Anisotropy-based sensing with reference fluorophores

We describe a new approach to fluorescence sensing based on measurements of steady-state anisotropies in the presence of reference fluorophores with known anisotropies. The basic concept is that the anisotropy of a mixture reflects a weighted average of the anisotropies of the emitting species. By use of reference fluorophores the starting anisotropy can be near zero, or near 0.9 for oriented films which contain the reference fluorophore. Changing intensities of the analyte result in changes in anisotropy. A wide dynamic range of anisotropies is available because of the freedom to select high or low starting values. Anisotropy-based sensing was demonstrated for pH using 6-carboxyfluorescein and for protein affinity or immunoassay using an oriented film with high anisotropy and a protein labeled with a metal-ligand complex. The latter measurements were performed with a simple light-emitting diode excitation source without an excitation polarizer. The sensitive range of the assay can be adjusted by changing the intensity of the reference fluorophore. Anisotropy-based sensing can have numerous applications in clinical and analytical chemistry.     

Kinetic properties of prompt and delayed fluorescence of chlorophyll a with λmax= nm when electron transport is blocked on acceptor side of photosystem II

This work is a theoretical consideration of steady-state kinetics of prompt and delayed fluorescence of chlorophyll a entering into the pigment matrices of photosynthetic units of photosystem II when the electron transport from the primary to secondary acceptor of this system is blocked. It has been shown that in such a system of quantum yields of prompt and delayed fluorescence are complementary. At low intensities of excitation light the quantum yield of delayed fluorescence is several times more than that of prompt fluorescence. With an increase in the light intensity the reverse situation is observed. The literature data given sustain the results obtained. it has also been unambiguously shown what values, when changed, may be responsible for the corresponding changes in prompt and delayed fluorescence yields.     

Applying 6-Methylisoxanthopterin-Enhanced Fluorescence To Examine Protein-DNA Interactions in the Picomolar Range

Incorporation of fluorescent nucleoside analogues into duplex DNA usually leads to a reduction in quantum yield, which significantly limits their potential use and application. We have identified two pentamer DNA sequences containing 6-methylisoxanthopterin (6-MI) (ATFAA and AAFTA, where F is 6-MI) that exhibit significant enhancement of fluorescence upon formation of duplex DNA with quantum yields close to that of monomeric 6-MI. The enhanced fluorescence dramatically increases the utility and sensitivity of the probe and is used to study protein-DNA interactions of nanomolar specificity in this work. The increased sensitivity of 6-MI allows anisotropy binding measurements to be performed at DNA concentrations of 1 nM and fluorescence intensity measurements at 50 pM DNA. The ATFAA sequence was incorporated into DNA constructs to measure the binding affinity of four different protein-DNA interactions that exhibit sequence-specific and non-sequence-specific recognition. In all cases, the K(d) values obtained were consistent with previously reported values measured by other methods. Time-resolved and steady-state fluorescence measurements demonstrate that 6-MI fluorescence is very sensitive to local distortion and reports on different degrees of protein-induced perturbations with single-base resolution, where the largest changes occur at the site of protein binding.     

Characterization of the substrate-induced conformational change of N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine-labeled sarcoplasmic reticulum Ca2(+)-ATPase by using different kinds of substrate

Cys-674 of the sarcoplasmic reticulum Ca2(+)-ATPase was labeled with N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine without a loss of the catalytic activity, and changes in the fluorescence intensity upon addition of seven kinds of substrate were followed by the stopped-flow method. The steady-state fluorescence intensity and anisotropy were also determined. When Ca2+ was present, the fluorescence intensity and anisotropy decreased greatly upon addition of any substrate used. The observed affinity for each substrate agreed with the previously observed affinity of the catalytic site. The fluorescence drop induced by the adenine nucleotides, ATP and adenosine 5'-(beta, gamma-methylene)triphosphate (a nonhydrolyzable ATP analog), was much faster than that induced by other substrates. The ATP-induced fluorescence drop preceded phosphoenzyme formation when the ATP concentration was high, but the fluorescence drop coincided with phosphoenzyme formation when it was slowed by reducing ATP concentrations. The fluorescence drop induced by ITP or acetyl phosphate was slow even at high concentrations of the substrate, and it coincided with phosphoenzyme formation. When Ca2+ was absent, the fluorescence intensity and anisotropy decreased only slightly upon addition of any substrate other than the adenine nucleotides. They decreased substantially upon addition of the adenine nucleotides, but the kinetics of this fluorescence drop were quite different from that of the fluorescence drop induced by any substrate in the presence of Ca2+. These results show that the conformational change, which makes the bound label less constrained, is induced by substrate binding to the catalytic site of the Ca2(+)-activated enzyme. This change precedes phosphoenzyme formation in the catalytic cycle and is greatly accelerated by the adenine moiety of the substrate.     

Studies of the early photoactive forms of the chlorophyll precursor in the plant leaves using fluorescence spectroscopy at 20°C

Using fluorescence spectroscopic method, accumulation of several forms of the chlorophyll precursor at the early stages of their formation at 20°C has been observed, due to the lowered intensity of the excitation light applied for inhibition of the photoreaction. A high quantum yield of the initial fluorescence of the short-wavelength (638 nm) form of the embryonic leaves sharply falls down with the accumulation of the pigment precursor. The fluorescence yield of its main form with a maximum at 653 nm is decreased less drastically. At the temperature of ?196°C, an intensive increase in fluorescence yield is observed, particularly pronounced (10-fold) for the main 655 nm form of the precursor. Changes in the fluorescence spectra observed in the course of the photoconversion testify to the fact that at the early stages of the chlorophyll biosynthesis only the first of two sequential reactions of photoreduction proceeds in vivo. A complicated character of the kinetic curves of fluorescence in the course of the photoreaction is attributable to the effects of the concentration change and changes in the quantum yields of the converting forms.     

Membrane dynamic alterations associated with viral transformation and reversion. Decay of fluorescence emission and anisotropy studies of 3T3 cells.

Fluorescence lifetimes, anisotropies and rotational correlation time values of 1,6-diphenyl-1,3,5-hexatriene (DPH) in membranes of normal, transformed, and revertant 3T3 cells were determined by nanosecond (nsec), photon counting spectrofluorimetry. No change in lifetime values with transformation or reversion is observed. Fluorescence anisotropy decay curves show at least two components; an initial relatively fast decay and a non-zero “plateau” level component. The observed changes in the average anisotropy values, which qualitatively follow steady-state fluorescence polarization values, is due primarily to changes in the non-zero “plateau” level component. The anisotropy decay curves suggest that the rotational motion of the probe is restricted to a limited angular range. The present results are compared with model membrane systems.     

The Effect of Fluorophore Conjugation on Antibody Affinity and the Photophysical Properties of Dyes

Because the degree of labeling (DOL) of cell-bound antibodies, often required in quantitative fluorescence measurements, is largely unknown, we investigated the effect of labeling with two different fluorophores (AlexaFluor546, AlexaFluor647) in a systematic way using antibody stock solutions with different DOLs. Here, we show that the mean DOL of the cell-bound antibody fraction is lower than that of the stock using single molecule fluorescence measurements. The effect is so pronounced that the mean DOL levels off at approximately two fluorophores/IgG for some antibodies. We developed a method for comparing the average DOL of antibody stocks to that of the isolated, cell-bound fraction based on fluorescence anisotropy measurements confirming the aforementioned conclusions. We created a model in which individual antibody species with different DOLs, present in an antibody stock solution, were assumed to have distinct affinities and quantum yields. The model calculations confirmed that a calibration curve constructed from the anisotropy of antibody stocks can be used for determining the DOL of the bound fraction. The fluorescence intensity of the cell-bound antibody fractions and of the antibody stocks exhibited distinctly different dependence on the DOL. The behavior of the two dyes was systematically different in this respect. Fitting of the model to these data revealed that labeling with each dye affects quantum yield and antibody affinity differentially. These measurements also implied that fluorophores in multiply labeled antibodies exhibit self-quenching and lead to decreased antibody affinity, conclusions directly confirmed by steady-state intensity measurements and competitive binding assays. Although the fluorescence lifetime of antibodies labeled with multiple fluorophores decreased, the magnitude of this change was not sufficient to account for self-quenching indicating that both dynamic and static quenching processes occur involving H-aggregate formation. Our results reveal multiple effects of fluorophore conjugation, which must not be overlooked in quantitative cell biological measurements.     

Nanosecond fluorescence anisotropy decays of 1,6-diphenyl-1,3,5-hexatriene in membranes.

Nanosecond decays of the fluorescence anisotropy, r, were studied for the emission of 1,6-diphenyl-1,3,5-hexatriene (DPH) embedded in a series of mixed multilamellar liposomes containing egg yolk phosphatidylcholine, phosphatidylethanolamine and cholesterol in varying molar ratios, as well as in membranes of intact cells and in virus envelopes. The relative contributions of the fast and the infinitely slow decaying component to the steady-state value r, of the fluorescence anisotropy were very similar for artifical and biological membranes. Angles, theta, of the cone, by which the motion of the fluorescent molecule is limited, were calculated from the intensity of the infinitely slow decaying anisotropy component and compared with steady-state fluorescence anisotropies and with 'microviscosities', (eta). An increase in (eta) from 1.5 to 5.2 P in our systems was accompanied by a decrease in theta from 49 degrees to 30 degrees while the decrease in the mean motional relaxation times, phi f, of the label molecule was not more than 1 ns and due mainly to changes in the potential, by which the diffusion of DPH in the membrane is restricted. From these observations we conclude that differences in the steady-state fluorescence anisotropy and in 'microviscosities' of cholesterol-containing membranes (r greater than 0.15) represent changes in the degree of static orientational constraint rather than changes in diffusion rates of the label.     

Cooperativity in oxidation reactions catalyzed by cytochrome P450 1A2: highly cooperative pyrene hydroxylation and multiphasic kinetics of ligand binding

Rabbit liver cytochrome P450 (P450) 1A2 was found to catalyze the 5,6-epoxidation of alpha-naphthoflavone (alphaNF), 1-hydroxylation of pyrene, and the subsequent 6-, 8-, and other hydroxylations of 1-hydroxy (OH) pyrene. Plots of steady-state rates of product formation versus substrate concentration were hyperbolic for alphaNF epoxidation but highly cooperative (Hill n coefficients of 2-4) for pyrene and 1-OH pyrene hydroxylation. When any of the three substrates (alphaNF, pyrene, 1-OH pyrene) were mixed with ferric P450 1A2 using stopped-flow methods, the changes in the heme Soret spectra were relatively slow and multiphasic. Changes in the fluorescence of all of the substrates were much faster, consistent with rapid initial binding to P450 1A2 in a manner that does not change the heme spectrum. For binding of pyrene to ferrous P450 1A2, the course of the spectra revealed sequential changes in opposite directions, consistent with P450 1A2 being involved in a series of transitions to explain the kinetic multiphasicity as opposed to multiple, slowly interconverting populations of enzyme undergoing the same event at different rates. Models of rabbit P450 1A2 based on a published crystal structure of a human P450 1A2-alphaNF complex show active site space for only one alphaNF or for two pyrenes. The spectral changes observed for binding and hydroxylation of pyrene and 1-OH pyrene could be fit to a kinetic model in which hydroxylation occurs only when two substrates are bound. Elements of this mechanism may be relevant to other cases of P450 cooperativity.     

High-sensitivity fluorescence anisotropy detection of protein-folding events: application to alpha-lactalbumin

An experimental procedure has been devised to record simultaneously fluorescence intensity and fluorescence anisotropy. A photoelastic modulator on the excitation beam enables the anisotropy signal to be recorded in one pass using a single photomultiplier tube and eliminates the need for a polarizer on the emission path. In conjunction with a stopped-flow mixer, providing a time-resolved capability, this procedure was used to study the refolding of apo alpha-lactalbumin following dilution from guanidinium chloride. Although the fluorescence intensity does not change detectably, the fluorescence anisotropy was found to resolve the conformational changes occurring between the initial unfolded state and the molten globule state formed either kinetically during refolding at pH 7.0 or at equilibrium at pH 2.0 (A-state). This result provides further evidence that fluorescence anisotropy is a valuable probe of protein structural transitions and that the information it provides concerning the rotational mobility of a fluorophore can be complementary to the information about the local environment provided by fluorescence intensity.     

Global analysis of steady-state polarized fluorescence spectra using trilinear curve resolution.

Global analysis using trilinear curve resolution is described and shown to be a powerful method for the resolution of polarized fluorescence data arrays, in which the measured fluorescence intensity is a separable function of polarization orientation, excitation wavelength, and emission wavelength. This methodology is applicable to mixtures the components of which have linearly independent excitation and emission spectra and distinct anisotropies. Normalized excitation and emission spectra of individual components can be uniquely determined without prior assumptions concerning spectral shapes (e.g., sum of Gaussians) and without the uncertainties inherent in bilinear techniques such as principal component analysis or factor analysis. The normalized excitation and emission vectors are combined with the total absorption spectrum of the multicomponent mixture to compute absolute absorption and emission spectra. The precision of this methodology is evaluated as a function of noise, overlap, relative intensity, and anisotropy difference between components using simulated mixtures of the DNA bases. The ability of this method to extract individual spectra from steady-state fluorescence data arrays is illustrated for mixtures containing two and three components.     

Confocal microscopic dual-laser dual-polarization FRET (2polFRET) at the acceptor side for correlating rotations at different distances on the cell surface

Relationship of donor and acceptor fluorescence anisotropies as well as efficiency of fluorescence resonance energy transfer (FRET) has been investigated in a confocal microscope in the context of FRET systems comprised of donor and acceptor-labeled MHCI and MHCII receptors on the surface of Kit-225 K6 human T-cells. The measurements have been carried out in a 2-laser, 5-signal platform where the total donor fluorescence intensity and 2 acceptor fluorescence intensities with their anisotropies – one at the donor's excitation wavelength, the other at the acceptor's excitation wavelength – have been detected. This configuration enabled the determination of FRET efficiency and correlating it with the two acceptor fluorescence anisotropies as a kind of calibration. Estimations for the FRET-enhanced donor fluorescence anisotropy, the directly excited acceptor fluorescence anisotropy, and the fluorescence anisotropy of sensitized emission have been obtained. Procedures for determining FRET by measuring only the total donor intensity and the acceptor intensity and its anisotropy, or two acceptor intensities and their anisotropies have been elaborated, the errors of which have been estimated based on the fluorescence anisotropy values obtained in the calibration with the method of flow cytometric energy transfer (FCET).The combined detection of the donor and acceptor fluorescence anisotropies enabled also the determination of the lower and upper limits of the orientation factor for FRET (κ²). An increase in range for κ² with increasing FRET efficiency has been observed, with average κ² values different from the dynamic random average of 2/3. These observations call for the need of κ² determination in proximity measurements, where the donor and acceptor orientations are not predictable.An increasing range of κ² with increasing intermolecular proximity of the MHCI and MHCII receptors has been observed. This indicates that molecular flexibility in the clusters of the MHCI and MHCII receptors reduces with increasing cluster density, i.e. a “fluidity gradient” exists in the clusters. More specifically, the local density dependent flexibility can also be taken as a direct proof for that the association of these receptors is non-random, but mediated by some type of physical interaction, a finding as a benefit of FRET detection by polarization spectroscopy.Two new quantities – the quenched donor fluorescence anisotropy and a fluorescence anisotropy analogue, the “dissymmetry index” of the polarized FRET efficiency components – have also been introduced for the characterization of the orientational dynamics of the excited state during FRET.     

Changes in the steady-state fluorescence anisotropy of N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine attached to the specific thiol of sarcoplasmic reticulum Ca2+-ATPase throughout the catalytic cycle

Cys674 of the sarcoplasmic reticulum Ca2+-ATPase was selectively labeled with N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine without a loss of the catalytic activity, and the steady-state fluorescence anisotropy of this label and its total fluorescence intensity were followed throughout the catalytic cycle. At 25 degrees C, the anisotropy and the total fluorescence intensity increased by 2.1 and 9.4%, respectively, upon Ca2+ binding to the high affinity sites. Upon subsequent ATP binding to the catalytic site, the anisotropy and the total fluorescence intensity decreased by 6.8 and 23.9%, respectively. These drops likely occurred in the enzyme.ATP complex. The extents of changes upon additions of Ca2+ and ATP in the anisotropy, but not in the total fluorescence intensity, were greatly reduced by lowering the temperature. Slight drops in the anisotropy and the total fluorescence intensity occurred upon conversion of phosphoenzyme (EP) from the ADP-sensitive form to the ADP-insensitive form. The anisotropy and the total fluorescence intensity returned to the initial level when EP was hydrolyzed. Mg2+-dependent Pi-induced drops in the anisotropy and the total fluorescence intensity occurred coincidently with EP formation from Pi. These demonstrate that the ATP-induced drops in the anisotropy and the total fluorescence intensity are predominant throughout the catalytic cycle. Most probably, the changes in the anisotropy are due to changes in the rotational diffusion of the label. These findings indicate that ATP binding to the catalytic site induces a relaxed conformation in the microenvironment of the label bound to Cys674.     

A fluorescence study of dehydroergosterol in phosphatidylcholine bilayer vesicles

The fluorescent sterol delta 5,7,9(11),22-ergostatetraen-3 beta-ol (dehydroergosterol) was incorporated into 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) small unilamellar vesicles (SUV) with and without cholesterol in order to monitor sterol-sterol interactions in model membranes. In the range 0-5 mol % fluorescent sterol, dehydroergosterol underwent a concentration-dependent relaxation characterized by red-shifted wavelengths of maximum absorption as well as altered ratios of absorbance maxima and fluorescence excitation maxima at 338 nm/324 nm. Fluorescence intensity per mole of dehydroergosterol increased up to 5 mol % in POPC vesicles. In contrast, quantum yield, steady-state anisotropy, limiting anisotropy, lifetime, and rotational rate remained relatively constant in this concentration range. Similarly, addition of increasing cholesterol in the range 0-5 mol % in the presence of 3 mol % dehydroergosterol also increased the fluorescence intensity per mole of dehydroergosterol, red-shifted wavelengths of maximum absorption, and altered ratios of absorbance maxima. In POPC vesicles containing between 5 and 33 mol % dehydroergosterol, the fluorescent dehydroergosterol interacted to self-quench, thereby decreasing the fluorescence intensity, quantum yield, steady-state anisotropy, and limiting anisotropy and increasing the rotational rate (decreased rotational relaxation time) of the fluorescent sterol. The fluorescence lifetime of dehydroergosterol remained unchanged. The results were in accord with the interpretation that below 5 mol% sterol, the sterols behaved as monomers exposed to some degree to the aqueous solvent in POPC bilayers.(ABSTRACT TRUNCATED AT 250 WORDS)     

Kinetics of the E. coli replication factor DnaC protein-nucleotide interactions. II. Fluorescence anisotropy and transient,dynamic quenching stopped-flow studies of the reaction intermediates

The nature of the intermediates in the binding of MANT-ATP and MANT-ADP to the E. coli replicative factor DnaC protein (accompanying paper) has been examined using the fluorescence intensity, anisotropy, and transient dynamic quenching stopped-flow techniques. Using molar fluorescence intensities of individual intermediates of the reaction, we derived the Stern-Volmer equation that provides a direct method to quantitatively address the quenching of the fluorescence of a transient intermediate by an external, neutral quencher. The data indicate that in the first intermediate, (C)(1), the solvent has full access to the MANT group. Thus, the nucleotide-binding site is located on the surface of the protein, fully open to the solvent. Moreover, formation of the first intermediate does not affect the structure of the binding site. On the other hand, in the second intermediate, (C)(2), the entire binding site changes its conformation, resulting in diminished access of the solvent to the bound nucleotide. The time course of the fluorescence anisotropy in the reaction provides direct, unique insight into the mobility of bound nucleotides in each intermediate. The analysis is facilitated by the fact that the anisotropy can be expressed as a function of the relative molar intensities and steady-state anisotropies of the individual intermediates. The major decrease of the nucleotide mobility occurs in the formation of the first intermediate and reflects the fact that the MANT group is immobilized to a similar extent as the ribose region of the bound nucleotides. Transition to the second intermediate and closing of the binding site leads to only a moderate, additional decrease of nucleotide mobility. The temperature effect on the studied interactions indicates that the formation of individual intermediates is accompanied by very different enthalpy and entropy changes predominantly generated from the structural changes of the protein. Analysis of the salt effect indicates that the net release of a single ion, observed in equilibrium studies, occurs in the formation of the first intermediate. The lack of any salt effect on the (C)(1) <--> (C)(2) transition indicates that the closing of the binding site does not include a net ion release or uptake. Moreover, prior to the nucleotide binding, the conformational transition of the DnaC protein is exclusively controlled by the nucleotide binding and release.     

Mismatched and matched dNTP incorporation by DNA polymerase beta proceed via analogous kinetic pathways

While matched nucleotide incorporation by DNA polymerase beta (Pol beta) has been well-studied, a true understanding of polymerase fidelity requires comparison of both matched and mismatched dNTP incorporation pathways. Here we examine the mechanism of misincorporation for wild-type (WT) Pol beta and an error-prone I260Q variant using stopped-flow fluorescence assays and steady-state fluorescence spectroscopy. In stopped-flow, a biphasic fluorescence trace is observed for both enzymes during mismatched dNTP incorporation. The fluorescence transitions are in the same direction as that observed for matched dNTP, albeit with lower amplitude. Assignments of the fast and slow fluorescence phases are designated to the same mechanistic steps previously determined for matched dNTP incorporation. For both WT and I260Q mismatched dNTP incorporation, the rate of the fast phase, reflecting subdomain closing, is comparable to that induced by correct dNTP. Pre-steady-state kinetic evaluation reveals that both enzymes display similar correct dNTP insertion profiles, and the lower fidelity intrinsic to the I260Q mutant results from enhanced efficiency of mismatched incorporation. Notably, in comparison to WT, I260Q demonstrates enhanced intensity of fluorescence emission upon mismatched ternary complex formation. Both kinetic and steady-state fluorescence data suggest that relaxed discrimination against incorrect dNTP by I260Q is a consequence of a loss in ability to destabilize the mismatched ternary complex. Overall, our results provide first direct evidence that mismatched and matched dNTP incorporations proceed via analogous kinetic pathways, and support our standing hypothesis that the fidelity of Pol beta originates from destabilization of the mismatched closed ternary complex and chemical transition state.     

Dynamic depolarization of interacting fluorophores. Effect of internal rotation and energy transfer.

Effects of internal rotation on the fluorescence decay functions and time-dependent anisotropies of fluorophores bound to a spherical macromolecule are theoretically investigated in the presence of the intramolecular energy transfer interaction by solving relevant rotational diffusion equations. The model system examined is one in which the energy donor is internally rotating around an axis fixed at the macromolecule and the acceptor is fixed at a definite position in the macromolecule. The effect of internal rotation in the system is described by Hill's functions with two cosine terms. The fluorescence decay function and anisotropy decay are functions of the ratio of energy-transfer probability averaged over the internal rotation angle to the rotary diffusion co-efficient. When the internal rotation is much faster than energy transfer, the decay function of the donor is predicted to be a single exponential, and the anisotropy decay is essentially described by the expression derived by Gotlieb and Wahl (1963. J. Chim. Phys. 60:849-856). However, deviation from it becomes pronounced as the rotation becomes slower. Methods of numerical analysis are presented for decay function and anisotropy decay, as well as relative quantum yield and polarization anisotropy under steady-state excitation, and examined for a simplified system under the variation of the diffusion coefficient.     

The effects of cholesterol on the time-resolved emission anisotropy of 12-(9-anthroyloxy)stearic acid in dipalmitoylphosphatidylcholine bilayers

The time-resolved fluorescence emission anisotropy of 12-(9-anthroyloxy)stearic acid (12-AS) and 1,6-diphenyl-1,3,5-hexatriene (DPH) have been measured in dipalmitoylphosphatidylcholine liposomes in the presence and absence of 40 mol% cholesterol at temperatures above and below the phase transition temperature (41°C). By using a synchronously-pumped mode-locked frequency-doubled dye laser and single photon counting detection with an excitation response function of 300 picosecond, rotational correlation times down to less than 1 nanosecond could be resolved. Whereas DPH showed only small changes in the limiting anisotropy on the addition of cholesterol, 12-AS showed significant increases in this parameter with the effect being potentiated at higher temperatures. This difference in behaviour has been attributed to a fluorophore-cholesterol interaction that resulted in a change in the fluorophore geometry. Not only do DPH and 12-AS sense different depolarizing rotations due to the different directions of their emission dipoles but also differ in their lipid interactions which alter their limiting anisotropies. The implication is that the comparison of steady-state anisotropy measurements between chemically identical fluorophores in different lipid environments may be complicated by molecular distortions that change the motions to which the steady-state fluorescence parameters will be sensitive.     

Differential polarized phase fluorometric investigations of diphenylhexatriene in lipid bilayers. Quantitation of hindered depolarizing rotations.

Differential polarized phase fluorometry has been used to investigate the depolarizing rotations of 1,6-diphenyl-1,3,5-hexatriene (DPH) in isotropic solvents and in lipid bilayers. For DPH dissolved in isotropic solvents, there is a precise agreement between the observed and predicted values for maximum differential tangents, indicating that in these media DPH is a free isotropic rotator. In lipid bilayers the tangent defects (i.e., the differences between the calculated and the observed maximum differential tangents) are too large to be explained by anisotropy in the depolarizing rotations but are accounted for by hindered isotropic torsional motions for the fluorophore [Weber, G (1978) Acta Phys. Pol A 54, 173]. This theory describes the depolarizing rotations of the fluorophore by its rotational rate R (in radians/second) and the limiting fluorescence anisotropy (r) at times long compared with the fluorescence lifetime. Through the combined use of both steady-state anisotropy measurements and differential phase measurements, we have demonstrated that one may obtain unique solutions for both R and r. For DPH embedded in vesicles prepared from dimyristoyl-, dipalmitoyl-, and distearoylphosphatidylcholines, the depolarizing motions are highly hindered at temperatures below the transition temperature (Tc) but are unhindered above Tc. The apparent rotational rates of the probe do not change significantly at Tc. These data suggest that the changes observed in the steady-state anisotropy near Tc derive primarily from changes in the degree to which the probe's rotations are hindered, and only to a small extent from changes in rotational rate. For DPH embedded in bilayers that contained 25 mol % cholesterol, no clear transition occurred and the rotations appeared to be hindered at all temperatures. The rotational motions of DPH embedded in dioleolyphosphatidylcholine were found to be far less hindered, but the rotational rates were similar to those obtained in the saturated phosphatidylcholines. Finally, the data show that in an anisotropic environment, such as that of a lipid bilayer, steady-state fluorescence anisotropy measurements alone cannot yield quantitatively meaningful rotational rates. Extrapolation of steady-state aniosotropy data to the quantitation of membrane viscosity is therefore difficult, if not invalid; however, qualitative comparisons can be useful.     

Fluorometry of turbid and absorbant samples and the membrane fluidity of intact erythrocytes.

In employing intrinsic or extrinsic fluorophores in the study of whole cells, or other strongly absorbant and/or scattering samples, the measured fluorescence intensity and polarization is seriously affected by absorption and scattering within the sample cuvet. These artifacts are analyzed and simple protocols are provided for overcoming them. An expression relating attenuation of the observed emission anisotropy to sample turbidity is derived. The validity of the method is confirmed by experiments in which the emission anisotropies and fluorescence yields of membrane probes in intact erythrocytes was measured with precision. It is also shown that the rotational mobility of the membrane probe 1-phenyl-3-(2-naphthyl)-2-pyrazoline is the same for intact erythrocytes and ghosts. These protocols are particularly useful in measuring the intrinsic fluorescence yield ratio for excimeric and monomeric emission of pyrene-containing membrane probes. This provides a method for determining the local lateral mobility of excimeric probes in intact erythrocytes.