A family of mitogen-activated protein (MAP) kinases comprising the extracellular signal-regulated kinases (ERKs), c-Jun N-terminal kinases (JNKs), and p38 MAP kinases are involved in proliferation and apoptosis. However, there are some arguments concerning the role of these kinases in Ag-induced B cell apoptosis. Two of the B lymphoma cell lines (CH31 and WEHI-231) susceptible to anti-IgM-induced apoptosis were used as a model. To address these issues, we examined the kinetics of anti-IgM-induced activation of MAP kinases and established cell lines overexpressing a dominant-negative (dn) mutant form of JNK1 (dnJNK1). Anti-IgM induced a sustained JNK1 activation with a peak at 8 h, with a marginal activation of ERK1/ERK2 in CH31 cells. The sustained JNK1 activation was not a secondary event through a caspase activation. The peak point of the JNK1 activation was just before the onset of a decline in mitochondrial membrane potential, which preceded anti-IgM-induced cell death. Following anti-IgM stimulation, dnJNK1 prevented a decline in mitochondrial membrane potential at 24 h, with a prolonged inhibition up to 72 h in WEHI-231, although it did so only partially during a later time period in CH31. The dnJNK1 cells also demonstrated diminished procaspase-3 activation and a decreased rate of apoptosis upon anti-IgM stimulation, with a concomitant increased arrest in G1 phase, which could be explained by enhanced levels of cyclin-dependent kinase inhibitor p27Kip1 protein. Thus, anti-IgM-induced JNK activation might be implicated in cell cycle progression as well as in apoptosis regulation, probably involving p27Kip1 protein.
We studied x-ray diffraction from the left ventricular wall of an excised, perfused whole heart of a rat using x rays from the third-generation synchrotron radiation facility, SPring-8. With the beam at right angles to the long axis of the left ventricle, well-oriented, strong equatorial reflections were observed from the epicardium surface. The reflections became vertically split arcs when the beam passed through myocardium deeper in the wall, and rings were observed when the beam passed into the inner myocardium of the wall. These diffraction patterns were explained by employing a layered-spiral model of the arrangement of muscle fibers in the heart. In a quiescent heart with an expanded left ventricle, the muscle fibers at the epicardium surface were found to have a (1,0) lattice spacing smaller than in the rest of the wall. The intensity ratio of the (1,0) and (1,1) equatorial reflections decreased on contraction with a similar time course in all parts of the wall. The results show that it is possible to assign the origin of reflections in a diffraction diagram from a whole heart. This study offers a basis for interpretation of x-ray diffraction from a beating heart under physiologically and pathologically different conditions.
We examined the sarcomere length-dependence of the spacing of the hexagonal lattice of the myofilaments and the mass transfer of myosin cross-bridges during contraction of right ventricular papillary muscle of the rat. The lattice spacing and mass transfer were measured by using X-ray diffraction, and the sarcomere length was monitored by laser diffraction at the same time. Although the lattice spacing and the sarcomere length were inversely related, their relationship was not exactly isovolumic. The cell volume decreased by about 15% when the sarcomere length was shortened from 2.3 micro m to 1.8 micro m. Twitch tension increased with sarcomere length (the Frank-Starling law). At the peak tension, the ratio of the intensity of the (1,0) equatorial reflection to that of the (1,1) reflection was smaller when the tension was greater, showing that the larger tension at a longer sarcomere length accompanies a larger amount of mass transfer of cross-bridges from the thick to the thin filament. The result suggests that the Frank-Starling law is due to an increase in the number of myosin heads attached to actin, not in the average force produced by each head.
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