Soluble amyloid beta-oligomers affect dielectric membrane properties by bilayer insertion and domain formation: implications for cell toxicity

It is well established that Alzheimer's amyloid beta-peptides reduce the membrane barrier to ion transport. The prevailing model ascribes the resulting interference with ion homeostasis to the formation of peptide pores across the bilayer. In this work, we examine the interaction of soluble prefibrillar amyloid beta (Abeta(1-42))-oligomers with bilayer models, observing also dramatic increases in ion current at micromolar peptide concentrations. We demonstrate that the Abeta-induced ion conductances across free-standing membranes and across substrate-supported "tethered" bilayers are quantitatively similar and depend on membrane composition. However, characteristic signatures of the molecular transport mechanism were distinctly different from ion transfer through water-filled pores, as shown by a quantitative comparison of the membrane response to Abeta-oligomers and to the bacterial toxin alpha-hemolysin. Neutron reflection from tethered membranes showed that Abeta-oligomers insert into the bilayer, affecting both membrane leaflets. By measuring the capacitance of peptide-free membranes, as well as their geometrical thicknesses, the dielectric constants in the aliphatic cores of 1,2-dioleoyl-sn-glycero-3-phosphocholine and 1,2-diphytanoyl-sn-glycero-3-phosphocholine bilayers were determined to be epsilon = 2.8 and 2.2, respectively. The magnitude of the Abeta-induced increase in epsilon indicates that Abeta-oligomers affect membranes by inducing lateral heterogeneity in the bilayers, but an increase in the water content of the bilayers was not observed. The activation energy for Abeta-induced ion transport across the membrane is at least three times higher than that measured for membranes reconstituted with alpha-hemolysin pores, E(a) = 36.8 vs. 9.9 kJ/mol, indicating that the molecular mechanisms underlying both transport processes are fundamentally different. The Abeta-induced membrane conductance shows a nonlinear dependence on the peptide concentration in the membrane. Moreover, E(a) depends on peptide concentration. These observations suggest that cooperativity and/or conformational changes of the Abeta-oligomer particles upon transfer from the aqueous to the hydrocarbon environment play a prominent role in the interaction of the peptide with the membrane. A model in which Abeta-oligomers insert into the hydrophobic core of the membrane-where they lead to a local increase in epsilon and a concomitant reduction of the membrane barrier-describes the experimental data quantitatively.     

Peptide binding to lipid bilayers. Nonclassical hydrophobic effect and membrane-induced pK shifts.

The binding of the cyclic peptide (+)-D-Phe1-Cys2-Phe3-D-Trp4-(+)-Lys5-Thr6- Cys7-Thr(ol)8, a somatostatin analogue (SMS 201-995), and the potential-sensitive dye 2-(p-toluidinyl)naphthalene-6-sulfonate (TNS) to lipid membranes was investigated with high-sensitivity titration calorimetry. The binding enthalpy of the peptide was found to vary dramatically with the vesicle size. For highly curved vesicles with a diameter of d congruent to 30 nm, the binding reaction was enthalpy-driven with delta H congruent to -7.0 +/- 0.3 kcal/mol; for large vesicles with more tightly packed lipids, the binding reaction became endothermic with delta H congruent to +1.0 +/- 0.3 kcal/mol and was entropy-driven. In contrast, the free energy of binding was almost independent of the vesicle size. The thermodynamic analysis suggests that the observed enthalpy-entropy compensation of about 8 kcal/mol can be related to a change in the internal tension of the bilayer and is brought about by an entropy increase of the lipid matrix. The "entropy potential" of the membrane may have its molecular origin in the excitation of the hydrocarbon chains to a more disordered configuration and may play a more important role in membrane partition equilibria than the classical hydrophobic effect. The binding of the peptide to the membrane surface induced a pK shift of the peptide terminal amino group. Neutral membranes were found to destabilize the NH3+ group, leading to a decrease in pK; negatively charged membranes, generated an apparent increase in pK due to the increase in proton concentration near the membrane surface. No pK shifts were seen for TNS. Titration calorimetry combined with the Gouy-Chapman theory can be used to determine both the reaction enthalpy and the binding constant of the membrane-binding equilibrium.     

Interaction of carbonylcyanide <Emphasis Type="Italic">p</Emphasis>-trifluoromethoxyphenylhydrazone (FCCP) with lipid membrane systems: a biophysical approach with relevance to mitochondrial uncoupling

FCCP (carbonylcyanide p-trifluoromethoxyphenylhydrazone), a classical uncoupler of mitochondrial oxidative phosphorylation, is used in this study as a model to clarify how interactions of uncouplers with membrane lipid bilayers may influence membrane biophysics and their protonophoric activity itself. In order to disclose putative effects that may be important when considering using uncouplers for pharmacological purposes, an extensive characterization of FCCP membrane lipid interactions using accurate biophysical approaches and simple model lipid systems was carried out. Differential scanning calorimetry studies showed that FCCP molecules disturb lipid bilayers and favor lateral phase separation in mixed lipid systems. ³¹P NMR assays indicated that FCCP alters the curvature elastic properties of membrane models containing non-bilayer lipids, favoring lamellar/H_II transition, probably by alleviation of hydrocarbon-packing constraints in the inverted hexagonal phase. Taking advantage of FCCP quenching effects on the fluorescent probes DPH (1,6-diphenyl-1,3,5-hexatriene) and DPH-PA (3-(p-(6-phenyl)-1,3,5-hexatrienyl)phenylpropionic acid), it is demonstrated that FCCP distributes across the bilayer thickness in both a single and a ternary lipid system mimicking the inner mitochondrial membrane. This behavior is consistent with the ability of the compound to migrate through the thickness of the inner mitochondrial membrane, an event required for its protonophoric activity. Finally, the study of the membrane fluidity in different lipid systems, as reported by the rotational correlation time (θ) of DPH or DPH-PA, showed that the extension at which FCCP disturbs membrane properties associated with the dynamics and the order of lipid molecules depends on the lipid composition of the model lipid system assayed.     

Supported phospholipid/alkanethiol biomimetic membranes: insulating properties.

A novel model lipid bilayer membrane is prepared by the addition of phospholipid vesicles to alkanethiol monolayers on gold. This supported hybrid bilayer membrane is rugged, easily and reproducibly prepared in the absence of organic solvent, and is stable for very long periods of time. We have characterized the insulating characteristics of this membrane by examining the rate of electron transfer and by impedance spectroscopy. Supported hybrid bilayers formed from phospholipids and alkanethiols are pinhole-free and demonstrate measured values of conductivity and resistivity which are within an order of magnitude of that reported for black lipid membranes. Capacitance values suggest a dielectric constant of 2.7 for phospholipid membranes in the absence of organic solvent. The protein toxin, melittin, destroys the insulating capability of the phospholipid layer without significantly altering the bilayer structure. This model membrane will allow the assessment of the effect of lipid membrane perturbants on the insulating properties of natural lipid membranes.     

Effect of carbonylcyanide-4-(trifluoromethoxy)phenylhydrazone (FCCP) on the interaction of 1-anilino-8-naphthalene sulfonate (ANS) with phosphatidylcholine liposomes

The weak hydrophobic acid carbonylcyanide-4-(trifluoromethoxy)phenylhydrazone (FCCP) is a protonophoric uncoupler of oxidative phosphorylation in mitochondria. It dissipates the electrochemical proton gradient (Δμ_H ⁺) increasing the mitochondrial oxygen consumption. However, at concentrations higher than 1 μM it exhibits additional effects on mitochondrial energy metabolism, which were tentatively related to modifications of electrical properties of the membrane. Here we describe the effect of FCCP on the binding of 1-anilino-8-naphthalene sulfonate (ANS) to 1, 2-dioleoyl-sn-glycero-3-phosphocholine (DOPC) and 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) unilamellar vesicles. FCCP inhibited the binding of ANS to liposomes either in the gel or in the liquid crystalline phase, by increasing the apparent dissociation constant of ANS. Smaller effect on the dissociation constant was observed at high ionic strength, suggesting that the effect of FCCP is through modification of the electrostatic properties of the membrane interface. In addition, FCCP also decreased (approximately 50 %) the quantum yield and increased the intrinsic dissociation constant of membrane-bound ANS, results that suggest that FCCP makes the environment of the ANS binding sites more polar. On those grounds we postulate that the binding of FCCP: i) increases the density of negative charges in the membrane surface; and ii) distorts the phospholipid bilayer, increasing the mobility of the polar headgroups making the ANS binding site more accessible to water.     

Dehydration of model membranes induced by lectins from Ricinus communis and Viscum album.

The effects of ribosome-inactivating proteins (RIPs) from Ricinus communis and from Viscum album on the water permeability, Pf, and the surface dielectric constant, epsilon, of model membranes were studied. Pf was calculated from microelectrode measurements of the ion concentration distribution in the immediate vicinity of a planar membrane, and epsilon was obtained from the fluorescence of dansyl phosphatidylethanolamine incorporated into unilamellar vesicles. Pf and epsilon of fully saturated phosphatidylcholine membranes were affected only in the presence of a lectin receptor (monosialoganglioside, GM1) in the bilayer. It is suggested that the membrane area occupied by clustered lectin-receptor complexes is markedly less permeable to water. Protein binding to the receptor was not a prelude for hydrophobic lipid-protein interactions when the membranes were formed from a mixture of natural phospholipids with a high content of unsaturated fatty acids. These membranes, characterized by a high initial water permeability, were found to interact with the RIPs unspecifically. From a decrease of both Pf and epsilon it was concluded that not only water partitioning but also protein adsorption correlates with looser packing of polyunsaturated lipids at the lipid-water interface.     

The epsilon subunit of Escherichia coli coupling factor 1 is required for its binding to the cytoplasmic membrane.

The coupling factor, F1-ATPase of Escherichia coli (ECF1) contains five different subunits, alpha, beta, gamma, delta, and epsilon. Properties of delta-deficient ECF1 have previously been described. F1-ATPase containing only the alpha, beta, and gamma subunits was prepared from E. coli by passage of delta-deficient ECF1 through an affinity column containing immobilized antibodies to the epsilon subunit. The delta, epsilon-deficient enzyme has normal ATPase activity but cannot bind to ECF1-depleted membrane vesicles. Both the delta and epsilon subunits are required for the binding of delta, epsilon-deficient ECF1 to membranes and the restoration of oxidative phosphorylation. Either delta or epsilon will bind to the deficient enzyme to form a four-subunit complex. Neither four-subunit enzyme binds to depleted membranes. The epsilon subunit, does, however, slightly improve the binding affinity between delta and delta-deficient enzyme suggesting a possible interaction between the two subunits. Neither subunit binds to trypsin-treated ECF1, which contains only the alpha and beta subunits. A role for gamma in the binding of epsilon to F1 is suggested. epsilon does not bind to ECF1-depleted membranes. Therefore, the in vitro reconstitution of depleted membranes requires an initial complex formation between epsilon and the rest of ECF1 prior to membrane attachment. Reconstitution experiments indicate that only one epsilon is required per functional ECF1 molecule.     

Uncoupler antagonism of valinomycin induced bilayer membrane conductance

We have found that an uncoupler of oxidative phosphorylation, tetrachloro-2-trifluoromethylbenzimidazole (TTFB), can block valinomycin induced potassium ion, (K⁺), conductance through bilayer membranes. Blocking is most pronounced at high K⁺ concentration, (≥ 0.1 M), and at a pH greater than the pK of TTFB. A blocking mechanism involving competition for membrane sites, together with association of oppositely charged species within the membrane, is proposed.     

Carboxyatractylate inhibits the uncoupling effect of free fatty acids

The ATP/ADP-antiporter inhibitors and ADP decrease the palmitate-induced stimulation of the mitochondrial respiration in the controlled state. The degree of inhibition decreases in the order: carboxyatractylate greater than bongkrekic acid, palmitoyl-CoA, ADP greater than atractylate. GDP is ineffective. The inhibiting concentration of carboxyatractylate coincides with this arresting the state 3 respiration. Carboxyatractylate inhibition decreases when the palmitate concentration increases. Stimulation of controlled respiration by FCCP or gramicidin D at any concentration of these uncouplers is carboxyatractylate-resistant, whereas that by low concentrations of DNP is partially suppressed by carboxyatractylate. These data together with observations that palmitate does not increase H+ conductance in bilayer phospholipid membranes and in cytochrome oxidase-asolectin proteoliposomes indicate that the ATP/ADP-antiporter is somehow involved in the uncoupling by low concentrations of fatty acids (or DNP), whereas that by FCCP and gramicidin D is due to their effect on the phospholipid bilayer. It is suggested that the antiporter facilitates translocation of palmitate anion across the mitochondrial membrane.     

A study of the inhomogeneity of bilayer lipid membranes by measurements of higher harmonics of transmembrane current

Higher harmonics of alternating current in bilayer lipid membranes caused by sinusoidal voltage applied to the membrane were measured. The bilayer lipid membranes were prepared from diphytanoylphosphatidylcholine in n-decane and n-tetradecane, and measurements were conducted with the aid of an analog-to-digital converter of 16th category. Sinusoidal voltage was formed using a digital-to-analog converter of the 16th category. The dynamic region of measurements was up 90 dB. The results of measurements were used to determine the alpha and beta coefficients of the expansion of membrane capacity C in terms of membrane voltage U C = C0 (1 + alphaU2 + betaU4). We showed in the framework of the electrostriction model that the relation between the alpha and beta coefficients characterizes the inhomogeneity of bilayer lipid membrane with respect to its thickness and Young modulus of elasticity.     

The redox properties of cytochromes b imposed by the membrane electrostatic environment.

The effect of the dipole potential field of extended membrane spanning alpha-helices on the redox potentials of b cytochromes in energy transducing membranes has been calculated in the context of a three phase model for the membrane. In this model, the membrane contains three dielectric layers; (i) a 40-A hydrophobic membrane bilayer, with dielectric constant em = 3-4, (ii) 10-20-A interfacial layers of intermediate polarity, ein = 12-20, that consist of lipid polar head groups and peripheral protein segments, and (iii) an external infinite water medium, ew = 80. The unusually positive midpoint potential, Em = +0.4 V, of the "high potential" cytochrome b-559 of oxygenic photosynthetic membranes, a previously enigmatic property of this cytochrome, can be explained by (i) the position of the heme in the positive dipole potential region near the NH2 termini of the two parallel helices that provide its histidine ligands, and (ii) the loss of solvation energy of the heme ion due to the low dielectric constant of its surroundings, leading to an estimate of +0.31 to +0.37 V for the cytochrome Em. The known tendency of this cytochrome to undergo a large -delta Em shift upon exposure of thylakoid membranes to proteases or damaging treatments is explained by disruption of the intermediate polarity (ein) surface dielectric layer and the resulting contact of the heme with the external water medium. Application of this model to the two hemes (bn and bp) of cytochrome b of the cytochrome bc1 complex, with the two hemes placed symmetrically in the low dielectric (em) membrane bilayer, results in Em values of hemes bn and bp that are, respectively, somewhat too negative (approximately -0.1 V), and much too positive (approximately +0.3 V), leading to a potential difference, Em(bp) - Em(bn), with the wrong sign and magnitude, +0.25 V instead of -0.10 to -0.15 V. The heme potentials can only be approximately reconciled with experiment, if it is assumed that the two hemes are in different dielectric environments, with that of heme bp being more polar.     

Lipid distribution and transport across cellular membranes

In eukaryotic cells, the membranes of different intracellular organelles have different lipid composition, and various biomembranes show an asymmetric distribution of lipid types across the membrane bilayer. Membrane lipid organization reflects a dynamic equilibrium of lipids moving across the bilayer in both directions. In this review, we summarize data supporting the role of specific membrane proteins in catalyzing transbilayer lipid movement, thereby controlling and regulating the distribution of lipids over the leaflets of biomembranes.     

Incorporation of surface tension into molecular dynamics simulation of an interface: a fluid phase lipid bilayer membrane.

In this paper we report on the molecular dynamics simulation of a fluid phase hydrated dimyristoylphosphatidylcholine bilayer. The initial configuration of the lipid was the x-ray crystal structure. A distinctive feature of this simulation is that, upon heating the system, the fluid phase emerged from parameters, initial conditions, and boundary conditions determined independently of the collective properties of the fluid phase. The initial conditions did not include chain disorder characteristic of the fluid phase. The partial charges on the lipids were determined by ab initio self-consistent field calculations and required no adjustment to produce a fluid phase. The boundary conditions were constant pressure and temperature. Thus the membrane was not explicitly required to assume an area/phospholipid molecule thought to be characteristic of the fluid phase, as is the case in constant volume simulations. Normal to the membrane plane, the pressure was 1 atmosphere, corresponding to the normal laboratory situation. Parallel to the membrane plane a negative pressure of -100 atmospheres was applied, derived from the measured surface tension of a monolayer at an air-water interface. The measured features of the computed membrane are generally in close agreement with experiment. Our results confirm the concept that, for appropriately matched temperature and surface pressure, a monolayer is a close approximation to one-half of a bilayer. Our results suggest that the surface area per phospholipid molecule for fluid phosphatidylcholine bilayer membranes is smaller than has generally been assumed in computational studies at constant volume. Our results confirm that the basis of the measured dipole potential is primarily water orientations and also suggest the presence of potential barriers for the movement of positive charges across the water-headgroup interfacial region of the phospholipid.     

Evaluation of the thickness of lipid bilayers of biological membranes by measurement of specific capacity

The estimate of the thickness of the hydrophobic part of biological membranes by means of its formula for plane capacitor leads to a necessity of very high values of protein dielectric permeability. The current estimate can be performed if the membrane possesses a wavy cross-section. Due to the existence of integral proteins which occupy about 1/3 of the bilayer surface and have dielectric permeability epsilon = 6 divided by 8 and also due to some peculiarities of intermembrane electric field the thickness of hydrophobic bilayer region can be estimated from membrane specific capacity as 3 divided by 3.5 nm, this value coincides with X-ray data.     

pH-induced conformational changes of the Fe(2+)-N epsilon (His F8) linkage in deoxyhemoglobin trout IV detected by the Raman active Fe(2+)-N epsilon (His F8) stretching mode.

To investigate heme-protein coupling via the Fe(2+)-N epsilon (His F8) linkage we have measured the profile of the Raman band due to the Fe(2+)-N epsilon (His F8) stretching mode (nu Fe-His) of deoxyHb-trout IV and deoxyHbA at various pH between 6.0 and 9.0. Our data establish that the band of this mode is composed of five different sublines. In deoxyHb-trout IV, three of these sublines were assigned to distinct conformations of the alpha-subunit (omega alpha 1 = 202 cm-1, omega alpha 2 = 211 cm-1, omega alpha 3 = 217 cm-1) and the other two to distinct conformations of the beta-subunit (omega beta 1 = 223 cm-1 and omega beta 2 = 228 cm-1). Human deoxyHbA exhibits two alpha-chain sublines at omega alpha 1 = 203 cm-1, omega alpha 2 = 212 cm-1 and two beta-chain sublines at omega beta 1 = 217 cm-1 and omega beta 2 = 225 cm-1. These results reveal that each subunit exists in different conformations. The intensities of the nu Fe-His sublines in deoxyHb-trout IV exhibit a significant pH dependence, whereas the intensities of the corresponding sublines in the deoxyHbA spectrum are independent on pH. This finding suggests that the structural basis of the Bohr effect is different in deoxyHbA and deoxyHb-trout IV. To analyse the pH dependence of the deoxyHb-trout IV sublines we have applied a titration model describing the intensity of each nu Fe-His subline as an incoherent superposition of the intensities from sub-sublines with the same frequency but differing intrinsic intensities due to the different protonation states of the respective subunit. The molar fractions of these protonation states are determined by the corresponding Bohr groups (i.e., pK alpha 1 = pK alpha 2 = 8.5, pK beta 1 = 7.5, pK beta 2 = 7.4) and pH. Hence, the intensities of these sublines reflect the pH dependence of the molar fractions of the involved protonation states. Fitting this model to the pH-dependent line intensities yields a good reproduction of the experimental data.(ABSTRACT TRUNCATED AT 400 WORDS)     

The kinetic mechanism of action of an uncoupler of oxidative phosphorylation.

The chemiosmotic hypothesis predicts that the mechanism by which weak acids uncouple oxidative phosphorylation in mitochondria is identical to the mechanism by which they transport hydrogen ions across artificial bilayer membranes. We report here the results of a kinetic study of uncoupler-mediated hydrogen ion transport across bilayer membranes. We made electrical relaxation measurements on black lipid membranes exposed to the substituted benzimidazole 5,6-dichloro-2-trifluoromethylbenzimidazole. The simplest model consistent with our experimental data allowed us to deduce values for adsorption coefficients and rate constants. Our major conclusions are that the back diffusion of the neutral species is the rate limiting step for the steady state transport of hydrogen ions, that both the neutral and charged forms of the uncoupler adsorb strongly to the interfaces, and that the reactions at the membrane-solution interfaces occur sufficiently rapidly for equilibrium to be maintained. Independent measurements of the adsorption coefficients of both the neutral and anionic forms of the weak acid and also of the permeability of the membrane to the neutral form agreed well with the values deduced from the kinetic study.     

Transport of fatty acids across membranes by the diffusion mechanism

In early research on fatty acid transport, passive diffusion seemed to provide an adequate explanation for movement of fatty acids through the membrane bilayer. This simple hypothesis was later challenged by the discovery of several proteins that appeared to be membrane-related fatty acid transporters. In addition, some biophysical studies suggested that fatty acids moved slowly through the simple model membranes (phospholipid bilayers), which would provide a rationale for protein-assisted transport. Furthermore, it was difficult to rationalize how fatty acids could diffuse passively across the bilayer as anions. Newer studies have shown that fatty acids are present in membranes in the un-ionized as well as the ionized form, and that the un-ionized form can cross a protein-free phospholipid bilayer quickly. This flip-flop mechanism has been validated in cells by intracellular pH measurements. The role of putative fatty acid transport proteins remains to be clarified.     

Reversible electrical breakdown of lipid bilayer membranes: A charge-pulse relaxation study

Summary Charge-pulse experiments were performed with lipid bilayer membranes from oxidized cholesterol/n-decane at relatively high voltages (several hundred mV). The membranes show an irreversible mechanical rupture if the membrane is charged to voltages on the order of 300 mV. In the case of the mechanical rupture, the voltage across the membrane needs about 50–200 sec to decay completely to zero. At much higher voltages, applied to the membrane by charge pulses of about 500 nsec duration, a decrease of the specific resistance of the membranes by nine orders of magnitude is observed (from 10⁸ to 0.1 cm²), which is correlated with the reversible electrical breakdown of the lipid bilayer membrane. Due to the high conductance increase (breakdown) of the bilayer it is not possible to charge the membrane to a larger value than the critical potential differenceV _c. For 1m alkali ion chloridesV _c was about 1 V. The temperature dependence of the electrical breakdown voltageV _c is comparable to that being observed with cell membranes.V _c decreases between 2 and 48°C from 1.5 to 0.6 V in the presence of 1m KCl.Breakdown experiments were also performed with lipid bilayer membranes composed of other lipids. The fast decay of the voltage (current) in the 100-nsec range after application of a charge pulse was very similar in these experiments compared with experiments with membranes made from oxidized cholesterol. However, the membranes made from other lipids show a mechanical breakdown after the electrical breakdown, whereas with one single membrane from oxidized cholesterol more than twenty reproducible breakdown experiments could be repeated without a visible disturbance of the membrane stability.The reversible electrical breakdown of the membrane is discussed in terms of both compression of the membrane (electromechanical model) and ion movement through the membrane induced by high electric field strength (Born energy).     

Density functional theory calculations on the dielectric constant dependence of the oxidation potential of chlorophyll: implication for the high potential of P680 in photosystem II

The primary donor chlorophyll (Chl) of photosystem II (PSII), P680, has an extremely high oxidation redox potential (E(ox)) of approximately 1.2 V, which is essential for photosynthetic water oxidation. The mechanism for achieving a high potential such as that of P680 has been one of the central questions in photosynthesis research. Here, we have examined the dielectric constant (epsilon) dependence of the E(ox) of monomer Chl using density functional theory calculations with the polarizable continuum model. The calculated E(ox) of a model Chl compound exhibited a sharp increase with a decrease in epsilon in the relatively low epsilon region (epsilon < 5). In contrast, in the higher-epsilon region, E(ox) was rather insensitive to epsilon and converged to a constant value at very high epsilon values. This tendency in the high-epsilon region explains the experimental E(ox) values of isolated Chl a that have been observed in a relatively narrow range of 0.74-0.93 V. The E(ox) of Chl in an ideal hydrophobic protein was estimated to be approximately 1.4 V at an epsilon value of 2. This value indicates that Chl in a hydrophobic environment originally has a high E(ox) that is sufficient for oxidizing water (E(ox) = 0.88 V at pH 6). On the basis of the reported X-ray crystallographic structures, the protein environment of P680 in PSII was estimated to be more hydrophobic than that of the primary donors in bacterial reaction centers. It is therefore suggested that the low-dielectric environment around P680 is one of the major factors in its very high E(ox), and thus, introducing nonpolar amino acids into the binding pocket of P680 was an important process in the evolution of PSII.     

The kinetic mechanism of action of an uncoupler of oxidative phosphorylation

Summary The chemiosmotic hypothesis predicts that the mechanism by which weak acids uncouple oxidative phosphorylation in mitochondria is identical to the mechanism by which they transport hydrogen ions across artificial bilayer membranes. We report here the results of a kinetic study of uncoupler-mediated hydrogen ion transport across bilayer membranes. We made electrical relaxation measurements on black lipid membranes exposed to the substituted benzimidazole 5,6-dichloro-2-trifluoromethylbenzimidazole. The simplest model consistent with our experimental data allowed us to deduce values for adsorption coefficients and rate constants. Our major conclusions are that the back diffusion of the neutral species is the rate limiting step for the steady state transport of hydrogen ions, that both the neutral and charged forms of the uncoupler adsorb strongly to the interfaces, and that the reactions at the membrane-solution interfaces occur sufficiently rapidly for equilibrium to be maintained. Independent measurements of the adsorption coefficients of both the neutral and anionic forms of the weak acid and also of the permeability of the membrane to the neutral form agreed well with the values deduced from the kinetic study.