Unidirectional fluxes in saturated single-file pores of biological and artificial membranes I. Pores containing no more than one vacancy

A theoretical treatment of isotope fluxes in filled single-file pores is given. The treatment is confined to pores permitting only one vacancy at a time. Tracer flux, unidirectional fluxes and net flux are calculated. The exponent n which is obtained by representing the ratio of unidirectional fluxes as a power of the electrochemical activity-ratio proves to be closely related with m, the number of sites per pore. The minimum and maximum values of n are m?1 and m. It is shown that measurement of n provides sufficient information to determine m if the energetic properties of sites and barriers do not change too much with varying concentrations. Unlike the unidirectional fluxes, the net fluxes yield no direct information about the number of sites. The concentration dependence of the net fluxes, however, can be used to discriminate between the two limiting cases, n = m?1 and n = m. It is interesting with regard to the instantaneous potassium currents of nerve membranes that a suitable choice of the energetic parameters of a filled pore leads to a quasi-linearity of the net flux-voltage curves, which is only slightly affected by variation of the external concentration.     

Rate theory models for ion transport through rigid pores. II. Time-dependent analysis of the single-file model with special reference to oscillatory behavior

This article deals with the time-dependent evolution of the single-file movement of ions through channels of both biological and artificial membranes. The single-file transport process may exhibit not only the usual relaxation behaviour but also oscillatory behaviour as a steady state is approached after an initial perturbation. A necessary condition for the occurrence of oscillations is that the system acts sufficiently far from equilibrium. The occurrence of oscillations is due to the interactions within the transport system which are taken into account by the single-file model; these are the electrostatic repulsion between the ions being transported, and the competition of the ions for the free binding sites within the pore. Information about the strength of the interactions can be obtained by measuring the damping of the transport observables (e.g. the electric current): The stronger the inter-ionic repulsion, the more apparent the oscillatory behaviour will become. Furthermore, the damping is influenced by the microscopic structure of the transport system (i.e. the energy profile of the pores). With an increasing degree of microscopicity, i.e. with a decreasing number of binding sites and an increasingly irregular pore profile, the oscillations become more damped. However, a considerable oscillatory behaviour can only be predicted for pores with both a sufficiently regular structure and a sufficiently large number of binding sites. For this class of pores, however, the measurement of the damping represents an appropriate method of gaining information which could exceed that obtainable from the usual methods of measuring stationary quantities (e.g. stationary conductance). Moreover, our goal is to explain theoretically how the oscillatory behaviour can be interpreted in terms of the order inherent in the ionic movement, which is determined by both the external and internal forces and the microscopic properties of the system.     

Large-ligand adsorption to membranes: II. Disk-like ligands and shape-dependence at low saturation

Large-ligand adsorption to membranes or cells is considered in the absence of cooperative interactions. For the low-saturation regime, a general and exact treatment is given by means of the concept of excluded areas. With the help of this formalism, shape dependence of the adsorption behavior can be discussed quantitatively. In addition, a formalism is presented which allows to calculate binding curves at arbitrary saturation for ligands having a symmetric shape (disks, regular polygons). The underlying model is a modified version of the hard core fluid theory of Andrews (Andrews, F.C. (1976) J. Chem. Phys. 64, 1941–1947). Apart from applications to symmetric ligands, the results can be used to derive limiting conditions for ligands of any shape.     

Oxytocin interaction with lipids of artificial and biological membranes

It is established on the liposomes, lipid and proteolipid monolayers, that the first process of bounding of oxytocin with plasmatic membrane of smooth muscle cells of small intestine is the interaction of hormone molecules with molecules of membrane lipids, adsorption and the instillation of peptide into lipid mono- and bilayer.     

Diltiazem at high concentration increases the ionic permeability of biological membranes

Summary The effects of diltiazem, a drug which inhibits the calcium channels in cardiac muscle as well as the light-sensitive channels in photoreceptor cells, were studied on ionic fluxes in both membrane and intact cell preparations. Diltiazem nonselectively increased the ionic permeability to both anions and cations in photoreceptor rod outer segment and synaptic membrane vesicles as well as in intact erythrocytes. Under our conditions, the estimated threshold for the diltiazem effect varied between 12.5 and 200 m. In each case the concentration dependence exhibited the sigmoidal shape characteristic of positive cooperativity. The effect of diltiazem on ionic fluxes from phospholipid vesicles were strongly influenced by phospholipid composition and membrane charge. By contrast, diltiazem inhibited the efflux of⁸⁶Rb from photoreceptor cells of intact aspartate-isolated retina, an effect opposite to that of diltiazem on ionic permeabilities in photoreceptor membrane vesicle preparations.These data raise serious doubts on the specificity of diltiazem as a calcium channel blocker or as a cGMP channel blocker when used at concentrations higher than 10 m.     

Effects of saturated long-chain N-acylethanolamines on voltage-dependent Ca2+ fluxes in rabbit T-tubule membranes

The effects of saturated long-chain (C: 16-22) N-acylethanolamines and a series of saturated fatty acids with the same length of carbon chains were investigated on depolarization-induced (45)Ca(2+) fluxes mediated by voltage-dependent Ca(2+) channels in transverse tubule membrane vesicles from rabbit skeletal muscle. Vesicles were loaded with (45)Ca(2+) and membrane potentials were generated by establishing potassium gradients across the vesicle using the ionophore valinomycin. Arachidonoylethanolamide and docosaenoylethanolamide but not palmitoylethanolamide and stearoylethanolamide (all 10 microM) caused a significant inhibition of depolarization-induced (45)Ca(2+) fluxes and specific binding of [(3)H]Isradipine to transverse tubule membranes. On the other hand, saturated fatty acids including palmitic, stearic, arachidic, and docosanoic acids (all 10 microM) were ineffective in functional and radioligand binding experiments. Additional experiments using endocannabinoid metabolites suggested that whereas ethanolamine and arachidic acids were ineffective, arachidonoylethanolamide inhibited Ca(2+) effluxes and specific binding of [(3)H]Isradipine. Further studies indicated that only those fatty acids containing ethanolamine as a head group and having a chain length of more than 18 carbons were effective in inhibiting depolarization-induced Ca(2+) effluxes and specific binding of [(3)H]Isradipine. In conclusion, results indicate that depending on the chain length and the head group of fatty acid, N-acylethanolamines have differential effects on the function of voltage-dependent Ca(2+) channels and on the specific binding of [(3)H]Isradipine in skeletal muscle membranes.     

Electrical excitability of artificial enzyme membranes: II. Electrochemical and enzyme properties of immobilized acetylcholinesterase membranes

This paper deals with aspects of the reciprocal interaction between enzyme activity and the microenvironment or the potential difference in artificial proteinaceous membranes bearing cross-linked acetylcholinesterase. The potential difference resulting from asymmetric substrate injection into the system is recorded as a function of time. The influence of the membrane charge density on both enzyme activity and potential difference is studied by varying the external solution pH. The enzyme specific potential is initiated by local change of pH at the membrane level and the dependence on the buffer strength is studied. The recorded potential difference appears to be the result of the reciprocal interaction between enzyme reaction and the diffusion of substrate or products.     

Omiganan interaction with bacterial membranes and cell wall models. Assigning a biological role to saturation

Omiganan pentahydrochloride (ILRWPWWPWRRK-NH₂·5Cl) is an antimicrobial peptide currently in phase III clinical trials. This study aims to unravel the mechanism of action of this drug at the membrane level and address the eventual protective role of peptidoglycan in cell walls. The interaction of omiganan pentahydrochloride with bacterial and mammalian membrane models - large unilamellar vesicles of different POPC:POPG proportions - was characterized by UV-Vis fluorescence spectroscopy. The molar ratio partition constants obtained for the two anionic bacterial membrane models were very high ((18.9 ± 1.3) × 10³ and (43.5 ± 8.7) × 10³) and about one order of magnitude greater than for the neutral mammalian models ((3.7 ± 0.4) × 10³ for 100% POPC bilayers). At low lipid:peptide ratios there were significant deviations from the usual hyperbolic-like partition behavior of peptide vesicle titration curves, especially for the most anionic systems. Membrane saturation can account for such observations and mathematical models were derived to further characterize the peptide-lipid interaction under those conditions; a possible relation between saturation and MIC was deduced; this was supported by differential quenching studies of peptide internalization. Interaction with the bacterial cell wall was assessed using Staphylococcus aureus peptidoglycan extracts as a model. A strong partition towards the peptidoglycan mesh was observed, but not as large as for the membrane models.     

Omiganan interaction with bacterial membranes and cell wall models. Assigning a biological role to saturation

Omiganan pentahydrochloride (ILRWPWWPWRRK-NH(2).5Cl) is an antimicrobial peptide currently in phase III clinical trials. This study aims to unravel the mechanism of action of this drug at the membrane level and address the eventual protective role of peptidoglycan in cell walls. The interaction of omiganan pentahydrochloride with bacterial and mammalian membrane models - large unilamellar vesicles of different POPC:POPG proportions - was characterized by UV-Vis fluorescence spectroscopy. The molar ratio partition constants obtained for the two anionic bacterial membrane models were very high ((18.9+/-1.3)x10(3) and (43.5+/-8.7)x10(3)) and about one order of magnitude greater than for the neutral mammalian models ((3.7+/-0.4)x10(3) for 100% POPC bilayers). At low lipid:peptide ratios there were significant deviations from the usual hyperbolic-like partition behavior of peptide vesicle titration curves, especially for the most anionic systems. Membrane saturation can account for such observations and mathematical models were derived to further characterize the peptide-lipid interaction under those conditions; a possible relation between saturation and MIC was deduced; this was supported by differential quenching studies of peptide internalization. Interaction with the bacterial cell wall was assessed using Staphylococcus aureus peptidoglycan extracts as a model. A strong partition towards the peptidoglycan mesh was observed, but not as large as for the membrane models.     

Oxygen diffusion in biological and artificial membranes determined by the fluorochrome pyrene

Quenching of pyrene fluorescence by oxygen was used to determine oxygen diffusion coefficients in phospholipid dispersions and erythrocyte plasma membranes. The fluorescence intensity and lifetime of pyrene in both artificial and natural membranes decreases about 80% in the presence of 1 atm O2, while the fluorescence excitation and emission spectra and the absorption spectrum are unaltered. Assuming the oxygen partition coefficient between membrane and aqueous phase to be 4.4, the diffusion coefficients for oxygen at 37 degrees C are 1.51 X 10(-5) cm2/s in dimyristoyl lecithin vesicles, 9.32 X 10(-6) cm2/s in dipalmitoyl lecithin vesicles, and 7.27 X 10(-6) cm2/s in erythrocyte plasma membranes. The heats of activation for oxygen diffusion are low (less than 3 kcal/degree-mol). A dramatic increase in the diffusion constant occurs at the phase transition of dimyristoyl and dipalmitoyl lecithin, which may result from an increase in either the oxygen diffusion coefficient, partition coefficient, or both. The significance of the change in oxygen diffusion below and above the phase transition for biological membranes is discussed.