QUENCHING OF PYRENE FLUORESCENCE BY TRYPTOPHAN IN MICELLAR SOLUTIONS

Deactivation of excited pyrene incorporated to cationic (cetyltrimethylammonium chloride), anionic (sodium dodecyl sulfate) and neutral (Triton X-100) micelles by tryptophan has been investigated over a wide pH range. Data obtained allow an estimation of the tryptophan association to the micelles, of the tryptophan apparent p K in the micellar solutions, and of the dynamics of tryptophan incorporation to the micellar pseudophase. In particular, the data obtained at pH 7 allow an estimation of the effect of the micellar charge upon the binding capacity of the tryptophan zwitterion.     

TIME-RESOLVED FLUORESCENCE SPECTRA OF TRYPTOPHAN IN MONOMERIC GLUCAGON*

Abstract— The fluorescence decay of tryptophan-25 in monomeric glucagon at pH 8.2 was measured at a series of emission wavelengths using pulsed laser excitation and single photon counting techniques. Double exponential kinetics were consistently observed, with time constants 3.26 and 1.11 ns. This allowed the steady-state emission spectrum to be resolved into two components with differing intensities but similar emission maxima near 350 nm. Decay parameters were almost unchanged in the presence of 5.5 M guanidinium chloride. The dual emission is thought to reflect different conformers of the indole ring or of the peptide chain.     

KINETIC STUDIES OF THE TRYPTOPHAN TRIPLET STATE IN SOLID FILM AND IN WOOL KERATIN

Abstract— The triplet state of tryptophan in the solid environments of a polyvinyl alcohol) (PVA) film and the protein wool keratin has been studied by emission and absorption spectroscopy at room temperature. The decay kinetics of the triplet state vary depending on the conditions under which the study is made. The observation of second order kinetics suggests triplet-triplet interactions play a major role in the deactivation of the tryptophan triplet state in PVA films plasticised by the presence of water vapour. For wool keratin in the presence of air the major mechanism appears to be a first order reaction between tryptophan residues and oxygen. The actual effects of moisture and oxygen on the tryptophan triplet state are discussed.     

RESOLUTION OF SPECTRAL AND LIFETIME HETEROGENEITY OF TRYPTOPHAN FLUORESCENCE IN BACTERIORHODOPSIN

Abstract— The picosecond time-resolved fluorescence decay of bacteriorhodopsin (BR) was analyzed by the maximum entropy method. Results showed five distributions of lifetimes indicating at least five decay components. A wavelength-dependent study of emission decay of BR was carried out in the wavelength region from 310 to 390 nm. The decay at each wavelength was resolvable into four decay components by the discrete exponential analysis. The three short lifetime components (100 ± 20 ps, 400 ± 50 ps and 1.0 ± 0.1 ns) were independent of wavelength, whereas the longest lifetime component was wavelength dependent (varying from 4.1 ns at 310 nm to 5.7 ns at 390 nm). These results are inconsistent with the existing model of associating the fluorescence of bacteriorhodopsin with two or four lifetime components. An attempt is made to associate the five decay components with the emitting tryptophans of BR.     

FLUORESCENCE AND THE LOCATION OF TRYPTOPHAN RESIDUES IN PROTEIN MOLECULES

Abstract— Fluorescence spectra of a number of native and denaturated proteins have been analysed, using spectral band width (ΔΛ), spectral maximum position (Λ_m), fluorescence quenching by external ionic quenchers, lifetime (b), and quantum yield ( q ) and its changes upon denaturation. The results enabled a model of fluorescence properties of tryptophan residues in the proteins to be substantiated by considering the existence of three discrete spectral classes, one buried in nonpolar regions of the protein (Λ_m 330–332 nm, ΔΛ= 48–49nm, q 0.11, τ= 2.1 ns) and two on the surface. One of the latter is completely exposed to water (Λ_m# 350–353 nm, ΔΛ= 59–61 nm, q # 0.2, τ= 5.4 ns); the other is in limited contact with water which is probably immobilized by bonding at the macromolecular surface (Λ_m# 340–342 nm, ΔΛ= 53–55 nm, q # 0.3, = 4.4 ns). Some quantitative predictions from the model, for (a) the fraction of fluorescence that is quenched by ionic quenchers, (b) the mean values of quantum yield, and (c) the mean values of fluorescence lifetime for various proteins, show good concordance with independent experimentally determined values.     

DISTANCE-DEPENDENT FLUORESCENCE QUENCHING OF TRYPTOPHAN BY ACRYLAMIDE

Abstract We used GHz frequency-domain fluorometry to investigate the time-dependent intensity decays of N -acetyl -L-trytophanamide (NATA) when collisionally quenched by acrylamide in propylene glycol at 20°C. The intensity decays of NATA became increasingly heterogeneous in the presence of acrylamide. The NATA intensity decays were not consistent with the Collins-Kimball radiation boundary condition (RBC) model for quenching. The steady-state Stern-Volmer plots show significant upward curvature. At low temperature in vitrified propylene glycol (-60%), where translational diffusion cannot occur during the lifetime of the excited state, quenching of NATA by acrylamide was observed. The Smoluchowski and RBC quenching models do not predict any quenching in the absence of translational diffusion. Hence, these frequency-domain and steady-state data indicate a through-space quenching interaction between NATA and acrylamide. The rate for quenching of NAT A by acrylamide appears to depend exponentially on the fluorophore-quencher separation distance. Comparison of the time-resolved and steady-state data provides a sensitive method to determine the distance dependence of the fluorophore-quencher interaction. The distance-dependent rate of quenching also explains the upward curvature of the Stern-Volmer plot, which is often observed for quenching by acrylamide. These results suggest that the distance-dependent quenching rates need to be considered in the interpretation of quenching data of proteins by acrylamide.     

FLUORESCENCE OF TYROSINE AND TRYPTOPHAN IN PROTEINS USING ONE- AND TWO-PHOTON EXCITATION

Abstract— We examined the emission spectra of tyrosine- and tryptophan-containing proteins using one-photon (270–310 nm) and two-photon (565–610 nm) excitation. Emission spectra for two-photon excitation of native and denatured human serum albumin and of three purine nucleoside phosphorylases indicated an absence of the tyrosine emission normally seen for one-photon excitation below 290 nm. We examined the one-photon and two-photon excitation spectra of tyrosine-tryptophan mixtures to determine the origin of selective excitation of the tryptophan residues. These results confirmed a short-wavelength shift of the tyrosine two-photon excitation spectrum relative to that of tryptophan, as recently reported by Rehms and Callis (1993) Chem. Phys. Lett . 208 , 276–282.     

A COMPARISON OF FLUORESCENCE QUENCHING AND FLUORESCENCE DECAY STUDIES WITH TRYPTOPHAN

Abstract— The quenching of the fluorescence of aqueous tryptophan solutions has been studied as a function of emission wavelength using acrylamide as a collisional quencher. Our quenching studies are consistent with recent observations of the heterogeneity of tryptophan fluorescence, but they show a slight discrepancy when compared to certain analyses of the decay of tryptophan fluorescence in terms of two components.     

TRYPTOPHAN FLUORESCENCE LIFETIMES AS A FUNCTION OF EXCITATION WAVELENGTH*

Abstract— –Fluorescence decay times of aqueous dilute solutions (?20 µM) of L-tryptophan have been determined using the phase shift technique as well as single photon-counting coupled with synchrotron radiation (ACO at Orsay and SPEAR at Stanford). Decay times were obtained as a function of the excitation wavelength (in the spectral region 220–320 nm) monitoring emission of λ> 320 nm (in certain specified cases, λ> 360 nm). We have found that, at neutral pH and 20°C. fluorescence decays are single exponentials and independent of the excitation wavelength; under these conditions we find τ= 3.1 ± 0.1 ns.     

TYROSYL FLUORESCENCE SPECTRA OF PROTEINS LACKING TRYPTOPHAN: EFFECTS OF INTRAMOLECULAR INTERACTIONS

Abstract— The fluorescence spectra of class A proteins which lack tryptophanyl residues were examined in detail, and revealed some differences in the position of maximum and half-width of the tyrosine emission band between proteins and tyrosine itself. These parameters were affected by conformational changes in protein molecules (denaturation, thermal effects, ion binding) which also induced variations in absorption spectra and fluorescence quantum yields. These observations are thought to be related to the formation of hydrogen bonds between the hydroxyl group of the tyrosyl residues and proton acceptor groups in the protein.     

AN EVALUATION OF CHARGE EFFECTS ON THE QUENCHING OF TRYPTOPHAN FLUORESCENCE IN SMALL PEPTIDES BY IODIDE ION

Abstract— Charge effects on the quenching of tryptophan fluorescence in small peptides by iodide ion have been analyzed by the conventional "static" quenching model and by a recently proposed competitive quenching model. The former involves a fit of the quenching data using two quenching parameters—one for dynamic and one for static quenching contributions. The latter model involves a single parameter fit in which the fitting parameter is the characteristic rate constant for quenching of the fluorescent state. Both models indicate a clear charge effect on the efficiency of quenching by iodide ion. However, the static model results are obscured by the interdependence of the two fitting parameters and the fact that the true physical meaning of the static parameter is uncertain. Rate constants derived from the competitive model can be converted into relative quenching efficiencies. These efficiencies, which vary by more than a factor of two for the molecules studied, are greatest when the positive charge is on the tryptophan and least when this residue contains a negative charge.     

A NEW FLUORESCENT PHOTOPRODUCT OF TRYPTOPHAN EVIDENCED BY LONG WAVELENGTH EXCITATION OF FLUORESCENCE

Abstract— Besides the normal tryptophan (Trp) fluorescence in aqueous solution (emission maximum at 350 nm), a new emission, peaking around 380 nm, appears by long wavelength excitation. Its fluorescence yield (φ_s 0.24) is higher than that of tryptophan (φ_Trp= 0.13). The growth of this emission is observed under different experimental conditions, mainly under UV anaerobic irradiation. To explain this observation, the formation of a C₃-hydroxylated derivative is tentatively suggested.     

EXCITATION-ENERGY TRANSFER BETWEEN TYROSINE AND TRYPTOPHAN IN PROTEINS EVALUATED BY THE SIMULTANEOUS MEASUREMENT OF FLUORESCENCE AND ABSORBANCE

Abstract— The efficiencies of the excitation–energy transfer from tyrosine to tryptophan residues in eight globular proteins in the native and denatured states are obtained by studying the wavelength dependence of the fluorescence quantum yield. The measurements are made over a wide wavelength range using a computer-controlled spectrophotometer which can measure the fluorescence and absorbance simultaneously in one sample solution (Wada et al. , 1980). The values of the energy transfer efficiencies ranged from 0.17 ± 0.12 to 0.69 ± 0.06 in the native state and from -0.04 ± 0.09 to 0.12 ± 0.06 in the denatured state. These values are considerably lower than the values reported by Kronman and Holmes (1971); in particular, an almost complete absence of energy transfer for the denatured state is shown.     

DIRECT RECORDING OF THE INITIALLY EXCITED AND THE SOLVENT RELAXED FLUORESCENCE EMISSION SPECTRA OF TRYPTOPHAN BY PHASE SENSITIVE DETECTION OF FLUORESCENCE

Abstract Phase sensitive detection of fluorescence was used to directly record the initially excited and the solvent-relaxed emission spectra of N-acetyl-L-tryptophanamide in propylene glycol. Emission from the initially excited state was suppressed by adjusting the phase sensitive detector to be out of phase with the emission on the short wavelength side of the fluorescence spectrum. Then, the phase sensitive intensities revealed the emission spectrum of the solvent relaxed state. Similarly, the emission from the solvent relaxed state was suppressed by adjusting the detector to be out of phase with the emission on the long wavelength side of the spectrum, allowing the spectrum of the initially excited state to be directly recorded. Distinct emission spectra could be recorded when the solvent relaxation time was comparable to the fluorescence lifetime. At higher or lower temperatures, emission occurs predominantly from a single state, and suppression of the fluorescence signal at any arbitrary wavelength resulted in suppression of the entire emission. A simple theory is described which allows the spectral relaxation times to be estimated from the phase sensitive intensities. From this analysis we obtained an activation energy for spectral relaxation of 3 kcal/mol. This activation energy is smaller than that found for the temperature dependence of fluorescence depolarization, 7.8 kcal/mol. We attribute this difference to the smaller molecular motions required for spectral relaxation.
The method of phase sensitive detection of fluorescence shows excellent resolving power and sensitivity, and this method should facilitate measurement of spectral relaxation around tryptophan residues in proteins.     

THE PHOTOLYSIS OF TRYPTOPHAN IN THE PRESENCE OF OXYGEN

Abstract— Quantum yields for the destruction of tryptophan by a single 500 J flash in aqueous solution have been determined over the pH range 1–13 in both air-equilibrated and nitrogen-saturated conditions. When these quantum yields are compared with the quantum yields for radical formation and photoejection of electrons, it is found that there is good agreement only for the nitrogen-saturated case. In air-equilibrated solutions of tryptophan, there is a large disparity between the measured degradation quantum yields and those for photoejection of electrons and radical formation. Oxygen, therefore, is playing a major role in the photochemical decomposition and it is proposed that the major reaction which occurs, under normal atmospheric conditions, is the reaction of the lowest triplet excited state of tryptophan with oxygen.
Preliminary photolysis-product distributions against pH are discussed, and indicate that a total of nine major products are formed in the presence of oxygen.     

低聚壳聚糖与角质层蛋白相互作用的体外研究

以脱脂鼠角质层和提取角蛋白为模型,利用电化学交流阻抗谱、SEM、DSC、FTIR等手段,研究了低聚壳聚糖及氨基葡萄糖与角质层蛋白之间的相互作用.结果发现,氨基葡萄糖溶液处理不影响脱脂角质层膜的阻抗,而低聚壳聚糖溶液处理却可明显降低脱脂角质层膜的阻抗,阻抗值由3.79×106Ω·cm2降至8.379×105Ω·cm2.此外,壳聚糖溶液和氨基葡萄糖溶液都可明显破坏角蛋白表面致密均匀的结构,并使得角蛋白二级结构中α-螺旋结构含量减少,同时推动角蛋白α-螺旋结构向β-折叠结构和无规则卷曲结构转变.这些结果表明低聚壳聚糖与角质层蛋白相互作用,一方面可有效降低鼠角质层结构的紧密程度,另一方面可影响角蛋白的微结构,使其结构松散并出现微细孔道,从而为药物的经皮吸收与传送疏通了通道.     

DEUTERIUM-ISOTOPE EFFECT ON THE FLUORESCENCE YIELDS AND LIFETIMES OF INDOLE DERIVATIVES–INCLUDING TRYPTOPHAN AND TRYPTAMINE

Abstract— The fluorescence yields and lifetimes of indole, five of its alkyl detivatives, tryptophan, and tryptamine have been determined in degassed, heavy and light water at room temperature. All of the compounds have radiative lifetimes nearly identical to the parent compound indole, and a comparison of these results with recently reported data on tryptophyl derivatives disclosed a striking uniformity in radiative lifetimes between indole and many amino acids and peptides which contain the indole group as the fluorescence unit. The fluorescence rate k _f in H₂O, was found to be 4.5 × 10⁷ sec^-1. The nonradiative decay rates were found to vary between 5.1 and 46 × 10⁷ sec^-1 and from a study of the deuterium-solvent isotope effect and the deuterium-substituent effect a mechanism for nonradiative deactivation is proposed which includes an isotopically dependent proton transfer and a pathway involving energy loss via the ring carbon hydrogen vibrations. Tryptophan at pH 7 was found to have a unique nonradiative decay scheme not evidenced at a pH 1 or pH 10.     

PHOTOSENSITIZATION OF METHYL LINOLEATE OXIDATION BY TRYPTOPHAN IN PEPTIDES

The ability of tryptophan in peptides to photosensitize the oxidation of methyl linoleate (ML) was evaluated. Purified ML was irradiated (λ > 270 nm) alone or in the presence of a tryptophan-containing peptide in ethanol solution. Oxidation was monitored by measuring the dienc hydroperoxides formed from ML by high performance liquid chromatography. N-acetylphenylalanyltryptophan (NAPT) and N-acetyltryptophan were about 2-fold more effective as photosensitizers than leucyltryptophan and tryptophylleucine. N-acetylphenylalanyltryptophan photolyzed in ethanol to form multiple photoproducts including N-formylkynurenine-type compounds. However, the NAPT photoproducts did not photosensitize the oxidation of ML and N-formylkynurenine was about 8% as effective as NAPT. Sodium azide partially quenched the photooxidation sensitized by NAPT.     

PRIMARY PRODUCTS IN THE FLASH PHOTOLYSIS OF TRYPTOPHAN*

There has been considerable interest in the photochemistry of tryptophan in connection with ultraviolet inactivation of enzymes. Earlier flash photolysis work has demonstrated that the hydrated electron (e^-_aq) is an initial product in the irradiation of indole derivatives, accompanied by a longer-lived transient absorption near 500 nm attributed to an aromatic radical species[1–5]. Similar transients were observed in a recent flash photolysis study of lysozyme[6] in which it was proposed that inactivation is a consequence of electron ejection from 1 to 2 essential tryptophan residues in the active center. However, there has been uncertainty concerning the tryptophan radical structure and its relationship to the triplet state and radical spectra reported for tryptophan photolysis in low-temperature rigid media. This note reports a flash photolysis investigation of L-tryptophan (Trp) and 1-Methyl-L-tryptophan (1-MeTrp) undertaken to clarify these points. The flash photolysis apparatus and methods employed are described in Ref. [6].     

POLARIZATION OF FLUORESCENCE OF RIBOFLAVIN IN ANISOTROPIC MEDIUM

Abstract— The dichroism and anisotropy of emission of polyvinyl alcohol (PVA) film with riboflavin (RF) were measured. The short axis of the RF molecule seems to be oriented in the direction of stretching of the film. The transition moment of the weak absorption band at 300 nm is also parallel to this direction, but it forms an angle greater than 50° with the emission oscillator. The transition moments of absorption bands at 440 , 360 and 270 nm are intermediate in direction between long and short axes of the RF molecule. The extinction at 360 nm probably involves more than one electronic transition. Angles between absorption oscillators are very close to those obtained by Song and Kurtin. The mode of orientation of RF molecules suggests appearance of some type of binding between RF and the PVA matrix.