Search PubMed⌕ Search

Biomedical subjects

S Ishiwata

Publications and source records attributed to S Ishiwata.

At least 109 records · Page 6Linked to original sources
PubMed1992

Regulation of tension development by MgADP and Pi without Ca2+. Role in spontaneous tension oscillation of skeletal muscle.

The length of sarcomeres in isolated myofibrils fixed at both ends spontaneously oscillates when MgADP and Pi coexist with MgATP in the absence of Ca2+ (Okamura, N., and S. Ishiwata, 1988. J. Muscle Res. Cell. Motil. 9:111-119). Here, we report that MgADP and Pi function as an activator and an inhibitor, respectively, of tension development of single skeletal muscle fibers in the absence of Ca2+ and the coexistence of MgADP and Pi with MgATP induces spontaneous tension oscillation. First, the isometric tension sharply increased when the concentration of MgADP became higher than approximately 3x that of MgATP and saturated at approximately 90% of the tension obtained under full Ca2+ activation; in parallel with this sigmoidal increase of tension, MgATPase activity appeared. The inhibition of contraction by the regulatory system seems to be desuppressed by the allosteric effect of actomyosin-ADP complex, similarly to so-called rigor complex. The ADP-induced tension was decreased along a reversed sigmoidal curve by the addition of Pi; actomyosin-ADP-Pi complex, which has no desuppression function, may be formed by exogenous Pi; accompanying the decline of tension, spontaneous oscillations of tension and sarcomere length appeared. It is suggested that the length oscillation of each (half) sarcomere would occur through the transition of cross-bridges between force-generating (on) and non-force-generating (off) states, which may be regulated by the mechanical states (strain) of cross-bridges and/or thin filaments.

Adenosine Diphosphate↗
PubMed1992

Spontaneous oscillation of tension and sarcomere length in skeletal myofibrils. Microscopic measurement and analysis.

We have devised a simple method for measuring tension development of single myofibrils by micromanipulation with a pair of glass micro-needles. The tension was estimated from the deflection of a flexible needle under an inverted phase-contrast microscope equipped with an image processor, so that the tension development is always accompanied by the shortening of the myofibril (auxotonic condition) in the present setup. The advantage of this method is that the measurement of tension (1/30 s for time resolution and about 0.05 micrograms for accuracy of tension measurement; 0.05 microns as a spatial resolution for displacement of the micro-needle) and the observation of sarcomere structure are possible at the same time, and the technique to hold myofibrils, even single myofibrils, is very simple. This method has been applied to study the tension development of glycerinated skeletal myofibrils under the condition where spontaneous oscillation of sarcomeres is induced, i.e., the coexistence of MgATP, MgADP and inorganic phosphate without free Ca2+. Under this condition, we found that the tension of myofibrils spontaneously oscillates accompanied by the oscillation of sarcomere length with a main period of a few seconds; the period was lengthened and shortened with stretch and release of myofibrils. A possible mechanism of the oscillation is discussed.

Animals↗
PubMed1992

Diagnostic use of anti-modified nucleoside monoclonal antibody.

By use of monoclonal antibodies (MoAbs) termed APU-6 and AMA-2, we determined the usefulness of urinary modified nucleosides, pseudouridine and 1-methyladenosine, as markers for malignancy. In patients with leukemia and other forms of cancer, these nucleosides elevated significantly and reflected the disease status of patients. The immunohistochemical analysis showed that cancer cells were specifically stained with the MoAbs. Chemical identification of the cellular components reactive with the MoAbs revealed that APU-6-associated antigens were mainly rRNA and AMA-2-associated antigens were mainly tRNA. These results suggest that APU-6 and AMA-2 would be useful tools for clinical and biological studies of cancer.

Adenosine↗
PubMed1991

Spontaneous oscillatory contraction (SPOC) of sarcomeres in skeletal muscle.

Skeletal myofibrils spontaneously oscillate under a condition where ATP, ADP, and Pi coexist and the concentration of free Ca2+ is less than about 1 microM. Although this oscillation phenomenon called SPOC is apparently simple, the molecular mechanism seems to be complex. The SPOC condition and the space-time pattern of SPOC wave suggest that the dynamics of association and dissociation of Pi (ADP) is regulated by the mechanical strain imposed on actin and myosin; the enzymatic activity (ATPase) of actomyosin complex and the mechanical event (contraction) are thus coupled to each other. In this sense, the nature of the mechanochemical enzyme, actomyosin ATPase, is revealed in SPOC.

Adenosine Diphosphate↗
PubMed1991

Dual-view microscopy with a single camera: real-time imaging of molecular orientations and calcium.

A new microscope technique, termed "W" (double view video) microscopy, enables simultaneous observation of two different images of an object through a single video camera or by eye. The image pair may, for example, be transmission and fluorescence, fluorescence at different wavelengths, or mutually perpendicular components of polarized fluorescence. Any video microscope can be converted into a dual imager by simple insertion of a small optical device. The continuous appearance of the dual image assures the best time resolution in existing and future video microscopes. As an application, orientations of actin protomers in individual, moving actin filaments have been imaged at the video rate. Asymmetric calcium influxes into a cell exposed to an intense electric pulse have also been visualized.

Actin Cytoskeleton↗
PubMed1991

[Natural history of 82 patients with hypertrophic cardiomyopathy: follow-up for over ten years].

The natural courses of 82 patients with hypertrophic cardiomyopathy (HCM) were investigated in follow-up periods of over 10 years (mean follow-up: 11.7 yrs.). Twelve patients had obstructive, 30 non-obstructive and 40 apical HCM. There were 76 males and 6 females. The mean age at the initial diagnosis was 48 years. All patients underwent cardiac catheterization and left ventriculography, and two-dimensional echocardiography was conducted in some patients. To determine the clinical features influencing the prognosis, their serial laboratory and clinical data were reviewed and analyzed. Five patients died of non-cardiac causes. Only one died suddenly. Congestive heart failure developed in 3 patients, 2 with obstructive and one with non-obstructive HCM. Two patients had cavity dilatation and deteriorated ventricular function, and finally exhibited dilated cardiomyopathy-like features. Characteristically, in this deteriorating group, a decrease in the QRS voltage and an abnormal Q wave gradually developed without clinical evidence of myocardial infarction. Two patients with apical HCM in this group had decreases in their QRS voltages and in the depths of their giant negative T waves. They developed apical left ventricular asynergy without myocardial infarction or congestive heart failure. There were no specific clinical or laboratory parameters predictive of sudden death. Atrial fibrillation occurred in 9 patients, resulting in 3 cases of cerebral infarction, one myocardial infarction, and one congestive heart failure. One patient received pacemaker implantation because of the sick sinus syndrome. Three had acute myocardial infarction. Aortocoronary bypass grafting was performed in 3 patients. These results indicate that the good long-term life prognosis of HCM can be expected in all types of HCM. Among the 82 patients, only one died suddenly. However, since the natural history of HCM can take a variety of courses, careful observation is necessary.

Atrial Fibrillation↗
PubMed1990

Elastic filaments in skeletal muscle revealed by selective removal of thin filaments with plasma gelsolin.

Muscle needs an elastic framework to maintain its mechanical stability. Removal of thin filaments in rabbit skeletal muscle with plasma gelsolin has revealed the essential features of elastic filaments. The selective removal of thin filaments was confirmed by staining with phalloidin-rhodamine for fluorescence microscopy, examination of arrowhead formation with myosin subfragment 1 by electron microscopy, and analysis by SDS-PAGE. Thin section electron microscopy revealed the elastic fine filaments (approximately 4 nm in diameter) connecting thick filaments and the Z line. After removal of thin filaments, both rigor stiffness and active tension generation were lost, but the resting tension remained. These observations indicate that the thin filament-free fibers maintain a framework composed of the serial connections of thick filaments, the elastic filaments, and the Z line, which gives passive elasticity to the contractile system of skeletal muscle. The resting tension that remained in the thin filament-free fibers was decreased by mild trypsin treatment. The only protein component that was digested in parallel with the decrease in the resting tension and the disappearance of the elastic filaments was alpha-connectin (also called titin 1), which was transformed from the alpha to the beta form (from titin 1 to 2, respectively). Thus, we conclude that the main protein component of the elastic filaments is alpha-connectin (titin 1).

Actin Cytoskeleton↗
PubMed1989

Diffraction rings obtained from a suspension of skeletal myofibrils by laser light illumination. Study of internal structure of sarcomeres.

Diffraction rings corresponding to the first, second, and third order were obtained by laser light illumination from a suspension of rabbit glycerinated psoas myofibrils (diameter, 1-2 microns; average length of the straight region, 44 microns; average sarcomere length, 2.2-2.6 microns) of which the optical thickness was appropriately chosen. Dispersed myofibrils were nearly randomly oriented in two dimensions, so that the effects of muscle volume were minimized; these effects usually interfere significantly with a quantitative analysis of laser optical diffraction in the fiber system. The diameters of diffraction rings represented the average sarcomere length. By using this system, we confirmed the ability of the unit cell (sarcomere) structure model to explain the intensity change of diffraction lines accompanying the dissociation from both ends of thick filaments in a high salt solution. The length of an A-band estimated from the relative intensity of diffraction rings and that directly measured on phase-contrast micrographs coincided well with each other. Also, we found that myofibrils with a long sarcomere length shorten to a slack length accompanying the decrease in overlap between thick and thin filaments produced by the dissociation of thick filaments.

Animals↗
PubMed1988

Spontaneous oscillatory contraction of sarcomeres in skeletal myofibrils.

We found that the lengths of all sarcomeres spontaneously oscillated in an isolated skeletal myofibril, when both ends were fixed, submillimolar to millimolar concentrations of ATP, ADP and inorganic phosphate (Pi) were present, and Ca2+ was removed. Narrowing and widening of an H-zone and an I-band were observed corresponding to the shortening and lengthening of a sarcomere, suggesting that thick and thin filaments slide past each other. The oscillation of each sarcomere was asymmetrical, consisting of a rapid lengthening phase and a slow shortening phase. The period of oscillation was about 3s; the peak-to-peak amplitude of oscillation reached as much as 30% of the average sarcomere length. The propagation of the sarcomere oscillation along the long axis of the myofibril was observed occasionally in single myofibrils and frequently in bundles of myofibrils. The 'state'-diagram showing the concentration range of ADP and Pi in which contraction, oscillation or relaxation of myofibrils occurs in the presence of ATP and the absence of Ca2+ suggested that the oscillation is a third state of skeletal muscle located in between the contracting and relaxing states.

Adenosine Diphosphate↗
PubMed1988

Beta-actinin: a capping protein at the pointed end of thin filaments in skeletal muscle.

We examined the function of beta-actinin as a pointed end capping protein of thin filaments in skeletal muscle. An improvement in preparing beta-actinin yielded purified beta-actinin which retained its activity for more than a week. Two-dimensional gel electrophoresis showed that the two subunits, beta I and beta II, of beta-actinin are, respectively, split into two to three components (isoforms) with different isoelectric points. Polyclonal antibody was raised by injecting such purified and undenatured chicken breast muscle beta-actinin composed of several components into a rabbit. Immuno-gold labeling examination with electron microscopy of an F-actin-beta-actinin complex decorated with HMM showed that 85% of bound gold particles was on the pointed end of actin filaments, while the remaining 15% was on the barbed end. This suggests that in beta-actinin preparation pointed end and barbed end capping proteins inevitably coexist. Immunofluorescence and immunoelectron microscopy directly showed that beta-actinin is located at the pointed end of thin filaments in myofibrils; it was also suggested that a capping protein having common antigenic determinants to beta-actinin is located at Z-line. Thus, the physiological function of beta-actinin as a pointed end capping protein was examined as follows: When beta-actinin was dissociated from the pointed end of thin filaments in an I-Z-I brush by using a high salt solution, thin filaments could be disassembled at the pointed ends at concentrations of exogenous actin lower than a critical value. At a physiological ionic strength, these salt-washed thin filaments gradually shortened at a constant rate of about 45 nm/h. Both the association and dissociation of monomeric actin at the pointed end were suppressed by the rebinding of exogenous beta-actinin. The main physiological role of beta-actinin is therefore to stabilize thin filaments in the sarcomere by preventing addition and removal of actin monomers at the pointed filament end.

Actin Cytoskeleton↗
PubMed1988

Transition of beta-actinin isoforms during development of chicken skeletal muscle.

We examined by means of the immunoblotting technique the transition of beta-actinin isoforms during the development of the chicken from 5 day embryo to adult. As an antigen, beta-actinin was prepared from adult chicken breast muscle (pectoralis major) and polyclonal antibody was obtained by injecting undenatured beta-actinin into a rabbit. Immunoblotting examination of breast muscle at several stages of development (except 5 day embryo, in which the whole body minus the head and limbs was examined) showed that the species of beta-actinin subunits change during development: 1) beta I is already present in 5 day embryo, whereas beta II appears only after 9 days. 2) In 5 day embryo, we found, instead of beta II, a new subunit (designated beta III) that cross-reacts with the antibody, has the apparent molecular weight of 30,000 daltons and has a slightly alkaline isoelectric point compared with beta I. The content of beta III gradually decreased and beta III completely disappeared a week after hatching. Such a type of transition of the isoforms in beta-actinin subunits is similar to that observed in other muscle proteins. The transition of beta-actinin isoforms may correlate to the organization of an I-Z-I brush, especially to the length determination of thin filaments, because the developmental stage at which beta III disappears coincides with that at which the length of thin filaments is strictly determined.

Actinin↗
PubMed1988

Beta-actinin isoforms in various types of muscle and non-muscle tissues.

We found that beta-actinin isoforms are present in various types of tissues in adult chicken by using immunoblotting after two dimensional gel electrophoresis; for this purpose, an antibody was raised against beta-actinin purified from adult chicken breast muscle (pectoralis major). One of the beta-actinin subunits, beta I, was present in all tissues we examined, i.e. skeletal (pectoralis major, semitendinosus, and anterior latissimus dorsi), cardiac, and smooth (gizzard) muscles, non-muscle (brain, liver, and kidney) tissues and blood, whereas another subunit, beta II, was present only in muscle tissues. A new subunit (designated beta III) that was found in the embryonic stages of skeletal muscle (Asami, Funatsu & Ishiwata (1988) J. Biochem. 103, 72-75) was present instead of beta II in non-muscle tissues and blood. In cardiac and smooth muscles, beta III coexisted with beta I and beta II. The antibody of beta-actinin did not cross-react to cytoplasmic beta-actinin (molecular weight, 80,000 daltons) found in kidney. It was suggested that the combination of beta I and beta III present in non-muscle tissues and blood is identical to the barbed end capping protein isolated from brain by Killiman and Isenberg (EMBO J. 1, 889-894 (1982)). It is likely that beta-actinin forms a genetic family whose constituents have an ability to cap either the pointed or barbed end of actin filaments.

Actinin↗
PubMed1988

Optical anisotropy decay studies of the dynamic structure of myosin filaments.

We applied flash-induced absorption and phosphorescence anisotropy decay methods to the study of rotational motions of myosin heads in solution), myofibrils and muscle fibers); myosin heads were selectively labeled with a triplet probe EMI (5-eosinylmaleimide). EMI-labeled subfragment 1 (S1) showed a single exponential decay of anisotropy over two decades; the analysis indicated that if S1 is modeled as a prolate ellipsoid of revolution, the major axis was 16-17 nm and the minor axis 4.7-4.5 nm. The decay curve of myosin filaments could be simulated by double-exponentials-plus-constant approximation. The data could be analyzed by a double-cone model), in which we assumed that a head part (S1), wobbles in the first cone and a rod portion next to the head also wobbles in the second cone. The semiangle of each cone was estimated to be 35 and 48 degrees, respectively. We found that myosin heads in myofibrils under relaxing conditions extensively rotated as in myosin filaments in solution. When the spacing between thick and thin filaments was artificially reduced by the increase of osmotic pressure with the addition of polyvinylpyrrolidone (PVP), restriction of the angular range of the rotational motion was observed. Under rigor conditions no motion was observed in a 10 microsecond time scale, indicating that the heads were immobilized by binding to thin filaments. Preliminary results on the rotational motions of myosin heads in muscle fibers are also reported.

Animals↗
PubMed1987

Rotational motions of myosin heads in myofibril studied by phosphorescence anisotropy decay measurements.

We studied the rotational Brownian motions of myosin heads, of which the sulfhydryl group was selectively labeled with the triplet probe 5-eosinylmaleimide, in myofibril by using flash-induced phosphorescence anisotropy decay measurements. The anisotropy decay curve under relaxing conditions consisted of a fast (submicrosecond) and a slow (a few microseconds) component and a small constant part as in the synthetic myosin filaments in solution. The decay curves could be analyzed by assuming that a head part, i.e. subfragment 1 (S1), wobbles in the first cone and a part connecting S1 and the tail of a myosin molecule of which the length is shorter than subfragment 2 (S2) wobbles in the second cone (a double-cone model); the semiangles of the former and the latter cones were about 30 degrees and 50 degrees, respectively. The rotational freedom of myosin heads was only slightly restricted by the limited space of the filament lattice in myofibrils. Under rigor conditions, no motion of myosin heads was observed in the 10-microseconds time scale.

Animals↗
PubMed1987

Dynamic light-scattering study of muscle F-actin. II.

By dynamic light scattering, the intensity autocorrelation function, G2(tau) = B[1 + beta[g1(tau)[2], was obtained over the scattering angles (theta) from 30 to 130 degrees in steps of 10 degrees for semidilute solutions of muscle F-actin and of F-actin complexed with heavy meromyosin in the absence of ATP (acto-HMM), where B is the baseline and beta a constant. The main findings were: (1) A 0.5 mg/ml F-actin solution gave nonreproducible spectra at theta less than or equal to 40 degrees but quite reproducible spectra at theta greater than or equal to 50 degrees, with beta = 0.9-0.8 at all theta values. Nonreproducibility of spectra at low theta values was concluded to be due to restricted motions of very long filaments confined in cages or zig-zag tubing formed by a major fraction of filaments, where the very long filaments were those at a distant tail of an exponential length distribution and the major fraction of filaments were those with lengths around Ln-2Ln, Ln being the number-average length. Spectral widths were compared with theoretical ones for rigid rods averaged over the length distribution with Ln = 900 nm, and were suggested to be largely contributed at high theta values from bending motions of filaments. (2) Acto-HMM solutions at 0.5 mg/ml F-actin and at weight ratios of HMM to F-actin of 0.5-2 gave spectra which, with respect to theta, behaved very similarly to those of F-actin alone. The spectral widths, however, drastically decreased with the weight ratio up to unity and stayed virtually constant above unity. In contrast to a previous study (F.D. Carlson and A.B. Fraser, J. Mol. Biol. 89 (1974) 273), beta values of acto-HMM were as large as those of F-actin alone. Acto-HMM was concluded to travel a distance far greater than 1/K with a mobility smaller than that of F-actin, where K = (4 pi/lambda) sin(theta/2), lambda being the wavelength of light in the medium. These results suggest that acto-HMM gels are very soft even though they did not pour from an inverted cell. Based on several intuitive models which give a mutual relationship between the beta value and modes of motion of scatterers, we discuss the restricted motions responsible for nonreproducibility of spectra at low angles and large beta values of acto-HMM gels at all theta values and weight ratios so far studied.

Actins↗