菌紫质稳态异构体光致变色反应动力学初探

实验证实,在适当的酸度调节下暗适应菌紫质（BR）的光致变色反应由B→蓝膜→P→Q→B的循环转换构成。在无光照下,B、Q态在中性介质中,蓝膜、P态在酸性介质中均呈高化学稳定性;蓝膜→P和Q→B的态转换须分别用650nm和400nm可见光激励,用紫外－可见光谱对两个光化学过程的动力学特性进行监测,证实它们均为一级反应。菌紫质的四个稳态在可见光区具有不同的特征吸收波长,在信息记录方面可望有一定应用前景。     

自旋标记法研究不同因素对嗜盐菌紫膜类脂物性的影响

本文用自旋标记方法研究了不同的pH和盐介质对光照前后嗜盐菌(H.halobium)紫膜类脂的影响.在低盐介质中,紫膜类脂序参数S的大小依次为pH2.5>pH7.0>pH12.0:旋转相关时间τ均在10~(-a)sec范围之内.pH12.0的暗适应和光适应悬液的ESR波谱十分相似,其它的ESR波谱均为暗适应>光适应.悬浮于Triton X-100中的紫膜的序参数最小,τ_e值在10~(-9)--10~(-10)sec之间;但其暗适应和光适应的ESR波谱仍有差别.在高盐介质中,紫膜类脂序参数均大于低盐介质,结构最为刚硬.实验表明类脂的序态变化与bR分子的构象改变有密切关系.     

菌紫质研究的新进展

菌紫质(BR)是嗜盐菌紫膜中的唯一蛋白质,野生型的BR分子含有248个氨基酸残基,其中一个视黄醛通过希夫碱基连结在第216位赖氨酸上,它具有质子泵的功能．光照下,BR进行光循环,光循环又与质子泵过程相关联．菌紫质的结构和功能方面的研究已有很大进展,但其光循环途径和质子泵的机理还不太清楚．文章概述了近年来对菌紫质结构,光循环和质子泵机理研究的进展,尤其对争论较大的菌紫质光循环途径的四类模型作了较详细的介绍．     

菌紫质膜对315nm辐照的光反应

利用仪器本身的测量光束３１５ｎｍ光照对紫膜薄膜中菌紫质的光反应的影响的ＣＤ谱研究说明：３１５ｎｍ的近紫外光可以激发薄膜中菌紫质的光反应,３１５ｎｍ与４０８ｎｍ、３３５ｎｍ光激发的光反应变化类型一致,但与５６８ｎｍ光激发的反应变化类型不一致;３１５ｎｍ光激发的光反应与菌紫质的初始样品状态有关,与菌紫质所处的分子状态的分布有关,而不是直接与初始样品状态存在的表现条件有关。结果认为利用包括近ＵＶ光在内的不同光照条件来调控ＢＲ的光反应是有可能的。     

菌紫质膜对315nm辐照的光反应

利用仪器本身的测量光束３１５ｎｍ光照对紫膜薄膜中菌紫质的光反应的影响的ＣＤ谱研究说明：３１５ｎｍ的近紫外光可以激发薄膜中菌紫质的光反应,３１５ｎｍ与４０８ｎｍ、３３５ｎｍ光激发的光反应变化类型一致,但与５６８ｎｍ光激发的反应变化类型不一致;３１５ｎｍ光激发的光反应与菌紫质的初始样品状态有关,与菌紫质所处的分子状态的分布有关,而不是直接与初始样品状态存在的表现条件有关。结果认为利用包括近ＵＶ光在内的不同光照条件来调控ＢＲ的光反应是有可能的。     

紫膜上菌紫质(BR)分子间光协同作用研究

菌紫质（ＢＲ）光循环中Ｍ４１２产物受作用光强调制的现象完全可以用紫膜上ＢＲ三聚体内的光协同效应来解释。这种协同效应不仅与紫膜上ＢＲ呈三聚体的聚集状态有关,也与ＢＲ分子在紫膜上的晶型有序排列有关。紫膜在碱性介质中,加温至５０－６０℃时,三聚体仍然存在,但晶格结构已有破坏,此时也不存在协同效应。     

夜蛾复眼转化速度与光暗适应的时间关系

夜行蛾类的复眼,随光、暗适应时间而逐步转化,这种转化是可逆的.以屏蔽色素分布范围的大小为指标来判断复眼的转化速度得以下结果:1.从亮眼到暗眼:亮眼进入暗适应后其屏蔽色素随暗适应时间的增加而逐步向远心端方向集中.屏蔽色素的移动是减速进行的.暗适应开始后的前3分钟,每分钟移动百分率为10.7,当暗到10—15分钟时每分钟移动百分率为4.6,再暗到60—150分钟时每分钟移动百分率为0.7.屏蔽色素移动的速度个体间差异较大,完成全过程大多数个体需150分钟,少数个体只需60分钟,另有个别个体经过270分钟暗适应仍尚未完成全过程.2.从暗眼到亮眼:暗眼受光后,其屏蔽色素随光适应时间的增加而向近心端方向扩散,色素移动速度随时间的增加而减缓.转化全过程约需60分钟.     

紫膜在含水凝胶中的定向和状态

用几种光谱学方法研究了紫膜凝胶的定向度、生色团视黄醛的状态以及其光循环中间产物M的动力学过程。结果表明:用通常采用的制备方法所得到的紫膜凝胶虽然能得到光电响应信号,但其定向度并不理想,生色团视黄醛的构象受到较大扰动,光循环中间产物M的产出及衰减也受到抑制,部分样品甚至由于其视黄醛的脱落而完全失去颜色,其质子泵功能也随之丧失。这说明虽然紫膜凝胶是目前研究紫膜质子泵机理(光电响应测量)和构造分子电子器件较好的和有希望的人工膜系统之一,但由于该系统对紫膜结构和功能的扰动仍然较大,紫膜的定向较难控制,所以,我们仍需在凝胶的形成体系及方法的改进上作大量工作。     

大猿叶虫夏滞育的诱导：基于定量的光周期反应

为了探明大猿叶虫Colaphellus bowringi Baly夏滞育诱导的光周期时间测量特性, 我们通过室内实验系统比较了该虫在25℃、 不同长光照条件下,夏滞育的发生以及诱导50%个体进入夏滞育所需求的光 暗循环数。结果表明：不同长光照诱导的夏滞育比率有显著差异, 其中15 h或16 h光照诱导的滞育比率最高, 短于或长于这两个光照其滞育率均明显下降。在不同光 暗循环实验中, 14 h诱导的滞育比率均低于50%, 诱导50%个体进入夏滞育所需求的光 暗循环数在L15∶D9, L16∶D8, L17∶ D7和L18∶D6分别为2.61, 3.72, 4.64和5.92 d, 处理间存在显著差异。这些结果提示该虫夏滞育的诱导是基于定量的光周期反应。     

W86F/W86A突变对细菌视紫红质光循环影响的差异性分析

细菌视紫红质(bacteriorhodopsin,bR)是一种光驱受体蛋白,每个活性单元由3个单体组成,每个单体由一分子视蛋白和一分子的视黄醛发色团共价结合而成,其功能为从胞内向胞外定向传输质子,利用形成的质子浓度梯度将光能转化为化学能.光照后视黄醛发色团构型发生all-trans向13-cis转变,蛋白的构象也随之发生了一系列具有稳定中间态的变化并驱动质子的定向传递.为探讨bR视黄醛键合区保守性氨基酸色氨酸86 (Tryptop-han86,w86)对其光循环中间态和质子泵功能的影响,本研究采用定点突变技术将W86突变为侧链大小不同的F86和A86,通过原位紫外-可见光吸收光谱、闪光光解光谱、pH滴定、固体核磁共振等技术手段,探究W86F和W86A突变对bR光循环及质子泵功能影响差异性的分子机制.结果 表明,W86F和W86A突变均造成了bR暗适应状态下视黄醛顺反异构平衡向顺式构型占优的方向移动,且W86F突变可造成反式构型的完全消失.此外,无论是W86F还是W86A突变都造成了蛋白光循环中间态的减弱且衰减延长,以及质子泵功能减弱,但影响机制各有所不同,这可能与这两个突变对视黄醛多烯链上电子云的分布以及周围残基造成的扰动程度不同有关.     

草地贪夜蛾成虫复眼明暗适应及黄光照射下明适应状态转化率

【目的】蛾类昆虫的趋光性与复眼明暗适应状态的转化有着直接的关系，本研究旨在阐明光照与草地贪夜蛾Spodotera frugiperda复眼明暗适应状态转化的关系。【方法】在光、暗适应条件和不同光照强度黄光照射下，在不同时间段，用相机迅速拍照，观察统计草地贪夜蛾成虫复眼的明暗适应状态及明、暗适应状态转化率。【结果】在明适应状态下，草地贪夜蛾成虫经黄光照射1 h后，随光照强度的增加，复眼明适应状态保持率逐步升高：雄成虫复眼在0.1~0.5 lx时明适应状态保持率为67.77%(有32.23%的转化为暗适应状态与中间状态)，4~6 lx时明适应状态保持率达到100%；雌成虫复眼在7~10 lx时，明适应状态保持率达98.90%。在明适应状态下，经黄光照射3 h后，草地贪夜蛾成虫复眼明适应状态保持率亦随着光照强度的增加逐步升高，在0.1~0.5 lx时雄成虫复眼明适应状态保持率为50.00%,雌成虫为32.23%；在光照强度7~10 lx时，雌雄成虫复眼明适应状态保持率分别为90.00%和100%。在暗适应状态下，草地贪夜蛾成虫经不同光照强度的黄光照射30 min后，成虫复眼向明适应状态逐渐转化：在0.1~0.5 lx光照强度时雌、雄成虫复眼明适应状态转化率均为93.33%；当光照强度达到0.6~0.9 lx时雌成虫复眼的明适应状态转化率达到100%，雄成虫复眼则在1~2 lx时达到100%。【结论】结果说明，草地贪夜蛾成虫有较强的光敏感性，且雌虫对黄光的光敏感性略强于雄虫。     

A comparison of the second harmonic generation from light-adapted, dark-adapted, blue, and acid purple membrane.

The second order nonlinear polarizability and dipole moment changes upon light excitation of light-adapted bacteriorhodopsin (BR), dark-adapted BR, blue membrane, and acid purple membrane have been measured by second harmonic generation. Our results indicate that the dipole moment changes of the retinal chromophore, delta mu, are very sensitive to both the chromophore structure and protein/chromophore interactions. Delta mu of light-adapted BR is larger than that of dark-adapted BR. The acid-induced formation of the blue membrane results in an increase in the delta mu value, and formation of acid purple membrane, resulting from further reduction of pH to 0, returns the delta mu to that of light-adapted BR. The implications of these findings are discussed.     

New intermediates in the photochemical transformation of rhodopsin

The conditions of preferential accumulation of intermediates of the photochemical reaction cycle of bacteriorhodopsin (BR) P550 and P419 at low temperature are found. Upon illumination P550 and P419 undergo photochemical conversions into the light-adapted form of BR (P570), forming during this conversions a number of new intermediates: P550 leads to P560-- -- -- leads to P570; P419 leads to P421-- -- -- leads to P565-- -- -- leads to P585-- -- -- leads to P570; P419 leads to P470-- -- -- leads to P570. All intermediates are photoactive. All light reactions are photoreversible and give formation to the products with absorption maximum shifted to the red as compared to the initial state. The absorption spectra of intermediates are complex and include several bands which are more pronounced in the spectrum of P419 (maxima at 442, 419, 398 nm, a shoulder at 375 nm) and P421, less in the spectrum of P570 (maximum at 578 nm, shoulders at 540 and 608 nm) and others.     

Transient photovoltages in purple membrane multilayers. Charge displacement in bacteriorhodopsin and its photointermediates

The photovoltaic properties of bacteriorhodopsin molecules and their photochemical intermediates have been investigated in an experimental cell consisting of multilayered films of highly oriented, dry fragments of purple membrane and lipid sandwiched between two metal (Pd) electrodes. The electrical time constant of these sandwich cells containing between 5 and 30 layers is less than 10(-5) S. Bright illumination of these cells with actinic flashes of approximately 1 ms duration generates transient photovoltages. These photovoltages, which make the extracellular surface of purple membrane positive with respect to the intracellular surface, follow the time course of the flash with no detectable latency. The amplitude of the photovoltages increases linearly with light intensity and their action spectrum matches the absorption spectrum of the light-adapted state of bacteriorhodopsin, BR570. In these dry multilayer cells, the slow photointermediates of bacteriorhodopsin, M412, N520 and O640 are long lived. Illumination of the sandwich cells with long duration (200 ms) pulses of light results, therefore, in the formation of photomixtures containing all these slow photointermediates. Flash illumination of the sandwich cells immediately following the conditioning pulse produces photovoltages whose action spectra match the absorption spectra of the M412 and N520 photointermediates. The M412 photovoltages, like the BR570 photovoltages, follow the time course of the actinic flash with no detectable latency and increase in amplitude linearly with light intensity. But, unlike the BR570 photovoltage, the M412, N520 and O640 photovoltages make the extracellular surface of purple membrane negative with respect to the intracellular surface. Through the of their specific photovoltaic signals, M412 and N520 are shown to be kinetically distinct photointermediates of bacteriorhodopsin. Detection of fast photovoltages with these characteristics in the absence of any ionic solution, and in parallel with spectrophotometric changes, suggest that they arise from charge displacements in the bacteriorhodopsin molecules and their photointermediates as they undergo photochemical conversion in response to the absorption of photons.     

Two forms of the Photosystem II D1 protein alter energy dissipation and state transitions in the cyanobacterium Synechococcus sp. PCC 7942

Synechococcus sp. PCC 7942 (Anacystis nidulans R2) contains two forms of the Photosystem II reaction centre protein D1, which differ in 25 of 360 amino acids. D1: 1 predominates under low light but is transiently replaced by D1:2 upon shifts to higher light. Mutant cells containing only D1:1 have lower photochemical energy capture efficiency and decreased resistance to photoinhibition, compared to cells containing D1:2. We show that when dark-adapted or under low to moderate light, cells with D1:1 have higher non-photochemical quenching of PS II fluorescence (higher q_N) than do cells with D1:2. This is reflected in the 77 K chlorophyll emission spectra, with lower Photosystem II fluorescence at 697–698 nm in cells containing D1:1 than in cells with D1:2. This difference in quenching of Photosystem II fluorescence occurs upon excitation of both chlorophyll at 435 nm and phycobilisomes at 570 nm. Measurement of time-resolved room temperature fluorescence shows that Photosystem II fluorescence related to charge stabilization is quenched more rapidly in cells containing D1:1 than in those with D1:2. Cells containing D1:1 appear generally shifted towards State II, with PS II down-regulated, while cells with D1:2 tend towards State I. In these cyanobacteria electron transport away from PS II remains non-saturated even under photoinhibitory levels of light. Therefore, the higher activity of D1:2 Photosystem II centres may allow more rapid photochemical dissipation of excess energy into the electron transport chain. D1:1 confers capacity for extreme State II which may be of benefit under low and variable light.Abbreviations D1 the atrazine-binding 32 kDa protein of the PS II reaction centre core - D1:1 the D1 protein constitutively expressed during acclimated growth in Synechococcus sp. PCC 7942 - D1:2 an alternate form of the D1 protein induced under excess excitation in Synechococcus sp. PCC 7942 - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethyl urea - Fo minimal fluorescence in the dark-adapted state - Fo minimal fluorescence in a light-adapted state - F_M maximum fluorescence with all quenching mechanisms at a minimum, measured in presence of DCMU - F_M maximal fluorescence in a light-adapted state, measured with a saturating flash - F_Mdark maximal fluorescence in the dark-adapted state - F_V variable fluorescence in a light-adapted state (F_M-Fo) - PAM pulse amplitude modulated fluorometer - q_N non-photochemical quenching of PS II fluorescence - q_N (dark) q_N in the dark adapted state - q_P photochemical quenching of fluorescence     

Effect of light-adaptation on the photoreaction of bacteriorhodopsin from Halobacterium halobium

Light-induced formation of the 410 nm intermediate was investigated on dark-and light-adapted bacteriorhodopsin. The amplitude of the light-induced absorption increase at 410 nm of the light-adapted bacteriorhodopsin was twice as large as that of the dark-adapted bacteriorhodopsin. The amount of protons released from bacteriorhodopsin in response to illumination was also enhanced by light-adaptation. The degree of the enhancement was independent of the temperature in the dark-adaptation. The relation between these photochemical events and the isomeric configurations of retinal is discussed.     

Effect of light-adaptation on the photoreaction of bacteriorhodopsin from Halobacterium halobium

Light-induced formation of the 410 nm intermediate was investigated on dark-and light-adapted bacteriorhodopsin. The amplitude of the light-induced absorption increase at 410 nm of the light-adapted bacteriorhodopsin was twice as large as that of the dark-adapted bacteriorhodopsin. The amount of protons released from bacteriorhodopsin in response to illumination was also enhanced by light-adaptation. The degree of the enhancement was independent of the temperature in the dark-adaptation. The relation between these photochemical events and the isomeric configurations of retinal is discussed.     

Novel effects of methyl viologen on photosystem II function in spinach leaves

Methyl viologen (MV) is a well-known electron mediator that works on the acceptor side of photosystem I. We investigated the little-known, MV-induced inhibition of linear electron flow through photosystem II (PS II) in spinach-leaf discs. Even a low [MV] decreased the (1) average, light-adapted photochemical efficiency of PS II traps, (2) oxidation state of the primary quinone acceptor Q_A in PS II during illumination, (3) photochemical efficiency of light-adapted open PS II traps, (4) fraction of absorbed light energy dissipated constitutively in a light-independent manner or as chlorophyll (Chl) a fluorescence emission, (5) Chl a fluorescence yield corresponding to dark-adapted open reaction-center traps (F _o) and closed reaction-center traps (F _m), and (6) half-time for re-oxidation of Q_A⁻ in PS II after a single-turnover flash. These effects suggest that the presence of MV accelerates various “downhill” electron-transfer steps in PS II. Therefore, when using the MV to quantify cyclic electron flow, the inhibitory effect of MV on PS II should be taken into account.     

Photocycles of bacteriorhodopsin in light- and dark-adapted purple membrane studied by time-resolved absorption spectroscopy.

Nanosecond time-resolved absorption spectra have been measured throughout the photocycle of bacteriorhodopsin in both light-adapted and dark-adapted purple membrane (PM). The data from dark-adapted samples are interpretable as the superposition of two photocycles arising independently from the all-trans and 13-cis retinal isomers that coexist in the dark-adapted state. The presence of a photocycle in dark-adapted PM which is indistinguishable from that observed for light-adapted PM under the same experimental conditions is demonstrated by the observation of the same five relaxation rates associated with essentially identical changes in the photoproduct spectra. This cycle is attributed to the all-trans component. The cycle of the 13-cis component is revealed by scaling the data measured for the light-adapted sample and subtracting it from the data on the dark-adapted mixture. At times less than 1 ms, the resulting difference spectra are nearly time-independent. The peak of the difference spectrum is near 600 nm, although there appears to be a slight (approximately 2 nm) blue-shift in the first few microseconds. Subsequently the amplitude of this spectrum decays and the peak of the difference spectrum shifts in two relaxations. Most of the amplitude of the photoproduct difference spectrum (approximately 80%) decays in a single relaxation having a time constant of approximately 35 ms. The difference spectrum remaining after this relaxation peaks at approximately 590 nm and is indistinguishable from the classical light-dark difference spectrum, which we find, in experiments performed on a much longer time scale, to peak at 588 nm. The decay of this remaining photo-product is not resolvable in the nanosecond kinetic experiments, but dark adaptation of a completely light-adapted sample is found to occur exponentially with a relaxation time of approximately 2,000 s under the conditions of our experiments.     

Light-dependent fluorescence variations in intact leaves

Transient variations in the fluorescence from intact Phytolaccaamericana leaves after the onset of illumination were measuredunder various light and dark conditions. Dark-adapted leaveswhen illuminated with strong light underwent an intensity variationwith a peak; the fluorescence intensity reaching its peak severalseconds after the onset of illumination then decreasing to asteady level. The peak height relative to the steady level increasedwith the increasing intensity of actinic light. Pre-illuminationof the dark-adapted leaves with strong light caused a markedlowering of the peak. About 20 min of dark incubation was requiredfor the light-adapted leaves to return to the dark-adapted state.All of the action spectra, for the peak, the steady level andthe effect of light in post-illumination to inhibit recoveryto the dark state, showed high bands due to chlorophyll b andcarotenoid absorption and low bands due to chlorophyll a absorption.We concluded that the light absorbed by photosystem 2 is responsiblefor these phenomena. (Received April 21, 1975; )