Triton X-100对细菌视紫红质中间产物M_(412)的效应

本文研究用非离子表面活性剂Triton X-100处理后的细菌视紫红质(BR Bacteriorhodo-psin)光循环中间产物M_(412)动力学过程的变化.实验结果表明,用不同浓度的Triton处理pH=6.5的BR体系时,其中间产物M_(412).快衰减成分的半衰期(τ_(1/2)~f)在Triton浓度为0.05%(w/w)附近突然变慢,随着Triton浓度的加大,τ_(1/2)~f又逐渐加快;慢衰减部分的半衰期(τ_(1/2)~s)则随Tri-ton浓度的增加逐渐变慢.BR的生色团峰发生蓝移.说明不同浓度的Triton在水溶液中聚集状态不同,可不同程度地破坏膜脂的液晶态结构,从而导致镶嵌在其中的BR发生构象的变化,使转运质子的氢键通道受到不同程度的影响,故质子泵转运通道发生改变、致使M_(412)的衰减速率改变.     

酶切菌紫质(bR)C端对紫膜光循环和质子泵效率的影响

本文研究紫膜悬浮液经低剂量木瓜蛋酶处理去掉菌紫质(Bacteriorhodopsin简写bR)分子C-末端后。其光循环产物和质子泵效率的变化。实验发现经酶切后,M_(412)产物中慢衰减组份M_(412)降低了20％,O_(640)降低了50％,而质子泵效率降低了70％。双光脉冲实验表明酶解作用并不影响光循环周期。这些事实说明了去C-端所引起的质子泵效率降低,不是通过光循环的途径而产生的。介质中离子强度对正常紫膜和酶解紫膜的质子泵效率有明显不同的影响 说明了C端在不同盐浓度中的构象对质子泵行为有很重要的作用。     

水在菌紫质光循环和质子泵中的作用

用圆二色仪和闪光动力学先谱仪分别测量了空气干燥紫膜薄层的圆二色谱及紫膜LB膜的M_(412)的衰减过程.在于燥紫膜的圆二色谱上出现412nm的正峰,它是光循环中间体M_(412)的特征峰.在无水介质中,紫膜LB膜中的BR仍能进行先化学循环而检测到中间体M_(412),但M_(412)的衰减速度减慢,产生M_(412)的堆积,质子化过程受阻.在有水的介质中,只要有足够的H~+存在,紫膜LB膜中的BR的中间体M_(412)的衰减速度明显加快.说明水介质的H~+是完成正常光化学循和质子化过程必不可少的.     

CHAPS对M_(412)的动力学和共振拉曼光谱的影响

研究了表面活性剂CHAPS对紫膜中菌紫质在光循环过程中M_(412)的衰减速率及质子泵功能的影响.光循环中间体M_(412)快、慢衰减组分的衰减速率及质子衰减速率均受到CHAPS的影响,综合激光拉曼光谱对M_(412)和其它光循环中间体相对含量的测定,表明CHAPS对紫膜的影响是通过影响其膜脂完整的液晶结构,而使紫膜光循环动力学过程及质子泵功能发生变化的.     

两种化学修饰菌紫质的光化循环和光电位

本文分别用两种氮氧自由基对菌紫质(bR)中的两种氨基酸残基——赖氨酸和丝氨酸进行了修饰,并对修饰后的bR光循环中间产物M_(412)动力学过程、质子泵效率及光电响应信号进行了测量。通过与正常紫膜进行比较,可以看出:赖氨酸被修饰后,M_(412)快、慢组分的衰减及质子的吸收过程均减慢,M_(412)和质子的产额、跨膜光电位信号均有不同程度的提高;丝氨酸被修饰后,M_(412)和质子的动力学过程的变化与赖氨酸基本相同,但M_(412)和质子的产额及跨膜光电位提高很大,且光电位出现缓慢反向现象。结果表明赖氨酸不大可能直接参与质子的传递过程,其对紫膜质子泵的影响主要是通过其所带电荷对表面电位的贡献;而丝氨酸却似乎对bR的功能影响很大并对维持质子通道构象环境的稳定起着很大作用。     

蜂毒对菌紫质(bR)光循环中间体M_(412)和质子泵的影响

蜂毒对菌紫质(bR)光循环中间体M_(412)及质子泵的动力学过程有较大影响.表现在M_(412)慢衰减组分(M_(412~S))和质子的半衰期增大及产出量的减小,说明蜂毒分子的介入抑制了M_(412)的生成和衰减过程,同时也阻碍了紫膜的质子泵功能.但似乎对M_(412)快衰减组分影响不大.以上结果支持了M_(412~S)与质子泵功能有关的说法.实验结果同时反映出蜂毒除与膜脂分子存在强烈作用外还与bR本身直接作用.因此,蜂毒是一种研究膜脂蛋白相互作用及膜蛋白功能的较好材料.     

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(ts1/2)值在(4.1±1.1)ms左右;pH＞7.3时,ts1/2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.     

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.     

菌紫质光循环中间体的时间分辨谱

利用毫微秒时间分辨的吸收变化和微秒的闪光动力学光谱研究了室温下菌紫质光循环中间体的形成过程及衰减过程。实验结果表明,室温下,K_(610)和M_(412)中间体同样出现,L_(550)中间体还不能得到证实,有待于进一步研究。     

肼对蓝膜的影响

利用紫外可见吸收光谱和动力学光谱法研究了无水肼对蓝膜的影响,研究结果表明:无水肼可以使蓝膜转化为紫膜,同时光循环也得到恢复,但是光循环中间体M412的衰减加快,这与金属阳离子加入到蓝膜溶液中时的现象是完全不同的(这个过程中M412的衰减是减慢的).同时研究了pH和温度对无水肼与蓝膜之间相互作用的影响.在无水肼加入到蓝膜溶液中时,重组反应的灵敏度是pH和温度依赖的.在pH4.8到pH2之间,灵敏度随酸性的增加而降低.在20～40℃之间,无水肼与蓝膜溶液的反应灵敏度随着温度的升高而降低.     

Time-resolved X-ray diffraction study of structural changes associated with the photocycle of bacteriorhodopsin.

The time course of structural changes accompanying the transition from the M412 intermediate to the BR568 ground state in the photocycle of bacteriorhodopsin (BR) from Halobacterium halobium was studied at room temperature with a time resolution of 15 ms using synchrotron radiation X-ray diffraction. The M412 decay rate was slowed down by employing mutated BR Asp96Asn in purple membranes at two different pH-values. The observed light-induced intensity changes of in-plane X-ray reflections were fully reversible. For the mutated BR at neutral pH the kinetics of the structural alterations (tau 1/2 = 125 ms) were very similar to those of the optical changes characterizing the M412 decay, whereas at pH 9.6 the structural relaxation (tau 1/2 = 3 s) slightly lagged behind the absorbance changes at 410 nm. The overall X-ray intensity change between the M412 intermediate and the ground state was about 9% for the different samples investigated and is associated with electron density changes close to helix G, B and E. Similar changes (tau 1/2 = 1.3-3.6 s), which also confirm earlier neutron scattering results on the BR568 and M412 intermediates trapped at -180 degrees C, were observed with wild type BR retarded by 2 M guanidine hydrochloride (pH 9.4). The results unequivocally prove that the tertiary structure of BR changes during the photocycle.     

The role of back-reactions and proton uptake during the N----O transition in bacteriorhodopsin's photocycle: a kinetic resonance Raman study

The kinetics of bacteriorhodopsin's photocycle have been analyzed at pH 5, 6, 7, 8, and 8.6 by using time-resolved resonance Raman spectroscopy. The concentrations of the various intermediates as a function of time were determined by following their resonance Raman intensities using 502-nm (L550, N550, BR568), 458-nm (M412), and 752-nm (O640) excitation. The spectral contributions to the pump + probe data from each intermediate were quantitatively separated by least-squares decomposition. These relative concentrations were then converted to absolute concentrations by using a conservation of molecules constraint. This enabled the unambiguous refinement of a variety of kinetic models to find the simplest one that accurately describes the data. The kinetic data, including the biphasic decay of L550 and M412, are best reproduced by a sequential scheme including back-reactions (BR----L----M----N----O----BR). In addition, the kinetics of the L----M and N----O steps are found to be pH-dependent. Both the forward and reverse rate constants connecting L550 and M412 increase with pH, confirming earlier proposals of catalyzed Schiff base deprotonation at alkaline pH. Below pH 7, the N550----O640 rate constant is independent of pH, but it decreases linearly with pH above 7. This indicates that the protein must pick up a proton during the N550----O640 transition and that this process becomes rate determining above pH 7. There must, therefore, be an intermediate between N550 and O640 which we denote as N+550. A molecular graphics model is presented which incorporates these observations into a mechanism for proton pumping.     

The photophobic receptor from Natronobacterium pharaonis: temperature and pH dependencies of the photocycle of sensory rhodopsin II.

The photocycle of the photophobic receptor sensory rhodopsin II from N. pharaonis was analyzed by varying measuring wavelengths, temperature, and pH, and by exchanging H2O with D2O. The data can be satisfactorily modeled by eight exponents over the whole range of modified parameters. The kinetic data support a model similar to that of bacteriorhodopsin (BR) if a scheme of irreversible first-order reactions is assumed. Eight kinetically distinct protein states can then be identified. These states are formed from five spectrally distinct species. The chromophore states Si correspond in their spectral properties to those of the BR photocycle, namely pSRII510 (K), pSRII495 (L), pSRII400 (M), pSRII485 (N), and pSRII535 (O). In comparison to BR, pSRII400 is formed approximately 10 times faster than the M state; however, the back-reaction is almost 100 times slower. Comparison of the temperature dependence of the rate constants with those from the BR photocycle suggests that the differences are caused by changes of DeltaS. The rate constants of the pSRII photocycle are almost insensitive to the pH variation from 9.0 to 5.5, and show only a small H2O/D2O effect. This analysis supports the idea that the conformational dynamics of pSRII controls the kinetics of the photocycle of pSRII.     

Tyrosine and carboxyl protonation changes in the bacteriorhodopsin photocycle. 1. M412 and L550 intermediates

The role of tyrosines in the bacteriorhodopsin (bR) photocycle has been investigated by using Fourier transform infrared (FTIR) and UV difference spectroscopies. Tyrosine contributions to the BR570----M412 FTIR difference spectra recorded at several temperatures and pH's were identified by isotopically labelling tyrosine residues in bacteriorhodopsin. The frequencies and deuterium/hydrogen exchange sensitivities of these peaks and of peaks in spectra of model compounds in several environments suggest that at least two different tyrosine groups participate in the bR photocycle during the formation of M412. One group undergoes a tyrosinate----tyrosine conversion during the BR570----K630 transition. A second tyrosine group deprotonates between L550 and M412. Low-temperature UV difference spectra in the 220--350-nm region of both purple membrane suspensions and rehydrated films support these conclusions. The UV spectra also indicate perturbation(s) of one or more tryptophan group(s). Several carboxyl groups appear to undergo a series of protonation changes between BR570 and M412, as indicated by infrared absorption changes in the 1770--1720-cm-1 region. These results are consistent with the existence of a proton wire in bacteriorhodopsin that involves both tyrosine and carboxyl groups.     

The photocycle of bacteriorhodopsin immobilized in poly(vinyl alcohol) film

The kinetics of photoelectric and optical signals were measured on samples containing oriented purple membranes immobilized in a poly(vinyl alcohol) film and on purple membranes introduced into a PVA-H2O mixture. The bacteriorhodopsin photocycle in the PVA-H2O mixture was complete. The only observed changes were the slowing down of the optical and electrical signals in relation to the M412-O640 and O640-bRall-trans steps. In the PVA film the O640 intermediate disappeared and a negative photoelectric signal appeared.     

Determination of retinal chromophore structure in bacteriorhodopsin with resonance Raman spectroscopy

The analysis of the vibrational spectrum of the retinal chromophore in bacteriorhodopsin with isotopic derivatives provides a powerful "structural dictionary" for the translation of vibrational frequencies and intensities into structural information. Of importance for the proton-pumping mechanism is the unambiguous determination of the configuration about the C13=C14 and C=N bonds, and the protonation state of the Schiff base nitrogen. Vibrational studies have shown that in light-adapted BR568 the Schiff base nitrogen is protonated and both the C13=C14 and C=N bonds are in a trans geometry. The formation of K625 involves the photochemical isomerization about only the C13=C14 bond which displaces the Schiff base proton into a different protein environment. Subsequent Schiff base deprotonation produces the M412 intermediate. Thermal reisomerization of the C13=C14 bond and reprotonation of the Schiff base occur in the M412------O640 transition, resetting the proton-pumping mechanism. The vibrational spectra can also be used to examine the conformation about the C--C single bonds. The frequency of the C14--C15 stretching vibration in BR568, K625, L550 and O640 argues that the C14--C15 conformation in these intermediates is s-trans. Conformational distortions of the chromophore have been identified in K625 and O640 through the observation of intense hydrogen out-of-plane wagging vibrations in the Raman spectra (see Fig. 2). These two intermediates are the direct products of chromophore isomerization. Thus it appears that following isomerization in a tight protein binding pocket, the chromophore cannot easily relax to a planar geometry. The analogous observation of intense hydrogen out-of-plane modes in the primary photoproduct in vision (Eyring et al., 1982) suggests that this may be a general phenomenon in protein-bound isomerizations. Future resonance Raman studies should provide even more details on how bacterio-opsin and retinal act in concert to produce an efficient light-energy convertor. Important unresolved questions involve the mechanism by which the protein catalyzes deprotonation of the L550 intermediate and the mechanism of the thermal conversion of M412 back to BR568. Also, it has been shown that under conditions of high ionic strength and/or low light intensity two protons are pumped per photocycle (Kuschmitz & Hess, 1981). How might this be accomplished?(ABSTRACT TRUNCATED AT 400 WORDS)     

Mechanism of Nonlinear Photoinduced Anisotropy in Bacteriorhodopsin and its Derivatives

Polymer films made with photosensitive chromophore protein bacteriorhodopsin (BR) from the extreme halophile Halobacterium salinarium as well as films made with BR derivatives exhibit a nonlinear photoinduced anisotropy. Two different methods can be used to induce anisotropy in polymer BR films. The first method is based on the anisotropic properties of the initial form of the photocycle, BR570 (B-type anisotropy). Another method is based on the anisotropic properties of the longest-lived photocycle intermediate M412 (M-type anisotropy). CW gas lasers were employed to induce a reversible anisotropy in polymer BR films. Nonlinear photoinduced anisotropy is discussed in the context of a model for the anisotropic photoselection of BR molecules under linearly polarized light. A comparison of the experimental dependencies of nonlinear photoinduced anisotropy on laser intensity with similar calculated dependencies enables one to determine the molecular dichroism of BR and its derivatives not only for the initial form of the photocycle, B but also for the longest-lived intermediate M. Here we present the data showing the correlation between the laser induced nonlinear anisotropic properties and chromophore/protein interactions in BR. The effect of polymer binder on the nonlinear photoanisotropic properties of polymer BR films is also described.