Interactions of proteins and cholesterol with lipids in bilayer membranes

Mixtures of lipids and proteins, the ATPase from rabbit sarcoplasmic reticulum, were studied by freeze-fracture electron microscopy and by measurement of the amount of fluid lipid with the spin label 2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPO). In dimyristoyl phosphatidylcholine vesicles the protein molecules were randomly distributed above the transition temperature, $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$, of the lipid and aggregated below $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$. For mixtures af dimyristoyl and dipalmitoyl phosphatidylcholine the existence of fluid and solid domains was shown in the temperature interval predicted from earlier TEMPO measurements. When protein was incorporated into this lipid mixture, freeze-fracture particles were randomly distributed in fluid lipids, or aggregated when only solid lipids were present.In mixtures of dimyristoyl phosphatidylcholine with cholesterol the protein was distributed randomly above the transition temperature of the phosphatidylcholine. Below that transition temperature the protein was excluded from a banded phase of solid lipid in the case of 10 mol% cholesterol. In mixtures containing 20 mol% cholesterol, protein molecules formed linear arrays, 50–200 nm in length, around smooth patches of lipid.Phase diagrams for lipid/cholesterol and lipid/protein systems are proposed which account for many of the available data. A model for increasing solidification of lipid around protein molecules or cholesterol above the transition temperarture of the lipid is discussed.     

A restatement of melittin-induced effects on the thermotropism of zwitterionic phospholipids

Perturbations induced by melittin on the thermotropism of dimyristoyl-, dipalmitoyl-, distearoylphosphatidylcholine and natural sphingomyelin are investigated and rationalized from data obtained by fluorescence polarization, differential scanning calorimetry and Raman spectroscopy. Depending on the technique and / or experimental conditions used, the observed effects differ at the same lipid to protein molar ratio, due to partial binding of melittin. The binding is more efficient for tetrameric than for monomeric melittin, but in both cases its affinity is weaker for phosphatidylcholine dispersions in the gel phase than for sonicated vesicles. For temperatures $\text{T ? T}{}_{\mathrm{<mtext>m</mtext>}}$ efficient binding occurs whatever the initial state of the lipids is. One can summarize the effects induced by melittin on the transition temperature as follows: (i) No upward shift is observed on synthetic phosphatidylcholines when lipid degradation is avoided. This is achieved by using highly purified melittin, phospholipase inhibitors, and / or non-hydrolysable lipids. (ii) Melittin monomer does not change $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$. (iii) When melittin tetramer is stabilized, it decreases $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ by 10–15 deg. C. The transition broadens, and is finally abolished for $\text{R}{}_{\mathrm{<mtext>i</mtext>}}\text{? 2}$. Very similar results are found for natural sphingomyelin. Fluorescence polarization indicates similar changes in order and dynamics of the acyl chains for all lipid studied. For $\text{T ? T}{}_{\mathrm{<mtext>m</mtext>}}$, fluorescence and Raman show that melittin decreases the amount of CH₂ groups in ‘trans’ conformation and the intermolecular order of the chains. According to fluorescence data, there is an increase of the rigid-body orientational order at $\text{T ? T}{}_{\mathrm{<mtext>m</mtext>}}$, while from Raman the positional intermolecular order decreases without significant change in the CH₂ groups ‘trans’/‘gauche’ ratio.     

Asymmetric antagonistic effects of an inhalation anesthetic and high pressure on the phase transition temperature of dipalmitoyl phosphatidic acid bilayers

The phase transition temperature ($\text{T}{}_{\mathrm{<mtext>t</mtext>}}$) of dipalmitoyl phosphatidic acid multilamellar liposomes is depressed 10°C by the inhalation anesthetic methoxyflurane at a concentration of 100 mmol/mol lipid. Application of 100 atm of helium pressure to pure phosphatidic acid liposomes increased $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ only 1.5°C. However, application of 100 atm helium pressure to dipalmitoyl phosphatidic acid lipsomes containing 100 mmol methoxyflurane/mol lipid almost completely antagonized the effect of the anesthetic. A nonlinear pressure effect is observed. In a previous study, a concentration of 60 mmol methoxyflurane/mol dipalmitoyl phosphatidylcholine depressed $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ only 1.5°C, exhibiting a linear pressure effect. The completely different behavior in the charged membrane is best explained by extrusion of the anesthetic from the lipid phase.     

Phosphatidylinositol distribution and translocation in sonicated vesicles. A study with exchange protein and phospholipase C

The distribution of phosphatidylinositol and phosphatidylcholine in sonicated phospholipid vesicles (phosphatidylcholine: diphosphatidylglycerol: phosphatidylinositol, 90:5:5 mol%) has been determined by the use of exchange protein from beef heart and phosphatidylinositol-specific phospholipase C from Staphylococcus aureus. Approximately 70% of the phosphatidylinositol in the sonicated vesicles was accessible to the exchange protein and 70–75% was accessible to the phospholipase C. A similar proportion (65%) of the phosphatidylcholine was accessible to the exchange protein suggesting that phosphatidylinositol was not preferentially located in either surface of the phospholipid bilayer. The rate of translocation of both phospholipids was very slow but the rate for phosphatidylcholine ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 4–7}\text{days}$) appeared to be greater than that for phosphatidylinositol ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 8–60}\text{days}$). Production of asymmetric vesicles by removing phosphatidylinositol from the outer surface with either exchange protein or phospholipase C did not induce rapid phospholipid translocation.     

Phospholipid exchange between bilayer membranes

The mode of interaction of aqueous dispersions of phospholipid vesicles is investigated. The vesicles (average diameter 950 Å) are prepared from total lipid extracts of Escherichia coli composed of phosphatidylethanolamine, phosphatidylglycerol and cardiolipin. One type of vesicle contains $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$, the other type $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$ as predominant acyl chain component. The vesicles show order?disorder transitions at transition temperatures, $\text{T}{}_{\mathrm{<mtext>t</mtext>}}\text{= 42°}\text{C}$ and $\text{T}{}_{\mathrm{<mtext>t</mtext>}}\text{= 29°}\text{C}$, respectively. A mixture of these vesicles is incubated at 45° C and lipid transfer is studied as a function of time using the phase transition as an indicator. The system reveals the following properties: Lipids are transferred between the two vesicle types giving rise to a vesicle population where both lipid components are homogeneously mixed. Lipid transfer is asymmetric, i.e. $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$-containing lipid molecules appear more rapidly in the $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$-containing vesicles than vice versa. At a given molar ratio of the two types of vesicles the rate of lipid transfer is independent of the total vesicle concentration. It is concluded that lipid exchange through the water phase by way of single molecules or micelles is the mode of communication of these negatively charged lipid vesicles.     

Differential polarized phase fluorometric studies of phospholipid bilayers under high hydrostatic pressure

Differential polarized phase fluorometry was used to quantify the rotational rate ($\text{R}$) and limiting anisotropy ($\text{r}{}_{\mathrm{\infty }}$) of the membrane probe diphenylhexatriene (DPH) in solvents and lipid vesicles exposed to hydrostatic pressures ranging from 1 bar to 2 kbar. These measurements reveal the effect of pressure on the phase-transition temperatures of the phosphatidylcholine vesicles, and the effects of pressure on order parameter of the acyl side-chain region of the membranes, the latter as indicated by $\text{r}{}_{\mathrm{\infty }}$. In addition to the well-known elevation of the transition temperature ($\text{T}{}_{\mathrm{<mtext>c</mtext>}}$) with pressure, our results demonstrate that increased pressure restores the order of the bilayers to that representative of temperatures below the transition temperature. We also found that solvents which allowed free isotropic rotation of DPH at 1 bar no longer allowed free rotation when sufficiently compressed; moreover, the apparent DPH rotational rate increased with $\text{r}{}_{\mathrm{\infty }}$. Pressure studies using both DPH and the charged DPH analogue, trimethylammonium DPH (TMA-DPH) indicated that the $\text{T}{}_{\mathrm{<mtext>c</mtext>}}$ of dipalmitoylphosphatidylcholine vesicles increased 23 K/kbar and an apparent volume change of 0.036 ml/mol lipid at the phase transition. Assuming, as has been proposed, that TMA-DPH is localized near the glycerol backbone region of the bilayers, these results indicate a similar temperature- and pressure-dependent phase transition in this region and the acyl side-chain region of the membrane.     

Lateral and transversal diffusion and phase transitions in erythrocyte membranes. An excimer fluorescence study

The lateral diffusion of the excimer-forming probe pyrene decanoic acid has been determined in erythrocyte membranes and in vesicles of the lipid extracts. The random walk of the probe molecules is characterized by their jump frequency, v_j, within the lipid matrix. At T = 35°C a value of v_j = 1.6 · 10³ s^?1 is found in erythrocyte membranes. A somewhat slower mobility is determined in vesicles prepared from lipid extracts of the erythrocyte membrane. Depending on structure and charge of the lipids we obtain jump frequencies between 0.8 · 10⁸ s^?1 and 1.5 · 10⁸ s^?1 at T = 35°C. The results are compared with jump frequencies yielded in model membranes.The mobility of molecules perpendicular to the membrane surface (transversal diffusion) is investigated. Erythrocyte ghosts doped with pyrene phosphatidylcholine were mixed with undoped ghosts in order to study the exchange kinetics of the probe molecule. A fast transfer between the outer layers of the ghost cells ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 1.6}\text{min at}\text{T = 37°}\text{C}$) is found. The exchange process between the inner and the outer layer of one erythrocyte ghost (flip-flop process) following this fast transfer occurs with a half-life time value of $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 100}\text{min at}\text{T = 37°}\text{C}$.The application of excimer-forming probes presumes a fluid state of the membrane. Therefore we investigated the phase transition behaviour using the excimer technique. Beside a thermotropic phase transition at T = 23°C and T = 33°C we observed an additional fluidity change at T = 38°C in erythrocyte ghosts. This transition is attached to a separation of the boundary lipid layer from the intrinsic proteins. No lipid phase transition is observed in liposomes from isolated extracts of the erythrocyte membrane with our methods.     

Lipid-protein interactions in membrane models fluorescence polarization study of cytochrome b5-phospholipids complexes

According to previous authors, cytochrome $\text{b}{}_5$, when extracted from bovine liver by a detergent method, is called cytochrome $\text{d-b}{}_5$. On the other hand, the protein obtained after trypsin action, which eliminates an hydrophobic peptide of about 54 residues, is called cytochrome $\text{t-b}{}_5$.Fluorescence polarization of the dansyl phosphatidylethanolamine probe inserted into phospholipid vesicles is very senstive to the binding of proteins, and so is a useful method to study lipid-protein interactions.The chromophore mobility, $\text{R}$, decreases markedly when dipalmitoyl phosphatidylcholine vesicles are incubated with cytochrome $\text{d-b}{}_5$, whereas $\text{R}$ does not change for cytochrome $\text{c}$ and cytochrome $\text{t-b}{}_5$. This can be interpreted as a strengthening of the bilayer, only due to the interaction of the hydrophobic peptide tail.Interaction of dipalmitoyl phosphatidylcholine vesicles with cytochrome $\text{d-b}{}_5$ occurs either below or above the melting temperature of the aliphatic chains (41 °C). Even for a high protein to lipid molar ratio (1 molecule of protein for 40 phospholipid molecules), the melting temperature is apparently unaffected.Phosphatidylserine and phosphatidylinositol do not interact at pH 7.7 with cytochrome $\text{d-b}{}_5$, because electrostatic forces prevent formation of complexes. At low pH, the interaction with the protein occurs, but the binding is mainly of electrostatic nature.     

Induction of a relatively fast transbilayer movement of phosphatidylcholine in vesicles. A 13C NMR study

[$\text{N-}{}^{13}\text{CH}{}_3$] Phosphatidylcholines are introduced into the outer monolayer of phosphatidylcholine vesicles with the phosphatidylcholine exchange protein from bovine liver. The transbilayer distribution of the [$\text{N-}{}^{13}\text{CH}{}_3$] phosphatidylcholine is measured with ¹³C NMR. The transbilayer movements of $\text{[N-}{}^{13}\text{CH}{}_3\text{]-}\text{dioleoyl}$ phosphatidylcholine and [$\text{N-}{}^{13}\text{CH}{}_3$] dimyristoyl phosphatidylcholine at 30°C in vesicles composed of these phosphatidylcholines are extremely slow processes with estimated half-times of days. [$\text{N-}{}^{13}\text{CH}{}_3$] Dioleoyl phosphatidylcholine introduced into dimyristoyl phosphatidylcholine vesicles migrates from the outer to the inner monolayer with a half-time of less than 12 h. The data suggest that differential changes in the lateral packing of the two monolayers might be a driving force for transbilayer transport of phospholipids.     

Transversal mobility in bilayer membrane vesicles: Use of pyrene lecithin as optical probe

Pyrene lecithin, a new excimer-forming lipid molecule, has been synthesized to examine the transversal mobility of probe molecules in lecithin bilayer vesicles. The rate of the lipid exchange is obtained by following the excimer yield as a function of time after mixing of fluorescence doped and undoped vesicles. A rapid exchange ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 11}\text{s}$) is followed by a slow transfer ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 8}\text{h}$). Above the lipid phase transition the fast transfer can be attributed to an exchange of lipid molecules from the outer layer of one vesicle to the outer layer of another one. The slow exchange is interpreted in terms of the ‘flip-flop’ process between the two layers of a single bilayer vesicle.Using pyrene and pyrene decanoic acid as probe molecules only the fast transfer through the water phase is observed ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 4}\text{s}$ for pyrene and $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 7}\text{s}$ for pyrene decanoic acid). This indicates that molecules like fatty acids or apolar membrane constituents must equilibrate very rapidly in a single bilayer vesicle.The water solubility or the critical micelle concentration of the probe molecules is determined and related to the transfer rates. An exchange process through the water phase via a monomeric state can be excluded.     

Phase transitions in phospholipid vesicles Fluorescence polarization and permeability measurements concerning the effect of temperature and cholesterol

We have studied the solid to liquid-crystalline phase transition of sonicated vesicles of dipalmitoylphosphatidylglycerol and dipalmitoylphosphatidylcholine. The transition was studied by both fluorescence polarization of perylene embedded in the vesicles, and by the efflux rate of trapped ²²Na⁺.Fluorescence polarization generally decreases with temperature, showing an inflection in the region 32–42°C with a mid-point of approximately 37.5 °C. On the other hand, the perylene fluorescence intensity increases abruptly in this region. To explain this result, we have proposed that, for $\text{T < T}{}_{\mathrm{<mtext>c</mtext>}}$ where $\text{T}{}_{\mathrm{<mtext>c</mtext>}}$ is the transition temperature, perylene is excluded from the hydrocarbon interior of the membranes, whereas, $\text{T < T}{}_{\mathrm{<mtext>c</mtext>}}$ this probe may be accommodated in the membrane interior to a large extent.The self-diffusion rates of ²²Na⁺ through dipalmitoylphosphatidylglycerol vesicles exhibit a complex dependence on temperature. There is an initial large increase in diffusion rates (approximately 100-fold) between 30 and 38 °C, followed by a decrease (approximately 4-fold) between 38 and 48 °C. A monotonic increase is then observed at temperatures higher than 48 °C. The local maximum of ²²Na⁺ self-diffusion rates at approximately 38 °C coincides with the mid-point of phase transition as detected by changes in fluorescence polarization of perylene with the same vesicles. Vesicles composed of dipalmitoylphosphatidylcholine show the same general behavior in terms of ²²Na⁺ self-diffusion rates at different temperatures, except that the local maximum occurs at approximately 42 °C.The temperature dependence of the permeability and the appearance of a local maximum at the phase transition region could be explained in terms of a domain structure within the plane of the membranes. This explanation is based on the possibility that boundary regions between liquid and solid domains would exhibit relatively high permeability to ²²Na⁺.Mixed vesicles composed of equimolar amounts of dipalmitoyl phospholipids and cholesterol show no abrupt changes in the temperature dependence of either perylene fluorescence polarization or ²²Na⁺ diffusion rate measurements. This is taken to indicate the absence of agross phase transition in the presence of cholesterol.     

Binding of bovine cytochrome b5 to phosphatidycholine liposomes Characterization of the reconstituted lipid-protein vesicles

Cytochrome $\text{b}{}_5$ was extracted and purified from beef liver by a detergent method (cytochrome $\text{d-b}{}_5$). The hydrophilic moiety which carries the heme group (cytochrome $\text{t-b}{}_5$) was prepared by trypsin action upon pure cytochrome $\text{d-b}{}_5$.Single-shelled lecithin liposomes form complexes with cytochromes $\text{d-b}{}_5$ up to a molar ratio of one protein for 35 phospholipids. The lipid-protein complexes were isolated by gel filtration on Sepharose 4B. They are hollow vesicles in which [³H]-glucose can be trapped. Their diameter is greater than that of the initial liposomes.Cytochrome $\text{t-b}{}_5$ does not interact with the vesicles. These results show that the hydrophobic tail is necessary for the binding and that the hydrophilic part of the protein is located on the outer face of the vesicles. This asymmetry is also proved by the action of reducing agents.Experiments with saturated phosphatidylcholines show that the protein interacts with the lipids both below the transition temperature $\text{T}{}_{\mathrm{M}}$. i.e. when the aliphatic chains are in a crystalline state, and above $\text{T}{}_{\mathrm{M}}$, when the alipathic chain are in a fluid state.¹H NMR spectra show that even at the maximum cytochrome $\text{d-b}{}_5$ concentration the presence of the proteins does not markedly change the dynamics to the phospholipid molecules. An asymmetric single-shelled vesicle structure is proposed for the complex.     

Role of the plasma membrane in the mechanism of cholesterol efflux from cells

In order to investigate the role of the plasma membrane in determining the kinetics of removal of cholesterol from cells, the efflux of [³H]cholesterol from intact cells and plasma membrane vesicles has been compared. The release of cholesterol from cultures of Fu₅AH rat hepatoma and WIRL-3C rat liver cells to complexes of egg phosphatidylcholine (1 mg / ml) and human high-density apolipoprotein is first order with respect to concentration of cholesterol in the cells, with half-times ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$) for at least one-third of the cell cholesterol of 3.2 ± 0.6 and 14.3 ± 1.5 h, respectively. Plasma membrane vesicles (0.5–5.0 μm diameter) were produced from both cell lines by incubating the cells with 50 mM formaldehyde and 2 mM dithiothreitol for 90 min. The efflux of cholesterol from the isolated vesicles follows the same kinetics as the intact, parent cells: the $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values for plasma membrane vesicles of Fu₅AH and WIRL cells are 3.9 ± 0.5 and 11.2 ± 0.7 h, respectively. These $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values reflect the rate-limiting step in the cholesterol efflux process, which is the desorption of cholesterol molecules from the plasma membrane into the extracellular aqueous phase. The fact that intact cells and isolated plasma membranes release cholesterol at the same rate indicates that variations in the plasma membrane structure account for differences in the kinetics of cholesterol release from different cell types. In order to investigate the role of plasma membrane lipids, the kinetics of cholesterol desorption from small unilamellar vesicles prepared from the total lipid isolated from plasma membrane vesicles of Fu₅AH and WIRL cells were measured. Half-times of cholesterol release from plasma membrane lipid vesicles of Fu₅AH and WIRL cells were the same, with values of 3.1 ± 0.1 and 2.9 ± 0.2 h, respectively. Since bilayers formed from isolated plasma membrane lipids do not reproduce the kinetics of cholesterol efflux observed with the intact plasma membranes, it is likely that the local domain structure, as influenced by membrane proteins, is responsible for the differences in $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values for cholesterol efflux from these cell lines.     

Lipid structural order parameters (reciprocal of fluidity) in biomembranes derived from steady-state fluorescence polarization measurements

This paper presents an interpretation of fluorescence polarization measurements in lipid membranes which are labelled with the apolar probe 1,6-diphenyl-1,3,5-hexatriene. The steady-state fluorescence anisotropy, $\text{r}{}_{\mathrm{<mtext>S</mtext>}}$, is resolved into a fast decaying or kinetic component, $\text{r}{}_{\mathrm{<mtext>f</mtext>}}$, and an infinitely slow decaying or static component, $\text{r}{}_{\mathrm{\infty }}$. The latter contribution, which predominates in biological membranes, is exclusively determined by the degree of molecular packing (order) in the apolar regions of the membrane; $\text{r}{}_{\mathrm{\infty }}$ is proportional to the square of the lipid order parameter. An empirical relation between $\text{r}{}_{\mathrm{<mtext>S</mtext>}}$ and $\text{r}{}_{\mathrm{\infty }}$ is presented, which is in agreement with a prediction based on a theory of rotational dynamics in liquid crystals. This relation enabled us to estimate a lipid structural order parameter directly from simple steady-state fluorescence polarization measurements in a variety of isolated biological membranes. It is shown that major factors determining the order parameter in biomembranes are the temperature, the cholesterol and sphingomyelin content and (in a few systems) the membrane intrinsic proteins.     

A NMR study of the ionization of fatty acids,fatty amines and N-acylamino acids incorporated in phosphatidylcholine vesicles

The ionization of fatty acids, fatty amines and $\text{N-}\text{acylamino}$ acids incorporated in phosphatidylcholine single-walled vesicles has been measured. The guest molecules have been specifically enriched with ¹³C and titrated by using NMR spectroscopy. The apparent p$\text{K}{}_{\mathrm{a}}$ of fatty acids in phosphatidylcholine bilayers is 7.2–7.4 and those of fatty amines are approx. 9.5. These p$\text{K}{}_{\mathrm{a}}$ values depend on many different parameters related to the structure of the lipid/ solution interface, to the composition of the aqueous medium and to the localization of the ionizable groups. A special sensitivity to the ionic strength and to the surface charge has been found. A positive surface charge decreases the p$\text{K}{}_{\mathrm{a}}$ value whereas a negative one increases it, the total range of variation being 2.5–3 units. In a qualitative macroscopic interpretation, it is proposed that p$\text{K}{}_{\mathrm{a}}$ is essentially determined by the low polarity of the lipidic matrix.     

The influence of charge on phosphatidic acid bilayer membranes

A complete titration of phosphatidic acid bilayer membranes was possible for the first time by the introduction of a new anaologue, $\text{1,2-}\text{dihexadecyl}\text{-sn-}\text{glycerol-3-phosphoric}$ acid, which has the advantage of a high chemical stability at extreme pH values. The synthesis of this phosphatidic acid is described and the phase transition behaviour in aqueous dispersions is compared with that of three ester phosphatidic acids; $\text{1,2-}\text{dimyristoyl}\text{-sn-}\text{glycerol-3-phosphoric}$ acid, 1,3-dimyristoylglycerol-2-phosphoric acid and $\text{1,2-}\text{dipalmitoyl}\text{-sn-}\text{glycerol-3-phosphoric}$ acid.The phase transition temperatures ($\text{T}{}_{\mathrm{<mtext>t</mtext>}}$) of aqueous phosphatidic acid dispersions at different degrees of dissociation were measured using fluorescence spectroscopy and 90° light scattering. The $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ values are comparable to the melting points of the solid phosphatidic acids in the fully protonated states, but large differences exist for the charged states.The $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ vs. pH diagrams of the four phosphatidic acids are quite similar and of a characteristic shape. Increasing ionisation results in a maximum value for the transition temperatures at pH 3.5 ($\text{p}\text{K}{}_1$). The regions between the first and the second $\text{p}\text{K}$ of the phosphatidic acids are characterised by only small variations in the transition temperatures (extended plateau) in spite of the large changes occurring in the surface charge of the membranes. The slope of the plateau is very shallow with increasing ionisation. A further decrease in the H⁺ concentration results in an abrupt change of the transition temperature. The slope of the $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ vs. pH diagram beyond $\text{p}\text{K}{}_2$ becomes very steep. This is the     

N-NBD-l-α-Dilauroylphosphatidylethanolamine. A new fluorescent probe to study spontaneous lipid transfer

Migration of the fluorescent phospholipid $\text{N-(7-}\text{nitro-2,1,3-benzoxadiazol-4-yl)-}\text{l}\text{-α-dilauroylphosphatidyl-ethanolamine}$ between small sonicated egg phosphatidylcholine vesicles was studied by use of the fluorescence resonance energy transfer method. Contrary to the results of lipid transfer experiments reported for acyl chain NBD-labeled phospholipids (Nichols, J.W. and Pagano, R.E. (1982) Biochemistry 21, 1720–1728), the migration kinetics of N-NBD-DLPE had to be described by a sum of two exponential functions. The fast component $\text{(t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 38}\text{min}\text{)}$ was assigned to lipid transfer via soluble monomers and the slow component $\text{(t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 400}\text{min}\text{)}$ to transbilayer motion. A reversible four-stage process is suggested as a kinetic model. Mathematical treatment of this scheme is given yielding an analytical expression for the time dependence of NBD emission intensity. The use of N-NBD-DLPE in the resonance energy transfer measurements offers the advantage of simple chemical synthesis of the fluorescent probe and leads to additional information on transbilayer motion which was not available with the NBD-labeled lipids used so far.     

A mechanism for ethanol-induced damage to liver mitochondrial structure and function

Mitochondria isolated from rats chronically fed ethanol demonstrated a marked inability to produce energy. The respiratory control ratio, the ADP/O ratio and state 3 respiration rates were all decreased. Coupled with other data, a progression of ethanol-induced changes is proposed with site I being altered prior to site II. Quantitation of mitochondrial cytochromes revealed decreases in cytochromes $\text{b}$ and $\text{aa}{}_3$ and an increase in $\text{c}{}_1$. Evaluation of respiration activity in relation to temperature showed ethanol-induced changes in the transition temperature ($\text{T}{}_{\mathrm{f}}$) which may have been related to changes in the lipid composition of the inner membrane. Mitochondrial membranes were separated, and analysis of fatty acids and phospholipids was performed. Various fatty acids were altered in both membranes; however, the outer membrane was altered more severely. A decrease in the arachidonate : linoleate ratio was observed only in the outer membrane; however, there was no ethanol-induced change in degree of unsaturation in either membrane. Phospholipid quantitation showed a reduction of total lipid phosphorous/mg protein in both membrane fractions; however, the inner membrane was most affected. Cardiolipin was the only phospholipid in this membrane which remained unaltered. The evidence indicates that the mechanism for ethanol-induced damage to the liver mitochondrion involves lipid compositional changes as well as changes in cytochromes and possibly other proteins.