Weak binding of divalent cations to plasma gelsolin

Calcium binding of swine plasma gelsolin was examined. When applied to ion-exchange chromatography, its elution volume was drastically altered depending on the free Ca2+ concentration of the medium. The presence of two classes of Ca2+ binding sites, high-affinity sites (Kd = 7 microM) and low-affinity sites (Kd = 1 mM), was suggested from the concentration dependence of the elution volume. The tight binding sites were specific for Ca2+. The weakly bound Ca2+ could be replaced by Mg2+ once the tight binding sites were occupied with Ca2+. The binding of metal ions was totally reversible. Circular dichroism measurement of plasma gelsolin indicated that most change in secondary structure was associated with Ca2+ binding to the high-affinity sites. Binding of Mg2+ to the low-affinity sites caused a secondary structural change different from that caused by Ca2+ bound to the high-affinity sites. Gel permeation chromatography exhibited a small change in Stokes radius with and without Ca2+. Microheterogeneity revealed by isoelectric focusing did not relate to the presence of two classes of Ca2+ binding sites. These results indicated that plasma gelsolin drastically altered its surface charge property due to binding of Ca2+ or Ca2+, Mg2+ with a concomitant conformational change.     

Calmodulin binding to platelet plasma membranes

Calmodulin copurifies with platelet plasma membranes isolated by glycerol-induced lysis and density gradient centrifugation. These membranes also bind ¹²⁵I-labeled calmodulin in vitro in the presence of Ca²⁺. Binding is largely reduced by replacing Ca²⁺ by Mg²⁺ or by addition of an excess unlabeled calmodulin. The specific component of binding is saturable, with an apparent K_d of 27 nM and a maximum of 15.9 pmol binding sites per mg of membrane protein. This is equivalent to approx. 4100 binding sites per platelet. Binding was inhibited by addition of phenothiazines, a group of calmodulin antagonists. Half-maximal inhibition was attained with approx. 20 μM trifluoperazine or 50 μM chlorpromazine. In contrast, chlorpromazine-sulfoxide which is inactive towards calmodulin, did not affect the binding. Calmodulin binding polypeptides of the plasma membrane were identified by a gel-overlay technique. A major calmodulin-binding component of molecular weight 149 000 was detected. Binding to this band was Ca²⁺-dependent and inhibited by chlorpromazine. The molecular weight of this polypeptide is similar to that of glycoprotein I and also that of the red cell (Ca²⁺ + Mg²⁺)-stimulated ATPase, which is known to bind calmodulin. The possible role of calmodulin in platelet activation is analysed.     

The binding of divalent cations to myosin.

Centrifuge transport, equilibrium dialysis, and electron paramagnetic resonance studies on the binding of Mn2+ to myosin revealed two sets of noninteracting binding sites which are characterized at low ionic strength (0.016 M KCl) by affinity constants of 10(6) M-1 (Class I) and 10(3) M-1 (Class II), respectively. At 0.6 M KCl concentration, the affinity of Mn2+ for both sets of sites is reduced. The maximum number of binding sites is 2 for the high affinity and 20 to 25 for the low affinity set. Other divalent metal ions displace Mn2+ from the high affinity sites in the following order of effectiveness: Ca greater than Mg = Zn = Co greater than Sr greater than Ni. The inhibitory effects of Mg2+ and Ca2+ upon the Mn2+ binding are competitive with inhibitor constants of 0.75 to 1 mM which is similar to that of the low affinity divalent metal ion binding sites. Exposure of myosin to 37 degrees partially inhibits Mn2+ binding to Class I parallel with inhibition of ATPase activity. The binding of Mn2+ to the high affinity binding sites is not significantly influenced by ADP or PPi, although Mn2+ increases the affinity of ADP binding to myosin at high ionic strength.     

Dissociation of the glycoprotein IIb-IIIa complex in isolated human platelet membranes. Dependence of pH divalent cations

The platelet membrane glycoproteins IIb and IIIa normally exist as a complex which forms a predominant immunoprecipitate after crossed immunoelectrophoresis of Triton-X-100-solubilized platelets. Dissociation of the complex occurs by solubilization in the presence of EDTA or EGTA at pH 8.7 and is readily verified by crossed immunoelectrophoresis. Incubations of isolated membranes with EDTA or EGTA at various pH levels were performed. Removal of the chelators and solubilization showed no dissociation of the glycoprotein IIb-IIIa complex in membranes incubated at pH below 8.0. At pH above 8.0 a dissociation which increased with increasing pH was seen. Under these conditions, dissociation appears to take place already in the intact membranes. The tendency of the glycoprotein IIb-IIIa complex to become dissociated with EDTA or EGTA at increasing pH seems to be due to increased chelating capacity of the chelators concomitant with a decreased chelating capacity of glycoprotein IIb and IIIa. The divalent cations Ca2+ and Mg2+, but not Cu2+, Zn2+, Mn2+ or Sr2+, in molar concentrations below that of EGTA were able to prevent the dissociation of the glycoprotein IIb-IIIa complex by the chelator at pH 9.0, indicating that Ca2+ as well as Mg2+ can be used to keep the complex together. In some experiments it was possible to reverse the dissociation in the membranes after removal of EDTA. At pH 7.5 reassociation occurred within 15 min whether divalent cations were added or not. At pH 9.0. reassociation occurred within 2 h provided Ca2+ was present. The tendency of glycoprotein IIb and IIIa to form a complex thus appeared to be most pronounced over the physiological pH range and to be a rapid process in platelet membranes under such conditions.     

Platelet-activating factor binding to human platelet membranes

Previously reported methods for quantifying platelet-activating factor (PAF) binding to rabbit platelet membranes were modified for studies of PAF binding to human platelet membranes. The membranes were prepared by the "glycerol lysis" method and PAF binding was quantified by using polyethylene glycol precipitation to recover membrane-bound PAF. Optimal PAF binding required buffers containing 3 to 10 mm KCl and either 5 to 10 mM MgCl2 or 5 to 10 mM CaCl2. NaCl was not as effective as KCl and concentrations of NaCl greater than 3 mM strongly inhibited PAF binding. Maximal binding occurred after incubation for 60 min at 0 degree C and was reversed by the addition of excess unlabeled PAF. PAF binding was saturable. Scatchard analysis of PAF binding to 50 micrograms of membrane protein revealed 10.3 +/- 1.7 x 10(11) receptors per milligram of membrane protein and the receptors had a Kd of 7.6 +/- 1.9 nM. The calculated receptor number, binding affinity, and specificity of binding are similar to those previously calculated for PAF binding to intact human platelets, suggesting that the membrane binding site for PAF is the PAF receptor.     

Binding of thrombin to human platelet plasma membranes

Binding of ²⁵I-labeled thrombin to isolated human platelet plasma membranes was studied. Two classes of sites, one with high and one with low affinity for thrombin, were demonstrated. The apparent dissociation constants for the high and low affinity sites were 3.2 and 600 nM, respectively, similar to values obtained with intact platelets. Maximum binding was within 10 s, the shortest time measured, and then decreased with time to a constant level of binding within 45 s. When th equilibrium was perturbed by dilution, the system re-equilibrated with less thrombin bound than in a control that was diluted before mixing thrombin and membranes. Neither the time-dependent decrease nor the dilution effect were observed with phenylmethylsulfonyl-¹²⁵I-labelled thrombin, an irreversibly inhibited thrombin, suggesting that these phenomena may involve a thrombin-catalyzed modification of the membranes leading to decreased binding.     

The adsorption of divalent cations to phosphatidylcholine bilayer membranes

Electrophoretic mobility and ³¹P NMR measurements were combined to test whether the combination of the Henry, Boltzmann and Grahame equations is capable of describing the adsorption of divalent cations to phosphatidylcholine membranes. Cobalt was chosen for this study because, of all the common divalent cations, its effects on the ³¹P NMR spectrum of phosphatidylcholine membranes are easiest to interpret. Both the ³¹P NMR data on the adsorption of cobalt and the zeta potential data calculated from the electrophoretic mobility in the presence of cobalt are well described by the combination of these three equations. Electrophoretic mobility measurements were also performed with a number of other divalent cations and the zeta potentials were, in all cases, well described by the combination of these three equations. The binding deduced from such measurements decreases in the sequence: Mn²⁺, Mg²⁺, Ca²⁺, Co²⁺, Ni²⁺, Sr²⁺, Ba²⁺. If we assume that a lipid molecule occupies an area of 60 Ų and that there is a 1: 1 stoichiometry for the binding of the divalent ions to phosphatidylcholine, the dissociation constants are, respectively: 0.3, 1.0, 1.0, 1.2, 1.2, 2.8, 3.6 M.     

Adsorption of divalent cations to bilayer membranes containing phosphatidylserine

The Stern equation, a combination of the Langmuir adsorption isotherm, the Boltzmann relation, and the Grahame equation from the theory of the diffuse double layer, provides a simple theoretical framework for describing the adsorption of charged molecules to surfaces. The ability of this equation to describe the adsorption of divalent cations to membranes containing brain phosphatidylserine (PS) was tested in the following manner. Charge reversal measurements were first made to determine the intrinsic 1:1 association constants of the divalent cations with the anionic PS molecules: when the net charge of a PS vesicle is zero one-half of the available sites are occupied by divalent cations. The intrinsic association constant, therefore, is equal to the reciprocal of the divalent cation concentration at which the mobility of a PS vesicle reverses sign. The Stern equation with this association constant is capable of accurately describing both the zeta potential data obtained with PS vesicles at other concentrations of the divalent cations and the data obtained with with vesicles formed from mixtures of PS and zwitterionic phospholipids. Independent measurements of the number of ions adsorbed to sonicated PS vesicles were made with a calcium-sensitive electrode. The results agreed with the zeta potential results obtained with multilamellar vesicles. When membranes are formed at 20 degrees C in 0.1 M NaCl, the intrinsic 1:1 association constants of Ni, Co, Mn, Ba, Sr, Ca, and Mg with PS are 40, 28, 25, 20, 14, 12, and 8 M-1, respectively.     

The adsorption of divalent cations to phosphatidylglycerol bilayer membranes

The ability of the Stern equation to describe the adsorption of divalent cations to phosphatidylglycerol membranes was tested by combining ³¹P-NMR and electrophoretic mobility measurements. In 0.1 M sodium chloride both the ³¹P-NMR and the zeta potential data are well described by the Stern equation. ³¹P-NMR and ¹³C-NMR results indicate that cobalt forms inner-sphere complexes only with the phosphate group of phosphatidylglycerol molecules and that a substantial fraction of the adsorbed cobalt ions form outer-sphere complexes. Evidence is presented that suggests the alkaline earth cations also bind to phospholipids mainly by forming outer sphere complexes. Electrophoretic mobility measurements were performed with several different divalent cations. In all cases the zeta potentials in 0.1 M sodium chloride were well described by the Stern equation. The intrinsic 1 : 1 association constants (M^?1) for the phosphatidylglycerol complexes decreased in the sequence: Mn²⁺, 11.5; Ca²⁺, 8.5; Ni²⁺, 7.5; Co²⁺, 6.5; Mg²⁺, 6.0; Ba²⁺, 5.5 and Sr²⁺, 5.0.     

Regulation by divalent cations of 3H-baclofen binding to GABAB sites in rat cerebellar membranes

When investigating the effects of divalent cations (Mg2+, Ca2+, Sr2+, Ba2+, Mn2+ and Ni2+) on 3H-baclofen binding to rat cerebellar synaptic membranes, we found that the specific binding of 3H-baclofen was not only dependent on divalent cations, but was increased dose-dependently in the presence of these cations. The effects were in the following order of potency: Mn2+ congruent to Ni2+ greater than Mg2+ greater than Ca2+ greater than Sr2+ greater than Ba2+. Scatchard analysis of the binding data revealed a single component of the binding sites in the presence of 2.5 mM MgCl2, 2.5 mM CaCl2 or 0.3 mM MnCl2 whereas two components appeared in the presence of 2.5 mM MnCl2 or 1 mM NiCl2. In the former, divalent cations altered the apparent affinity (Kd) without affecting density of the binding sites (Bmax). In the latter, the high-affinity sites showed a higher affinity and lower density of the binding sites than did the single component of the former. As the maximal effects of four cations (Mg2+, Ca2+, Mn2+ and Ni2+) were not additive, there are probably common sites of action of these divalent cations. Among the ligands for GABAB sites, the affinity for (-), (+) and (+/-) baclofen, GABA and beta-phenyl GABA increased 2-6 fold in the presence of 2.5 mM MnCl2, in comparison with that in HEPES-buffered Krebs solution (containing 2.5 mM CaCl2 and 1.2 mM MgSO4), whereas that for muscimol was decreased to one-fifth. Thus, the affinity of GABAB sites for its ligands is probably regulated by divalent cations, through common sites of action.     

Interactions of divalent cations with phosphatidylserine bilayer membranes

The interaction of divalent cations with a homologous series of diacylphosphatidylserines (diacyl-PS) has been studied by differential scanning calorimetry and X-ray diffraction. Hydrated di-C14-PS (DMPS) exhibits a gel leads to liquid-crystal bilayer transition at 39 degrees C (delta H = 7.2 kcal/mol of DMPS). With increasing MgCl2 concentration, progressive conversion to a phase exhibiting a high melting (98 degrees C), high enthalpy (delta H congruent to 11.0 kcal/mol of DMPS) transition is observed. Similar behavior is observed for DMPS with increasing CaCl2 concentration. In this case, the high-temperature transition of the Ca2+-DMPS complex occurs at approximately 155 degrees C and is immediately followed by an exothermic transition probably associated with PS decomposition. For di-C12-, di-C14-, di-C16- (DPPS), and di-C18-PS, the transition temperatures of the Ca2+-PS complexes are in the range 151-155 degrees C; only di-C10-PS exhibits a significantly lower value, 142 degrees C. A different pattern of behavior is exhibited by DPPS in the presence of Sr2+ or Ba2+, with transitions in the range 70-80 degrees C being observed. X-ray diffraction of the Ca2+-PS complexes at 20 degrees C provides evidence of structural homology. All Ca2+-PS complexes exhibit bilayer structures, the bilayer periodicity increasing linearly from 35.0 A for di-C10-PS to 52.5 A for di-C18-PS. Wide-angle X-ray diffraction data indicate that hydrocarbon chain "crystallization" occurs on Ca2+-PS complex formation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Network formation in negative charged membranes by two divalent cations and the catastrophe

The ligands of Ca2+-Cu2+-phosphatidylserine (PS) complexes in membrane networks at the water-oil interface through the symmetry breaking instability and the head groups of PS molecules were changed into a solid-like state. A first step in this transition is described by the following scheme in one unit in which the molar ratio is Ca2+: Cu2+: PS = 1:2:4; [Oh]+2[Oh]*----3[Oh]*, where [Oh]* denotes a little distorted ligand structure [LnM2+...2H2O] from [LnM2+2H2O], where Ln is PS molecules (n = 2 to Cu2+ and 4 to Ca2+). All the ligands are changed to [D4h] by the unit-unit interaction due to the network formation; [Oh]*----[D4h]. The whole system is equivalent to Schl?gl's scheme and is given by a cubic state equation for suitable variables transformations: x = -x3 - ux - v, where x corresponds to the concentration of [Oh]*, and u and v are related to rate constants in the first and the second steps, and they also depend on the initial [Oh] and the final [D4h] concentrations. This system is transferred into a new state with a cusp catastrophe.     

Large divalent cations and electrostatic potentials adjacent to membranes. A theoretical calculation

We have extended the Gouy-Chapman theory of the electrostatic diffuse double layer by considering the finite size of divalent cations in the aqueous phase adjacent to a charged surface. The divalent cations are modeled as either two point charges connected by an infinitely thin, rigid "rod" or two noninteracting point charges connected by an infinitely thin, flexible "string." We use the extended theory to predict the effects of a cation of length 10 A (1 nm) on the zeta and surface potentials of phospholipid bilayer membranes. The predictions of the rod and string models are similar to one another but differ markedly from the predictions of the Gouy-Chapman theory. Specifically, the extended model predicts that a large divalent cation will have a smaller effect on the potential adjacent to a negatively charged bilayer membrane than a point divalent cation, that the magnitude of this discrepancy will decrease as the Debye length increases, and that a large divalent cation will produce a negative zeta potential on a membrane formed from zwitterionic lipids. These predictions agree qualitatively with the experimental results obtained with the large divalent cation hexamethonium. We discuss the biological relevance of our calculations in the context of the interaction of cationic drugs with receptor sites on cell membranes.     

Conformational changes induced by binding of divalent cations to calregulin

Scatchard analysis of equilibrium dialysis studies have revealed that in the presence of 3.0 mM MgCl2 and 150 mM KCl, calregulin has a single binding site for Ca2+ with an apparent dissociation constant (apparent Kd) of 0.05 microM and 14 binding sites for Zn2+ with apparent Kd(Zn2+) of 310 microM. Ca2+ binding to calregulin induces a 5% increase in the intensity of intrinsic fluorescence and a 2-3-nm blue shift in emission maximum. Zn2+ binding to calregulin causes a dose-dependent increase of about 250% in its intrinsic fluorescence intensity and a red shift in the emission maximum of about 11 nm. Half-maximal wavelength shift occurs at 0.4 mol of Zn2+/mol of calregulin, and 100% of the wavelength shift is complete at 2 mol of Zn2+/mol of calregulin. In the presence of Zn2+ and calregulin the fluorescence intensity of the hydrophobic fluorescent probe 8-anilino-1-napthalenesulfonate (ANS) was enhanced 300-400% with a shift in emission maximum from 500 to 480 nm. Half-maximal Zn2+-induced shift in ANS emission maximum occurred at 1.2 mol of Zn2+/mol of calregulin, and 100% of this shift occurred at 6 mol of Zn2+/mol of calregulin. Of 12 cations tested, only Zn2+ and Ca2+ produced changes in calregulin intrinsic fluorescence, and none of these metal ions could inhibit the Zn2+-induced red shift in intrinsic fluorescence emission maximum. Furthermore, none of these cations could inhibit or mimic the Zn2+-induced blue shift in ANS emission maximum. These results suggest that calregulin contains distinct and specific ligand-binding sites for Ca2+ and Zn2+. While Ca2+ binding results in the movement of tryptophan away from the solvent, Zn2+ causes a movement of tryptophan into the solvent and the exposure of a domain with considerable hydrophobic character.     

Anion influence on the binding of divalent cations to phosphatidylcholine

We have used the osmotic pressure technique of Rand, Parsegian and co-workers (Nature 259 (1976) 601–603) to investigate the effect of anion species on the binding of M²⁺ to dipalmitoylphosphatidylcholine bilayers. Calcium and magnesium salts show a complex behavior which is consistent with both anion binding and screening. We observe virtually no change, within the accuracy of our experiment, in the decay of repulsive pressure with inter-bilayer separation for the acetate and nitrate salts of magnesium and calcium; however, the chloride salt does show a different pressure decay. At any given bilayer separation, , with calcium and magnesium salts present, the anions produce a decrease in the repulsive pressure in the order acetate⁻ > Cl⁻ > NO₃⁻.     

Further studies on the binding of divalent cations to the phosphoglycoprotein phosvitin.

Dialysis equilibrium measurements at 25 degrees indicate that, at pH 6.8 and at a concentration of 1.0 times 10(-10) 3 M MnC12 or CoC12, phosvitin binds 113 Mn2+ and 120 Co2+. The binding is cooperative at low cation concentrations. The number of Mg2+, Ca2+, Mn2+, and Co2+ bound is not affected by temperatures of up to 60 degrees; however, the cooperactivity is enhanced. Optical rotatory dispersion and circular dichroism studies indicate that a conformational change occurs on binding of Mn2+ and Co2+ which parallels the one produced by Ca2+ and reported elsewhere [Grizzuti, K., and Perlmann, G.E. (1973), Biochemistry 12, 4399]. The conformational changes induced by Mg2+ and Mn2+ follow different paths. Upon binding of Mn2+ and Co2+ the intrinsic viscosity, [eta], of phosvitin decreases from about 0.5 to 0.03 dl/g, while Mg2+ and Ca2+ decrease [eta] to 0.048 dl/g. The ultraviolet absorption spectrum of phosvitin is altered upon binding of Ca2+, Mn2+, and Co2+, but not upon binding of Mg2+; an increase of the temperature to 60% has no further effect on the spectra.     

Large divalent cations and electrostatic potentials adjacent to membranes. Experimental results with hexamethonium.

A simple extension of the Gouy-Chapman theory predicts that the ability of a divalent cation to screen charges at a membrane-solution interface decreases significantly if the distance between the charges on the cation is comparable with the Debye length. We tested this prediction by investigating the effect of hexamethonium on the electrostatic potential adjacent to negatively charged phospholipid bilayer membranes. The distance between the two charges of an extended hexamethonium molecule is approximately 1 nm, which is the Debye length in the 0.1 M monovalent salt solutions used in these experiments. Six different experimental approaches were utilized. We measured the electrophoretic mobility of multilamellar vesicles to determine the zeta potential, the line width of the 31P nuclear magnetic resonance (NMR) signal from sonicated vesicles to calculate the change in potential at the phosphodiester moiety of the lipid, and the conductance of planar bilayer membranes exposed to either carriers (nonactin) or pore formers (gramicidin) to estimate the change in potential within the membrane. We also measured directly the effect of hexamethonium on the potential above a monolayer formed from negative lipids, and attempted to calculate the change in the surface potential of a bilayer membrane from capacitance measurements. With the exception of the capacitance calculations, each of the techniques gave comparable results: hexamethonium exerts a smaller effect on the potential than that predicted by the classic screening theory. The results are consistent with the predictions of the extended Gouy-Chapman theory and are relevant to the interpretation of physiological and pharmacological experiments that utilize hexamethonium and other large divalent cations.     

Somatostatin binding to pituitary plasma membranes.

A method has been developed for the study of somatostatin binding to anterior pituitary plasma membranes. When 5×10^?9M [¹²⁵I]Tyr¹-somatostatin (SA 18 Ci/mmol) was incubated with isolated pituitary plasma membranes (protein = 100 μg), 13.6% of total radioactivity was bound excluding nonspecific binding. The Scatchard plot could be resolved into two distinct components and analyzed to yield: K₁diss = 3.3×10^?8M and K₂diss = 7.7×10^?6M. This binding was shown to be specific for somatostatin.     

Selective binding of divalent cations toward heme proteins

Potential toxicity of transition metals like Hg, Cu and Cd are well known and their affinity toward proteins is of great concern. This work explores the selective nature of interactions of Cu²⁺, Hg²⁺ and Cd²⁺ with the heme proteins leghemoglobin, myoglobin and cytochrome C. The binding profiles were analyzed using absorbance spectrum and steady-state fluorescence spectroscopy. Thermodynamic parameters like enthalpy, entropy and free energy changes were derived by isothermal calorimetry and consequent binding parameters were compared for these heme proteins. Free energy (DG) values revealed Cu²⁺ binding toward myoglobin and leghemoglobin to be specific and facile in contrast to weak binding for Hg²⁺ or Cd²⁺. Time correlated single photon counting indicated significant alteration in excited state lifetimes for metal complexed myoglobin and leghemoglobin suggesting bimolecular collisions to be involved. Interestingly, none of these cations showed significant affinity for cytochrome c pointing that, presence of conserved sequences or heme group is not the only criteria for cation binding toward heme proteins, but the microenvironment of the residues or a specific folding pattern may be responsible for these differential conjugation profile. Binding of these cations may modulate the conformation and functions of these biologically important proteins.