Fluorescence lifetime and quenching studies on some interesting diphenylhexatriene membrane probes

The fluorescence lifetimes of a number of membrane probes based on the 1,6-diphenylhexatriene (DPH) chromophore have been measured in small unilamellar phospholipid vesicles and found to be multiphasic. These probes were quenched by sodium iodide with different efficiencies in vesicles and this has been attributed to the depth of the particular probe in the bilayer. The distribution of the probe between the outer and inner monolayer has been determined for those probes with fixed positions in the bilayer. The iodide ion permeability of the bilayer was found to be immeasurably small over a 3 h period.     

Fluorescence lifetime quenching and anisotropy studies of ribonuclease T1

The time-resolved fluorescence of the lone tryptophanyl residue of ribonuclease T1 was investigated by using a mode-locked, frequency-doubled picosecond dye laser. The fluorescence decay could be characterized by a single exponential function with a lifetime of 3.9 ns. The fluorescence was readily quenched by uncharged solutes but was unaffected by iodide ion. These observations are interpreted in terms of the electrostatic properties of the amino acid residues at the active site of the protein, which would appear to restrict the access of solute species to the tryptophanyl residue. The temperature dependence of the fluorescence lifetime and anisotropy decay time could be rationalized in terms of a model which postulates a significant ordering of the solvent layer immediately surrounding the surface of the protein.     

Fluorescence quenching studies with proteins

A review is presented on the use of the technique of solute fluorescence quenching to study the structure and dynamics of proteins. A number of factors are discussed that must be considered in analyzing such data. Among these factors are the efficiency of the quenching process, the relative importance of static quenching, the heterogeneity of the emission, and the tendency of the quencher to interact with the protein.     

Fluctuation domains in myoglobin. Fluorescence quenching studies

The dynamics of two domains in the myoglobin molecule, close to the heme and inside the protein medium including the surface, are investigated through the study of the fluorescence oxygen quenching of two probes imbedded in the heme pocket: zinc protoporphyrin IX (with a fluorescence lifetime of 2.1 ns) and metal-free protoporphyrin IX (with a fluorescence lifetime of 17.8 ns).     

Fluorescence studies on the active sites of proteinases

Summary Recent studies on the interaction of several proteinases (pepsin, papain, chymotrypsin, trypsin, thermolysin) with specific substrates or inhibitors bearing a fluorescent probe group have shown that the extended active sites of these enzymes differ in their conformational flexibility. In addition the use of such extrinsic probe groups, measurements of changes in the intrinsic tryptophan fluorescence, and of the energy transfer from tryptophan to a probe group, have given further information about the flexibility of the active sites of proteinases.     

Fluorescence quenching studies of Trp repressor-operator interaction

Steady-state quenching and time-resolved fluorescence measurements of L-tryptophan binding to the tryptophan-free mutant W19/99F of the tryptophan repressor of Escherichia coli have been used to observe the coreperessor microenvirnment changes upon ligand binding. Using iodide and acrylamide as quenchers, we have resolved the emission spectra of the corepressor into two components. The bluer component of L-tryptophan buried in the holorepressor exhibits a maximum of the fluorescence emission at 336 nm and can be characterized by a Stern–Volmer quenching constant equal to about 2.0–2.3 M^–1. The second, redder component is exposed to the solvent and possesses the fluorescence emission and Stern–Volmer quenching constant characteristic of L-tryptophan in the solvent. When the Trp holorepressor is bound to the DNA operator, further alterations in the corepressor fluorescence are observed. Acrylamide quenching experiments indicate that the Stern–Volmer quenching constant of the buried component of the corepressor decreases drastically to a value of 0.56 M^–1. The fluorescence lifetimes of L-tryptophan in a complex with Trp repressor decrease substantially upon binding to DNA, which indicates a dynamic mechanism of the quenching process.     

Fluorescence lifetime imaging.

We describe a new fluorescence imaging methodology in which the image contrast is derived from the fluorescence lifetime at each point in a two-dimensional image and not the local concentration and/or intensity of the fluorophore. In the present apparatus, lifetime images are created from a series of images obtained with a gain-modulated image intensifier. The frequency of gain modulation is at the light-modulation frequency (or a harmonic thereof), resulting in homodyne phase-sensitive images. These stationary phase-sensitive images are collected using a slow-scan CCD camera. A series of such images, obtained with various phase shifts of the gain-modulation signal, is used to determine the phase angle and/or modulation of the emission at each pixel, which is in essence the phase or modulation lifetime image. An advantage of this method is that pixel-to-pixel scanning is not required to obtain the images, as the information from all pixels is obtained at the same time. The method has been experimentally verified by creating lifetime images of standard fluorophores with known lifetimes, ranging from 1 to 10 ns. As an example of biochemical imaging we created life-time images of Yt-base when quenched by acrylamide, as a model for a fluorophore in distinct environments that affect its decay time. Additionally, we describe a faster imaging procedure that allows images in which a specific decay time is suppressed to be calculated, allowing rapid visualization of unique features and/or regions with distinct decay times. The concepts and methodologies of fluorescence lifetime imaging (FLIM) have numerous potential applications in the biosciences. Fluorescence lifetimes are known to be sensitive to numerous chemical and physical factors such as pH, oxygen, temperature, cations, polarity, and binding to macromolecules. Hence the FLIM method allows chemical or physical imaging of macroscopic and microscopic samples.     

Fluorescence quenching studies of nitrated polycyclic aromatic hydrocarbons

The analysis of nitrated polycyclic aromatic hydrocarbons (NPAHs) is of great importance because of the mutagenicity and possible carcinogenic activity of these compounds, which are distributed widely in the environment. Nitro‐substituents in aromatic compounds are known to quench fluorescence and NPAHs have no intrinsic fluorescence, but they can be determined using their quenching effects on other fluorophores. The quenching effects of several important NPAHs on 1,2,3,4‐ tetrahydro‐1‐naphthol,5,6,7,8‐tetrahydro‐1‐naphthol,4‐(2‐hydroxy‐4‐sulfo‐1‐naphthylazo)‐2‐naphthalene carboxylic acid and 7‐amino‐4‐methyl coumarin have been studied. The singlet emission of these fluorophores is efficiently quenched by all the NPAHs, the quenching following the Stern–Volmer relationship. Quenching constants and the limits of detection and linear ranges of the quenchers have been determined in each case: the limits of detection are ca 1 µm . Copyright © 2010 John Wiley & Son, Ltd.     

Fluorescence quenching studies on binding fluoreno-9-spiro-oxazolidinedione to human serum albumin.

Human serum albumin fluorescence quenching by fluorene-9-spiro-oxazolidinedione has been analyzed as a function of temperature. Such temperature dependence suggests that the mechanism of the quenching process is static in origin. This type of quenching implies that a non-fluorescent complex between oxazolidinedione and serum albumin has been formed and following the Stern-Volmer relationship we have calculated the binding constant. Thermodynamic parameters were also determined. The positive and large values of entropy and the negative value for enthalpy suggest that both hydrophobic and electrostatic interactions may play an important role in the stabilization of the complex. Finally, the irreversible changes in the spectral properties of HSA are interpreted in binding terms.     

Fluorescence lifetime imaging system for in vivo studies

In this article, a fluorescence lifetime imaging system for small animals is presented. Data were collected by scanning a region of interest with a measurement head, a linear fiber array with fixed separations between a single source fiber and several detection fibers. The goal was to localize tumors and monitor their progression using specific fluorescent markers. We chose a near-infrared contrast agent, Alexa Fluor 750 (Invitrogen Corp., Carlsbad, CA). Preliminary results show that the fluorescence lifetime for this dye was sensitive to the immediate environment of the fluorophore (in particular, pH), making it a promising candidate for reporting physiologic changes around a fluorophore. To quantify the intrinsic lifetime of deeply embedded fluorophores, we performed phantom experiments to investigate the contribution of photon migration effects on observed lifetime by calculating the fluorescence intensity decay time. A previously proposed theoretical model of migration, based on random walk theory, is also substantiated by new experimental data. The developed experimental system has been used for in vivo mouse imaging with Alexa Fluor 750 contrast agent conjugated to tumor-specific antibodies (trastuzumab [Herceptin]). Three-dimensional mapping of the fluorescence lifetime indicates lower lifetime values in superficial breast cancer tumors in mice.     

Accessibilities of the sulfhydryl groups of native and photooxidized lens crystallins: a fluorescence lifetime and quenching study

Fluorescence lifetime and acrylamide quenching studies on the N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl)ethylenediamine (1,5-IAEDANS)-labeled sulfhydryl groups of bovine lens alpha-, beta H-, and gamma-crystallins were carried out to characterize the microenvironment of the sulfhydryls and changes produced by singlet oxygen mediated photooxidation. For the untreated proteins, the lifetimes of the major decay component of the fluorescence-labeled crystallins were 15.2, 14.4, and 13.0 ns, and the quenching rate constant, kq, values were 16.6 x 10(7), 26.9 x 10(7), and 32.7 x 10(7) M-1 s-1 for alpha-, beta H-, and gamma-crystallins, respectively. The results indicate that as the polarity of the sulfhydryl site increased (i.e., its lifetime decreased), its accessibility to collisional quenching by acrylamide also increased. The minor decay component of the fluorescence label was not significantly quenched by acrylamide for all three classes of crystallins. When the proteins were irradiated in the presence of methylene blue, in a system generating singlet oxygen, the kq value for acrylamide quenching of the major decay component of alpha-crystallin decreased to zero, while its lifetime decreased to 6 ns. Neither the lifetime nor the kq of alpha-crystallin recovered completely in the presence of the singlet oxygen quencher sodium azide. Light-induced binding of the photosensitizer methylene blue to the crystallins was observed by absorption spectroscopy. The bound photosensitizer partially quenches the fluorescence lifetime of the N-acetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine (AEDANS) label in irradiated alpha-crystallin. Further decrease in the lifetime occurs as a result of the singlet oxygen mediated conformational change. The results suggest that the fluorescence lifetime of the AEDANS is fully quenched in the irradiated alpha-crystallin and there is no further quenching by acrylamide. An increase in the fraction of the minor component of beta H-crystallin which was inaccessible to acrylamide quenching was observed after irradiation. There was no effect of irradiation on the kq for acrylamide quenching of the major component of the decay of AEDANS bound to beta H- or gamma-crystallins. Static quenching was found to contribute significantly to the steady-state quenching plots of the polar sulfhydryl sites of irradiated alpha-crystallin and of untreated and irradiated beta H- and gamma-crystallins, but it had no detectable role in the case of untreated alpha-crystallin. Fluorescence anisotropy of the AEDANS label bound to the crystallins was higher in the irradiated crystallins as compared with the controls.     

Fluorescence lifetime analysis of DNA intercalated ethidium bromide and quenching by free dye

The fluorescence characteristics of ethidium bromide (Eb) complexed to calf thymus DNA have been examined using fluorescence lifetime analysis for a range of DNA (effective nucleotide concentration) to Eb molar ratios. Control of both temperature and ion concentration is necessary for reproducible analyses. Eb complexed to double stranded DNA has a maximum fluorescence lifetime of 23 ns and is easily distinguishable from a fluorescence lifetime value of 1.67 ns corresponding to unbound Eb. In a solution of calf thymus DNA containing excess Eb a binding equilibrium is reached, and this corresponds to one Eb molecule for every five nucleotides. With increasing amounts of unbound Eb, the fluorescence lifetime of the DNA-Eb complex decreases with a concomitant drop in the steady state fluorescence intensity, without a change in the amount of Eb bound to DNA. It is concluded that unbound Eb, acting via a quenching mechanism, shortens the fluorescence lifetime of bound Eb and consequently decreases the overall fluorescence intensity. This means that a different approach is necessary: time-resolved fluorescence spectroscopy directly distinguishes between a decrease in fluorescence intensity due to quenching by an excess of unbound Eb from that due to a decrease in Eb binding to double-stranded DNA. These studies suggest that techniques which measure total steady state fluorescence intensity of bound Eb in order to infer relative amounts of double-stranded DNA must be interpreted with caution. For such assays to be valid it is essential that no unbound Eb be present; otherwise a variable correction factor is required to account for unbound Eb.     

Fluorescence quenching studies of Trp repressor using single-tryptophan mutants

Time-resolved and steady-state fluorescence have been used to resolve the heterogeneous emission of single-tryptophan-containing mutants of Trp repressors W19F and W99F into components. Using iodide as the quencher, the fluorescence-quenching-resolved spectra (FQRS) have been obtained The FQRS method shows that the fluorescence emission of Trp99 can be resolved into two component spectra characterized by maxima of fluorescence emission at 338 and 328 nm. The redder component is exposed to the solvent and participates in about 21% of the total fluorescence emission of TrpR W19F. The second component is inacessible to iodide, but is quenched by acrylamide. The tryptophan residue 19 present in TrpR W99F can be resolved into two component spectra using the FQRS method and iodide as a quencher. Both components of Trp19 exhibit similar maxima of emission at 322–324 nm and both are quenchable by iodide. The component more quenchable by iodide participates in about 38% of the total TrpR W99F emission. The fluorescence lifetime measurements as a function of iodide concentration support the existence of two classes of Trp99 and Trp19 in the Trp repressor. Our results suggest that the Trp aporepressor can exist in the ground state in two distinct conformational states which differ in the microenvironment of the Trp residues.Abbreviations TrpR tryptophan aporepressor fromE. coli - TrpR W19F TrpR mutant with phenylalanine substituted for tryptophan at position 19 - TrpR W99F TrpR mutant with phenylalanine substituted for tryptophan at position 99 - FQRS fluorescence-quenching-resolved spectra - FPLC fast protein liquid chromatography     

Fluorescence lifetime distributions in proteins.

The fluorescence lifetime value of tryptophan residues varies by more than a factor of 100 in different proteins and is determined by several factors, which include solvent exposure and interactions with other elements of the protein matrix. Because of the variety of different elements that can alter the lifetime value and the sensitivity to the particular environment of the tryptophan residue, it is likely that non-unique lifetime values result in protein systems. The emission decay of most proteins can be satisfactorily described only using several exponential components. Here it is proposed that continuous lifetime distributions can better represent the observed decay. An approach based on protein dynamics is presented, which provides fluorescence lifetime distribution functions for single tryptophan residue proteins. First, lifetime distributions for proteins interconverting between two conformations, each characterized by a different lifetime value, are derived. The evolution of the lifetime values as a function of the interconversion rate is studied. In this case lifetime distributions can be obtained from a distribution of rates of interconversion between the two conformations. Second, the existence of a continuum of energy substates within a given conformation was considered. The occupation of a particular energy substate at a given temperature is proportional to the Boltzmann factor. The density of energy states of the potential well depends upon the width of the well, which determines the degree of freedom the residue can move in the conformational space. Lifetime distributions can be obtained by association of each energy substate with a different lifetime value and assuming that the average conformation can change as the energy of the substate is increased.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence quenching studies on the interaction of riboflavin with tryptophan and its analytical application

The ineraction between riboflavin (RBF) and tryptophan (Trp) was investigated using fluorescence spectroscopy and UV–vis absorption spectroscopy under physiological conditions. The fluorescence of Trp was quenched by RBF via dynamic quenching, which was analyzed using the Stern–Volmer relation. The value of the Forster distance R₀ (2.31 nm) was obtained according to the Forster's theory of nonradiative energy transfer. Under physiological conditions, a linear relationship could be established between the quenched fluorescence intensity of Trp and the concentration of RBF in the range of 5.8 × 10^‐7–2.0 × 10^‐5 mol/L. The detection limit was 1.8 × 10^‐7 mol/L. The method was successfully applied to determine riboflavin concentrations in pharmaceutical samples. Copyright © 2012 John Wiley & Sons, Ltd.     

Fluorescence quenching studies of bovine growth hormone in several conformational states

The use of steady-state fluorescence quenching methods is reported as a probe of the accessibility of the single fluorescent tryptophan residue of bovine growth hormone (bGH, bovine somatotropin, bSt) in four solution-state conformations. Different bGH conformations were prepared by using previous knowledge of the multi-state nature of the equilibrium unfolding pathway for bGH: alterations in denaturant and protein concentration yielded different bGH conformations (native, monomeric intermediate, associated intermediate and unfolded). Because the intramolecular fluorescence quenching which occurs in the native state is reduced when the protein unfolds to any of the other conformations, steady-state fluorescence intensity measurements can be used to monitor bGH unfolding as well as the formation of the associated intermediate. These steady-state intensity changes have been confirmed with fluorescence lifetime measurements for the different conformational states of bGH. Fluorescence quenching results were obtained using the quenchers iodide (ionic), acrylamide (polar) and trichloroethanol (non-polar). Analysis of the results for native-state bGH reveals that the tryptophan environment is slightly non-polar (in agreement with the emission maximum of 335 nm) and the tryptophan is more exposed to acrylamide than most native-state tryptophan residues which have been studied. The tryptophan is most accessible to all quenchers in the unfolded state, because no steric restrictions inhibit quencher interaction with the tryptophan residue. The iodide quenching results indicate that the associated intermediate tryptophan is not accessible to iodide, probably due to negative charges inhibiting iodide penetration. The associated intermediate tryptophan is less accessible to all three quenchers than the monomeric intermediate tryptophan, due to tight packing of molecules in the associated intermediate state.     

Fluorescence lifetime imaging: association of cortical actin with a PIP3-rich membrane compartment

We have used fluorescence lifetime imaging (FLIM) to study actin and plasma membrane dynamics in B16-F1 melanoma cells. In the absence of a FRET acceptor, significant changes in the fluorescence lifetime of GFP were induced simply by linking the fluorophore to different functional probes, including beta-actin, the PH domains of PLCdelta and Akt, the Ras farnesylation signal, and the neuromodulin palmitoylation signal (MEM). In contrast, the lifetime of GFP-actin was constant despite the many different local environments of G- and F-actin within the cell. Treatment with cytochalasin D but not latrunculin A significantly shortened the lifetime of GFP-beta-actin in the absence of a FRET acceptor. Robust lifetime shifts were observed using either a GFP-RFP chimera or co-transfection of GFP-MEM with RFP-MEM. In contrast to previous reports we observed a photobleaching-dependent change in the lifetime of GFP which could complicate the interpretation of FRET experiments. Of the membrane probes tested only the fluorescence lifetime of GFP-Akt was influenced by the presence of mRFP-actin, suggesting that the cortical actin meshwork is associated with a PIP3-enriched compartment of the plasma membrane. These results will aid in the design of new FRET-based approaches to study cytoskeletal interactions at the molecular level.