Electrostatic interaction between ion-penetrable multi-layered membranes

A theory of the double layer interaction regulated by the Donnan potential between two ion-penetrable membranes in an electrolyte solution developed previously by Ohshima and Kondo is extended to the case in which the membranes consist of many layers having different thickness and densities of membrane-fixed charges. The interaction force is found to be determined mainly by the contributions from layers located within the depth of 1/kappa (kappa, Debye-Hückel parameter) from the membrane surface. It is also predicted that the interaction force may alter its sign with changing electrolyte concentration.     

Electrostatic interaction between merocyanine 540 and liposomal and mitochondrial membranes

Summary The fluorescence of merocyanine 540 (MC) in liposomal and mitochondrial suspensions was measured under various conditions. Under a given condition, both the amount of dye bound to the membrane and the zeta potential were determined simultaneously. It was found that the fluorescence intensity was proportional to the amount of bound dye and correlated with the zeta potential of particles. The fluorescence intensity was represented quantitatively in terms of the Langmuir adsorption isotherm, when the electrostatic interaction acting between MC and membrane surface was properly taken into account. It was concluded that the changes in MC fluorescence in the liposomal and mitochondrial suspensions are mainly attributed to the changes in the surface potential of the membranes.     

Electrostatic interaction between two charged spherical molecules

An explicit analytic expression is obtained for the electrostatic energy of the interaction between two ion-impenetrable space-charged hard spheres as a model for spherical molecules in an electrolyte solution on the basis of the linearized Poisson-Boltzmann equation. An explicit expression for the potential distribution in a 3D-space is also found. The polarization effects due to the mutual influence between the spheres are taken into account. The analysis is done by assuming different dielectric permittivities of the respective spheres and of the solution as well. It is shown that the correction terms in the expression for the total energy of interaction arising from the polarization effects always correspond to forces of attraction between the spheres. The contribution of these terms to the total energy of interaction depends on the distance between the two spheres and the dielectric permittivities of the spheres and the solution as well as on the electrolyte concentration in the solution. A numerical simulation of the potential field topography is carried out at several values of the Debye-Hückel parameter. It is shown that the polarization effect can produce significant changes in the potential distribution in the case of strong interacting spheres.     

Evidence for negative gating charges in Myxicola axons

In Myxicola giant axons, the total amount of intramembrane charge available to move over the range -80 to + 120 mV decreases by 23% when the external pH is reduced from 7.3 to 5.5. The remaining charge moves more slowly at the onset of depolarizing pulse, but the rate of charge movement at the end of the pulse is unchanged. In contrast to acidic external pH, intramembrane charge movements are insensitive to alkaline external pH or any change in the internal pH. The results are consistent with a hypothesis in which a portion of the initial outward gating current consists of titratable negative charges moving inward.     

Surface charges on membranes

Summary The equations of membrane potential developed by Kobatake and coworkers have been applied to the literature data on the resting membrane potential of the crayfish andMyxicola axons to derive values for the surface charge density present on the axon membranes. Some shortcomings of the method are briefly discussed. The value for the surface charge density derived for the squid axon membrane agreed with a similar value derived from measurements of shifts in Na and/or potassium conductance-voltage relations following changes in the concentration of calcium in the solutions bathing the axons.     

Electrostatic interaction between redox cofactors in photosynthetic reaction centers

Intramolecular electron transfer within proteins is an essential process in bioenergetics. Redox cofactors are embedded in proteins, and this matrix strongly influences their redox potential. Several cofactors are usually found in these complexes, and they are structurally organized in a chain with distances between the electron donor and acceptor short enough to allow rapid electron tunneling. Among the different interactions that contribute to the determination of the redox potential of these cofactors, electrostatic interactions are important but restive to direct experimental characterization. The influence of interaction between cofactors is evidenced here experimentally by means of redox titrations and time-resolved spectroscopy in a chimeric bacterial reaction center (Maki, H., Matsuura, K., Shimada, K., and Nagashima, K. V. P. (2003) J. Biol. Chem. 278, 3921-3928) composed of the core subunits of Rubrivivax gelatinosus and the tetraheme cytochrome of Blastochloris viridis. The absorption spectra and orientations of the various cofactors of this chimeric reaction center are similar to those found in their respective native protein, indicating that their local environment is conserved. However, the redox potentials of both the primary electron donor and its closest heme are changed. The redox potential of the primary electron donor is downshifted in the chimeric reaction center when compared with the wild type, whereas, conversely, that of its closet heme is upshifted. We propose a model in which these reciprocal shifts in the midpoint potentials of two electron transfer partners are explained by an electrostatic interaction between them.     

Electrostatic interaction in the reaction between porphyrin and DNA

The association of tetrakis(4-N-methylpyridyl)porphine with salmon testes DNA in solution has been investigated in the presence of ethanol at 25 degrees C. It was found that the association constant was 1.14 x 10(6) M-1 and it increased with increasing the mole fraction of added ethanol. The behavior was very different from that in the case of usual intercalaters.     

The interaction between hemoglobin and two surfactants with different charges

The interactions of hemoglobin (Hb) with sodium dodecyl sulfate (SDS) and dodecyl trimethylammonium bromide (DTAB) are investigated by several methods. We observed the formation of hemichrome below the critical micelle concentration (cmc) of surfactant and the release of heme from Hb above the cmc. When pH value of Hb/surfactant system is lower than isoelectric point (pI) of Hb, the interaction of SDS with Hb is both electrostatic and hydrophobic, while the interaction of DTAB with Hb is hydrophobic mainly. On the contrary, when pH > pI, the interaction of SDS with Hb is hydrophobic mainly, while the interaction of DTAB with Hb is both electrostatic and hydrophobic. In the case where both the electrostatic interaction and hydrophobic interaction exist, the electrostatic interaction plays a more important role. Thus, SDS tends to interact with Hb more obviously than DTAB does when pH < pI and the interaction between DTAB and Hb is stronger when pH > pI.     

Electrostatic and hydrophobic interactions governing the interaction and binding of beta-lactoglobulin to membranes

The role of electrostatic and hydrophobic interactions in the binding and penetration of beta-lactoglobulin (betaLG) to preformed lipid membranes was studied using various phospholipid micelles and vesicles. Zwitterionic lysophospholipid micelles are able to induce the beta-sheet to alpha-helix transition, as judged by circular dichroism (CD), but the degree of transition is dramatically below and the amount of lipid required above that for anionic phospholipids with equivalent hydrocarbon chains. Anionic phospholipids with short hydrocarbon chains induce only low alpha-helical content in betaLG as compared to phospholipids with the same head group but longer hydrocarbon chains. These results suggest that both electrostatic and hydrophobic interactions are indispensable in betaLG-lipid interaction. Furthermore, air-water interface monolayer surface pressure and fluorescence anisotropy studies reveal that the membrane insertion of betaLG strongly depends on the nature of phospholipids, given the identical headgroup, particularly lipid packing. These results are supported by urea denaturation and acrylamide fluorescence quenching tests and by the FTIR-ATR polarization results for betaLG in multilayers on a surface. Under the same experimental conditions, the membrane binding and insertion of betaLG as well as the stability of the betaLG-lipid complexes can be enhanced by lowering the pH. Collectively, electrostatic interactions play a crucial role in all the processes involved in the betaLG-lipid interaction, while the presence of hydrophobic interaction remains necessary. Finally, betaLG biological function in the transport of fatty acids was tested by demonstrating the release of 2-AS from a 2-AS-betaLG complex on binding to lipids.     

Electrostatic recognition between enzyme and inhibitor: interaction between papain and leupeptin

Electrostatic forces are involved in a wide variety of molecular interactions that are of biological interest, including, among others, DNA-Protein interactions, protein folding, and the interactions between enzymes and their substrates and inhibitors. In this work, the interaction between papain and an inhibitor, leupeptin, is analyzed from the point of view of their electrostatic interaction. The computations enable one to suggest that negatively charged amino acids located in the region of the active site are responsible for creating an environment that enables efficient binding of the inhibitor. This binding occurs despite the fact that the net global charge of both molecules is positive; an explanation for this apparent contradiction is proposed.     

Estimation of surface charges in some biological membranes

Summary The resting membrane potential data existing in the literature for the giant axon of the squid, frog muscle and barnacle muscle have been analyzed from the standpoint of the theory of membrane potential due to Kobatake and co-workers. The average values derived for the effective charge density (where is a constant, , and represents the fraction of counterions that are free, and is the stoichiometric charge density in the membrane) present on the different biomembranes existing in their normal ionic environment are 0.3, 0.325 and 0.17 M for the squid axon, frog and barnacle muscles, respectively. On the assumption that the values of are 0.4 and 0.2 for nerve and muscle membranes, respectively, values of 0.75, 1.62 and 0.85 M have been derived for the stoichiometric charge density present in the respective biological membranes. These correspond to 1 negative charge per 222, 103 and 195 Å of the membrane area of the squid axon, frog and barnacle muscles, respectively.     

Mobile charges in the cell membranes ofHalicystis parvula

Charge-pulse experiments were performed on cells of the giant marine algaHalicystis parvula. At normal pH (8.2), the voltage decay following a charge-pulse of 500 ns duration fed to the vacuole could be described by summing two exponential relaxations. The amplitudes and time constants of these relaxations were widely separated. The parameters of the two relaxation processes were found to be pH-dependent. Reduction of the external pH value from pH 8.2 to 5 resulted in a complete change of the two relaxation processes within a few minutes. Only one relaxation process could be observed at pH 5, within the time resolution of our instrumentation. The experimental data could not be explained by a two-membrane model with reasonable values for the specific capacitances of tonoplast and plasmalemma. The results of the charge-pulse relaxations were found to be consistent with the assumption that both membranes have very similar electrical properties and that both contain mobile charges with a total surface concentration of about 30 nmol·m^-2 and a translocation-rate constant of about 500·s^-1. The mobile charges became neutralized at pH 5 hhich led to a decrease of the apparent specific capacitance of the algal cells. They are presumably either part of a transport system for cations or connected with the chloride pump ofHalicystis parvula.Abbreviation RC (R)esistance·(C)apacitance     

Electrostatic interaction in atomic force microscopy

In atomic force microscopy, the stylus experiences an electrostatic force when imaging in aqueous medium above a charged surface. This force has been calculated numerically with continuum theory for a silicon nitrite or silicon oxide stylus. For comparison, the Van der Waals force was also calculated. In contrast to the Van der Waals attraction, the electrostatic force is repulsive. At a distance of 0.5 nm the electrostatic force is typically 10^-12-10^-10 N and thus comparable in strength to the Van der Waals force. The electrostatic force increases with increasing surface charge density and decreases roughly exponentially with distance. It can be reduced by imaging in high salt concentrations. Below surface potentials of ≈50 mV, a simple analytical approximation of the electrostatic force is described.     

Potential-dependent interaction of chemical reagents with the gating mechanism of the nerve fiber sodium channel

The action of two water-soluble carbodiimides and of Woodward's reagent K on the properties of the gating mechanism of sodium channels of the Ranvier node membrane was investigated. Treatment with carbodiimide solution (pH 4.8–5.2) at a potential of –80 to –100 mV was shown to delay activation and inactivation of the channels considerably and to reduce the sensitivity of both gating functions to changes in membrane potential. The effective activation charge, determined relative to the limiting logarithmic slope of the activation curve (z_ef) was reduced by 1.7 times. Treatment of the membrane under the same conditions, but at zero holding potential, induced much smaller changes in properties of the gating mechanism; under these conditions z_ef remained unchanged. Woodward's reagent at high negative potential induced the same changes in the gating system as carbodiimide at 0 mV. The action of Woodward's reagent also depended on potential, but by a lesser degree than when carbodiimides were used. The results suggest that two types of carboxyl groups exist on the outer surface of the membrane: "mobile," which perform the role of gating particles and which are moved from the surface when the channel changes into the open or inactivated state, and "immobile," which face the external solution whatever the state of the channel.Institute of Cytology, Academy of Sciences of the USSR, Leningrad. Translated from Neirofiziologiya, Vol. 16, No. 5, pp. 577–590, September–October, 1984.     

pH dependence of electrostatic interaction between ion-penetrable membranes

A theory on the electrostatic repulsion between ion-penetrable membranes proposed previously by us is extended by taking into account the degree of dissociation of the membrane-fixed ionizable groups. A system of equations which determines the pH dependence of the membrane interaction is presented. The density of membrane-fixed charges is consistently determined as a function of the electric potential so that both the membrane-fixed charge density and the potential are not constant but functions of the membrane separation. The pH at the surface of interacting membranes is also calculated as a function of the membrane separation.     

Lipophilic interaction between thylakoid membranes and aliphatic compounds

Spinach chloroplasts pre-incubated at various temperatures, changed their photosynthetic activities (measured at 15°C) as the incubation temperature was raised; these activities showed characteristic activitytemperature profiles as follows:

1. The profiles were shifted to lower temperatures if various aliphatic compounds were present in the incubation mixture.
2. In general, the extent of the shift was proportional to the product of the concentration and the partition coefficient of the compound, i.e. to the concentration of the compound partitioned in the lipophilic chloroplast phase.

The combined effects of heat and the aliphatic compounds tested indicated that the lipophilic groups in these compounds play a determinative role in the heat denaturation of thylakoids. The consequence of such structure alterations is inactivation of photosynthetic functions. The lipophilic properties of the spinach thylakoid membrane as compared with certain artificial and natural membranes are described.     

Environment of the gating charges in the Kv1.2 Shaker potassium channel

Recently, the structure of the Shaker channel Kv1.2 has been determined at a 2.9-angstroms resolution. This opens new possibilities in deciphering the mechanism underlying the function of voltage-gated potassium (Kv) channels. Molecular dynamics simulations of the channel, embedded in a membrane environment show that the channel is in its open state and that the gating charges carried by S4 are exposed to the solvent. The hydrated environment of S4 favors a local collapse of the electrostatic potential, which generates high electric-field gradients around the arginine gating charges. Comparison to experiments suggests furthermore that activation of the channel requires mainly a lateral displacement of S4. Overall, the results agree with the transporter model devised for Kv channels from electrophysiology experiments, and provide a possible pathway for the mechanistic response to membrane depolarization.