Mast cell-lysosomal cationic protein interaction: effects of metabolic inhibitors and decay of activated cells on enhanced fluorescence of anilinonaphthalene sulfonate

It has been shown earlier that the interactions of the isolated rat peritoneal mast cells with cationic protein from rabbit neutrophil lysosomes (band 2 protein) can be studied using anilinonaphthalene sulfonate (ANS) as a fluorescent probe. In the present communication, binding of ANS dye to the mast cells interacting of histamine release by metabolic inhibitors was found to have no effect on enhancement of ANS fluorescence. On the other hand, inhibition of histamine release at high concentration of Ca2+ (14.4 mM) was accompanied by the decrease in enhance fluorescence. In the presence of 7.2 mM of Sr2+, the release of histamine was enhanced with small but significant increase in ANS fluorescence. The cells heated to 42 degrees C partially lost their capacity to release histamine without the loss of enhanced fluorescence. The mast cells interacting with B2 at 10 degrees C for various time intervals showed time-dependent loss in histamine releasing capacity with concomitant loss in enhanced fluorescence. These studies suggest that the enhancement of ANS fluorescence is associated with the early events of the cell membrane caused by interaction of B2 with the cells. The extracellular cations significantly influence this early event.     

Virus inactivation by anilinonaphthalene sulfonate compounds and comparison with other ligands

Bis-(8-anilinonaphthalene-1-sulfonate) (bis-ANS) causes inactivation of vesicular stomatitis virus (VSV) at micromolar concentrations while butyl-ANS and ANS are effective at concentrations one and two orders of magnitude higher, respectively. VSV fully inactivated by the combined effects of 10 microM bis-ANS and 2.5 kbar hydrostatic pressure elicited a high titer of neutralizing antibodies. Incubation of VSV with >/=2 M urea at atmospheric pressure caused very little virus inactivation, whereas at a pressure of 2.5 kbar, 1 M urea caused inactivation that exceeded by more than two orders of magnitude the sum of the inactivating effects produced by urea and pressure separately. Measurements of bis-ANS fluorescence showed that increasing the urea concentration reduces the pressure required to disrupt the structure. We conclude that anilinonaphthalene sulfonate compounds inactivate VSV by a mechanism similar to that produced by pressure. The most effective antiviral compound was bis-ANS which can be used for the preparation of safe viral vaccines or as an antiviral drug eventually.     

Time-resolved fluorescence studies of flavodoxin. Fluorescence decay and fluorescence anisotropy decay of tryptophan in Desulfovibrio flavodoxins

The time-resolved fluorescence characteristics of tryptophan in flavodoxin isolated from the sulfate-reducing bacteria Desulfovibrio vulgaris and Desulfovibrio gigas have been examined. By comparing the results of protein preparations of normal and FMN-depleted flavodoxin, radiationless energy transfer from tryptophan to FMN has been demonstrated. Since the crystal structure of the D. vulgaris flavodoxin is known, transfer rate constants from the two excited states ¹ L _a and ¹ L _b can be calculated for both tryptophan residues (Trp 60 and Trp 140). Residue Trp 60, which is very close to the flavin, transfers energy very rapidly to FMN, whereas the rate of energy transfer from the remote Trp 140 to FMN is much smaller. Both tryptophan residues have the indole rings oriented in such a way that transfer will preferentially take place from the ¹ L _a excited state. The fluorescence decay of all protein preparations turned out to be complex, the parameter values being dependent on the emission wavelength. Several decay curves were analyzed globally using a model in which tryptophan is involved in some nanosecond relaxation process. A relaxation time of about 2 ns was found for both D. gigas apo- and holoflavodoxin. The fluorescence anisotropy decay of both Desulfovibrio FMN-depleted flavodoxins is exponential, whereas that of the two holoproteins is clearly non-exponential. The anisotropy decay was analyzed using the same model as that applied for fluorescence decay. The tryptophan residues turned out to be immobilized in the protein. A time constant of a few nanoseconds results from energy transfer from tryptophan to flavin, at least for D. gigas flavodoxin. The single tryptophan residue in D. gigas flavodoxin occupies a position in the polypeptide chain remote from the flavin prosthetic group. Because of the close resemblance of steady-state and time-resolved fluorescence properties of tryptophan in both flavodoxins, the center to center distance between tryptophan and FMN in D. gigas flavodoxin is probably very similar to the distance between Trp 140 and FMN in D. vulgaris flavodoxin (i.e. 20 Å). Offprint requests to: A.J.W.G. Visser     

Intracellular pH-determination by fluorescence measurements.

A method was developed to determine the intracellular pH (pHi) of individual cells by use of fluorescence measurements. The method is based on the observation that the fluorescence excitation spectrum of fluorescein is pH-dependent. Fluorescence excitation spectra from individual rat bone marrow cells treated with fluorescein diacetate (FDA) were compared with those of fluorescein solutions of known pH values. Cells which were suspended in media of pH between 4.0 and 8.1 with high to normal buffering capacities had pHi values equal to those of the media. Cells suspended in media with low buffering capacities maintained a pH,i of 6.7 +/- 0.2. Preliminary results indicated that the pHi of individual cells may also be determined by using flow cytometry.     

The application of time decay characteristics of laser‐induced fluorescence in the classification of vegetation

In this study, the time decay of the chlorophyll fluorescence intensity (TDCFI) of vegetation was measured based on laser‐induced fluorescence (LIF) technology with a 355 nm laser serving as the excitation light source. The pseudo‐color diagram of the TDCFI (PDTDCFIs) was proposed for use as a characteristic fingerprint for the analysis of various plant species based on variations in the fluorescence intensity over time. Compared with the steady‐state fluorescence spectra, two‐dimensional PDTDCFIs contained more spectral information, including variations in both the shape of the laser‐induced fluorescence spectra and the relative intensity. The experimental results demonstrated that the PDTDCFIs of various plant species show distinct differences, and this was successfully applied in the classification of plant species. Therefore, the PDTDCFIs of plants could provide researchers with a more reliable and useful tool for the characterization of vegetation. Copyright © 2016 John Wiley & Sons, Ltd.     

Anilinonaphthalene sulfonate fluorescence and amino acid transport in yeast

Summary Fluorescence of 1-anilinonaphthalene-8-sulfonate in yeast membranes appears to be caused predominantly by binding to lipids (ANS_proteinANS_lipid120) as indicated by the fluorescence lifetime, degree of polarization, and excitation spectra. It was insensitive to short-circuiting the membrane potential. Fluorescence intensity increased as cells (especially after pretreatment with energy donors such as glucose) were exposed to some amino acids, in particular, aspartic and glutamic acids. The character of fluorescence shifted to that of protein-bound ANS, suggesting an exposure of new protein sites accessible to the probe. This shift could be prevented by inhibitors of energy transduction as well as of transport. TheK _1/2 of the shift was at 2.5mm aspartic acid.     

Intracellular dye heterogeneity determined by fluorescence lifetimes

The cellular localization of a fluorescent probe molecule depends on both the chemical structure of the dye and the cellular environment. To study the number and types of environments in an epithelial cell line, we have measured in Madin-Darby canine kidney (MDCK) cells the fluorescence lifetimes of three structurally distinct fluorescent dyes — rhodamine-B, 3,3′-dihexadecylindocarbocyanine-(C₃) (diI), and Collarein — incorporated into these cells. The latter is a rhodamine-cardiolipin conjugate that we designed and synthesized for the property of exclusive localization in the plasma membrane. The former two dyes required at least two exponential components to fit their fluorescence decay curves, while the decay of Collarein was characterized by a single exponential. These data are consistent with fluorescence microscopic observations, in which diI and rhodamine-B exhibit heterogeneous spatial distributions, while Collarein appears to be located on the cell surface.     

F/F deconvolution of fluorescence decay data

An approach for the deconvolution of multiexponential fluorescence decay data in which a single exponential decay is used in place of the usual excitation profile is described. For analysis by the method of moments, the resulting decay lifetimes are identical to those in the multiexponential decay, while the pre-exponential factors are a simple function of the true values and the parameters of the single exponential decay. This approach, which we call the F/F deconvolution method, is capable of eliminating the errors in decay analyses which arise from the wavelength dependence of the instrument response function.     

Orientational exchange approach to fluorescence anisotropy decay.

Fluorescence depolarization is a powerful technique in resolving dynamics of molecular systems. Data obtained in fluorescence depolarization experiments are highly complex. Mathematical models for analyzing data from depolarization due to rotational motion have been largely based on the rotational diffusion equation. These results have been verified by Monte Carlo simulations. It has been implicitly stated that a 90 degrees jump model between predefined orientations such as presented by G. Weber (1971. J. Chem. Phys. 55:2399-2411) should, for the specific case of fluorescence depolarization, give the same answer as the diffusion equation. Since the highly symmetric cases considered by G. Weber gave the same result as the diffusion equation, it has been desirable to use this method in cases where depolarization arises from both discrete processes and rotational diffusion. We have derived, in a compartmental formalism, the general result for excitation and emission dipoles not necessarily coincident with any of the principal rotational axes of the fluorophore from this exchange model, and have found it to be different from that of the diffusion equation approach. We have also verified this difference with a Monte Carlo simulation of our exchange model. This derivation allows us to define the limits of validity of the 90 degrees exchanges to model rotational diffusion. Also, for systems where movements may be jumps between a few preferred orientations, the actual physical mechanism of depolarization may not be accurately represented by continuous diffusion. The compartmental formalism developed here can be used to easily combine rotational motions with discrete position jumps or other level kinetics.(ABSTRACT TRUNCATED AT 250 WORDS)     

Analysis of fluorescence decay kinetics measured in the frequency domain using distributions of decay times

We describe the theoretical and practical aspects of analyzing complex fluorescence decay kinetics using continuous distributions of decay times. Our analysis uses frequency-domain data, provides for global analysis of multiple data sets and includes the possibility of excited-state processes. Simulated data were used to estimate the types of distributions which can be reasonably recovered from the measurements. Additionally, we describe a variety of distributions recovered from experimental data. For mixtures of one, two or three exponentially decaying fluorophores we recovered narrow lifetime distributions, which are essentially identical to a multiexponential decay. Similarly, a two-state excited-state reaction also yielded a narrow distribution with negative preexponential factors. The presence of time-dependent spectral relaxation of labeled lipids results in a wide distribution of decay times, which becomes narrower for faster relaxation rates at higher temperatures. Hence, the decay-time distributions appear to be sensitive to the dynamics of the environment surrounding the fluorophore. Additionally, distributions of decay times were observed to result from transient effects in collisional quenching, from energy transfer in the presence of a range of donor-to-acceptor distances, and for several single-tryptophan proteins.     

On the wobbling-in-cone analysis of fluorescence anisotropy decay.

Interpretation of fluorescence anisotropy decay for the case of restricted rotational diffusion often requires a model. To investigate the extent of model dependence, two models are compared: a strict cone model, in which a fluorescent probe wobbles uniformly within a cone, and a Gaussian model, where the stationary distribution of the probe orientation is of a Gaussian type. For the same experimental anisotropy decay, analysis by the Gaussian model predicts a smaller value for the rate of wobbling motion than the strict cone analysis, but the difference is 35% at most; the cone angle obtained by the strict cone analysis agrees closely with the effective width of the Gaussian distribution. The results suggest that, when only two parameters (the rate and the angular range) are extracted from an experiment, the choice of a model is not crucial as long as the model contains the essential feature, e.g., the more-or-less conical restriction, of the motion under study. Model-independent analyses are also discussed.     

A theory of fluorescence polarization decay in membranes.

Decay of fluorescence polarization after an impulsive excitation is correlated with wobbling motion of fluorescent molecules in membranes. The motion is characterized by two parameters, a "wobbling diffusion constant" and a "degree of orientational constraint" both of which can be determined directly from experimentally obtained decay. Detailed discussion, including theoretically calculated time-courses of polarization decay, is given for several types of molecules embedded in lipid bilayers; these types cover a large part of fluorescent probes available at present. The theory is useful for the analysis of fluorescence polarization decay in any system where the orientation of fluorophore is restricted by the surrounding structure.     

Analytical approach to the recovery of short fluorescence lifetimes from fluorescence decay curves.

Considerable effort in instrument development has made possible detection of picosecond fluorescence lifetimes by time-correlated single-photon counting. In particular, efforts have been made to narrow markedly the instrument response function (IRF). Less attention has been paid to analytical methods, especially to problem of discretization of the convolution integral, on which the detection and quantification of short lifetimes critically depends. We show that better discretization methods can yield acceptable results for short lifetimes even with an IRF several times wider than necessary for the standard discretization based on linear approximation (LA). A general approach to discretization, also suitable for nonexponential models, is developed. The zero-time shift is explicitly included. Using simulations, we compared LA, quadratic, and cubic approximations. The latter two proved much better for detection of short lifetimes and, in that respect, they do not differ except when the zero-time shift exceeds two channels, when one can benefit from using the cubic approximation. We showed that for LA in some cases narrowing the IRF beyond FWHM = 150 ps is actually counterproductive. This is not so for quadratic and cubic approximations, which we recommend for general use.     

The temperature dependence of the fluorescence decay of low-density lipoproteins

The decay of the intrinsic tryptophan fluorescence of low-density lipoproteins (LDL) is measured using a picosecond laser system with an excitation wavelength of 295 nm. The emission wavelengths were observed at 320, 340 and 360 nm. The measurements were performed in the temperature range 10–45°C. The fluorescence decay data are analysed in terms of: (i) three exponentials; (ii) a continuous distribution of exponentials; and (iii) the average decay time. The results indicate that the tryptophans are in a non-polar environment and that the fluorescence is not affected by phase transitions found to occur in the lipid core of the LDL molecule.