Raman spectroscopic study of an interdigitated lipid bilayer. Dipalmitoylphosphatidylcholine dispersed in glycerol

Dipalmitoylphosphatidylcholine (DPPC) dispersed in perdeuterated glycerol was investigated in order to determine the effects on the Raman spectra of hydrocarbon chain interdigitation in gel-phase lipid bilayers. Interdigitated DPPC bilayers formed from glycerol dispersions in the gel phase showed a decrease in the peak height intensity $\text{I}{}_{2850}\text{/I}{}_{2880}$ ratio, for the symmetric and asymmetric methylene CH stretching modes, respectively, as compared to non-interdigitated DPPC/water gel-phase dispersions. The decrease in this spectral ratio is interpreted as an increase in chain-chain lateral interactions. Spectra recorded in the 700–740 cm^?1 CN stretching mode region, the 1000–1200 cm^?1 CC stretching mode region and the 1700–1800 cm^? CO stretching mode region were identical for both the interdigitated and non-interdigitated hydrocarbon chain systems. At low temperatures the Raman peak height intensity ratios $\text{I}{}_{2935}\text{/I}{}_{2880}$ were identical for the DPPC/glycerol and DPPC/water dispersions, indicating that this specific index for monitoring bilayer behavior is insensitive to acyl chain interdigitation. The increase, however, in the change of this index at the gel-liquid crystalline phase transition temperature for the DPPC/glycerol dispersions implies a larger entropy of transition in comparison to the non-interdigitated DPPC/water bilayer system.     

Transport kinetics of dipicrylamine through lipid bilayer membranes. Effects of membrane structure

Charge-pulse current-relaxation studies have been performed with lipid bilayer membranes in the presence of the hydrophobic ion dipicrylamine. From the analysis of the relaxation times and amplitudes the translocation rate constant $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ of dipicrylamine as well as the partition coefficient β between membrane surface and water could be evaluated. In a first series of experiments membranes made from monoolein or dioleoylphosphatidylcholine in a number of different $\text{n-}\text{alkane}$ solvents were studied, as well as virtually solvent-free bilayer membranes made from monolayers. The thickness $\text{d}$ of the hydrocarbon layer of these membranes varied between 5.0 and 2.5 nm. While β was almost insensitive to variations in $\text{d}$, a strong decrease of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ with increasing membrane thickness was found; the observed dependence of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ on $\text{d}$ approximately agreed with the theoretically expected influence of membrane thickness on the height of the dielectric barrier. No specific differences between Mueller-Rudin films and solvent-free (Montal-Mueller) membranes other than differences in thickness were found. In a further series of experiments the chemical structure of the lipid was systematically varied (number and position of double bonds in the hydrocarbon chain, nature of the polar head group). The translocation rate constant $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ was much larger in phosphatidylethanolamine membranes than in phosphatidylcholine membranes. A strong increase of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ was found when the number of double bonds in the hydrocarbon chain was increased from one to three. These changes were discussed in terms of membrane fluidity and dielectric barrier height. Much higher values of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ were observed in lipids with ester linkage between hydrocarbon chain and glycerol backbone, as compared with the corresponding ether analogs. This finding is qualitatively consistent with determinations of dipolar potentials in monolayers of ester and ether lipids. When cholesterol is added to phosphatidylcholine membranes, the translocation rate constant $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ increases up to five-fold, while the partition coefficient β remains virtually constant. The variation of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ in this case can be largely accounted for by a decrease in membrane thickness and a concomitant reduction in dielectric barrier height. In membranes made from the negatively charged lipid phosphatidylserine the partition coefficient of dipicrylamine strongly increased with ionic strength, as expected from the Gouy-Chapman theory of the surface potential.     

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.     

Raman studies of conformational changes in model membrane systems

Laser Raman spectra of concentrated samples of phosphatidyl choline and phosphatidyl ethanolamine were taken at approximately 10° intervals over a temperature range of 90°–19°C. The spectral region from 30 to 3300 cm^?1 was investigated. Several new spectral features were discovered which are correlated to phospholipid liquid crystalline structure. It is shown that 1) frequency shifts occur in the $\text{PO}{}_2{}^{\mathrm{?}}$ symmetric stretch band which suggest a change in exposure of the PO₂ group to the solvent upon melting, 2) the frequency of the translational hydrocarbon mode around 150 cm^?1 appears to indicate the degree to which the hydrocarbon chain is extended, 3) the methyl and methylene stretch bands at 2890 and 2850 cm^?1 very clearly demonstrate hydrocarbon chain melting, and 4) the 720 cm^?1 band, previously assigned to the symmetric OPO diester stretch, appears to be due instead to the symmetric CN stretch of choline.     

Effect of calcium ionophore A23187 on electrogenic acid-base transport in turtle bladder Inhibition of acidification and stimulation of alkalinization

Turtle bladders bathed on both surfaces with identical HCO^?₃/CO₂-rich, Cl^?-free Na⁺ media and treated with ouabain and amiloride exhibit a transepithelial potential serosa electronegative to mucosa and a short-circuit current ($\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$) which is a measure of the net luminal acidification rate. Addition of calcium ionophore A23187 (10 μM) to the mucosal side of the epithelium rapidly reverses the direction of the potential difference and $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ and decreases tissue resistance. The resulting positive $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ resembles that previously observed in response to isobutylmethylxanthine (IBMX) and cAMP analogs. Reversal of the $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ is enhanced in bladders from severely alkalotic turtles. In contrast, in severely acidotic turtles, ionophore A23187 decreases, but does not reverse, the $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$. The data suggest that, like IBMX and cAMP analogs, the Ca ionophore stimulates an electrogenic alkalinization mechanism, but, unlike the former agents inhibits the concurrent acidification process as well.     

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.     

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.     

Nonelectrolyte substitution for water in phosphatidylcholine bilayers

Glycerol substitutes for water in multilamellar phosphatidylcholine liposomes in that the fluid spaces between bilayers, as well as their main transition temperatures, heat capacities, and ethalpies are very similar in water and in pure glycerol. One major difference is that the gel state phase of dipalmitoylphosphatidylcholine (DPPC) in glycerol consists of bilayers with fully interdigitated hydrocarbon chains. Interdigitated DPPC phases are also formed in ethylene glycol or in methanol (at low methanol content). In solutions of glycerol and water, the fluid spacing between bilayers is a function of mole fraction of glycerol X_g, reaching maximum values at $\text{X}{}_{\mathrm{<mtext>g</mtext>}}\text{≌ 0.1}$ for lipid in the liquid crystalline phase and at $\text{X}{}_{\mathrm{<mtext>g</mtext>}}\text{≌ 0.3}$ for the gel phase. These changes are explained in terms of a modification of the long-range Van der Waals attractive forces by glycerol.     

Cooperative unit size in the gel-liquid crytalline phase transition of dipalmitoyl phosphatidylcholine-water multilayers: An estimate from raman spectroscopy

The temperature dependence of the Raman spectral transitions assigned to the acyl chain C-C stretching modes of dipalmitoyl phosphatidylcholine was determined for the gel, phase transition and liquid crystalline states of the lipid multilayers. The van't Hoff enthalpy differences $\text{ΔH}{}_{\mathrm{<mtext>VH</mtext>}}$ between trans and gauche rotational isomers were obtained from the Raman spectral data for the temperature region characteristics of each bilayer state. An average size for the cooperative unit undergoing the chain melting process during the phase transition was estimated from the ratio of the appropriate van't Hoff enthalpy to an adjusted calorimetric enthalpy.     

Further studies on the effect of aldosterone on electrical resistance of toad bladder

The fall in transepithelial electrical resistance which accompanies aldosterone stimulation of short-circuit current ($\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$) in toad urinary bladder has been studied further to evaluate the possible causal role of this response in hormonal stimulation of Na⁺ transport. A steady-state change in tissue conductance was found to depend upon both the simultaneous stimulation of transport by the steroid and the metabolic state of the tissue. Changes in metabolic state alone did not alter resistance. A sustained increase in Na⁺ transport, dependent on pretreatment with aldosterone and elicited by addition of glucose, could be obtained without a sustained decrease in resistance. Amiloride, an inhibitor of Na⁺ uptake, produced changes in $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ that were linearly correlated with its effects on tissue conductance. On the basis of the $\text{conductance}\text{-I}{}_{\mathrm{<mtext>sc</mtext>}}$ relationship with amiloride, the $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ response to aldosterone was about two-fold higher than would be predicted from its effects on conductance alone. Despite the apparent lack of a simple quantitative dependence of the change in $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ on the change in conductance when the response is fully developed, the results suggest that conductance changes may mediate the initial or early stage of the response.     

Deuterated phospholipids as raman spectroscopic probes of membrane structure: Phase diagrams for the dipalmitoyl phosphatidylcholine(and its d62 derivative)-dipalmitoyl phosphatidylethanolamine system

Raman spectroscopic techniques have been used to construct phase diagrams for the binary phospholipid systems, DPPC-d₆₂/DPPE and DPPC/DPPE (DPPC, dipalmitoyl phosphatidylcholine; DPPE, dipalmitoyl phosphatidylethanolamine). For the former, the half-width of the C-²H stretching modes of the deuterated component near 2100 cm^?1 serves as an indicator of phospholipid fluidity. The phase behavior is described semi-quantitatively using regular solution theory with the following non-ideality parameters:

$\text{ρ}{}_0{}^{\mathrm{(1)}}\text{=0.75}\text{kcal/mol and}\text{ρ}{}_0{}^{\mathrm{(s)}}\text{=1.05}\text{kcal/mol}$

The use of deuterated phospholipids as one component of a binary mixture permits direct evaluation of the conformation of a particular component in the mixture throughout the phase separation region. The approach is demonstrated with the help of a simple model correlating the half-width of the symmetric C-²H stretching mode with the fraction of DPPC-d₆₂ hydrocarbon chains in the liquid crystalline state.The effect of chain perdeuteration on the phase behavior of DPPC with DPPE is evaluated by comparison of the phase diagram of the DPPC-d₆₂/DPPE system with that of DPPC-DPPE. The latter has been constructed previously from both probe and calorimetric techniques, and is created from the Raman spectroscopic data using the $\text{I(}\text{1130}\text{1100}\text{)}$ ratio to characterize the transgauche population ratio in non-deuterated hydrocarbon chains. A reasonable fit to the phase behavior is obtained using:

$\text{ρ}{}_0{}^{\mathrm{(1)}}\text{=0.85}\text{kcal/mol and}\text{ρ}{}_0{}^{\mathrm{(s)}}\text{=0.90}\text{kcal/mol}$

The similarities of the non-ideality parameters in the two phase diagrams indicate that the effect of perdeuteration on the phase behavior of DPPC is not extensive. The use of deuterated phospholipids as essentially unperturbed components of a model membrane system is justified.     

Influence of sterols on ion transport through lipid bilayer membranes

Charge-pulse relaxation experiments with the negatively charged lipophilic ions, dipicrylamine and tetraphenylborate, (as well as with the positively charged carrier system Rb⁺-valinomycin) have been carried out in order to study the influence of sterols on the ion transport through the lipid bilayer membrane. The mol fraction of the sterols (cholesterol, epicholesterol, ergosterol, stigmasterol, dihydrocholsterol, epicoprostanol and cholesterololeate) as referred to total lipid was varied in a wide range (mol fractions 0–0.8).The monoolein/sterol or dioleoylphosphatidylcholine/sterol mixtures were dissolved in $\text{n}$-hexadecane in order to minimize effects of the sterol on the membrane thickness.Cholesterol had a strong influence on the transport of the lipophilic ions. Its incorporation into monoolein membranes increased the rate constant ${}_{\mathrm{<mtext>i</mtext>}}$ of translocation up to 8-fold, but incorporation into phosphatidylcholine membranes had virtually no influence on $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$. The other sterols with one hydroxy group and cholesterololeate had no influence on the rate constant or the partition coefficient β. The results are discussed on the basis of a possible change of dipole potential of the membrane caused by cholesterol and its derivatives.In the case of valinomycin-mediated Rb⁺ transport only cholesterol had a strong influence on transport properties. The rate constants of association ($\text{k}{}_{\mathrm{<mtext>R</mtext>}}$) as well as the rate constants of translocation of the complex ($\text{k}{}_{\mathrm{<mtext>MS</mtext>}}$) and of the free carrier ($\text{k}{}_{\mathrm{<mtext>S</mtext>}}$) were reduced by incorporation of cholesterol up to eight-fold. The decrease of $\text{k}{}_{\mathrm{<mtext>S</mtext>}}$ and $\text{k}{}_{\mathrm{<mtext>MS</mtext>}}$ are possibly caused by a decrease of membrane fluidity, whereas the decrease of $\text{k}{}_{\mathrm{<mtext>R</mtext>}}$ may be due to an increase of surface potential. The different action of cholesterol on the two transport systems is discussed under the assumption that the adsorption plane of the lipophilic ion is located more towards the aqueous side and that of the ion-carrier complexes more towards the hydrocarbon side of the dipole layer.     

Photophosphorylation in bacterial chromatophores entrapped in alginate gel: Improvement of the physical and biochemical properties of gel beads with barium as gel-inducing agent

The immobilization of Rhodopseudomonas capsulata chromatophores by entrapment in an alginate gel is described. Alginate beads were prepared with Ba²⁺, Sr²⁺ and Ca²⁺ as gel-forming agents and compared for their mechanical strength, chemical resistance against disruption by phosphate-induced swelling, and yield of photophosphorylation activity. Barium alginate beads proved to have better physico-chemical properties than the more commonly used calcium alginate beads. After embedding in barium alginate gel, R. capsulata chromatophores retained a high yield (up to 70%) of their photophosphorylation capacity. Alginate entrapment did not cause a large increase in the Michaelis constant for ADP and phosphate, the substrates of adenosinetriphosphatase (ATPase). These constants were $\text{K}{}^{\mathrm{ADP}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 1.4 × 10}{}^{\mathrm{?5}}\text{m}$ and $\text{K}{}^{\mathrm{P}}{}_{\mathrm{i}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 2.2 × 10}{}^{\mathrm{?4}}\text{m}$ for free chromatophores and $\text{K}{}^{\mathrm{ADP}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 2.3 × 10}{}^{\mathrm{?4}}\text{m}$ and $\text{K}{}^{\mathrm{P}}{}_{\mathrm{i}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 5.6 × 10}{}^{\mathrm{?4}}\text{m}$ for chromatophores entrapped in barium alginate gel. However, embedding gave no additional protection against rapid inactivation of chromatophores upon storage at 3°C. Preliminary results with a batch reactor for continuous ATP regeneration are presented. The barium alginate method has two features which are not generally encountered at the same time, extremely mild conditions for entrapment and excellent physical properties of the gels beads, which make this method a suitable tool for the construction of bioreactors with immobilized cells or organelles.     

A reaction between the superoxide free radical and lipid hydroperoxide in sodium linoleate micelles

The oxidation of unsaturated fatty acid micelles by the superoxide free radical ($\text{O}{}^{\mathrm{?}}{}_2$), during γ irradiation in the presence of formate, is kinetically distinct from oxidation by hydroxyl free radicals (HO.). The evidence suggests that a direct reaction between ($\text{O}{}^{\mathrm{?}}{}_2$) and lipid hydroperoxide initiates a chain oxidation process in the micelles. While tetranitromethane, which reacts rapidly with ($\text{O}{}^{\mathrm{?}}{}_2$), protects the micelles from oxidation, active superoxide dismutase is no more effective than its apoprotein, due to lack of penetration of the micellar environment. We discuss these findings in the light of recent literature, and with reference to their possible significance for biological systems.     

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.     

Electrical capacity of black lipid films and of lipid bilayers made from monolayers

Planar bilayer membranes were formed from monolayers of a series of monounsaturated monoglycerides and lecithins. The hydrocarbon thickness of these membranes, as calculated from the electrical capacity, increases with the length of the fatty acid chain. The specific capacity of monoolein bilayers was found to be 0.745 μF/cm² which is nearly twice that of a monoolein black film made in the presence of decane, but is close to that obtained after freezing out the solvent from the black film. The hydrocarbon thickness of the bilayer, as calculated with a dielectric constant of 2.1, is considerably less than twice the length of the extended hydrocarbon chain of the monoglyceride.The specific capacity ($\text{C}{}_{\mathrm{<mtext>m</mtext>}}$) of bilayers made from monoolein monolayers showed a negligible voltage dependence, whereas the $\text{C}{}_{\mathrm{<mtext>m</mtext>}}$ increased significantly at a voltage of 150 mV in the case of Mueller-Rudin-type monoolein films with $\text{n-}\text{decane}$ as a solvent.     

The influence of cholesterol on head group mobility in phospholipid membranes

The dielectric dispersion in the MHz range of the zwitterionic dipolar phosphocholine head groups has been measured from 0–70°C for various mixtures of $\text{1,2-}\text{dipalmitoyl}\text{-sn-}\text{glycero-3-phosphocholine}$ (DPPC) and cholesterol. The abrupt change in the derived relaxation frequency $\text{f}{}_2$ observed for pure DPPC at the gel-to-liquid crystalline phase transition at 42°C reduces to a more gradual increase of frequency with temperature as the cholesterol content is increased. In general the presence of cholesterol increases the DPPC head group mobility due to its spacing effect. Below 42°C no sudden changes in $\text{f}{}_2$ are found at 20 or 33 mol% cholesterol, where phase boundaries have been suggested from other methods. Above 42°C, however, a decrease in $\text{f}{}_2$ at cholesterol contents up to 20–30 mol% is found. This is thought to be partly due to an additional restricting effect of the cholesterol on the number of hydrocarbon chain conformations and consequently on the area occupied by the DPPC molecules.