Effects of electric field on the photocycle of bacteriorhodopsin

The photoconversion of bacteriorhodopsin and the effects of an applied electric field (5 · 10⁷ V · m^?1) were studied in dry films of purple membranes from Halobacterium halobium. The electric field was found to cause at least two different effects: (1) it blocks in part the formation of the batho-bacteriorhodopsin (K), most probably due to electrically-induced dark transition of some bacteriorhodopsin molecules into the photochemically inactive form; (2) it decreases the rate of the intermediate M decay, the rise time of the M formation being unaffected by electric field. The observed phenomena may suggest a feedback control mechanism for the regulation of the bacteriorhodopsin photocycle in purple membranes.     

Time-resolved refractive index change during the bacteriorhodopsin photocycle

Kinetic refractive index spectroscopy has been applied to the study of the bacteriorhodopsin photocycle. A fully hydrated purple membrane film was examined in the temperature range from 10° to 40°C using 532 nm excitation (doubled Nd YAG laser) and 633 nm (He–Ne laser) testing beam. Multiexponential fitting of the data revealed five processes. Four of them are well known from kinetic optical absorption studies. The fifth process has only recently been observed in optical absorption experiments where it has a relatively small amplitude. In our refractive index experiments it has an amplitude of up to 30% of the full signal amplitude. It is characterized by an Arrhenius temperature dependence with an activation enthalpy of 40±5 kJ/mol and a decay time of about 0.8 ms at 20°C.     

Fast electric response signals in the bacteriorhodopsin photocycle

The time behavior of flash-induced charge movements during the first steps in the bacteriorhodopsin photocycle was measured on a suspension of purple membranes oriented by an electric field. The experiments were done in the temperature range 80–278 K. During the formation of the intermediate K, two negative (with respect to the direction of the proton pump) components of the response signal are well resolved with time constants τ₁ < 3 μs and $\text{τ}{}_2\text{? 150 μ}\text{s}$ at 200 K. The distances of the charge displacements responsible for the electric signals are estimated. On the basis of the results the two components are assigned to two steps in the trans-cis isomerization of the retinal. A third negative component appears at higher temperatures which is related by time constant measurements to the K → L transition.     

Absorption spectra of intermediates of bacteriorhodopsin measured by laser photolysis at room temperatures

Picosecond laser spectroscopic analysis was applied to determine how many intermediates existed in the primary photochemical process of trans-bacteriorhodopsin (light-adapted bacteriorhodopsin) at room temperature (18°C) and to calculate their absorption spectra. Irradiation of bacteriorhodopsin with a laser pulse (wavelength, 532 nm; pulse width, 25 ps) yielded the K intermediate (K) which was produced through a precursor, having an absorption maximum (λ_max) longer than that of K. K was stable during a picosecond time range (50–900 ps). The λ_max was located at 610 nm and the extinction coefficient (?_max) was 0.92-times that of bacteriorhodopsin. The same K intermediate was produced from bacteriorhodopsin even when it was excited with a high-energy pulse by which a saturation effect was induced. A transient difference spectrum measured at 150 ns after the excitation of bacteriorhodopsin was different in shape from that of the K intermediate, suggesting that an intermediate was formed by thermal decay of K. This intermediate, tentatively called the KL intermediate (KL), had a λ_max at 596 nm and an ?_max 0.80-times that of bacteriorhodopsin. KL decayed to the L intermediate (L) with a time constant of 2.2 μs. L has a λ_max at 543 nm and an ?_max 0.66-times that of bacteriorhodopsin.     

pH-dependence of interaction between melittin and bacteriorhodopsin

Melittin differentially slowed down the fast (M412f) and the slow (M412s) decay components of the photocyde intermediate M of trimeric bacteriorhodopsin in purple membrane while it accelerated the M412s of Triton X-100-solubilized bacteriorhodopsin monomers. Raising the bulk pH could enhance the effect of melittin on the M412s of bacteriorhodopsin in these two states. From pH 5.5 to 8.8, melittin slightly influenced the yield of intermediate M in purple membrane, whereas the yield of M412s decreased and subsequently reversed with the addition of melittin. Moreover, the monomeric bacteriorhodopsin bleached more readily in the presence of melittin and the higher pH made the bleaching effect of melittin more intensive as well. These results re-certify our former suggestions that there was electrostatic interaction between melittin and bacteriorhodopsin, and indicate that the biphasic M decay may not result from the well-known linear kinetic scheme (M→N →BR). At last the mechanisms underlying the interact     

细菌视紫红质光循环中间体M412的动力学初探

采用紫外可见吸收光谱技术和闪光光解技术,初步观察了细菌视紫红质(BR)分子在宽pH范围（2.1～12.3）内的特征吸收峰以及M₄₁₂的相对浓度和M₄₁₂的慢成分半衰期的变化,并对其结构和光循环功能进行了讨论.紫外可见吸收光谱实验结果显示：pH=5.0～10.0时,BR最大特征吸收峰值约为568 nm;pH＜5.0时,BR最大特征吸收峰发生红移;pH＞10.0时,BR最大特征吸收峰发生蓝移.闪光动力学光谱结果显示：pH为7.3～9.5时,M₄₁₂的相对浓度(M₀)基本稳定在0.038左右;pH＜7.3时,M₀逐渐减小;pH＞9.5时,M₀明显上升,在pH=11.8时达到最大值0.1355,随后又快速下降.pH为2.1～7.3时,M₄₁₂的慢成分半衰期(t^s_1/2)值在(4.1±1.1)ms左右;pH＞7.3时,t^s_1/2值急剧延长到40 677.4 ms.推测在高pH条件下,BR分子的光循环有新的路径和机理.     

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.     

Dynamics of primary events in the photocycle of excited bacteriorhodopsin

Transient dynamic behavior of the excited bacteriorhodopsin (BR), which was isolated from the strain H. salinarum, was studied at excitation wavelength from 585 to 639 nm. With the one-color femtosecond (fs) pump-probe technique, we revealed the primary events in BR's photocycle that took place in an ultrafast time scale. From the analysis of the decay components of the dynamical traces, it was evident that the isomerization of the retinal     

Simulations of frequency-dependent photoacoustic magnitude signals and their implications for bacteriorhodopsin photocycle energetics

The modulation frequency dependence of photoacoustic signals obtained from photoactive samples can provide information on the time-dependent enthalpy changes occurring during the light-induced process. The experimental requirements for this type of calorimetry, and the interpretation ot the results, are critically examined with reference to the light-driven proton pump bacteriorhodopsin. For a three-step unbranched model of the bacteriorhodopsin photocycle we derive an expression for the photoacoustic magnitude signal as a function of frequency. Simulations are performed for various values of the rate constants and energetic changes. It is shown that the net heat uptake during a low, final step postulated by some workers should be reflected in the photoacoustic magnitude frequency spectrum, giving rise to a characteristic maximum. However, this effect, which has been observed experimentally, may also be produced by a fast, strongly endothermic step occurring earlier. The precise chronology of an endothermic transition cannot be resolved unambiguously by magnitude measurements alone, although they are free from assumptions regarding difficult-to-measure phase relationships. Hence, the published photoacoustic observations showing the effect are consistent with a cyclic sequence of events in which the bacteriorhodopsin system first undergoes an increase of entropy, followed by a decrease on returning to the initial state, as well as the reverse. It is argued that the molecular disorder-order sequence is more probable.     

Light adaptation of bacteriorhodopsin in the presence of valinomycin and potassium. pH-dependence

In the presence of valinomycin and K⁺, bacteriorhodopsin undergoes (i) a decrease of its maximum absorbance, (ii) a blue shift of the maximum wavelength of both the light and the dark adapted forms. However (iii) a normal light adaptation is maintained and (iv) the retinal-retinal interactions are not perturbed. The role of valinomycin as a K⁺-carrier allowing a H⁺-K⁺ competition as well as the stabilization of the deprotonated Schiff-base (linking retinal to the apo-opsin) is shown and discussed.Abbreviations bR bacteriorhodopsin - CD circular dichroism - DA dark-adapted - LA light-adapted - M-412 Meta-intermediate of the bacteriorhodopsin photocycle     

Bacteriorhodopsin. Correspondence of the photocycle and electrogenesis with sites of the molecule

Correspondence of phases of electrogenesis, photocycle transitions, and proton transfer with the proton transporting groups of bacteriorhodopsin was studied. The structure of bacteriorhodopsin was considered by the file 1c3w and projections of sites of the proton movement pathway onto the normal to the purple membrane were measured. The dielectric permeability of the terminal site of the semichannel Schiff base external surface of the purple membrane was noticeably higher than in the center of the membrane.Translated from Biokhimiya, Vol. 69, No. 12, 2004, pp. 1725–1728.Original Russian Text Copyright © 2004 by Khitrina, Ksenofontov.     

Mechanism of proton transport in bacteriorhodopsin from crystallographic structures of the K,L, M1, M2, and M2' intermediates of the photocycle

We produced the L intermediate of the photocycle in a bacteriorhodopsin crystal in photo-stationary state at 170 K with red laser illumination at 60% occupancy, and determined its structure to 1.62 A resolution. With this model, high-resolution structural information is available for the initial bacteriorhodopsin, as well as the first five states in the transport cycle. These states involve photo-isomerization of the retinal and its initial configurational changes, deprotonation of the retinal Schiff base and the coupled release of a proton to the extracellular membrane surface, and the switch event that allows reprotonation of the Schiff base from the cytoplasmic side. The six structural models describe the transformations of the retinal and its interaction with water 402, Asp85, and Asp212 in atomic detail, as well as the displacements of functional residues farther from the Schiff base. The changes provide rationales for how relaxation of the distorted retinal causes movements of water and protein atoms that result in vectorial proton transfers to and from the Schiff base.     

Simultaneous measurements of fast optical and proton current kinetics in the bacteriorhodopsin photocycle using an enhanced spectrophotometer

A one-of-a-kind high speed optical multichannel spectrometer was designed and built at NIH and described in this journal in 1997 [J.W. Cole, R.W. Hendler, P.D. Smith, H.A. Fredrickson, T.J. Pohida, W.S. Friauf. A high speed optical multichannel analyzer. J Biochem Biophys Methods 1997;35:16–174.]. The most unique aspect of this instrument was the ability to follow an entire time course from a single activation using a single sample. The instrument has been used to study rapid kinetic processes in the photon-driven bacteriorhodopsin photocycle and electron transport from cytochrome c to cytochrome aa₃ and from cytochrome aa₃ to oxygen. The present paper describes a second generation instrument with a number of important enhancements which significantly improve its capabilities for multichannel kinetic studies. An example application is presented in which the kinetics of photon-induced proton flow across the biological membrane is measured simultaneously with the individual steps of the photocycle determined optically. Matching the time constants for the two processes indicates which molecular transformations are associated with major proton movements.     

M-decay in the bacteriorhodopsin photocycle: effect of cooperativity and pH

The dependence of the bacteriorhodopsin (bR) photocycle on the intensity of the exciting flash was investigated in purple membranes. The dependence was most pronounced at slightly alkaline pH values. A comparison study of the kinetics of the photocycle and proton uptake at different intensities of the flash suggested that there exist two parallel photocycles in purple membranes at a high intensity of the flash. The photocycle of excited bR in a trimer with the two other bR molecules nonexcited is characterized by an almost irreversible M --> N transition. Excitation of two or three bR in a trimer induces the N --> M back reaction and accelerates the N --> bR transition. Based on the qualitative similarity of the pH dependencies of the photocycles of solubilized bR and excited dimers and trimers we proposed that the interaction of nonexcited bR in trimers alters the photocycle of the excited monomer as compared to solubilized bR and the changes in the photocycles in excited dimers and trimers are the result of decoupling of this interaction.     

Studies on the temperature effect on bacteriorhodopsin of purple and blue membrane by fluorescence and absorption spectroscopy

Fluorescence and absorption spectra were used to study the temperature effect on theconformation of bacteriorhodopsin (bR) in the blue and purple membranes (termed as bRb and bRprespectively).The maximum emission wavelengths of tryptophan fluorescence in both proteins at roomtemperature are 340 nm,and the fluorescence quantum yield of bRb is about 1.4 fold higher than that of bRp.As temperature increases,the tryptophan fluorescence of bRb decreases,while the tryptophan fluorescenceof bRp increases.The binding study of extrinsic fluorescent probe bis-ANS indicated that the probe can bindonly to bRb,but not to bRp.These results suggest that significant structural difference existed between bRband bRp.It was also found that both kinds of bR are highly thermal stable.The maximum wavelength of theprotein fluorescence emission only shifted from 340 nm to 346 nm at 100℃.More interestingly,as tempera-ture increased,the characteristic absorption peak of bRb at 605 nm decreased and a new absorption peak at380 nm formed.The transition occurred at a narrow temperature range (65℃-70℃).These facts indicatedthat an intermediate can be induced by high temperature.This phenomenon has not been reported before.     

Electric field promotion of the bacteriorhodopsin BR570 to BR412 photoconversion in films of Halobacterium halobium purple membranes

The combined action of electric field (10⁵–10⁷ V · m^?1) and light (380–580 nm, 80 W · m^?2) activating the photoenergetic reaction of bacteriorhodopsin (BR) in dry films of purple membranes from Halobacterium halobium was studied. A new stimulating effect of the field on the BR₄₁₂ intermediate accumulation in the normal photochromic cycle of BR₅₇₀ has been observed. The formation of the product BR₄₁₂ is supposed to be accompanied by specific rearrangements of certain charged, polar and polarizable groups in the BR pigment-protein matrix. Such an intrinsic polarization could be promoted by an external electric field, the displacement vector of those groups being oriented in the direction of the field. The dielectric polarization properties of the purple membranes have been demonstrated by electret-thermal analysis.     

High-resolution crystal structures of transient intermediates in the phytochrome photocycle

1. Download : Download high-res image (234KB)
2. Download : Download full-size image

     

Thermal equilibration between the M and N intermediates in the photocycle of bacteriorhodopsin.

The stages in the photocycle of bacteriorhodopsin (BR) involving the M and N intermediates are investigated using a double pulse excitation method. A first (cycling) pulse at 532 nm is followed, with an appropriate time delay, by a second pulse (337, 406, 446, or 470 nm) which induces the M-->BR back-photoreaction. After depletion by the second pulse a repopulation of M in the millisecond range is observed which is interpreted in terms of a thermal N-->M relaxation. It is thus concluded that a (thermal) M<-->N equilibrium accounts for the biphasic decay of M in the BR photocycle. Other models for this stage of the light-driven proton-pump are therefore unnecessary.     

Temperature and pH sensitivity of the O640 intermediate of the bacteriorhodopsin photocycle

The temperature and pH dependencies of the O₆₄₀ intermediate of the photocycle of bacteriorhodopsin (bR) were investigated by flash photolysis and T-jump experiments. The maximal concentration of the O₆₄₀ intermediate was found to be dependent on the temperature, which is described by a sigmoidal relationship. With increasing pH the midpoint of the sigmoidal curves shifts to higher temperatures. The Van't Hoff equation provides enthalpy and entropy values of the observed states. These results indicate that, in the investigated temperature (0-60°C) and pH (pH 4.0-10.0) range, the sequence of the principal intermediates in the pathway “M-N-O-bR” does not change. The observations of the O₆₄₀ intermediate at pH < 8.0 and of the N₅₅₀ intermediate at pH > 8.0 are most probably due only to changes of the intrinsic rate constants of the bR photocycle, not to a different mechanism.     

The absorbance spectrum of the brown holo-membrane and the comparison of pI values of bacteriorhodopsin solubilized from purple membrane and from brown holo-membrane

Brown holo-membrane was prepared by the addition of all-trans-retinal to brown apo-membrane which was isolated from Halobacterium halobium grown in the presence of nicotine. The effects of pH and NaCI concentration on the absorbance spectrum of the brown holo-membrane were investigated in comparison with those of the purple membrane. The λ_max of the dark-adapted brown holo-membrane shifted from 560 to 600 nm by lowering pH. The pK value which was determined as the mid-point pH for the spectral red-shift was 5.8 in the absence of NaCl. It was lowered to 4.5 and 3.4 in 0.1 and 1 M NaCl solutions, respectively. The pK value for the brown holo-membrane was larger than the corresponding value for the purple membrane in the NaCl solution. Bacteriorhodopsins present in the purple membrane and in the brown holo-membrane were solubilized in the nonionic detergent, lauryl ester of sucrose. For both solubilized bacteriorhodopsins, the pK value of spectral red-shift was about 3.1 in water, and the pI value, determined by chromatofocusing, was about 4.6 at 22°C.