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

SERS detection of microRNA biomarkers for cancer diagnosis using gold-coated paramagnetic nanoparticles to capture SERS-active gold nanoparticles

A highly sensitive magnetic-capture SERS assay for detecting cancer-related microRNAs was developed by enhancing the formation of SERS “hot spots”.

Cholesterol in the rod outer segment: A complex role in a "simple" system

The rod outer segment (ROS) of retinal photoreceptor cells consists of disk membranes surrounded by the plasma membrane. It is a relatively uncomplicated system in which to investigate cholesterol distribution and its functional consequences in biologically relevant membranes. The light sensitive protein, rhodopsin is the major protein in both membranes, but the lipid compositions are significantly different in the disk and plasma membranes. Cholesterol is high in the ROS plasma membrane. Disk membranes are synthesized at the base of the ROS and are also high in cholesterol. However, cholesterol is rapidly depleted as the disks are apically displaced. During this apical displacement the disk phospholipid fatty acyl chains become progressively more unsaturated, which creates an environment unfavorable to cholesterol. Membrane cholesterol has functional consequences. The high cholesterol found in the plasma membrane and in newly synthesized disks inhibits the activation of rhodopsin. As disks are apically displaced and cholesterol is depleted rhodopsin becomes more responsive to light. This effect of cholesterol on rhodopsin activation has been shown in both native and reconstituted membranes. The modulation of activity can be at least partially explained by the effect of cholesterol on bulk lipid properties. Cholesterol decreases the partial free volume of the hydrocarbon region of the bilayer and thereby inhibits rhodopsin conformational changes required for activation. However, cholesterol binds to rhodopsin and may directly affect the protein also. Furthermore, cholesterol stabilizes rhodopsin to thermal denaturation. The membrane must provide an environment that allows rhodopsin conformational changes required for activation while also stabilizing the protein to thermal denaturation. Cholesterol thus plays a complex role in modulating the activity and stability of rhodopsin, which have implications for other G-protein coupled receptors.

Sparse and incomplete factorial matrices to screen membrane protein 2D crystallization

Electron crystallography is well suited for studying the structure of membrane proteins in their native lipid bilayer environment. This technique relies on electron cryomicroscopy of two-dimensional (2D) crystals, grown generally by reconstitution of purified membrane proteins into proteoliposomes under conditions favoring the formation of well-ordered lattices. Growing these crystals presents one of the major hurdles in the application of this technique. To identify conditions favoring crystallization a wide range of factors that can lead to a vast matrix of possible reagent combinations must be screened. However, in 2D crystallization these factors have traditionally been surveyed in a relatively limited fashion. To address this problem we carried out a detailed analysis of published 2D crystallization conditions for 12 β-barrel and 138 α-helical membrane proteins. From this analysis we identified the most successful conditions and applied them in the design of new sparse and incomplete factorial matrices to screen membrane protein 2D crystallization. Using these matrices we have run 19 crystallization screens for 16 different membrane proteins totaling over 1300 individual crystallization conditions. Six membrane proteins have yielded diffracting 2D crystals suitable for structure determination, indicating that these new matrices show promise to accelerate the success rate of membrane protein 2D crystallization.

Mercury-induced dark-state instability and photobleaching alterations of the visual g-protein coupled receptor rhodopsin

Mercuric compounds were previously shown to affect the visual phototransduction cascade, and this could result in vision impairment. We have analyzed the effect of mercuric chloride on the structure and stability of the dim light vision photoreceptor rhodopsin. For this purpose, we have used both native rhodopsin immunopurified from bovine retinas and a recombinant mutant rhodopsin carrying several Cys to Ser substitutions in order to investigate the potential binding site of mercury on the receptor. Our results show that mercuric chloride dramatically reduces the stability of dark-state rhodopsin and alters the molecular features of the photoactived conformation obtained upon illumination by eliciting the formation of an altered photointermediate. The thermal bleaching kinetics of native and mutant rhodopsin is markedly accelerated by mercury in a concentration-dependent manner, and its chromophore regeneration ability is severely reduced without significantly affecting its G-protein activation capacity. Furthermore, fluorescence spectroscopic measurements on the retinal release process, ensuing illumination, suggest that mercury impairs complete retinal release from the receptor binding pocket. Our results provide further support for the capacity of mercury as a hazardous metal ion with reported deleterious effect on vision and provide a molecular explanation for such an effect at the rhodopsin photoreceptor level. We suggest that mercury could alter vision by acting in a specific manner on the molecular components of the retinoid cycle, particularly by modifying the ability of the visual photoreceptor protein rhodopsin to be regenerated and to be normally photoactivated by light.

Agonist-dependent phosphorylation of the formyl peptide receptor is regulated by the membrane proximal region of the cytoplasmic tail

Formyl peptide receptor (FPR) is a chemoattractant G protein-coupled receptor (GPCR) involved in the innate immune response against bacteria. Receptor activation is terminated by receptor phosphorylation of two serine- and threonine-rich regions located in the distal half of the cytoplasmic tail. In this study we show that introduction of an amino acid with a bulky side chain (leucine or glutamine) adjacent to a single leucine, L320, in the membrane-proximal half of the cytoplasmic tail, significantly enhanced receptor phosphorylation, beta-arrestin1/2 translocation, and receptor endocytosis, without affecting G(i)-mediated ERK1/2 activation and release of intracellular calcium. In addition, the point mutations resulted in diminished susceptibility to trypsin, suggesting a conformation different from that of wild type FPR. Alignment of the FPR sequence with the rhodopsin sequence showed that L320 resides immediately C-terminal of an amphipathic region that in rhodopsin forms helix 8. Deletion of seven amino acids (Delta309-315) from the predicted helix 8 of FPR (G307-S319) caused reduced cell signaling as well as defects in receptor phosphorylation, beta-arrestin1/2 translocation and endocytosis. Thus, the amino acid content in the N-terminal half of the cytoplasmic tail influences the structure and desensitization of FPR.

Projection maps of three members of the KdgM outer membrane protein family

We present the projection structures of the three outer membrane porins KdgM and KdgN from Erwinia chrysanthemi and NanC from Escherichia coli, based on 2D electron crystallography. A wide screening of 2D crystallization conditions yielded tubular crystals of a suitable size and quality to perform high-resolution electron microscopy. Data processing of untilted samples allowed us to separate the information of the two crystalline layers and resulted in projection maps to a resolution of up to 7A. All three proteins exhibit a similar putative beta-barrel structure and the three crystal forms have the same symmetry. However, there are differences in the packing arrangements of the monomers as well as the densities of the projections. To interpret these projections, secondary structure prediction was performed using beta-barrel specific prediction algorithms. The predicted transmembrane beta-barrels have a high similarity in the arrangement of the putative beta-strands and the loops, but do not match those of OmpG, a related protein porin whose structure was solved.

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.

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.

G protein-coupled receptor rhodopsin: a prospectus

Rhodopsin is a retinal photoreceptor protein of bipartite structure consisting of the transmembrane protein opsin and a light-sensitive chromophore 11-cis-retinal, linked to opsin via a protonated Schiff base. Studies on rhodopsin have unveiled many structural and functional features that are common to a large and pharmacologically important group of proteins from the G protein-coupled receptor (GPCR) superfamily, of which rhodopsin is the best-studied member. In this work, we focus on structural features of rhodopsin as revealed by many biochemical and structural investigations. In particular, the high-resolution structure of bovine rhodopsin provides a template for understanding how GPCRs work. We describe the sensitivity and complexity of rhodopsin that lead to its important role in vision.

Light-induced changes in the structure and accessibility of the cytoplasmic loops of rhodopsin in the activated MII state

Bovine rhodopsin was specifically labeled on the cytoplasmic surface at cysteine 140 (the first residue of the loop connecting helices III and IV) or at cysteine 316 (in the loop connecting helix VII and the palmitoylation sites) with the fluorescent labels fluorescein and Texas Red. These loops are involved in activation and signal transduction. The time-resolved fluorescence depolarization was measured in the dark state and in the M(II) state, with labeled samples consisting of rhodopsin-octylglucoside micelles or rod outer segment (ROS) membranes. In this way the diffusional dynamics of the flexible loops of rhodopsin were measured for the first time directly on the nanosecond time scale. Control experiments showed that the large number of weak excitation pulses required in these single photon counting experiments leads to <5% bleaching of the sample. Rhodopsin was trapped in the activated M(II) state for the duration of the fluorescence experiments ( approximately 20 min) after illumination at pH 6 and 5 degrees C. For both types of samples and at both labeled positions the dynamics of the label and loop motion as monitored by the time constants of the depolarization were not significantly different in the two states of the receptor. The end-anisotropy increased, however, from 0.09 in the dark to 0.16 in the M(II) state for ROS samples labeled at C140. The corresponding numbers for the C316 position are 0.06 and 0.12. Light-induced activation in M(II) is thus associated with a large increase in the loop steric hindrance due to a changed loop domain structure on the cytoplasmic surface. These results are supported by fluorescence quenching experiments with I(-), which indicate a significant decrease in the collisional quenching constant k(q) and in accessibility in the M(II) state at both positions. The rotational correlation time of the rhodopsin micelles increased from 48 ns in the dark state to 60 ns in M(II). This increase is caused by a change in volume and/or shape and is consistent with a structural change. These results demonstrate that time-resolved fluorescence depolarization is a powerful tool to study the changes in conformation and dynamics of the cytoplasmic loops that accompany the activation of rhodopsin and other G-protein coupled receptors.