Conformational changes in bacteriorhodopsin studied by infrared attenuated total reflection

Rhodopsins: An Excitingly Versatile Protein Species for Research, Development and Creative Engineering

The first member and eponym of the rhodopsin family was identified in the 1930s as the visual pigment of the rod photoreceptor cell in the animal retina. It was found to be a membrane protein, owing its photosensitivity to the presence of a covalently bound chromophoric group. This group, derived from vitamin A, was appropriately dubbed retinal. In the 1970s a microbial counterpart of this species was discovered in an archaeon, being a membrane protein also harbouring retinal as a chromophore, and named bacteriorhodopsin. Since their discovery a photogenic panorama unfolded, where up to date new members and subspecies with a variety of light-driven functionality have been added to this family. The animal branch, meanwhile categorized as type-2 rhodopsins, turned out to form a large subclass in the superfamily of G protein-coupled receptors and are essential to multiple elements of light-dependent animal sensory physiology. The microbial branch, the type-1 rhodopsins, largely function as light-driven ion pumps or channels, but also contain sensory-active and enzyme-sustaining subspecies. In this review we will follow the development of this exciting membrane protein panorama in a representative number of highlights and will present a prospect of their extraordinary future potential.

Infrared Difference Spectroscopy of Proteins: From Bands to Bonds

Infrared difference spectroscopy probes vibrational changes of proteins upon their perturbation. Compared with other spectroscopic methods, it stands out by its sensitivity to the protonation state, H-bonding, and the conformation of different groups in proteins, including the peptide backbone, amino acid side chains, internal water molecules, or cofactors. In particular, the detection of protonation and H-bonding changes in a time-resolved manner, not easily obtained by other techniques, is one of the most successful applications of IR difference spectroscopy. The present review deals with the use of perturbations designed to specifically change the protein between two (or more) functionally relevant states, a strategy often referred to as reaction-induced IR difference spectroscopy. In the first half of this contribution, I review the technique of reaction-induced IR difference spectroscopy of proteins, with special emphasis given to the preparation of suitable samples and their characterization, strategies for the perturbation of proteins, and methodologies for time-resolved measurements (from nanoseconds to minutes). The second half of this contribution focuses on the spectral interpretation. It starts by reviewing how changes in H-bonding, medium polarity, and vibrational coupling affect vibrational frequencies, intensities, and bandwidths. It is followed by band assignments, a crucial aspect mostly performed with the help of isotopic labeling and site-directed mutagenesis, and complemented by integration and interpretation of the results in the context of the studied protein, an aspect increasingly supported by spectral calculations. Selected examples from the literature, predominately but not exclusively from retinal proteins, are used to illustrate the topics covered in this review.

Decoupled side chain and backbone dynamics for proton translocation - M2 of influenza A

The 97 amino acid bitopic membrane protein M2 of influenza A forms a tetrameric bundle in which two of the monomers are covalently linked via a cysteine bridge. In its tetrameric assembly the protein conducts protons across the viral envelope and within intracellular compartments during the infectivity cycle of the virus. A key residue in the translocation of the protons is His-37 which forms a planar tetrad in the configuration of the bundle accepting and translocating the incoming protons from the N terminal side, exterior of the virus, to the C terminal side, inside the virus. With experimentally available data from NMR spectroscopy of the transmembrane domains of the tetrameric M2 bundle classical MD simulations are conducted with the protein bundle in different protonation stages in respect to His-37. A full correlation analysis (FCA) of the data sets with the His-37 tetrad either in a fully four times unprotonated or protonated state, assumed to mimic high and low pH in vivo, respectively, in both cases reveal asymmetric backbone dynamics. His-37 side chain rotation dynamics is increased at full protonation of the tetrad compared to the dynamics in the fully unprotonated state. The data suggest that proton translocation can be achieved by decoupled side chain or backbone dynamics. Graphical abstract Visualization of the tetrameric bundle of the transmembrane domains of M2 of influenza A after 200 ns of MD simulations (upper left). The four histidine residues 37 are either not protonated as in M2⁰ or fully protonated is in M2⁴⁺. The asymmetric dynamics of the backbones are shown after a full correlation analysis (FCA) in blue (lower left). The rotational dynamics of the χ2 dihedral angles of the histidines in M2⁰ (upper right) are less than those in M2⁴⁺ (lower right).

FTIR spectral signature of anticancer drugs. Can drug mode of action be identified?

Infrared spectroscopy has brought invaluable information about proteins and about the mechanism of action of enzymes. These achievements are difficult to transpose to living organisms as all biological molecules absorb in the mid infrared, with usually a high degree of overlap. Deciphering the contribution of each enzyme is therefore almost impossible. On the other hand, small changes in the infrared spectra of cells induced by environmental conditions or drugs may provide an accurate signature of the metabolic shift experienced by the cell as a response to a change in the growth medium. The present paper aims at reviewing the contribution of infrared spectroscopy to the description of small chemical changes that occur in cells when they are exposed to a drug. In particular, this review will focus on cancer cells and anti-cancer drugs. Results accumulated so far tend to demonstrate that infrared spectroscopy could be a very accurate descriptor of the mode of action of anticancer drugs. If confirmed, such a segmentation of potential drugs according to their "mode of action" will be invaluable for the discovery of new therapeutic molecules. This article is part of a Special Issue entitled: Physiological Enzymology and Protein Functions.

Light-dark adaptation of channelrhodopsin C128T mutant

Channelrhodopsins are microbial type rhodopsins that operate as light-gated ion channels. Largely prolonged lifetimes of the conducting state of channelrhodopsin-2 may be achieved by mutations of crucial single amino acids, i.e. cysteine 128. Such mutants are of great scientific interest in the field of neurophysiology because they allow neurons to be switched on and off on demand (step function rhodopsins). Due to their slow photocycle, structural alterations of these proteins can be studied by vibrational spectroscopy in more detail than possible with wild type. Here, we present spectroscopic evidence that the photocycle of the C128T mutant involves three different dark-adapted states that are populated according to the wavelength and duration of the preceding illumination. Our results suggest an important role of multiphoton reactions and the previously described side reaction for dark state regeneration. Structural changes that cause formation and depletion of the assumed ion conducting state P520 are only small and follow larger changes that occur early and late in the photocycle, respectively. They require only minor structural rearrangements of amino acids near the retinal binding pocket and are triggered by all-trans/13-cis retinal isomerization, although additional isomerizations are also involved in the photocycle. We will discuss an extended photocycle model of this mutant on the basis of spectroscopic and electrophysiological data.

Distributed kinetics of the charge movements in bacteriorhodopsin: evidence for conformational substates

The flash-induced charge movements during the photocycle of light-adapted bacteriorhodopsin in purple membranes attached to a black lipid membrane were investigated under voltage clamp and current clamp conditions. Signal registration ranged from 200 ns to 30 s after flash excitation using a logarithmic clock, allowing the equally weighted measurement of the electrical phenomena over eight decades of time. The active pumping signals were separated from the passive system discharge on the basis of an equivalent circuit analysis. Both measuring methods were shown to yield equivalent results, but the charge translocation could be accurately monitored over the whole time range only under current clamp conditions. To describe the time course of the photovoltage signals a model based on distributed kinetics was found to be more appropriate than discrete first order processes suggesting the existence of conformational substates with distributed activation energies. The time course of the active charge displacement is characterised by a continuous relaxation time spectrum with three broad peaks plus an unresolved fast transient (<0.3 mus) of opposite polarity. The time constants and relative amplitudes (in brackets) derived from the peak rate constants and relative areas of the three bands are: tau(1) = 32 mus (20%), tau(2) = 0.89 ms (15%) and tau(3) = 18 ms (65%) at 25 degrees C in 150 mM KCl at pH7. The Arrhenius plots of the peak rate constants were linear yielding activation energies of E(A1) = 57 kJ/mol, E(A2) = 52 kJ/mol, and E(A3) = 44 kJ/mol. The electrical signal at 890 mus has no counterpart in the photocycle of bacteriorhodopsin suspensions. Fits with a sum of exponentials required 5 to 6 components and were not reproducible. Analysis of photoelectrical signals with continuous relaxation time spectra gave equally good fits with fewer parameters and were well reproducible.

Assembly of purple membranes on polyelectrolyte films

The membrane protein bacteriorhodopsin in its native membrane bound form (purple membrane) was adsorbed and incorporated into polyelectrolyte multilayered films, and adsorption was in situ monitored by optical waveguide light-mode spectroscopy. The formation of a single layer or a double layer of purple membranes was observed when adsorbed on negatively or positively charged surfaces, respectively. The purple membrane patches adsorbed on the polyelectrolyte multilayers were also evidenced by atomic force microscopy images. The driving forces of the adsorption process were evaluated by varying the ionic strength of the solution as well as the purple membrane concentration. At high purple membrane concentration, interpenetrating polyelectrolyte loops might provide new binding sites for the adsorption of a second layer of purple membranes, whereas at lower concentrations only a single layer is formed. Negative surfaces do not promote a second protein layer adsorption. Driving forces other than just electrostatic ones, such as hydrophobic forces, should play a role in the polyelectrolyte/purple membrane layering. The subtle interplay of all these factors determines the formation of the polyelectrolyte/purple membrane matrix with a presumably high degree of orientation for the incorporated purple membranes, with their cytoplasmic, or extracellular side toward the bulk on negatively or positively charged polyelectrolyte, respectively. The structural stability of bacteriorhodopsin during adsorption onto the surface and incorporation into the polyelectrolyte multilayers was investigated by Fourier transform infrared spectroscopy in attenuated total reflection mode. Adsorption and incorporation of purple membranes within polyelectrolyte multilayers does not disturb the conformational majority of membrane-embedded alpha-helix structures of the protein, but may slightly alter the structure of the extramembraneous segments or their interaction with the environment. This high stability is different from the lower stability of the predominantly beta-sheet structures of numerous globular proteins when adsorbed onto surfaces.

Molecular recognition between protein and nicotinamide dinucleotide in intact, proton-translocating transhydrogenase studied by ATR-FTIR Spectroscopy

Nicotinamide dinucleotide binding to transhydrogenase purified from Escherichia coli was investigated by attenuated total reflectance-Fourier transform infrared (ATR-FTIR) spectroscopy. Detergent-free transhydrogenase was deposited as a thin film on an ATR prism, and spectra were recorded during perfusion with buffers in the presence and absence of dinucleotide (NADP(+), NADPH, NAD(+), or NADH) in both H(2)O and D(2)O media. IR spectral changes were attributable to the bound dinucleotides and to changes in the protein itself. The dissociation constant of NADPH was estimated to be approximately 5 muM from a titration of the magnitude of the IR changes against the nucleotide concentration. IR spectra of related model compounds were used to assign principle bands of the dinucleotides. This information was combined with IR data on amino acids and with protein crystallographic data to identify interactions between specific parts of the dinucleotides and their binding sites in the protein. Several IR bands of bound nucleotide were sharpened and/or shifted relative to those in aqueous solution, reflecting a restriction to motion and a change in environment upon binding. Alterations in the protein secondary structure indicated by amide I/II changes were distinctly different for NADP(H) and for NAD(H) binding. The data suggest that NADP(H) binding leads to perturbation of a deeply buried part of the polypeptide backbone and to protonation of a carboxylic acid residue.

ATR-IR spectroscopy as applied to nucleic acid films

For the first time the ATR technique was applied to obtain IR absorption spectra of DNA and RNA dry films. There was worked out procedure of the nucleic acid removal from germanium plate, which obviously was a main obstacle to application of ATR-IR spectroscopy to nucleic acids. This technique of IR spectroscopy was applied to confirmation of RNA tropism of aurin tricarboxylic acid observed by molecular biological methods.

Identification of a Cd2+- and Zn2+-Binding Site in CytochromecUsing FTIR Coupled to an ATR Microdialysis Setup and NMR Spectroscopy†

Fourier transform infrared (FTIR) difference spectroscopy allows the study of molecular changes occurring at active sites in proteins with high sensitivity. Reactions are triggered by light, potential, or temperature steps and more recently by the diffusion of buffers containing effectors above membrane proteins deposited as films on ATR crystals. We have adapted a microdialysis system to an ATR, to study metal sites in soluble proteins. In this study, we identified a Cd(2+)- or Zn(2+)-binding site in cytochrome c with dissociation constants of 17 and 42 microM, respectively, which affects the oxidation rate of ferrocytochrome c by hydrogen peroxide. Using the microdialysis ATR-FTIR setup, we determined that a histidine and the carboxylate group of a glutamate are involved in Zn(2+) binding. The implication of His 33 and Glu 104 in the binding site was deduced from the comparison of FTIR data recorded with horse heart and the variant tuna cytochrome c lacking these two amino acids. A two-dimensional NMR analysis of the Zn(2+)-binding site in horse heart cytochrome c confirmed that His 33 and residues close to the C terminus are sensitive to Zn(2+) binding. This study demonstrates that the microdialysis ATR-FTIR setup is promising for the analysis of metal sites in proteins. From H(2)O/(2)H(2)O exchange experiments, we concluded that the impact of Zn(2+) and Cd(2+) binding on the oxidation kinetics of ferrocytochrome c by H(2)O(2) is associated to the perturbation of a hydrogen-bonding network involving His 33 that is sensitive to the redox state of cytochrome c.

The Effect of Metal Cation Binding on the Protein, Lipid and Retinal Isomeric Ratio in Regenerated Bacteriorhodopsin of Purple Membrane¶

The effect of metal cation binding on bacteriorhodopsin (bR) in purple membrane has been examined using in situ attenuated total reflection-Fourier transform infrared difference spectroscopy in aqueous media. It is known that adding metal cations to deionized bR regenerates the purple state from its blue state and recovers the proton pump function. During this process, infrared spectral changes in the frequency region of 1800-1000 cm-1 are monitored. The results reveal that metal cation binding affects the protein conformation, the retinal isomeric composition as well as lipid head groups. It is also observed that metal cation binding induces conformational changes in the alpha 1-helix region of bR, converting the portion of its alpha 1-helical domain into beta-turn or disordered coil. In addition, the influence of Ho3+ binding on the protein and lipid is observed to be larger than that of Ca2+. These results suggest that some of the metal cation binding sites are on the membrane lipid domain, while others could be on the intrahelical domain or interhelical loops where the Asp and Glu are located (binding with their COO- groups). Our results also suggest that the removal of the C-terminal of bR increase the accessibility of the binding site of metal cations, which affects protein conformational structure. All these observations are discussed in terms of the two proposals given in the literature regarding the metal cation binding sites.

FTIR spectroscopy of complexes formed between metarhodopsin II and C-terminal peptides from the G-protein alpha- and gamma-subunits

Metarhodopsin II (MII) provides the active conformation of rhodopsin for interaction with the G-protein, Gt. Fourier transform infrared spectra from samples prepared by centrifugation reflect the pH dependent equilibrium between MII and inactive metarhodopsin I. C-terminal synthetic peptides (Gtalpha(340-350) and Gtgamma(60-71)farnesyl) stabilize MII. We find that both peptides cause similar spectral changes not seen with control peptides (Gtalpha (K341R, L349A) and non-farnesylated Gtgamma). The spectra reflect all the protonation dependent bands normally observed when MII is formed at acidic pH. Beside the protonation dependent bands, additional features, similar with both peptides, appear in the amide I and II regions.

Structural difference in the H+,K+-ATPase between the E1 and E2 conformations. An attenuated total reflection infrared spectroscopy, UV circular dichroism and raman spectroscopy study

Conformational changes taking place in the gastric H+,K+-ATPase when shifting from the K+-induced E2 form to the E1 form upon replacing K+ ions by Na+ were investigated by different spectroscopic approaches. No significant secondary-structure change or secondary-structure reorientation with respect to the membrane plane could be measured by attenuated total reflection Fourier transform infrared spectroscopy of oriented films. Circular dichroism and Raman spectra obtained on tubulovesicle suspensions indicated no significant secondary structure or tyrosine and tryptophan side-chain environment changes in tubulovesicle suspensions. The smallest observable structural changes are discussed in term of the number of amino-acid residues involved for each technique.

Photoactivation of rhodopsin causes an increased hydrogen-deuterium exchange of buried peptide groups

A key step in visual transduction is the light-induced conformational changes of rhodopsin that lead to binding and activation of the G-protein transducin. In order to explore the nature of these conformational changes, time-resolved Fourier transform infrared spectroscopy was used to measure the kinetics of hydrogen/deuterium exchange in rhodopsin upon photoexcitation. The extent of hydrogen/deuterium exchange of backbone peptide groups can be monitored by measuring the integrated intensity of the amide II and amide II' bands. When rhodopsin films are exposed to D2O in the dark for long periods, the amide II band retains at least 60% of its integrated intensity, reflecting a core of backbone peptide groups that are resistant to H/D exchange. Upon photoactivation, rhodopsin in the presence of D2O exhibits a new phase of H/D exchange which at 10 degrees C consists of fast (time constant approximately 30 min) and slow (approximately 11 h) components. These results indicate that photoactivation causes buried portions of the rhodopsin backbone structure to become more accessible.

Asp76 is the Schiff base counterion and proton acceptor in the proton-translocating form of sensory rhodopsin I

Both sensory rhodopsin I, a phototaxis receptor, and bacteriorhodopsin, a light-driven proton pump, have homologous residues which have been identified as critical for bacteriorhodopsin functioning. This includes Asp76, which in the case of bacteriorhodopsin (Asp85) functions as both the Schiff base counterion and the proton acceptor. Sensory rhodopsin I exists in a pH dependent equilibrium between two different forms in the absence of its transducer protein HtrI. At pH below 7, it exists primarily in a blue form (lambda max = 587 nm) which functions as a phototaxis signal transducer when complexed to HtrI, while at higher pH, it converts to a purple proton-transporting form similar to bacteriorhodopsin (lambda max = 550 nm). We report ATR-FTIR difference spectra obtained from both low- and high-pH forms of purified sensory rhodopsin I reconstituted into lipid vesicles. The low-pH species has an ethylenic C = C stretch mode at 1520 cm-1 which shifts to 1526 cm-1 in the high-pH form. No frequency shift was found for the mutant D76N, in agreement with visible absorption measurements. Weak negative/positive bands at 1763/1751 cm-1 previously assigned to a perturbation of the C = O stretch mode of Asp76 during S373 formation in the low-pH form are replaced by a single intense positive band near 1749 cm-1 in the high-pH form. These results along with the effects of H/D exchange show that Asp76 is protonated in the signal-transducing form of sensory rhodopsin I and is ionized and functions as the counterion and Schiff base proton acceptor in the proton-transporting high-pH form of sensory rhodopsin I similar to bacteriorhodopsin.

Fourier transform infrared spectroscopy and site-directed isotope labeling as a probe of local secondary structure in the transmembrane domain of phospholamban

Phospholamban is a 52-amino acid residue membrane protein that regulates Ca(2+)-ATPase activity in the sarcoplasmic reticulum of cardiac muscle cells. The hydrophobic C-terminal 28 amino acid fragment of phospholamban (hPLB) anchors the protein in the membrane and may form part of a Ca(2+)-selective ion channel. We have used polarized attenuated total reflection-Fourier transform infrared (ATR-FTIR) spectroscopy along with site-directed isotope labeling to probe the local structure of hPLB. The frequency and dichroism of the amide I and II bands appearing at 1658 cm-1 and 1544 cm-1, respectively, show that dehydrated and hydrated hPLB reconstituted into dimyristoylphosphatidycholine bilayer membranes is predominantly alpha-helical and has a net transmembrane orientation. Specific local secondary structure of hPLB was probed by incorporating 13C at two positions in the protein backbone. A small band seen near 1614 cm-1 is assigned to the amide I mode of the 13C-labeled amide carbonyl group(s). The frequency and dichroism of this band indicate that residues 39 and 46 are alpha-helical, with an axial orientation that is approximately 30 degrees relative to the membrane normal. Upon exposure to 2H2O (D2O), 30% of the peptide amide groups in hPLB undergo a slow deuterium/hydrogen exchange. The remainder of the protein, including the peptide groups of Leu-39 and Leu-42, appear inaccessible to exchange, indicating that most of the hPLB fragment is embedded in the lipid bilayer. By extending spectroscopic characterization of PLB to include hydrated, deuterated as well as site-directed isotope-labeled hPLB films, our results strongly support models of PLB that predict the existence of an alpha-helical hydrophobic region spanning the membrane domain.

Protein conformational changes during the bacteriorhodopsin photocycle. A Fourier transform infrared/resonance Raman study of the alkaline form of the mutant Asp-85-->Asn

Bacteriorhodopsin is a light-driven proton pump, which undergoes a photocycle consisting of several distinct intermediates. Previous studies have established that the M-->N step of this photocycle involves a major conformational change of membrane embedded alpha-helices. In order to further investigate this conformational change, we have studied the photocycle of the high pH form of the mutant Asp-85-->Asn (D85Nalk). In contrast to wild type bacteriorhodopsin, D85Nalk has a deprotonated Schiff base and a blue-shifted absorption near 410 nm, yet it still transports protons in the same direction as wild type bacteriorhodopsin (Tittor, J., Schweiger, U., Oesterhelt, D. and Bamberg, E. (1994) Biophys. J., 67, 1682-1690). Resonance Raman spectroscopy of D85Nalk and D85Nalk regenerated with retinal labeled at the C-15 position with deuterium reveals the existence of an all-trans configuration of the chromophore. Fourier transform infrared difference spectroscopy shows that the photocycle of this light-adapted form involves similar events as the wild type bacteriorhodopsin photocycle including the M-->N protein conformational change. These results help to explain the ability of D85Nalk to transport protons and demonstrate that the M-->N conformational change can occur even in the photocycle of an unprotonated Schiff base form of bacteriorhodopsin.

Effects of hydrostatic pressure on the kinetics reveal a volume increase during the bacteriorhodopsin photocycle

A protein structural change in the photocycle of the proton pump, bacteriorhodopsin, detected earlier in the M photointermediate by diffraction, consists mainly of changes at the cytoplasmic surface that include an outward tilt of the cytoplasmic end of helix F. Such a conformational rearrangement would result in greater exposure of the interhelical cavity to the medium, increased binding of water, and thus an increase in volume. In order to correlate the structural change with the kinetics of the photoreaction cycle, we measured the effects of hydrostatic pressure between 1 bar and 1 kbar on the rate constants of the photocycles of wild type bacteriorhodopsin and the D96N mutant. Combining the results provided all of the activation volumes and, therefore, the changes of volume in the various states after the K photointermediate is formed. There is an approximately 32 mL/mol volume increase after deprotonation of the retinal Schiff base to the extracellular side, during the M1 --> M2 reaction, that is not reversed until well after its reprotonation from the cytoplasmic side. The magnitude of this volume increase is about as predicted by the increase of the lattice constant in the M state. It occurs in the photocycle at the proposed reprotonation switch, supporting the idea that this conformation change is what alters the accessibility of the Schiff base from one membrane side to the other. Additionally, we observe a large positive (approximately 50 mL/mol) activation volume for proton exchange between D96 and the Schiff base of the wild type protein.(ABSTRACT TRUNCATED AT 250 WORDS)

The use and misuse of FTIR spectroscopy in the determination of protein structure

Fourier transform infrared (FTIR) spectroscopy is an established tool for the structural characterization of proteins. However, many potential pitfalls exist for the unwary investigator. In this review we critically assess the application of FTIR spectroscopy to the determination of protein structure by (1) outlining the principles underlying protein secondary structure determination by FTIR spectroscopy, (2) highlighting the situations in which FTIR spectroscopy should be considered the technique of choice, (3) discussing the manner in which experiments should be conducted to derive as much physiologically relevant information as possible, and (4) outlining current methods for the determination of secondary structure from infrared spectra of proteins.

Energy coupling in an ion pump. The reprotonation switch of bacteriorhodopsin

The active site of an ion pump must communicate alternately with the two opposite membrane surfaces. In the light-driven proton pump, bacteriorhodopsin, the retinal Schiff base is first the proton donor to D85 (with access to the extracellular side), and then it becomes the acceptor of the proton of D96 (with access to the cytoplasmic side). This "reprotonation switch" has been associated with a protein conformation change observed during the photocycle. When D85 is replaced with asparagine, the pKa value of the Schiff base is lowered from above 13 to about 9. We determined the direction of the loss or gain of the Schiff base proton in unphotolyzed and in photoexcited D85N, and the D85N/D96N and D85N/D96A double mutants, in order to understand the intrinsic and the induced connectivities of the Schiff base to the two membrane surfaces. The influence of D96 mutations on proton exchange and on acceleration of proton shuttling to the surface by azide indicated that in either case the access of the Schiff base on D85N mutants is to the cytoplasmic side. In the wild-type protein (but with the pKa of the Schiff base lowered by 13-trifluoromethyl retinal substitution) the results suggested that the Schiff base can communicate also with the extracellular side. Raising the pH without illumination of D85N so as to deprotonate the Schiff base caused the same, or nearly the same, change of X-ray scattering as observed when the Schiff base deprotonates during the wild-type photocycle. The results link the charge state of the active site to the global protein conformation and to the connectivity of the Schiff base proton to the membrane surfaces. Their relationship suggests that the conformation of the unphotolyzed wild-type protein is stabilized by coulombic interaction of the Schiff base with its counter-ion. A proton is translocated across the membrane after light-induced transfer of the Schiff base proton to D85, because the protein assumes an alternative conformation that separates the donor from the acceptor and opens new conduction pathways between the active site and the two membrane surfaces.

pH-induced structural changes in bacteriorhodopsin studied by Fourier transform infrared spectroscopy

Previous C13-NMR studies showed that two of the four internal aspartic acid residues (Asp-96 and Asp-115) of bacteriorhodopsin (bR) are protonated up to pH = 10, but no accurate pKa of these residues has been determined. In this work, infrared spectroscopy with the attenuated total reflection technique was used to characterize pH-dependent structural changes of ground-state, dark-adapted wild-type bacteriorhodopsin and its mutant (D96N) with aspartic acid-96 replaced by asparagine. Data indicated deprotonation of Asp-96 at high pH (pKa = 11.4 +/- 0.1), but no Asp-115 titration was observed. The analysis of the whole spectral region characteristic to complex conformational changes in the protein showed a more complicated titration with an additional pKa value (pKa1 = 9.3 +/- 0.3 and pKa2 = 11.5 +/- 0.2). Comparison of results obtained for bR and the D96N mutant of bR shows that the pKa approximately 11.5 characterizes not a direct titration of Asp-96 but a protein conformational change that makes Asp-96 accessible to the external medium.

The Schiff base counterion of bacteriorhodopsin is protonated in sensory rhodopsin I: spectroscopic and functional characterization of the mutated proteins D76N and D76A

Both sensory rhodopsin I (SR-I), a phototaxis receptor, and bacteriorhodopsin (BR), a light-driven proton pump, share residues which have been identified as critical for BR functioning. This includes Asp76, which in the case of bacteriorhodopsin (Asp85) functions both as the Schiff base counterion and proton acceptor. We found that substituting an Asn for Asp76 (D76N) in SR-I has no effect on its visible absorption unlike the analogous mutation (D85N) in BR which shifts the absorption to longer wavelengths. The mutated proteins D76N and D76A are also fully functional as phototaxis receptors in contrast to BR, where the analogous substitutions block proton transport. D76N was also found to exhibit a spectrally normal SR587-->S373 transition. However, FTIR difference spectroscopy reveals that two bands in the SR587-->S373 difference spectrum at 1766/1749 cm-1 (negative/positive), assigned to the C=O stretch mode of a carboxylic acid, disappear in D76N, although no changes are observed in the carboxylate region. In addition, the kinetics and yield of this photoreaction are altered. On this basis, it is concluded that, unlike Asp85 in bacteriorhodopsin, Asp76 is protonated in SR-I and undergoes an increase in its hydrogen bonding during the SR587-->S373 transition. This model accounts for the difference in color of SR-I and BR and the finding that Asn can substitute for Asp76 without greatly altering the SR-I phenotype. Interestingly, parallels exist between this residue and Asp83 in the visual receptor rhodopsin which has recently been found to exist in a protonated form and to undergo an almost identical change in hydrogen bonding during rhodopsin activation.

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.

Incorporation of the nicotinic acetylcholine receptor into planar multilamellar films: characterization by fluorescence and Fourier transform infrared difference spectroscopy

A method for preparing thin, planar films of nicotinic acetylcholine receptor (nAChR) membranes that retain the ability to undergo the resting to desensitized state transition and that are suitable for spectroscopic studies has been developed. Native, alkaline-extracted nAChR membranes from Torpedo are dried under nitrogen on either a plastic microscope coverslip or a germanium internal reflection element (IRE) and then equilibrated with buffer. The drying procedure has no effect on the functional state of the nAChR as judged by a fluorescence assay using the probe ethidium bromide. The times required for an acetylcholine analogue (carbamylcholine), a local anesthetic (dibucaine), and a fluorescent probe (ethidium bromide) to penetrate films of varying degrees of thickness, interact with the receptor, and then to be washed from the films have been established. Under these conditions, the nAChR films can be repetitively cycled between the resting and desensitized states. Both fluorescence and infrared spectroscopy show that the films adhere strongly to either support even with buffer flowing continuously past the film surface. Fourier transform infrared difference spectra calculated from spectra recorded in the presence and absence of carbamylcholine show small, reproducible bands which reflect changes in nAChR structure upon desensitization.

Surface pH controls purple-to-blue transition of bacteriorhodopsin. A theoretical model of purple membrane surface

We have developed a surface model of purple membrane and applied it in an analysis of the purple-to-blue color change of bacteriorhodopsin which is induced by acidification or deionization. The model is based on dissociation and double layer theory and the known membrane structure. We calculated surface pH, ion concentrations, charge density, and potential as a function of bulk pH and concentration of mono- and divalent cations. At low salt concentrations, the surface pH is significantly lower than the bulk pH and it becomes independent of bulk pH in the deionized membrane suspension. Using an experimental acid titration curve for neutral, lipid-depleted membrane, we converted surface pH into absorption values. The calculated bacteriohodopsin color changes for acidification of purple, and titrations of deionized blue membrane with cations or base agree well with experimental results. No chemical binding is required to reproduce the experimental curves. Surface charge and potential changes in acid, base and cation titrations are calculated and their relation to the color change is discussed. Consistent with structural data, 10 primary phosphate and two basic surface groups per bacteriorhodopsin are sufficient to obtain good agreement between all calculated and experimental curves. The results provide a theoretical basis for our earlier conclusion that the purple-to-blue transition must be attributed to surface phenomena and not to cation binding at specific sites in the protein.