Specificity of anion binding in the substrate pocket of bacteriorhodopsin

The structure of the D85S mutant of bacteriorhodopsin with a nitrate anion bound in the Schiff base binding site and the structure of the anion-free protein have been obtained in the same crystal form. Together with the previously solved structures of this anion pump, in both the anion-free state and bromide-bound state, these new structures provide insight into how this mutant of bacteriorhodopsin is able to bind a variety of different anions in the same binding pocket. The structural analysis reveals that the main structural change that accommodates different anions is the repositioning of the polar side chain of S85. On the basis of these X-ray crystal structures, the prediction is then made that the D85S/D212N double mutant might bind similar anions and do so over a broader pH range than does the single mutant. Experimental comparison of the dissociation constants, K(d), for a variety of anions confirms this prediction and demonstrates, in addition, that the binding affinity is dramatically improved by the D212N substitution.     

The influence of a transmembrane pH gradient on protonation probabilities of bacteriorhodopsin: the structural basis of the back-pressure effect

Bacteriorhodopsin pumps protons across a membrane using the energy of light. The proton pumping is inhibited when the transmembrane proton gradient that the protein generates becomes larger than four pH units. This phenomenon is known as the back-pressure effect. Here, we investigate the structural basis of this effect by predicting the influence of a transmembrane pH gradient on the titration behavior of bacteriorhodopsin. For this purpose we introduce a method that accounts for a pH gradient in protonation probability calculations. The method considers that in a transmembrane protein, which is exposed to two different aqueous phases, each titratable residue is accessible for protons from one side of the membrane depending on its hydrogen-bond pattern. This method is applied to several ground-state structures of bacteriorhodopsin, which residues already present complicated titration behaviors in the absence of a proton gradient. Our calculations show that a pH gradient across the membrane influences in a non-trivial manner the protonation probabilities of six titratable residues which are known to participate in the proton transfer: D85, D96, D115, E194, E204, and the Schiff base. The residues connected to one side of the membrane are influenced by the pH on the other side because of their long-range electrostatic interactions within the protein. In particular, D115 senses the pH at the cytoplasmic side of the membrane and transmits this information to D85 and the Schiff base. We propose that the strong electrostatic interactions found between D85, D115, and the Schiff base as well as the interplay of their respective protonation states under the influence of a transmembrane pH gradient are responsible for the back-pressure effect on bacteriorhodopsin.     

Crystal structures of bR(D85S) favor a model of bacteriorhodopsin as a hydroxyl-ion pump

Structural features on the extracellular side of the D85S mutant of bacteriorhodopsin (bR) suggest that wild-type bR could be a hydroxyl-ion pump. A position between the protonated Schiff base and residue 85 serves as an anion-binding site in the mutant protein, and hydroxyl ions should have access to this site during the O-intermediate of the wild-type bR photocycle. The guanidinium group of R82 is proposed (1) to serve as a shuttle that eliminates the Born energy penalty for entry of an anion into this binding pocket, and conversely, (2) to block the exit of a proton or a related proton carrier.     

Atomic resolution structures of bacteriorhodopsin photocycle intermediates: the role of discrete water molecules in the function of this light-driven ion pump

High-resolution X-ray crystallographic studies of bacteriorhodopsin have tremendously advanced our understanding of this light-driven ion pump during the last 2 years, and emphasized the crucial role of discrete internal water molecules in the pump cycle. In the extracellular region an extensive three-dimensional hydrogen-bonded network of protein residues and seven water molecules leads from the buried retinal Schiff base via water 402 and the initial proton acceptor Asp85 to the membrane surface. Near Lys216 where the retinal binds, transmembrane helix G contains a pi-bulge that causes a non-proline kink. The bulge is stabilized by hydrogen bonding of the main chain carbonyl groups of Ala215 and Lys216 with two buried water molecules located in the otherwise very hydrophobic region between the Schiff base and the proton donor Asp96 in the cytoplasmic region. The M intermediate trapped in the D96N mutant corresponds to a late M state in the transport cycle, after protonation of Asp85 and release of a proton to the extracellular membrane surface, but before reprotonation of the deprotonated retinal Schiff base. The M intermediate from the E204Q mutant corresponds to an earlier M, as in this mutant the Schiff base deprotonates without proton release. The structures of these two M states reveal progressive displacements of the retinal, main chain and side chains induced by photoisomerization of the retinal to 13-cis,15-anti, and an extensive rearrangement of the three-dimensional network of hydrogen-bonded residues and bound water that accounts for the changed pK(a)s of the Schiff base, Asp85, the proton release group and Asp96. The structure for the M state from E204Q suggests, moreover, that relaxation of the steric conflicts of the distorted 13-cis,15-anti retinal plays a critical role in the reprotonation of the Schiff base by Asp96. Two additional waters now connect Asp96 to the carbonyl of residue 216, in what appears to be the beginning of a hydrogen-bonded chain that would later extend to the retinal Schiff base. Based on the ground state and M intermediate structures, models of the molecular events in the early part of the photocycle are presented, including a novel model which proposes that bacteriorhodopsin pumps hydroxide (OH(-)) ions from the extracellular to the cytoplasmic side.     

Wild-type and mutant bacteriorhodopsins D85N, D96N, and R82Q: purification to homogeneity, pH dependence of pumping, and electron diffraction.

Bacterioopsin, expressed in Escherichia coli as a fusion protein with 13 heterologous residues at the amino terminus, has been purified in the presence of detergents and retinylated to give bacteriorhodopsin. Further purification yielded pure bacteriorhodopsin, which had an absorbance ratio (A280/A lambda max) of 1.5 in the dark-adapted state in a single-detergent environment. This protein has a folding rate, absorbance spectrum, and light-induced proton pumping activity identical with those of bacteriorhodopsin purified from Halobacterium halobium. Protein expressed from the mutants D85N, D96N, and R82Q and purified similarly yielded pure protein with absorbance ratios of 1.5. Proton pumping rates of bacteriorhodopsins with the wild-type sequence and variants D85N, D96N, and R82Q were determined in phospholipid vesicles as a function of pH. D85N was inactive at all pH values, whereas D96N was inactive from pH 7.0 to pH 8.0, where wild type is most active, but had some activity at low pH. R82Q showed diminished proton pumping with the same pH dependence as for wild type. Bacteriorhodopsin purified from E. coli crystallized in two types of two-dimensional crystal lattices suitable for low-dose electron diffraction, which permit detailed analysis of structural differences in site-directed variants. One lattice was trigonal, as in purple membrane, and showed a high-resolution electron diffraction pattern from glucose-sustained patches. The other lattice was previously uncharacterized with unit cell dimensions a = 127 A, b = 67 A, and symmetry of the orthorhombic plane group pgg.     

Electrooptical studies on proton-binding and -release of bacteriorhodopsin

Electric field induced pH changes of purple membrane suspensions were investigated in the pH range from 4.1 to 7.6 by measuring the absorbance change of pH indicators. In connection with the photocycle and proton pump ability, three different states of bacteriorhodopsin were used: (1) the native purple bacteriorhodopsin (magnesium and calcium ions are bound, the M intermediate exists in the photocycle and protons are pumped), (2) the cation-depleted blue bacteriorhodopsin (no M intermediate), and (3) the regenerated purple bacteriorhodopsin which is produced either by raising the pH or by adding magnesium ions (the M intermediate exists). In the native purple bacteriorhodopsin there are, at least, two types of proton binding sites: one releases protons and the other takes up protons in the presence of the electric field. On the other hand, blue bacteriorhodopsin and the regenerated purple bacteriorhodopsin (pH increase) show neither proton release nor proton uptake. When magnesium ions are added to the suspensions; the field-induced pH change is observed again. Thus, the stability of proton binding depends strongly on the state of bacteriorhodopsin and differences in proton binding are likely to be related to differences in proton pump activity. Furthermore, it is suggested that the appearance of the M intermediate and proton pumping are not necessarily related.     

Local-global conformational coupling in a heptahelical membrane protein: transport mechanism from crystal structures of the nine states in the bacteriorhodopsin photocycle

Proton pumps utilize a chemical or photochemical reaction to create pH and electrical gradients between the interior and the exterior of cells and organelles that energize ATP synthesis and the accumulation and extrusion of solutes and ions. G-protein coupled receptors bind agonists and assume signaling states that communicate with the coupled transducers. How these two kinds of proteins convert chemical potential to a proton transmembrane electrochemical potential or a signal are the great questions in structural membrane biology, and they may have a common answer. Bacteriorhodopsin, a particularly simple integral membrane protein, functions as a proton pump but has a heptahelical structure like membrane receptors. Crystallographic structures are now available for all of the intermediates of the bacteriorhodopsin transport cycle, and they describe the proton translocation mechanism, step by step and in atomic detail. The results show how local conformational changes propagate upon the gradual relaxation of the initially twisted photoisomerized retinal toward the two membrane surfaces. Such local-global conformational coupling between the ligand-binding site and the distant regions of the protein may be the shared mechanism of ion pumps and G-protein related receptors.     

Transducer protein HtrI controls proton movements in sensory rhodopsin I

Sensory rhodopsin I (SR-I lambda(max) 587 nm) is a phototaxis receptor in the archaeon Halobacterium salinarium. Photoisomerization of retinal in SR-I generates a long-lived intermediate with lambda(max) 373 nm which transmits a signal to the membrane-bound transducer protein HtrI. Although SR-I is structurally similar to the electrogenic proton pump bacteriorhodopsin (BR), early studies showed its photoreactions do not pump protons, nor result in membrane hyperpolarization. These studies used functionally active SR-I, that is, SR-I complexed with its transducer HtrI. Using recombinant DNA methods we have expressed SR-I protein containing mutations in ionizable residues near the protonated Schiff base, and studied wild-type and site-specifically mutated SR-I in the presence and absence of the transducer protein. UV-Vis kinetic absorption spectroscopy, FT-IR, and pH and membrane potential probes reveal transducer-free SR-I photoreactions result in vectorial proton translocation across the membrane in the same direction as that of BR. This proton pumping is suppressed by interaction with transducer which diverts the proton movements into an electroneutral path. A key step in this diversion is that transducer interaction raises the pK(a) of the aspartyl residue in SR-I (Asp76) which corresponds to the primary proton-accepting residue in the BR pump (Asp85). In transducer-free SR-I, our evidence indicates the pK(a) of Asp76 is 7.2, and ionized Asp76 functions as the Schiff base proton acceptor in the SR-I pump. In the SR-I/HtrI complex, the pK(a) of Asp76 is 8.5, and therefore at physiological pH (7.4) Asp76 is neutral. Protonation changes on Asp76 are clearly not required for signaling since the SR-I mutants D76N and D76A are active in phototaxis. The latent proton-translocation potential of SR-I may reflect the evolution of the SR-I sensory signaling mechanism from the proton pumping mechanism of BR.     

Structure of bacteriorhodopsin at 1.55 A resolution.

Th?e atomic structure of the light-driven ion pump bacteriorhodopsin and the surrounding lipid matrix was determined by X-ray diffraction of crystals grown in cubic lipid phase. In the extracellular region, an extensive three-dimensional hydrogen-bonded network of protein residues and seven water molecules leads from the buried retinal Schiff base and the proton acceptor Asp85 to the membrane surface. Near Lys216 where the retinal binds, transmembrane helix G contains a pi-bulge that causes a non-proline? kink. The bulge is stabilized by hydrogen-bonding of the main-chain carbonyl groups of Ala215 and Lys216 with two buried water molecules located between the Schiff base and the proton donor Asp96 in the cytoplasmic region. The results indicate extensive involvement of bound water molecules in both the structure and the function of this seven-helical membrane protein. A bilayer of 18 tightly bound lipid chains forms an annulus around the protein in the crystal. Contacts between the trimers in the membrane plane are mediated almost exclusively by lipids.     

Engineered Passive Potassium Conductance in the KR2 Sodium Pump

Light-driven sodium pumps (NaRs) are microbial rhodopsins that utilize light energy to actively transport sodium ions out of the cell. Here, we used targeted mutagenesis and electrophysiological methods in living cells to demonstrate that NaRs can be converted into light-activated cation channels by molecular engineering. Specifically, introduction of the R109Q mutation into the sodium ion pump of Dokdonia eikasta (KR2) results in passive ion conductance, with a high preference for potassium over sodium ions. However, in this mutant, residual active outward pumping of sodium ions competes with passive inward transport of potassium. Channel-like behavior could also be achieved by introduction of other mutations into the KR2 counterion complex, and further, these modifications were transferrable to other NaRs. Combining the R109Q replacement with modifications at position S70 removed the residual sodium pumping and greatly enhanced the channel-like activity. However, passive photocurrents were only observed in leak mutants if the KR2 counterions, D116 and D251, were deprotonated, which was only observed under alkaline conditions. Overall, our results reveal that interactions between R109 and the nearby residues, L75, S70, D116, and D251, prevent passive backflow during ion transport in NaRs.     

Mechanism of a molecular valve in the halorhodopsin chloride pump

Halorhodopsin is a light-driven chloride anion pump in which the trans-->cis photoisomerization of a retinal chromophore triggers a photocycle resulting in the translocation of chloride across the plasma membrane. The mechanism of chloride transfer past the cis retinal is determined here by computing multiple pathways for this process. The calculations reveal two conditions of the valve mechanism. First, a lumen absent in the ground state structure is transiently opened by chloride passage. Second, this activated opening, which is achieved by flexible deformation of the surrounding protein, is shown to significantly raise the chloride translocation barrier between photocycles, thus preventing chloride backflow. Unlike macroscopic valve designs, the protein allows differential ion flows in the pumping and resting states that are tuned to match the physiological timescales of the cell, thus creating a "kinetic" valve.     

Lipidic cubic phase crystallization of bacteriorhodopsin and cryotrapping of intermediates: towards resolving a revolving photocycle

Bacteriorhodopsin is a small retinal protein found in the membrane of the halophilic bacterium Halobacterium salinarum, whose function is to pump protons across the cell membrane against an electrostatic potential, thus converting light into a proton-motive potential needed for the synthesis of ATP. Because of its relative simplicity, exceptional stability and the fundamental importance of vectorial proton pumping, bacteriorhodopsin has become one of the most important model systems in the field of bioenergetics. Recently, a novel methodology to obtain well-diffracting crystals of membrane proteins, utilizing membrane-like bicontinuous lipidic cubic phases, has been introduced, providing X-ray structures of bacteriorhodopsin and its photocycle intermediates at ever higher resolution. We describe this methodology, the new insights provided by the higher resolution ground state structures, and review the mechanistic implications of the structural intermediates reported to date. A detailed understanding of the mechanism of vectorial proton transport across the membrane is thus emerging, helping to elucidate a number of fundamental issues in bioenergetics.     

High-throughput screening of bacteriorhodopsin mutants in whole cell pastes

A high-throughput screening method has been developed which enables functional analysis of bacteriorhodpsin in whole cell pastes. Reflectance spectra, from as little as 5 ml of Halobacterium salinarum cells, show close correspondence to that obtained from the purified purple membrane (PM), containing bacteriorhodopsin (BR) as the sole protein component. We demonstrate accurate quantification of BR accumulation by ratiometric analysis of BR (A_max 568) and a membrane-bound cytochrome (A_max 410). In addition, ground-state light- and dark-adapted (LA and DA, respectively) spectral differences were determined with high accuracy and precision. Using cells expressing the BR mutant D85N, we monitored transitions between intermediate-state homologues of the reprotonation phase of the light-activated proton pumping mechanism. We demonstrate that phenotypes of three mutants (D85N/T170C, D85N/D96N, and D85N/R82Q) previously characterized for their effect on photocycle transitions are reproduced in the whole cell samples. D85N/T170C stabilizes accumulation of the N state while D85N/D96N accumulates no N state. D85N/R82Q was found to have perturbed the pK_a of M accumulation. These studies illustrate the correspondence between pH-dependent ground-state transitions accessed by D85N and the transitions accessed by the wild-type protein following photoexcitation. We demonstrate that whole cell reflectance spectroscopy can be used to efficiently characterize the large numbers of mutants generated by engineering strategies that exploit saturation mutagenesis.     

Chemical and physical evidence for multiple functional steps comprising the M state of the bacteriorhodopsin photocycle

In the photocycle of bacteriorhodopsin (bR), light-induced transfer of a proton from the Schiff base to an acceptor group located in the extracellular half of the protein, followed by reprotonation from the cytoplasmic side, are key steps in vectorial proton pumping. Between the deprotonation and reprotonation events, bR is in the M state. Diverse experiments undertaken to characterize the M state support a model in which the M state is not a static entity, but rather a progression of two or more functional substates. Structural changes occurring in the M state and in the entire photocycle of wild-type bR can be understood in the context of a model which reconciles the chloride ion-pumping phenotype of mutants D85S and D85T with the fact that bR creates a transmembrane proton-motive force.     

Two pumps, one principle: light-driven ion transport in halobacteria

Comparison of the primary structure of the chloride pump halorhodopsin with that of the proton pump bacteriorhodopsin provides insight into light-driven ion transport by retinal proteins. Several conserved amino acid residues in the membrane-spanning region of both proteins and their interaction with different isomerization states of retinal are suggested to be the key element for ion transport in both proteins.     

Analogies between halorhodopsin and bacteriorhodopsin

The light-activated proton-pumping bacteriorhodopsin and chloride ion-pumping halorhodopsin are compared. They belong to the family of retinal proteins, with 25% amino acid sequence homology. Both proteins have seven alpha helices across the membrane, surrounding the retinal binding pocket. Photoexcitation of all-trans retinal leads to ion transporting photocycles, which exhibit great similarities in the two proteins, despite the differences in the ion transported. The spectra of the K, L, N and O intermediates, calculated using time-resolved spectroscopic measurements, are very similar in both proteins. The absorption kinetic measurements reveal that the chloride ion transporting photocycle of halorhodopsin does not have intermediate M characteristic for deprotonated Schiff base, and intermediate L dominates the process. Energetically the photocycle of bacteriorhodopsin is driven mostly by the decrease of the entropic energy, while the photocycle of halorhodopsin is enthalpy-driven. The ion transporting steps were characterized by the electrogenicity of the intermediates, calculated from the photoinduced transient electric signal measurements. The function of both proteins could be described with the 'local access' model developed for bacteriorhodopsin. In the framework of this model it is easy to understand how bacteriorhodopsin can be converted into a chloride pump, and halorhodopsin into a proton pump, by changing the ion specificity with added ions or site-directed mutagenesis.     

Compositional heterogeneity reflects partial dehydration in three-dimensional crystals of bacteriorhodopsin

Absorption, fluorescence and excitation spectra of three-dimensional bacteriorhodopsin crystals harvested from a lipidic cubic phase are presented. The combination of the spectroscopic experiments performed at room temperature, controlled pH and full external hydration reveals the presence of three distinct protein species. Besides the well-known form observed in purple membrane, we find two other species with a relative contribution of up to 30%. As the spectra are similar to those of dehydrated or deionized membranes containing bacteriorhodopsin, we suggest that amino acid residues, located in the vicinity of the retinal chromophore, have changed their protonation state. We propose partial dehydration during crystallization and/or room temperature conditions as the main source of this heterogeneity. This assignment is supported by an experiment showing interconversion of the species upon intentional dehydration and by crystallographic data, which have indicated an in-plane unit cell in 3D crystals comparable to that of dehydrated bacteriorhodopsin membranes. Full hydration of the proteins after the water-withdrawing crystallization process is hampered. We suggest that this hindered water diffusion originates mainly from a closure of hydrophobic crystal surfaces by lipid bilayers. The present spectroscopic work complements the crystallographic data, due to its ability to determine quantitatively compositional heterogeneity resulting from proteins in different protonation states.     

Metal-ATP complexes as substrates and free metal ions as activators of the red cell calcium pump

The plasma membrane calcium pump in most mammalian cells is the basic mechanism for assuring a low cytoplasmic calcium concentration. In inside-out human red cell membrane vesicles /IOVs/ the substrate and metal specificity as well as the intracellular protein /calmodulin/ regulation of the ATP-dependent active calcium transport can be investigated $\text{in}$$\text{situ}$. In this paper we demonstrate that Me²⁺. ATP^4? /in the following MeATP/ complexes, including MgATP, MnATP, CoATP, FeATP, and NiATP, can serve as substrates for the calcium pump in IOVs. Calcium pumping is activated by the above metals, while Sr, Ba, Cu, Cd ions or the trivalent cations are ineffective in this respect. Calmodulin-stimulation of the calcium transport is present independent of the metal ions used for the activation of the pump. Based on kinetic studies we suggest that divalent metal ions interact with the red cell calcium pump at four different sites: 1./ MeATP complex is the true substrate of the pump; 2./ Ca or Sr ions activate the system by binding to the transport site/s/ and other metal ions competitively inhibit this binding; 3./ the presence of free divalent metal ions /Mg, Mn, Co, Fe, or Ni, but not Ca, Sr, Ba/ is required for activating calcium translocation; 4./ interaction with a Ca — calmodulin complex specifically stimulates calcium pumping.     

Energy transduction in transmembrane ion pumps

Recent crystallographic structures of three different ion pumps provide a first view of the mechanisms by which these molecular machines transfer ions across cell membranes against an electrochemical gradient. Each of the structures reinforces the concept that several buried counter ions have central roles in substrate recruitment, substrate binding and energy transduction during ion pumping. The spatial organization of the counter ions suggests that, initially, one or more counter ions lowers the Born energy cost of binding a substrate ion in the low-dielectric interior of the membrane. Subsequently, a ligand-induced conformational change seems to close a charged access gate to prevent backflow from a subsequent, low-affinity state of the pump. A final role of the buried counter ions might be to couple the input of external energy to a small charge separation between the substrate ion and the buried counter ions, thereby decreasing the binding affinity for the substrate ion in preparation for its release on the high-energy side of the membrane.     

Membrane regulation of the Na+,K+-ATPase during the neuroblastoma cell cycle: correlation with protein lateral mobility

The pumping activity of the plasma membrane-bound Na+,K+-ATPase shows considerable variation during the cell cycle of mouse neuroblastoma Neuro-2A cells. Addition of external ATP at millimolar concentrations, which selectively enhances the plasma membrane permeability of Neuro-2A cells for sodium ions, stimulates the Na+,K+-ATPase pumping activity at all phases of the cell cycle from a factor of 1.05 in mitosis up to 2.2 in G1 phase. Determination of the number of Na+,K+-ATPase copies per cell by direct 3H-ouabain binding studies in the presence of external ATP shows a gradual increase in the number of pump sites on passing from mitosis to the late S/G2-phase by approximately a factor of 2. From these data the pumping activity per copy of Na+,K+-ATPase, optimally stimulated with respect to its various substrate ions, has been determined during the various phases of the cell cycle. This optimally stimulated pumping activity per enzyme copy, which is a reflection of the physicochemical state of the plasma membrane, is high in mitosis, almost twofold lower in early G1 phase, and increases gradually again during the other phases of the cell cycle. This shows that the observed regulation of Na+,K+-ATPase activity during the cell cycle is caused by a combination of three independent factors--namely variation in intracellular substrate availability (Na+), changes in number of enzyme copies per cell, and modulation of the plasma membrane environment of the protein molecules. The modulation of the optimal pumping activity per enzyme copy shows a good correlation (rho = 0.96) with the known modulation of protein lateral mobility during the cell cycle, such that a high protein lateral mobility correlates with a low enzyme activity. It is concluded that changes in plasma membrane properties take place during the Neuro-2A cell cycle that result in changes in the rate of protein lateral diffusion and Na+,K+-ATPase activity in directly correlated way.