We recorded transmembrane potential in whole cell recording mode from small clusters (2-4 cells) of spontaneously beating 7-day embryonic chick ventricular cells after 1-3 days in culture and investigated effects of the blockers D-600, diltiazem, almokalant, and Ba 2ϩ . Electrical activity in small clusters is very different from that in reaggregates of several hundred embryonic chick ventricular cells, e.g., TTX-sensitive fast upstrokes in reaggregates vs. TTX-insensitive slow upstrokes in small clusters (maximum upstroke velocity ϳ100 V/s vs. ϳ10 V/s). On the basis of our voltageand current-clamp results and data from the literature, we formulated a Hodgkin-Huxley-type ionic model for the electrical activity in these small clusters. The model contains a Ca 2ϩ current (ICa), three K ϩ currents (IKs, IKr, and IK1), a background current, and a seal-leak current. ICa generates the slow upstroke, whereas IKs, IKr, and IK1 contribute to repolarization. All the currents contribute to spontaneous diastolic depolarization, e.g., removal of the seal-leak current increases the interbeat interval from 392 to 535 ms. The model replicates the spontaneous activity in the clusters as well as the experimental results of application of blockers. Bifurcation analysis and simulations with the model predict that annihilation and single-pulse triggering should occur with partial block of I Ca. Embryonic chick ventricular cells have been used as an experimental model to investigate various aspects of spontaneous beating of cardiac cells, e.g., mutual synchronization, regularity of beating, and spontaneous initiation and termination of reentrant rhythms; our model allows investigation of these topics through numerical simulation.pacemaker; seal-leak current; rapid delayed rectifier potassium current block; slow inward calcium current block; bifurcation analysis SPONTANEOUS ACTIVITY based on generation of the pacemaker potential (spontaneous phase 4, or diastolic, depolarization) is not normally found in adult ventricular muscle in situ, nor is it normally found in single cells freshly isolated from adult ventricular muscle. In contrast, early enough during development, ventricular muscle (or areas of the heart destined to eventually become ventricular muscle) can beat spontaneously (1, 97). Spontaneous electrical activity can also be seen in single cells and in small clusters of cells isolated from the embryonic chick ventricle (10,17,26,49,51,78,95), in the embryonic mouse ventricle (117), and in the neonatal rat ventricle (86).After a couple of days in culture, the electrical activity in an isolated embryonic chick ventricular cell, in a small cluster of a few such cells, or in a sparse monolayer is very different from that in situ or in a reaggregate of hundreds or thousands of cells isolated from the ventricle. For example, when trypsin-dispersed ventricular cells from 7-day embryonic chick hearts are used, the upstroke velocity is much lower in single cells, in small clusters of cells, and in sparse monolayers (17,49,51,95) than...

1. Whole-cell and single-channel patch-clamp recordings of calcium (Ca2+) currents were made in acutely dissociated neurons from the medial septum (MS) and nucleus of the diagonal band (nDB) of adult guinea pig. Barium (Ba2+) was used as the charge carrier across the Ca2+ channel and multiple channel types were identified in different cell types. 2. Both low-voltage-activated (LVA) and high-voltage-activated (HVA) currents were distinguished on the basis of steady-state voltage dependence, activation and inactivation properties, and pharmacological sensitivity. HVA currents had activation thresholds approximately 20 mV more positive than LVA currents. Steady-state inactivation of HVA currents was approximately 50% when the holding potential was shifted from -80 to -40 mV. 3. The dihydropyridines had consistent effects on HVA currents. The amplitude was increased and the activation threshold shifted by 10 mV in the hyperpolarizing direction in the presence of the agonist Bay K 8644 (2-5 microM). The antagonist nifedipine (10 microM) produced approximately 50% inhibition of HVA currents from a holding potential of -80 mV. 4. A second component of the HVA current was blocked by omega-conotoxin (omega-CTX) (300-700 nM). At a holding potential of -80 mV, omega-CTX inhibited 45% of the HVA current. 5. LVA currents were activated near -70 mV and displayed time-dependent inactivation during a 200- to 300-ms voltage step. Voltage-dependent inactivation of LVA currents was also observed and could be described by a single Boltzman relationship with a half-inactivation potential of -84 mV. LVA currents were not significantly changed by Bay K 8644 and were not blocked by low concentrations of nifedipine or omega-CTX. 6. Single voltage-gated Ca2+ channels were investigated using cell-attached patches. In these experiments, 100 mM Ba2+ was used in the patch pipette and the membrane potential was zeroed with isotonic potassium (K+)-aspartate. A low-conductance channel was activated at negative potentials and inactivated rapidly during a 200- to 300-ms voltage step. Unitary amplitudes were determined at different membrane potentials with single-channel conductances calculated to be 7.8 +/- 1.2 (SD) pS. These channels were not blocked by nifedipine (10 microM) and appeared similar to T channels previously reported in both peripheral and central neurons. Ensemble averages from cell-attached patches of T channels resembled LVA currents recorded in the whole-cell configuration.(ABSTRACT TRUNCATED AT 400 WORDS)

The transmembrane potential is recorded from small isopotential clusters of 2-4 embryonic chick ventricular cells spontaneously generating action potentials. We analyze the cycle-to-cycle fluctuations in the time between successive action potentials (the interbeat interval or IBI). We also convert an existing model of electrical activity in the cluster, which is formulated as a Hodgkin-Huxley-like deterministic system of nonlinear ordinary differential equations describing five individual ionic currents, into a stochastic model consisting of a population of ∼20 000 independently and randomly gating ionic channels, with the randomness being set by a real physical stochastic process (radio static). This stochastic model, implemented using the Clay-DeFelice algorithm, reproduces the fluctuations seen experimentally: e.g., the coefficient of variation (standard deviation/mean) of IBI is 4.3% in the model vs. the 3.9% average value of the 17 clusters studied. The model also replicates all but one of several other quantitative measures of the experimental results, including the power spectrum and correlation integral of the voltage, as well as the histogram, Poincaré plot, serial correlation coefficients, power spectrum, detrended fluctuation analysis, approximate entropy, and sample entropy of IBI. The channel noise from one particular ionic current (I), which has channel kinetics that are relatively slow compared to that of the other currents, makes the major contribution to the fluctuations in IBI. Reproduction of the experimental coefficient of variation of IBI by adding a Gaussian white noise-current into the deterministic model necessitates using an unrealistically high noise-current amplitude. Indeed, a major implication of the modelling results is that, given the wide range of time-scales over which the various species of channels open and close, only a cell-specific stochastic model that is formulated taking into consideration the widely different ranges in the frequency content of the channel-noise produced by the opening and closing of several different types of channels will be able to reproduce precisely the various effects due to membrane noise seen in a particular electrophysiological preparation.