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.     

Phospholipid order in gel- and fluid-phase cell-size liposomes measured by digitized video fluorescence polarization microscopy.

Low-light digitized video fluorescence microscopy has been utilized to measure the steady-state polarized fluorescence from the membrane probe diphenylhexatriene (DPH) and its cationic and phosphatidylcholine derivatives 1-(4-trimethylammoniumphenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) and 2-[3-(diphenylhexatrienyl)propanoyl]-3-palmitoyl-L-alpha-phosphati dylcholine (DPH-PC), respectively, in cell-size (10-70 microns) unilamellar vesicles composed of gel-or fluid-phase phospholipid. Using an inverted microscope with epi-illumination optics and an intensified silicon intensified target camera interfaced to a minicomputer, fluorescence images of single vesicles were obtained at emission polarizer orientations of 0 degrees, 45 degrees, 90 degrees, and 135 degrees relative to the excitation light polarization direction. Fluorescence intensity ratios F90 degrees/F0 degrees (= F perpendicular/F parallel) and F135 degrees/F45 degrees were calculated on a pixel-by-pixel basis from digitized image pairs. Theoretical expressions were derived for collected polarized fluorescence as a function of position on the membrane surface as well as the degree of lipid order, in terms of the fluorophore's maximum angular motional freedom in the bilayer (identical to theta max), using a modification of the method of D. Axelrod (1979. Biophys. J. 26:557-574) together with the "wobbling-in-a-cone" model of probe rotational diffusion. Comparison of experimental polarization ratios with theoretical ratios yielded the following results. In gel-phase dipalmitoyl-phosphatidylcholine, the data for all three probes correspond to a model in which the cone angle theta max = 17 +/- 2 degrees and there exists a collective tilt of the phospholipid acyl chains of 30 degrees relative to the bilayer normal. In addition, approximately 5% of DPH and TMA-DPH molecules are aligned parallel to the plane of the bilayer. In fluid-phase palmitoyloleoyl-phosphatidylcholine, the data are well fit by models in which theta max = 60 +/- 2 degrees for DPH and DPH-PC and 32 +/- 4 degrees for TMA-DPH, with approximately 20% of DPH molecules and 10% of TMA-DPH molecules aligned parallel to the bilayer plane, and a net phospholipid tilt at or near the headgroup region of approximately 30 degrees. The results demonstrate that lipid order can be measured with a spatial resolution of approximately 1 micron2 in cell-size vesicles even with high aperture observation through a microscope.     

Lipid-phase structure in epithelial cell membranes: comparison of renal brush border and basolateral membranes

The lipid-phase structures of brush border membrane vesicles (BBMV) and basolateral membrane vesicles (BLMV) isolated from rabbit renal cortex were compared by steady-state and phase-modulation measurements of diphenylhexatriene (DPH) and trans- and cis-parinaric acid (tPnA and cPnA) fluorescence. A temperature-scanning system was used which gave reproducible temperature profiles of steady-state and dynamic fluorescence parameters with a resolution of 0.1 degrees C. Steady-state anisotropy of DPH showed a triphasic dependence on temperature with slope discontinuities at 22 +/- 4 and 47 +/- 3 degrees C (BBMV) and at 23 +/- 2 and 48 +/- 1 degrees C (BLMV). At all temperatures, DPH anisotropy in BBMV was greater than that in BLMV. Ground-state heterogeneity analysis of tPnA and cPnA fluorescence lifetime data demonstrated the presence of long (greater than 12 ns) and short (less than 5 ns) lifetime components, interpreted in terms of solid-phase and fluid-phase lipid domains. The fraction of solid-phase phospholipid decreased from 0.9 to 0.1 for BBMV and from 0.7 to 0.3 in BLMV with increasing temperature (10-50 degrees C). In both membranes, tryptophan-PnA fluorescence energy-transfer measurements showed that membrane proteins were surrounded by a fluidlike phospholipid phase. These results demonstrate the inadequacy of steady-state DPH anisotropy data in defining the structural characteristics of complex biological membranes. Results obtained with the phase-sensitive parinaric acid probes demonstrate major differences in the phase structure of the two opposing cell membranes in both the bulk lipid and the lipid microenvironment around membrane proteins.     

Use of a FACS III for fluorescence depolarization with DPH

We have previously demonstrated age-related differences in human lymphocyte membrane fluidity, by use of steady-state polarization measurements on bulk cell suspensions with the fluorescence probe DPH. However, for exact analysis of the possible functional importance of these changes, single-cell measurements were deemed of interest. We have now used an analog division device to measure fluorescence depolarization "p" of DPH in real time with a FACS III flow cytometer. The measurements are reliable, as we have been able to confirm the differences in DPH "p" between monocytes and lymphocytes previously shown in bulk suspension and to demonstrate the expected differences in fluidity of lipid-modulated cells. We also found significant differences in DPH "p" between lymphocytes of young and elderly blood donors. Lymphocyte subsets did not differ in polarization values but did differ in fluorescence intensity with Th less than Ts less than B = NK cells.     

DPH标记细胞膜的动力学与膜脂流动性的荧光偏振校正测量

用稳态荧光技术测得经过校正的荧光成分,由此算出用DPH标记的细胞膜的偏振度。方法是作荧光偏振值在随时间变化的曲线,将其外推至零标记时间求出该时间的荧光偏振值。用此法测定了艾氏腹水癌细胞的膜流动性。结果表明流动性比用整个细胞测得之值小,说明膜脂的有序程度和包装密度比胞浆中的脂大。实验结果和用三房空模型分析所得的理论值符合较好,提示荧光探剂的标记过程主要受分子扩散所控制。     

Fluidity of intact erythrocyte membranes. Correction for fluorescence energy transfer from diphenylhexatriene to hemoglobin

Membranes of intact erythrocytes were labeled by the fluorescent probe 1,6-diphenyl-1,3,5-hexatriene (DPH) using an improved labeling procedure described previously (Plásek, J. and Jarolím, P. (1987) Gen. Physiol. Biophys. 6, 425-437). The relationship between the steady-state DPH fluorescence anisotropy r and the mean corpuscular hemoglobin concentration (MCHC) was studied. Fluorescence anisotropy increased with increasing MCHC. A linear dependence of r = 0.0026 (MCHC) + 0.113 was obtained which enabled us to measure the fluidity of intact red cell membranes. Without this correction for fluorescence quenching by hemoglobin, incorrect conclusions about membrane fluidity could be made. This fact is demonstrated in a group of pyruvate kinase deficient patients compared with a group of healthy blood donors.     

Rotational relaxation of 1,6-diphenylhexatriene in membrane lipids of cells acclimated to high and low growth temperatures.

Measurement of the time-resolved fluorescence depolarization of 1,6-diphenylhexatriene (DPH) in artificial bilayers of microsomal membrane lipids from Tetrahymena gives detailed information concerning the molecular motion of this probe and fluid properties of the membrane lipids which are obscured with steady-state methods. The rotational motion of DPH in these lipids from cells acclimated to 15 and 39.5 degrees C growth temperatures was anisotropic, which agrees with recent time-resolved studies of this probe in synthetic phospholipid systems. Evaluation of DPH polarization data obtained from these lipid fractions at their respective growth temperatures showed differences in physical properties which suggest that "viscosity", per se, of the microsomal lipids is not a strictly regulated as it is in prokaryotic systems. Rotational relaxation of DPH in 39.5 degrees C microsomal lipids measured at 15 degrees C is more complex than that of either lipid fraction measured at its actual growth temperature, suggesting that the probe has partitioned into two dissimilar environments within the bilayer. Similar effects are observed in the microsomes of 39.5 degrees C cells by freeze-fracture electron microscopy following rapid cooling to 15 degrees C. Under these conditions, two distinct regions are observed on the fracture faces, suggesting a correlation between lipid phase changes and alterations in membrane structure.     

Interactions of pyrethroids with gramicidin-containing liposomal membranes

Fluorescence steady-state anisotropy and phase-modulation lifetime techniques have been utilized to study the interactions of pyrethroid compounds with fluid-phase phosphatidylcholine membranes containing the polypeptide gramicidin. This polypeptide is considered to be a model of hydrophobic regions of cellular integral membrane proteins. The pyrethroids disorder lipid packing in cellular membranes and gel-phase liposomes but do not disorder lipid packing in fluid-phase lipid (Stelzer, K.J. and Gordon, M.A. (1984) J. Immunopharmacol. 6, 381-410; (1985) Biochim. Biophys. Acta 812, 361-368) Irrespective of liposomal size, gramicidin incorporation resulted in a substantial increase in anisotropy of the fluorescent probe, 1,6-diphenyl-1,3,5-hexatriene (DPH), in fluid phase lipid. In the absence of gramicidin, permethrin and three other pyrethroids, allethrin, cypermethrin and fenpropathrin, increased DPH anisotropy. In these fluid phase systems, as the protein:lipid ratio was increased, the extent of the pyrethroid-mediated increase in fluorescence anisotropy diminished. Also, the pyrethroids shortened DPH fluorescence lifetimes. At high gramicidin:lipid ratios, permethrin substantially lowered anisotropy in the fluid phase lipid, relative to controls. The data suggest that pyrethroids disturb fluid-phase lipids which have been promoted to a relative state of order by proximity to an integral membrane protein. This type of order is one which is represented by DPH fluorescence anisotropy. A model based on these results is proposed to explain the effects of pyrethroids on lipid packing order in cellular membranes, as determined by DPH fluorescence anisotropy.     

Shape and lipid-binding site of the nonspecific lipid-transfer protein (sterol carrier protein 2): a steady-state and time-resolved fluorescence study

The nonspecific lipid-transfer protein (nsL-TP) from bovine liver was studied with time-resolved and steady-state fluorescence techniques. From the decay of the intrinsic tryptophanyl fluorescence, it was estimated that the rotational correlation time of nsL-TP is 15 ns. This parameter increased only slightly upon addition of an excess of negatively charged vesicles, indicating that the basic nsL-TP is not immobilized at the membrane surface under these conditions. Binding studies using fluorescent lipid analogues revealed that nsL-TP is able to extract sn-2-(pyrenehexanoyl) phosphatidylcholine and 1-palmitoyl-2-[3-(diphenylhexatrienyl) propionyl]-sn-3-phosphocholine (DPHp-PC) from a quenched donor vesicle. The fluorescence increase resulting from this binding was poorly quenched by either acrylamide or iodide. This indicates that nsL-TP shields the bound PC molecules from the aqueous environment. Time-resolved analysis of DPH fluorescence originating from DPHp-PC bound to nsL-TP yielded a rotational correlation time of 7.4 ns. This correlation time strongly suggests that the DPH moiety of the bound molecule is immobilized and that the nsL-TP/DPHp-PC complex is not attached to the donor vesicle. In view of the longer rotational correlation time obtained for the intrinsic tryptophanyl fluorescence, we conclude that nsL-TP is highly asymmetric. The data are consistent with a model in which the shape of nsL-TP is ellipsoidal with an axis ratio of 2.8. The implications for the mode of action of nsL-TP are discussed.     

Electron spin resonance and steady-state fluorescence polarization studies of lipid bilayers containing integral proteins

We derive equations that describe changes in the steady-state fluorescence polarization of the probe 1,6-diphenyl-1,3,5-hexatriene (DPH) or in the spectrum of electron spin resonance (ESR) nitroxide spin-labeled lipid probes as a function of the intrinsic molecule concentration in lipid bilayer membranes. We make use of an assumption used by us in an earlier paper. The equations are independent of any membrane model. They are valid when a DPH probe or a spin-labeled chain is equivalent to an unlabeled lipid hydrocarbon chain only as far as their general space-filling properties are concerned. We consider cases where the bilayer is either in a single homogeneous phase or in a two-phase region. We apply our equations to analyze ESR data from delipidated sarcoplasmic reticulum membranes and from egg yolk phosphatidylcholine bilayers containing Ca2+-ATPase, and DPH data from dipalmitoylphosphatidylcholine (DPPC) bilayers containing Ca2+-ATPase, both for T greater than Tc. The following conclusions were derived: (i) Ca2+-ATPase oligomers are "randomly" distributed, for the concentrations studied, in the fluid phase. (ii) There is no fixed stoichiometric ratio of "boundary" lipids and oligomers. (iii) Between 24k and 28k lipid molecules are able to surround each isolated oligomer composed of k Ca2+-ATPase monomers. Finally, we apply our equations to analyze DPH studies on DPPC bilayers containing Ca2+-ATPase for T less than Tc. We find that the results reported are in accord with the predictions of the model. In the Appendix, we show that an analytical expression for probabilities used by us is in very good agreement with the results of computer simulation.     

Evidence for a regular distribution of cholesterol in phospholipid bilayers from diphenylhexatriene fluorescence.

Cholesterol/dimyristoylphosphatidylcholine (DMPC) multilamellar vesicles were studied by steady-state fluorescence using diphenylhexatriene (DPH) as a probe. A series of dips were found in the plot of DPH fluorescence intensity versus cholesterol concentration at certain specific cholesterol concentrations. This observation indicates that there are dominant domains in which cholesterol molecules are regularly distributed on a hexagonal superlattice in the acyl chain matrix of DMPC at critical cholesterol concentrations. These concentrations can be predicted by an equation or a mathematical series, except the one at 33 mol %. These dips of DPH fluorescence intensity are temperature dependent. The excellent agreement between experimental data and calculated values as well as similar previous findings of dips and/or kinks in the excimer-over-monomer fluorescence in pyrenephosphatidylcholine/phospholipid mixtures confirm our conclusion about lateral organizations of cholesterol and acyl lipid chains in cholesterol/phospholipid multilamellar vesicles. The regular distribution model at critical concentration is consistent with the phase diagram of cholesterol/DMPC. Using the model of regular distribution, the physical origin of the liquid-disordered (Ld) phase, liquid-ordered phase (Lo), and coexistence of liquid-disordered phase and Lo phase (Lo + Ld) is discussed on the molecular level.     

Alterations in erythrocyte membrane fluidity in children with trisomy 21: a fluorescence study.

Membrane fluidity of erythrocytes obtained from 15 children with trisomy 21 and 20 healthy controls were studied by measuring steady-state fluorescence anisotropy and fluorescence lifetime of 1,6-diphenyl-1,3,5-hexatriene (DPH) and 1-(4-trimethylammoniumphenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) incorporated in hemoglobin-free erythrocyte membranes. Our results demonstrate a significant decrease in DPH fluorescence anisotropy and a significant increase in TMA-DPH fluorescence anistropy in erythrocytes from subjects with trisomy 21. No significant differences between the two groups were observed in the fluorescence lifetime of DPH and TMA-DPH. These data suggest an increase in membrane fluidity in the interior part of the membrane and a decrease in fluidity at the lipid-water interface region. This could be in part attributed to an increased oxidative damage in trisomy 21.     

The fluidity of DOPC bilayers and membrane fractions prepared from murine plasmacytoma cells is unchanged after incorporation of pristane (2,6,10,14-tetramethylpentadecane) as assessed by fluorescence polarization analysis.

The nature of the plasmacytomagenic activity of pristane (2,6,10,14-tetramethylpentadecane) is poorly defined. However, evidence for tumor promoting properties of pristane has recently come forward that includes direct cellular effects on B lymphocytes; i.e., the plasmacytoma precursor cell. Bly et al. (Cancer Biochem. Biophys. 11, 1990, 145-154) observed changed membrane fluidities in lymphocytes after administration of pristane in vivo. We measured steady-state fluorescence polarization using DPH (1,6-diphenyl-1,3,5-hexatriene) and APCL (1-acyl-2-[12-(9-anthryl)-11-trans-dodecenoyl]-sn-glycero-3- phosphocholine) as probes in DOPC (L-alpha-dioleoylphosphatidylcholin) model membranes and membrane fractions derived from plasmacytoma cells after incorporation of pristane in vitro. In a previous investigation, we verified the in vitro uptake of pristane into DOPC bilayers under the conditions employed here (Gawrisch and Janz, Biochim. Biophys. Acta 1070, 1991, 409-418). However, neither in DOPC bilayers nor in plasmacytoma membrane fractions could we detect changes in fluorescence polarization after in vitro incorporation of pristane within reasonable error limits. Therefore, we suggest that the observed alterations in membrane fluidity in lymphocytes from pristane-treated animals are the indirect result of the in vivo treatment but not a direct effect of pristane on membrane fluidity.     

A differential polarized phase fluorometric study of the effects of high hydrostatic pressure upon the fluidity of cellular membranes

The effects of high hydrostatic pressure (up to 2 kbar) upon the fluidity and order of the synaptic and myelin membrane fractions of goldfish brain have been studied by using steady-state and differential polarized phase fluorometry. Probe motion provided a measure of membrane order (r infinity) and probe rotational rate (R). Membrane order became progressively greater as pressure was increased up to approximately 2 kbar. This effect was similar over the temperature range 5.6-34.3 degrees C. An increase in pressure of 1 kbar had an effect on membrane order that was equivalent to a 13-19 degrees C reduction in temperature. Membrane order was essentially identical during pressurization and depressurization. At 5.6 degrees C, pressurization caused a large increase in R, and similar, though less dramatic, anomalies occurred at higher temperatures. It is suggested that this is due to the segregation of probe molecules in highly ordered membranes, which leads either to excitation transfer between 1,6-diphenyl-1,3,5-hexatriene (DPH) molecules or to changes in the rotational motion of DPH from "sticking" to "slipping".     

Fluorescence depolarization studies of melanosomal membranes from different sources

In the present paper we report a comparative study of physical properties and biochemical composition of isolated melanosomal membranes extracted from bovine eyes and from an equine spleen melanoma. Some biophysical characteristics of such membranes were obtained by steady-state and time resolved fluorescence spectroscopy using DPH as fluorescent probe. By these methods we have measured both static fluorescence polarization and fluorescence lifetimes and from the experimental data we have calculated the rotational correlation times by Perrin's equation. Since dynamic and static parameters, such as fluidity and molecular order, can be determined by these methods, the results are discussed on the basis of the recent theories of the role of the biochemical composition in the molecular structure and properties of membranes.     

Decreased lipid order induced by microsomal cytochrome P-450 and NADPH-cytochrome P-450 reductase in model membranes: fluorescence and electron spin resonance studies

Cytochrome P-450 and NADPH-cytochrome P-450 reductase were reconstituted in unilamellar lipid vesicles prepared by the cholate dialysis technique from pure dimyristoylphosphatidylcholine (DMPC), pure dipalmitoylphosphatidylcholine (DPPC), pure dioleoylphosphatidylcholine (DOPC), and phosphatidylcholine/phosphatidylethanolamine/phosphatidylserine (PC/PE/PS) (10:5:1). As probes for the vesicles' hydrocarbon region, 1,6-diphenyl-1,3,5-hexatriene (DPH) and spin-labeled PC were used. The steady-state and time-resolved fluorescence parameters of DPH were determined as a function of temperature and composition of liposomes. Incorporation of either protein alone or together increased the steady-state fluorescence anisotropy (rs) of DPH in DOPC and PC/PE/PS (10:5:1) liposomes. In DMPC and DPPC vesicles, the proteins decreased rs significantly below the transition temperature (Tc) of the gel to liquid-crystalline phase transition. Time-resolved fluorescence measurements of DPH performed in reconstituted PC/PE/PS and DMPC proteoliposomes showed that the proteins disorder the bilayer both in the gel and in the liquid-crystalline phase. Little disordering by the proteins was observed by a spin-label located near the mid-zone of the bilayer 1-palmitoyl-2-(5-doxylstearoyl)-3-sn-phosphatidylcholine (8-doxyl-PC), whereas pronounced disordering was detected by 1-palmitoyl-2-(8-doxylpalmitoyl)-3-sn-phosphatidylcholine (5-doxyl-PC), which probes the lipid zone closer to the polar part of the membrane. Fluorescence lifetime measurements of DPH indicate an average distance of greater than or equal to 60 A between the heme of cytochrome P-450 and DPH.     

Charged anesthetics selectively alter plasma membrane order

Although indirect evidence supporting differential lipid fluidity in the two monolayers of plasma membranes has accumulated, unambiguous demonstration of this difference has been difficult to obtain. In the present study, the fluorescent probe 1,6-diphenyl-1,3,5-hexatriene (DPH), selective quenching of fluorescence by trinitrophenyl groups, and differential polarized phase fluorescence techniques were used to directly examine the static (order) and dynamic (rotational rate) components of lipid motion in the exofacial and cytofacial leaflets of LM fibroblast plasma membranes. The limiting anisotropy (0.137), the order parameter (0.590), and the rotational relaxation time (1.20 ns) of DPH in the plasma membranes (inner plus outer leaflet) indicated rapid but restricted probe motion in the lipid environment. However, the statics and dynamics of DPH motion in the individual monolayers were significantly (p less than 0.025) different. The limiting anisotropy, order parameter, and rotational relaxation time of DPH in the cytofacial monolayer were 0.036, 0.08, and 0.16 ns, respectively, greater than calculated for the exofacial monolayer of the LM plasma membrane. At appropriate concentrations, phenobarbital and, to a lesser degree, pentobarbital preferentially reduced the limiting anisotropy of DPH calculated for the exofacial leaflet while prilocaine reduced the limiting anisotropy of DPH in the cytofacial leaflet of LM fibroblast plasma membranes. In contrast, the putative cytofacial anesthetic procaine failed to show any preference for either leaflet. Arrhenius plots of DPH fluorescence in LM plasma membranes showed a prominent characteristic break point near 30-32 degrees C. Phenobarbital, pentobarbital, and procaine did not affect this break point while prilocaine selectively abolished it. The break point was therefore assigned to the inner monolayer of the LM plasma membrane.     

Effects of non-electrolyte molecules with anesthetic activity on the physical properties of DMPC multilamellar liposomes

The effects of 13 non-electrolytes with moderate anesthetic potency on the order of DMPC liposomes were examined. Changes in order were monitored by steady-state fluorescence polarization techniques using 1,6-diphenyl-1,3,5-hexatriene (DPH) and 1-(4-trimethylammoniumphenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPG). At 30 degrees C, all of the compounds tested decreased the DPH steady-state anisotropy (rs), with potencies highly correlated to their oil/water partition coefficients. However, only the most hydrophobic anesthetics decreased TMA-DPH RS. Some of the most hydrophilic compounds, including ethanol and urethane, actually increased TMA-DPH rs, suggestive of an increase in membrane order. The concept of selectivity was borrowed from partitioning theory and used to explain some effects on anesthetic potency of decreasing temperature to 18 degrees C. In the gel as opposed to the liquid crystalline phase, selectivity for decreasing membrane order (as monitored by DPH) markedly increased, suggesting that anesthetic partitioning and/or the site of anesthetic action was occurring in a more hydrophobic domain. The solute-independent difference (or capacity) between two membranes for perturbation was defined as membrane sensitivity. Sensitivity appeared to also decrease with decreasing temperature, despite the decrease in membrane partitioning. This effect is thought to result from the selective delivery of the anesthetic solute to the membrane interior and away from more hydrophilic domains where anesthetics may order membrane structure.     

Dynamic structure of lipid bilayers studied by nanosecond fluorescence techniques

Molecular motions in liposomes of dipalmitoyl-phosphatidylcholine (DPPC) were studied by nanosecond fluorescence techniques. As a fluorescent probe for the hydrocarbon region, 1,6-diphenyl-1,3,5-hexatriene (DPH) was used. Time courses of fluorescence intensity IT(t) and emission anisotropy r(t) of DPH embedded in DPPC liposomes were measured at various temperatures. The value of the fluorescence lifetime tau obtained froma single exponential decay of IT(t) was somewhat higher than that in liquid paraffin below the transition temperature Tt and decreased above Tt. Higher values of tau below Tt indicate the almost complete hydrophobic environment. The decay curves of r(t) were separated into two phases: an initial fast decreasing phase of the order of one nanosecond and a second almost constant phase. This indicates that the orientational motion of DPH in the hydrocarbon region is described by a wobbling diffusion restricted by a certain anisotropic potential. The results were analyzed on the model that the wobbling diffusion is confined in a cone with a uniform diffusion constant. Though temperature dependence of the cone angle was sigmoidal, that of the wobbling diffusion constant was like the exponential function. The change in the cone angle at Tt was sharper than that in the wobbling diffusion constant at Tt. Estimated values of the viscosity in the cone were an order of magnitude smaller than the values of "microviscosity" which were estimated from the steady-state emission anisotropy without considering the restrictions on the rotational motion.     

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.