Shigeru Chaen

Comparison of Unitary Displacements and Forces Between 2 Cardiac Myosin Isoforms by the Optical Trap Technique: Molecular Basis for Cardiac Adaptation

To provide information on the mechanism of cardiac adaptation at the molecular level, we compared the unitary displacements and forces between the 2 rat cardiac myosin isoforms, V1 and V3. A fluorescently labeled actin filament, with a polystyrene bead attached, was caught by an optical trap and brought close to a glass surface sparsely coated with either of the 2 isoforms, so that the actin-myosin interaction took place in the presence of a low concentration of ATP (0.5 micromol/L). Discrete displacement events were recorded with a low trap stiffness (0.03 to 0.06 pN/nm). Frequency distribution of the amplitude of the displacements consisted of 2 gaussian curves with peaks at 9 to 10 and 18 to 20 nm for both V1 and V3, suggesting that 9 to 10 nm is the unitary displacement for both isoforms. The duration of the displacement events was longer for V3 than for V1. On the other hand, discrete force transients were recorded with a high trap stiffness (2.1 pN/nm), and their amplitude showed a broad distribution with mean values between 1 and 2 pN for V1 and V3. The durations of the force transients were also longer for V3 than for V1. These results indicate that both the unitary displacements and forces are similar in amplitude but different in duration between the 2 cardiac myosin isoforms, being consistent with the reports that the tension cost is higher in muscles consisting mainly of V1 than those consisting mainly of V3.

Carp expresses fast skeletal myosin isoforms with altered motor functions and structural stabilities to compensate for changes in environmental temperature

1. 1. Myosin and its subfragment-1 (Sl) from carp acclimated to 10°C showed higher actin-activated Mg2+-ATPase activity and lower thermostability than their counterparts from carp acclimated to 30°C. Accordingly, filament velocity for the 10°C-acclimated carp myosin was higher at any measuring temperatures from 3 to 23°C than that for the 30°C-acclimated carp myosin. 2. 2. Three types of cDNA clones encoding myosin heavy chains were isolated from thermally acclimated carp. The 10 and 30°C types were predominating in carp acclimated to 10 and 30°C, respectively, whereas the intermediate type was found as a minor component in the 10°C-acclimated carp with an intermediate feature in both DNA nucleotide and deduced amino acid sequences between those of the 10 and 30°C types. 3. 3. The three types of myosin rod all showed a typical coiled-coil structure of α-helices. DSC scans demonstrated that myosin rod prepared from carp acclimated to 10°C had a lower thermostability than that from carp acclimated to 30°C, showing that low thermostability in cold-acclimated carp myosin prevails over the entire molecule. 4. 4. cDNA clones encoding myosin alkali light chains were isolated from thermally acclimated carp. Northern blot analysis showed that the ratios of LC3LC1 mRNAs were significantly higher (3.92) in the 30°C- than 10°C-acclimated (3.10) carp.

Direct demonstration of the cross-bridge recovery stroke in muscle thick filaments in aqueous solution by using the hydration chamber

Despite >50 years of research work since the discovery of sliding filament mechanism in muscle contraction, structural details of the coupling of cyclic cross-bridge movement to ATP hydrolysis are not yet fully understood. An example would be whether lever arm tilting on the myosin filament backbone will occur in the absence of actin. The most direct way to elucidate such movement is to record ATP-induced cross-bridge movement in hydrated thick filaments. Using the hydration chamber, with which biological specimens can be kept in an aqueous environment in an electron microscope, we have succeeded in recording ATP-induced cross-bridge movement in hydrated thick filaments consisting of rabbit skeletal muscle myosin, with gold position markers attached to the cross-bridges. The position of individual cross-bridges did not change appreciably with time in the absence of ATP, indicating stability of time-averaged cross-bridge mean position. On application of ATP, individual cross-bridges moved nearly parallel to the filament long axis. The amplitude of the ATP-induced cross-bridge movement showed a peak at 5–7.5 nm. At both sides of the filament bare region, across which the cross-bridge polarity was reversed, the cross-bridges were found to move away from, but not toward, the bare region. Application of ADP produced no appreciable cross-bridge movement. Because ATP reacts rapidly with the cross-bridges (M) to form complex (M·ADP·Pi) with an average lifetime >10 s, the observed cross-bridge movement is associated with reaction, M + ATP → M·ADP·Pi. The cross-bridges were observed to return to their initial position after exhaustion of ATP. These results constitute direct demonstration of the cross-bridge recovery stroke.

Measurement of work done by ATP-induced sliding between rabbit muscle myosin and algal cell actin cables in vitro

1. The basic properties of the ATP‐dependent actin‐myosin interaction responsible for muscle contraction were studied using an in vitro force‐movement assay system, in which a glass microneedle coated with rabbit skeletal muscle myosin was made to slide on the actin filament arrays (actin cables) in the internodal cell of an alga Nitellopsis obtusa with ionophoretic application of ATP. 2. In response to an ATP current pulse (intensity, 5‐85 nA; duration, 0.5‐10 s), the myosin‐coated needle moved for a distance and eventually stopped, indicating reformation of rigor actin‐myosin linkages to prevent elastic recoil of the bent needle. A subsequent ATP current pulse again produced the needle movement starting from the baseline force attained by the preceding needle movement. 3. With a constant amount of ATP application, the amount of work done by the ATP‐induced actin‐myosin sliding first increased with increasing baseline force from zero to 0.4‐0.6P0, and then decreased with further increasing baseline force, thus giving a bell‐shaped work versus baseline force relation. 4. With increasing amount of ATP application, the amount of work done by the actin‐myosin sliding increased more steeply as the baseline force was increased from zero to 0.4‐0.6P0. 5. These results are discussed in connection with the basic properties of the actin‐myosin sliding in muscle contraction.

Force–velocity relationships in actin–myosin interactions causing cytoplasmic streaming in algal cells

SUMMARY Cytoplasmic streaming in giant internodal cells of green algae is caused by ATP-dependent sliding between actin cables fixed on chloroplast rows and cytoplasmic myosin molecules attached to cytoplasmic organelles. Its velocity (≥50 μm s-1) is many times larger than the maximum velocity of actin–myosin sliding in muscle. We studied kinetic properties of actin–myosin sliding causing cytoplasmic streaming in internodal cell preparations of Chara corallina, into which polystyrene beads, coated with cytoplasmic myosin molecules, were introduced. Constant centrifugal forces directed opposite to the bead movement were applied as external loads. The steady-state force–velocity (P–V) curves obtained were nearly straight, irrespective of the maximum isometric force generated by cytoplasmic myosin molecules, indicating a large duty ratio of cytoplasmic myosin head. The large velocity of cytoplasmic streaming can be accounted for, at least qualitatively, by assuming a mechanically coupled interaction between cytoplasmic myosin heads as well as a large distance of unitary actin–myosin sliding.

Different cardiac myosin isoforms exhibit equal force-generating ability in vitro

We measured forces generated by myosin molecules and a single actin filament using an optical trap system. The force per unit length of actin filament did not differ significantly between cardiac myosin isoforms. V1 and V3. This indicates that the ability to generate force is equal between V1 and V3, despite their difference in the unloaded sliding velocity past actin.

FORCE-VELOCITY RELATIONS OF RAT CARDIAC MYOSIN ISOZYMES SLIDING ON ALGAL CELL ACTIN CABLES IN VITRO

The difference in kinetic properties between two myosin isozymes (V1 and V3) in rat ventricular myocardium was studied by determining the steady-state force-velocity (P-V) relations in the ATP-dependent movement of V1 and V3-coated polystyrene beads on actin cables of giant algal cells mounted on a centrifuge microscope. The maximum unloaded velocity of bead movement was larger for V1 than for V3. The velocity of bead movement decreased with increasing external load applied by the centrifuge microscope, and eventually reached zero when the load was equal to the maximum isometric force (P0) generated by the myosin heads. The maximum isometric force P0 was less than 10 pN, and did not differ significantly between V1 and V3. The P-V curves consisted of a hyperbolic part in the low force range and a non-hyperbolic part in the high force range. The critical force above which the curve deviated from the hyperbola was much smaller for V1 than for V3. An analysis using a model with an extremely small number of myosin heads involved in the bead movement suggested a marked difference in kinetic properties between V1 and V3.

A Point Mutation in the SH1 Helix Alters Elasticity and Thermal Stability of Myosin II

Movement generated by the myosin motor is generally thought to be driven by distortion of an elastic element within the myosin molecule and subsequent release of the resulting strain. However, the location of this elastic element in myosin remains unclear. The myosin motor domain consists of four major subdomains connected by flexible joints. The SH1 helix is the joint that connects the converter subdomain to the other domains, and is thought to play an important role in arrangements of the converter relative to the motor. To investigate the involvement of the SH1 helix in elastic distortion in myosin, we have introduced a point mutation into the SH1 helix of Dictyostelium myosin II (R689H), which in human nonmuscle myosin IIA causes nonsyndromic hereditary deafness, DFNA17. The mutation resulted in a significant impairment in motile activities, whereas actin-activated ATPase activity was only slightly affected. Single molecule mechanical measurements using optical trap showed that the step size was not shortened by the mutation, suggesting that the slower motility is caused by altered kinetics. The single molecule measurements demonstrated that the mutation significantly reduced cross-bridge stiffness. Motile activities produced by mixtures of wild-type and mutant myosins also suggested that the mutation affected the elasticity of myosin. These results suggest that the SH1 helix is involved in modulation of myosin elasticity, presumably by modulating the converter flexibility. Consistent with this, the mutation was also shown to reduce thermal stability and induce thermal aggregation of the protein, which might be implicated in the disease process.

Enhancement of Force Generated by Individual Myosin Heads in Skinned Rabbit Psoas Muscle Fibers at Low Ionic Strength

Although evidence has been presented that, at low ionic strength, myosin heads in relaxed skeletal muscle fibers form linkages with actin filaments, the effect of low ionic strength on contraction characteristics of Ca2+-activated muscle fibers has not yet been studied in detail. To give information about the mechanism of muscle contraction, we have examined the effect of low ionic strength on the mechanical properties and the contraction characteristics of skinned rabbit psoas muscle fibers in both relaxed and maximally Ca2+-activated states. By progressively decreasing KCl concentration from 125 mM to 0 mM (corresponding to a decrease in ionic strength μ from 170 mM to 50 mM), relaxed fibers showed changes in mechanical response to sinusoidal length changes and ramp stretches, which are consistent with the idea of actin-myosin linkage formation at low ionic strength. In maximally Ca2+-activated fibers, on the other hand, the maximum isometric force increased about twofold by reducing KCl concentration from 125 to 0 mM. Unexpectedly, determination of the force-velocity curves indicated that, the maximum unloaded shortening velocity Vmax, remained unchanged at low ionic strength. This finding indicates that the actin-myosin linkages, which has been detected in relaxed fibers at low ionic strength, are broken quickly on Ca2+ activation, so that the linkages in relaxed fibers no longer provide any internal resistance against fiber shortening. The force-velocity curves, obtained at various levels of steady Ca2+-activated isometric force, were found to be identical if they are normalized with respect to the maximum isometric force. The MgATPase activity of muscle fibers during isometric force generation was found not to change appreciably at low ionic strength despite the two-fold increase in Ca2+-activated isometric force. These results can be explained in terms of enhancement of force generated by individual myosin heads, but not by any changes in kinetic properties of cyclic actin-myosin interaction.

Distinct kinetic properties of cardiac myosin isoforms revealed by in vitro studies.

To clarify the physiological significance of myosin isoform redistribution in cardiac adaptation process, we compared the kinetic property of the two cardiac myosin isoforms using in vitro motility assay techniques. Cardiac myosin isoforms V1 and V3 were obtained from ventricular muscle of young rats and hypothyroid rats respectively. On each of these myosin isoforms fixed on a glass coverslip, fluorescently labeled actin filaments were made to slide in the presence of ATP. To measure the force generated by actomyosin interaction, a small latex bead was attached to the barbed end of an actin filament and the bead was captured by the laser optical trap installed in a microscope. The force was determined from the distance between the bead and the trap positions under either auxotonic or isometric conditions. The time-averaged force generated by multiple cross-bridges did not differ significantly between the two isoforms. On the other hand, the unitary force measurement revealed the same level of amplitude but a longer duration for V3 isoform. The same level of time-averaged force is in agreement with not only our previous finding but the results of maximum force measurement in muscle preparations. The difference in kinetic characteristics of the two isoforms could account for the difference in economy of force development and the basis for cardiac adaptation mechanism.