Measurements of calcium transients in ventricular cells during discontinuous action potential conduction

The L-type calcium current (I(Ca)) is important in sustaining propagation during discontinuous conduction. In addition, I(Ca) is altered during discontinuous conduction, which may result in changes in the intracellular calcium transient. To study this, we have combined the ability to monitor intracellular calcium concentration ([Ca(2+)](i)) in an isolated cardiac cell using confocal scanning laser fluorescence microscopy with our "coupling clamp" technique, which allows action potential propagation from the real cell to a real-time simulation of a model cell. Coupling a real cell to a model cell with a value of coupling conductance (G(C) = 8 nS) just above the critical value for action potential propagation results in both an increased amplitude and an increased rate of rise of the calcium transient. Similar but smaller changes in the calcium transient are caused by increasing G(C) to 20 nS. The increase of [Ca(2+)](i) by discontinuous conduction is less than the increase of I(Ca), which may indicate that much of [Ca(2+)](i) is the result of calcium released from the sarcoplasmic reticulum rather than the integration of I(Ca).     

Modulating L-type calcium current affects discontinuous cardiac action potential conduction.

We have used pairs of cardiac cells (i.e., one real guinea pig ventricular cell and a real-time simulation of a numerical model of a guinea pig ventricular cell) to evaluate the effects on action potential conduction of a variable coupling conductance in combination with agents that either increase or decrease the magnitude of the L-type calcium current. For the cell pairs studied, we applied a direct repetitive stimulation to the real cell, making it the "leader" cell of the cell pair. We have demonstrated that significant delays in action potential conduction for a cell pair can occur either with a decreased value of coupling conductance or with an asymmetry in size such that the follower cell is larger than the leader cell. In both conditions we have shown that isoproterenol, applied to the real cell at very low concentrations, can reversibly decrease the critical coupling conductance (below which action potential conduction fails) for a cell pair with fixed cell sizes, or, for a fixed value of coupling conductance, increase the maximum allowable asymmetry in cell size for successful conduction. For either of these effects, we were able to show that treatment of the real cell with BayK 8644, which more specifically increases the magnitude of the L-type calcium current, was able to mimic the actions of isoproterenol. Treatment of the leader cell of the cell pair (the real cell) with nifedipine, which selectively lowers the magnitude of the L-type calcium current, had effects opposite those of isoproterenol or BayK 8644. The actions of nifedipine, isoproterenol, and BayK 8644 are all limited to conditions in which the conduction delay is on the order of 5 ms or more, whether this delay is caused by limited coupling conductance or by asymmetry in size of the cells. This limitation is consistent with the time course of the L-type calcium current and suggests that the effects of calcium channel blockers or beta-adrenergic blocking drugs, in addition to being selective for regions of the heart that depend on the L-type calcium current for the upstroke of the action potential, would also be somewhat selective for regions of the heart that have discontinuous conduction, either normally or because of some pathological condition.     

Influence of dynamic gap junction resistance on impulse propagation in ventricular myocardium: a computer simulation study

The gap junction connecting cardiac myocytes is voltage and time dependent. This simulation study investigated the effects of dynamic gap junctions on both the shape and conduction velocity of a propagating action potential. The dynamic gap junction model is based on that described by Vogel and Weingart (J. Physiol. (Lond.). 1998, 510:177-189) for the voltage- and time-dependent conductance changes measured in cell pairs. The model assumes that the conductive gap junction channels have four conformational states. The gap junction model was used to couple 300 cells in a linear strand with membrane dynamics of the cells defined by the Luo-Rudy I model. The results show that, when the cells are tightly coupled (6700 channels), little change occurs in the gap junction resistance during propagation. Thus, for tight coupling, there are negligible differences in the waveshape and propagation velocity when comparing the dynamic and static gap junction representations. For poor coupling (85 channels), the gap junction resistance increases 33 MOmega during propagation. This transient change in resistance resulted in increased transjunctional conduction delays, changes in action potential upstroke, and block of conduction at a lower junction resting resistance relative to a static gap junction model. The results suggest that the dynamics of the gap junction enhance cellular decoupling as a possible protective mechanism of isolating injured cells from their neighbors.     

Connexin32 gap junction channels in stably transfected cells: unitary conductance.

Pairs of SKHep1 cells, which are derived from a highly metastatic human hepatoma, were studied using the whole cell voltage clamp technique with patch-type electrodes containing CsCl as the major ionic species. In 12 of 81 cell pairs, current flow through junctional membranes was detectable; in the remaining 69 cell pairs, junctional conductance was less than the noise limit of our recording apparatus (worst case: 10 pS). Macroscopic junctional conductance (gj) in the small percentage of pairs where it was detectable ranged from 100 to 600 pS. Unitary junctional conductance (gamma j) determined in the lowest conductance pairs or after reducing conductance with a short exposure to the uncoupling agent halothane was 25-35 pS. To study properties of gap junction channels formed of connexin32, the parental SKHep1 cell line was stably transfected with a plasmid containing cDNA that encodes connexin32, the major gap junction protein of rat liver cells. In 85 of 98 pairs of voltage clamped connexin32-transfected SKHep1 cells, macroscopic gj was greater than 1 nS; gj increased with time after dissociation (from 1.8 +/- 0.6 [mean +/- SE; n = 7] nS at 2 h after plating to 9.3 +/- 2.2 [n = 9] nS, the maximal value, at 24 h). Unitary conductance of gap junction channels between pairs of transfected SKHep1 cells was measured in low conductance pairs and after reducing gj by exposure to halothane or heptanol. Histograms of gamma j values in transfected cells, in 10 experiments where greater than 100 transitions were measurable, displayed two peaks; 120-130 pS and 25-35 pS. The smaller size corresponded to channels that were occasionally detected in the parental cells. We therefore conclude that connexin32 forms gap junctions channels of the 120-130 pS size class.     

Fast pacing facilitates discontinuous action potential propagation between rabbit atrial cells

We examined the critical coupling conductance (G(C)) for propagation at different pacing cycle lengths (CLs) (1,000 and 400 ms). As G(C) was progressively reduced, propagation failed at a CL of 1,000 ms, whereas propagation succeeded at a CL of 400 ms over a range of G(C) values before failing at a CL of 400 ms at a lower G(C), showing facilitation of propagation at the shorter CL. Critical G(C) was (means +/- SE) 0.8 +/- 0.1 nS for a CL of 400 ms and 1.3 +/- 0.1 nS for a CL of 1,000 ms (a 63% increase, P < 0.002, n = 9 cell pairs). In 14 uncoupled cells, action potential duration at 30% repolarization (APD(30)) increased from 19.9 +/- 2.5 to 41.8 +/- 2.6 ms (P < 0.001) as CL decreased from 1,000 to 400 ms. In five cell pairs, critical G(C) with 4-aminopyridine (4-AP) was reduced to 0.4 +/- 0.1 nS at a CL of 1,000 ms (P < 0.05 compared with control solution), and critical G(C) in 4-AP was unchanged by decreasing CL to 400 ms. It is possible that the "remodeling" of atrial cells due to atrial fibrillation or tachycardia, which has been shown to produce a decrease in the transient outward current, may result in an enhanced ability to propagate, possibly facilitating further development of fibrillation under conditions of decreased cellular coupling.     

Electrical interactions between a real ventricular cell and an anisotropic two-dimensional sheet of model cells

We have extended our "coupling clamp" technique, in which we couple a real cell to a real-time simulation of a model cell, to now incorporate a real cardiac cell as the central element of a two-dimensional sheet of model cells, in which the coupling conductances may be different in the x and y directions and a specific region of lack of coupling conductance may serve as a resistive barrier. We stimulated the real cell in the central location and determined the critical size of the real cell for successful activation of the entire sheet. We found that this critical size was decreased when anisotropy was present compared with the isotropic case and was further decreased when the central site of stimulation was close to the resistive barrier. The heart normally has some degree of anisotropy, and it has been shown that the remodeling that occurs in peri-infarction zones produces a particular loss of lateral connections compared with end-to-end connections among heart cells. We propose that the normal existence of anisotropy and enhancement of the degree of anisotropy both by loss of lateral gap junctions and the development of resistive barriers may play a facilitating role in the development of ectopic foci that may lead to cardiac arrhythmias.     

Proposed mechanism of insulin-resistant glucose transport in the isolated guinea pig adipocyte. Small intracellular pool of glucose transporters

A marked resistance to the stimulatory action of insulin on glucose metabolism has previously been shown in guinea pig, compared to rat, adipose tissue and isolated adipocytes. The mechanism of insulin resistance in isolated guinea pig adipocytes has, therefore, been examined by measuring 125I-insulin binding, the stimulatory effect of insulin on 3-0-methylglucose transport and on lipogenesis from [3-3H]glucose, the inhibitory effect of insulin on glucagon-stimulated glycerol release, and the translocation of glucose transporters in response to insulin. The translocation of glucose transporters was assessed by measuring the distribution of specific D-glucose-inhibitable [3H]cytochalasin B binding sites among the plasma, and high and low density microsomal membrane fractions prepared by differential centrifugation from basal and insulin-stimulated cells. At a glucose concentration (0.5 mM) where transport is thought to be rate-limiting for metabolism, insulin stimulates lipogenesis from 30 to 80 fmol/cell/90 min in guinea pig cells and from 25 to 380 fmol/cell/90 min in rat cells with half-maximal effects at approximately 100 pM in both cell types. Insulin similarly stimulates 3-O-methylglucose transport from 0.40 to 0.70 fmol/cell/min and from 0.24 to 3.60 fmol/cell/min in guinea pig and rat fat cells, respectively. Nevertheless, guinea pig cells bind more insulin per cell than rat cells, and insulin fully inhibits glucagon-stimulated glycerol release. In addition, the differences between guinea pig and rat cells in the stimulatory effect of insulin on lipogenesis and 3-O-methylglucose transport cannot be explained by the greater cell size of the former compared to the latter (0.18 and 0.09 micrograms of lipid/cell, respectively). However, the number of glucose transporters in the low density microsomal membrane fraction prepared from basal guinea pig cells is markedly reduced compared to that from rat fat cells (12 and 70 pmol/mg of membrane protein, respectively) and the translocation of intracellular glucose transporters to the plasma membrane fraction in response to insulin is correspondingly reduced. These results suggest that guinea pig adipocytes are markedly resistant to the stimulatory action of insulin on glucose transport and that this resistance is the consequence of a relative depletion in the number of intracellular glucose transporters.     

Effect of simulated I(to) on guinea pig and canine ventricular action potential morphology

The transient outward current (I(to)) is a major repolarizing current in the heart. Marked reduction of I(to) density occurs in heart failure and is accompanied by significant action potential duration (APD) prolongation. To understand the species-dependent role of I(to) in regulating the ventricular action potential morphology and duration, we introduced simulated I(to) conductance in guinea pig and canine endocardial ventricular myocytes using the dynamic clamp technique and perforated patch-clamp recordings. The effects of simulated I(to) in both types of cells were complex and biphasic, separated by a clear density threshold of approximately 40 pA/pF. Below this threshold, simulated I(to) resulted in a distinct phase 1 notch and had little effect on or moderately prolonged the APD. I(to) above the threshold resulted in all-or-none repolarization and precipitously reduced the APD. Qualitatively, these results agreed with our previous studies in canine ventricular cells using whole cell recordings. We conclude that 1) contrary to previous gene transfer studies involving the Kv4.3 current, the response of guinea pig ventricular myocytes to a fully inactivating I(to) is similar to that of canine ventricular cells and 2) in animals such as dogs that have a broad cardiac action potential, I(to) does not play a major role in setting the APD.     

Characterization of impulse propagation at the microscopic level across geometrically defined expansions of excitable tissue: multiple site optical recording of transmembrane voltage (MSORTV) in patterned growth heart cell cultures

Impulse propagation across sudden expansions of excitable tissue has been shown to exhibit various forms of conduction disturbance on a macroscopic scale, ranging from small delays to unidirectional or complete conduction block. With the present study, we attempted to characterize systematically the dependence of impulse propagation on the geometry of the underlying excitable tissue on a microscopic scale by investigating the spatio-temporal pattern of transmembrane voltage changes associated with impulse propagation from a narrow cell strand to a large cell area using multiple site optical recording of transmembrane voltage (MSORTV) in conjunction with patterned growth of neonatal rat heart cells in culture. While action potential propagation was smooth in the case of funneled expansions, delays of variable size occurred during propagation into rectangular or incised expansions. Close to the abrupt expansion, which functionally represented an increased electrical load to the narrow cell strand, the delays were accompanied by marked distortions of the action potential upstroke, exhibiting, in extreme cases, an initial depolarization to 50% followed by a delayed secondary depolarization to 100% of the full-signal amplitude. These distortions, which were based on bidirectional electrotonic interactions across the transition, were maximal immediately downstream from the expansion. The maximal slowing of impulse conduction across abrupt expansions was, in agreement with recently published results obtained from two-dimensional computer simulations, always situated in the expanded region. At high stimulation rates, the delays sometimes turned into intermittent unidirectional blocks, as revealed by reverse stimulation. These blocks were always characterized by a marked abbreviation of the action potentials upstream from the region causing the block which might, in an appropriate network, facilitate reentry because of the associated shortening of the refractory period. Because the patterns were composed of cells having identical membrane properties, the results show that the local action potential shape can be modulated profoundly by the two- dimensional architecture of the underlying cell ensemble alone.     

Immunohistochemical demonstration of airway epithelial cell markers of guinea pig

The guinea pig (Cavea porcellus) is a mammalian non-rodent species in the Caviidae family. The sensitivity of the respiratory system and the susceptibility to infectious diseases allows the guinea pig to be a useful model for both infectious and non-infectious lung diseases such as asthma and tuberculosis. In this report, we demonstrated for the first time, the major cell types and composition in the guinea pig airway epithelium, using cell type-specific markers by immunohistochemical staining using the commercial available immunological reagents that cross-react with guinea pig. Our results revealed the availability of antibodies cross-reacting with airway epithelial cell types of basal, non-ciliated columnar, ciliated, Clara, goblet and alveolar type II cells, as well as those cells expressing Mucin 5AC, Mucin 2, Aquaporin 4 and Calcitonin Gene Related Peptide. The distribution of these various cell types were quantified in the guinea pig airway by immunohistochemical staining and were comparable with morphometric studies using an electron microscopy assay. Moreover, this study also demonstrated that goblet cells are the main secretory cell type in the guinea pig's airway, distinguishing this species from rats and mice. These results provide useful information for the understanding of airway epithelial cell biology and mechanisms of epithelial–immune integration in guinea pig models.     

Voltage-clamp studies of gap junctions between uterine muscle cells during term and preterm labor.

Gap junctions between myometrial cells increase dramatically during the final stages of pregnancy. To study the functional consequences, we have applied the double-whole-cell voltage-clamp technique to freshly isolated pairs of cells from rat circular and longitudinal myometrium. Junctional conductance was greater between circular muscle-cell pairs from rats delivering either at term (32 +/- 16 nS, mean +/- SD, n = 128) or preterm (26 +/- 17 nS, n = 33) compared with normal preterm (4.7 +/- 7.6 nS, n = 114) and postpartum (6.5 +/- 10 nS, n = 16); cell pairs from the longitudinal layer showed similar differences. The macroscopic gap junction currents decayed slowly from an instantaneous, constant-conductance level to a steady-state level described by quasisymmetrical Boltzmann functions of transjunctional voltage. In half of circular-layer cell pairs, the voltage dependence of myometrial gap junction conductance is more apparent at smaller transjunctional voltages (< 30 mV) than for other tissues expressing mainly connexin-43. This unusual degree of voltage dependence, although slow, operates over time intervals that are physiologically relevant for uterine muscle. Using weakly coupled pairs, we observed two unitary conductance states: 85 pS (85-90% of events) and 25 pS. These measurements of junctional conductance support the hypothesis that heightened electrical coupling between the smooth muscle cells of the uterine wall emerges late in pregnancy, in preparation for the massive, coordinate contractions of labor.     

A voltage-dependent persistent sodium current in mammalian hippocampal neurons

Currents generated by depolarizing voltage pulses were recorded in neurons from the pyramidal cell layer of the CA1 region of rat or guinea pig hippocampus with single electrode voltage-clamp or tight-seal whole-cell voltage-clamp techniques. In neurons in situ in slices, and in dissociated neurons, subtraction of currents generated by identical depolarizing voltage pulses before and after exposure to tetrodotoxin revealed a small, persistent current after the transient current. These currents could also be recorded directly in dissociated neurons in which other ionic currents were effectively suppressed. It was concluded that the persistent current was carried by sodium ions because it was blocked by TTX, decreased in amplitude when extracellular sodium concentration was reduced, and was not blocked by cadmium. The amplitude of the persistent sodium current varied with clamp potential, being detectable at potentials as negative as -70 mV and reaching a maximum at approximately -40 mV. The maximum amplitude at -40 mV in 21 cells in slices was -0.34 +/- 0.05 nA (mean +/- 1 SEM) and -0.21 +/- 0.05 nA in 10 dissociated neurons. Persistent sodium conductance increased sigmoidally with a potential between -70 and -30 mV and could be fitted with the Boltzmann equation, g = gmax/(1 + exp[(V' - V)/k)]). The average gmax was 7.8 +/- 1.1 nS in the 21 neurons in slices and 4.4 +/- 1.6 nS in the 10 dissociated cells that had lost their processes indicating that the channels responsible are probably most densely aggregated on or close to the soma. The half-maximum conductance occurred close to -50 mV, both in neurons in slices and in dissociated neurons, and the slope factor (k) was 5-9 mV. The persistent sodium current was much more resistant to inactivation by depolarization than the transient current and could be recorded at greater than 50% of its normal amplitude when the transient current was completely inactivated. Because the persistent sodium current activates at potentials close to the resting membrane potential and is very resistant to inactivation, it probably plays an important role in the repetitive firing of action potentials caused by prolonged depolarizations such as those that occur during barrages of synaptic inputs into these cells.     

Simulation of developmental changes in action potentials with ventricular cell models

During cardiomyocyte development, early embryonic ventricular cells show spontaneous activity that disappears at a later stage. Dramatic changes in action potential are mediated by developmental changes in individual ionic currents. Hence, reconstruction of the individual ionic currents into an integrated mathematical model would lead to a better understanding of cardiomyocyte development. To simulate the action potential of the rodent ventricular cell at three representative developmental stages, quantitative changes in the ionic currents, pumps, exchangers, and sarcoplasmic reticulum (SR) Ca²⁺ kinetics were represented as relative activities, which were multiplied by conductance or conversion factors for individual ionic systems. The simulated action potential of the early embryonic ventricular cell model exhibited spontaneous activity, which ceased in the simulated action potential of the late embryonic and neonatal ventricular cell models. The simulations with our models were able to reproduce action potentials that were consistent with the reported characteristics of the cells in vitro. The action potential of rodent ventricular cells at different developmental stages can be reproduced with common sets of mathematical equations by multiplying conductance or conversion factors for ionic currents, pumps, exchangers, and SR Ca²⁺ kinetics by relative activities.     

Propagation of normal beats and re-entry in a computational model of ventricular cardiac tissue with regional differences in action potential shape and duration

There is substantial experimental evidence from studies using both intact tissue and isolated single cells to support the existence of different cell types within the ventricular wall of the heart, each possessing different electrical properties. However other studies have failed to find these differences, and instead support the idea that electrical coupling in vivo between regions with different cell types smoothes out differences in action potential shape and duration. In this study we have used a computational model of electrical activation in heterogenous 2D and 3D cardiac tissue to investigate the propagation of both normal beats and arrhythmias. We used the Luo–Rudy dynamic model for guinea pig ventricular cells, with simplified Ca²⁺ handling and transmural heterogeneity in I_Ks and I_to. With normal cell-to-cell coupling, a layer of M cells was not necessary for the formation of an upright T wave in the simulated electrocardiogram, and the amplitude and configuration of the T wave was not greatly affected by the thickness and configuration of the M cell layer. Transmural gradients in repolarisation pushed re-entrant waves with an intramural filament towards either the base or the apex of the ventricles, and caused transient break up of re-entry with a transmural filament.     

Effect of thymol on calcium handling in mammalian ventricular myocardium

Concentration-dependent effects of thymol on calcium handling were studied in canine and guinea pig cardiac preparations (Langendorff-perfused guinea pig hearts, canine ventricular trabeculae, canine sarcoplasmic reticular vesicles and single ryanodine receptors). Thymol induced a concentration-dependent negative inotropic action in both canine and guinea pig preparations (EC(50) = 297 +/- 12 microM in dog). However, low concentrations of thymol reduced intracellular calcium transients in guinea pig hearts without decreasing contractility. At higher concentrations both calcium transients and contractions were suppressed. In canine sarcoplasmic reticular vesicles thymol induced rapid release of calcium (V(max) = 0.47 +/- 0.04 nmol s(-1), EC(50) = 258 +/- 21 microM, Hill coefficient = 3.0 +/- 0.54), and decreased the activity of the calcium pump (EC(50) = 253 +/- 4.7 microM, Hill coefficient = 1.62 +/- 0.05). Due to the less sharp concentration-dependence of the ATPase inhibition, this effect was significant from 50 microM, whereas the thymol-induced calcium release only from 100 microM. In single ryanodine receptors incorporated into artificial lipid bilayer thymol induced long lasting openings, having mean open times increased with 3 orders of magnitude, however, the specific conductance of the channel remained unaltered. This effect of thymol was not voltage-dependent and failed to prevent the binding of ryanodine. In conclusion, the negative inotropic action of thymol can be explained by reduction in calcium content of the sarcoplasmic reticulum due to the combination of the thymol-induced calcium release and inhibition of the calcium pump. The calcium-sensitizer effect, observed at lower thymol concentrations, indicates that thymol is likely to interact with the contractile machinery also.     

Modelling changes in transmural propagation and susceptibility to arrhythmia induced by volatile anaesthetics in ventricular tissue

Volatile anaesthetics such as halothane, isoflurane and sevoflurane inhibit membrane currents contributing to the ventricular action potential. Transmural variation in the extent of current blockade induces differential effects on action potential duration (APD) in the endocardium and epicardium which may be pro-arrhythmic. Biophysical modelling techniques were used to simulate the functional impact of anaesthetic-induced blockade of membrane currents on APD and effective refractory period (ERP) in rat endocardial and epicardial cell models. Additionally, the transmural conduction of excitation waves in 1-dimensional cell arrays, the tissue's vulnerability to arrhythmogenesis and dynamic behaviour of re-entrant excitation in 2-dimensional cell arrays were studied. Simulated anaesthetic exposure reduced APD and ERP in both epicardial and endocardial cell models. The reduction in APD was greater in endocardial than epicardial cells, reducing transmural APD dispersion consistent with experimental data. However, the transmural ERP dispersion was augmented. All three anaesthetics increased the width of the tissue's vulnerable window during which a premature stimulus could induce unidirectional conduction block but only halothane reduced the critical size of ventricular substrates necessary to initiate and sustain re-entrant excitation. All three anaesthetics accelerated the rate of re-entrant excitation waves, but only halothane prolonged the lifespan of re-entry. These data illustrate in silico, that modest changes in ion channel conductance abbreviate rat ventricular APD and ERP, reduce transmural APD dispersion, but augment transmural ERP dispersion. These changes collectively enhance the propensity for arrhythmia generation and provide a substrate for re-entry circuits with a longer half life than in control conditions.     

Aberrant cell-to-cell coupling in Ca2+-overloaded guinea pig ventricular muscles

To investigate how intercellular coupling can be changed during Ca²⁺ overloading of ventricular muscle, we studied Ca²⁺ signals in individual cells and the histochemistry of the major gap junction channel, connexin43 (Cx43), using multicellular preparations. Papillary muscles were obtained from guinea pig ventricles and loaded with rhod-2. Sequential Ca²⁺ images of surface cells were obtained with a confocal microscope. In intact muscles, all cells showed simultaneous Ca²⁺ transients in response to field stimulation over a field of view of 0.3 x 0.3 mm². In severely Ca²⁺-overloaded muscles, obtained by high-frequency stimulation in nonflowing Krebs solution, cells became less responsive to stimulation. Furthermore, nonsimultaneous but serial onsets of Ca²⁺ transients were often detected, suggesting a propagation delay of action potentials. The time lag of the onset between two aligned cells was sometimes as long as 100 ms. Similar lags were also observed in muscles with gap junction channels inhibited by heptanol. To investigate whether the phosphorylation state of Cx43 is affected in Ca²⁺-overloaded muscles, the distributions of phosphorylated and nonphosphorylated Cx43 were determined using specific antibodies. Most of the Cx43 was phosphorylated in the nonoverloaded muscles, whereas nonphosphorylated Cx43 was significantly elevated in severely Ca²⁺-overloaded muscles. Our results suggest that the propagation delay of action potential within a small area, a few square millimeters, can be a cause of abnormal conduction and a microreentry in Ca²⁺-overloaded heart. Inactivation of Na⁺ channels and inhibition of gap junctional communication may underlie the cell-to-cell propagation delay. Ca²⁺ transient; connexin43; propagation delay; gap junction; arrhythmia     

A spontaneously active focus drives a model atrial sheet more easily than a model ventricular sheet

Tachycardias can be produced when focal activity at ectopic locations in either the atria or the ventricles propagates into the surrounding quiescent myocardium. Isolated rabbit atrioventricular nodal cells were coupled by an electronic circuit to a real-time simulation of an array of cell models. We investigated the critical size of an automatic focus for the activation of two-dimensional arrays made up of either ventricular or atrial model cells. Over a range of coupling conductances for the arrays, the critical size of the focus cell group for successful propagation was smaller for activation of an atrial versus a ventricular array. Failure of activation of the arrays at smaller focus sizes was due to the inhibition of pacing of the nodal cells. At low levels of coupling conductance, the ventricular arrays required larger sizes of the focus due to failure of propagation even when the focus was spontaneously active. The major differences between activation of the atrial and ventricular arrays is due to the higher membrane resistance (lower inward rectifier current) of the atrial cells.     

In vitro toxicity of alloxan for guinea pig B cells: comparison with rat B cells

Previous studies have shown that guinea pigs are resistant to the in vivo diabetogenic action of alloxan and that this resistance may be accompanied by a regeneration of B cells in the initial days following administration of the drug. In the studies reported here, we used the measurement of insulin and glucagon released over a 7-day culture period as indices of islet cell viability and examined effects of in vitro exposure to alloxan upon subsequent release of insulin and glucagon from guinea pig (alloxan-resistant) and rat (alloxan-sensitive) islet cell cultures. An alloxan dose-dependent decrease in subsequent insulin release was found. However, whereas the lowest concentration of the drug (1 mM) produced a significant depression in insulin release in rat islet cultures, with maximal depression occurring after exposure to 5 mM alloxan, insulin release from guinea pig cultures was not significantly depressed by 1 or 2 mM alloxan, and 5 mM alloxan treatment produced a submaximal depression. Furthermore, insulin release from guinea pig but not rat cultures increased transiently at between 6 and 18 hr during the first day following exposure to all doses of alloxan. Treatment with high doses of the drug (40 mM or greater) caused the same maximal chronic depression of insulin release for both species. In contrast, glucagon release from cultures of both species was not affected significantly following alloxan treatment. Thus, guinea pig B cells are more resistant than those of the rat to the action of alloxan, but this resistance can be overcome by employing high doses of the drug. Other factions unidentified by the present studies may also be involved in the failure of guinea pigs to develop diabetes following in vivo treatment with alloxan.     

Regulation of potassium levels by Müller cells in the vertebrate retina

The membrane properties of Müller cells, the principal glial cells of the vertebrate retina, have been characterized in a series of physiological experiments on freshly dissociated cells. In species lacking a retinal circulation (tiger salamander, rabbit, guinea pig), the end-foot of the Müller cell has a much higher K+ conductance than do other cell regions. In species with retinal circulation (mouse, cat, owl monkey) the K+ conductance of the end-foot is greater than the conductance of the proximal process of the cell. In these species, however, the K+ conductance of the soma and distal process is equal to, or greater than, the end-foot conductance. Müller cells also possess four voltage-dependent ion channels, including an inward rectifying K+ channel. These membrane specializations may aid in the regulation of extracellular K+ levels by Müller cells in the retina. High end-foot conductance shunts excess K+ out through the end-foot, where it diffuses into the vitreous humor. In vascularized retinae, excess K+ may also be transferred to the ablumenal wall of capillaries, where it could be transported into the blood.