The surface potential on the purple membrane measured using a modified bacteriorhodopsin chromophore as the spectroscopic probe

The surface potential of the purple membrane was measured by a novel method by using an artificial bacteriorhodopsin whose chromophore was 13-CF₃ retinal instead of retinal. When attached to the apoprotein by a Schiff base, the intrinsic pK of the 13-CF₃ chromophore is around 7.3. The apparent p_K of this pigment depends on the surface potential and thus on the electrolyte concentration. This allowed us to determine the surface charge density using the Gouy-Chapman equation. The surface charge density was found to be −1.65 ± 0.15 × 10⁻³ electronic charges per Ų or about 2 negative charges/bacteriorhodopsin. This large value for the surface potential probably explains both part of the strong apparent association of divalent cations with the membrane and the effect of low salt concentrations on light-induced proton release from the purple membrane.     

Regulation of bacteriorhodopsin synthesis by growth rate in continuous cultures of Halobacterium halobium

The independent effects of oxygen tension and growth rate on bacteriorhodopsin synthesis in Halobacterium halobium have been studied in chemostat cultures. Bacteriorhodopsin synthesis occurs only at low growth rates and is stimulated by low oxygen tension. Fast growth rates override the stimulatory effects of oxygen tension, with the result that bacteriorhodopsin can scarcely be detected. Illumination of cultures maintained at low growth rate and low oxygen tension significantly increases the steady state cell yield. This finding suggests that under these conditions the purple membrane proton pump is coupled to energy transduction.     

Introduction of a method for three-dimensional mapping of the charge motion in bacteriorhodopsin

Electric signals associated with the photocycle of bacteriorhodopsin carry valuable information about the proton transport process. Photocurrents measured by different experimental methods are interpreted in terms of intramolecular charge displacements. Permanent electrical asymmetry of the sample is considered to be a prerequisite for the detection of electric signals. The various photoelectric measuring techniques can be distinguished by the way of achievement of this asymmetry. A common feature of the available methods, however, is that the samples are cylindrically symmetric. Consequently, intramembraneous charge displacements can normally be monitored only along the axis of the membrane normal. We developed a novel method that allows also the detection of the in-plane components of the charge displacements. Samples containing oriented purple membrane fragments were used in the experiments, and the rotational symmetry was transiently broken via anisotropic excitation of the bR molecules by linearly polarized light. Kinetics of the normal and in-plane components were measured and interpreted as a result of spatial charge displacements associated with the proton transport process in bacteriorhodopsin.     

The transverse location of tryptophan residues in the purple membranes of Halobacterium halobium studied by fluorescence quenching and energy transfer

Fluorescence quenching by a series of spin-labelled fatty acids is used to map the transverse disposition of tryptophan residues in bacteriorhodopsin (the sole protein in the purple membranes of Halobacterium halobium). A new method of data analysis is employed which takes into account differences in the uptake of the quenchers into the membrane. Energy transfer from tryptophan to a set of $\text{n-(9-}\text{anthroyloxy)}$ fatty acids is used as a second technique to confirm the transverse map of tryptophan residues revealed by the quenching experiments. The relative efficiencies of quenching and energy transfer obtained experimentally are compared with those predicted on the basis of current models of bacteriorhodopsin structure. Most of the tryptophan fluorescence is located near the surface of the purple membrane. When the retinal chromophore of bacteriorhodopsin is removed, tryptophan residues deep in the membrane become fluorescent. These results indicate that the deeper residues transfer their energy to retinal in the native membrane. The retinal moiety is therefore located deep within the membrane rather than at the membrane surface.     

Segregation of modified bacteriorhodopsin aggregations in reconstituted vesicle membrane induced by the change of thermodynamical parameters

It was clearly shown that the change in thermodynamical parameters could cause the segregation of membrane protein aggregations in the phospholipid membrane. At first, reconstituted vesicles were prepared with a membrane protein, bacteriorhodopsin and a constituent phospholipid of biomembranes, L-alpha-dimyristoyl phosphatidylcholine. When the temperature of the suspension was decreased or the osmotic pressure was increased by adding poly(ethylene glycol) to this vesicle suspension at 23 degrees, the circular dichroism spectra showed a typical band indicating bacteriorhodopsin trimer formation implying their aggregation. This suggests that the aggregation of trimers proceeded by adding poly(ethylene glycol) into vesicle suspension, just as it proceeded by decreasing the temperature. Next, vesicles were prepared with fluorescein isothiocyanate-labeled bacteriorhodopsin, photoemissive bacteriorhodopsin and L-alpha-dimyristoyl phosphatidylcholine. The excitation energy transfer between the two modified proteins was measured by fluorescence spectroscopy. In this case, however, when poly(ethylene glycol) was added into the suspension, the yield of the excitation energy transfer decreased. This result indicates that modified proteins aggregate separately in a segregated form in the vesicle membrane.     

Directly probing rapid membrane protein dynamics with an atomic force microscope: a study of light-induced conformational alterations in bacteriorhodopsin.

This paper demonstrates that an atomic force microscope can be used to directly monitor rapid membrane protein dynamics. For this demonstration the membrane-bound proton pump, bacteriorhodopsin, has been investigated. It has been unequivocally shown that the light-induced dynamic alterations that have been observed do not arise from external artifacts such as heating of the sample by the incident light, but that these changes can be directly linked to the light-induced protein conformational alterations in this membrane. In essence, it has been shown that the light energy absorbed by bacteriorhodopsin is converted not only to chemical energy but also to mechanical energy. In summary a new ultrasensitive tool is described for monitoring the molecular dynamics of materials with wide applicability to fundamental and applied science.     

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.     

A measurement of the proton pump current generated by bacteriorhodopsin in black lipid membranes

The light-induced electrical current generated by black lipid membranes containing bacteriorhodopsin from Halobacterium halobium has been measured directly. It is shown that a measurement of membrane potential can also be used to obtain the proton pump current developed during illumination. Evidence is presented that the charge movement across the membrane is associated with the release of protons in the photoreaction cycle of bacteriorhodopsin. The time variation of the pump current when the light is turned on suggests the rapid depopulation of some initially occupied state.     

Picosecond and Nanosecond Components in Bacteriorhodopsin Light-Induced Electric Response Signal

Numerous investigations on the primary events of the bacteriorhodopsin photocycle indicate that the first steps of the energy transformation process take place in the 500 fs-5 ps region. These processes are known to be followed by others in the μs and ms regions. Recent observations indicate also the existence of nanosecond intermediate(s). Here we are reporting on direct measurements of the light-induced electric response signal of purple membrane carried out in the ps and ns regions. The laser flash-induced electric response of dried oriented purple membrane samples were detected by an ultrafast sampling oscilloscope. The measured kinetic curves were analyzed by exponential fitting and by a simulation-optimization method taking into account the time characteristics of the measuring setup. This analysis revealed a two phase real charge separation process. The first phase (tau = 21 ± 2 ps) coincides well with the overall bR-[unk] K transition. The second phase (tau = 6 ± 0.5 ns) can be correlated with the nanosecond optical transitions reported by several workers, or may be an optically silent charge movement inside the protein moiety or on the surface of the membrane.     

Characterization of the binding of valinomycin to bacteriorhodopsin

Circular dichroism spectroscopy has been used to investigate the binding of valinomycin to bacteriorhodopsin in purple membrane suspensions. Addition of valinomycin to purple membrane suspensions obtained from Halobacterium halobium causes the circular dichroism spectrum to shift from an aggregate spectrum to one resembling a monomer spectrum, indicating a loss of chromophore-chromophore interactions. By observing the spectral change upon titration of valinomycin, an apparent dissociation constant of 30–40 M for valinomycin binding was determined. Kinetics of dark adaptation for valinomycin-treated purple membrane are comparable to those for monomeric bacteriorhodopsin. Centrifugation studies demonstrate that valinomycin-treated purple membrane sediments the same as untreated purple membrane suspensions. These results are consistent with a model in which valinomycin binds specifically to bacteriorhodopsin without disrupting the purple membrane fragments.Abbreviations BR bacteriorhodopsin - CD circular dichroism - Tricine N-[tris-(hydroxymethyl) methyl] glycine     

切割菌紫质分子C端多肽对脂质泡中菌紫质分子在膜中旋转运动的影响

本实验用闪光诱导的瞬间二向色性方法分别测量了重组在DMPC脂质泡中的菌紫质分子和用木瓜蛋白酶切割C端多肽的菌紫质分子的旋转扩散运动。酶切的菌紫质分子与原菌紫质分子相比 前者旋转扩散运动加快,不可动分子的比例下降。在蜂毒或乙酰蜂毒存在下,酶切的菌紫质分子旋转扩散运动也受到较少的阻碍     

细菌视紫红质的质子传输机理

细菌视紫红质（bR）是嗜盐菌紫膜中的唯一蛋白质成分, 具有质子泵、电荷分离和光致变色功能. bR分子中的发色团视黄醛通过质子化席夫碱以共价键与Lys216相连. bR分子受可见光照射后, 视黄醛发生从全-反到13-顺式构型的异构化, 导致席夫碱的去质子化,继之以可极化基团位置的改变. 力场的变化引起包括蛋白质三级结构在内的诸多变化, 这些变化促进并保证了质子从细胞质侧向细胞外侧的定向传输.     

Location and orientation of the chromophore in bacteriorhodopsin: Analysis by fluorescence energy transfer

The spatial location and orientation of the retinal chromophore in bacteriorhodopsin were estimated from a fluorescence energy transfer study. The energy donor used in this study was a fluorescent retinal derivative, which was obtained by partial reduction of the purple membrane with sodium borohydride, and the energy acceptor was the native chromophore remaining in the same membrane. Since bacteriorhodopsin forms a two-dimensional crystal with P₃ symmetry in the purple membrane, and the membrane structure is maintained after the reduction, the rate of energy transfer from a donor to any acceptor existing in the same membrane can be calculated as a function of the location and orientation of the chromophores in the unit cell. Quantitative analyses of the fluorescence decay curve and the quantum yield, with various extents of reduction, enabled us to determine the most probable location and orientation. The result suggested that the chromophore was situated near the centre of the protein in such an orientation that the dipole-dipole interaction with neighbouring chromophores was close to minimum.     

A triangle lattice model that predicts transmembrane helix configuration using a polar jigsaw puzzle

We developed a method of predicting the tertiary structures of seven transmembrane helical proteins in triangle lattice models, assuming that the configuration of helices is stabilized by polar interactions. Triangle lattice models having 12 or 11 nearest neighbor pairs were used as general templates of a seven-helix system, then the orientation angles of all helices were varied at intervals of 15 degrees. The polar interaction energy for all possible positions of each helix was estimated using the calculated polar indices of transmembrane helices. An automated system was constructed and applied to bacteriorhodopsin, a typical membrane protein with seven transmembrane helices. The predicted optimal and actual structures were similar. The top 100 predicted helical configurations indicated that the helix-triangle, CFG, occurred at the highest frequency. In fact, this helix-triangle of bacteriorhodopsin forms an active proton-pumping site, suggesting that the present method can identify functionally important helices in membrane proteins. The possibility of studying the structure change of bacteriorhodopsin during the functional process by this method is discussed, and may serve to explain the experimental structures of photointermediate states.     

光敏蛋白菌紫质固相支撑人工膜系统的界面电荷

以固相支撑的菌紫质人工膜系统,在分子电子器件研究中占有重要地位。本文对其两种类型,Ｎ固相型和Ｃ固相型的界面电荷进行了研究,并提出了相关的模型。     

Structure and thermal stability of monomeric bacteriorhodopsin in mixed phospholipid/detergent micelles

Thermal unfolding experiments on bacteriorhodopsin in mixed phospholipid/detergent micelles were performed. Bacteriorhodopsin was extracted from the purple membrane in a denatured state and then renatured in the micellar system. The purpose of this study was to compare the changes, if any, in the structure and stability of a membrane protein that has folded in a nonnative environment with results obtained on the native system, i.e., the purple membrane. The purple membrane crystalline lattice is an added factor that may influence the structural stability of bacteriorhodopsin. Micelles containing bacteriorhodopsin are uniformly sized disks 105 +/- 13 A in diameter (by electron microscopy) and have an estimated molecular mass of 210 kDa (by gel filtration HPLC). The near-UV CD spectra (which is indicative of tertiary structure) for micellar bacteriorhodopsin and the purple membrane are very similar. In the visible CD region of retinal absorption, the double band seen in the spectrum of the purple membrane is replaced with a broad positive band for micellar bacteriorhodopsin, indicating that in micelles, bacteriorhodopsin is monomeric. The plot of denaturational temperature vs. pH for micellar bacteriorhodopsin is displaced downward on the temperature axis, illustrating the lower thermal stability of micellar bacteriorhodopsin when compared to the purple membrane at the same pH. Even though micellar bacteriorhodopsin is less stable, similar changes in response to pH and temperature are seen in the visible absorption spectra of micellar bacteriorhodopsin and the purple membrane. This demonstrates that changes in the protonation state or temperature have a similar affect on the local environment of the chromophore and the protein conformation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Mechanism of generation and regulation of photopotential by bacteriorhodopsin in bimolecular lipid membrane. The quenching effect of blue light

Photoelectric properties of bacteriorhodopsin incorporated into a bimolecular lipid membrane were investigated with special regard to the mechanism of photoelectric field generation. It was shown that besides its proton pump and electric generator functions bacteriorhodopsin works as a possible molecular regulator of the light-induced membrane potential. When a bimolecular lipid membrane containing bacteriorhodopsin is continuously illuminated in its main visible absorption band, and afterwards by superimposed blue light matching the absorption band of the long-living photobleached bacteriorhodopsin (M₄₁₂) as well, the latter either enhances or decreases the steady-state photoresponse, depending upon the intensity of the green light. Thus, the additional blue-light illumination tends to cause the resultant photoelectric membrane potential to become stabilized. Two alternative schemes are tentatively proposed for the photochemical cycle of bacteriorhodopsin whereby blue light can control photovoltage generation. A kinetic model of the proton pump and the regulation of the photoelectric membrane potential is presented. This model fits all the experimental findings, even quantitatively. From the model some kinetic and physical parameters of this light-driven pump could be determined.     

Pump and displacement currents of reconstituted ATP synthase on black lipid membranes

Summary Purified ATP synthase (F ₀ F ₁) fromRhodospirillum rubrum was reconstituted into asolectin liposomes which were than adsorbed to a planar lipid bilayer. After the addition of an inactive photolabile ATP derivative (caged ATP), ATP was released after illumination with UV light, which led to a transient current in the system. The transient photocurrent indicates that the vesicles and the planar membrane are capacitatively coupled. Stationary pump currents were obtained after addition of protonophores. These currents are specifically inhibited by oligomycin and stimulated threefold by inorganic phosphate (P _i ). In analogy oligomycin-sensitive pump currents in the reverse direction coupled to net ATP synthesis were induced by a light-induced concentration jump of ADP out of caged ADP, demonstrating the reversibility of the pump. For this, a preformed proton motive force and P _i were necessary.In a second series of experiments, proteoliposomes containing both ATP synthase and bacteriorhodopsin were adsorbed to a planar bilayer. The system was excited by a laser flash. The resulting photocurrents were measured with a time resolution of 2 sec. In the presence of ADP, the signal was modulated by the electrical activity of ATP synthase. ADP-induced charge displacements in ATP synthase, with time constants of 11 and 160 sec were obtained. The kinetics of the charge movements were slowed down byF ₀ specific inhibitors (DCCD or oligomycin) and were totally absent if ADP binding toF ₁ is prevented by the catalytic site-blocking agent NBD-Cl. The charge displacement of ATP synthase is coupled only to the membrane potential induced by the electrical activity of bacteriorhodopsin. The charge movements are interpreted as conformational transitions during early steps of the reaction cycle of ATP synthase.     

Modeling the membrane potential generation of bacteriorhodopsin

The archaeon Halobacterium salinarum can grow phototrophically with only light as its energy source. It uses the retinal containing and light-driven proton pump bacteriorhodopsin to enhance the membrane potential which drives the ATP synthase. Therefore, a model of the membrane potential generation of bacteriorhodopsin is of central importance to the development of a mathematical model of the bioenergetics of H. salinarum. To measure the current produced by bacteriorhodopsin at different light intensities and clamped voltages, we expressed the gene in Xenopus laevis oocytes. We present current-voltage measurements and a mathematical model of the current-voltage relationship of bacteriorhodopsin and its generation of the membrane potential. The model consists of three intermediate states, the BR, L, and M states, and comparisons between model predictions and experimental data show that the L to M reaction must be inhibited by the membrane potential. The model is not able to fit the current-voltage measurements when only the M to BR phase is membrane potential dependent, while it is able to do so when either only the L to M reaction or both reactions (L to M and M to BR) are membrane potential dependent. We also show that a decay term is necessary for modeling the rate of change of the membrane potential.     

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.