The lipophilic fluorescent probe 4-dimethylaminochalcone: factors responsible for the fluorescence yield

Factors responsible for fluorescence quenching of the lipophylic fluorescent probe 4-dimethylaminochalcone in nonpolar and polar media were studied. The femtosecond dynamics of 4-dimethylaminochalcone excited state was measured using the absorption method of "excitation probing". In nonpolar hexane where the fluorescence quantum yield is very low (0.001), all excited 4-dimethylaminochalcone molecules go to the triplet state with a rate constant of 2.10(11) s(-1). At the same time, the radiation rate constant is 1000 times lower; therefore, such a fast transition to triplet is the major cause of the very small fluorescence yield. In polar acetone, the fluorescence yield is 220 times higher than in hexane. In acetone, no transitions to triplet state were detected. At the same time, a radiationless conversion to the ground state took place with a rate constant of 10(9) s(-1), which decreased the fluorescence yield to 0.22. The activation energy of the quenching processes is polarity dependent and decreases from 6 in nonpolar to 3 kcal/mol in polar media. The yield of 4-dimethylaminochalcone fluorescence varies hundreds times in media of different polarity but is a linear function of the Lippert's polarity parameter f(epsilon,n) where epsilon is the dielectric constant at low frequencies. It is supposed that polar media stabilize the "flat" conformation of the 4-dimethylaminochalcone molecule prior to its excitation, and this conformation is optimal for fluorescence. In this case, stabilization is determined only by medium polarity.     

Thermodynamic investigation into the mechanism of the chlorophyll fluorescence quenching in isolated photosystem II light-harvesting complexes

Chlorophyll fluorescence quenching can be stimulated in vitro in purified photosystem II antenna complexes. It has been shown to resemble nonphotochemical quenching observed in isolated chloroplasts and leaves in several important respects, providing a model system for study of the mechanism of photoprotective energy dissipation. The effect of temperature on the rate of quenching in trimeric and monomeric antenna complexes revealed the presence of two temperature-dependent processes with different activation energies, one between approximately 15 and 35 degrees C and another between approximately 40 and 60 degrees C. The temperature of the transition between the two phases was higher for trimers than for monomers. Throughout this temperature range, the quenching was almost completely reversible, the protein CD was unchanged, and pigment binding was maintained. The activation energy for the low temperature phase was consistent with local rearrangements of pigments within some of the protein domains, whereas the higher temperature phase seemed to arise from large scale conformational transitions. For both phases, there was a strong linear correlation between the quenching rate and the appearance of an absorption band at 685 nm. In addition, quenching was correlated with a loss of CD at approximately 495 nm from Lutein 1 and at 680 nm from chlorophylls a1 and a2, the terminal emitters. The results obtained indicate that quenching of chlorophyll fluorescence in antenna complexes is brought about by perturbation of the lutein 1/chlorophyll a1/chlorophyll a2 locus, forming a poorly fluorescing chlorophyll associate, either a dimer or an excimer.     

Thermal unfolding of myosin rod and light meromyosin: circular dichroism and tryptophan fluorescence studies

Rabbit skeletal myosin rod, which is the coiled-coil alpha-helical portion of myosin, contains two tryptophan residues located in the light meromyosin (LMM) portion whose fluorescence contributes 27% to the fluorescence of the entire myosin molecule. The temperature dependence of several fluorescence parameters (quantum yield, spectral position, polarization) of the rod and its LMM portion was compared to the thermal unfolding of the helix measured with circular dichroism. Rod unfolds with three major helix unfolding transitions: at 43, 47, and 53 degrees C, with the 43 and 53 degrees C transitions mainly located in the LMM region and the 47 degrees C transition mainly located in the subfragment 2 region. The fluorescence study showed that the 43 degrees C transition does not involve the tryptophan-containing region and that the 47 degrees C transition produces an intermediate with different fluorescence properties from both the completely helical and fully unfolded states. That is, although the fluorescence of the 47 degrees C intermediate is markedly quenched, the tryptophyl residues do not become appreciably exposed to solvent until the 53 degrees C transition. It is suggested that although the intermediate that is formed in the 47 degrees C transition contains an extensive region which is devoid of alpha-helix, the unfolded region is not appreciably solvated or flexible. It appears to have the properties of a collapsed nonhelical state rather than a classical random coil.     

Thermostability and photostability of photosystem II of the resurrection plant Haberlea rhodopensis studied by chlorophyll fluorescence

The stability of PSII in leaves of the resurrection plant Haberlea rhodopensis to high temperature and high light intensities was studied by means of chlorophyll fluorescence measurements. The photochemical efficiency of PSII in well-hydrated Haberlea leaves was not significantly influenced by temperatures up to 40 degrees C. Fo reached a maximum at 50 degrees C, which is connected with blocking of electron transport in reaction center II. The intrinsic efficiency of PSII photochemistry, monitored as Fv/Fm was less vulnerable to heat stress than the quantum yield of PSII electron transport under illumination (phiPSII). The reduction of phiPSII values was mainly due to a decrease in the proportion of open PSII centers (qP). Haberlea rhodopensis was very sensitive to photoinhibition. The light intensity of 120 micromol m(-2) s(-1) sharply decreased the quantum yield of PSII photochemistry and it was almost fully inhibited at 350 micromol m(-2) s(-1). As could be expected decreased photochemical efficiency of PSII was accompanied by increased proportion of thermal energy dissipation, which is considered as a protective effect regulating the light energy distribution in PSII. When differentiating between the three components of qN it was evident that the energy-dependent quenching, qE, was prevailing over photoinhibitory quenching, qI, and the quenching related to state 1-state 2 transitions, qT, at all light intensities at 25 degrees C. However, the qE values declined with increasing temperature and light intensities. The qI was higher than qE at 40 degrees C and it was the major part of qN at 45 degrees C, indicating a progressing photoinhibition of the photosynthetic apparatus.     

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.     

Changes in protein conformation and stability accompany complex formation between human C1 inhibitor and C1-s

The fluorescence spectrum of C1 inhibitor (C1-Inh) in aqueous buffer has a maximum at 324 nm which shifts to 358 nm in 6.0 M guanidinium chloride (GdmC1), indicating that fluorescent tryptophans are buried in the native protein. When titrated with GdmC1, the fluorescence intensity, polarization, and emission maximum of C1-Inh and C1-s exhibited clear transitions which were more prominent than those of the enzyme-inhibitor complex. Two of the variables (intensity and emission maximum) suggest biphasic unfolding of C1-Inh. Differential absorption measurements and sodium iodide quenching of intrinsic fluorescence were consistent with a net increase in the exposure of tryptophans and tyrosines upon complex formation. This reaction, i.e., complex formation, was also accompanied by an increase in the ability to enhance the fluorescence of the hydrophobic probe 8-anilino-1-naphthalenesulfonate. Fluorescence assays of heat denaturation showed transitions at 40 and 52 degrees C for C1-s and at 60 degrees C for C1-Inh whereas there was no detectable melting transition for the complex. Similarly, differential scanning calorimetric measurements revealed transitions at 42, 52, and 62 degrees C for C1-s and one transition at 60 degrees C for C1-Inh, with no major transitions detectable for the complex. The ratio of the calorimetric enthalpy to the apparent van't Hoff enthalpy for thermal unfolding of C1-Inh was 1.6. Taken together, these results suggest that C1-Inh and C1-s are each composed of at least two independently unfolding domains and that complex formation, which involves conformational change, yields a protein substantially more stable than either component alone.     

Multiple conformational transitions of hen egg-white lysozyme in aqueous acetic acid solutions

Circular dichroism measurements revealed that hen egg-white lysozyme underwent multiple conformational transitions upon the addition of acetic acid. The transitions were reversible as judged from complete recoveries of enzymatic activity, electrophoretic mobility in SDS-polyacrylamide gel, and of ellipticity. Two transitions, with the mid-concentrations of 26 and 38% (v/v), were observed with the CD spectra in the amide absorption region. The two transitions were essentially athermal in the temperature ranges, 0 to 25 degrees C for the former and -10 to 10 degrees C for the latter. The trough ellipticity for the product of the transition at the higher acetic acid concentration (DII form) very closely approached the value for the synthetic polypeptides in the beta-conformation as the temperature was lowered. Molecular weight measurements by sedimentation equilibrium indicated that the products were both monomeric. Measurements of CD spectra in the aromatic absorption region showed another transition, whose mid-concentration varied with temperature from 26% (v/v) (at about 25 degrees C) to 38% (v/v) (at -10 degrees C). A change in the hydrodynamic volume detectable by exclusion chromatography was associated with this transition only.     

Fluorescence quenching in lecithin and lecithin/cholesterol liposomes by parmagenetic lipid analogues. Introduction of a new probe approach.

1. Perylene, whether incorporated into lecithin or lecithin/cholesterol (1:1) liposomes, exhibits identical fluorescence spectra, but fluorescence in the presence of cholesterol is enhanced by 30-50%. 2. The fluorescence of perylene in pure dipalmitoyllecithin vesicles increases sharply at the transition temperature (Tt equals 41 degrees C). No such fluorescence jump is observed in lecithin/cholesterol (1:1) micelles. 3. In lecithin liposomes maximal quenching of perylene fluorescence at 25 degrees C is effected by cholestane spin label (80%) followed by androstane spin label (70%), 5-nitroxide stearate (60%) and 16-nitroxide stearate (50%). 4. In liposomes containing 5 mol % cholesterol these differences are reduced; however, the sequence of quenching efficiencies is the same except for the nitroxide stearates, which interchange their positions. 5. 5. Paramagnetic quenching of perylene fluorescence is stable below 35 degrees C and above 45 degrees C, but decreases sharply about the phase-transition temperature of dipalmitoyllecithin. 6. In lecithin/cholesterol (1:1, molar ratio) lipsomes fluorescence quenching diminishes linearly, but only slightly, with increasing temperature. 7. Cholestane spin label and androstane spin label at concentrations of greater than 20 mol % themselves suppress the quenching discontinuity at Tt, indicating a cholesterol-like structural effect. 8. The quenching phenomena observed are attributed to a non-random accommodation of fluorophore and quencher molecules (co-clustering) below the phase transition and a statistical distribution of both impurities above Tt. 9. In the presence of cholesterol the clustering tendencies are reduced or even eliminated; this is compatible with the concept that cholesterol fluidizes the phosphatide acyl chains below the transtion temperature.     

New fluorescence of nonenzymatically glucosylated human serum albumin

Glucosylated human serum albumin (G-HSA) obtained under incubation with glucose at 37 degrees C for 8 days showed a new fluorescence with a maximum at 430 nm, resulting in quenching of the fluorescence of only one tryptophan residue on HSA. The quantum yield of new fluorescence is 0.024 at 25 degrees C. The analysis of the excitation spectra allowed us to conclude the absence of energy transfer. In G-HSA, non-disulfide cross-linking hexamer was confirmed by SDS-PAGE.     

Luminescence of bacteriorhodopsin from Halobacterium halobium and its connection with the photochemical conversions of the chromophore

Red luminescence of purple membranes from Halobacterium halobium cells in suspension, dry film or freeze-dried preparations was studied and its emission, excitation and polarization spectra are reported. The emission spectra have three bands at 665–670, 720–730 and at 780–790 nm. The position (maximum at 580 nm) and shape of the excitation spectra are close to those of the absorption spectra. The spectra depend on experimental conditions, in particular on pH of the medium. Acidification increases the long wavelength part of the emission spectra and shifts the main excitation maximum 50–60 nm to the longer wavelength side. Low-temperature light-induced changes of the absorption, emission and excitation spectra are presented. Several absorbing and emitting species of bacteriorhodopsin are responsible for the observed spectral changes. The bacteriorhodopsin photoconversion rate constant was estimated to be about 1 · 10¹¹ s^?1 at ? 196°C from the quantum yields of the luminescence (1 · 10^?3) and photoreaction (1 · 10^?1). The temperature dependence of the luminescence quantum yield points to the existence of two or three quenching processes with different activation energies. High degree of luminescence polarization (about 45–47%) throughout the absorption and fluorescence spectra and its temperature independence show that there is no energy transfer between bacteriorhodopsin molecules and no chromophore rotation during the excitation lifetime. In carotenoid-containing membranes, energy migration from the bulk of carotenoids to bacteriorhodopsin was not found either. Bacteriorhodopsin phosphorescence was not observed in the 500–1100 nm region and the emission is believed to be fluorescence by nature.     

Characterization of lens alpha-crystallin tryptophan microenvironments by room temperature phosphorescence spectroscopy

Room temperature phosphorescence techniques were used to study the structural and dynamic features of the tryptophan residues in bovine alpha-crystallin. Upon excitation at 290 nm, the characteristic signature of tryptophan phosphorescence was observed with an emission maximum at 442 +/- 2 nm. The phosphorescence intensity decay was biphasic with lifetimes of 5.4 ms (71%) and 42 ms (29%). Phosphorescence quenching measurements strongly suggest that each component corresponds to one class of tryptophans with the more buried residues having the longer emission lifetime. Three small-molecule quenchers were surveyed, and in order of increasing quenching efficiency: iodide less than nitrite less than acrylamide. A heavy-atom effect was observed in iodide solutions, and an upper limit of 5% was placed on the quantum yield of triplet formation in iodide-free solutions, while the phosphorescence quantum yield was estimated to be approximately 3.2 x 10(-4). The temperature dependence of the phosphorescence lifetime was measured between 5 and 40 degrees C. Arrhenius plots exhibited discontinuities at 26 and 29 degrees C for the short- and long-lived components, respectively, corresponding to abrupt transitions in segmental flexibility. Denaturation studies revealed conformational transitions between 1 and 2 M guanidine hydrochloride, and 4 and 6 M urea. Long-lived phosphorescence lifetimes of 3 and 7 ms were measured in 6 M guanidine hydrochloride and 8 M urea, respectively, suggesting that some structural features are preserved even at very high concentrations of denaturant. Our studies demonstrate the sensitivity of room temperature phosphorescence spectroscopy to the structure of alpha-crystallin, and the applicability of this technique for monitoring conformational changes in lens crystallin proteins.(ABSTRACT TRUNCATED AT 250 WORDS)     

Investigations into the polymorphism of lipid A from lipopolysaccharides of Escherichia coli and Salmonella minnesota by Fourier-transform infrared spectroscopy

The polymorphism of lipid A, the endotoxic principle of the lipopolysaccharides of gram-negative bacteria, has been investigated in the fully hydrated state at temperatures between 5 degrees and 58 degrees C via Fourier-transform infrared spectroscopy. These measurements were supplemented by X-ray diffraction, fluorescence intensity techniques and differential thermal analysis. Up to three distinct phase transitions could be detected, with the main transition temperatures lying at approximately 41 degrees, 46 degrees, 44 degrees and 47 degrees C for Escherichia coli lipid A, Salmonella minnesota lipid A, and the synthetic lipid A compounds 506 and 516, respectively. 4'-Monophosphoryl-lipid A samples exhibited their main transition temperatures at considerably higher temperatures (about 52 degrees C for E. coli lipid A). The analysis of greater than CH2 stretching absorption bands as well as the wide-angle scattering behaviour of the lipid A samples showed that the main transition apparently involved the completion of hydrocarbon chain melting of lipid A, as typically observed for phospholipids. However, the phase transition behaviour was found to be much more complex than that usually observed for model phospholipid systems. Even below the main transition temperature, considerable amounts of the methylene segments of the acyl chains of lipid A were found to assume gauche conformations. These conformational changes might be related to the occurrence of up to two further transitions located at about 22 degrees, 30 degrees, 27 degrees and 25.5 degrees C (first transition) and at about 34 degrees, 42 degrees, 38.5 degrees and 40.5 degrees C (second transition) for E. coli lipid A, S. minnesota lipid A and the synthetic lipid A compounds 506 and 516, respectively. Furthermore, by the analysis of some characteristic infrared absorption bands related to the hydrophilic backbone, it could be demonstrated that the temperature-induced conformational changes occurring within the hydrocarbon chains were constantly and simultaneously accompanied by detectable rearrangements within the interfacial region and the polar head group of lipid A. The following conclusions were drawn: Up to about 30 degrees C the lipid A assemblies were supposed to adopt virtually bilayered, true lamellar arrangements, as revealed by the analysis of greater than CH2 scissoring vibrations and X-ray diffraction pattern. However, as indicated by fluorometric techniques, no stable closed vesicles seemed to be formed even under these conditions.(ABSTRACT TRUNCATED AT 400 WORDS)     

热锻炼对甘蓝幼苗叶片激发能分配的影响

以喜温凉的蔬菜甘蓝为试材,研究了热锻炼与对照甘蓝幼苗叶片光合速率和叶绿素荧光参数对高温胁迫的响应．结果表明,叶片温度在25-35℃之间,热锻炼苗和对照苗叶片叶绿素可变荧光(Ｆv)、光化学猝灭(qP)、非光化学猝灭(qN)、PSⅡ化学效率(ФPSⅡ)没有明显的变化;当叶温高于35℃时。热锻炼苗的Fv、qP和中ФPSⅡ均明显高于对照,37℃时Fv、qP和ФPSⅡ分别比对照高53％、24％和86％;qN较对照低22％,尤其是与光抑制(光破坏)有关的qNs明显降低,以维持较高的高能态猝灭(qNf)耗散过剩激发能。保护PSⅡ反应中心不受破坏。减轻了光抑制,这与热锻炼幼苗叶片在高温下具有较高的光合能力是一致的。     

Iodide penetration into lipid bilayers as a probe of membrane lipid organization.

The quenching efficiency of iodide as a penetrating fluorescence quencher for a membrane-associated fluorophore was utilized to measure the molecular packing of lipid bilayers. The KI quenching efficiency of tryptophan-fluorescence from melittin incorporated in DMPC bilayer vesicles peaks at the phase transition temperature (24 degrees C) of DMPC, whereas acrylamide quenching efficiency does not depend on temperature. The ability of iodide to penetrate the hydrocarbon region of the bilayer was examined by measuring the fluorescence quenching of the pyrene-phosphatidylcholine incorporated into DMPC vesicles (pyrene was attached to the 10th carbon of the sn-2 chain). The quenching efficiency of pyrene by iodide again shows a maximum at the lipid phase transition. We conclude that iodide penetrates the membrane hydrocarbon region at phase transition through an increased number of bilayer defects. The magnitude of change in quenching efficiency of iodide during lipid phase transition provides a sensitive technique to probe the lipid organization in membranes.     

Quenching of intrinsic tryptophan fluorescence in membranes of rat pituitary cells.

The GH4C1 strain of hormone-producing rat pituitary cells has specific receptors for the tripeptide thyrotropin-releasing hormone (TRH). Membranes prepared from GH4C1 cells show intrinsic tryptophan fluorescence which was quenched by low concentrations (10--100 nM) of TRH and Ntau-methyl TRH but not by biologically inactive analogs of TRH. Membranes from GH4C1 cells were subjected to thermal denaturation. A conformational transition was noted above 40 degrees C and an irreversible denaturation was observed at 52 degrees C. TRH-induced quenching of intrinsic fluorescence was lost completely in membranes previously incubated for 10 min at 30 degrees C while loss of [3H]-TRH binding was only about 20% at this temperature. Collisional quenching by iodide revealed that about 38% of the tryptophanyl residues in GH4C1 membranes were exposed to solvent. Quenching by TRH occurred with a shift in wavelength maximum from 336 to 342 nm suggesting that few of the tryptophanyl residues quenched by the tripeptide are totally exposed. Membranes prepared from cells preincubated with 20 nM TRH for 48 h, in which TRH receptors were decreased to 30% of control values, showed no quenching of tryptophan fluorescence in response to freshly added TRH. We conclude that the TRH-receptor interaction in GH4C1 cells is associated with a change in membrane conformation that can be measured by differential spectrofluorometry of intrinsic tryptophan fluorescence.     

Fluorescence studies of endothelin-1

Fluorescence measurements and singlet singlet energy transfer experiments on endothelin-1 provide information on the conformation of this peptide in dilute aqueous solution. The tyrosine fluorescence quantum yield in the absence of transfer (in [Phe²¹]endothelin-1) is relatively large (Φ_tyr = 0.39), indicating the side-chain is oriented away from fluorescence quenching groups such as the two disulfide bonds of the peptide. The fluorescence emission maximum (λ = 351 nm) and quantum yield (Φ_trp = 0.099) of tryptophan in endothelin-I suggests that this residue is fully accessible to the solvent and that the indole ring is not located near the fluorescence quenching histidinium moiety or the disulfide bonds.

Singlet-singlet fluorescence energy transfer measurements of the Tyr¹³/Trp²¹ intramolecular distance by both donor fluorescence quenching and relative enhancement of acceptor fluorescence yield a distance of about 12.8 ± 0.6 Å. Molecular modeling of a fully extended C-terminal hexapeptide indicates a Tyr¹³/Trp²¹ distance of about 25 Å. Thus, the C-terminal residues must bend back towards the bicyclic portion of the molecule.     

Phospholipid lateral phase separation and the partition of cis-parinaric acid and trans-parinaric acid among aqueous, solid lipid, and fluid lipid phases.

The partition of cis-parinaric acid (9,11,13,15-cis, trans, trans,cis-octadecatetraenoic acid, cis-PnA) and trans-parinaric acid (9,11,13,15-all-trans-octadecatetraenoic acid, trans-PnA) among aqueous, solid lipid, and fluid lipid phases has been measured by three spectroscopic parameters: absorption spectral shifts, fluorescence quantum yield, and fluorescence polarization. The solid lipid was dipalmitoylphosphatidylcholine (DPPC); the fluid lipid was palmitoyldocosahexaenoylphosphatidylcholine (PDPC). Mole fraction partition coefficients between lipid and water were determined by absorption spectroscopy to be for ci--PnA, 5.3 X 10(5) with a solid lipid and 9 X 10(5) with fluid lipid and, for trans-PnA, 5 X 10(6) with solid lipid and 1.7 X 10(6) with fluid lipid. Ratios of the solid to the fluid partition coefficients (Kps/f) are 0.6 +/- 0.2 for cis-PnA and 3 +/- 1 for trans-PnA. A phase diagram for codispersions of DPPC and PDPC has been constructed from the measurements of the temperature dependence of the fluorescence quantum yield and polarization of cis-PnA and trans-PnA and their methyl ester derivatives. A simple analysis based on the phase diagram and fluorescence data allows additional calculations of Kps/f's which are determined to be 0.7 +/- 0.2 for the cis probes and 4 +/- 1 for the trans probes. The relative preference of trans-PnA for solid phase lipids and its enhanced quantum yield in solid phase lipids make it sensitive to a few percent solid. The trans probes provide evidence that structural order may persist in dispersions of these phospholipids 10 degrees C or more above their transition temperature. It is concluded that measurements of PnA fluorescence polarization vs. temperature are better suited than measurements of quantum yield vs. temperature for determining phospholipid phase separation.     

Evaluation of lipid exposure of tryptophan residues in membrane peptides and proteins

Fluorescence quenching is used to gain information on the exposure of tryptophan residues to lipid in membrane-bound proteins and peptides. A protocol is developed to calculate this exposure, based on a comparison of quenching efficiency and of a fluorescence lifetime (or quantum yield) measured for a protein and for a model tryptophan-containing compound. Various methods of analysis of depth-dependent quenching are compared and three universal measures of quenching profile are derived. One of the measures, related to the area under profile, is used to estimate quenching efficiency. The method is applied to single tryptophan mutants of a membrane-anchoring nonpolar peptide of cytochrome b(5) and of an outer membrane protein A. Analysis of quenching of the cytochrome's nonpolar peptide by a set of four brominated lipids reveals a temperature-controlled reversible conformational change, resulting in increased exposure of tryptophan to lipid and delocalization of its transverse position. Kinetic quenching profiles and fluorescence binding kinetics reported by Kleinschmidt et al. (Biochemistry (1999) 38, 5006-5016) were analyzed to extract information on the relative exposure of tryptophan residues during folding of an outer membrane protein A. Trp-102, which translocates across the bilayer, was found to be noticeably shielded from the lipid environment throughout the folding event compared to Trp-7, which remains on the cis side. The approach described here provides a new tool for studies of low-resolution structure and conformational transitions in membrane proteins and peptides.     

Effect of the medium on functional and structural properties of serum albumins. IV. The state of human serum albumin in the pH range from 5 to 10

In order to investigate the effects of temperature and ionic strength on the N-B-transition and the alkaline denaturation of the human serum albumin, the pH-dependences of fluorescence position and relative yield of Trp-24 and of protein bound dye ANS were measured. The measurements were carried out at temperatures from 10 to 45 degrees C and ionic strengths (NaCl) from 0.001 to 0.2. The pH-induced structural transitions have different realization in environments of tryptophanyl and tightly bound ANS. The alkaline denaturation does not change the Trp-214 fluorescence. The N-B-transition gives rise to the slight polarity and/or mobility lowering in the Trp-214 environment (the shorter-wave-length spectral shift). Increase in the temperature and ionic strength induces the shift of the transition midpoint from ca. 8 to 8.7 and reduces the spectral shift amplitude. At low ionic strengths, the new structural transition in the Trp-214 environment is observed at pH change from 6.7 to 5.7. This transition is not observable using ANS fluorescence. The N-B-transition is accompanied by an enhancement and longer-wavelength shift of the ANS fluorescence spectra. The transition midpoint is independent of temperature, but is shifted to lower pH values at a decrease of ionic strength value. At ionic strengths less than or equal to 0.01 the shorter-wavelength spectral shift is seen at pH from 7.5 to 9, which seems to reflect the disulfide B-A-isomerisation. The alkaline denaturation gives rise to the sharp quenching of ANS fluorescence, probably due to the ANS binding site decomposition.(ABSTRACT TRUNCATED AT 250 WORDS)     

The primary event in vision investigated by time-resolved fluorescence spectroscopy.

The picosecond fluorescence kinetics and quantum yield from bovine rhodopsin were measured in the 5-40 degrees K range. The fluorescence rise and decay times are faster than our resolution of 15 ps (full width at half maximum) over this entire temperature range. The size of the observed emission was also temperature independent, and we find that the upper limit of rhodopsin's fluorescence quantum yield to be phi f approximately equal to 10(-5). Replacing all of rhodopsin's exchangeable protons with deuterons by suspending rhodopsin in D2O had no effect on either the kinetics of the emission or the value of the quantum yield. Our data provide strong confirmation of the idea that the first step in the visual process is an excited-state cis-to-trans isomerization about the C11-C12 double bond of retinal.