The role of surface charge on the accelerating action of heparin on the antithrombin III-inhibited activity of alpha-thrombin

We have compared surface charge and the surface charge density on the polyanions heparin and potassium polyvinyl sulfate (KPVS), as well as on hydrolyzed heparin and KPVS, with their accelerating effect on the inhibitory action of antithrombin III on thrombin. Polyelectrolyte titration of thrombin with KPVS or heparin at pH 7.4 clearly indicates an electrostatic interaction. In contrast, at the same pH no electrostatic interaction is observed between polyanions and antithrombin III. KPVS accelerates the inhibitory action of antithrombin III to the same extent as heparin on the basis of charge equivalence. Heparin and KPVS with a mean distance between two charged centers of less than 0.75 and 0.95 nm, respectively, accelerate strongly whereas hydrolysates with lower charge densities are far less active. The following observations are indicated. Intramolecular neutralization of oppositely charged residues occurs within thrombin, antithrombin III, and partially hydrolyzed heparin. Heparin acts on the antithrombin III-thrombin reaction through cooperative electrostatic binding to thrombin and nonelectrostatic interaction with antithrombin III. This indicates a quasi-catalytic action of the polyelectrolyte. Hydrolysis of only a few N-sulfate residues within the heparin molecule decreases the linear surface charge density to such an extent that the accelerating action is drastically reduced. The loss of accelerating capacity agrees with the sudden loss of counterion condensation due to the decrease of the linear surface charge density beyond limits postulated by Manning in a theory of polyelectrolytes.     

Electrostatic modulation in steroid receptor recruitment of LXXLL and FXXLF motifs

Coactivator recruitment by activation function 2 (AF2) in the steroid receptor ligand binding domain takes place through binding of an LXXLL amphipathic alpha-helical motif at the AF2 hydrophobic surface. The androgen receptor (AR) and certain AR coregulators are distinguished by an FXXLF motif that interacts selectively with the AR AF2 site. Here we show that LXXLL and FXXLF motif interactions with steroid receptors are modulated by oppositely charged residues flanking the motifs and charge clusters bordering AF2 in the ligand binding domain. An increased number of charged residues flanking AF2 in the ligand binding domain complement the two previously characterized charge clamp residues in coactivator recruitment. The data suggest a model whereby coactivator recruitment to the receptor AF2 surface is initiated by complementary charge interactions that reflect a reversal of the acidic activation domain-coactivator interaction model.     

Surface charge distribution on the endothelial cell of liver sinusoids

The topography of the charged residues on the endothelial cell surface of liver sinusoid capillaries was investigated by using electron microscopic tracers of different size and charge. The tracers used were native ferritin (pl 4.2-4.7) and its cationized (pl 8.4) and anionized (pl 3.7) derivatives, BSA coupled to colloidal gold (pl of the complex 5.1), hemeundecapeptide (pl 4.85), and alcian blue (pl greater than 10). The tracers were either injected in vivo or perfused in situ through the portal vein of the mouse liver. In some experiments, two tracers of opposite charge were sequentially perfused with extensive washing in between. The liver was processed for electron microscopy and the binding pattern of the injected markers was recorded. The electrostatic nature of the tracer binding was assessed by perfusion with high ionic strength solutions, by aldehyde quenching of the plasma membrane basic residues, and by substituting the cell surface acidic moieties with positively charged groups. Results indicate that the endothelial cells of the liver sinusoids expose on their surface both cationic and anionic residues. The density distribution of these charged groups on the cell surface is different. While the negative charge is randomly and patchily scattered all over the membrane, the cationic residues seem to be accumulated in coated pits. The charged groups co-exist in the same coated pit and bind the opposite charged macromolecule. It appears that the fixed positive and negative charges of the coated pit glycocalyx are mainly segregated in space. The layer of basic residues is located at 20-30-nm distance of the membrane, while most of the negative charges lie close to the external leaflet of the plasmalemma.     

Lipid demixing and protein-protein interactions in the adsorption of charged proteins on mixed membranes

The adsorption free energy of charged proteins on mixed membranes, containing varying amounts of (oppositely) charged lipids, is calculated based on a mean-field free energy expression that accounts explicitly for the ability of the lipids to demix locally, and for lateral interactions between the adsorbed proteins. Minimization of this free energy functional yields the familiar nonlinear Poisson-Boltzmann equation and the boundary condition at the membrane surface that allows for lipid charge rearrangement. These two self-consistent equations are solved simultaneously. The proteins are modeled as uniformly charged spheres and the (bare) membrane as an ideal two-dimensional binary mixture of charged and neutral lipids. Substantial variations in the lipid charge density profiles are found when highly charged proteins adsorb on weakly charged membranes; the lipids, at a certain demixing entropy penalty, adjust their concentration in the vicinity of the adsorbed protein to achieve optimal charge matching. Lateral repulsive interactions between the adsorbed proteins affect the lipid modulation profile and, at high densities, result in substantial lowering of the binding energy. Adsorption isotherms demonstrating the importance of lipid mobility and protein-protein interactions are calculated using an adsorption equation with a coverage-dependent binding constant. Typically, at bulk-surface equilibrium (i.e., when the membrane surface is "saturated" by adsorbed proteins), the membrane charges are "overcompensated" by the protein charges, because only about half of the protein charges (those on the hemispheres facing the membrane) are involved in charge neutralization. Finally, it is argued that the formation of lipid-protein domains may be enhanced by electrostatic adsorption of proteins, but its origin (e.g., elastic deformations associated with lipid demixing) is not purely electrostatic.     

In vitro kinetic analysis of the role of the positive charge at the amino-terminal region of signal peptides in translocation of secretory protein across the cytoplasmic membrane in Escherichia coli

By using an in vitro system for the translocation of secretory proteins in Escherichia coli, detailed and quantitative studies were performed as to the function of the positively charged amino acid residues at the amino terminus of the signal peptide. Uncleavable OmpF-Lpp, a model secretory protein carrying an uncleavable signal peptide, and mutant proteins derived from it were used as translocation substrates. When the positive charge, +2 (LysArg) for the wild-type, was changed to 0, -1, or -2, little or no translocation was observed. The number of the positive charge was altered by introducing different numbers of Lys or Arg residues into the amino terminus. The rate of translocation was roughly proportional to this number, irrespective of whether the charged amino acid residues were Lys or Arg. When the amino-terminal LysArg was replaced by His residues, translocation took place more efficiently at pH 6.5 than pH 8.0, whereas that of the wild-type was about the same as the two pH values. We conclude that the signal peptide requires a positive charge at its amino-terminal region to function in the translocation reaction and that the rate of translocation is roughly proportional to the number of the positively charged group, irrespective of the amino acid species that donates the charge. Evidence suggesting that the positive charge is involved in the binding of precursor proteins to the membrane surface to initiate translocation is also presented.     

Interactions of erythrocytes with an artificial wall: influence of the electrical surface charge

Electrical charge on any biological surface plays a crucial role in its interaction with other molecules or surfaces. Here, we study, under flow conditions, the interactions of erythrocytes with an artificial surface: a platinum microelectrode whose charge density ranges from –15 to +27 μC/cm². This artificial surface could be similar in surface charge to an endothelium or a biomaterial. In this model, interactions are measured as a transient relative increase of the electrolyte resistance obtained by impedance measurement of a microelectrode. A maximal interaction of erythrocytes with the charged surface is calculated in the 0 to +10 μC/cm² charge density range. At negative surface charge, a less efficient contact was obtained because of electrostatic repulsion forces. High positive surface charge (charge density >10 μC/cm²) does not improve the contact but induces a progressive decrease in the contact efficiency, which could be explained by a rearrangement of macromolecules on the erythrocyte surface or an effect of positive groups on the cell membrane. This work suggests that a greater surface area of contact is obtained in the 0 to +10 μC/cm² charge density range and that this is provided by more molecular bridges. Received: 23 February 1996 / Accepted: 26 April 1996     

Optimization of DNA immobilization on gold electrodes for label-free detection by electrochemical impedance spectroscopy

The ability to immobilize DNA probes onto gold substrates at an optimum surface density is key in the development of a wide range of DNA biosensors. We present a method to accurately control probe DNA surface density by the simultaneous co-immobilization of thiol modified probes and mercaptohexanol. Probe surface density is controlled by the thiol molar ratio in solution, with a linear relationship between thiol molar ratio and probe density spanning (1-9) x10(12)/cm2. The probe surface density per microscopic surface area was determined using chronocoulometry, and a detailed analysis of the method presented. Using this sample preparation method, the effect of probe density and hybridization on the charge transfer resistance with the negatively charged ferri/ferrocyanide redox couple was determined. Above a threshold probe surface density of 2.5 x 10(12)/cm2, electrostatic repulsion from the negatively charged DNA modulates the charge transfer resistance, allowing hybridization to be detected. Below the threshold density no change in charge transfer resistance with probe density or with hybridization occurs. The probe surface density was optimized to obtain the maximum percentage change in charge transfer resistance with hybridization.     

Molecular dynamics investigation of the ionic liquid/enzyme interface: Application to engineering enzyme surface charge

Molecular simulations of the enzymes Candida rugosa lipase and Bos taurus α‐chymotrypsin in aqueous ionic liquids 1‐butyl‐3‐methylimidazolium chloride and 1‐ethyl‐3‐methylimidazolium ethyl sulfate were used to study the change in enzyme–solvent interactions induced by modification of the enzyme surface charge. The enzymes were altered by randomly mutating lysine surface residues to glutamate, effectively decreasing the net surface charge by two for each mutation. These mutations resemble succinylation of the enzyme by chemical modification, which has been shown to enhance the stability of both enzymes in ILs. After establishing that the enzymes were stable on the simulated time scales, we focused the analysis on the organization of the ionic liquid substituents about the enzyme surface. Calculated solvent charge densities show that for both enzymes and in both solvents that changing positively charged residues to negative charge does indeed increase the charge density of the solvent near the enzyme surface. The radial distribution of IL constituents with respect to the enzyme reveals decreased interactions with the anion are prevalent in the modified systems when compared to the wild type, which is largely accompanied by an increase in cation contact. Additionally, the radial dependence of the charge density and ion distribution indicates that the effect of altering enzyme charge is confined to short range (≤1 nm) ordering of the IL. Ultimately, these results, which are consistent with that from prior experiments, provide molecular insight into the effect of enzyme surface charge on enzyme stability in ILs. Proteins 2015; 83:670–680. © 2015 Wiley Periodicals, Inc.     

Surface potential determination in planar lipid bilayers: A simplification of the conductance-ratio method

One of the methods available for the measurement of surface potentials of planar lipid bilayers uses the conductance ratio between a charged and a neutral bilayer doped with ionophores to calculate the surface potential of the charged bilayer. We have devised a simplification of that method which does not require the use of an electrically neutral bilayer as control. The conductance of the charged bilayer is measured before and after the addition of divalent cations (Ba²⁺) to the bathing solution. Ba²⁺ ions screen fixed surface charges, decreasing the surface potential. If the membrane is negatively charged the screening has the effect of decreasing the membrane conductance to cations. The resulting conductance ratio is used to calculate the surface potential change, which is fed into an iterative computer program. The program generates pairs of surface potential values and calculates the surface charge density for the two conditions. Since the surface charge density remains constant during this procedure, there is only one pair of surface potentials that satisfies the condition of constant charge density.Applying this method to experimental data from McLaughlin et al. [McLaughlin, S.G.A., Szabo, G. and Eisenman, G., Divalent ions and the surface potential of charged phospholipid membranes, J. Gen. Physiol., 58 (1971) 667–687.] we have found very similar results. We have also successfully used this method to determine the effect of palmitic acid on the surface potential of asolectin membranes.     

Effect of pectin charge density on formation of multilayer films with chitosan

The effect of pectin charge density on the formation of multilayer films with chitosan (PEC/CHI) is studied by means of electro-optics. Pectins of low (21%) and high (71%) degrees of esterification, which are inversely proportional to the pectin charge density, are used to form films on colloidal beta-FeOOH particles at pH 4.0 when the CHI is fully ionized. We find that, after deposition of the first 3-4 layers, the film thickness increases linearly with the number of adsorbed layers. However, the increase in the film thickness is larger when the film is terminated with CHI. Irregular increase of the film thickness is more marked for the PEC with higher density of charge. Oscillation in the electrical polarizability of the film-coated particles with the number of deposited layers is also registered in the PEC/CHI films. The charge balance of the multilayers, calculated from electrical polarizability of the film-coated particles, is positive, with larger excess of positive charge within the film constructed from CHI and less charged PEC. This is attributed to the ability of CHI to diffuse into the film at each deposition step. Despite the CHI diffusion, the film thickness increases linearly due to the dissolution of unstable PEC/CHI complexes from the film surface.     

Spontaneous vesiculation of aqueous lipid dispersions

The swelling properties of lipid mixtures consisting of phosphatidylcholine and a charged single-chain detergent have been studied. The work presented here is confined to lipid mixtures forming smectic lamellar phases in H2O. These mixtures exhibit continuous swelling with increasing water content, provided the surface charge density exceeds a threshold value of about 1-2 microC/cm2. In excess H2O, such mixtures undergo spontaneous vesiculation: unilamellar vesicles form spontaneously when excess H2O or salt solutions of moderate ionic strength (I less than 0.2) are added to the dried film of such lipid mixtures. The resulting dispersion of unilamellar vesicles is usually polydisperse. Its average size depends on the detergent/phospholipid mole ratio, decreasing with increasing detergent content. It is shown that in the phase diagram of three-component systems consisting of phosphatidylcholine, a charged single-chain detergent, and excess H2O there is a compositional range, though narrow, within which the small unilamellar vesicle (diameter less than 100 nm) is the thermodynamically most stable structure. This behavior is characteristic of charged, single-chain detergents of 14 and more C atoms. Many pharmacologically active compounds are amphiphilic and surface-active, and as such, they will orient at phospholipid-water interfaces, imparting a net surface charge to neutral lipid surfaces. It is shown that such drugs exhibit detergent-like action. Mixed films of phosphatidylcholine and a pharmacologically active compound behave similarly to phosphatidylcholine-detergent mixtures: they undergo spontaneous vesiculation when excess H2O or salt solutions of moderate ionic strength are added. In this case, the drug itself induces vesiculation; possible pharmacological implications of this finding are discussed.     

Removal of acidic residues of the prodomain of PCSK9 increases its activity towards the LDL receptor

Proprotein convertase subtilisin/kexin type 9 (PCSK9) binds to the low density lipoprotein receptor (LDLR) at the cell surface and mediates intracellular degradation of the LDLR. The amino-terminus of mature PCSK9, residues 31–53 of the prodomain, has an inhibitory effect on this function of PCSK9, but the underlying mechanism is not fully understood. In this study, we have identified two highly conserved negatively charged segments (residues 32–40 and 48–50, respectively) within this part of the prodomain and performed deletions and substitutions to study their importance for degradation of the LDLRs.Deletion of the acidic residues of the longest negatively charged segment increased PCSK9’s ability to degrade the LDLR by 31%, whereas a modest 8% increase was observed when these residues were mutated to uncharged amino acids. Thus, both the length and the charge of this part of the prodomain were important for its inhibitory effect. Deletion of the residues of the shorter second negatively charged segment only increased PCSK9’s activity by 8%. Substitution of the amino acids of both charged segments to uncharged residues increased PCSK9’s activity by 36%. These findings indicate that the inhibitory effect of residues 31–53 of the prodomain is due to the negative charge of this segment. The underlying mechanism could involve the binding of this peptide segment to positively charged structures which are important for PCSK9’s activity. One possible candidate could be the histidine-rich C-terminal domain of PCSK9.     

Surface, subunit interfaces and interior of oligomeric proteins

The solvent-accessible surface area (As) of 23 oligomeric proteins is calculated using atomic co-ordinates from high-resolution and well-refined crystal structures. As is correlated with the protein molecular weight, and a power law predicts its value to within 5% on average. The accessible surface of the average oligomer is similar to that of monomeric proteins in its hydropathy and amino acid composition. The distribution of the 20 amino acid types between the protein surface and its interior is also the same as in monomers. Interfaces, i.e. surfaces involved in subunit contacts, differ from the rest of the subunit surface. They are enriched in hydrophobic side-chains, yet they contain a number of charged groups, especially from Arg residues, which are the most abundant residues at interfaces except for Leu. Buried Arg residues are involved in H-bonds between subunits. We counted H-bonds at interfaces and found that several have none, others have one H-bond per 200 A2 of interface area on average (1 A = 0.1 nm). A majority of interface H-bonds involve charged donor or acceptor groups, which should make their contribution to the free energy of dissociation significant, even when they are few. The smaller interfaces cover about 700 A2 of the subunit surface. The larger ones cover 3000 to 10,000 A2, up to 40% of the subunit surface area in catalase. The lower value corresponds to an estimate of the accessible surface area loss required for stabilizing subunit association through the hydrophobic effect alone. Oligomers with small interfaces have globular subunits with accessible surface areas similar to those of monomeric proteins. We suggest that these oligomers assemble from preformed monomers with little change in conformation. In oligomers with large interfaces, isolated subunits should be unstable given their excessively large accessible surface, and assembly is expected to require major structural changes.     

Changes in surface charge density on liposomes induced by Escherichia coli endotoxin.

Changes in surface charge density of liposomes induced by E. coli endotoxin were studied by microelectrophoresis. Endotoxin altered the surface charge of phosphatidylcholine liposomes from neutral to negative. The negative charge of the endotoxin-phosphatidylcholine complex was neutralized electrostatically by binding with Ca2+ (2 mM). Phosphatidylcholine liposomes were made positive by addition of the positively charged detergent, hexadecyltrimethylammonium chloride. Endotoxin made the positively charged liposomes less charged. On the other hand, phosphatidylserine liposomes which were negatively charged became less charged in the presence of high concentration of endotoxin (8 mg/ml). The endotoxin effect on phosphatidylserine liposomes was abolished by EDTA (1 mM) but potentiated by CaCl2 (0.1--2 mM). These results indicate that endotoxin interacts with liposomes both hydrophobically and electrostatically.     

Point charge distributions and electrostatic steering in enzyme/substrate encounter: Brownian dynamics of modified copper/zinc superoxide dismutases

The electrostatic steering mechanism of bovine erythrocyte Cu/Zn superoxide dismutase (SOD) was investigated through the use of Brownian dynamics. Simulations of enzyme/substrate encounter were carried out on 14 different SOD models defined by simple changes in the enzyme's point charge distribution. The magnitude and ionic strength dependence of reaction rates, rates for collision anywhere on the enzyme surface, and collision efficiency factors were analyzed to elucidate both the general and specific roles for point charges associated with amino acid residues. Collision rates for the general enzyme surface appear to be solely determined by the net charge on the enzyme. At physiological ionic strength this effect is negligible, with only 6% variation in collision rates observed as the net charge ranges from +2e to -10e. With the exception of a few charged residues in the active-site channel of SOD, point charge modifications had modest effects on reaction rates. For a large region within and surrounding the channel, reaction rates increased or decreased by only 10-15% with the addition or subtraction of a protonic unit of charge, respectively. This effect simply disappeared with increasing distance from the active site. More dramatic effects were seen at only three residues: arginine-141, glutamate-131, and lysine-134. Implications for rate enhancement through site-directed mutagenesis are discussed.     

Spatial sign-alternating charge clusters in globular proteins

Large sign-alternating charge clusters formed by the charged side groups of amino acid residues and N- and C-terminal groups were found in the majority of considered globular proteins, namely 235 in a total of 274 protein structures, i.e. 85.8%. The clusters were determined by the criteria proposed earlier: charged groups were included in the cluster if their charged N and O atoms were located at distances between 2.4 and 7.0 A. The set of selected proteins consisted of known non-homologous protein structures from the Protein Data Bank with a resolution less than or equal to 2.5 A and pair sequence similarity less than 25%. Molecular masses of the proteins were from 5.5 to 91.5 kDa and protein chain length from 50 to 830 residues. The distribution of charged groups on the protein surface between isolated charged groups, small clusters with two and three groups, and large clusters with four or more groups were found to be approximately similar making 33, 35 and 32% of the total amount of protein charged groups, respectively. The large sign-alternating charge clusters with four or more charged groups were studied in greater detail. The amount of such clusters depends on the protein chain length. The small proteins contain 1-3 clusters while the large proteins display 4-6 or more clusters. On average, 1.5 clusters per each 100 residues were observed. In contrast with this, the size of a cluster, i.e. the number of charged groups inside a cluster, does not depend on the protein molecular mass, and large clusters are observed for proteins from a range of molecular masses. Clusters consisting of four to six charged groups occur most frequently, although extra large clusters are also often revealed. We can conclude that sign-alternating charge clusters are a common feature of the protein surface of globular protein. They are suggested to play a general functional role as a local polar factor of protein surface.     

An electrodiffusion model for the blood-brain barrier permeability to charged molecules

The endothelial surface glycocalyx layer (SGL) and the basement membrane (BM) are two important components of the blood-brain barrier (BBB). They provide large resistance to solute transport across the BBB in addition to the tight junctions in the cleft between adjacent endothelial cells. Due to their glycosaminoglycan compositions, they carry negative charge under physiological conditions. To investigate the charge effect of the SGL and BM on the BBB permeability to charged solutes, we developed an electrodiffusion model for the transport of charged molecules across the BBB. In this model, constant charge densities were assumed in the SGL and in the BM. Both electrostatic and steric interaction and exclusion to charged molecules were considered within the SGL and the BM and at their interfaces with noncharged regions of the BBB. On the basis of permeability data for the positively charged ribonuclease (+4,radius=2.01?nm) and negatively charged α-lactalbumin (-10,radius=2.08?nm) measured in intact rat mesenteric and pial microvessels, our model predicted that the charge density in both SGL and BM would be ～30?mEq/L, which is comparable to that in the SGL of mesenteric microvessels. Interestingly, our model also revealed that due to the largest concentration drop in the BM, there is a region with a higher concentration of negatively charged α-lactalbumin in the uncharged inter-endothelial cleft, although the concentration of α-lactalbumin is always lower than that of positively charged ribonuclease and that of a neutral solute in the charged SGL and BM.     

To flip or not to flip: lipid-protein charge interactions are a determinant of final membrane protein topology

The molecular details of how lipids influence final topological organization of membrane proteins are not well understood. Here, we present evidence that final topology is influenced by lipid–protein interactions most likely outside of the translocon. The N-terminal half of Escherichia coli lactose permease (LacY) is inverted with respect to the C-terminal half and the membrane bilayer when assembled in mutants lacking phosphatidylethanolamine and containing only negatively charged phospholipids. We demonstrate that inversion is dependent on interactions between the net charge of the cytoplasmic surface of the N-terminal bundle and the negative charge density of the membrane bilayer surface. A transmembrane domain, acting as a molecular hinge between the two halves of the protein, must also exit from the membrane for inversion to occur. Phosphatidylethanolamine dampens the translocation potential of negative residues in favor of the cytoplasmic retention potential of positive residues, thus explaining the dominance of positive over negative amino acids as co- or post-translational topological determinants.     

Effects of net charge and the number of positively charged residues on the biological activity of amphipathic alpha-helical cationic antimicrobial peptides

In our previous study, we utilized a 26-residue amphipathic alpha-helical antimicrobial peptide L-V13K (Chen et al., Antimicrob Agents Chemother 2007, 51, 1398-1406) as the framework to study the effects of peptide hydrophobicity on the mechanism of its antimicrobial action. In this study, we explored the effects of net charge and the number of positively charged residues on the hydrophilic/polar face of L-V13K on its biological activity (antimicrobial and hemolytic) and biophysical properties (hydrophobicity, amphipathicity, helicity, and peptide self-association). The net charge of V13K analogs at pH 7 varied between -5 and +10 and the number of positively charged residues varied from 1 to 10. The minimal inhibitory concentrations (MIC) against six strains of Pseudomonas aeruginosa as well as other gram-negative and gram-positive bacteria were determined along with the maximal peptide concentration that produces no hemolysis of human red blood cells (MHC). Our results show that the number of positively charged residues on the polar face and net charge are both important for both antimicrobial activity and hemolytic activity. The most dramatic observation is the sharp transition of hemolytic activity on increasing one positive charge on the polar face of V13K i.e., the change from +8 to +9 resulted in greater than 32-fold increase in hemolytic activity (250 microg/ml to <7.8 microg/ml, respectively).