Immunodetection and intracellular localization of caldesmon-like proteins in Amoeba proteus

Summary. Caldesmon immunoanalogues were detected in Amoeba proteus cell homogenates by the Western blot technique. Three immunoreactive bands were recognized by polyclonal antibodies against the whole molecule of chicken gizzard caldesmon as well as by a monoclonal antibody against its C-terminal domain: one major and two minor bands corresponding to proteins with apparent molecular masses of 150, 69, and 60 kDa. The presence of caldesmon-like protein(s) in amoebae was revealed as well in single cells after their fixation, staining with the same antibodies, and recording their total fluorescence in a confocal laser scanning microscope. Proteins recognized by the antibodies bind to filamentous actin. This was established by a cosedimentation assay in cell homogenates and by colocalization of the caldesmon-related immunofluorescence with the fluorescence of filamentous actin stained with rhodamine-labelled phalloidin, demonstrated in optical sections of single cells in a confocal microscope. Caldesmon is colocalized with filamentous actin in the withdrawn cell regions where the cortical actomyosin network contracts and actin is depolymerized, in the frontal zone where actin is polymerized again and the cortical cytoskeleton is reconstructed, inside the nucleus and in the perinuclear cytoskeleton, and probably at the cell-to-substratum adhesion sites. The regulatory role of caldesmon in these functionally different regions of locomoting amoebae is discussed.Correspondence and reprints: Department of Cell Biology, Nencki Institute of Experimental Biology, ulica Pasteura 3, 02-093 Warsaw, Poland.Received October 7, 2002; accepted December 2, 2002; published online August 26, 2003     

Muscle contraction: energy rate equations in relation to efficiency and step-size distance

We derive the energy rate equation for muscle contraction. Our equation has only two parameters m, the maintenance heat rate and 1/S, the shortening heat coefficient. The impulsive model (previously described in earlier papers) provides a physical basis for parameter 1/S as well as for constants a and b in Hill’s force–velocity equation. We develop new theory and relate the efficiency and the step-size distance to our energy rate equation. Correlation between the efficiency and the step-size distance is established. The various numbers are listed in Table 1: we use data from five different muscles in the literature. In summary, our analysis strongly supports the impulsive model as the correct model of contraction.     

Models in which many cross-bridges attach simultaneously can explain the filament movement per ATP split during muscle contraction

Contractile filaments in skeletal muscle are moved by less than 2 nm for each ATP used. If just one cross-bridge is attached to each thin filament at any instant then this distance represents the fundamental myosin cross-bridge step size (i.e. the distance one cross-bridge moves a thin filament in one ATP-splitting cycle). However, most contraction models assume many cross-bridges are attached at any instant along each thin filament. The purpose of this study was to establish whether the net filament sliding per ATP used could be explained quantitatively in terms of a cross-bridge model in which multiple cross-bridges are attached along each thin filament. It was found that the relationship between net filament sliding per ATP split and the load against which the muscle shortens is compatible with such a model and furthermore predicts that the cross-bridge step size is between 7.5 and 12.5 nm over most of the range of loads. These values were similar for different muscle fibre types.     

Calcium-induced calcium release in smooth muscle: loose coupling between the action potential and calcium release

Calcium-induced calcium release (CICR) has been observed in cardiac myocytes as elementary calcium release events (calcium sparks) associated with the opening of L-type Ca(2+) channels. In heart cells, a tight coupling between the gating of single L-type Ca(2+) channels and ryanodine receptors (RYRs) underlies calcium release. Here we demonstrate that L-type Ca(2+) channels activate RYRs to produce CICR in smooth muscle cells in the form of Ca(2+) sparks and propagated Ca(2+) waves. However, unlike CICR in cardiac muscle, RYR channel opening is not tightly linked to the gating of L-type Ca(2+) channels. L-type Ca(2+) channels can open without triggering Ca(2+) sparks and triggered Ca(2+) sparks are often observed after channel closure. CICR is a function of the net flux of Ca(2+) ions into the cytosol, rather than the single channel amplitude of L-type Ca(2+) channels. Moreover, unlike CICR in striated muscle, calcium release is completely eliminated by cytosolic calcium buffering. Thus, L-type Ca(2+) channels are loosely coupled to RYR through an increase in global [Ca(2+)] due to an increase in the effective distance between L-type Ca(2+) channels and RYR, resulting in an uncoupling of the obligate relationship that exists in striated muscle between the action potential and calcium release.     

Overexpression of SERCA2 ATPaase in vascular smooth muscle cells treated with oxidized low density lipoprotein

Oxidized low density lipoprotein (oxLDL) has been identified as a potentially important atherogenic factor. Atherosclerosis is characterized by the accumulation of lipid and calcium in the vascular wall. OxLDL plays a significant role in altering calcium homeostasis within different cell types. In our previous study, chronic treatment of vascular smooth muscle cells (VSMC) with oxLDL depressed Ca²⁺ _i homeostasis and altered two Ca²⁺ release mechanisms in these cells (IP₃ and ryanodine sensitive channels). The purpose of the present study was to further define the effects of chronic treatment with oxLDL on the smooth muscle sarcoplasmic reticulum (SR) Ca²⁺ pump. One of the primary Ca²⁺ uptake mechanisms in VSMC is through the SERCA2 ATPase calcium pump in the sarcoplasmic reticulum. VSMC were chronically treated with 0.005-0.1 mg/ml oxLDL for up to 6 days in culture. Cells treated with oxLDL showed a significant increase in the total SERCA2 ATPase content. These changes were observed on both Western blot and immunocytochemical analysis. This increase in SERCA2 ATPase is in striking contrast to a significant decrease in the density of IP₃ and ryanodine receptors in VSMC as the result of chronic treatment with oxLDL. This response may suggest a specific adaptive mechanism that the pump undergoes to attempt to maintain Ca²⁺ homeostasis in VSMC chronically exposed to atherogenic oxLDL.     

A model of troponin-I in complex with troponin-C using hybrid experimental data: the inhibitory region is a beta-hairpin

We present a model for the skeletal muscle troponin-C (TnC)/troponin-I (TnI) interaction, a critical molecular switch that is responsible for calcium-dependent regulation of the contractile mechanism. Despite concerted efforts by multiple groups for more than a decade, attempts to crystallize troponin-C in complex with troponin-I, or in the ternary troponin-complex, have not yet delivered a high-resolution structure. Many groups have pursued different experimental strategies, such as X-ray crystallography, NMR, small-angle scattering, chemical cross-linking, and fluorescent resonance energy transfer (FRET) to gain insights into the nature of the TnC/TnI interaction. We have integrated the results of these experiments to develop a model of the TnC/TnI interaction, using an atomic model of TnC as a scaffold. The TnI sequence was fit to each of two alternate neutron scattering envelopes: one that winds about TnC in a left-handed sense (Model L), and another that winds about TnC in a right-handed sense (Model R). Information from crystallography and NMR experiments was used to define segments of the models. Tests show that both models are consistent with available cross-linking and FRET data. The inhibitory region TnI(95-114) is modeled as a flexible beta-hairpin, and in both models it is localized to the same region on the central helix of TnC. The sequence of the inhibitory region is similar to that of a beta-hairpin region of the actin-binding protein profilin. This similarity supports our model and suggests the possibility of using an available profilin/actin crystal structure to model the TnI/actin interaction. We propose that the beta-hairpin is an important structural motif that communicates the Ca2+-activated troponin regulatory signal to actin.     

Reflections on a quarter century of research on contractile systems

By the early 1970s studies of muscle contraction reached a high level and the field gave birth to a new line of investigation into the molecular basis of cellular movements. The molecular diversity in these motile systems has proven to be greater than anticipated. Actin filament assembly without direct participation of myosin is used more widely for motility than expected. Atomic structures of key proteins and important technical advances, including single-molecule methods, have enabled detailed investigation of the mechanisms of muscle contraction and cellular motility. However, much work lies ahead to understand the mechanism of force production and to elucidate the signaling pathways that control cellular motility.     

Interaction of myosin LYS-553 with the C-terminus and DNase I-binding loop of actin examined by fluorescence resonance energy transfer

Fluorescence resonance energy transfer (FRET) experiments were carried out in the absence of nucleotide (rigor) or in the presence of MgADP between fluorescent donor probes (IAEDANS (5((((2-iodoacetyl)amino)ethyl)amino)-naphthalene-1-sulfonic acid) at Cys-374 or DANSYL (5-dimethylamino naphthalene-1-(N-(5-aminopentyl))sulfonamide) at Gln-41 of actin and acceptor molecules (FHS (6-[fluorescein-5(and 6)-carboxamido] hexanoic acid succinimidyl ester) at Lys-553 of skeletal muscle myosin subfragment 1. The critical F?rster distance (R(0)) was determined to be 44 and 38 A for the IAEDANS-FHS and DANSYL-FHS donor-acceptor pairs, respectively. The efficiency of energy transfer between the acceptor molecules at Lys-553 of myosin and donor probes at Cys-374 or Gln-41 of actin was calculated to be 0.78 +/- 0.01 or 0.94 +/- 0.01, respectively, corresponding to distances of 35.6 +/- 0.4 A and 24.0 +/- 1.6 A, respectively. MgADP had no significant effect on the distances observed in rigor. Thus, rearrangements in the acto-myosin interface are likely to occur elsewhere than in the lower 50-kDa subdomain of myosin as its affinity for actin is weakened by MgADP binding.     

胃动素和胃泌素引起大鼠胃窦平滑肌细胞收缩的信号转导通路

应用大鼠游离胃窦平滑肌细胞,观察胃动素和胃泌素对胃窦平滑肌细胞收缩作用的胞内信号转导通路。结果显示：⑴胃动素和胃泌素对胃窦平滑肌细胞均有收缩作用;⑵Ｇａｉ－３抗体可抑制胃动素和胃泌素加强胃窦平滑肌细胞的收缩,胃动素、胃泌明显增加Ｇａｉ－３抗体与「＾３５Ｓ」ＣＴＰγＳ的结合;⑶磷脂酶抑制剂Ｕ－７３１２２、三磷酸肌醇受体拮抗剂肝素可抑制胃坳素和胃泌素引起的胃窦平滑肌细胞的收缩。结果表明：胃坳素和胃泌表     

Muscle contraction: viscous-like frictional forces and the impulsive model

Apart from a few experimental studies muscle viscosity has not received much recent analytical attention as a determinant of the contractile process. This is surprising, since any muscle cell is 80% water, and may undergo large shape changes during its working cycle. Intuitively one might expect the viscosity of the solvent to be an important determinant of the physiological activity of muscle tissue. This was apparent to pioneers of the study of muscle contraction such as Hill and his contemporaries, whose putative theoretical formulations contained terms related to muscle viscosity. More recently, though, a hydrodynamic calculation by Huxley, using a solvent viscosity close to that of water, has been held to demonstrate that viscous forces are negligible in muscle contraction. We have re-examined the role of viscosity in contraction, postulating impulsive acto-myosin forces that are opposed by a viscous resistance between the filaments. The viscous force required, 10⁴ times the hydrodynamic estimate, is close to recent experimental measurements, themselves 10²–10³ times the hydrodynamic estimate. This also agrees with contemporary measurements of cytoplasmic viscosity in other biological cells using magnetic bead micro-rheometry. These are several orders of magnitude greater than the viscosity of water. In the course of the analysis we have derived the force-velocity equation for an isolated half-sarcomere containing a single actin filament for the first time, and from first principles. We conclude that muscle viscosity is indeed important for the contractile process, and that it has been too readily discounted.