Depolarisation of the plasma membrane in the arsenic trioxide (As2O3)-and anti-CD95-induced apoptosis in myeloid cells

Depolarisation of the plasma membrane has been shown to be actively regulated during lymphocyte-apoptosis. Here, we present data about anti-Fas and As2O3 induced depolarisation of myeloid U-937 cells. Anti-Fas but not As2O3-induced depolarisation was significantly dependent on caspase-activation. Na+-fluxes contributed to the depolarisation in early stages of As2O3-induced apoptosis, whereas the membrane potential in late stages depended on Cl- -fluxes. Cl- -channels also played an important role in the induction of cell shrinkage in As2O3-induced apoptosis. However, none of these ions contributed significantly to anti-Fas induced depolarisation. This indicates the existence of different mechanisms for apoptotic plasma membrane depolarisation within one cell type.     

Depolarisation and repolarisation sequences of ventricular epicardium in chickens (Gallus gallus domesticus)

Activation and recovery sequences were mapped by means of 64-channel synchronous recording of extracellular potentials on ventricular epicardium in chickens. Ventricular epicardium was depolarized due to multiple breakthroughs. The recovery of ventricular epicardium occurs from the apex to the base of heart and does not repeat the activation sequence. Gradients of repolarisation exist over the ventricular epicardium in birds. Repolarisation pattern of ventricular epicardium depends primarily on intrinsic spatial heterogeneities of ARIs over epicardium.     

Light sensitivity of the ciliate Tetrahymena vorax induced by the fluorescent dye acridine orange.

The ciliate Tetrahymena vorax is normally insensitive to light. However, after uptake of acridine orange, blue light evokes instant backward swimming. The dye accumulates mainly in posterior vacuoles, with half-maximal uptake after 1 min. Illumination for 10 s induced a depolarisation of approximately 15 mV lasting less than 2 s, followed by a sustained hyperpolarisation of approximately 20 mV. Deciliated cells displayed a similar response. The hyperpolarisation was linked to reduced membrane resistance, showed a reversal potential of approximately -55 mV and was blocked by 1 mmol l(-1) TEA. The rate of rise of electrically evoked Ca(2+)-spikes was reduced during the hyperpolarisation, which is compatible with elevated cytosolic Ca(2+) concentration. This suggests that the hyperpolarisation may be caused by activation of Ca(2+)-sensitive K(+) channels. The depolarisation was abolished in Ca(2+)-free medium, whereas the hyperpolarisation was unaffected. Illumination for 2 s, or prolonged stimulation restricted to the anterior part of the cell, induced depolarisation only. Illumination of the posterior part caused delayed hyperpolarisation with no preceding depolarisation. We conclude that the induced backward swimming is associated with Ca(2+) influx through anterior channels, while Ca(2+) released from intracellular stores activates K(+) channels responsible for the delayed hyperpolarisation.     

Comparative study of the space constant of electrotonic decay in the endocardium and epicardium of the rabbit right atrium

The distribution of the electronic potential in the endocardium and epicardium of the rabbit right atrium was studied. The distribution of the electronic potential was studied by the method of intracellular polarization of cardiac fibers via a suction electrode perfused from the inside with a KCl isotonic solution. The space constant of electronic decay along and across cardiac fibers in the endocardium and epicardium of rabbit right atrium was measured. It was shown that the space constant of electronic potential decay in rabbit the right atrium endocardium in the areas of ordered arrangement of trabecules both along (lambda x = 2117 +/- 653 microns) and across (lambda y = 394 +/- 212 microns) the fiber was higher (p < 0.001) than that in epicardium (lambda x and lambda y equal to 1361 +/- 486 microns and 212 +/- 63 microns, respectively). The values lambda x and lambda y do not significantly differ between separate areas of the epicardium. The degree of electrotonic anisotropy in all the structures investigated was almost the same, its value ranging from 2 to 17.     

Cardiac electric field at the period of depolarization and repolarization of the frog heart ventricle

Multichannel mapping of electrical field on heart ventricle epicardium and the body surface in frogs Rana esculenta and Rana temporaria was performed at periods of the ventricular myocardium depolarization and repolarization. The zone of the epicardium early depolarization is located on epicardium of the ventricle base posterior wall, while the late depolarization zone--on its apex and on the base anterior wall. The total vector of sequence of the ventricle epicardium depolarization is directed from the base to the apex. The zone of the early repolarization is located in the apical area, while that of the late one--in the area of the base. On the frog body surface the cardioelectric field with the cranial zone of negative and the caudal zone of positive potentials is formed before the appearance of the QRS complex on ECG. At the period of the heart ventricle repolarization the zone of the cardioelectric field negative potentials is located in the cranial, while that of the positive ones--in the body surface caudal parts. The cardioelectric field on the frog body surface at the periods of depolarization and repolarization of the ventricle myocardium reflects adequately the projection of sequence of involvement with excitation and of distribution of potentials on epicardium.     

Transmural reentry triggered by epicardial stimulation during acute ischemia in canine ventricular muscle

Ischemia depresses tissue excitability more rapidly in the ventricular epicardium than in the endocardium. We hypothesized that this would provide the substrate for transmural reentry originating in the epicardium. We mapped transmural conduction in isolated and perfused wedges taken from canine left ventricles during global ischemia while pacing alternately between the epicardium and endocardium. Ischemia reduced conduction velocity more in the epicardium than in the endocardium. We observed that the epicardial-initiated activation penetrated the ventricular wall transmurally while failing to conduct laterally along the epicardium, then conducted laterally along the endocardium and midmyocardium, and reentered the epicardium in 9 of 16 wedges during epicardial stimulation after 600 +/- 182 s of ischemia. Endocardial stimulation applied immediately before or after the epicardial stimulation initiated activation that spread quickly along the endocardium and then transmurally to the epicardium without reentry in six of the nine wedges. The transmural asymmetric conduction was not observed in four separate wedges after the endocardium was removed. Therefore, ischemia-induced transmural gradient of excitability provided the substrate for reentry during epicardial stimulation.     

Cardiac electric field at the period of depolarization and repolarization of the frog heart ventricle

Multichannel mapping of electrical field on heart ventricle epicardium and the body surface in frogs Rana esculenta and Rana temporaria was performed at periods of the ventricular myocardium depolarization and repolarization. The zone of the epicardium early depolarization is located on epicardium of the ventricle base posterior wall, while the late depolarization zone—on its apex and on the base anterior wall. The total vector of sequence of the ventricle epicardium depolarization is directed from the base to the apex. The zone of the early repolarization is located in the apical area, while that of the late one—in the area of the base. On the frog body surface the cardioelectric field with the cranial zone of negative and the caudal zone of positive potentials is formed before the appearance of the QRS complex on ECG. At the period of the heart ventricle repolarization the zone of the cardioelectric field negative potentials is located in the cranial, while that of the positive ones—in the body surface caudal parts. The cardioelectric field on the frog body surface at the periods of depolarization and repolarization of the ventricle myocardium reflects adequately the projection of sequence of involvement with excitation and of distribution of potentials on epicardium.     

Light sensitivity of the ciliate Tetrahymena vorax induced by the fluorescent dye acridine orange

The ciliate Tetrahymena vorax is normally insensitive to light. However, after uptake of acridine orange, blue light evokes instant backward swimming. The dye accumulates mainly in posterior vacuoles, with half-maximal uptake after 1 min. Illumination for 10 s induced a depolarisation of approximately 15 mV lasting less than 2 s, followed by a sustained hyperpolarisation of approximately 20 mV. Deciliated cells displayed a similar response. The hyperpolarisation was linked to reduced membrane resistance, showed a reversal potential of approximately −55 mV and was blocked by 1 mmol l⁻¹ TEA. The rate of rise of electrically evoked Ca²⁺-spikes was reduced during the hyperpolarisation, which is compatible with elevated cytosolic Ca²⁺ concentration. This suggests that the hyperpolarisation may be caused by activation of Ca²⁺-sensitive K⁺ channels. The depolarisation was abolished in Ca²⁺-free medium, whereas the hyperpolarisation was unaffected. Illumination for 2 s, or prolonged stimulation restricted to the anterior part of the cell, induced depolarisation only. Illumination of the posterior part caused delayed hyperpolarisation with no preceding depolarisation. We conclude that the induced backward swimming is associated with Ca²⁺ influx through anterior channels, while Ca²⁺ released from intracellular stores activates K⁺ channels responsible for the delayed hyperpolarisation.     

Effect of carbacholine on proximal and distal regions of motor nerve terminals in the frog]

Carbacholine depressed postsynaptic currents in the frog m. sartorius leaving intact presynaptic currents in proximal and distal portions of the motor nerve ending. The carbacholine depressing action was followed by an increase in the time gap between the beginning of presynaptic depolarisation and subsequent quantal release. This effect was considerably more obvious in the distal portions of the nerve endings. Effect of extracellular potassium was evident in a diminishing of presynaptic currents due to membrane depolarisation. The data obtained suggest that carbacholine presynaptically depresses synaptic transmission via metabotropic cholinergic receptors controlling the time course of the transmitter release.     

Postcatelectrotonic potentials and trace changes in the nerve fiber excitability

When cathode subthreshold impulse was turned off, excitable membranes of isolated nerve fibres and nervous trunk show postelectrotonic depolarisation (PED), that is a slow recovery of membrane potential to the resting level. PED of the single nodes of Ranvier and nervous trunk is registered not only in normal conditions, but also after complete block of sodium channels. The size and duration of nervous trunk PED under subthreshold depolarising current increase along with duration of applied depolarisation: when cathode current 1 ms in duration was used, they were 0.093 +/- +/- 0.004 mV and 7.123 +/- 0.576 ms, respectively; when current was 5 ms in duration, they were 0.189 +/- 0.005 mV and 23.212 +/- 1.186 ms, whereas a 10-ms depolarisation yields values of 0.220 +/- 0.011 mV and 68.721 +/- 3.389 ms. Application of the train of catelectrotonic impulses leads to PED built-up. As PED is found not only in normal conditions but also after complete block of sodium channels, it is reasonable to suggest that the most probable reason for PED is an outward potassium current.     

Hyperpolarization of the cell membrane during Na,K-ATPase inactivation

The relationship equation between the resting potential and potassium and sodium active currents is deduced in terms of a generally accepted model of electrogenesis. It is demonstrated that an increase of Na,K-ATPase activity to the estimated magnitude results in hyperpolarization of the cell membrane (CM), but the subsequent increase of the activity led to CM depolarisation. CM depolarisation results in an increase of the cell volume.     

Sustained depolarisation induces changes in the extracellular concentrations of purine and pyrimidine nucleosides in the rat thalamus

ATP and adenosine are well-known neuroactive compounds. Other nucleotides and nucleosides may also be involved in different brain functions. This paper reports on extracellular concentrations of nucleobases and nucleosides (uracil, hypoxanthine, xanthine, uridine, 2'-deoxycytidine, 2'-deoxyuridine, inosine, guanosine, thymidine, adenosine) in response to sustained depolarisation, using in vivo brain microdialysis technique in the rat thalamus. High-potassium solution, the glutamate agonist kainate, and the Na(+)/K(+) ATPase blocker ouabain were applied in the perfusate of microdialysis probes and induced release of various purine and pyrimidine nucleosides. All three types of depolarisation increased the level of hypoxanthine, uridine, inosine, guanosine and adenosine. The levels of measured deoxynucleosides (2'-deoxycytidine, 2'-deoxyuridine and thymidine) decreased or did not change, depending on the type of depolarisation. Kainate-induced changes were TTX insensitive, and ouabain-induced changes for inosine, guanosine, 2'-deoxycytidine and 2'-deoxyuridine were TTX sensitive. In contrast, TTX application without depolarisation decreased the extracellular concentrations of hypoxanthine, uridine, inosine, guanosine and adenosine.Our data suggest that various nucleosides may be released from cells exposed to excessive activity and, thus, support several different lines of research concerning the regulatory roles of nucleosides.     

Simple models of stimulation of neurones in the brain by electric fields

The excitation of pyramidal cells in the motor cortex, produced by electric fields generated by distant electrodes or by electromagnetic induction, has been modelled. Linear, steady-state models of myelinated axons capture most of the geometrical aspects of neurone activation in electric fields. Some non-linear features can be approximated. Models with a proximal sealed-end and distal infinite axon, or of finite length, are both serviceable. Surface anodal stimulation produces hyperpolarisation of the proximal axon (closest to the anode) and depolarisation in the distal axon. The point of maximum depolarisation can be influenced by the location of the cathode (greater separation of anode and cathode causes more distal depolarisation). Axon bends can produce very localised depolarisation. Cathodal stimulation may be less effective than anodal as a result of anodal block of conduction of action potentials in the distal axon. The latencies of responses to anodal stimulation, recorded in the distal axon, will decrease as the stimulus strength is increased and the point of action potential initiation moves distally node by node. Larger jumps in latency will be produced when the point of action potential initiation moves from one axon bend to another.     

遗传谱系示踪技术揭示小鼠胚胎前体心外膜向心外膜转化过程

心外膜的形成是胚胎心脏发育的关键生理过程之一。利用遗传谱系示踪技术示踪观察前体心外膜向心外膜细胞转化过程,具有重要的科学研究价值。本研究拟利用Tbx18+前体/心外膜祖细胞遗传谱系示踪模型,揭示胚胎心外膜的起源及前体心外膜向心外膜转化的过程。利用整胚和切片原位杂交技术揭示,Tbx18 mRNA特异性表达于胚龄（E）9.5 d小鼠胚胎前体心外膜;故Tbx18是前体心外膜的特异性标记基因。利用整胚X-Gal染色,揭示报告基因Lacz在E9.5 d遗传谱系示踪模型鼠胚前体心外膜中大量表达,此时报告基因从前体心外膜逐渐迁移并开始少量表达于心外膜。Lacz在E10～E10.5 d双杂合鼠胚前体心外膜中表达逐渐减少,而在心外膜组织中逐渐增多;在E11.5 d,报告基因在前体心外膜中表达基本消失,而在心外膜组织中大量表达。切片进行X-Gal染色也揭示,报告基因Lacz定位于早期胚胎前体心外膜及心外膜。免疫荧光染色证实,早期胚胎心外膜细胞呈现未分化的祖细胞状态。通过报告基因的表达变化模式揭示,胚胎心外膜的形成经历了启动、转化、完成3个阶段;E9.5～11.5 d左右这个时间段发生的前体心外膜向心外膜转化,可能是心外膜形成的主要来源和形式。     

Depolarisation-Dependent Protein Phosphorylation and Dephosphorylation in Rat Cortical Synaptosomes Is Modulated by Calcium

The effect of calcium on protein phosphorylation was investigated using intact synaptosomes isolated from rat cerebral cortex and prelabelled with 32Pi. For nondepolarised synaptosomes a group of calcium-sensitive phosphoproteins were maximally labelled in the presence of 0.1 mM calcium. The phosphorylation of these proteins was slightly decreased in the presence of strontium and absent in the presence of barium, consistent with the decreased ability of these cations to activate calcium-stimulated protein kinases. Addition of calcium alone to synaptosomes prelabelled in its absence increased phosphorylation of a number of proteins. On depolarisation in the presence of calcium certain of the calcium-sensitive phosphoproteins were further increased in labelling above nondepolarised levels. These increases were maximal and most sustained after prelabelling at 0.1 mM calcium. On prolonged depolarisation at this calcium concentration a slow decrease in labelling was observed for most phosphoproteins, whereas a greater rate and extent of decrease occurred at higher calcium concentrations. At 2.5 mM calcium a rapid and then a subsequent slow dephosphorylation was observed, indicating two distinct phases of dephosphorylation. Of all the phosphoproteins normally stimulated by depolarisation, only phosphoprotein 59 did not exhibit the rapid phase of dephosphorylation at high calcium concentrations. Replacing calcium with strontium markedly decreased the extent of change observed on depolarisation whereas barium decreased phosphorylation changes even further. Taken together these data suggest that an influx of calcium into synaptosomes initially activates protein phosphorylation, but as the levels of intrasynaptosomal calcium rise protein dephosphorylation predominates. Other phosphoproteins were dephosphorylated immediately on depolarisation in the presence of calcium. The fine control of protein phosphorylation levels exerted by calcium supports the idea that the synaptosomal phosphoproteins could play a role in modulating events such as neurotransmitter release in the nerve terminal.     

Cardioelectric field on the atrial surface in pigs

The form and distribution of extracellular cardioelectric potentials and the sequence of the excitation wave propagation on epicardium of the pig atria were studied by the method of multichannel synchronous cardioelectrotopography. The studies have shown that in pig the excitation wave breaks on epicardium of the right atrium at the base of the upper vena cava. Negative initial atrial complexes are registered in this area. Two fronts of excitation wave spread from the zone of initial epicardial activation: one--to upper segments of dorsal and ventral sides of the right atrium, the second--to inter-atrial septum. The excitation wave comes to the left atrium with a delay relative to the beginning of depolarization of the right atrium. On account of the successive movement of the front of the excitation wave from pacemaker the two-phase potentials are formed on greater part of the epicardium of the pig atria. The lower part of the auricle of the left atrium is depolarized in atrial epicardium in the last turn. The sequence of excitation wave propagation in atrial epicardium close to ravenous (dog) and ungulate (sheep) animals and man is typical for the pig, but herewith the differences in time of covering the atria with excitation do exist.     

Depolarisation-Dependent Protein Phosphorylation in Rat Cortical Synaptosomes: Factors Determining the Magnitude of the Response

Abstract: The sequence of molecular events linking depolarisation-dependent calcium influx to the release of neurotransmitters from nerve terminals is unknown; however, calcium-stimulated protein phosphorylation may play a role. In this study the incorporation of phosphate into proteins was investigated using an intact postmitochondrial pellet isolated from rat cerebral cortex. The rate and relative incorporation of label into individual phosphoproteins depended on the prelabelling time and buffer concentrations of calcium and phosphate. After prelabelling for 45 min, depolarisation caused a >20% increase in the labelling of 10 phosphoproteins, and this initial increase was maximal with 41 mM K⁺ for 5 s, or 30 μ M veratridine for 15 s, in the presence of 1 mM calcium. Both agents also led to an initial dephosphorylation of four phosphoproteins. Depolarisation for 5 min led to a significant decrease in the labelling of all phosphoproteins. All of the depolarisation-stimulated changes in protein phosphorylation were calcium-dependent. The depolarisation conditions found to optimally alter the phosphorylation of synaptosomal proteins find many parallels in studies on calcium uptake and neurotransmitter release. However, the uniform responses of such a large number of phosphoproteins to the multitude of depolarisation conditions studied suggest that the changes could equally well relate to recovery events such as biosynthesis of neurotransmitters and regulation of intraterminal metabolic activity.     

Swell activated chloride channel function in human neutrophils

Non-excitable cells such as neutrophil granulocytes are the archetypal inflammatory immune cell involved in critical functions of the innate immune system. The electron current generated (I_e) by the neutrophil NADPH oxidase is electrogenic and rapidly depolarises the membrane potential. For continuous function of the NADPH oxidase, I_e has to be balanced to preserve electroneutrality, if not; sufficient depolarisation would prevent electrons from leaving the cell and neutrophil function would be abrogated. Subsequently, the depolarisation generated by the neutrophil NADPH oxidase I_e must be counteracted by ion transport. The finding that depolarisation required counter-ions to compensate electron transport was followed by the observation that chloride channels activated by swell can counteract the NADPH oxidase membrane depolarisation. In this mini review, we discuss the research findings that revealed the essential role of swell activated chloride channels in human neutrophil function.     

Effect of diastolic pressure on MLC2v phosphorylation in the rat left ventricle

The effect of passive muscle stretch on the extent of MLC2v phosphorylation was investigated. We used an isolated rat heart preparation and controlled the passive pressure of the left ventricle (LV) at 0 or 15 mmHg. The hearts were flash frozen and the LV free wall was split into epicardial and the endocardial halves. The samples were solubilized using a novel method that minimizes changes in the phosphate content of MLC2v under non-denaturing conditions. The proteins were separated by urea glycerol PAGE and identified by mass spectrometry and Western blots. At 0 mmHg passive pressure, the extent of MLC2v phosphorylation of the epicardium (34.1+/-1.7%) was the same as that of the endocardium (35.3+/-3.4%). At 15 mmHg passive pressure, we found a significant increase in MLC2v phosphorylation in the epicardium (to 41.5+/-2.0%) and a significant reduction in the endocardium (to 24.2+/-1.2%), giving rise to a gradient in the extent of MLC2v phosphorylation from epicardium (high) to endocardium (low). These changes in MLC2v phosphorylation that take place in response to increased diastolic pressure are likely to impact on the calcium sensitivity of actomyosin interaction (with an increased sensitivity towards the epicardium) and may play a role in the Frank-Starling mechanism of the heart.