X-ray diffraction of bacteriorhodopsin photocycle intermediates

Recent advances in the crystallography of bacteriorhodopsin, the light-driven proton pump, have yielded structural models for all intermediates of the photochemical cycle. For seven of the species, X-ray diffraction data were collected from trapped photostationary states in crystals, and for the two remaining ones the structures of selected mutants are available. The changes of the retinal chromophore, protein and bound water describe, at an atomic level, how accommodation of the twisted photoisomerized retinal to its binding site causes de-protonation of the retinal Schiff base and initiates cascades of gradual conformational rearrangements of the protein. One cascade propagates in the extracellular direction and results in proton release, and the other in the cytoplasmic direction and results in side-chain and main-chain rearrangements, formation of a chain of hydrogen-bonded water, and proton uptake from the bulk. Such local-global conformational coupling, with gradual spreading of a local perturbation over the rest of the protein, might be the uniting principle of transporters and receptors.     

Bacteriorhodopsin: a high-resolution structural view of vectorial proton transport

Recent 3-D structures of several intermediates in the photocycle of bacteriorhodopsin (bR) provide a detailed structural picture of this molecular proton pump in action. In this review, we describe the sequence of conformational changes of bR following the photoisomerization of its all-trans retinal chromophore, which is covalently bound via a protonated Schiff base to Lys216 in helix G, to a 13-cis configuration. The initial changes are localized near the protein's active site and a key water molecule is disordered. This water molecule serves as a keystone for the ground state of bR since, within the framework of the complex counter ion, it is important both for stabilizing the structure of the extracellular half of the protein, and for maintaining the high pK_a of the Schiff base (the primary proton donor) and the low pK_a of Asp85 (the primary proton acceptor). Subsequent structural rearrangements propagate out from the active site towards the extracellular half of the protein, with a local flex of helix C exaggerating an early movement of Asp85 towards the Schiff base, thereby facilitating proton transfer between these two groups. Other coupled rearrangements indicate the mechanism of proton release to the extracellular medium. On the cytoplasmic half of the protein, a local unwinding of helix G near the backbone of Lys216 provides sites for water molecules to order and define a pathway for the reprotonation of the Schiff base from Asp96 later in the photocycle. A steric clash of the photoisomerized retinal with Trp182 in helix F drives an outward tilt of the cytoplasmic half of this helix, opening the proton transport channel and enabling a proton to be taken up from the cytoplasm. Although bR is the first integral membrane protein to have its catalytic mechanism structurally characterized in detail, several key results were anticipated in advance of the structural model and the general framework for vectorial proton transport has, by and large, been preserved.     

Bacteriorhodopsin: a high-resolution structural view of vectorial proton transport

Recent 3-D structures of several intermediates in the photocycle of bacteriorhodopsin (bR) provide a detailed structural picture of this molecular proton pump in action. In this review, we describe the sequence of conformational changes of bR following the photoisomerization of its all-trans retinal chromophore, which is covalently bound via a protonated Schiff base to Lys216 in helix G, to a 13-cis configuration. The initial changes are localized near the protein's active site and a key water molecule is disordered. This water molecule serves as a keystone for the ground state of bR since, within the framework of the complex counter ion, it is important both for stabilizing the structure of the extracellular half of the protein, and for maintaining the high pK(a) of the Schiff base (the primary proton donor) and the low pK(a) of Asp85 (the primary proton acceptor). Subsequent structural rearrangements propagate out from the active site towards the extracellular half of the protein, with a local flex of helix C exaggerating an early movement of Asp85 towards the Schiff base, thereby facilitating proton transfer between these two groups. Other coupled rearrangements indicate the mechanism of proton release to the extracellular medium. On the cytoplasmic half of the protein, a local unwinding of helix G near the backbone of Lys216 provides sites for water molecules to order and define a pathway for the reprotonation of the Schiff base from Asp96 later in the photocycle. A steric clash of the photoisomerized retinal with Trp182 in helix F drives an outward tilt of the cytoplasmic half of this helix, opening the proton transport channel and enabling a proton to be taken up from the cytoplasm. Although bR is the first integral membrane protein to have its catalytic mechanism structurally characterized in detail, several key results were anticipated in advance of the structural model and the general framework for vectorial proton transport has, by and large, been preserved.     

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.     

Molecular dynamics study of the M412 intermediate of bacteriorhodopsin.

Molecular dynamics simulations have been carried out to study the M412 intermediate of bacteriorhodopsin's (bR) photocycle. The simulations start from two simulated structures for the L550 intermediate of the photocycle, one involving a 13-cis retinal with strong torsions, the other a 13,14-dicis retinal, from which the M412 intermediate is initiated through proton transfer to Asp-85. The simulations are based on a refined structure of bR568 obtained through all-atom molecular dynamics simulations and placement of 16 waters inside the protein. The structures of the L550 intermediates were obtained through simulated photoisomerization and subsequent molecular dynamics, and simulated annealing. Our simulations reveal that the M412 intermediate actually comprises a series of conformations involving 1) a motion of retinal; 2) protein conformational changes; and 3) diffusion and reconfiguration of water in the space between the retinal Schiff base nitrogen and the Asp-96 side group. (1) turns the retinal Schiff base nitrogen from an early orientation toward Asp-85 to a late orientation toward Asp-96; (2) disconnects the hydrogen bond network between retinal and Asp-85 and tilts the helix F of bR, enlarging bR's cytoplasmic channel; (3) adds two water molecules to the three water molecules existing in the cytoplasmic channel at the bR568 stage and forms a proton conduction pathway. The conformational change (2) of the protein involves a 60 degrees bent of the cytoplasmic side of helix F and is induced through a break of a hydrogen bond between Tyr-185 and a water-side group complex in the counterion region.     

Suppression of the back proton-transfer from Asp85 to the retinal Schiff base in bacteriorhodopsin: a theoretical analysis of structural elements

The transfer of a proton from the retinal Schiff base to the nearby Asp85 protein group is an essential step in the directional proton-pumping by bacteriorhodopsin. To avoid the wasteful back reprotonation of the Schiff base from Asp85, the protein must ensure that, following Schiff base deprotonation, the energy barrier for back proton-transfer from Asp85 to the Schiff base is larger than that for proton-transfer from the Schiff base to Asp85. Here, three structural elements that may contribute to suppressing the back proton-transfer from Asp85 to the Schiff base are investigated: (i) retinal twisting; (ii) hydrogen-bonding distances in the active site; and (iii) the number and location of internal water molecules. The impact of the pattern of bond twisting on the retinal deprotonation energy is dissected by performing an extensive set of quantum-mechanical calculations. Structural rearrangements in the active site, such as changes of the Thr89:Asp85 distance and relocation of water molecules hydrogen-bonding to the Asp85 acceptor group, may participate in the mechanism which ensures that following the transfer of the Schiff base proton to Asp85 the protein proceeds with the subsequent photocycle steps, and not with back proton transfer from Asp85 to the Schiff base.     

Water and bacteriorhodopsin: structure, dynamics, and function

A wealth of information has been gathered during the past decades that water molecules do play an important role in the structure, dynamics, and function of bacteriorhodopsin (bR) and purple membrane. Light-induced structural alterations in bR as detected by X-ray and neutron diffraction at low and high resolution are discussed in relationship to the mechanism of proton pumping. The analysis of high resolution intermediate structures revealed photon-induced rearrangements of water molecules and hydrogen bonds concomitant with conformational changes in the chromophore and the protein. These observations led to an understanding of key features of the pumping mechanism, especially the vectoriality and the different modes of proton translocation in the proton release and uptake domain of bR. In addition, water molecules influence the function of bR via equilibrium fluctuations, which must occur with adequate amplitude so that energy barriers between conformational states can be overcome.     

Conformational coupling between the cytoplasmic carboxylic acid and the retinal in a fungal light-driven proton pump

Many fungal rhodopsins, eukaryotic structural homologues of the archaeal light-driven proton pump bacteriorhodopsin, have been discovered in the course of genome sequencing projects. Recently, two fungal rhodopsins were characterized in vitro and exhibited very different photochemical behavior. Neurospora rhodopsin possesses a slow photocycle and shows no ion transport, reminiscent of sensory rhodopsins, while Leptosphaeria rhodopsin has a fast bacteriorhodopsin-like photocycle and pumps protons light-dependently. Such a dramatic difference is surprising considering the very high degree of sequence homology of the two proteins. In this paper, we investigate whether the chemical structure of a cytoplasmic carboxylic acid, the homologue of Asp-96 of bacteriorhodopsin serving as a proton donor for the retinal Schiff base, can define the photochemical properties of fungal rhodopsins. We studied mutants of Leptosphaeria rhodopsin in which this aspartic acid was replaced with Glu or Asn using spectroscopy in the infrared and visible ranges. We show that Glu at this position is inefficient as a proton donor similar to a nonprotonatable Asn. Moreover, this replacement induces long-range structural perturbations of the retinal environment, as evidenced by changes in the vibrational bands of retinal (especially, hydrogen-out-of-plane modes) and neighboring aspartic acids and water molecules. The conformational coupling of the mutation site to the retinal may be mediated by helical rearrangements as suggested by the changes in amide and proline vibrational bands. We conclude that the difference in the photochemical behavior of fungal rhodopsins from Leptosphaeria and Neurospora may be ascribed, to some extent, to the replacement of the cytoplasmic proton donor Asp with Glu.     

Crystallographic structure of the retinal and the protein after deprotonation of the Schiff base: the switch in the bacteriorhodopsin photocycle

We illuminated bacteriorhodopsin crystals at 210K to produce, in a photostationary state with 60% occupancy, the earliest M intermediate (M1) of the photocycle. The crystal structure of this state was then determined from X-ray diffraction to 1.43 A resolution. When the refined model is placed after the recently determined structure for the K intermediate but before the reported structures for two later M states, a sequence of structural changes becomes evident in which movements of protein atoms and bound water are coordinated with relaxation of the initially strained photoisomerized 13-cis,15-anti retinal. In the K state only retinal atoms are displaced, but in M1 water 402 moves also, nearly 1A away from the unprotonated retinal Schiff base nitrogen. This breaks the hydrogen bond that bridges them, and initiates rearrangements of the hydrogen-bonded network of the extracellular region that develop more fully in the intermediates that follow. In the M1 to M2 transition, relaxation of the C14-C15 and C15=NZ torsion angles to near 180 degrees reorients the retinylidene nitrogen atom from the extracellular to the cytoplasmic direction, water 402 becomes undetectable, and the side-chain of Arg82 is displaced strongly toward Glu194 and Glu204. Finally, in the M2 to M2' transition, correlated with release of a proton to the extracellular surface, the retinal assumes a virtually fully relaxed bent shape, and the 13-methyl group thrusts against the indole ring of Trp182 which tilts in the cytoplasmic direction. Comparison of the structures of M1 and M2 reveals the principal switch in the photocycle: the change of the angle of the C15=NZ-CE plane breaks the connection of the unprotonated Schiff base to the extracellular side and establishes its connection to the cytoplasmic side.     

The influence of hydration on the conformation of lysozyme studied by solid-state 13C-nmr spectroscopy

¹³C proton decoupled cross-polarization magic-angle spinning nmr spectra of lysozyme are reported as a function of hydration. Increases in hydration level enhance the resolution of the spectra, particularly in the aliphatic region, but has no significant effect on either the rotating frame proton spin–lattice relaxation time or the cross-relaxation time. The enhancement in spectral resolution with hydration is attributed to a decrease in the distribution of isotropic chemical shifts, which reflects a decrease in the distribution of conformational states sampled by the protein. Changes in the distribution of isotropic chemical shifts occur after the addition of water to the charged groups as coverage of the polar side chains and peptide groups takes place. The onset of this behavior occurs at a hydration level of about, 0.1–0.2 g water/g protein and is largely complete at about 0.3 g water/g protein, the same hydration range where changes in the heat capacity are observed. That hydrogen exchange of buried protons can occur at hydration levels significantly lower than those at which changes in the distribution of conformational states are first observed suggests that some motions that mediate exchange are already present in the dry protein. The preservation of efficient dipolar coupling indicates that the conformational rearrangements that do-occur on hydration are small and do not involve any significant overall expansion of free volume or weakening of interactions that would increase the reorientational freedom of protein groups. © 1993 John Wiley & Sons, Inc.     

Proton translocation by bacteriorhodopsin in the absence of substantial conformational changes

Unlike wild-type bacteriorhodopsin (BR), the BR triple mutant D96G/F171C/F219L has been shown to undergo only minor structural rearrangements during its photocycle. Nonetheless, the mutant is capable of transporting protons at a rate of 125(+/-40) H+/BR per minute under light-saturating conditions. Light adaptation of the triple mutant's retinal proceeds in a pH-dependent manner up to a maximum of 63% all-trans. These two findings imply that the transport activity of the triple mutant comprises 66% of the wild-type activity. Time-resolved spectroscopy reveals that the identity and sequence of intermediates in the photocycle of the triple mutant in the all-trans configuration correspond to that of wild-type BR. The only differences relate to a slower rise and decay of the M and O intermediates, and a significant spectral contribution from a 13-cis component. No indication for accumulation of the N intermediate is found under a variety of conditions that normally favor the formation of this species in wild-type BR. The Fourier transform infrared (FTIR) spectrum of the M intermediate in the triple mutant resembles that of wild type. Minor changes in the amide I region during the photocycle suggest that only small movements of the protein backbone occur. Electron microscopy reveals large differences in conformation between the unilluminated state of the mutant protein and wild-type but no light-induced changes in time-resolved measurements. Evidently, proton transport by the triple mutant does not require the major conformational rearrangements that occur on the same time-scale with wild-type. Thus, we conclude that large conformational changes observed in the photocycle of the wild-type and many BR mutants are not a prerequisite for the change in accessibility of the Schiff base nitrogen atom that must occur during vectorial catalysis to allow proton transport.     

Early structural rearrangements in the photocycle of an integral membrane sensory receptor

Sensory rhodopsins are the primary receptors of vision in animals and phototaxis in microorganisms. Light triggers the rapid isomerization of a buried retinal chromophore, which the protein both accommodates and amplifies into the larger structural rearrangements required for signaling. We trapped an early intermediate of the photocycle of sensory rhodopsin II from Natronobacterium pharaonis (pSRII) in 3D crystals and determined its X-ray structure to 2.3 A resolution. The observed structural rearrangements were localized near the retinal chromophore, with a key water molecule becoming disordered and the retinal's beta-ionone ring undergoing a prominent movement. Comparison with the early structural rearrangements of bacteriorhodopsin illustrates how modifications in the retinal binding pocket of pSRII allow subtle differences in the early relaxation of photoisomerized retinal.     

The chromophore retinal hinders passive proton/hydroxide ion translocation through bacteriorhodopsin

Experiments have been performed to examine any influence of the chromophore retinal in bacteriorhodopsin (BR) on the passive proton/hydroxide ion flux through this integral membrane protein. BR was reconstituted into dimyristoylphosphatidylcholine (DMPC)-phosphatidylserine or DMPC-dimyristoylphosphatidylglycerol unilamellar vesicles with molar lipid to protein ratios ranging from 30 to 150. The entrapped fluorescence dye pyranine served as a reliable indicator of the internal proton concentration. Transmembrane pH-gradients were quickly established across the vesicular membrane and the kinetics of the induced fluorescence changes were compared for vesicles with incorporated native BR, BR bleached to the chromophore-free protein bacterioopsin, and BR regenerated from bacterioopsin with all-trans-retinal, respectively. For aggregated protein molecules, the H+/OH- diffusion across bacterioopsin was always considerably faster than that through the protein containing covalently bound retinal. The decay rate of the imposed pH-gradient was 4.4-9.1 and 2.0-5.1 times slower for native and regenerated BR, respectively, as compared to bacterioopsin. Stepwise regeneration of bacterioopsin with all-trans-retinal revealed a linear dependence of the predominant delta pH-decay time on the degree of regeneration. Essentially the same observations were made with monomeric protein molecules in vesicular lipid membranes. The results demonstrate that the chromophore retinal itself blocks the H+/OH- conducting pathway across the transmembrane protein BR or indirectly controls this path by inducing conformational changes in the protein upon binding.     

Oxygen reactions in p-hydroxybenzoate hydroxylase utilize the H-bond network during catalysis

para-Hydroxybenzoate hydroxylase is a flavoprotein monooxygenase that catalyses a reaction in two parts: reduction of the flavin adenine dinucleotide (FAD) in the enzyme by reduced nicotinamide adenine dinucleotide phosphate (NADPH) in response to binding p-hydroxybenzoate to the enzyme and oxidation of reduced FAD with oxygen to form a hydroperoxide, which then oxygenates p-hydroxybenzoate. These different reactions are coordinated through conformational rearrangements of the protein and isoalloxazine ring during catalysis. Earlier research showed that reduction of FAD occurs when the isoalloxazine of the FAD moves to the surface of the protein to allow hydride transfer from NADPH. This move is coordinated with protein rearrangements that are triggered by deprotonation of buried p-hydroxybenzoate through a H-bond network that leads to the surface of the protein. In this paper, we examine the involvement of this same H-bond network in the oxygen reactions-the initial formation of a flavin-C4a-hydroperoxide from the reaction between oxygen and reduced flavin, the electrophilic attack of the hydroperoxide upon the substrate to form product, and the elimination of water from the flavin-C4a-hydroxide to form oxidized enzyme in association with product release. These reactions were measured through absorbance and fluorescence changes in the FAD during the reactions. Results were collected over a range of pH for the reactions of wild-type enzyme and a series of mutant enzymes with the natural substrate and substrate analogues. We discovered that the rate of formation of the flavin hydroperoxide is not influenced by pH change, which indicates that the proton required for this reaction does not come from the H-bond network. The rate of the hydroxylation reaction increases with pH in a manner consistent with a pK(a) of 7.1. We conclude that the H-bond network abstracts the phenolic proton from p-hydroxybenzoate in the transition state of oxygen transfer. The rate of formation of oxidized enzyme increases with pH in a manner consistent with a pK(a) of 7.1, indicating the involvement of the H-bond network. We conclude that product deprotonation enhances the rate of a specific conformational change required for both product release and the elimination of water from C4a-OH-FAD.     

Excitation of the L intermediate of bacteriorhodopsin: electric responses to test x-ray structures

The L intermediate of bacteriorhodopsin was excited, and its electrical response was measured. Two positive components were found in it with respect to the direction of proton pumping: an unresolved fast component, and a slower one (tau=7 micros) of small amplitude. The fast component was assigned to a charge motion corresponding to reisomerization of the retinal moiety, whereas the slow one was attributed to charge rearrangements reestablishing the ground state. Because three x-ray crystallographic structures have recently been reported for the L intermediate, it seemed important to calculate the intramolecular dipole moment changes associated to bR-->L for all three structures, so as to compare them with similar quantities determined from the electrical signals. The results are discussed in terms of amino acid side chains possibly contributing to the observed effect. We propose to use electrical signals as a verification tool for intermediate structures of the photocycle, and thus for molecular models of proton pumping.     

Cytoplasmic shuttling of protons in anabaena sensory rhodopsin: implications for signaling mechanism

It was found recently that Anabaena sensory rhodopsin (ASR), which possibly serves as a photoreceptor for chromatic adaptation, interacts with a soluble cytoplasmic transducer. The X-ray structure of the transducer-free protein revealed an extensive hydrogen-bonded network of amino acid residues and water molecules in the cytoplasmic half of ASR, in high contrast to its haloarchaeal counterparts. Using time-resolved spectroscopy of the wild-type and mutant ASR in the visible and infrared ranges, we tried to determine whether this hydrogen-bonded network is used to translocate protons and whether those proton transfers are important for interaction with the transducer. We found that the retinal Schiff base deprotonation, which occurs in the M intermediate of the photocycle of all-trans-ASR, results in protonation of Asp217 on the cytoplasmic side of the protein. The deprotonation of the Schiff base induces a conformational change of ASR observed through the perturbation of associated lipids. We suggest that the cytoplasmic shuttling of protons in the photocycle of all-trans-ASR and the ensuing conformational changes might activate the transducer. Consequently, the M intermediate may be the signaling state of ASR.     

Rhodopsin and 9-demethyl-retinal analog: effect of a partial agonist on displacement of transmembrane helix 6 in class A G protein-coupled receptors

Rhodopsin is the visual pigment of rod cells and a prototypical G protein-coupled receptor. It is activated by cis-->trans photoisomerization of the covalently bound chromophore 11-cis-retinal, which acts in the cis configuration as an inverse agonist. Light-induced formation of the full agonist all-trans-retinal in situ triggers conformational changes in the protein moiety. Partial agonists of rhodopsin include a retinal analog lacking the methyl group at C-9, termed 9-demethyl-retinal (9-dm-retinal). Rhodopsin reconstituted with this retinal (9-dm-rhodopsin) activates G protein poorly. Here we investigated the molecular nature of the partial agonism in 9-dm-rhodopsin using site-directed spin labeling. Earlier site-directed spin labeling studies of rhodopsin identified a rigid-body tilt of the cytoplasmic segment of [corrected] transmembrane helix 6 (TM6) by approximately 6A as a central event in rhodopsin activation. Data presented here provide additional evidence for this mechanism. Only a small fraction of photoexcited 9-dm pigments reaches the TM6-tilted conformation. This fraction can be increased by increasing proton concentration or [corrected] by anticipation of the activating protonation step by the mutation E134Q in 9-dm-rhodopsin. These results on protein conformation are in complete accord with previous findings regarding the biological activity of the 9-dm pigments. When the proton concentration is further increased, a new state arises in 9-dm pigments that is linked to direct proton uptake at the retinal Schiff base. This state apparently has a conformation distinguishable from the active state.     

Structural changes in the L photointermediate of bacteriorhodopsin

The L to M reaction of the bacteriorhodopsin photocycle includes the crucial proton transfer from the retinal Schiff base to Asp85. In spite of the importance of the L state in deciding central issues of the transport mechanism in this pump, the serious disagreements among the three published crystallographic structures of L have remained unresolved. Here, we report on the X-ray diffraction structure of the L state, to 1.53-1.73 A resolutions, from replicate data sets collected from six independent crystals. Unlike earlier studies, the partial occupancy refinement uses diffraction intensities from the same crystals before and after the illumination to produce the trapped L state. The high reproducibility of inter-atomic distances, and bond angles and torsions of the retinal, lends credibility to the structural model. The photoisomerized 13-cis retinal in L is twisted at the C(13)=C(14) and C(15)=NZ double-bonds, and the Schiff base does not lose its connection to Wat402 and, therefore, to the proton acceptor Asp85. The protonation of Asp85 by the Schiff base in the L-->M reaction is likely to occur, therefore, via Wat402. It is evident from the structure of the L state that various conformational changes involving hydrogen-bonding residues and bound water molecules begin to propagate from the retinal to the protein at this stage already, and in both extracellular and cytoplasmic directions. Their rationales in the transport can be deduced from the way their amplitudes increase in the intermediates that follow L in the reaction cycle, and from the proton transfer reactions with which they are associated.     

Coupling of retinal, protein, and water dynamics in squid rhodopsin

The light-induced isomerization of the retinal from 11-cis to all-trans triggers changes in the conformation of visual rhodopsins that lead to the formation of the activated state, which is ready to interact with the G protein. To begin to understand how changes in the structure and dynamics of the retinal are transmitted to the protein, we performed molecular dynamics simulations of squid rhodopsin with 11-cis and all-trans retinal, and with two different force fields for describing the retinal molecule. The results indicate that structural rearrangements in the binding pocket, albeit small, propagate toward the cytoplasmic side of the protein, and affect the dynamics of internal water molecules. The sensitivity of the active-site interactions on the retinal force-field parameters highlights the coupling between the retinal molecule and its immediate protein environment.     

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.