Urea unfolding of opsin in phospholipid bicelles.

Opsin is the unstable apo-protein of the light-activated G protein-coupled receptor rhodopsin. We investigated the stability of bovine opsin, solubilized in 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC)/detergent bicelles, against urea-induced unfolding. A single irreversible protein unfolding transition was observed from changes in intrinsic tryptophan fluorescence and far-UV circular dichroism. This unfolding transition correlated with loss of protein activity. Changes in tertiary structure, as indicated by fluorescence measurements, were concomitant with an approximate 50% reduction in alpha-helical content of opsin, indicating that global unfolding had been induced by urea. The urea concentration at the midpoint of unfolding was dependent on the lipid/detergent environment, occurring at approximately 1.2 m urea in DMPC/1,2-dihexanoyl-sn-glycero-3-phosphocholine bicelles, while being significantly stabilized to approximately 3.5 m urea in DMPC/3-[(cholamidopropyl)dimethylammonio]-1-propanesulfonate bicelles. These findings demonstrate that interactions with the surrounding lipids and detergent are highly influential in the unfolding of membrane protein structure. The urea/bicelle system offers the possibility for a more detailed understanding of the structural changes that take place upon irreversible unfolding of opsin.

Opsin stability and folding: modulation by phospholipid bicelles.

Integral membrane proteins do not fare well when extracted from biological membranes and are unstable or lose activity in detergents commonly used for structure and function investigations. We show that phospholipid bicelles provide a valuable means of preserving alpha-helical membrane proteins in vitro by supplying a soluble lipid bilayer fragment. Both 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC)/3-[(cholamidopropyl)dimethyl-ammonio]-1-propane sulfonate (Chaps) and DMPC/l-alpha-1,2-dihexanoyl-sn-glycero-3-phosphocholine (DHPC) bicelles dramatically increase the stability of the mammalian vision receptor rhodopsin as well as its apoprotein, opsin. Opsin is particularly unstable in detergent solution but can be directly purified into DMPC/Chaps. We show that opsin can also be directly purified in DMPC/DHPC bicelles to give correctly folded functional opsin, as shown by the ability to regenerate rhodopsin to approximately 70% yield. These well-characterised DMPC/DHPC bicelles enable us to probe the influence of bicelle properties on opsin stability. These bicelles are thought to provide DMPC bilayer fragments with most DHPC capping the bilayer edge, giving a soluble bilayer disc. Opsin stability is shown to be modulated by the q value, the ratio of DMPC to DHPC, which reflects changes in the bicelle size and, thus, proportion of DMPC bilayer present. The observed changes in stability also correlate with loss of opsin secondary structure as determined by synchrotron far-UV circular dichroism spectroscopy; the most stable bicelle results in the least helix loss. The inclusion of Chaps rather than DHPC in the DMPC/Chaps bicelles, however, imparts the greatest stability. This suggests that it is not just the DMPC bilayer fragment in the bicelles that stabilises the protein, but that Chaps provides additional stability either through direct interaction with the protein or by altering the DMPC/Chaps bilayer properties within the bicelle. The significant stability enhancements and preservation of secondary structure reported here in bicelles are pertinent to other membrane proteins, notably G-protein-coupled receptors, which are unstable in detergent solution.

Opsin stability and folding: the role of Cys185 and abnormal disulfide bond formation in the intradiscal domain.

The structure in the extracellular, intradiscal domain of rhodopsin surrounding the Cys110-Cys187 disulfide bond has been shown to be important for correct folding of this receptor in vivo. Retinitis pigmentosa misfolding mutants of the apoprotein opsin (such as P23H) misfold, as defined by a deficiency in ability to bind 11-cis retinal and form rhodopsin. These mutants also possess an abnormal Cys185-Cys187 disulfide bond in the intradiscal domain. Here, by mutating Cys185 to alanine, we eliminate the possibility of forming this abnormal disulfide bond and investigate the effect of combining the C185A mutation with the retinitis pigmentosa mutation P23H. Both the P23H and P23H/C185A double mutant suffer from low expression and poor 11-cis retinal binding. Our data suggest that misfolding events occur that do not have an absolute requirement for abnormal Cys185-Cys187 disulfide bond formation. In the detergent-solubilised, purified state, the C185A mutation allows formation of rhodopsin at wild-type (WT) levels, but has interesting effects on protein stability. C185A rhodopsin is less thermally stable than WT, whereas C185A opsin shows the same ability to regenerate rhodopsin in detergent as WT. Purified C185A and WT opsins, however, have contrasting 11-cis retinal binding kinetics. A high proportion of C185A opsin binds 11-cis retinal with a slow rate that reflects a denatured state of opsin reverting to a fast-binding, open-pocket conformation. This slower rate is not observed in a stabilising lipid/detergent system, 1,2-dimyristoyl-sn-glycero-3-phosphocholine/Chaps, in which C185A exhibits WT (fast) retinal binding. We propose that the C185A mutation destabilises the open-pocket conformation of opsin in detergent resulting in an equilibrium between correctly folded and denatured states of the protein. This equilibrium can be driven towards the correctly folded rhodopsin state by the binding of 11-cis retinal.

Rhodopsin photointermediates in two-dimensional crystals at physiological temperatures.

Bovine rhodopsin photointermediates formed in two-dimensional (2D) rhodopsin crystal suspensions were studied by measuring the time-dependent absorbance changes produced after excitation with 7 ns laser pulses at 15, 25, and 35 degrees C. The crystalline environment favored the Meta I(480) photointermediate, with its formation from Lumi beginning faster than it does in rhodopsin membrane suspensions at 35 degrees C and its decay to a 380 nm absorbing species being less complete than it is in the native membrane at all temperatures. Measurements performed at pH 5.5 in 2D crystals showed that the 380 nm absorbing product of Meta I(480) decay did not display the anomalous pH dependence characteristic of classical Meta II in the native disk membrane. Crystal suspensions bleached at 35 degrees C and quenched to 19 degrees C showed that a rapid equilibrium existed on the approximately 1 s time scale, which suggests that the unprotonated predecessor of Meta II in the native membrane environment (sometimes called MII(a)) forms in 2D rhodopsin crystals but that the non-Schiff base proton uptake completing classical Meta II formation is blocked there. Thus, the 380 nm absorbance arises from an on-pathway intermediate in GPCR activation and does not result from early Schiff base hydrolysis. Kinetic modeling of the time-resolved absorbance data of the 2D crystals was generally consistent with such a mechanism, but details of kinetic spectral changes and the fact that the residuals of exponential fits were not as good as are obtained for rhodopsin in the native membrane suggested the photoexcited samples were heterogeneous. Variable fractional bleach due to the random orientation of linearly dichroic crystals relative to the linearly polarized laser was explored as a cause of heterogeneity but was found unlikely to fully account for it. The fact that the 380 nm product of photoexcitation of rhodopsin 2D crystals is on the physiological pathway of receptor activation suggests that determination of its structure would be of interest.

Structure of bovine rhodopsin in a trigonal crystal form.

We have determined the structure of bovine rhodopsin at 2.65 A resolution using untwinned native crystals in the space group P3(1), by molecular replacement from the 2.8 A model (1F88) solved in space group P4(1). The new structure reveals mechanistically important details unresolved previously, which are considered in the membrane context by docking the structure into a cryo-electron microscopy map of 2D crystals. Kinks in the transmembrane helices facilitate inter-helical polar interactions. Ordered water molecules extend the hydrogen bonding networks, linking Trp265 in the retinal binding pocket to the NPxxY motif near the cytoplasmic boundary, and the Glu113 counterion for the protonated Schiff base to the extracellular surface. Glu113 forms a complex with a water molecule hydrogen bonded between its main chain and side-chain oxygen atoms. This can be expected to stabilise the salt-bridge with the protonated Schiff base linking the 11-cis-retinal to Lys296. The cytoplasmic ends of helices H5 and H6 have been extended by one turn. The G-protein interaction sites mapped to the cytoplasmic ends of H5 and H6 and a spiral extension of H5 are elevated above the bilayer. There is a surface cavity next to the conserved Glu134-Arg135 ion pair. The cytoplasmic loops have the highest temperature factors in the structure, indicative of their flexibility when not interacting with G protein or regulatory proteins. An ordered detergent molecule is seen wrapped around the kink in H6, stabilising the structure around the potential hinge in H6. These findings provide further explanation for the stability of the dark state structure. They support a mechanism for the activation, initiated by photo-isomerisation of the chromophore to its all-trans form, that involves pivoting movements of kinked helices, which, while maintaining hydrophobic contacts in the membrane interior, can be coupled to amplified translation of the helix ends near the membrane surfaces.

Crystals of native and modified bovine rhodopsins and their heavy atom derivatives.

Rhodopsin, the pigment protein responsible for dim-light vision, is a G protein-coupled receptor that converts light absorption into the activation of a G protein, transducin, to initiate the visual response. We have crystallised detergent-solubilised bovine rhodopsin in the native form and after chemical modifications as needles 10-40 microm in cross-section. The crystals belong to the trigonal space group P3(1), with two molecules of rhodopsin per asymmetric unit, related by a non-crystallographic 2-fold axis parallel with the crystallographic screw axis along c (needle axis). The unit cell dimensions are a=103.8 A, c=76.6 A for native rhodopsin, but vary over a wide range after heavy atom derivatisation, with a between 101.5 A and 113.9 A, and c between 76.6 A and 79.2 A. Rhodopsin molecules are packed with the bundle of transmembrane helices tilted from the c-axis by about 100 degrees . The two molecules in the asymmetric unit form contacts along the entire length of their transmembrane helices 5 in an antiparallel orientation, and they are stacked along the needle axis according to the 3-fold screw symmetry. Hence hydrophobic contacts are prominent at protein interfaces both along and normal to the needle axis. The best crystals of native rhodopsin in this crystal form diffracted X-rays from a microfocused synchrotron source to 2.55 A maximum resolution. We describe steps taken to extend the diffraction limit from about 10 A to 2.6 A.

Electron crystallography reveals the structure of metarhodopsin I.

Rhodopsin is the prototypical G protein-coupled receptor, responsible for detection of dim light in vision. Upon absorption of a photon, rhodopsin undergoes structural changes, characterised by distinct photointermediates. Currently, only the ground-state structure has been described. We have determined a density map of a photostationary state highly enriched in metarhodopsin I, to a resolution of 5.5 A in the membrane plane, by electron crystallography. The map shows density for helix 8, the cytoplasmic loops, the extracellular plug, all tryptophan residues, an ordered cholesterol molecule and the beta-ionone ring. Comparison of this map with X-ray structures of the ground state reveals that metarhodopsin I formation does not involve large rigid-body movements of helices, but there is a rearrangement close to the bend of helix 6, at the level of the retinal chromophore. There is no gradual build-up of the large conformational change known to accompany metarhodopsin II formation. The protein remains in a conformation similar to that of the ground state until late in the photobleaching process.

Rhodopsin photoproducts in 2D crystals.

The published electron microscope and X-ray structures of rhodopsin have made available a detailed picture of the inactive dark state of rhodopsin. Yet, the photointermediates of rhodopsin that ultimately lead to the activated receptor species still await a similar analysis. Such an analysis first requires the generation and characterization of the photoproducts that can be obtained in crystals of rhodopsin. We therefore studied with Fourier-transform infrared (FTIR) difference spectroscopy the photoproducts in 2D crystals of bovine rhodopsin in a p22(1)2(1) crystal form. The spectra obtained by cryotrapping revealed that in this crystal form the still inactive early intermediates batho, lumi, and meta I are similar to those obtained from rhodopsin in native disk membranes, although the transition from lumi to meta I is shifted to a higher temperature. However, at room temperature, the formation of the active state, meta II, is blocked in the crystalline environment. Instead, an intermediate state is formed that bears some features of meta II but lacks the specific conformational changes required for activity. Despite being unable to activate its cognate G protein, transducin, to a significant extent, this intermediate state is capable of interacting with functional transducin-derived peptides to a limited extent. Therefore, while unable to support formation of rhodopsin's active state meta II, 2D p22(1)2(1) crystals proved to be very suitable for determining 3D structures of its still inactive precursors, batho, lumi, and meta I. In future studies, FTIR spectroscopy may serve as a sensitive assay to screen crystals grown under altered conditions for potential formation of the active state, meta II.

The three-dimensional structure of bovine rhodopsin determined by electron cryomicroscopy.

G-protein-coupled receptors are integral membrane proteins that respond to environmental signals and initiate signal transduction pathways, which activate cellular processes. Rhodopsin, a well known member of the G-protein-coupled receptor family, is located in the disk membranes of the rod outer segment, where it is responsible for the visualization of dim light. Rhodopsin is the most extensively studied G-protein-coupled receptor, and knowledge about its structure serves as a template for other related receptors. We have gained detailed structural knowledge from the crystal structure (1), which was solved by x-ray crystallography in 2000 using three-dimensional crystals. Here we report a three-dimensional density map of bovine rhodopsin determined by electron cryomicroscopy of two-dimensional crystals with p22(1)2(1) symmetry. The usage of relatively small and disordered crystals made the process of structure determination challenging. Special attention was paid to the extraction of amplitudes and phases, since usable raw data were limited to a maximum tilt of 45 degrees. In the refinement process, an improved unbending procedure was applied. This led to a final resolution of 5.5 A in the membrane plane and approximately 13 A perpendicular to it, making our electron density map the most accurate map of a G-protein-coupled receptor currently available by electron microscopy. Most important is the information we gain about the center of the membrane plane and the orientation of the molecule relative to the bilayer. This information cannot be retrieved from the three-dimensional crystals. In our electron density map, all seven transmembrane helices were identified, and their arrangement is in agreement with the arrangement known from the crystal structure (1). In the retinal binding pocket, a density peak adjacent to helix 3 suggests the position of the beta-ionine ring of the chromophore, and in its vicinity several of the bigger amino acids can be identified.

X-ray diffraction of heavy-atom labelled two-dimensional crystals of rhodopsin identifies the position of cysteine 140 in helix 3 and cysteine 316 in helix 8.

We have used site-specific heavy-atom labelling and X-ray diffraction to localize single amino acid residues in the cytoplasmic domain of the integral membrane protein rhodopsin, the dim-light photoreceptor of retinal vertebrate rod cells. Two-dimensional orthorhombic crystals of the space group p22(1)2(1) (a=59.5(+/-1) A and b=82.7(+/-1.5) A) were produced from detergent-solubilized, partially delipidated rhodopsin. To obtain milligram amounts of two-dimensional crystals, which are required for X-ray diffraction, the yield of the crystalline material was significantly increased by reconstitution of rhodopsin in the presence of cholesterol (1:2 to 1:10 mol/mol) and by adding polar organic solvents to the dialysis buffer. The native cysteine residues C140 and C316 were then selectively labelled with mercury using the sulphydryl-specific reagent p-chloromercuribenzoate (1.6-2.1 mol Hg per mol rhodopsin). The labelling did not affect the unit cell dimensions. Optical absorption spectra of labelled and native two-dimensional rhodopsin crystals showed the characteristic 11-cis-retinal peak at 498 nm, which corresponds to the dark state of rhodopsin. The in-plane position of the mercury label was calculated at 9.5 A resolution from the intensity differences in the X-ray diffraction patterns of labelled and native crystals using Fourier difference methods and the phase information from electron crystallography. The label positions were in excellent agreement with the positions of C140 at the cytoplasmic end of helix 3 and of C316 in the cytoplasmic helix 8 recently obtained from three-dimensional rhodopsin crystals. Whereas these high-resolution diffraction studies were performed under cryogenic conditions (100 K), our results were obtained at room temperature with fully hydrated membranes and in the absence of loop-loop crystal contacts. To study the structural changes of the cytoplasmic loops involved in activation and signal transduction, our more physiological conditions offer important advantages. Furthermore, the localization of C316 is the first direct proof that the electron density on top of helix 1 observed by cryo-electron microscopy is a part of the C-terminal loop. Our approach is of particular interest for investigations of other membrane proteins, for which 3D crystals are not available. Structural constraints from heavy-atom labels at strategic sites enable the assignment of a position in the amino acid sequence to features visible in a low-resolution density map and the study of conformational changes associated with different functional states of the membrane protein.