Conformational changes in sensory rhodopsin I: similarities and differences with bacteriorhodopsin, halorhodopsin, and rhodopsin

FTIR difference spectra have been obtained for the sR587----S373 phototransition of sensory rhodopsin I (sR-I), a signal-transducing protein of Halobacterium halobium. The vibrational modes of the sR587 chromophore have frequencies close to those of the bacteriorhodopsin bR568 chromophore, confirming that the two chromophores have very similar structures and environments. However, the sR-I Schiff base C = N stretch frequency is downshifted relative to bR, consistent with weaker hydrogen bonding with its counterion(s). The carboxyl (COOH) stretch modes of sR-I and halorhodopsin (hR) are at the same frequencies. On the basis of sequence homologies, these bands can be assigned to Asp-106 in helix D and/or Asp-201 in helix G. In contrast, no band was found that could be assigned to the protonation of Asp-76. In bR, the homologous residue Asp-85 serves as the acceptor group for the Schiff base proton. Bands appear in the amide I and II regions at similar frequencies in sR-I, hR, and bR, indicating that despite their different functions they all undergo closely related structural changes. Bands are also detected in the C-H stretch region, possibly due to alterations in the membrane lipids. Similar spectral features are also observed in the lipids of rhodopsin-containing photoreceptor membrane upon light activation.     

Modeling of halorhodopsin and rhodopsin based on bacteriorhodopsin

Bacteriorhodopsin (BR), halorhodopsin (HR), and rhodopsin (Rh) all belong to the class of seven-helix membrane proteins. For BR, a structural model at atomic resolution is available; for HR, diffraction data are available only down to a resolution of 6 Å in the membrane plane, and for Rh, down to 9 Å. BR and HR are closely related proteins with a sequence homology of 34%, while Rh does not share any sequence homology with BR. An atomic model for HR is derived that is based on sequence alignment and the atomic model for BR and is improved by molecular dynamics simulations. The model structure obtained accounts well for the experimentally observed difference between HR and BR in the projection map, where HR exhibits a higher density in the region between helices D and E. The reason for this difference lies partially in the different side chains and partially in slightly different helix tilts. The scattering amplitudes and phases of the model structure are calculated and agree with the experimental data down to a resolution of about 8 Å. If the helix positions are adopted from the projection map for HR and used as input in the model, this number improves to 7 Å. Analogously, an atomic model for Rh is derived based on the atomic model for BR and subjected to molecular dynamics simulations. Optimal agreement with the experimental projection map for Rh is obtained when the entire model structure is rotated slightly about two axes in the membrane plane. The agreement with the experimental projection map is not as satisfactory as for HR, but the results indicate that even for a nonhomologous, but structurally related, protein such as Rh, an acceptable model structure can be derived from the structure of BR. © 1996 Wiley-Liss, Inc.     

Surface-enhanced Raman spectroscopy of biopolymers: membrane proteins, bacteriorhodopsin and rhodopsin adsorbed on silver electrodes and silver hydrosols

Surface-enhanced Raman (SER) spectra of purple membranes of Halobacterium halobium and photoreceptor disks of the rod outer segments adsorbed on silver hydrosols were analysed. It has been shown that the intensity of SER spectra of bacterial and visual rhodopsins increases 5 X 10(4) times at adsorption. Concentration relationship of the signal intensity of SER spectra has the maximum at bacteriorhodopsin concentration about 2 X 10(-7) M. It has been shown that adsorption on silver hydrosol leads to fixation of light-induced photochemical transformations in bacterial and visual rhodopsins. Adsorption on the "smooth" electrodes at the potential of the zero charge of silver does not affect the photocycle of bacteriorhodopsin. An increase or decrease of the electrode potential relative to the zero charge point of silver leads to the accumulation of kinetic intermediate K610 and a decrease of the concentration of the form BRh570. It has been shown that on the "smooth" electrode primarily the long-range component of the SER mechanism is realized. Bands corresponding to the vibrations of the atom groups directly contacting with the metal are mainly intensified after redox cycle which increases the concentration of chemosorption centres. A conclusion is drawn that the method of SER spectroscopy of biomolecules adsorbed on "smooth" electrodes, permits obtaining information similar to that obtained from the analysis of Raman spectra of unadsorbed molecules, but at concentrations by two orders less. Adsorption on the electrodes treated with the help of redox cycle permits to obtain highly oriented preparations and to study topography of biopolymers in water solutions and suspensions.     

Interdisciplinary biophysical studies of membrane proteins bacteriorhodopsin and rhodopsin

The centenary of the birth of H. Gobind Khorana provides an auspicious opportunity to review the origins and evolution of parallel advances in biophysical methodology and molecular genetics technology used to study membrane proteins. Interdisciplinary work in the Khorana laboratory in the late 1970s and for the next three decades led to productive collaborations and fostered three subsequent scientific generations whose biophysical work on membrane proteins has led to detailed elucidation of the molecular mechanisms of energy transduction by the light-driven proton pump bacteriorhodopsin (bR) and signal transduction by the G protein–coupled receptor (GPCR) rhodopsin. This review will highlight the origins and advances of biophysical studies of membrane proteins made possible by the application of molecular genetics approaches to engineer site-specific alterations of membrane protein structures.     

Circular dichroism of halorhodopsin: comparison with bacteriorhodopsin and sensory rhodopsin I

Circular dichroic (CD) spectra of three related protein pigments from Halobacterium halobium, halorhodopsin (HR), bacteriorhodopsin (BR), and sensory rhodopsin I (SR-I), are compared. In native membranes the two light-driven ion pumps, HR and BR, exhibit bilobe circular dichroism spectra characteristic of exciton splitting in the region of retinal absorption, while the phototaxis receptor, SR-I, exhibits a single positive band centered at the SR-I absorbance maximum. This indicates specific aggregation of protein monomers of HR, as previously noted [Sugiyama, Y., & Mukohata, Y. (1984) J. Biochem. (Tokyo) 96, 413-420], similar to the well-characterized retinal/retinal exciton interaction in the purple membrane. The absence of this interaction in SR-I indicates SR-I is present in the native membrane as monomers or that interactions between the retinal chromophores are weak due to chromophore orientation or separation. Solubilization of HR and BR with nondenaturing detergents eliminates the exciton coupling, and the resulting CD spectra share similar features in all spectral regions from 250 to 700 nm. Schiff-base deprotonation of both BR and HR yields positive CD bands near 410 nm and shows similar fine structure in both pigments. Removal of detergent restores the HR native spectrum. HR differs from BR in that circular dichroic bands corresponding to both amino acid and retinal environments are much more sensitive to external salt concentration and pH. A theoretical analysis of the exciton spectra of HR and BR that provides a range of interchromophore distances and orientations is performed.(ABSTRACT TRUNCATED AT 250 WORDS)     

Sensory rhodopsin II and bacteriorhodopsin: light activated helix F movement.

EPR spectroscopy in combination with site directed spin labeling (SDSL) has become a valuable tool for structural investigations as well as for kinetic studies on proteins. This method has been especially useful for membrane proteins in yielding structural and functional data. This information is not easily available from other techniques, like, e.g., X-ray crystallography or electron microscopy. In the first part of this two part review, the topology of the sensory rhodopsin II/transducer complex (NpSRII/NpHtrII) derived from EPR constraints is compared to that obtained from X-ray crystallography. In the second part, the helix F movement observed for both sensory rhodopsin and bacteriorhodopsin is evaluated and discussed in order to establish a common mechanism after photoreceptor activation.     

Matrix-assisted laser desorption mass spectrometry of rhodopsin and bacteriorhodopsin.

Matrix-assisted laser desorption ionization (MALDI) mass spectrometry has been used to obtain accurate molecular weight information for the integral membrane proteins bacteriorhodopsin and bovine rhodopsin desorbed from solubilized membrane preparations. Mass differences in the molecular weights measured for bleached and unbleached bacteriorhodopsin and rhodopsin indicate the removal of the retinal chromophores upon bleaching. The MALDI technique was also successful for determination of the major cleavage products obtained upon treatment of membrane bound rhodopsin with endoproteinase Asp-N and thermolysin. Our results indicate that the MALDI method is a useful means of obtaining accurate molecular weight information on hydrophobic proteins isolated in their native membranes.     

Arteriogenesis versus angiogenesis: similarities and differences

Cardiovascular diseases account for more than half of total mortality before the age of 75 in industrialized countries. To develop therapies promoting the compensatory growth of blood vessels could be superior to palliative surgical interventions. Therefore, much effort has been put into investigating underlying mechanisms. Depending on the initial trigger, growth of blood vessels in adult organisms proceeds via two major processes, angiogenesis and arteriogenesis. While angiogenesis is induced by hypoxia and results in new capillaries, arteriogenesis is induced by physical forces, most importantly fluid shear stress. Consequently, chronically elevated fluid shear stress was found to be the strongest trigger under experimental conditions. Arteriogenesis describes the remodelling of pre-existing arterio-arteriolar anastomoses to completely developed and functional arteries. In both growth processes, enlargement of vascular wall structures was proposed to be covered by proliferation of existing wall cells. Recently, increasing evidence emerges, implicating a pivotal role for circulating cells, above all blood monocytes, in vascular growth processes. Since it has been shown that monocytes/ macrophage release a cocktail of chemokines, growth factors and proteases involved in vascular growth, their contribution seems to be of a paracrine fashion. A similar role is currently discussed for various populations of bone-marrow derived stem cells and endothelial progenitors. In contrast, the initial hypothesis that these cells -after undergoing a (trans-)differentiation- contribute by a structural integration into the growing vessel wall, is increasingly challenged.     

Chromophore motion during the bacteriorhodopsin photocycle: polarized absorption spectroscopy of bacteriorhodopsin and its M-state in bacteriorhodopsin crystals.

The three-dimensional crystallization of bacteriorhodopsin was systematically investigated and the needle-shaped crystal form analysed. In these crystals the M-intermediate forms 10 times faster and decays 15 times more slowly than in purple membranes. Polarized absorption spectra of the crystals were measured in the dark and light adapted states. A slight decrease in the angle between the transition moment and the membrane plane was detected during dark adaptation. The crystallization of a mutated bacteriorhodopsin, in which the aspartic acid at residue 96 was replaced by asparagine, provided crystals with a long lived M-intermediate. This allowed polarized absorption measurements of the M-chromophore. The change in the polarization ratio upon formation of the M-intermediate indicates an increase in the angle between the main transition dipole and the membrane plane by 2.2 degrees +/- 0.5, corresponding to a 0.5 A displacement of one end of the chromophore out of the membrane plane of the bacteriorhodopsin molecule.     

Photoacoustic spectroscopy of bacteriorhodopsin photocycle

Photoacoustic spectroscopy was applied to study the energetics and the kinetics of the slow intermediates of the bacteriorhodopsin photocycle. An analysis of the modulation frequency dependence of the photoacoustic signal allowed us to estimate the enthalpy changes and the kinetic parameters associated with those intermediates. The effects of pH, salt concentration, and protein aggregation were studied. Three photoacoustic transitions were found. The two low frequency transitions were attributed to O660 and M412, respectively. The third transition was interpreted as resulting from a protein conformational change undetected spectrophotometrically. The frequency spectra were simulated between 5 and 180 Hz at pH's 5.1, 7.0, and 8.9 assuming a branching in the bacteriorhodopsin photocycle at the M412 level. The enthalpy changes associated with M412 and O660 were computed and compared with the experimental values.     

Pair distribution functions of bacteriorhodopsin and rhodopsin in model bilayers.

The pair distribution functions have been measured from freeze-fracture pictures of bacteriorhodopsin and rhodopsin recombinants with diacyl phosphatidylcholines (PC) of various hydrocarbon chain lengths. Pictures were used of samples that had been frozen from above the phase transition temperature of the lipid. Measured functions were compared with those calculated from two model interparticle potential energy functions, (a) a hard-disk repulsion only, and (b) a hard-disk repulsion plus electrostatic repulsion for a point charge buried in the membrane. The measured functions for bacteriorhodopsin di 12:0 PC, di 14:0 PC, and di 16:0 PC recombinants can be simulated using an interparticle hard-disk repulsion only. Bleached rhodopsin di 12:0 PC and di 18:1 trans-PC recombinants, and dark-adapted rhodopsin di 10:0 PC recombinants yield functions that are better simulated by assuming an additional repulsive interaction. The measured functions resemble those calculated using the hard-disk plus electrostatic repulsion model. The picture of dark-adapted rhodopsin in di 18:1 trans-PC frozen from 20 degrees C shows partial aggregation that is apparent in the measured pair distribution function. This attractive interaction persists even at 37 degrees C, where the measured function shows deviations from the hard-disk repulsive model, indicative of an attractive interparticle interaction. Implications of these results are discussed in terms of protein-lipid interactions.     

Acetylcholinesterases--the structural similarities and differences

Acetylcholinesterase (AChE) is a widely spread enzyme playing a very important role in nerve signal transmission. As AChE controls key processes, its inhibition leads to the very fast death of an organism, including humans. However, when this feature is to be used for killing of unwanted organisms (i.e. mosquitoes), one is faced with the question - how much do AChEs differ between species and what are the differences? Here, a theoretical point of view was utilized to identify the structural basis for such differences. The various primary and tertiary alignments show that AChEs are very evolutionary conserved enzymes and this fact could lead to difficulties, for example, in the search for inhibitors specific for a particular species.     

Conformations of the rhodopsin third cytoplasmic loop grafted onto bacteriorhodopsin

BACKGROUND: The third cytoplasmic loop of rhodopsin (Rho EF) is important in signal transduction from the retinal in rhodopsin to its G protein, transducin. This loop also interacts with rhodopsin kinase, which phosphorylates light-activated rhodopsin, and arrestin, which displaces transducin from light-activated phosphorylated rhodopsin. RESULTS: We replaced eight residues of the EF loop of bacteriorhodopsin (BR) with 24 residues from the third cytoplasmic loop of bovine Rho EF. The surfaces of purple membrane containing the mutant BR (called IIIN) were imaged by atomic force microscopy (AFM) under physiological conditions to a resolution of 0.5-0.7 nm. The crystallinity and extracellular surface of IIIN were not perturbed, and the cytoplasmic surface of IIIN increased in height compared with BR, consistent with the larger loop. Ten residues of Rho EF were excised by V8 protease, revealing helices E and F in the AFM topographs. Rho EF was modeled onto the BR structure, and the envelope derived from the AFM data of IIIN was used to select probable models. CONCLUSIONS: A likely conformation of Rho EF involves some extension of helices E and F, with the tip of the loop lying over helix C and projecting towards the C terminus. This is consistent with mutagenesis data showing the TTQ transducin-binding motif close to loop CD, and cysteine cross-linking data indicating the C-terminal part of Rho EF to be close to the CD loop.     

Time-resolved step-scan Fourier transform infrared spectroscopy reveals differences between early and late M intermediates of bacteriorhodopsin

In this report, from time-resolved step-scan Fourier transform infrared investigations from 15 ns to 160 ms, we provide evidence for the subsequent rise of three different M states that differ in their structures. The first state rises with approximately 3 microseconds to only a small percentage. Its structure as judged from amide I/II bands differs in small but well-defined aspects from the L state. The next M state, which appears in approximately 40 microseconds, has almost all of the characteristics of the "late" M state, i.e., it differs considerably from the first one. Here, the L left arrow over right arrow M equilibrium is shifted toward M, although some percentage of L still persists. In the last M state (rise time approximately 130 microseconds), the equilibrium is shifted toward full deprotonation of the Schiff base, and only small additional structural changes take place. In addition to these results obtained for unbuffered conditions or at pH 7, experiments performed at lower and higher pH are presented. These results are discussed in terms of the molecular changes postulated to occur in the M intermediate to allow the shift of the L/M equilibrium toward M and possibly to regulate the change of the accessibility of the Schiff base necessary for effective proton pumping.     

Ultrafast infrared spectroscopy of bacteriorhodopsin.

Picosecond infrared spectroscopy is developed and used for the first time to study the dynamics of photoexcited bacteriorhodopsin (BR). Both spectral and time-resolved data are obtained. The results open an entirely new approach to investigations of the BR photocycle. The infrared difference spectrum (K minus BR570) recorded at ambient temperature between 1,560 and 1,700 cm-1 is not identical with the spectrum reported for a frozen sample. Three bands of the K state at 1,622, 1,610, and 1,580 cm-1 and the bleaching at 1,637 cm-1 (C = NH stretch) are seen. These new spectral lines appear in less than 10 ps.