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* Unidad de Biofísica (CSIC-UPV/EHU) and Departamento de Bioquímica, Universidad del País Vasco, 48080 Bilbao, Spain; and
MEMPHYS-Center for Biomembrane Physics, Department of Biochemistry and Molecular Biology, University of Southern Denmark, Odense, Denmark
Correspondence: Address reprint requests to Alicia Alonso, Tel.: 34-94-601 2625; Fax: 34-94-601 3360; E-mail: gbpaliza{at}lg.ehu.es.
| ABSTRACT |
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40°C) two gel (respectively Cer-rich and SM-rich) phases are directly observed using fluorescence microscopy. Although pure SM membranes are fully solubilized by Triton X-100 at room temperature, 5 mol % Cer is also enough to induce detergent resistance, even with a large detergent excess and lengthy equilibration times. Short-chain Cers do not give rise to detergent resistance. SM/Cer mixtures containing up to 30 mol % Cer become fully soluble at
50°C, i.e., well above the gel-fluid transition temperature of SM. The combined results of temperature-dependent solubilization and differential scanning calorimetry reveal that SM-rich domains are preferentially solubilized over the Cer-rich ones as soon as the former melt (i.e., at
40°C). As a consequence, at temperatures allowing only partial solubilization, the nonsolubilized residue is enriched in Cer with respect to the original bilayer composition. Fluorescence microscopy of giant unilamellar vesicles at room temperature clearly shows that SM-rich domains are preferentially solubilized over the Cer-rich ones and that the latter become more rigid and extensive as a consequence of the detergent effects. These observations may be relevant to the phenomena of sphingomyelinase-dependent signaling, generation of "raft platforms", and detergent-resistant cell membranes. | INTRODUCTION |
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However the physicochemical foundations of the detergent-resistance phenomenon are not clear. Studies of model membranes with defined lipid compositions have shown that neither the presence of lipids with a high Tm gel-to-fluid transition temperature (5
7
) nor the presence of sphingolipids (8
,6
) can by themselves explain the resistance. Membrane rafts are considered to exist in the liquid-ordered phase (9
,10
), and Sáez-Cirión et al. (11
) demonstrated that bilayers in the liquid-ordered phase are indeed less prone to solubilization than those in the fluid, or liquid-disordered, phase. An important observation is that the simultaneous presence of sphingomyelin (SM) and Ch, two typical "raft lipids", in the bilayers confers on them a high degree of resistance toward detergent solubilization (10
,12
). Nevertheless, even if the presence of SM and Ch in cell membrane rafts would account for their detergent resistance, a raft property that remains unexplained is that, according to many examples in the literature, these rafts are detergent resistant at 4°C but become solubilized at 37°C. Although it may seem counterintuitive, fluid lipid bilayers in general, and in particular those containing SM and Ch, are solubilized more easily at lower temperatures (12
,6
) because at these temperatures the bilayers can accommodate less detergent monomers before breaking down in the form of lipid-detergent mixed micelles (7
).
In the search for a simple (if possible binary) mixture of raft-related lipids that would be resistant toward Triton X-100 solubilization at low, but not at high, temperatures we have found the SM/ceramide (Cer) system. This work describes the properties of SM/Cer bilayers in the presence of Triton X-100. This simple system may be biologically relevant, because Cer is the end product of SM hydrolysis by sphingomyelinases, and sphingomyelinase activation appears to be at the origin of many cell signaling events (see for reviews Kolesnick et al. (13
), Cremesti et al. (14
), Goñi and Alonso (15
), and Futerman and Hannun (16
). Different kinds of vesicles have been used in this study as models for the cell membrane bilayers, namely multilamellar vesicles (MLV), large unilamellar vesicles (LUV), and giant unilamellar vesicles (GUV). Although all of them constitute generally accepted models of biologically meaningful lipid bilayers, each model has its particular advantages, i.e., MLV are convenient to prepare and are not surpassed by any other preparations for calorimetric phase transition studies, LUV are quickly equilibrated with detergents, thus very apt for solubilization studies, and GUV also equilibrate rapidly but have the additional advantage of their large size for microscopy observations. From the point of view of results analysis, all three systems are similar enough to allow generalization of conclusions based on one of them to the other two and, with the usual reservations, to the biological membranes. Our data reveal that Cer-enriched domains that existed in the native bilayer may be considerably modified, in composition and extent, by the detergent during the solubilization process, an observation that casts doubts on the identification of DRMs with physiologically meaningful raft domains.
| MATERIALS AND METHODS |
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MLV preparation
For MLV liposome preparation SM or occasionally other phospholipids and Cer were dissolved in chloroform/methanol (2:1, v/v), and the mixture was evaporated to dryness under a stream of nitrogen. Traces of solvent were removed by evacuating the samples under high vacuum for at least 2 h. The samples were hydrated at 45°C in 20 mM PIPES, 150 mM NaCl, 1 mM EDTA, pH 7.4, helping dispersion by stirring with a glass rod. To ensure homogeneous dispersion the hydrated samples were extruded between two syringes through a narrow tubing (0.5 mm internal diameter, 10 cm long) 100 times at 45°C. In these samples the amount of phospholipid was kept constant, whereas the amount of Cer and, correspondingly, that of total lipid varied. The final phospholipid concentration was measured in terms of lipid phosphorous, as described previously (5
,6
). Liposome suspensions were mixed with the appropriate detergent solutions to obtain the desired detergent/lipid (D/L) ratio. Final lipid concentration was always 1 mM. The mixtures were left to equilibrate (30 min for the preliminary observations or 24 h for equilibrium conditions), and solubilization was assessed from the changes in turbidity.
Solubilization assays
Solubilization was assayed using either the turbidity or the centrifugation methods. The turbidity method (17
) is based on the decrease in suspension turbidity that accompanies the lamellar-to-micellar transition. Turbidity was measured as absorbance at 500 nm in a Uvikon 922 spectrophotometer (Kontron, Regensdorf, Switzerland) equipped with thermoregulated cell holders. The turbidity values were normalized by setting 100% as the turbidity of the vesicle suspension without detergent, whereas 0% turbidity corresponded to pure buffer.
In the centrifugation assay of liposome solubilization, the nonsolubilized fraction after detergent treatment was separated from the micelles by centrifugation (14,500 x g, 20 min) in a standard Eppendorf centrifuge at room temperature. For quantitative analysis of the lipid compositions in the nonsolubilized membranes, the pellets were extracted with chloroform/methanol (2:1). The organic phase was concentrated and separated on thin-layer chromatography Silica Gel 60 plates, with chloroform/methanol/water (50:42:1, by volume). After charring the organic phase with a sulfuric acid reagent, the spot intensities of both SM and Cer were quantified using a Bio-Rad (Hercules, CA) GS-800 Calibrate Densitometer with the Quantity One software from Bio Rad.
Fluorescence quenching experiments
Quenching of the DPH fluorescence by TEMPO was measured as follows. Lipids, DPH, and (when required) TEMPO were mixed at a 300:1:1 ratio in organic solvent, then the solvent was evaporated, and the mixture was vacuum dried for at least 2 h in the dark. The vesicles were prepared in 20 mM PIPES, 150 mM NaCl, 1 mM EDTA, pH 7.4 as described above. Vesicles with and without TEMPO were prepared for all SM/Cer ratios. Fluorescence quenching was recorded in a SLM-AMINCO 8100 spectrofluorometer (Jobin Yvon, Longjumeau, France) equipped with thermoregulated cell holders. DPH fluorescence was excited at 360 nm; emission was recorded at 428 nm.
Differential scanning calorimetry experiments
For the differential scanning calorimetry (DSC) measurements both lipid suspensions and buffer were degassed before being loaded into the sample or reference cell of an MC-2 high-sensitivity scanning calorimeter (MicroCal, Northampton, MA). The final phospholipid (usually SM) concentration in the samples was 1 mM. Three heating scans, at 45°C/h, were recorded for each sample. Lipid phosphorous assays were carried out on all SM-containing samples after the DSC scans to obtain accurate
H values (in kcal/mole of phospholipid). Thermogram transition temperatures, enthalpies, and widths at half-height were determined using the software ORIGIN (Microcal) provided with the calorimeter. Complex thermograms suggesting more than one underlying transition were resolved mathematically into the number of necessary peaks, usually three, assuming independent transitions, so that the sum of these constituents gave the best fit to the original data. For curve fitting, the software GRAMS_32 Spectra Notebase (Galactic Industries, Salem, NH) was used (www.thermo.com/eThermo/CMA/PDFs/Product/productPDF_24179.pdf).
Giant vesicle preparation
GUV composed of egg SM/egg Cer mixtures were prepared as described previously, using the electroformation method originally developed by Angelova and Dimitrov (18
). A previously described special temperature controlled chamber (19
,20
) was used for this purpose. Briefly, the process can be described in three steps: 1),
3 µl of the stock solution of lipid organic solution (0.2 mg/ml premixed with the fluorescent probe at 0.5 mol %) were spread on the surface of each Pt wire. The chamber was located under a stream of N2 during this procedure and then placed under vacuum overnight to remove the organic solvent; 2), aqueous solution was added to the chamber (a 200 mOsm sucrose solution prepared with Millipore-filtered water 17.5 M
/cm). The sucrose solution was previously heated to the desired temperature (above the lipid mixture phase transition,
68°C) and then sufficient volume was added to cover the Pt wires (
300 µl); and 3), the Pt wires were connected immediately to a function generator (Digimess Fg 100 plug-In, Eichenau, Germany), and a low frequency alternating current (AC) field (sinusoidal wave function with a frequency of 10 Hz and an amplitude of 3 V) was applied for 120 min. After vesicle formation, the AC field was turned off and the vesicles were collected with a pipette and transferred to a plastic tube.
Observation of giant vesicles
Aliquots of giant vesicles suspended in sucrose were added to an equiosmolar concentration of glucose solution. Due to the density difference between the two solutions, the vesicles precipitate at the bottom of the chamber, which facilitates observation of the GUV in the inverted fluorescence microscope. GUV preparations were observed in 8-well plastic chambers (Lab-tek Brand Products, Naperville IL). The chamber was located in an inverted confocal/two photon excitation fluorescence microscope (Zeiss, Karlsruhe, Germany) LSM 510 META NLO) for observation. The Ti:Sa laser used for two photon excitation mode was a MaiTai XF-W2S (Broadband Mai Tai with 10 W Millennia pump laser, tunable excitation range 710980 nm, Spectra Physics, Mountain View, CA). The excitation wavelengths were 543 nm (for DiIC18 in one photon excitation mode) and 780 nm (for Laurdan in two photon excitation mode). The images were simultaneously collected in two different channels using band-pass filters of 590 ± 25 nm and 424 ± 37 nm for DiIC18 and Laurdan, respectively. All these experiments were performed at room temperature (25°C).
| RESULTS |
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3.5 (Fig. 1). Of the various binary lipid compositions tested, those containing SM and Ch at various proportions are markedly resistant toward detergent solubilization, as expected from previous studies (6
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45°C/h up to 57°C and A500 recorded. Solubilization increases markedly above
40°C, i.e., the gel-fluid transition temperature of egg SM (24
100 nm in diameter) are used instead of MLV.
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) phase. In the presence of Cer, in the temperature range between the onset and completion of the phase transition at least three domains coexist, as indicated by the complex, asymmetric thermograms.
The presence of coexisting domains with different degrees of fluidity in SM/Cer bilayers, within a wide range of temperatures, as shown by the calorimetric results in Fig. 6, is further confirmed using a very different technique, namely fluorescence spectroscopy. To this aim the SM/Cer lipid membranes are doped with a small proportion of the fluorescent probe DPH. This probe is known to distribute uniformly over domains either in the gel or in the fluid phase (30
). DPH fluorescence is recorded as a function of temperature both in the absence and in the presence of TEMPO, a spin probe that partitions into the disordered, but not into the ordered, domains in lipid membranes. When all membrane components are in the gel phase, TEMPO is largely in the aqueous medium. TEMPO has the effect of quenching DPH fluorescence. As a consequence, in the presence of TEMPO, DPH fluorescence arises mainly from the more ordered domains, and the F/Fo ratio of fluorescence emission "in the presence/in the absence" of TEMPO should provide information on the existence of ordered domains in the membranes. The results as a function of temperature are shown in Fig. 7 for pure SM (empty triangles) and for various SM/Cer mixtures. For all mixtures at 25°C, quenching by TEMPO is very small because the lipids are in the gel (solid-ordered) phase at that temperature. DPH fluorescence (expressed as the F/Fo ratio) is set at 1.0 under those conditions. For pure SM, increasing T up to
33°C leads to a decrease in quenching (i.e., an increase in F/Fo), presumably due to a thermal increase in internal conversion (31
) unrelated to phase effects. Above 33°C, with the onset of the phase transition, TEMPO begins partitioning into the lipid membranes, and consequently quenching rises and F/Fo decreases steeply. A minimum is reached at
40°C, i.e., when only the fluid-disordered L
phase exists (Fig. 6). At higher temperatures thermal effects again cause a slight decrease in quenching.
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A direct comparison of the solubilization, calorimetric, and fluorescence measurements provides additional insights into the process. An example is shown in Fig. 8, where DSC, fluorescence quenching, and solubilization data for the 10% Cer sample are jointly presented as a function of temperature. Five different temperature regions can be distinguished, the various techniques showing good agreement within ±12°C. The high-T boundaries of regions 2, 3, and 4 correspond to the thermotropic transition end-points for the three components observed in the DSC endotherm. Note that in DSC and solubilization experiments samples have been heated at the same rate (45°C/h), whereas fluorescence measurements have been performed under equilibrium conditions. This may explain small differences in the boundaries between the various regions, as detected through the different techniques. Region 1 (below 35°C) corresponds mainly to the rather featureless gel phase. Region 2 (35°C41°C) witnesses a rather cooperative calorimetric transition, corresponding probably to the melting of SM-rich domains, with the concomitant steep increase in DPH quenching by TEMPO (decrease in F/Fo). Solubilization increases at this stage. Region 3 (41°C49°C) is characterized by a small change in CP (DSC signal) and a continued decrease in F/Fo. The simplest interpretation is that, in this temperature range, low-cooperativity melting is taking place, i.e., melting of small domains. Low cooperativity is at the origin of the small change in CP; however, melting is shown by the decrease in F/Fo. It is interesting that a large increase in solubilization occurs within this temperature range, i.e., as soon as the highly cooperative SM-rich domains are melted (together with some melting of Cer-enriched domains). Region 4 (49°C57°C) corresponds to the completion of the melting of Cer-enriched domains. Solubilization is also completed at this stage. (Turbidity does not decrease any further, and it may even increase because of the "cloud point" of Triton X-100 near 55°C.) F/Fo continues to decrease, albeit less steeply. Finally, in region 5 (above 57°C) when the bilayer is in the pure L
(fluid) phase, no further effects are detected.
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| DISCUSSION |
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40°C), iii), the Cer-enriched domains are detergent resistant, and iv), the nonsolubilized residue is enriched in Cer over the original bilayer composition. We shall briefly comment on these results and then examine their possible implications for cell biology studies.
Cer domains
Formation of Cer-rich domains (Figs. 69![]()
) due to poor mixing of Cer and SM does not come as a surprise, since it has already been demonstrated by Massey (34
) using fluorescence probe techniques. Cer-rich domains have also been observed in glycerophospholipid membranes with a variety of techniques (26
,29
,35
37
). Carrer and Maggio (29
) have noted the coexistence of two gel phases differing in Cer concentration. However the coexistence of domains well above the gel-fluid transition temperature of SM (Figs. 68
) has not been previously detected in SM/Cer binary mixtures to our knowledge. Domain coexistence in glycerophospholipid-Cer mixtures above the main transition temperature of the glycerophospholipid has been observed by Holopainen et al. (38
) and by Hsueh et al. (37
), among others.
Detergent resistance
The observation of a detergent-resistant residue in Triton X-100-treated SM/Cer bilayers (Figs. 1 and 2) is interesting because in studies using vesicles with defined lipid compositions such an effect has only been observed in mixtures containing Ch (and in bilayers composed of pure saturated PCs, well below their Tm) (5
). Particularly under our conditions, i.e., large (20:1) molar excess of Triton X-100 and long (24 h) equilibration times, only mixtures containing SM and Ch or certain other sterols have been found to be detergent resistant (12
,39
). The SM/Cer binary mixture is a welcome addition to the (very limited) collection of detergent-resistant mixtures, because Cer is the end product of SM hydrolysis by sphingomyelinase, thus the mixture is likely to form under certain conditions in the cell membranes. The fact that detergent resistance is not seen with short-chain Cers or with unsaturated phospholipids (Fig. 4) indicates that tight packing of the lipid hydrocarbon chain is essential for the phenomenon to take place. Perhaps the rigidity of Cer chains, whose melting temperature is above 90°C (27
,28
), and the rigidity of Ch ring exert a comparable effect in giving rise to DRMs, specifically in opposing the insertion of disordered detergent hydrocarbon chains. London and co-workers (39
41
) have observed that Cer stabilizes domain formation in SM/PC/Ch mixtures and that Cer displaces Ch from those domains. These authors suggest that tight lipid chain packing is essential for sterol displacement by Cer and for preventing unfavorable contacts between sphingolipid hydrocarbon chains and water. Our results support this hypothesis, underlining in addition the difficulty for detergents to become inserted in ordered domains. A similar situation was found for the solubilization of the tightly packed purple membrane patches in Halobacterium membranes (42
) and for the case of dimyristoyl PC/Ch bilayers in the liquid-ordered state (11
). Our observation of an increased solubilization at temperatures above Tm of the phospholipids (Fig. 5), together with comparable results by Schnitzer et al. (7
) and with the observation by Xu et al. (39
) of decreased domain formation at comparable temperatures, support equally the notion that tightly packed hydrocarbon lipid chains prevent detergent monomer incorporation.
The data in Figs. 3 and 913 reveal that Cer does not only give rise to the phenomenon of detergent resistance but is itself less easily solubilized than SM, so that the nonsolubilized residue is enriched in Cer. This is shown by chemical analysis of the nonsolubilized pellets in Fig. 3 and by the selective loss of the fluorescent SM-rich domains in Fig. 10. Phenomena of preferential solubilization of some lipids have been reported both in cell (43
,44
) and model (6
,45
) membranes. However the formation of insoluble domains enriched in Cer that are hardly detectable in the original vesicles but become clearly visible through the detergent action is shown in Figs. 12 and 13 in a particularly clear way. The rigid appearance of the Cer-rich domains, in contrast to the convoluted profiles of the remaining SM-rich areas, is noteworthy as it confirms the predictions based on the Cer physical properties ((13
), and references therein).
Implications for cell biology
At least two aspects of this work may be relevant in the context of contemporary cell biology. One is the observation of in-plane separation of Cer-rich and -poor domains, clearly demonstrated in Fig. 9. This, together with the previous spectroscopic and calorimetric evidence (26
,27
,29
,34
37
) and our own data in Fig. 6, supports firmly the idea that Cer stabilizes cell membrane "rafts" (39
,41
,46
) and induces the formation of large "platforms" in plasma membranes (14
,47
). Note that physiological effects of Cers, e.g., apoptosis, appear to be driven by sphingomyelinase activity (reviews by Cremesti (14
) and Futerman and Hannun (16
)) and that Cer is precisely the end product of SM hydrolysis by sphingomyelinase, thus our results in model membranes may well mimic the situation in the SM-rich cell plasma membrane upon sphingomyelinase activation.
No less important is the relevance of our results for the interpretation of the findings of DRMs. Membrane fractions resistant to detergent solubilization are often, and not always correctly, identified with cell membrane rafts (3
). The dangerous assumption is often made, albeit implicitly, that the detergent-resistant fraction existed as such in the native membrane and that the detergent has not modified it in any significant way. Our results, particularly the images in Figs. 12 and 13, reveal clearly that Cer-rich domains are dramatically enlarged as a result of the preferential solubilization of SM by Triton X-100, i.e., that, at least in our case, the large detergent-resistant domains are partly a detergent artifact. Also interesting is the observation that, beyond a certain temperature, domains melt (Figs. 68
) (see also Xu et al. (39
)) and simultaneously become amenable to solubilization (Fig. 5). The rather common observation in cell biology studies that a DRM fraction is found at 4°C but becomes solubilized at 37°C has been rather puzzling for workers in the area of detergent biophysics, because in principle membranes at higher temperatures should be more and not less resistant to detergent solubilization (6
,7
), provided that there are no lipid phase changes in that temperature interval. No significant amounts of lipid are found in the cell membranes with a gel-fluid transition temperature above 4°C, with the exception of SM. Most molecular species of SM found in cell membranes have a Tm in the 35°C40°C range (48
). Thus in the SM-rich plasma membrane the conditions exist for the observation of detergent-resistant fractions when the membrane is solubilized at 4°C but not at 37°C.
| ACKNOWLEDGEMENTS |
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This work was supported in part by grants from the Spanish Ministerio de Educación y Ciencia (No. BFU 2004-02955 to F.M.G., and No. BMC 2002-00784 to A.A.), and the University of the Basque Country (UPV00042.310/13552 to F.M.G.). Research in the laboratory of LAB is funded by a grant from the Danish Natural Science Research Council (SNF) (21-03-0569) and the Danish National Research Foundation (which supports MEMPHYS-Center for Biomembrane Physics). J.S. is a graduate student supported by the Basque government.
| FOOTNOTES |
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Submitted on June 3, 2005; accepted for publication October 11, 2005.
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