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.     

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.     

Phase transition characteristics of diphosphatidylglycerol (cardiolipin) and stereoisomeric phosphatidyldiacylglycerol bilayers: Mono- and divalent metal ion effects

Synthesis and phase transition characteristics of aqueous dispersions of the homologous (12 : 0, 14 : 0, 16 : 0) diphosphatidylglycerols (cardiolipins) and phosphatidyldiacylglycerols are reported. Electron microscopy of the negatively stained aqueous dispersions reveals a characteristic lamellar structure suggesting that these phospholipid molecules are organized as bilayers in the aqueous dispersions. The phase transition temperature ($\text{T}{}_{\mathrm{<mtext>m</mtext>}}$) and the enthalpy of transition ($\text{ΔH}$) increase monotonically with chain length in the cardiolipin and phosphatidyldiacylglycerol series; $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ for phosphatidyldiacylglycerol is higher than that for cardiolipin of the same chain-length. The transition temperatures for the enantiomeric $\text{sn-3,3-}\text{and}\text{sn-1,1-}\text{phosphatidyldiacylglycerol}$ and for the diastereomeric, $\text{meso}\text{-sn-1,3-}\text{phosphatidyldiacylglycerol}$ are approximately the same. The molar enthalpy for the transition of cardiolipin-NH₄⁺ bilayers is approximately twice the value for the phosphatidylcholines of the same chain length, i.e., the molar enthalpy per acyl chain is approximately the same in the two systems. The transition temperatures for metal ion salts of C_{1 6}-cardiolipin exhibit a biphasic dependence upon the unhydrated ionic radii, i.e. the highest $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ is observed for Ca²⁺- cardiolipin and decreases for the salts of ions with smaller and larger ionic radii than that of Ca²⁺. The lowest $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ is observed for Rb⁺-cardiolipin. Monovalent metal salts of cardiolipin exhibit two phase transitions. This effect may result from different conformational packing of the four acyl chains due to differences in metal-phosphate binding.     

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.     

Effect of N-alkyl-N,N,N-trimethylammonium ions on phosphatidylcholine model membrane structure as studied by 31P-NMR

The interaction of |C_nH_2n+1N⁺(CH₃)₃| · I^? (n = 3, 6, 9, 12, 14, 16 or 18) with egg-yolk phosphatidylcholine-water dispersions has been studied by ³¹P-NMR spectroscopy. It is shown that the effective anisotropy of ³¹P chemical shift (?Δσ_eff) of the lamellar phospholipid liquid-crystalline phase L_α increases with increasing concentration and alkyl chain length of the drug. Addition of $\text{|}\text{C}{}_6\text{H}{}_{13}\text{N}{}^{\mathrm{+}}\text{(CH}{}_3\text{)}{}_3\text{| ·I}{}^{\mathrm{?}}$ or |C₉H₁₉N⁺(CH₃)₃|·I^? to the phospholipid-water dispersion at a molar ratio ammonium salt:phospholipid > 0.8 induces in the dispersion a structure with an effective isotropic phospholipid motion. This structure is unstable and slowly transforms into the hexagonal phase. These effects have not been observed in phospholipid-water dispersions mixed with the ammonium derivatives with the longer alkyl chains n  12, 14, 16 or 18. It is proposed that these results might explain the effects of the investigated drugs on the nerve, muscle and bacterial cells.     

The interaction of ions with phosphatidylcholine bilayers

The interaction of lanthanides and other cations with phosphatidylcholine bilayers present as single bilayer vesicles in ²H₂O has been investigated in terms of stoichiometry, apparent binding constants and environmental conditions.Lanthanides are shown to form 2 : 1 (molar ratio) phosphatidylcholine to metal ion complexes.The apparent binding constant $\text{K}{}_{\mathrm{<mtext>b</mtext>}}$ varies as a function of the quantity of metal ion bound and as a function of the Cl^? concentration. The apparent binding constant at “zero loading” is $\text{K}{}_0\text{= 1.25 · 10}{}^4\text{L}{}^2\text{·}\text{M}{}^{\mathrm{?}}\text{at}\text{0.15}\text{M KCl}$. It decreases exponentially with increased “loading” expressed as the molar ratio of metal ion bound to effective phosphatidylcholine concentration and increases exponential with Cl^? concentration.The interaction of lanthanides and divalent cations such as Ca²⁺ and Mg²⁺ is independent of pH in the pH range 3–7⁺ and 3–10 respectively, but is sensitive to the nature of the anion. The presence of anions enhances the interaction with polyvalent cations, the chaotropic anions showing the largest effect. The order of enhancement is $\text{Cl}{}^{\mathrm{?}}\text{< Br}{}^{\mathrm{?}}\text{< NO}{}_3{}^{\mathrm{?}}\text{< SCN}{}^{\mathrm{?}}\text{< I}{}^{\mathrm{?}}\text{< ClO}{}_4{}^{\mathrm{?}}$. The nature of the monovalent counterion (cation) has little effect on the enhanced binding of lanthanides in the presence of the above anions.The affinity of other polyvalent cations for phosphatidylcholine bilayers has been determined by competition with lanthanides. The physiologically important divalent cations Ca²⁺ and Mg²⁺ both bind less strongly (by about an order of magnitude) to the lipid surface. The order of binding of cations reflects direct binding to the phosphodiester group, with UO₂²⁺ showing the highest affinity.     

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.     

Amiloride stimulation of sodium transport in the presence of calcium and a divalent cation chelator

Amiloride in nM to μM concentrations stimulates the short circuit current ($\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$) of the toad urinary bladder by as much as 120% when applied in conjunction with apical Ca²⁺ and a divalent cation chelator. A significant decrease in transepithelial resistance ($\text{R}{}_{\mathrm{<mtext>t</mtext>}}$) is observed simultaneously. This response is spontaneously reversible and its amplitude is dependent upon apical sodium concentrations. The stimulated $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ persisted when acetazolamide (1 mM) was introduced, HPO₄^2? substituted for HCO₃^? or SO₄^2? replaced Cl^?. Consequently, the increase in $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ is not due to the change of Cl^?, H⁺ or HCO₃^? flux. This behavior in a ‘tight’ epithelium may be related to the mechanism controlling apical sodium permeability.     

Effects of anions on ADP-stimulated aggregation of bovine blood platelets

ADP-stimulated aggregation of bovine blood platelets was observed in media containing isotonic potassium salts of various monovalent anions. The aggregation depended on the anion in the medium, the order of aggregation being Cl^?, Br^?>I^?>SCN^?, $\text{ClO}{}_4{}^{\mathrm{?}}$. After 30-min incubation, the extent of aggregation of platelets in Cl^? or Br^? medium was little changed, whereas, that in SCN^? or $\text{ClO}{}_4{}^{\mathrm{?}}$ medium was remarkably decreased. This anion dependency of aggregation may be due to change in the membrane potential.     

Orientational order in the choline headgroup of sphingomyelin: A 14N-NMR study

An aqueous dispersion of fully hydrated bovine sphingomyelin was studied using ¹⁴N-NMR spectroscopy. Spectra were obtained as a function of temperature over the range 15–80°C, in both the liquid crystal and gel phases. In the liquid crystal phase, powder pattern lineshapes were obtained, whose quadrupolar splitting slowly decreases with increasing temperature. The spectra are increasingly broadened as the temperature is lowered through the phase transition into the gel phase. The linewidths and the second moments of these spectra indicate that the onset of a broad phase transition occurs at approx. 35°C, in agreement with previous calorimetric and ³¹P-NMR measurements. There is no evidence from the lineshapes for an hexagonal phase in this system, and this conclusion is supported by X-ray diffraction measurements carried out on aqueous dispersions of sphingomyelin in both phases. Assuming that the static nitrogen quadrupole coupling constant is the same for both sphingomyelin and dipalmitoyl-l-α-phosphatidylcholine (DPPC), the decrease observed in the quadrupolar splitting of sphingomyelin compared to that of DPPC indicates that the orientational order of the choline headgroup in liquid crystalline sphingomyelin is not the same as that of its counterpart in DPPC. Preliminary relaxation time measurements of $\text{T}{}_1$ and $\text{T}{}_2$ are presented which suggest that there are also dynamic differences between sphingomyelin and DPPC in the choline headgroup.     

Kinetics of phospholipid exchange between bilayer membranes

In an accompanying publication by Duckwitz-Peterlein, Eilenberger and Overath ((1977) Biochim. Biophys. Acta 469, 311–325) it is shown that the exchange of lipid molecules between negatively charged vesicles consisting of total phospholipid extracts from Escherichia coli occurs by the transfer of single lipid monomers or small micelles through the water. Here a kinetic interpretation is presented in terms of a rate constant, $\text{k}{}_{\mathrm{?}}$, for the escape of lipid molecules from the vesicle bilayer into the water. The evaluated rate constants are $\text{k}{}_{\mathrm{?}}{}^{\mathrm{<mtext>P</mtext>}}\text{= (0.86 ± 0.05) · 10}{}^{\mathrm{?5}}\text{s}{}^{\mathrm{?1}}$ and $\text{k}{}_{\mathrm{?}}{}^{\mathrm{<mtext>E</mtext>}}\text{= (1.09 ± 0.13) · 10}{}^{\mathrm{?6}}\text{s}{}^{\mathrm{?1}}$ for phospholipid molecules with $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$ and $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$, respectively, as the predominant acyl chain component. The rate constants are discussed in terms of the acyl chain and polar head group composition of the lipids.     

Dielectric dispersion of a single spherical bilayer membrane in suspension

Single spherical bilayer membranes of the Pagano-Thompson type (Pagano, R. and Thompson, T.E. (1967) Biochim. Biophys. Acta 144, 666–669), formed from monooleyl phosphate and cholesterol dissolved in CHCl₃/CH₃OH/n-decane, were subjected to a fast impedance analysis of high precision. Dielectric behavior of the whole system, as monitored from outside the spherical membrane, was sensitive to changes in the membrane state from the thick colored to the thin black state. With a spherical membrane 2–3 mm in diameter formed in the sample cavity containing 0.12 ml 10 mM NaCl, the former state was characterized by a dielectric dispersion having dielectric increment (Δ?) of some 10² and characteristic frequency ($\text{?}{}_{\mathrm{<mtext>c</mtext>}}$) around 10⁶ Hz, while the latter had $\text{Δ? ? 10}{}^5\text{and}\text{?}{}_{\mathrm{<mtext>c</mtext>}}\text{? 10}{}^3\text{Hz}$. Complex plane plots for both dispersions traced semicircles, indicating that the present system may be unequivocally analyzed to yield spherical radius and membrane capacity (C_m) on the basis of a well-established dielectric theory. C_m for the thin membranes has thus been determined to be 0.54 μF · cm^?2, in excellent agreement with a separate determination on planar membranes. The applicability of the present type of spherical membranes under dielectric monitoring to the study of membrane fusion or of exocytosis is suggested.     

Inhibition of nuclease activity in Bacillus subtilis following infection with bacteriophage SP82G.

The Raman Spectra of Blodgett-Langmuir multilayer assemblies made from behenic acid, barium behenate and barium cis-13 erucate are reported. In particular, the peak height intensity ratio of the hydrocarbon chain methylene CH stretch Raman bands, $\text{I}{}_{2890}\text{I}{}_{2850}$, for each multilayer assembly is compared to that of phosphatidylcholine in powders and water dispersions as well as to samples of crystalline hydrocarbon chains. It is found that the fatty acid multilayers are more ordered than the phospholipid samples but less ordered than the crystalline samples. It is suggested that Blodgett-Langmuir multilayer assemblies of lipid might be a useful reference in quantitative studies of packing order in lipid phases.     

The effect of a proteolipid from sarcoplasmic reticulum on the physical properties of artificial phospholipid membranes

Sarcoplasmic reticulum membranes from skeletal muscle contain a proteolipid ($\text{M}{}_{\mathrm{<mtext>r</mtext>}}\text{≈ 12 000}$) which reduces both the nonspecific ion and water permeabilities of artificial planar phospholipid bilayers. The proteolipid does not show any ionophoric effect or specific pore formation for Ca²⁺. The a.c. capacitance of the bilayers is unaffected whereas the refractive index is increased by the presence of proteolipid. The results support the view that the proteolipid interacts with the phospholipids in the bilayer interior and causes a condensation in the packing of the alkyl chains.     

Properties of bilayer membranes in the presence of dipicrylamine. A comparative study by optical absorption and electrical relaxation measurements

In order to test the question if a pool of lipophilic ions may exist in black lipid membranes which cannot be detected by electrical relaxation measurements we have performed simultaneously measurements of the optical absorption of a lipophilic ion. The absorbance of membrane-bound dipicrylamine at 410 nm was measured with a sensitive spectrophotometer which can detect absorbance changes $\text{? 4 · 10}{}^{\mathrm{?5}}$. A minimal concentration of about 6 · 10¹¹ dipicrylamine ions per cm² of the membrane could be detected with this instrument. The dipicrylamine concentration in the membrane obtained with the optical method $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ is compared with the concentrations $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$ obtained from simultaneous electrical relaxation measurements. $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ and $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$ agreed at low dipicrylamine concentrations (10^?8–10^?7 M in the aqueous phase) and showed saturation at higher concentrations (up to 5 · 10^?6 M). In the saturation range $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ was maximally four times higher than $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$. The significance of this difference is discussed together with general aspects of the saturation phenomenon.     

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.     

Effect of sanguinarine,a benzophenanthridine alkaloid,on frog skin potential difference and short circuit current

Sanguinarine, a benzophenanthridine alkaloid, causes an initial stimulation of frog skin short circuit current $\text{I}{}_{\mathrm{<mtext>sc</mtext>}}$ when present in the mucosal bathing medium at 10^?4 M. The stimulation is accompanied by an increase in spontaneous potential difference (PD) and increase in D.C. resistance. No effects are seen with sanguinarine in the serosal bathing medium. The initial stimulation is followed by a decrease in $\text{I}{}_{\mathrm{<mtext>se</mtext>}}$ and PD, but a continued increase in resistance. In skins whose initial spontaneous PD is high, no initial stimulation in ${}_{\mathrm{<mtext>se</mtext>}}$ and PD is seen; however, clamping these skins to a lower potential does not alter their initial inhibitory response to sanguinarine. Likewise, clamping the lower potential skins to higher potential does not alter their initial stimulatory response. Sanguinarine seems to be acting on the permeability barriers at the outer surface of the frog skin.