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.     

Interaction of the fluorescent probe 1,6-diphenyl-1,3,5-hexatriene with biomembranes

The relationship between the conditions of membrane labelling by the fluorescent probe 1,6-diphenyl-1,3,5-hexatriene (DPH) and its fluorescence parameters was investigated. In the labelling solutions prepared by the usual method, the presence of DPH microcrystals was revealed which led to the lower resultant fluorescence anisotropy values. Lower labelling efficiency was observed with DPH solutions in tetrahydrofuran when compared with solutions in acetone. Modifications of the labelling procedure are proposed which give better reproducibility of the results. There modified method involves the preparation of a 2 X 10(-4) mol. 1(-1) DPH stock solution in acetone, a 100-fold dilution in an appropriate buffer, subsequent bubbling through with nitrogen for 30 min and mixing the resulting solution with cell/membrane suspension in a 1:1 (v/v) ratio. Changes in intensity, anisotropy and spectra of DPH fluorescence in the course of membrane labelling were studied. A two-stage model of the incorporation of DPH into membranes was proposed, according to which DPH molecules first quickly adhere to the membrane surface and then are slowly translocated to the apolar regions of the membrane.     

Fluorescence lifetime distributions of 1,6-diphenyl-1,3,5-hexatriene in phospholipid vesicles

The fluorescence emission properties of 1,6-diphenyl-1,3,5-hexatriene (DPH) in 1,2-dipalmitoyl-3-sn-phosphatidylcholine and 1,2-dimyristoyl-3-sn-phosphatidylcholine multilamellar vesicles have been measured by using multifrequency phase fluorometry. The fluorescence decay of DPH in the phospholipid vesicles has been analyzed by assuming either that the decay is made up of a discrete sum of exponential components or that the decay is made up of one or more continuous distributions of lifetime components. The fit of the decay curve using exponentials required at least two terms, and the reduced X2 was relatively large. The fit using a continuous distribution of lifetime values used two continuous components. Several symmetric distribution functions were used: uniform, Gaussian, and Lorentzian. The distribution function that best described the decay was the Lorentzian. The full width at half-maximum of the Lorentzian distribution was about 0.6 ns at temperatures below the phase transition temperature. At the phospholipid phase transition and at higher temperatures, the distribution became quite narrow, with a width of about 0.1 ns. It is proposed that the lifetime distribution is generated by a continuum of different environments of the DPH molecule characterized by different dielectric constants. Below the transition temperature in the gel phase, the dielectric constant gradient along the membrane normal determines the distribution of decay rates. Above the transition, in the liquid-crystalline phase, the translational and rotational mobility of the DPH molecule increases, and the DPH experiences an average environment during the excited-state lifetime. Consequently, the distribution becomes narrower.(ABSTRACT TRUNCATED AT 250 WORDS)     

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

Nanosecond decays of the fluorescence anisotropy, $\text{r}$, were studied for the emission of 1,6-diphenyl-l,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, $\text{r}$, of the fluorescence anisotropy were very similar for artifical and biological membranes.Angles, θ, 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’, 〈η〉. An increase in 〈η〉 from 1.5 to 5.2 P in our systems was accompanied by a decrease in θ from 49° to 30° while the decrease in the mean motional relaxation times, $\text{φ}{}_{\mathrm{<mtext>f</mtext>}}$, 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 ($\text{r}\text{> 0.15}$) represent changes in the degree of static orientational constraint rather than changes in diffusion rates of the label.     

Temperature dependence of 1,6-diphenyl-1,3,5-hexatriene fluorescence in phophoslipid artificial membranes.

The fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene in phospholipid vesicles is a function of the physical state of the lipid. Below the phase transition, the polarization approaches the theoretical maximum for total immobilization while above the phase transition the fluorescence becomes nearly completely depolarized. The discontinuity in the temperature dependence of polarization occurs within a temperature range under 5 degrees C in the case of pure phospholipids, but for mixed phospholipids occurs over a temperature range greater than 20 degrees C. From these data, phase diagrams describing the gel-sol equilibrium can be constructed; the phase diagrams correspond well with those described in the literature which were constructed using spin-label probes or from x-ray diffraction patterns. The marked change in polarization at the phase transition may be related to the packing of the probe molecule into the lipid bilayer: fluorescence measurements on oriented bilayers indicate that below the phase transition the long axis of the probe is oriented perpendicular to the plane of the membrane while above the transition the probe is oriented randomly relative to the plane of the membrane.     

Interaction of a phosphatidylcholine derivative of 1,6-diphenyl-1,3,5-hexatriene (DPH-PC) with lymphocytes.

In this study we have demonstrated a transfer of a phosphatidylcholine derivative of 1,6-diphenyl-1,3,5-hexatriene (DPH-PC) from self-quenched lipid vesicles to intact lymphocytes. Membrane labeling was followed measuring the time dependent reexpression of fluorescence. The results of fluorescence quenching by 2,4,6-trinitrobenzene sulfonate and the decrease of fluorescence polarization values during incubation at 37 degrees C, suggest that the probe could remain localized at level of the plasma membrane until 20-30 minutes. DPH-PC is identical to the natural phospholipid with respect to head group structure and polarity therefore we suggest that under appropriate experimental conditions, it could represent an useful tool to study the physico-chemical properties of specific phospholipid domains in the plasma membrane of intact cells.     

Detection of phospholipid phase separation. A multifrequency phase fluorimetry study of 1,6-diphenyl-1,3,5-hexatriene fluorescence

Using multifrequency phase and modulation fluorometry and a nonlinear least-squares analysis of lifetime data, we were able to determine the complex decay of 1,6-diphenyl-1,3,5-hexatriene (DPH) in synthetic phospholipid bilayers. Our results showed a monoexponential decay of DPH in the pure isotropic solvents studied, over a wide temperature range, and a double-exponential decay of DPH in phospholipids, both above and below the transition. During the transition, and in mixed-phase phospholipids, a three-component analysis was successfully accomplished, and the pre-exponential factors of the two main components have been shown to be quantitatively representative of the gel and liquid-crystalline phases of the bilayer. The fractional intensity of the shorter lifetime component depends on the modalities of the sample preparation. The factors affecting this component are discussed. From the DPH fluorescence lifetime and from the anisotropy data in L-alpha-dimyristoyl-phosphatidylcholine/L-alpha-dipalmitoyl-phosphatidyl choline mixtures, a phase diagram was independently constructed. Conclusions about the sensitivity and the partition of the probe between gel and the liquid-crystalline phases of the bilayer are derived. Lifetime experiments on DPH in a L-alpha-dilauroyl-phosphatidylcholine/L-alpha-dipalmitoyl-phosphatidylch oline mixture suggested a general method for the determination and quantitation of the two different phases in the bilayer.     

Steady-state fluorescence anisotropy changes of 1,6-diphenyl-1,3,5,-hexatriene in membranes from Bacillus megaterium spores

The steady-state fluorescence anisotropy of 1,6-diphenyl-1,3,5-hexatriene incorporated into isolated Bacillus megaterium spore membranes was measured. Compounds capable of triggering spore germination in vivo caused an increase in the anisotropy of diphenylhexatriene. These increases in anisotropy of diphenylhexatriene in spore membranes are likely to represent at least a portion of the trigger mechanism for spore germination based on the following observations. First, there was an exceptional positive correlation between compounds that both triggered germination in vivo and caused changes in anisotropy in vitro. Second. the capacity of membranes to respond to germinants by increases in anisotropy was unique to membranes from spores but disappeared after germination. Third, alteration of spores chemically or genetically to block the in vivo triggering of germination by l-proline also blocked the in vitro anisotropy change with l-proline but not d-glucose. Finally, there was no correlation between the transport activities of specific compounds and the ability of these compounds to either trigger germination or alter the anisotropy of diphenylhexatriene in the membranes. Although we do not known the nature of the molecular interactions giving rise to the anisotropy changes, we hypothesize that they are due to changes in protein conformation that alter protein-protein and/or protein-lipid interactions. Such modifications of membrane structures could account for the rapid release of small molecular weight compounds such as K⁺ and Ca²⁺ early in germination.     

Nanosecond time-resolved emission anisotropy of the fluorescent probe 1,6-diphenyl-1,3,5-hexatriene in human amniotic fluid

The fluorescence emission anisotropy of 1,6-diphenyl-1,3,5-hexatriene in human amniotic fluid has been studied using nanosecond time-resolved emission techniques. These studies demonstrate that the previously reported decrease in the steady state emission anisotropy, 〈r〉, with gestational age is due to a change in the rate of rotational motion of the probe. The emission anisotropy decays to a limiting value (r_∞) greater than zero, suggesting a hindered rotation of the probe, and this is independent of gestational age. The decay function for the emission anisotropy of amniotic fluids from 17, 29, 40 and 41 weeks in gestational age can be best expressed as a single exponential plus a constant term, with rotational correlation times varying from 17 ns to 2.2 ns, respectively. The zero time emission anisotropy remains approx. 0.30 for both early and late gestational times.     

Studies of the ethanol-induced interdigitated gel phase in phosphatidylcholines using the fluorophore 1,6-diphenyl-1,3,5-hexatriene

It is now well established that a number of amphiphilic molecules such as ethanol can induce the formation of the fully interdigitated gel phase in phosphatidylcholines. We have shown earlier that alcohols such as ethanol induce biphasic melting behavior in phosphatidylcholines [Rowe, E. S. (1983) Biochemistry 22, 3299-3305] but not in phosphatidylethanolamines [Rowe, E. S. (1985) Biochim. Biophys. Acta 813, 321-330]. Simon and McIntosh [(1984) Biochim. Biophys. Acta 773, 169-172] showed that the alcohol-induced biphasic melting behavior in phosphatidylcholines is a consequence of acyl chain interdigitation. In the present study we demonstrate the detection of the transition of DPPC and DSPC to the interdigitated phase in the presence of ethanol using the fluorescence properties of the commonly used fluorophore 1,6-diphenyl-1,3,5-hexatriene (DPH). By correlating fluorescence and X-ray diffraction results, we have demonstrated the use of fluorescence to study the phase transition from the noninterdigitated to the interdigitated phase. Using this method, we have investigated the temperature and ethanol concentration dependence of the induction of the interdigitated phase in DSPC and DPPC and shown that the induction of interdigitation by ethanol is temperature dependent, with higher temperature favoring interdigitation. The temperature-ethanol phase diagrams have been determined for DPPC and DSPC.     

Membranes modification of differentiating proerythroblasts. Variation of 1,6-diphenyl-1,3,5-hexatriene lifetime distributions by multifrequency phase and modulation fluorimetry

The fluorescence emission of 1,6-diphenyl-1,3,5-hexatriene (DPH) in K562 cell membranes has been studied using multifrequency phase and modulation fluorimetry. The DPH decay data collected at various modulation frequencies were analysed by assuming either a model of discrete exponential components or a model of continuous lifetime distribution. The fits showed smaller values of the reduced chi square using the model of continuous lifetime distribution. The K562 cell membranes dynamics were investigated during the cell differentiation along the erythroid pathway. By using the continuous lifetime distribution method for the analysis of the DPH decay, marked variations were observed during the four initial days of the erythroid differentiation. Namely, the width of the DPH lifetime distribution increased by a factor of about two, while the center value of the distribution remained constant. By using the discrete exponential components model for the analysis of the DPH decay no variations were observed during the K562 differentiation.     

Molecular dynamics simulation of a dye molecule in the interior of a bilayer: 1,6-diphenyl-1,3,5-hexatriene in dipalmitoylphosphatidylcholine

A molecular dynamics simulation was carried out for a dipalmitoylphosphatidylcholine (DPPC) membrane in its liquid crystalline state containing different concentrations of the dye molecule 1,6-diphenyl-1,3,5-hexatriene (DPH). From a numerical analysis of the trajectories, we obtained information concerning structural changes of the membrane due to the presence of the probe and some hydrodynamic information concerning the probe itself. The hydrodynamic properties regarding dye molecules that have been reported in this article are: rotational and translational diffusion coefficient and relaxation times. From this analysis, we estimated a range of values of 0.6-0.9 cP for the micro-viscosity in the mid-membrane. These simulations also afforded us some information regarding structural changes in the membrane as a consequence of the presence of the fluorescent dyes at different concentrations. Thus, the disorder inside the membrane, the surface area per lipid and thickness of the membrane were also investigated.     

Rotational relaxation rate of 1,6-diphenyl-1,3,5-hexatriene in cytoplasmic membranes ofBacillus subtilis. A new model of heterogeneous rotations

The temperature dependence of fluorescence anisotropy, lifetime and differential tangent of 1,6-diphenyl-1,3,5-hexatriene (DPH) and its polar trimethylammonium derivative (TMA-DPH) were investigated in cytoplasmic membranes ofBacillus subtilis. The fluorescence parameters were compared in the two types of membranes prepared from bacteria cultivated at 20 and 40°C. Steady-state anisotropy measurements showed that within a broad range of temperatures, membranes cultivated at 20°C exhibit significantly lower values than those prepared from cells cultivated at 40°C. The temperature dependence of lifetime and differential tangent measurements (differential polarized phase fluorimetry) were fully consistent with steady-state anisotropy data of both DPH and TMA-DPH. The low anisotropy values in the case of TMA-DPH could be explained by a shorter lifetime and higher temperature-induced decrease as compared with DPH. Surprisingly, the temperature dependence of rotational rateR calculated according to the model of hindered rotations (Lakowicz 1983) gave misleading results. When increasing the temperature from 5 to 25°C, a marked drop of rotational relaxation rate was observed. The minimumR values were measured between 25 and 30°C and further increase of temperature (up to 60°C) was reflected as increase of theR values. Therefore, a new model of “heterogeneous rotations” was developed. This model assumes that even at low temperatures (approaching 0°C) where the differential tangent reaches zero, a fraction of fast rotating molecules exists. The ratio between fast and slowly rotating molecules may be expressed by this model, the newly calculated rotational rates are fully consistent with anisotropy, lifetime and differential tangent measurements and represent the monotonically increasing function of temperature.     

Cytoplasmic membrane fluidity measurements on intact living cells ofBacillus subtilis by fluorescence anisotropy of 1,6-diphenyl-1,3,5-hexatriene

A method for determination of membrane fluidity (microviscosity) in Bacillus subtilis cytoplasmic membrane under in vivo conditions is described. The membranes were labelled with the hydrophobic fluorescent probe 1,6-diphenyl-1,3,5-hexatriene during the exponential phase of growth. Fluorescence anisotropy measurements were carried out in an intact cell suspension having absorbance A as high as 0.2-0.3 (corresponding to a cell concentration of 100-300/nL).     

Dynamic motions of 1,6-diphenyl-1,3,5-hexatriene in interdigitated C(18):C(10)phosphatidylcholine bilayers.

This study investigates the dynamic behavior of 1,6-diphenyl-1,3,5-hexatriene (DPH) in C(18):C(10)phosphatidylcholine [C(18):C(10)PC] bilayers. C(18):C(10)PC is an asymmetric mixed-chain phosphatidylcholine known to form mixed-interdigitated structures below the transition temperature and form partially interdigitated bilayers above the transition temperature. The rotation of DPH in C(18):C(10)PC has been described in terms of the thermal coefficient of rotation using the modified Y-plot method which takes into account the limiting anisotropy value. During the phase transition of C(18):C(10)PC, DPH exhibits a thermal coefficient b2M = 0.41 - 0.51 degrees C-1 which is similar to the b2M values obtained with noninterdigitated phosphatidylcholine bilayers. Differential polarized phase-modulation fluorometry has also been employed to study the dynamic behavior of DPH in C(18):C(10)PC in real time. The data show that DPH contains considerable motion in the highly ordered mixed interdigitated bilayers. The DPH motion steadily increases with an increase in temperature as shown by the rotational correlation time, and the wobbling diffusion constant. However, the limiting anisotropy, the order parameter, and the width of the lifetime distribution undergo an abrupt decrease, and a corresponding abrupt increase in the cone angle, at approximately 16 degrees C. This temperature range is near the onset temperature of the phase transition as determined by differential scanning calorimetry. The rotational parameters show strong hysteresis on heating and cooling. All the rotational parameters derived from DPH fluorescence in mixed interdigitated C(18):C(10)PC exhibit magnitudes similar to those obtained from noninterdigitated gel phases of symmetric diacylphosphatidylcholines.(ABSTRACT TRUNCATED AT 250 WORDS)     

Correlation between the order parameter and the steady-state fluorescence anisotropy of 1,6-diphenyl-1,3,5-hexatriene and an evaluation of membrane fluidity

In this paper it is shown that for 1,6-diphenyl-1,3,5-hexatriene there exists a simple analytical relation between the orientational order parameter and the steady-state fluorescence anisotropy. This relation is derived on semi-empirical grounds. The order parameter and the true microviscosity for membranes as calculated from steady-state measurements are evaluated. For biological membranes the estimation of the order parameter from steady-state experiments is feasible, but the evaluation of the true microviscosity is not reliable. Also, the physiological relevance of the order parameter is discussed.     

Equilibrium and dynamic structure of large, unilamellar, unsaturated acyl chain phosphatidylcholine vesicles. Higher order analysis of 1,6-diphenyl-1,3,5-hexatriene and 1-[4-(trimethylammonio)phenyl]- 6-phenyl-1,3,5-hexatriene anisotropy decay

Equilibrium and dynamic structural properties of minimally to highly unsaturated acyl chain, large, unilamellar phosphatidylcholine (PC) vesicles have been characterized by the dynamic fluorescence properties of 1,6-diphenyl-1,3,5-hexatriene (DPH) and 1-[4-(trimethylammonio)phenyl]-6-phenyl-1,3,5-hexatriene (TMA-DPH). Fluorescence lifetimes and equilibrium and dynamic rotational properties of these probes were analyzed by limited-frequency phase-modulation fluorometry in egg PC, palmitoyloleoyl-PC (POPC), dioleoyl-PC (DOPC), palmitoylarachidonoyl-PC (PAPC), and palmitoyldocosahexaenoyl-PC (P-22:6-PC) vesicles over a temperature range from 5 to 37 degrees C. DPH equilibrium orientational distributions were derived according to a model permitting bimodal orientational distributions in which the parallel probability maximum was aligned parallel to the bilayer normal and the orthogonal probability maximum was oriented parallel to the plane of the bilayer. TMA-DPH orientational distributions were derived according to the same model except that all probability was constrained to the parallel orientation. TMA-DPH fluorescence lifetimes were much more sensitive than those of DPH to variations in acyl chain composition and temperature although the same qualitative behavior was generally observed with both probes. Greater acyl chain unsaturation and higher sample temperatures each gave rise to shorter lifetimes consistent with increased water penetrability into the bilayers. Equilibrium order of the hydrocarbon core (as probed by DPH) and of the interfacial and head group regions of the bilayers (as probed by TMA-DPH) was reduced by increasing levels of unsaturation and by higher sample temperatures.(ABSTRACT TRUNCATED AT 250 WORDS)