Biomedical subjects

J Borejdo

Publications and source records attributed to J Borejdo.

At least 19 recordsLinked to original sources

PubMed1992

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.

Actins↗

PubMed1992

Two different acto-S1 complexes.

Based on change in anisotropy of fluorescently labelled S1 and on increase in turbidity of acto-S1 complex when S1 bound to F-actin, we reported previously that depending on the molar ratio of S1 to actin two different complexes of actin monomer (A) and myosin subfragment 1 (S1) could be formed: A1*S1 (one actin with one S1) and A2*S1 (two actins with one S1). Here we extend these findings to F-actin labelled with pyrene and cross-linked to S1 with 1-ethyl-3-(3-dimethyl-aminopropyl)carbodiimide (EDC). The fluorescence of pyrene F-actin decreased with increase in S1 concentration and reached saturation at a molar ratio of S1 to actin of either 0.5 or 1.0, depending on whether S1 was added slowly (5 min) or quickly (10-20 s between additions). Incubation of A2*S1 complex in excess of S1 for > 1 h caused a shift in equilibrium towards the A1*S1 complex. The A2*S1 complexes were not formed at high S1 to actin ratios (> 1.0) owing to competition between heads. Crosslinking experiments showed that the formation of EDC crosslinked products, 175-185 kDa doublet and 265 kDa band, depended on the ratio S1 to actin. To assess the relative ratio of S1 and actin in crosslinked products, we labelled S1 and F-actin with different fluorescent probes (5-IAF and IATR). The S1 to actin ratio was proportional to the ratio of intensities of fluorescence of labelled S1 and actin. The S1 to actin ratio in 265 kDa product was two times smaller than in 175-185 kDa doublet (which is believed to be A1*S1 complex) and therefore 265 kDa band corresponded to A2*S1. Transition between two types of binding may be important to understanding how muscle contracts.

Actin Cytoskeleton↗

PubMed1992

Diffusion of heavy meromyosin in the presence of F-actin and ATP.

We looked for evidence that the diffusion of heavy meromyosin is modified by its interaction with actin. To be able to observe diffusion in one dimension, we electrophoresed the complex of F-actin and heavy meromyosin in agarose gels in thin capillaries. The intensity profile of the electrophoretic band of the complex showed a sharp peak, which in 1% agarose in the electric field of 17.8 V cm-1 at room temperature migrated at 3.2 cm h-1. The time evolution of the profile after the electrophoresis ended was a measure of the diffusion of heavy meromyosin. After 10 min the intensity profile of heavy meromyosin diffusing in the presence of F-actin and ATP had undergone as much change as the profile of free heavy meromyosin. Modelling of the diffusion process showed that the mean diffusion coefficient of heavy meromyosin moving over actin in the presence of ATP was 7.2 x 10(-7) cm2 s-1 and that it was not statistically different from the diffusion coefficient of free heavy meromyosin. This data is interpreted to show that the diffusion of heavy meromyosin is not modified by its interaction with actin.

Actins↗

PubMed1992

Motion of actin filaments in the presence of myosin heads and ATP.

We measured, by fluorescence correlation spectroscopy, the motion of actin filaments in solution during hydrolysis of ATP by acto-heavy meromyosin (acto-HMM). The method relies on the fact that the intensity of fluorescence fluctuates as fluorescently labeled actin filaments enter and leave a small sample volume. The rapidity of these number fluctuations is characterized by the autocorrelation function, which decays to 0 in time that is related to the average velocity of translation of filaments. The time of decay of the autocorrelation function of bare actin filaments in solution was 10.59 +/- 0.85 s. Strongly bound (rigor) heads slowed down the diffusion. Direct observation of filaments under an optical microscope showed that addition of HMM did not change the average length or flexibility of actin filaments, suggesting that the decrease in diffusion was not due to a HMM-induced change in the shape of filaments. Rather, slowing down of translational motion was caused by an increase in the volume of the diffusing complex. Surprisingly, the addition of ATP to acto-HMM accelerated the motion of actin filaments. The acceleration was the greatest at the low molar ratios of HMM:actin. Direct observation of filaments under an optical microscope showed that in the presence of ATP the average length of filaments did not change and that the filaments became stiffer, suggesting that acceleration of diffusion was not due to an ATP-induced increase in flexibility of filaments. These results show that some of the energy of splitting of ATP is impaired to actin filaments and suggest that 0.06 +/- 0.02 of HMM interferes with the diffusion of actin filaments during hydrolysis of ATP.

Actins↗

PubMed1992

Velocity of movement of actin filaments in in vitro motility assay. Measured by fluorescence correlation spectroscopy.

We have measured the velocity of actin filaments in in vitro motility assay by fluorescence correlation spectroscopy. In this method, one measures fluctuations in the number of filaments in an open sample volume. The number of filaments was calculated from measurements of fluorescence of rhodamine-phalloidin bound to F-actin. Sample volume was defined by a diaphragm placed in front of the photomultiplier. Fluctuations arise when actin filaments enter and leave the sample volume due to translations driven by mechanochemical interactions with myosin heads which are immobilized on a glass surface. The average velocity of the translation of filaments determined by the correlation method, (Vc), was equal to the diameter of the diaphragm divided by the half-time of the relaxation of fluctuations. The average number of moving filaments determined by correlation method, (Nc), was inversely proportional to the relative fluctuations. By the fluctuation method it was possible to determine the average velocity of over 800 moving filaments in less than 4 min. There was good agreement between (Vc) and (Nc) and the average velocity and the average number of moving filaments determined manually. To be able to apply correlation measurements to an experimental problem, neither (Vc) nor (Nc) must depend on the position of observation of filaments. We first confirmed that this was indeed the case. We then applied the method to investigate the dependence of motility on the ATPase activity of myosin heads. ATPase activity was varied by mixing intact heads with heads which were labeled with different thiol reagents. It was found that the motion was drastically influenced by the reagent used for modification. When the reagent was N-ethyl-maleimide, 1.5% modification was sufficient to completely inhibit the motion. When the reagent was 5-iodoacetamidofluorescein, motion declined hyperbolically with the fraction of modified heads.

Actins↗

PubMed1992

Distribution of actin filament lengths measured by fluorescence microscopy.

We analyzed the distribution of actin filament lengths by optical microscopy (OM). OM avoids possible alterations in the size or structure of actin filaments occurring during sample preparation for electron microscopy (EM). Images of F-actin labeled with tetramethylrhodamine isothiocyanate (TRITC)-phalloidin were analyzed for both size distribution and flexibility. In the standard buffer [25 mM potassium acetate, 4 mM MgSO4, 25 mM tris(hydroxymethyl)aminomethane acetate, pH 7.5, 20 mM beta-mercaptoethanol] filaments did not aggregate into bundles and remained stable at nanomolar concentrations for at least 1 h. At the same concentration, actin labeled directly with rhodamine (no phalloidin) formed unstable filaments whose average length decreased with time. The number average length of TRITC-phalloidin labeled filaments (Ln) was 4.90 microns, the ratio (rho) of the weight average length to the number average length was 2.06, and the correlation length (1/lambda) was 8.33 microns. These parameters were in good agreement with the values determined by EM for filaments shorter than 8 microns. Passing G-actin through a Sephadex G-150 column before polymerization did not have a significant effect on the distribution of lengths but made filaments more stiff (1/lambda = 12.5 microns). Millimolar concentration of ATP increased the correlation length, and gelsolin had the expected fragmenting effect on filaments. These results show that OM can be used as a fast and reliable method to analyze the distribution and flexibility of actin filaments and suggest that, in spite of extensive manipulation of actin filaments during sample preparation, EM is a valid tool for determination of size parameters of actin filaments.

Actins↗

PubMed1991

The myosin head can bind two actin monomers.

Force impulse is thought to be generated in muscle when myosin head (S-1), while weakly bound to actin filament, undergoes orientational change to form a strong (rigor) bond with actin. There is ample evidence that this bond involves interaction of 1 myosin head with 1 actin monomer. However, X-ray diffraction data of muscle decorated with S-1, as well as recently proposed model of the thin filaments, suggested that each S-1 molecule interacted with two actin monomers. We reinvestigated this controversy and found that the stoichiometry of acto-S-1 bond depended on the relative amounts of actin and myosin present during titrations: when increasing amounts of actin were added to a fixed amount of S-1 (i.e. when myosin heads were initially in excess over actin), the saturating stoichiometry was 1 mol of S-1 per 1 mol of actin. However, when increasing amounts of S-1 were added slowly to a fixed amount of F-actin (i.e. when actin was initially in excess over S-1), the stoichiometry at saturation was 1 mol of S-1 per 2 mols of actin. The ability of S-1 to bind either one or two actin monomers suggests a way that force could be generated during muscle contraction.

Actins↗

PubMed1991

Distribution of actin filament lengths and their orientation measured by gel electrophoresis in capillaries.

F-actin was electrophoresed in capillary tubes filled with agarose gel. The use of capillary imparted high resistance on the gel allowing the use of high enough concentration of salts to keep F-actin polymerized, and allowed the application of high electric fields without liberating considerable amount of heat. The intensity profile of the electrophoretic band of F-actin showed a peak, which in 1% agarose in the electric field of 17.8 V cm-1 at 0 degree C, migrated at 3.4 cm hr-1. Microscopic observation of actin filaments extracted from different positions along the gel showed that during electrophoresis filaments distributed themselves in such a manner that the longest polymers migrated slowest and the shortest migrated fastest. Using this observation we calculated the weight and number distributions of filament lengths from corresponding experimental intensity profiles. Phalloidin-labelled F-actin oriented in the gel upon application of an electric field. F-actin showed unusual orientational response: it oriented rapidly when the field was applied, but relaxed very slowly when the field was removed. Orientation of F-actin varied within an electrophoretic band, longest polymers showing the best orientation and short oligomers and monomers not orienting at all. The degree of orientation increased with the size of the electric field. When F-actin was labelled with phalloidin before electrophoresis, it was no longer able to migrate in the gel, but the electric field oriented it in the same way as when it was labelled after the electrophoresis. These results show that the electrophoresis of F-actin in agarose fractionates it according to its length, that by using electrophoresis it is possible to rapidly obtain distribution of filament lengths, and that F-actin migrates in agarose by the process of reptation.

Actins↗

PubMed1989

Differential behavior of two cysteine residues on the myosin head in muscle fibers.

We have previously shown that the orientation of (iodoacetamido)tetramethylrhodamine labels on SH1 thiol of S-1 moieties changes when MgADP is added to the fibers in rigor [Borejdo, J., Assulin, O., Ando, T., & Putnam, S. (1982) J. Mol. Biol. 158, 391-414. Burghardt, T.P., Ando, T., & Borejdo, J. (1983) Proc. Natl. Acad. Sci. U.S.A. 80, 7515-7519]. Here we report the results of experiments in which the SH2 of S-1 was labeled with maleimidorhodamine. The specificity of modification of thiols was checked by measuring the stoichiometry of attached dye, by determining the extent of the decrease in EDTA (K+)- and Ca2+-ATPase activities, and by the localization of the dyes on peptides containing SH1 and/or SH2. Labeled S-1 was diffused into single glycerinated fibers of rabbit psoas muscle, and the orientation of chromophores was measured by fluorescence detected dichroism. The dye attached to SH1 was oriented at 65 degrees with respect to the fiber axis in rigor and at 51 degrees in the presence of MgADP, regardless of whether SH2 was modified or not. The dye on SH2 was oriented near 42 degrees both in the presence and in the absence of ADP, regardless of whether SH1 was modified or not. Our results show that rhodamine oriented differently when attached to SH2 compared with when attached to SH1 and that in the former placement it was not sensitive to MgADP. We think this indicates that the SH2-containing region has a mobility different from that of the SH1-containing region, i.e., that this is evidence for internal flexibility of S-1.

Actins↗

PubMed1989

Electrophoresis and orientation of F-actin in agarose gels.

F-Actin was electrophoresed on agarose gels. In the presence of 2 mM MgCl2 and above pH 8.5 F-actin entered 1% agarose; when the electric field was 2.1 V/cm and the pH was 8.8, F-actin migrated through a gel as a single band at a rate of 2.5 mm/h. Labeling of actin with fluorophores did not affect its rate of migration, but an increase in ionic strength slowed it down. After the electrophoresis actin was able to bind phalloidin and heavy meromyosin (HMM) and it activated Mg2+-dependent ATPase activity of HMM. The mobility of F-actin increased with the rise in pH. Acto-S-1 complex was also able to migrate in agarose at basic pH, but at a lower rate than F-actin alone. The orientation of fluorescein labeled F-actin and of fluorescein labeled S-1 which formed rigor bonds with F-actin was measured during the electrophoresis by the fluorescence detected linear dichroism method. The former showed little orientation, probably because the dye was mobile on the surface of actin, but we were able to measure the orientation of the absorption dipole of the dye bound to S-1 which was attached to F-actin, and found that it assumed an orientation largely parallel to the direction of the electric field. These results show that actin can migrate in agarose gels in the F form and that it is oriented during the electrophoresis.

Actins↗

PubMed1989

Orientation of DNA in agarose gels.

An orientation of the lambda DNA during the electrophoresis in agarose gels was measured by a microscopic linear dichroism technique. The method involved staining the DNA with the dye ethidium bromide and measuring under the microscope the polarization properties of the fluorescence field around the electrophoretic band containing the nucleic acid. It was first established that the fluorescence properties of the ethidium bromide-DNA complex were the same in agarose gel and in a solution. Then the linear dichroism method was used to measure the dichroism of the absorption dipole of EB dye bound to lambda DNA. In a typical experiment the orientation of two-tenth of a picogram (2 x 10(-13)g) of DNA was measured. When the electric field was turned on, the dichroism developed rapidly and assumed a steady state value which increased with the strength of the field and with the size of DNA. A linear dichroism equation related the measured dichroism of fluorescence to the mean orientation of the absorption dipole of ethidium bromide and to an extent to which the orientation of this dipole deviated from the mean. The observed development of dichroism in the presence of an electric field was interpreted as an alignment of DNA along the direction of the field. The increase in the steady state value of dichroism with the rise in the strength of the field and with the increase of the size of DNA was interpreted as a better alignment of DNA along the direction of the field and as a smaller deviation from its mean orientation.

Bacteriophage lambda↗

PubMed1988

The orientation of DNA fragments in the agarose gels.

A microscopic method of measuring the orientation of nucleic acids in the agarose gels is described. A nucleic acid undergoing electrophoresis is stained with the dye ethidium bromide and is viewed under high magnification with a polarization microscope. A high-numerical-aperture microscope objective is used to illuminate and to collect the fluorescence signal, and therefore the orientation of the minute quantities of nucleic-acid can be measured: in a typical experiment we can detect the orientation of one-tenth of a picogram (10(13)g) of DNA. Polarization properties of the fluorescent light emitted by the separate bands corresponding to different molecular weights of the DNA are examined. A linear dichroism equation relates the measured fluorescence to the mean orientation of the absorption dipole of the ethidium bromide (and therefore DNA) and to the extent to which it is disorganized. As an example, we measured the orientation of phi X174 DNA RF/HaeIII fragments undergoing electrophoresis in a field of 10 V/cm. Ethidium bromide bound to the fragments with an angle of the absorption dipole largely perpendicular to the direction of the electrophoretic current. The dichroism declined as the molecular weight of the fragments decreased which is interpreted as an increase in the degree of disorder for shorter DNA.

DNA↗

PubMed1986

Interaction between actin and HMM.

It is shown that the interaction between actin and HMM results in a rapid precipitation of acto-HMM gel upon addition of MgATP. This is a simple demonstration of the idea that the formation of myosin filaments is not essential for mechanochemical reaction (muscle contraction) to occur and that the soluble myosin heads are competent to interact with actin to produce mechanical effect. Our findings also strongly support earlier suggestion that each head of one HMM molecule is able to bind to a different actin filament.

Actins↗

PubMed1986

Actin-attached and detached crossbridges in myofibrils: segregation into two populations according to their sensitivity to proteolytic digestion of myosin heavy chain.

Tryptic digestion of myofibrils was used to assess the interaction of crossbridges with thin filaments in the presence of ATP analogues. The relative amounts of 200 kDa fragment produced by trypsin from myosin heavy chain when the crossbridge is attached to actin, and of 160 kDa fragment produced when the crossbridge is detached from actin, served as a measure of crossbridge-actin interaction. In rigor only the 200 kDa fragment was produced suggesting that a great majority of the crossbridges were strongly attached to actin; in the presence of MgPPi at 0 degrees C only the 160 kDa fragment was finally produced suggesting that eventually all crossbridges detached from actin. In the presence of MgPPi or MgAMPPNP at 25 degrees C both 200 and 160 kDa fragments were present for several minutes after myosin heavy chain had been completely digested, suggesting that two populations of crossbridges (attached and detached) co-existed at the same time within the myofibril. It is concluded that the addition of ATP analogues to muscle does not simply affect the chemical equilibrium of binding of myosin heads to actin but that it causes rapid dissociation of one crossbridge population without significant effect on binding to actin of the remaining crossbridge population.

Actins↗

PubMed1985

The rate of MgADP binding to and dissociation from acto-S1.

The rate of binding and dissociation of MgADP from its ternary complex with actin and S1 was measured by following the extent to which fixed concentrations of MgADP slow down MgATP-induced dissociation of acto-S1. The solution of the equations describing this process shows that at any MgADP concentration the apparent rate of acto-S1 dissociation should be proportional to a square root of the equilibrium constant for MgADP dissociation and to MgATP concentration. By measuring the apparent rate of acto-S1 dissociation as a function of MgATP concentration, the rate of MgADP binding and dissociation were determined as 5 X 10(6) M-1 X s-1 and 1400 s-1, respectively. These rates were unchanged by modification of SH1 thiol of S1 by a variety of fluorescence and spin-labels, but dissociation rate was drastically reduced when SH1 was labelled with 5-iodoacetamidofluorescein.

Actins↗

PubMed1984

Hydrophobic interaction chromatography of myosin fragments: potential use in purification.

Myosin fragments were fractionated on columns of the hydrophobic gel phenyl-Sepharose CL-4B. In the presence of high NaCl concentrations the fragments bound tightly to the columns; they could be eluted by decreasing the ionic strength, by increasing the pH, or by applying various concentrations of ethylene glycol. In myosin subfragment-1 (S-1), the light chains underwent partial dissociation from the heavy chain and bound separately to the column matrix. The order of strength of binding of the various species to the column was heavy chain greater than A1 light chain greater than A2 light chain greater than native S-1 greater than denatured heavy chain or S-1. Thus the hydrophobic gel appears to be able to differentiate between enzymatically active and inactive S-1. Under appropriate elution conditions it was possible to obtain S-1 preparations depleted from nicked heavy chains and with specific ATPase activities 34-130% higher than those of untreated S-1. When S-1 (A2) was fractionated on phenyl-Sepharose a fivefold enrichment of the heavy chain with respect to the light chains was obtained, while the ATPase activity was equal or larger than that of the original S-1, implying that the light chains are not essential for ATPase activity. Thus, it seems that chromatography of S-1 on phenyl-Sepharose is a potentially useful method for obtaining a purified myosin heavy-chain fragment with a high ATPase specific activity.

Adenosine Triphosphatases↗

PubMed1984

Crossbridge order and orientation in resting single glycerinated muscle fibres studied by linear dichroism of bound rhodamine labels.

Linear dichroism of iodoacetyl-rhodamine labels attached to the highly reactive thiol of the myosin heads was measured in order to infer the spatial orientation and the degree of order in myosin crossbridges in single glycerinated rabbit psoas fibres at rest. We have previously shown that in rigor the chromophoric labels are well ordered and that in the presence of MgADP and during isometric contraction a large fraction of probes is also ordered but at an attitude different from that of rigor. Here we show that in relaxed muscle the probe order is dependent on total ionic strength: at and above 0.180 M there is little evidence for any preferred probe orientation, implying a high degree of crossbridge disorder. Below 0.160 M there is progressively more order with decreasing ionic strength down to 0.100 M, below which no measurements could be taken at room temperature (because the fibres would not relax). The dichroism observed under these conditions resembles that of the rigor state in that the dichroism peaks at the same polarization of excitation light, implying that the average probe attitude relative to the fibre axis is larger than 54.7 degrees. Stretching the muscle beyond the point of overlap between actin- and myosin-containing filaments does not affect the ionic strength dependence of the amount of order present in relaxed muscle, suggesting that the observed order is due to ionic interactions of crossbridges with the thick filament surface.

Animals↗

PubMed1984

Electrophoresis in the presence of Coomassie brilliant blue R-250 stains polyacrylamide gels during protein fractionation.

A method of staining polyacrylamide gels in which the dye is electrophoresed together with the sample is proposed. The method cuts short and simplifies the conventional electrophoresis procedure by eliminating the separate poststaining step. In the gels run in the presence of sodium dodecyl sulfate, the method produces protein staining patterns which are quantitatively identical to the ones obtained by conventional staining procedure. Additional advantages of the method are easy control over the degree of staining and homogenous staining independent of the gel thickness and concentration of the dye.

Electrophoresis, Polyacrylamide Gel↗