Pathways of the rise and decay of the M photointermediate(s) of bacteriorhodopsin

The photocycle of bacteriorhodopsin (BR) was studied at alkaline pH with a gated multichannel analyzer, in order to understand the origins of kinetic complexities in the rise and decay of the M intermediate. The results indicate that the biphasic rise and decay kinetics are unrelated to a photoreaction of the N intermediate of the BR photocycle, proposed earlier by others [Kouyama et al. (1988) Biochemistry 27, 5855-5863]. Rather, under conditions where N did not accumulate in appreciable amounts (high pH, low salt concentration), they were accounted for by conventional kinetic schemes. These contained reversible interconversions, either M in equilibrium with N in one of two parallel photocycles or L in equilibrium with as well as M in equilibrium with N in a single photocycle. Monomeric BR also showed these kinetic complications. Conditions were then created where N accumulated in a photo steady state (high pH, high salt concentration, background illumination). The apparent increase in the proportion of the slow M decay component by the background illumination could be quantitatively accounted for with the single photocycle model, by the mixing of the relaxation of the background light induced photo steady state with the inherent kinetics of the photocycle. Postulating a new M intermediate which is produced by the photoreaction of N was neither necessary nor warranted by the data. The difference spectra suggested instead that absorption of light by N generates only one intermediate, observable between 100 ns and 1 ms, which absorbs near 610 nm. Thus, the photoreaction of N resembles in some respects that of BR containing 13-cis-retinal.     

Nitration activates tyrosine toward reaction with the hydrated electron

3-Nitrotyrosine has been reported as an important biomarker of oxidative stress that may play a role in a variety of diseases. In this work, transient UV-visible absorption spectra and kinetics observed during the reaction of the hydrated electron, e(aq)(-), with 3-nitrotyrosine and derivatives thereof were investigated. The absorption spectra show characteristics of aromatic nitro anion radicals. The absorptivity of radical anion product at 300 nm is estimated to be (1.0 ± 0.2) × 10(4) M(-1) cm(-1) at pH 7.3. The rate constants determined for the reaction of e(aq)(-) with 3-nitrotyrosine, N-acetyl-3-nitrotyrosine ethyl ester and glycylnitrotyrosylglycine at neutral pH (3.0 ± 0.3) × 10(10) M(-1) s(-1), (2.9 ± 0.2) × 10(10) M(-1) s(-1) and (1.9 ± 0.2) × 10(10) M(-1) s(-1), respectively, approach the diffusion-control limit and are almost two orders of magnitude higher than those for the reactions with tyrosine and tyrosine-containing peptides. The magnitude of the rate constants supports reaction of e(aq)(-) at the nitro group, and the product absorbance at 300 nm is consistent with formation of the nitro anion radical. The pH dependence of the second-order rate constant for e(aq)(-) decay (720 nm) in the presence of 3-nitrotyrosine shows a decrease with increasing pH, consistent with unfavorable electrostatic interactions. The pH dependence of the second-order rate constant for formation of radical anion (300 nm) product suggests that deprotonation of the amino group slows the rate, which indicates that deamination to form the 1-carboxy-2-(4-hydroxy-3-nitrophenyl)ethyl radical occurs. We conclude that the presence of the nitro group activates tyrosine and derivatives toward reaction with e(aq)(-) and can affect the redox chemistry of biomolecules exposed to oxidative stress.     

Bacteriorhodopsin photoreaction: identification of a long-lived intermediate N (P,R350) at high pH and its M-like photoproduct

An alkaline suspension of light-adapted purple membrane exposed to continuous light showed a large absorption depletion at 580 nm and a small increase around 350 nm. We attribute this absorption change to an efficient photoconversion of bR570 into a photoproduct N (P,R350), which has a major absorption maximum between 550 and 560 nm but has lower absorbance than bR570. N was barely detectable at low pH, low ionic strength, and physiological temperature. However, when the thermal relaxation of N to bR570 was inhibited by increasing pH, increasing ionic strength, and decreasing temperature, its relaxation time could be as long as 10 s at room temperature. N is also photoactive; when it is present in significant concentrations, e.g., accumulated by background light, the flash-induced absorption changes of purple membrane suspensions were affected. Double-excitation experiments showed an M-like photoproduct of N,NM, with an absorption maximum near 410 nm and a much longer lifetime than M412. It may be in equilibrium with an L-like precursor NL. We suggest that N occurs after M412 in the photoreaction cycle and that its photoproduct NM decays into bR570. Thus, at high pH and high light intensity, the overall photoreaction of bR may be approximated by the two-photon cycle bR570----M412----N----(NL----NM)----bR570, whereas at neutral pH and low light intensity it can be described by the one-photon cycle bR570----M412----N----O640----bR570.(ABSTRACT TRUNCATED AT 250 WORDS)     

Characterization of the cycle of iron-mediated electron transfer from Adriamycin to molecular oxygen

The anticancer drug adriamycin binds iron and these complexes cycle to reduce molecular oxygen (Zweier, J. L. (1984) J. Biol. Chem. 259, 6056-6058). Optical absorption, EPR, and M?ssbauer spectroscopic data are correlated with polarographic O2 consumption and chemical Fe2+ extraction measurements in order to characterize each step in this cycle. Fe3+ binds to adriamycin at physiologic pH forming a complex with an optical absorbance maximum at 600 nm. EPR signals at g = 4.2 and g = 2.01, and a doublet M?ssbauer spectrum with isomer shift delta = 0.57 mm/s and quadrupole splitting delta EQ = 0.74 mm/s are observed indicating that the Fe3+ bound to adriamycin is high spin S = 5/2. Under anaerobic conditions the absorbance maximum at 600 nm decreases with an exponential decay constant = 0.77 h-1, and the EPR and M?ssbauer spectra of Fe3+-adriamycin similarly decrease as the Fe3+ is reduced to EPR silent Fe2+. The Fe2+-adriamycin complex which is formed exhibits a M?ssbauer spectrum with delta = 1.18 mm/s and delta EQ = 1.82 mm/s indicative of high spin Fe2+. As the EPR spectra of Fe3+-adriamycin decrease on reduction of the Fe3+ to Fe2+ a signal of the oxidized adriamycin free radical appears at g = 2.004 with line width of 8 G. On exposure to O2 the absorption maximum at 600 nm, the Fe3+ EPR, and the Fe3+ M?ssbauer spectra all return. Polarographic measurements demonstrate that O2 is consumed and that H2O2 is formed. Addition of high affinity Fe2+ chelators block O2 consumption indicating that Fe2+ formation is essential for O2 reduction. This cycle of iron-mediated O2 reduction can explain the formation of the reactive reduced oxygen and adriamycin radicals which are thought to mediate the biological activity of adriamycin.     

Proton interactions in the resting form of cytochrome oxidase.

The effect of pH on the near-UV absorption spectrum of cytochrome oxidase has been examined. Several lines of evidence implicate a proton binding site that can modulate the optical properties of cytochrome alpha 3 in the resting enzyme. Changing the pH within the range 6.5-10.5 was found to reversibly shift the position of the Soret band over an 11-nm range. The lower pH values caused a progressive blue shift in the Soret band, whereas the high-pH range promoted a gradual red shift. Limiting band positions were approximately 416 and 427 nm. The incubation time required to reach a stable band position varied somewhat as did the actual extent of the shift. In most cases, the shift was associated with an isosbestic point. A pH titration profile for the apparent equilibrium position of the Soret band was obtained. Nonlinear least-squares fitting to a scatter plot, assuming a single acid/base group, showed an apparent pKa of 7.8. Magnetic circular dichroism (MCD) spectra of the low-pH form at 416 nm, the high-pH form at 427 nm, and the cyanide derivative at 428 nm were compared. No evidence of a high-pH-dependent low-spin transition or a change in the redox state of cytochrome a3 was found, confirming earlier work [Baker, G. M., Noguchi, M., & Palmer, G. (1987) J. Biol. Chem. 262, 595-604]. Subtraction of ferricytochrome a [spectrum taken from Vanneste, W. H. (1966) Biochemistry 5, 838-848] from a series of blue-shifting spectra showed a band at 414 nm that progressively gained amplitude and a band at 430 nm that correspondingly lost amplitude. A series of red-shifting spectra showed the opposite behavior with a clear isosbestic point being evident in both cases. The difference extinction change at 414 and 430 nm depended linearly on the position of the Soret band, both showing a reversible dependence on pH. The 430-nm band is noted to be unusually red-shifted for high-spin ferric heme a. An additional, pH-insensitive band was observed at 408-410 nm which was eliminated by treatment with cyanide. The kinetics of the pH-induced blue shift and red shift were obtained at 416 nm by using dual-wavelength method and found to be biphasic, despite the occurrence of an isosbestic point.(ABSTRACT TRUNCATED AT 400 WORDS)     

Spectral heterogeneity and time-resolved spectroscopy of excitation energy transfer in membranes of Heliobacillus mobilis at low temperatures.

Transient absorption difference spectra in the Qy absorption band from membranes of Heliobacillus mobilis were recorded at 140 and 20 K upon 200 fs laser pulse excitation at 590 nm. Excitation transfer from short wavelength absorbing forms of bacteriochlorophyll g to long wavelength bacteriochlorophyll g occurred within 1-2 ps at both long wavelength bacteriochlorophyll g occurred within 1-2 ps at both temperatures. In addition, a slower energy transfer process with a time constant of 15 ps was observed at 20 K within the pool of long wavelength-absorbing bacteriochlorophyll g. Energy transfer from long wavelength antenna pigments to the primary electron donor P798 was observed, yielding the primary charge-separated state P798+A0-. The time constant for this process was 30 ps at 140 K and about 70 ps at 20 K. A decay component with smaller amplitude and a lifetime of up to hundreds of picoseconds was observed that was centered around 814 nm at 20 K. Kinetic simulations using simple lattice models reproduce the observed decay kinetics at 295 and 140 K, but not at 20 K. The kinetics of energy redistribution within the spectrally heterogeneous antenna system at low temperature argue against a simple "funnel" model for the organization of the antenna of Heliobacillus mobilis and favor a more random spatial distribution of spectral forms. However, the relatively high rate of energy transfer from long wavelength antenna bacteriochlorophyll g to the primary electron donor P798 at low temperature is difficult to explain with either of these models.     

Spectral properties of porcine plasminogen: study of the acidic transition (author's transl)]

The acidic transition of porcine plasminogen, prepared by affinity chromatography, was studied by non-destructive methods. These methods are based on the analysis of the behaviour of the tryptophyls under various conditions. The perturbation of the absorption and emission spectra by pH or temperature and the dynamic quenching of the intrinsic fluorescence are used to obtain information on structural changes which affect the environment of these residues. It is shown that by decreasing pH the fluorescence emission spectra are shifted toward the long wavelengths, with a broadening of the fluorescence band. The same effect can be obtained at constant pH by heating the protein solution. In order to analyze these phenomena, it is assumed that the fluorescence intensities at 355 nm and 328 nm reflect the proportion of the tryptophans which are exposed to the solvent, and buried, respectively. The plot of the ratio of the fluorescence intensities at these wavelengths versus pH or temperature leads to a titration curve showing an unmasking of tryptophans. The proportion of exposed tryptophans is measured by the dynamic fluorescence quenching technique and the data analyzed according to Lehrer. The plot of the fraction of exposed tryptophyls versus pH also shows the unmasking of these chromophores. Thermal perturbation of a solution of plaminogen at neutral pH induces a difference absorption spectrum whose amplitudes at the maxima are proportional to the number of exposed aromatic residues. The comparison with a solution of fully denatured plasminogen in 6 M guanidium chloride, where all the tryptophyls are exposed, shows that the percentage of exposure is equal to 59%. This number is significantly higher than the percentage found by the fluorescence quenching technique (20%), indicating that some tryptophyls are located in crevices, exposed to the solvent but not to the iodide. At acidic pH the absorption difference spectra induced by thermal perturbation are not classical, since they show an inversion and a new band between 300 nm and 305 nm. This band is mentioned in the literature as a minor band of tryptophan which appears when this chromophore is located in an asymmetric environment. On plotting the maximum amplitude of these spectra obtained at acidic pH versus temperature, we obtain a curve indicating that two types of antagonistic interactions are involved in the perturbation of the chromophores spectra. The spectrophotometric titration of plasminogen gives classical absorption difference spectra. By plotting the maximum amplitude at 292 nm versus pH, we obtain a titration curve with an apparent pK of 2.9 units. This pK is acidic which respect to the pK value of a normal carboxyl. This low value can be due to a positively charged group in the neighbourhood of a carboxyl, which interacts with one or more chromophores. When the carboxyl becomes protonated, this positively charged group is free and available to perturb the environment of some chromophores...     

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.     

Kinetic and spectroscopic evidence for an irreversible step between deprotonation and reprotonation of the Schiff base in the bacteriorhodopsin photocycle.

The photocycles of wild-type bacteriorhodopsin and its D96N form were investigated with a gated multichannel analyzer. Reconstruction of the spectra of the photointermediates from the measured time-resolved difference spectra allowed evaluation of the kinetics; the data at pH 7 in the presence of 100 mM NaCl were best fitted by the scheme K in eqiulibrium L in equilibrium M1----M2 in equilibrium N in equilibrium O----BR plus N----BR [Váró, G., & Lanyi, J. K. (1990) Biochemistry 29, 2241-2250]. The proposed two M states and the M1----M2 reaction were necessitated by anomalies in the kinetics of the decay of K and L. Additional support was provided by a 4-nm blue-shift in the maximum of M in Triton X-100 solubilized bacteriorhodopsin during the photocycle; the kinetics of the shift were consistent with the time course of the proposed M1----M2 transition. In the D96N mutant, the M state is stabilized, and the resulting equilibrium mixture for the intermediates could be evaluated with greater precision. The concentration ratio of L to M at the equilibrium was estimated to be no higher than 0.01. This requires the ratio of forward/reverse rates for the M1 to M2 conversion to be at least 200, i.e., a virtually irreversible reaction. Consistent with an earlier report, the data at lower pH and in the absence of NaCl are different and suggest the existence of a second L species; we propose that it is in equilibrium with M2.     

Moderate heat stress reduces the pH component of the transthylakoid proton motive force in light-adapted, intact tobacco leaves

We measured the Δ Ψ and ΔpH components of the transthylakoid proton motive force ( pmf ) in light-adapted, intact tobacco leaves in response to moderate heat. The Δ Ψ causes an electrochromic shift (ECS) in carotenoid absorbance spectra. The light–dark difference spectrum has a peak at 518 nm and the two components of the pmf were separated by following the ECS for 25 s after turning the light off. The ECS signal was deconvoluted by subtracting the effects of zeaxanthin formation (peak at 505 nm) and the qE-related absorbance changes (peak at 535 nm) from a signal measured at 520 nm. Heat reduced ΔpH while Δ Ψ slightly increased. Elevated temperature accelerated ECS decay kinetics likely reflecting heat-induced increases in proton conductance and ion movement. Energy-dependent quenching (qE) was reduced by heat. However, the reduction of qE was less than expected given the loss of ΔpH. Zeaxanthin did not increase with heat in light-adapted leaves but it was higher than would be predicted given the reduced ΔpH found at high temperature. The results indicate that moderate heat stress can have very large effects on thylakoid reactions.     

Time-resolved fluorescence spectroscopy of spinach chloroplast

Picosecond fluorescent kinetics and time-resolved spectra of spinach chloroplast were measured at room temperature and low temperatures. The measurement is conducted with 530 nm excitation at an average intensity of 2 · 10¹⁴ photons/cm², pulse and at a pulse separation of 6 ns for the 100 pulses used. The 685 nm fluorescent kinetics was found to decay with two components, a fast component with a 56 ps lifetime, and a slow component with a 220 ps lifetime. The 730 nm fluorescent kinetics at room temperature is a single exponential decay with a 100 ps lifetime. The 730 nm fluorescence lifetime was found to increase by a factor of 6 when the temperature was lowered from room temperature to 90 K, while the 685 and 695 nm fluorescent kinetics were unchanged. The time-resolved spectra data obtained within 10 ps after excitation is consistent with the kinetic data reported here. A two-level fluorescence scheme is proposed to explain the kinetics. The effect of excitation with high light intensity and multiple pulses is discussed.     

Synthesis and characterization of the dansyltyrosine derivatives of porcine pancreatic colipase

Steady-state and time-resolved fluorescence techniques were used to study dansyltyrosine derivatives of porcine pancreatic colipase. Nitration, reduction, acylation, and dansylation reactions were utilized to synthesize two fluorescently labeled colipases: (o-aminodansyltyrosine 55 porcine colipase) (DNStyr55PC) and o-aminodansyltyrosine 59 porcine colipase (DNStyr59PC). DNStyr55PC was 200% active, while the DNStyr59 derivative maintained 80% activity in a pH stat assay. Emission spectra, lifetime analysis, acrylamide quenching, polarization, and anisotropy decay studies indicated that Tyr55 was located on the solvent-exposed surface of the protein, where the fluorophore experienced free rotation. Identical experiments done on DNStyr59PC indicated that Tyr59 was in a partially buried environment and the motion of the dansyl tyrosine group was hindered. The double-exponential decay of the fluorescence emission of N-acetyl-o-aminodansyltyrosine ethyl ester (DNStyr) and the DNStyr derivatives of colipase was investigated with pH, temperature, solvent, and emission-resolved-lifetime experiments. The existence of excited-state processes was eliminated in both pH and emission-resolved-lifetime experiments, whereas temperature studies indicated either a rotational isomer or a differential solvent quenching mechanism for multiple decay kinetics. These experiments also showed that DNStyr was a sensitive probe of solvent polarity and viscosity, but not of pH.     

Photocycle and photoreversal of photoactive yellow protein at alkaline pH: kinetics, intermediates, and equilibria

Since the habitat of Halorhodospira halophila is distinctly alkaline, we investigated the kinetics and intermediates of the photocycle and photoreversal of the photoreceptor photoactive yellow protein (PYP) from pH 8 to 11. SVD analysis of the transient absorption time traces in a broad wavelength range (330-510 nm) shows the presence of three spectrally distinct species (I1, I1', and I2') at pH 10. The spectrum of I1' was obtained in two different ways. The maximal absorption is at 425 nm. I1' probably has a deprotonated chromophore and may be regarded as the alkaline form of I2'. At pH 10, the I1 intermediate decays in approximately 330 micros in part to I1' before I1 and I1' decay further to I2' in approximately 1 ms. From the rise of I2' (approximately 1 ms) to the end of the photocycle, the three intermediates (I1, I1', and I2') remain in equilibrium and decay together to P in approximately 830 ms. Assuming that the spectra of I1, I1', and I2' are pH-independent, their time courses were determined. On the millisecond to second time scale, they are in a pH-dependent equilibrium with a pKa of approximately 9.9. With an increase in pH, the I1 and I1' populations increase at the expense of the amount of I2'. The apparent rate constant for the recovery of P slows with an increase in pH with a pKa of approximately 9.7. The equal pH dependence of this rate and the equilibrium concentrations follows, if we assume that the equilibration rates between the intermediates are much faster than the recovery rate and that the recovery occurs from I2'. The pKa of approximately 9.9 is assigned to the deprotonation of the phenol of the surface-exposed chromophore in the I1'-I2' equilibrium. The I1-I1' equilibrium is pH-independent. Photoreversal experiments at pH 10 with the second flash at 355 nm indicate the presence of only one I2-like intermediate, which we assign on the basis of its lambda(max) value to I2'. After the rapid unresolved photoisomerization to I2'(trans), the reversal pathway back to P involves two sequential steps (60 micros and 3 ms). The amplitude spectra show that I1'(trans) and I1(trans) intermediates participate in this reversal.     

Magnetic circular dichroism studies of bovine liver catalase.

Absorption, circular dichroism (CD) and magnetic circular dichroism (MCD) spectra of beef liver catalase at pH 5.0 and 6.9, and its complexes with NaF, KCNO, NaCNS, NaN3 and NaCN, have been measured between 250 nm and 700 nm at room temperature. The pH 6.9 native catalase MCD shows the presence of several additional transitions not resolved in the absorption spectrum. While these bands can be seen in the spectra of all the derivatives, with the exception of the cyanide, their relative intensities changes considerably between complexes. Of special interest in the MCD of ferric hemes is the signal intensity at about 400 nm and 620 nm. The data indicate that the MCD intensity at 620 nm increases as the high spin iron porphyrin fraction increases, reaching a maximum with the fluoride complex. The 430 nm band intensity increases as the proportion of low spin iron increases, reaching a maximum with the cyanide complex. The MCD spectra also indicate clearly the existence of spin mixtures in the complexes with CNO-, CNS-, and N3-, where both the 430 nm and 620 nm bands have appreciable intensity. It is significant that despite almost identical absorption spectra the CNS- complex has higher fraction of low spin iron than either the CNO- or the N3- species. The differences between the pH 5 and 6.9 MCD spectra of the native catalase suggest that the environment of the heme centre is sensitive to protonation.     

Catalysis of the retinal subpicosecond photoisomerization process in acid purple bacteriorhodopsin and some bacteriorhodopsin mutants by chloride ions.

The dynamics and the spectra of the excited state of the retinal in bacteriorhodopsin (bR) and its K-intermediate at pH 0 was compared with that of bR and halorhodopsin at pH 6.5. The quantum yield of photoisomerization in acid purple bR was estimated to be at least 0.5. The change of pH from 6.5 to 2 causes a shift of the absorption maximum from 568 to 600 nm (acid blue bR) and decreases the rate of photoisomerization. A further decrease in pH from 2 to 0 shifts the absorption maximum back to 575 nm when HCl is used (acid purple bR). We found that the rate of photoisomerization increases when the pH decreases from 2 to 0. The effect of chloride anions on the dynamics of the retinal photoisomerization of acid bR (pH 2 and 0) and some mutants (D85N, D212N, and R82Q) was also studied. The addition of 1 M HCl (to make acid purple bR, pH 0) or 1 M NaCl to acid blue bR (pH 2) was found to catalyze the rate of the retinal photoisomerization process. Similarly, the addition of 1 M NaCl to the solution of some bR mutants that have a reduced rate of retinal photoisomerization (D85N, D212N, and R82Q) was found to catalyze the rate of their retinal photoisomerization process up to the value observed in wild-type bR. These results are explained by proposing that the bound Cl- compensates for the loss of the negative charges of the COO- groups of Asp85 and/or Asp212 either by neutralization at low pH or by residue replacement in D85N and D212N mutants.     

Effects of Asp-96----Asn, Asp-85----Asn, and Arg-82----Gln single-site substitutions on the photocycle of bacteriorhodopsin

Bacteriorhodopsin (BR) with the single-site substitutions Arg-82----Gln (R82Q), Asp-85----Asn (D85N), and Asp-96----Asn (D96N) is studied with time-resolved absorption spectroscopy in the time regime from nanoseconds to seconds. Time-resolved spectra are analyzed globally by using multiexponential fitting of the data at multiple wavelengths and times. The photocycle kinetics for BR purified from each mutant are determined for micellar solutions in two detergents, nonyl glucoside and CHAPSO, and are compared to results from studies on delipidated BR (d-BR) in the same detergents. D85N has a red-shifted ground-state absorption spectrum, and the formation of an M intermediate is not observed. R82Q undergoes a pH-dependent transition between a purple and a blue form with different pKa values in the two detergents. The blue form has a photocycle resembling that for D85N, while the purple form of R82Q forms an M intermediate that decays more rapidly than in d-BR. The purple form of R82Q does not light-adapt to the same extent as d-BR, and the spectral changes in the photocycle suggest that the light-adapted purple form of R82Q contains all-trans- and 13-cis-retinal in approximately equal proportions. These results are consistent with the suggestions of others for the roles of Arg-82 and Asp-85 in the photocycle of BR, but results for D96N suggest a more complex role for Asp-96 than previously suggested. In nonyl glucoside, the apparent decay of the M-intermediate is slower in D96N than in d-BR, and the M decay shows biphasic kinetics. However, the role of Asp-96 is not limited to the later steps of the photocycle. In D96N, the decay of the KL intermediate is accelerated, and the rise of the M intermediate has an additional slow phase not observed in the kinetics of d-BR. The results suggest that Asp-96 may play a role in regulating the structure of BR and how it changes during the photocycle.     

Monitoring the conformational changes of photoactivated rhodopsin from microseconds to seconds by transient fluorescence spectroscopy

The transient changes of the tryptophan fluorescence of bovine rhodopsin in ROS membranes were followed in time from 1 micros to 10 s after flash excitation of the photoreceptor. Up to about 100 micros the fluorescence did not change, suggesting that the tryptophan lifetimes in rhodopsin and the M(I) intermediate are similar. The fluorescence then decreases on the millisecond time scale with kinetics that match the rise of the M(II) state as measured on the same sample by the transient absorption increase at 360 nm. Both the sign and kinetics of the fluorescence change strongly suggest that it is due to an increase in energy transfer to the retinylidene chromophore caused by the increased spectral overlap in M(II). Calculation of the Forster radius of each tryptophan from the high-resolution crystal structure suggests that W265 and W126 are already completely quenched in the dark, whereas W161, W175, and W35 are located at distances from the retinal chromophore that are comparable to their Forster radii. The fluorescence from these residues is thus sensitive to an increase in energy transfer in M(II). Similar results were obtained at other temperatures and with monomeric rhodopsin in dodecyl maltoside micelles. A large light-induced transient fluorescence increase was observed with ROS membranes that were selectively labeled with Alexa594 at cysteine 316 in helix 8. Using transient absorption spectroscopy the kinetics of this structural change at the cytoplasmic surface was compared to the formation of the signaling state M(II) (360 nm) and to the kinetics of proton uptake as measured with the pH indicator dye bromocresol purple (605 nm). The fluorescence kinetics lags behind the deprotonation of the Schiff base. The proton uptake is even further delayed. These observations show that in ROS membranes (at pH 6) the sequence of events is Schiff base deprotonation, structural change, and proton uptake. From the temperature dependence of the kinetics we conclude that the Schiff base deprotonation and the transient fluorescence have comparable activation energies, whereas that of proton uptake is much smaller.     

Spectroscopic and kinetic studies on the oxygen-centered radical formed during the four-electron reduction process of dioxygen by Rhus vernicifera laccase.

The oxygen-centered radical bound to the trinuclear copper center was detected as an intermediate during the reoxidation process of the reduced Rhus vernicifera laccase with dioxygen and characterized by using absorption, stopped-flow, and electron paramagnetic resonance (EPR) spectroscopies and by super conducting quantum interface devices measurement. The intermediate bands appeared at 370 nm (epsilon approximately 1000), 420 nm (sh), and 670 nm (weak) within 15 ms, and were observable for approximately 2 min at pH 7.4 but for less than 5 s at pH 4.2. The first-order rate constant for the decay of the intermediate has been determined by stopped-flow spectroscopy, showing the isotope effect, k(H)/k(D) of 1.4 in D(2)O. The intermediate was found to decay mainly from the protonated form by analyzing pH dependences. The enthalpy and entropy of activation suggested that a considerable structure change takes place around the active site during the decay of the intermediate. The EPR spectra at cryogenic temperatures (<27 K) showed two broad signals with g approximately 1.8 and 1.6 depending on pH. We propose an oxygen-centered radical in magnetic interaction with the oxidized type III copper ions as the structure of the three-electron reduced form of dioxygen.     

Origin and properties of fluorescence emission from the extrinsic 33 kDa manganese stabilizing protein of higher plant water oxidizing complex

The fluorescence properties of the isolated extrinsic 33 kDa subunit acting as 'manganese stabilizing protein' (MSP) of the water oxidizing complex in photosynthesis was analyzed in buffer solution. Measurements of the emission spectra as a function of excitation wavelength, pH and temperature led to the following results: (a) under all experimental conditions the spectra monitored were found to be the composite of two contributions referred to as '306 nm band' and 'long-wavelength band', (b) the excitation spectra of these two bands closely resemble those of tyrosine and tryptophan in solution, respectively, (c) the spectral shape of the '306 nm band' is virtually independent on pH but its amplitude drastically decreases in the alkaline with a pK of 11.7, (d) the amplitude of the 'long-wavelength' emission band at alkaline pH slightly increases when the pH rises from 7.2 to about 11.3 followed by a sharp decline at higher pH, and (e) the shape of the overall spectrum at pH 7.2 is only slightly changed upon heating to 90 degrees C whereas the amplitude significantly declines. Based on these findings the two distinct fluorescence bands are ascribed to tyrosine(s) ('306 nm band') and the only tryptophan residue W241 of MSP from higher plants ('long-wavelength band') as emitters which are both embedded into a rather hydrophobic environment.     

Actinic light and pH effect on the proton pumping of bacteriorhodopsin

The actinic light effect on the bacteriorhodopsin (BR) photocycle kinetics led to the assumption of a cooperative interaction between the photocycling BR molecules. In this paper we report the results of the actinic light effect and pH on the proton release and uptake kinetics. An electrical method is applied to detect proton release and uptake during the photocycle [E. Papp, G. Fricsovszky, J. Photochem. Photobiol. B: Biol. 5 (1990) 321]. The BR photocycle kinetics was also studied by absorption kinetics measurements at 410 nm and the data were analyzed by the local analysis of the M state kinetics [E. Papp, V.H. Ha, Biophys. Chem. 57 (1996) 155]. While at high pH and ionic strength, we found a similar behavior as reported earlier, at low ionic strength the light effect proved to be more complex. The main conclusions are the following: Though the number of BR excited to the photocycle (fraction cycling, fc) goes to saturation with increasing laser pulse energy, the absorbed energy by BR increases linearly with pulse energy. From the local analysis we conclude that the light effect changes the kinetics much earlier, already at the L intermediate state decay. The transient electric signal, caused by proton release and uptake, can be decomposed into two components similarly to the absorption kinetic data of the M intermediate state. The actinic light energy affects mainly the ratio of the two components and the proton movements inside BR while pH has an effect on the kinetics of the proton release and uptake groups at the membrane surface.