phytochrome chromophoric domain, by low-temperature UV-visible and FTIR spectroscopy. UV-visible spectroscopy detected only one intermediate state, S390, in the temperature range from 77 to 295 K, indicating that the adduct is produced even at temperatures as low as 77 K, although a portion of D447 cannot be converted to S390 at low temperatures possibly because of motional freezing. In the whole temperature range, FTIR spectra in the S-H stretching frequency region showed that Cys966 of phy3-LOV2 is protonated in D447 and unprotonated on illumination, supporting adduct formation. The pK(a) of the S-H group in D447 is estimated to be >10. FTIR spectra also showed the light-induced appearance of a positive peak around 3621 cm(-1) in the whole temperature range, indicating that adduct formation accompanies rearrangement of a hydrogen bond of a water molecule(s), which can be either water25, water45, or both, near the chromophore. In contrast to the weak temperature dependence of the spectral changes in the UV-visible absorption and the FTIR of both S-H and O-H stretching bands, light-induced changes in the amide I vibration that probes protein backbone structure vary significantly with the increase in temperature. The spectral changes suggest that light excitation of FMN loosens the local structure around it, particularly in turns, in the early stages and that another change subsequently takes place to tighten it, mainly in beta-structure, but some occur in the alpha-helical structure of the protein moiety as well. Interestingly, these changes proceed without altering the shape of UV-visible spectra, suggesting the presence of multiple conformation states in S390.     

Water uptake and distribution in germinating lupine seeds studied by magnetic resonance imaging and NMR spectroscopy

Magnetic resonance imaging (MRI) was used to study temporal and spatial water uptake and distribution in germinating lupine ( Lupinus luteus L.) seeds. During 24 h of imbibition, water was unevenly distributed within the seed and some anatomical parts were more hydrated than others. Water entered the seed through the hilum and micropyle. The embryonic axis was the first to show hydration followed by seed coat and later cotyledons. The changes in water status were characterized by NMR spectroscopy. Analyses of T₂ relaxation times revealed a three-component water proton system (structural, intracellular and extracellular water) in germinating lupine seeds. The data on the components of transverse relaxation time studies indicated the complex exchange processes taking place between water components inside lupine seed over first 2.5 h of hydration, with a distinguished increase in structural water and decrease in other components. This speaks in favor of the high water-absorbing capacity of lupine seeds as related to high protein content. Germination was accompanied by swelling of protein bodies and changes in the organization of stored reserves with gradual disappearance of protein from the cells.     

Melting of individual lipid components in binary lipid mixtures studied by FTIR spectroscopy, DSC and Monte Carlo simulations

Monte Carlo (MC) simulations, Differential Scanning Calorimetry (DSC) and Fourier Transform InfraRed (FTIR) spectroscopy were used to study the melting behavior of individual lipid components in two-component membranes made of DMPC and DSPC. We employed Monte Carlo simulations based on parameters obtained from DSC profiles to simulate the melting of the different lipids as a function of temperature. The simulations show good agreement with the FTIR data recorded for deuterated and non-deuterated lipids, which demonstrates that the information on the differential melting of the individual components is already contained in the calorimetric profiles. In mixtures, both lipids melt over a wide temperature range. As expected, the lipid melting events of the lipid with the lower melting temperature occur on average at lower temperatures. The simulations also yield information on the lateral distribution of the lipids that is neither directly contained in the DSC nor in the FTIR data. In the phase coexistence region, liquid disordered domains are typically richer in the lower-melting-temperature lipid species.     

Pressure stability of the alpha-helix structure in a de novo designed protein (alpha-l-alpha)(2) studied by FTIR spectroscopy

The pressure-induced structural changes of a de novo designed four-helix bundle protein, (alpha-l-alpha)(2), in aqueous solution have been investigated by FTIR spectroscopy. Changes in the amide I' band intensity show that pressure induces disruption of tertiary interactions and stabilizes the solvated alpha-helical form. This may suggest that the exposure of the hydrophobic core to the solvent by pressure is not a sufficient condition for pressure-induced unfolding of the alpha-helices of proteins.