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At least 19 recordsLinked to original sources
PubMed1979

Electrostatic interactions at charged lipid membranes. Electrostatically induced tilt.

The changes in bilayer structure induced by surface charges in the case of an ionizable lipid were studied by X-ray diffraction, Raman spectroscopy, and film-balance measurements. With increasing surface charge in the ordered phase, the X-ray results show a decrease in bilayer thickness, whereas the hydrocarbon chain packing stays essentially constant, the Raman data signify that the internal chain ordering does not change, and the monolayer studies show a lateral expansion of the bilayer. These results are interpreted in terms of a tilt of the chains caused by the surface charges on the polar heads. The tilt angle between the direction of the chains and the bilayer normal is obtained by a detailed theoretical evaluation. The tilt allows for a better understanding of the electrostatically induced shift of the phase transition temperature and of the shift induced by the binding of water in the case of lecithin in contrast ethanolamine.

Hydrogen-Ion Concentration↗
PubMed1978

Electrostatic calculations for an ion channel. II. Kinetic behavior of the gramicidin A channel.

A theoretical model of the gramicidin A channel is presented and the kinetic behavior of the model is derived and compared with previous experimental results. The major assumption of the model is that the only interaction between ions in a multiply-occupied channel is electrostatic. The electrostatic calculations indicate in a multiply-occupied channel is electrostatic. The electrostatic calculations indicate that there will be potential wells at each end of the channel and, at high concentrations, that both wells can be occupied. The kinetics are based on two reaction steps: movement of the ion from the bulk solution to the well and movement between the two wells. The kinetics for this reaction rate approach are identical to those based on the Nernst-Planck equation in the limit where the movement between the two wells is rate limiting. The experimental results for sodium and potassium are consistent with a maximum of two ions per channel. To explain the thallium results it is necessary to allow three ions per channel. It is shown that this case is compatible with the electrostatic calculations if the presence of an anion is included. The theoretical kinetics are in reasonable quantitative agreement with the following experimental measurements: single channel conductance of sodium, potassium, and thallium; bi-ionic potential and permeability ratio between sodium-potassium and potassium-thallium; the limiting conductance of potassium and thallium at high applied voltages; current-voltage curves for sodium and potassium at low (but not high) concentrations; and the inhibition of sodium conductance by thallium. The results suggest that the potential well is located close to the channel mouth and that the conductance is partially limited by the rate going from the bulk solution to the well. For thallium, this entrance rate is probably diffusion limited.

Biological Transport↗
PubMed1975

Indicator dyes as probes of electrostatic potential changes on macromolecular surfaces.

An indicator dye attached to an electrostatically charged macromolecular surface generally has a pK value (pKb') different from that of uncombined dye (pKf'). The question if changes in (pKb' - pKf'), designated as increment incrementpK, records changes in the electrostatic potential at the binding site has been examined in spectrophotometric and binding experiments, using the interaction of Chlorophenol Red and Phenol Red with human serum albumin and cationic micelles as examples. (1) In serum albumin solutions increment incrementpK is decreased by a reduction of pH. The decrease is correlated with the increase in positive charges on the protein molecule, and the response is attenuated by high ionic strength in accordance with electrostatic theory. (2) Opposite changes in binding affinity to serum albumin and increment incrementpK as a function of pH are observed; the binding of basic (bivalent anion) dye is more susceptible to a change in pH than in the acidic (univalent anion) form. (3) Preferential uptake of the basic as compared to the acidic form of dye is observed by binding to cetyltrimethylammonium chloride and cetylpyridinium chloride micelles (mu equals 0.033, [Cl-] equals 0.033 M). An increase in the ionic strength is accompanied by a positive value of increment incrementpK. The results are consonant with the view that the observed increment incrementpK values reflect changes in the electrostatic potential at the binding site with consequently little, if any, effect on the intrinsic pK. The extension of the method to measure changes in the electrostatic potential at binding sites on cell membranes is briefly discussed.

Bromthymol Blue↗
PubMed1978

Electrostatic calculations for an ion channel. I. Energy and potential profiles and interactions between ions.

The electrostatic energy profile of one, two, or three ions in an aqueous channel through a lipid membrane is calculated. It is shown that the previous solution to this problem (based on the assumption that the channel is infinitely long) significantly overestimates the electrostatic energy barrier. For example, for a 3-A radius pore, the energy is 16 kT for the infinite channel and 6.7 kT for an ion in the center of a channel 25 A long. The energy as a function of the position of the ion is also determined. With this energy profile, the rate of crossing the membrane (using the Nernst-Planck equation) was estimated and found to be compatible with the maximum conductance observed for the gramicidin A channel. The total electrostatic energy (as a function of position) required to place two or three ions in the channel is also calculated. The electrostatic interaction is small for two ions at opposite ends of the channel and large for any positioning of the three ions. Finally, the gradient through the channel of an applied potential is calculated. The solution to these problems is based on solving an equivalent problem in which an appropriate surface charge is placed on the boundary between the lipid and aqueous regions. The magnitude of the surface charge is obtained from the numerical solution for a system of coupled integral equations.

Biological Transport↗
PubMed1979

Electrostatic stabilization in myoglobin. Interactive free energies between individual sites.

The pattern of electrostatic interactions between pairs of charge sites in sperm whale ferrimyoglobin was examined as a function of pH in terms of proton site occupancy, static solvent accessibility, and distance of separation. By grouping all examples of the most stabilizing interactions and all examples of the most destabilizing interactions, we can easily show that at pH 7.50 the former is much stronger; that is, the negative contributions to electrostatic free energy far outweigh the positive contributions. Much of the electrostatic energy of stabilization in native myoglobin is provided by specific charge-pair partners that are very highly conserved among 53 mammalian myoglobin species and is invariant substantially from pH 8.5 to 3.5. Destablizing interactions that become most significant, but not actually dominant, near the acid unfolding pH range can be recognized in emerging clusters of uncompensated positive charges. Binding of azide ion by the heme iron effectively reduces the most prominent destabilizing set of such interactions. In general, thoe charged residues that experience the largest summed stabilizing interactions with other groups are the most conserved between species. The histidine residues, however, show their best correlation of conservation with low values of static accessibility. Although histidine residue 64 has an effective pK corresponding to the midpoint of the unfolding transition near pH 4.2 at an ionic strength of 0.10 M and so might be called a "trigger group", its interactions contribute only a modest fraction of the overall pH-dependent free energy change. An examination of the primary stabilizing interactions represented by the charge-pair partners indicates a probably major role of electrostatic interactions in the nucleation and docking stages of the condensation of the polypeptide chain into the compact native structure.

Amino Acids↗
PubMed1977

[Investigations on the effect of an electrostatic field free of residual waves on the motility of the mouse (author's transl)].

Comparative investigations were carried out concerning the influence on the motility of mice of different electrobioclimatic conditions (electrostatic field with a residual wave component of 1% and a field strength of 4.500 V/m; pure residual wave component: 32 Vs/s, field strength 120 V/m/ss; electrostatic field established by batteries: initial voltage 900 V, field strength 4.500 V/m; shielded from ambient atmospheric electrical fields: damping efficiency at 99%). The Faraday condition represented the control as absolutely objective physical magnitude. All experimental chambers were positioned under Faraday shields. Following a 20 day period of acclimatization to the unaccustomed surroundings for the animals (adaptation period), we established the previously described electrophysical conditions in the cages for a further period of 20 days (experimental period). The lowest values measured during the daily readings were found in the Faraday cage, resp. in the pure electrostatic field, the highest in the DC-field with residual wave component resp. in the residual wave component alone. We draw the following conclusion from the findings: the pure DC-field apparently does not possess those bioclimatologically decisive importance that has been and is being postulated from several sides. Many of the stimtng effects observed and attributed to the electrostatic field are most probably due to the residual wave component resulting from the high-voltage generators employed.

Animals↗
PubMed1978

Electrostatic complexes of mitomycin C with nucleic acids and polyanions.

Reductively activated mitomycin C exhibits strong, non-covalent electrostatic binding to polyanions such as polyvinylsulfate and polyphosphate. The protonated C-2 amino group generated by the reduction is most likely responsible for this type of interaction. At moderate drug and salt concentrations only covalent binding to nucleic acids is observable. This is shown to be guanine-specific in DNA for the first time, as well as in synthetic polyribo- and polydeoxyribonucleotides at 10--20 times higher binding levels than previously tested. At higher mitomycin C concentration, however, strong non-covalent electrostatic binding to nucleic acids also occurs, resulting in a binding ratio up to 1 mol drug bound per mol mononucleotide, although this non-specific binding is relatively inhibited compared to polyvinylsulfate. Salts also have an inhibitory effect on the non-specific binding to nucleic acids. A series of mitomycin derivatives were compared for their binding and cross-linking abilities using DNA as substrate, with the following results: (a) the presence of a basic nitrogen . funtion at C-2 promotes binding, both covalent and electrostatic, presumably by kinetically facilitating the approach between positively charged nitrogen and DNA. (b) The aziridine ring is the major covalent binding site, indispensable for crosslinking and determines the guanine-specificity of the binding.

Anions↗
PubMed1975

Cation bindint to alpha-sl-casein B. A comparison of electrostatic models.

System characteristics which determine calcium binding to and subsequent proton release from alpha-sl-casein B are reported at pH 6.6 and [Na-plus] equal to 0.04, 0.0, and 0.16M. Values of protein solvation, G, site bound calcium, Ca,S, and net monomer charge, Z, permitted distributed charge models to be constructed. The models examined proved inadequate in that it was impossible to keep the dielectric constant, D, within acceptable limits and/or predict measured proton release. Three discrete charge models were constructed. At D equals 4, all three gave good agreement between predicted and experimental data as Ca, S increased. The known amino acid sequence was used to make rodlet models for the whole molecule andfor just the phosphate-containing acidic peptide portion. A comparison of these shows the electrostatic dominance of the acidic peptide and suggests that the electrostatic environment for the remainder of the binding sites is essentially constant as Ca, S increases during addition of calcium ion. The third discrete charge model bends the acidic peptide rodlet into a torus. In this case, data were matched with less assumed bond strain under conditions of high molecular charge than with the other two models. This indicates that conformation and association may be important factors to consider when constructing discrete charge models to calculate electrostatic free energy.

Amino Acid Sequence↗
PubMed1976

Electrostatic interactions at charged lipid membranes. I. Effects of pH and univalent cations on membrane structure.

Electrostatic interactions at charged lipid membranes make a significant contribution to the free energy of the system, and can be varied within a wide range by alteration either of the membrane's surface charge density or of the concentration of electrolytes in the surrounding medium. Changes in the charged membrane's structure, such as the ordered in equilibrium fluid phase transition, can thus be induced at constant temperature by variations in pH and salt concentration. An adequate quantitative description of these phenomena is obtained from the Gouy--Chapman theory. The good agreement between theory and experiment confirms that the expression derived for the electrostatic free energy especially in respect of its positive sign is correct. The classical expression derived for the electrostatic free energy, especially in respect of its positive sign, is correct. The classical expression for the "free energy of the double layer" derived by Verwey and Overbeek, which has a negative sign, is not applicable to lipid membranes with ionizable polar groups.

Cations, Monovalent↗
PubMed1979

Electrostatic effects in hemoglobin: Bohr effect and ionic strength dependence of individual groups.

The electrostatic treatment applied in the preceding paper in this issue [Matthew, J. B., Hanania, G.I.H., & Gurd, F.R.N. (1979) Biochemistry (preceding paper in this issue)] to the titration behavior of individual groups in human deoxyhemoglobin and oxyhemoglobin was applied to the computation of the alkaline Bohr effect at various values of ionic strength. The enhanced proton binding of deoxyhemoglobin in the pH range of 6--9 was accounted for at ionic strength 0.01 M by the effects of the unique charge distributions of ionizable groups in the two quaternary states. At ionic strength 0.10 M the effects of 2--4 bound anions had to be considered in addition in the deoxyhemoglobin charge configuration. At the higher ionic strength 10 groups per tetramer contributed to the Bohr effect, whereas 28 groups were contributory at the lower ionic strength. The ionic strength dependence of individual groups in the two tetrameric structures as well as in the alpha-chain monomer was explained in terms of the electrostatic treatment. This examination showed that the differences in electrostatic behavior of deoxy- and oxyhemoglobin follow from particular dissymmetries in their configurations with respect to charge and static solvent accessibility.

Electrochemistry↗
PubMed1978

Effect of electrostatic fields on the chromosomes of Ehrlich ascites tumor cells exposed in vivo.

An effect of electrostatic fields on the chromosomes of Ehrlich ascites tumor cells exposed in vivo has been demonstrated. Cells exposed to horizontal electrostatic fields for two weeks had almost a threefold increase in the percentage of abnormal chromosomes when compared to control cells or cells exposed to vertical electrostatic fields for the same period. Extended exposure times of 4--15 weeks resulted in the disappearance of the aberrant chromosomes. It is suggested that the effected cells were incapable of cellular replication resulting eventually in their disappearance via cell death.

Animals↗
PubMed1978

The acceleration of methanesulfonylation of acetylcholinesterase with cationic accelerators as an electrostatic effect.

1. In order to check our hypothesis of the electrostatic nature of the acceleration of methanesulfonylation of acetylcholinesterase (acetylcholine hydrolase, EC 3.1.1.7) with cationic accelerators, equations were solved for methane-sulfonylation with two accelerators and the reaction was studied in the presence of some single accelerators, including the sodium cation, and in the presence of two acclerators simultaneously. 2. The second-order rate constants for methanesulfonylation of the complexes between the enzyme and accelerators decamethonium, tetraethylammonium and tetramethylammonium are 90, 88 and 17 1 - mol-1 - s-1, respectively, which corresponds to a maximal acceleration of 29, 28 and 5.5 times, respectively. The dissociation constants for the binding of these accelerators to the enzyme, obtained from our acceleration experiments, are 3.7 - 10(-6), 3.2 - 10(-4) and 1.4 - 10(-3) M, respectively. These values are in good agreement with the dissociation constants of these ligands as inhibitors of acetylcholinesterase. It is interesting to note that the sodium cation also accelerates the methane-sulfonylation up to around three times, the corresponding second-order rate constant and the dissociation constant being 10 1 - mol-1 - s-1 and 1.3 M, respectively. 3. All tested cations compete in the acceleration with each other; they seem to accelerate the reaction in the same way and from the same site, the catalytic anionic site. 4. These findings confirm the hypothesis of the electrostatic nature of acceleration.

Acetylcholinesterase↗
PubMed1978

The influence of electrostatic and magnetic fields on mutation in Drosophila melanogaster spermatozoa.

Canton-S Drosophila melanogaster males were exposed to electrostatic and magnetic fields for 24 h to determine the influence of low energy fields on the production of sex-linked recessive lethal mutations in the mature, motile sperm. To detect sex-linked recessive lethal production in mature sperm the standard Muller-5 test was done. Exposure of the males to the magnetic field or the electrostatic field did not significantly affect the mutation frequency in mature sperm.

Animals↗
PubMed1976

Electrostatic free energy and shift of the phase transition for charged lipid membranes.

For a charged membrane in an electrolyte solution the electrostatic free energy is derived treating the system as a diffuse double layer. The dependence of the energy on external parameters like surface charge density and temperature is obtained and the physical basis discussed. As an application the charges are shown to exert an electrostatic surface pressure on the lipid chain packing which leads to a shift in the phase transition of membranes. The results confirm the interpretation of experimental data as given by Träuble et al. in the accompanying paper.

Lipids↗
PubMed1979

Electrostatic effects in hemoglobin: hydrogen ion equilibria in human deoxy- and oxyhemoglobin A.

The modified Tanford-Kirkwood theory of Shire et al. [Shire, S. J., Hanania, G.I.H., & Gurd, F.R.N. (1974) Biochemistry 13, 2967] for electrostatic interactions was applied to the hydrogen ion equilibria of human deoxyhemoglobin and oxyhemoglobin. Atomic coordinates for oxyhemoglobin were generated by the application of the appropriate rigid rotation function to alpha and beta chains of the deoxyhemoglobin structure [Fermi, G. (1975) J. Mol. Biol. 97, 237]. The model employs two sets of parameters derived from the crystalline protein structures, the atomic coordinates of charged amino acid residues and static solvent accessibility factors to reflect their individual degrees of exposure to solvent. Theoretical titration curves based on a consistent set of pKint values compared closely with experimental potentiometric curves. Theoretical pK values at half-titration for individual protein sites corresponded to available observed values for both quaternary states. The results bring out the cumulative effects of numerous electrostatic interactions in the tetrameric structures and the major effects of the quaternary transition that result from changes in static solvent accessibility of certain ionizable groups.

Amino Acids↗
PubMed1977

Duplex formation of a nonionic oligo(deoxythymidylate) analogue (heptadeoxythymidylyl-(3'-5')-deoxythymidine heptaethyl ester (d-(Tp(Et))7T)) with poly(deoxyadenylate). Evaluation of the electrostatic interaction.

The heptaethyl ester of heptadeoxythymidylyl-(3'-5')-deoxythymidine (d-[Tp(Et)]7T or d-T8-Et) has been prepared by chemical methods. The material, consisting of a mixture of diastereoisomers, forms a 1:1 complex with (dA)n in neutral aqueous buffer; this interaction is virtually independent of ionic strength. The octamer triester does not bind to (dA)n-(dT)n, and it interacts with (rA)n only at low temperatures. By cochromatography with (dA)n on Sephadex G-50, d-T8-Et fractions with different binding affinities for the polyadenylates were obtained. This heterogeneity in binding affinity is ascribed to the diastereoisomerism of d-T8-Et. Enthalpies of dupoex formation were determined by the concentration variation method. At 0.1 M sodium ion concentration, the enthalpy of binding of the various d-T8-Et fractions to (dA)n is essentially invariant (-8.1 kcal/mol of base pairs at 0 degrees C to -8.6 kcal at 25 degrees C) and 1.6 kcal/mol of base pairs more negative than the enthalpy of binding of the phosphodiester analogue, d-(Tp)7T, to (dA)n (-6.8 kcal/mol of base pairs at 11 degrees C). This difference is the electrostatic contribution to the enthalpy of duplex formation, arising from the interstrand electrostatic repulsion and the intrastrand repulsion in d-(Tp)7T. The entropy of binding to (dA)n is more negative for the octamer triesters than for the diester analogue, and is different for the various d-T8-Et fractions. This is interpreted in terms of varying degrees of restriction of rotational freedom for the ethyl substituents upon double helix formation.

Chromatography, Gel↗