Biomedical subjects

J Borejdo

Publications and source records attributed to J Borejdo.

At least 37 records · Page 2Linked to original sources

PubMed1995

Rigor cross-bridges bind to two actin monomers in thin filaments of rabbit psoas muscle.

The mode of binding of myosin subfragment-1 (S1) to actin is known to depend on their molar ratio: when actin is in excess, S1 binds to two actin monomers within the actin filament, and when S1 is in excess or is equimolar with actin, each S1 binds to one actin monomer. Since in vertebrate striated muscle actin is in molar excess over myosin, we expect that in fibers each myosin head binds to two actin monomers. To test this idea, we compared the conformation of the heads in native muscle with the conformation of S1 in fibers that were loaded with either high (S1 equimolar with actin) or low (excess of actin over S1) concentration of extrinsic S1. Conformation was assessed by the accessibility of heads to trypsin (measured by the rate of trypsinolysis) and by their orientation with respect to the muscle axis (measured by a combination of polarization of fluorescence and linear dichroism). In muscle fibers loaded with a high concentration of S1, the region of the heavy chain of the myosin head at the junction of 20 and 50 kDa proteolytic fragments was readily digested by trypsin and its orientation was approximately perpendicular to an axis of a thin filament. In contrast, when muscle fibers were loaded with a low concentration of S1, the 20/50 kDa junction of S1 was protected from trypsinolysis and its orientation was more parallel with a filament axis. Native muscle in rigor behaved like muscle irrigated with a low concentration of S1, i.e. the 20/50 kDa junction of the myosin head was protected from trypsinolysis and the orientation of the heads was parallel to the filament axis. We conclude that in rigor rabbit psoas muscle each myosin head binds to two actin monomers in a thin filament, and that this binding is different from the binding of S1 to actin in equimolar solutions.

Actins↗

PubMed1995

Fluorescence polarization study of the rigor complexes formed at different degrees of saturation of actin filaments with myosin subfragment-1.

A serine residue located in the active site of myosin head (S1) was labelled by 9-anthroylnitrile, an amino group located in the central domain of S1 was labelled by 7-diethylamino-3-(4'-isothio-cyanato-phenyl)-4-methylcoumari n, a cysteine residue located near the C-terminus of S1 was labelled by 5-[2-((iodoacetyl)-amino)ethyl]-amino-naphthalene-1-sulfonic acid (1,5-IAEDANS) and a cysteine residue located near the C-terminus of the alkali light chain 1 was labelled with iodoacetamido-tetramethyl-rhodamine. Polarization of fluorescence of S1 was measured in solution (where it indicated the mobility of actin-bound S1) and in myofibrils (where it indicated orientation of probes) to check whether the anisotropy of S1 labelled at different positions depended on the molar ratio S1:actin. In solution, when increasing amounts of actin were added to a fixed amount of labelled S1 (i.e. when myosin heads were initially in excess over actin), anisotropy saturated at 1 mol of S1 per 1 mol of actin. When increasing amounts of S1 were added to a fixed amount of F-actin (i.e. when actin was initially in excess over S1), the anisotropy saturated at 1 mol of S1 per 2 mols of actin. In myofibrils, orientation of S1 was different when S1 was added at nanomolar concentration (intrinsic actin was in excess over extrinsic S1) then when it was added at micromolar concentration (excess of S1 over actin). The fact that the anisotropy of S1 labelled at different positions depended on the molar ratio excluded the possibility that changes were confined to one part of the cross-bridge and supports our earlier proposal that the two rigor complexes which S1 can form with F-actin differ globally in conformation.

Actins↗

PubMed1994

Orientation of actin filaments during motion in in vitro motility assay.

Rhodamine-phalloidin was added to F-actin, and the orientation of transition dipoles of the dye was measured in single actin filaments by polarization of fluorescence. Rhodamine-phalloidin was well immobilized on the surface of actin, indicating that changes in orientation of the dye reported changes in orientation of actin monomers. In stationary filaments the dipoles were inclined at 49.3 degrees with respect to the filament axis. The disorganization of dipoles in stationary filaments was insignificant. When the filaments were made to translate, the average orientation of the dye did not change, but disorganization slightly increased. Disorganization increased significantly when filaments were free in solution. We concluded that, within the accuracy of our measurements (approximately 18%), actin monomers did not undergo major reorientations during motion, but that binding of myosin heads deformed the structure of filaments.

Actins↗

PubMed1993

Structure of the 265-kilodalton complex formed upon EDC cross-linking of subfragment 1 to F-actin.

The conventional model of force generation in muscle requires the presence of at least two different contact areas between the myosin head (S1) and the actin filament. It has been found that S1 has two sites available for carbodiimide cross-linking, but it is generally believed that the myosin head can be cross-linked to only one actin through either site. We provide here, for the first time, evidence that one S1 can be cross-linked to two separate actin molecules. The covalent complex of one S1 with two actins was found to have an apparent molecular mass of 265 kDa. The formation of the 265-kDa acto-S1 complex was strongly dependent on the ratio of S1 to actin. Limited tryptic digestion converted the 265-kDa product into the 240-kDa complex by releasing a 27-kDa N-terminal S1 fragment. Limited subtilisin digestion of the 265-kDa covalent acto-S1 complex yielded 29-, 93-, and 66-kDa peptides which corresponded to the 29-kDa N-terminal domain of S1, actin-44-kDa (central domain of S1) and actin-22-kDa (C-terminal domain of S1) complexes, respectively. These peptides could be generated only if a single S1 has been cross-linked to two separate actins. The 265-kDa acto-S1 complex (S1:actin ratio = 0.5) had 60% of the ATPase activity of the 175-185-kDa acto-S1 complex (S1:actin ratio = 1).(ABSTRACT TRUNCATED AT 250 WORDS)

Actins↗

PubMed1993

Two different rigor complexes of myosin subfragment 1 and actin.

Our previous titration and cross-linking experiments showed that myosin subfragment 1 (S1) can bind to one or two monomers in F-actin [Andreev, O. A., & Borejdo, J. (1991) Biochem. Biophys. Res. Commun. 177, 350-356; (1992a) J. Muscle Res. Cell Motil. 13, 523-533; (1992b) Biochem. Biophys. Res. Commun. 188, 94-101]. In the present work we used a sedimentation method to extend these studies to equilibrium binding and a stopped flow method to investigate its kinetics. Both equilibrium and kinetic data indicated the existence of two different rigor complexes. On the basis of these data we developed a model which suggested that binding of S1 to F-actin occurred in two steps: (i) initial rapid binding to one monomer of F-actin, A + M<==>A.M and (ii) a consequent slow binding to a neighboring monomer, A.M + A<==>A.M.A, where A stands for actin and M for myosin subfragment 1. The second reaction can proceed only if the neighboring actin site is unoccupied. The model fit the equilibrium and kinetic binding data with equilibrium constants K1 = 6 x 10(6) M-1 and K2 = 4 and kinetic constants k+1 = 10.5 x 10(6) M-1 s-1, k-1 = 1.75 s-1, k+2 = 0.8 s-1, and k-2 = 0.2 s-1, where the subscripts refer to the reactions i and ii. These results corroborate our hypothesis that myosin head can make two types of complexes with F-actin and support our speculation that during a power stroke in contracting muscle a myosin head may first bind to one and then to two actins.

Actins↗

PubMed1993

Measuring orientation of actin filaments within a cell: orientation of actin in intestinal microvilli.

Orientational distribution of actin filaments within a cell is an important determinant of cellular shape and motility. To map this distribution we developed a method of measuring local orientation of actin filaments. In this method actin filaments within cells are labeled with fluorescent phalloidin and are viewed at high magnification in a fluorescent microscope. Emitted fluorescence is split by a birefringent crystal giving rise to two images created by light rays polarized orthogonally with respect to each other. The two images are recorded by a high-sensitivity video camera, and polarization of fluorescence at any point is calculated from the relative intensity of both images at this point. From the value of polarization, the orientation of the absorption dipole of the dye, and thus orientation of F-actin, can be calculated. To illustrate the utility of the method, we measured orientation of actin cores in microvilli of chicken intestinal epithelial cells. F-actin in microvillar cores was labeled with rhodamine-phalloidin; measurements showed that the orientation was the same when microvillus formed a part of a brush border and when it was separated from it suggesting that "shaving" of brush borders did not distort microvillar structure. In the absence of nucleotide, polarization of fluorescence of actin cores in isolated microvilli was best fitted by assuming that a majority of fluorophores were arranged with a perfect helical symmetry along the axis of microvillus and that the absorption dipoles of fluorophores were inclined at 52 degrees with respect to the axis. When ATP was added, the shape of isolated microvilli did not change but polarization of fluorescence decreased, indicating statistically significant increase in disorder and a change of average angle to 54 degrees. We argue that these changes were due to mechanochemical interactions between actin and myosin-I.

Actins↗

PubMed1993

Polarization of fluorescently labeled myosin subfragment-1 fully or partially decorating muscle fibers and myofibrils.

Fluorescently labeled myosin heads (S1) were added to muscle fibers and myofibrils at various concentrations. The orientation of the absorption dipole of the dye with respect to the axis of F-actin was calculated from polarization of fluorescence which was measured by a novel method from video images of muscle. In this method light emitted from muscle was split by a birefringent crystal into two nonoverlapping images: the first image was created with light polarized in the direction parallel to muscle axis, and the second image was created with light polarized in the direction perpendicular to muscle axis. Images were recorded by high-sensitivity video camera and polarization was calculated from the relative intensity of both images. The method allows measurement of the fluorescence polarization from single myofibril irrigated with low concentrations of S1 labeled with dye. Orientation was also measured by fluorescence-detected linear dichroism. The orientation was different when muscle was irrigated with high concentration of S1 (molar ratio S1:actin in the I bands equal to 1) then when it was irrigated with low concentration of S1 (molar ratio S1:actin in the I bands equal to 0.32). The results support our earlier proposal that S1 could form two different rigor complexes with F-actin depending on the molar ratio of S1:actin.

Actins↗

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↗