F-actin and myosin II binding domains in supervillin

Detergent-resistant membranes contain signaling and integral membrane proteins that organize cholesterol-rich domains called lipid rafts. A subset of these detergent-resistant membranes (DRM-H) exhibits a higher buoyant density ( approximately 1.16 g/ml) because of association with membrane skeleton proteins, including actin, myosin II, myosin 1G, fodrin, and an actin- and membrane-binding protein called supervillin (Nebl, T., Pestonjamasp, K. N., Leszyk, J. D., Crowley, J. L., Oh, S. W., and Luna, E. J. (2002) J. Biol. Chem. 277, 43399-43409). To characterize interactions among DRM-H cytoskeletal proteins, we investigated the binding partners of the novel supervillin N terminus, specifically amino acids 1-830. We find that the supervillin N terminus binds directly to myosin II, as well as to F-actin. Three F-actin-binding sites were mapped to sequences within amino acids approximately 280-342, approximately 344-422, and approximately 700-830. Sequences with combinations of these sites promote F-actin cross-linking and/or bundling. Supervillin amino acids 1-174 specifically interact with the S2 domain in chicken gizzard myosin and nonmuscle myosin IIA (MYH-9) but exhibit little binding to skeletal muscle myosin II. Direct or indirect binding to filamin also was observed. Overexpression of supervillin amino acids 1-174 in COS7 cells disrupted the localization of myosin IIB without obviously affecting actin filaments. Taken together, these results suggest that supervillin may mediate actin and myosin II filament organization at cholesterol-rich membrane domains.     

Theoretical considerations in the equilibrium binding of myosin fragments on F-actin

In a previous paper, equilibrium constants for the binding of myosin fragments onto F-actin were assumed known and the statistical problems encountered when the actin sites are occupied to an arbitrary fractional extent were analyzed. The object of the present paper is to attempt to understand the observed order of magnitude of these equilibrium constants in terms of the statistical mechanical degrees of freedom involved. That is, we examine here the equilibrium constants them- selves rather than the statistical consequences of the equilibrium constants. The treatment given amounts to a semi-quantitative sketch or outline of the problem. Structural details are much too uncertain to warrant a careful and rigorous treatment at this time. But the discussion suffices to establish the essential qualitative features of the problem. The procedure used is to exa- mine the important equilibrium constants, one at a time, in terms of the factors (partition functions) that contribute to each constant, together with numerical estimates for these factors.     

Effect of F-actin upon the binding of ADP to myosin and its fragments.

The effect of F-actin upon the binding of ADP to rabbit skeletal muscle myosin, heavy meromyosin, and subfragment 1 was studied by equilibrium dialysis, ultracentrifuge transport, and light scattering techniques. Both myosin and H-meromyosin (HMM) bind a maximum of approximately 1.6 mol of ADP/mol of protein, while S-1 binds approximately 0.9 mol of ADP/mol of protein. The affinity for ADP of all three preparations was similar at a given ionic strength (approximately 10(6) M-1 at 0.05 M KCl) and decreased with increasing ionic strength. Under conditions similar to those used for the measurement of ADP binding, the binding sites of myosin, HMM, and subfragment 1 (S-1) are saturated with actin at molar ratios of 2, 2, and 1 mol of actin monomer/mol of protein, respectively, as determined by light scattering, ultracentrifuge transport, and in the case of myosin by ATPase measurements. F-actin was found to inhibit ADP binding, but even at an actin concentration at least twice that required for saturation of myosin, HMM, or S-1, significant ADP binding remained. This ADP binding was inhibited by 10(-4) M pyrophosphate. The observations are consistent with the formation of an actomyosin-ADP complex in which actin and ADP are bound to myosin at distinct but interacting sites.     

Electrostatic contributions to heat capacity changes of DNA-ligand binding.

Significant heat capacity changes (DeltaCp) often accompany protein unfolding, protein binding, and specific DNA-ligand binding reactions. Such changes are widely used to analyze contributions arising from hydrophobic and polar hydration. Current models relate the magnitude of DeltaCp to the solvent accessible surface area (ASA) of the molecule. However, for many binding systems-particularly those involving non-peptide ligands-these models predict a DeltaCp that is significantly different from the experimentally measured value. Electrostatic interactions provide a potential source of heat capacity changes and do not scale with ASA. Using finite-difference Poisson-Boltzmann methods (FDPB), we have determined the contribution of electrostatics to the DeltaCp associated with binding for DNA binding reactions involving the ligands DAPI, netropsin, lexitropsin, and the lambda repressor binding domain.     

Parking problem and negative cooperativity of binding of myosin subfragment 1 to F-actin

Previously we provided evidence that myosin subfragment 1 (S1) can bind either one (state 1) or two actin monomers (state 2) in solution and in muscle fiber. Here we present results of the kinetics study of binding of S1 to F-actin labeled with fluorescent dye pyrene. A transition from state 1 to state 2 depends on probability that the second actin is free, which is high when molar ratio of S1/actin (R) is less than 0.5, and it decreases dramatically when R>2.0 due to the parking problem. The kinetics data obtained at different molar ratios were well fitted by two binding states model. The sequential binding of myosin head initially with one actin monomer and then with the second actin monomer in F-actin can play a key role in force generation by actin-myosin and their directed movement.     

Properties of long myosin light chain kinase binding to F-actin in vitro and in vivo

Short and long myosin light chain kinases (MLCKs) are Ca(2+)/calmodulin-dependent enzymes that phosphorylate the regulatory light chain of myosin II in thick filaments but bind with high affinity to actin thin filaments. Three repeats of a motif made up of the sequence DFRXXL at the N terminus of short MLCK are necessary for actin binding (Smith, L., Su, X., Lin, P., Zhi, G., and Stull, J. T. (1999) J. Biol. Chem. 274, 29433-29438). The long MLCK has two additional DFRXXL motifs and six Ig-like modules in an N-terminal extension, which may confer unique binding properties for cellular localization. Two peptides containing either five or three DFRXXL motifs bound to F-actin and smooth muscle myofilaments with maximal binding stoichiometries consistent with each motif binding to an actin monomer in the filaments. Both peptides cross-linked F-actin and bound to stress fibers in cells. Long MLCK with an internal deletion of the five DFRXXL motifs and the unique NH(2)-terminal fragment containing six Ig-like motifs showed weak binding. Cell fractionation and extractions with MgCl(2) indicate that the long MLCK has a greater affinity for actin-containing filaments than short MLCK in vitro and in vivo. Whereas DFRXXL motifs are necessary and sufficient for short MLCK binding to actin-containing filaments, the DFRXXL motifs and the N-terminal extension of long MLCK confer high affinity binding to stress fibers in cells.     

Electrostatic contributions to the binding free energy of the lambdacI repressor to DNA.

A model based on the nonlinear Poisson-Boltzmann (NLPB) equation is used to study the electrostatic contribution to the binding free energy of the lambdacI repressor to its operator DNA. In particular, we use the Poisson-Boltzmann model to calculate the pKa shift of individual ionizable amino acids upon binding. We find that three residues on each monomer, Glu34, Glu83, and the amino terminus, have significant changes in their pKa and titrate between pH 4 and 9. This information is then used to calculate the pH dependence of the binding free energy. We find that the calculated pH dependence of binding accurately reproduces the available experimental data over a range of physiological pH values. The NLPB equation is then used to develop an overall picture of the electrostatics of the lambdacI repressor-operator interaction. We find that long-range Coulombic forces associated with the highly charged nucleic acid provide a strong driving force for the interaction of the protein with the DNA. These favorable electrostatic interactions are opposed, however, by unfavorable changes in the solvation of both the protein and the DNA upon binding. Specifically, the formation of a protein-DNA complex removes both charged and polar groups at the binding interface from solvent while it displaces salt from around the nucleic acid. As a result, the electrostatic contribution to the lambdacI repressor-operator interaction opposes binding by approximately 73 kcal/mol at physiological salt concentrations and neutral pH. A variety of entropic terms also oppose binding. The major force driving the binding process appears to be release of interfacial water from the protein and DNA surfaces upon complexation and, possibly, enhanced packing interactions between the protein and DNA in the interface. When the various nonelectrostatic terms are described with simple models that have been applied previously to other binding processes, a general picture of protein/DNA association emerges in which binding is driven by the nonpolar interactions, whereas specificity results from electrostatic interactions that weaken binding but are necessary components of any protein/DNA complex.     

The N-terminal domains of myosin binding protein C can bind polymorphically to F-actin

The regulation of vertebrate striated muscle contraction involves a number of different molecules, including the thin-filament accessory proteins tropomyosin and troponin that provide Ca²⁺-dependent regulation by controlling access to myosin binding sites on actin. Cardiac myosin binding protein C (cMyBP-C) appears to modulate this Ca²⁺-dependent regulation and has attracted increasing interest due to links with inherited cardiac diseases. A number of single amino acid mutations linked to clinical diseases occur in the N-terminal region of cMyBP-C, including domains C0 and C1, which previously have been shown to bind to F-actin. This N-terminal region also has been shown to both inhibit and activate actomyosin interactions in vitro. Using electron microscopy and three-dimensional reconstruction, we show that C0 and C1 can each bind to the same two distinctly different positions on F-actin. One position aligns well with the previously reported binding site that clashes with the binding of myosin to actin, but would force tropomyosin into an “on” position that exposes myosin binding sites along the filament. The second position identified here would not interfere with either myosin binding or tropomyosin positioning. It thus appears that the ability to bind to at least two distinctly different positions on F-actin, as observed for tropomyosin, may be more common than previously considered for other actin binding proteins. These observations help to explain many of the seemingly contradictory results obtained with cMyBP-C and show how cMyBP-C can provide an additional layer of regulation to actin-myosin interactions. They also suggest a redundancy of C0 and C1 that may explain the absence of C0 in skeletal muscle.     

Electrostatic contributions to the binding of Ca2+ in calbindin D9k

A set of accurate experimental data is provided for Ca2+ ion binding to calbindin D9k, a protein in the calmodulin superfamily of intracellular regulatory proteins. The study comprises both the role of protein surface charges and the effects of added electrolyte. The two macroscopic Ca2(+)-binding constants K1 and K2 are determined for the wild-type and eight mutant calbindins in 0, 0.05, 0.10, and 0.15 M KCl from titrations in the presence of Quin 2 or 5,5'-Br2BAPTA. The mutations involve replacement of surface carboxylates (of Glu17, Asp19, Glu26, and Glu60) with the corresponding amides. It is found that K1K2 may decrease by a factor of up to 2.5 x 10(5) (triple mutant in 0.15 M KCl as compared to the wild-type protein in 0 M KCl). Ca2(+)-binding constants of the individual Ca2+ sites (microscopic binding constants) have also been determined. The positive cooperativity of Ca2+ binding, previously observed at low salt concentration [Linse et al. (1987) Biochemistry 26, 6723-6735], is also present at physiological ionic strength and amounts to 5 kJ.mol-1 at 0.15 M KCl. The electrolyte concentration and some of the mutations are found to affect the cooperativity. 39K NMR studies show that K+ binds weakly to calbindin. Two-dimensional 1H NMR studies show, however, that potassium binding does not change the protein conformation, and the large effect of KCl on the Ca2+ affinity is thus of unspecific nature. Two-dimensional 1H NMR has also been used to assess the structural consequences of the mutations through assignments of the backbone NH and C alpha H resonances of six mutants.(ABSTRACT TRUNCATED AT 250 WORDS)     

Interaction of two heads of myosin with F-actin: binding of H-meromyosin with F-actin in the absence of nucleotide

The bindings of S-1 and the two heads of HMM with pyrene-labeled F-actin were studied using the change in light-scattering intensity or that in the fluorescence intensity of the pyrenyl group. At low ionic strength (50 mM KCl), both S-1 and HMM became bound tightly with F-actin (Kd less than 0.1 microM) and both heads of HMM became bound to F-actin. The affinities of S-1 and HMM for F-actin decreased with increasing KCl concentration. In 1 M KCl, the Kd values of S-1 and HMM for F-actin were 11 and 0.58 microM, respectively. Thus, HMM was bound to F-actin 19 times more tightly than S-1. We compared the extent of binding of HMM to F-actin measured by a centrifugation method with that measured by the fluorescence change of pyrenyl-group, and found that even in 1 M KCl, HMM became bound to F-actin with a two-headed attachment. We measured the kinetics of binding and dissociation of acto-S-1 and acto-HMM from the time course of the change in light-scattering intensity after mixing S-1 or HMM with F-actin at 1 M KCl and that after mixing 1 M KCl with acto-S-1 or acto-HMM formed at low ionic strength.(ABSTRACT TRUNCATED AT 250 WORDS)     

Changes in the thermal unfolding of p-phenylenedimaleimide-modified myosin subfragment 1 induced by its 'weak' binding to F-actin

Differential scanning calorimetry (DSC) was used to analyze the thermal unfolding of myosin subfragment 1 (S1) with the SH1 (Cys-707) and SH2 (Cys-697) groups cross-linked by N,N'-p-phenylenedimaleimide (pPDM-S1). It has been shown that F-actin affects the thermal unfolding of pPDM-S1 only at very low ionic strength, when some part of pPDM-S1 binds weakly to F-actin, but not at higher ionic strength (200 mM KCl). The weak binding of pPDM-S1 to F-actin shifted the thermal transition of pPDM-S1 by about 5 degrees C to a higher temperature. This actin-induced increase in thermal stability of pPDM-S1 was similar to that observed with 'strong' binding of unmodified S1 to F-actin. Our results show that actin-induced structural changes revealed by DSC in the myosin head occur not only upon strong binding but also on weak binding of the head to F-actin, thus suggesting that these changes may occur before the power-stroke and play an important role in the motor function of the head.     

Electrostatic contributions to oligonucleotide transitions

In a previous paper we employed Monte Carlo techniques to calculate distribution functions for distances between charged phosphates of randomly coiled oligonucleotides in solution. The average energy of the random coil, as well as the loop weighting function and bimolecular nucleation parameter, was obtained as a function of chain length and salt concentration. In the present paper we apply the results to a consideration of the electrostatic dependence of the helix–coil transition in oligonucleotides. By considering the equilibrium among three species: hairpin, dimer, and random coil, we have calculated (1) the variation in melting temperature of dimer, hairpin, and the dimer-hairpin mixture with salt concentration and chain length, (2) the variation in the equilibrium between dimer and hairpin as a function of salt concentration, temperature, and length, (3) the variation in the transition breadth with salt concentration and chain length.     

ADF/cofilin regulates actomyosin assembly through competitive inhibition of myosin II binding to F-actin

The contractile actin cortex is important for diverse fundamental cell processes, but little is known about how the assembly of F-actin and myosin II motors is regulated. We report that depletion of actin depolymerizing factor (ADF)/cofilin proteins in human cells causes increased contractile cortical actomyosin assembly. Remarkably, our data reveal that the major cellular defects resulting from ADF/cofilin depletion, including cortical F-actin accumulation, were largely due to excessive myosin II activity. We identify that ADF/cofilins from unicellular organisms to humans share a conserved activity to inhibit myosin II binding to F-actin, indicating a mechanistic rationale for our cellular results. Our study establishes an essential requirement for ADF/cofilin proteins in the control of normal cortical contractility and in processes such as mitotic karyokinesis. We propose that ADF/cofilin proteins are necessary for controlling actomyosin assembly and intracellular contractile force generation, a function of equal physiological importance to their established roles in mediating F-actin turnover.     

Microcalorimetric measurement of the enthalpy of binding of rabbit skeletal myosin subfragment 1 and heavy meromyosin to F-actin

The heat of binding of rabbit skeletal myosin subfragment 1 (myosin-S1) and heavy meromyosin (HMM) to F-actin has been measured by batch calorimetry. Proton release measurements in unbuffered solutions indicate that less than 0.1 mol of protons is absorbed or released per mol of myosin head bound to actin. Hence, the measured heats are approximately equal to the enthalpy of myosin-S1 and HMM binding to actin. The enthalpy of binding of myosin-S1 to actin was +22 +/- 3 and +27 +/- 5 kJ/mol of myosin-S1 in two series of experiments at 12 degrees C and +26 +/- 5 kJ/mol of myosin-S1 at 0 degrees C, indicating that delta Cp for this reaction in the range of 0-12 degrees C is small (-80 J/mol/K). The enthalpy of binding of HMM to actin at 12 degrees C was found to be +26 +/- 1 kJ/mol of myosin head. The enthalpies determined here and the equilibrium constants obtained from the literature for measurements at 20 degrees C under identical solvent conditions were used to estimate the entropy of the association of myosin S1 and HMM with F-actin: +235 J/mol/K for myosin-S1 and +190 J/mol of myosin head/K for HMM. Thermodynamic parameters of the interaction of myosin-S1 with actin and ADP or AMP-PNP can be evaluated using the enthalpy of association of myosin-S1 with actin determined here, together with literature values for the equilibrium constants and enthalpies of binding of these nucleotides to myosin-S1. The calculated enthalpies of binding of ADP or AMP-PNP to actomyosin-S1 are small and negative.     

Kinetic properties of binding of myosin subfragment-1 with F-actin in the absence of nucleotide

The rate constant for the binding of myosin subfragment-1 (S-1) with F-actin in the absence of nucleotide, k1, and that for dissociation of the F-actin-myosin subfragment-1 complex (acto-S-1), k-1, were measured independently. The rate of S-1 binding with F-actin was measured from the time course of the change in the light scattering intensity after mixing S-1 with various concentrations of F-actin and k1 was found to be 2.55 X 10(6) M-1 X S-1 at 20 degrees C. The dissociation rate of acto-S-1 was determined using F-actin labeled with pyrenyl iodoacetamide (Pyr-FA). Pyr-FA, with its fluorescence decreased by binding with S-1, was mixed with acto-S-1 complex and the rate of displacement of F-actin by Pyr-FA was measured from the decrease in the Pyr-FA fluorescence intensity. The k-1 value was calculated to be 8.5 X 10(-3) S-1 (or 0.51 min-1). The value of the dissociation constant of S-1 from acto-S-1 complex, Kd, was calculated from Kd = k-1/k1 to be 3.3 X 10(-9) M at 20 degrees C. Kd was also measured at various temperatures (0-30 degrees C), and the thermodynamic parameters, delta G degree, delta H degree, and delta S degree, were estimated from the temperature dependence of Kd to be -11.3 kcal/mol, +2.5 kcal/mol, and +47 cal/deg . mol, respectively. Thus, the binding of the myosin head with F-actin was shown to be endothermic and entropy-driven.     

Binding of myosin subfragment-1 to F-actin.

During a part of the hydrolytic cycle, myosin head (S1) carries no nucleotide and binds strongly to an actin filament forming a rigor bond. At saturating concentration of S1 in rigor, S1 is well known to form 1:1 complex with actin. However, we have provided evidence that under certain conditions S1 could also form a complex with 2 actin monomers in a filament (Andreev, O.A. & Borejdo, J. (1991) Biochem. Biophys. Res. Comm. 177, 350-356). This view was recently challenged by Carlier & Didry (Carlier, M-F. & Didry, D. (1992) Biochem. Biophys. Res. Comm. 183, 970-974) who interpreted our data by suggesting that F-actin underwent a simple depolymerization and implied that, when only actin in the F-form was scored, the real stoichiometry in our experiments was 1:1. We show here that under conditions of our experiments less than 8% of actin was depolymerized. Moreover, we have repeated the experiments in the presence of phalloidin and show that under these conditions too, when S1 was added slowly to a fixed concentration of F-actin, it formed a different complex with F-actin than when it was added quickly. This confirms our original conclusion that S1 can bind actin in two different ways and shows that depolymerization of F-actin is not responsible for this finding.     

Electrostatic contributions to binding of transition state analogues can be very different from the corresponding contributions to catalysis: phenolates binding to the oxyanion hole of ketosteroid isomerase

The relationship between binding of transition state analogues (TSAs) and catalysis is an open problem. A recent study of the binding of phenolate TSAs to ketosteroid isomerase (KSI) found a small change in the binding energy with a change in charge delocalization of the TSAs. This has been taken as proof that electrostatic effects do not contribute in a major way to catalysis. Here we reanalyze the relationship between the binding of the TSAs and the chemical catalysis by KSI as well as the binding of the transition state (TS), by computer simulation approaches. Since the simulations reproduce the relevant experimental results, they can be used to quantify the different contributions to the observed effects. It is found that the binding of the TSA and the chemical catalysis represent different thermodynamic cycles with very different electrostatic contributions. While the binding of the TSA involves a small electrostatic contribution, the chemical catalysis involves a charge transfer process and a major electrostatic contribution due to the preorganization of the active site. Furthermore, it is found that the electrostatic preorganization contributions to the binding of the enolate intermediate of KSI and the TS are much larger than the corresponding effect for the binding of the TSAs. This reflects the dependence of the preorganization on the orientation of the nonpolar form of the TSAs relative to the oxyanion hole. It seems to us that this work provides an excellent example of the need for computational studies in analyzing key experimental findings about enzyme catalysis.     

Electrostatic contributions to residue-specific protonation equilibria and proton binding capacitance for a small protein

Charge-charge interactions in proteins are important in a host of biological processes. Here we use 13C NMR chemical shift data for individual aspartate and glutamate side chain carboxylate groups to accurately detect site-specific protonation equilibria in a variant of the B1 domain of protein G (PGB1-QDD). Carbon chemical shifts are dominated by changes in the electron distribution within the side chain and therefore excellent reporters of the charge state of individual groups, and the data are of high precision. We demonstrate that it is possible to detect local charge interactions within this small protein domain that stretch and skew the chemical shift titration curves away from "ideal" behavior and introduce a framework for the analysis of such convoluted data to study local charge-charge interactions and electrostatic coupling. It is found that, due to changes in electrostatic potential, the proton binding affinity, Ka, of each carboxyl group changes throughout the titration process and results in a linearly pH dependent pKa value. This result could be readily explained by calculations of direct charge-charge interactions based on Coulomb's law. In addition, the slope of pKa versus pH was dependent on screening by salt, and this dependence allowed the selective study of charge-charge interactions. For PGB1-QDD, it was established that mainly differences in self-energy, and not direct charge-charge interactions, are responsible for shifted pKa values within the protein environment.