Publications by authors named "Sperelakis N"

Background: Propagation of simulated action potentials (APs) was previously studied in short single chains and in two-dimensional sheets of myocardial cells 123. The present study was undertaken to examine propagation in a long single chain of cells of various lengths, and with varying numbers of gap-junction (g-j) channels, and to compare propagation velocity with the cable properties such as the length constant (lambda).

Methods And Results: Simulations were carried out using the PSpice program as previously described.

View Article and Find Full Text PDF

Background: The effect of depth on propagation velocity within a bundle of cardiac muscle fibers is likely to be an important factor in the genesis of some heart arrhythmias. MODEL AND METHODS: The velocity profile of simulated action potentials propagated down a bundle of parallel cardiac muscle fibers was examined in a cross-section of the bundle using a PSpice model. The model (20 x 10) consisted of 20 chains in parallel, each chain being 10 cells in length.

View Article and Find Full Text PDF

Transverse propagation was previously found to occur in a two-dimensional model of cardiac muscle using the PSpice software program for electronic circuit design and analysis. Longitudinal propagation within each chain, and transverse propagation between parallel chains, occurred even when there were no gap-junction (g-j) channels inserted between the simulated myocardial cells either longitudinally or transversely. In those studies, there were pronounced edge (boundary) effects and end-effects even within single chains.

View Article and Find Full Text PDF

Background: In previous PSpice modeling studies of simulated action potentials (APs) in parallel chains of cardiac muscle, it was found that transverse propagation could occur between adjacent chains in the absence of gap-junction (gj) channels, presumably by the electric field (EF) generated in the narrow interstitial space between the chains. Transverse propagation was sometimes erratic, the more distal chains firing out of order.

Methods: In the present study, the propagation of complete APs was studied in a 2-dimensional network of 100 cardiac muscle cells (10 x 10 model).

View Article and Find Full Text PDF

Background: Previously, only the rising phase of the action potential (AP) in cardiac muscle and smooth muscle could be simulated due to the instability of PSpice upon insertion of a second black box (BB) into the K+ leg of the basic membrane unit. This restriction was acceptable because only the transmission of excitation from one cell to the next was investigated.

Methods: In the current work, the repolarization of the AP was accomplished by inserting a second BB into the Ca++ leg of the basic membrane unit.

View Article and Find Full Text PDF

Background: In previous studies on propagation of simulated action potentials (APs) in cardiac muscle using PSpice modeling, we reported that a second black-box (BB) could not be inserted into the K+ leg of the basic membrane unit because that caused the PSpice program to become very unstable. Therefore, only the rising phase of the APs could be simulated. This restriction was acceptable since only the mechanism of transmission of excitation from one cell to the next was being investigated.

View Article and Find Full Text PDF

Background: We previously demonstrated that transverse propagation of excitation (cardiac action potentials simulated with PSpice) could occur in the absence of low-resistance connections (gap--junction channels) between parallel chains of myocardial cells. The transverse transmission of excitation between the chains was strongly dependent on the longitudinal resistance of the interstitial fluid space between the chains: the higher this resistance, the closer the packing of the parallel chains within the bundle. The earlier experiments were carried out with 2-dimensional sheets of cells: 2 x 3, 3 x 4, and 5 x 5 models (where the first number is the number of parallel chains and the second is the number of cells in each chain).

View Article and Find Full Text PDF

Background: Propagation of repolarization is a phenomenon that occurs in cardiac muscle. We wanted to test whether this phenomenon would also occur in our model of simulated action potentials (APs) of cardiac muscle (CM) and smooth muscle (SM) generated with the PSpice program.

Methods: A linear chain of 5 cells was used, with intracellular stimulation of cell #1 for the antegrade propagation and of cell #5 for the retrograde propagation.

View Article and Find Full Text PDF

The effect of adding many gap-junctions (g-j) channels between contiguous cells in a linear chain on transverse propagation between parallel chains was examined in a 5 x 5 model (5 parallel chains of 5 cells each) for cardiac muscle. The action potential upstrokes were simulated using the PSpice program for circuit analysis. Either a single cell was stimulated (cell A1) or the entire chain was stimulated simultaneously (A-chain).

View Article and Find Full Text PDF

Background: We previously examined transverse propagation of action potentials between 2 and 3 parallel chain of cardiac muscle cells (CMC) simulated using the PSpice program. The present study was done to examine transverse propagation between 5 parallel chains in an expanded model of CMC and smooth muscle cells (SMC).

Methods: Excitation was transmitted from cell to cell along a strand of 5 cells not connected by low-resistance tunnels (gap-junction connexons).

View Article and Find Full Text PDF

Activation of a two-dimensional sheet network (5 parallel chains of 5 cells each) of simulated intestinal smooth muscle cells (SMCs) by one interstitial cell of Cajal (ICC) was modeled by PSpice simulation. The network of 25 cells was not interconnected by gap-junction channels; instead, excitation was transmitted by the electric field that develops in the junctional clefts (JC) when the prejunctional membrane fires an action potential (AP). Transverse propagation between the parallel chains occurs similarly.

View Article and Find Full Text PDF

Propagation of action potentials in cardiac muscle and smooth muscle were simulated using the PSpice program. Excitation was transmitted from cell to cell along a strand of 6 cells (cardiac muscle) or 10 cells (smooth muscle) either not connected (control) or connected by low-resistance tunnels (gap-junction connexons). A significant negative cleft potential (V(jv) ) develops in the narrow junctional cleft when the pre-JM fires.

View Article and Find Full Text PDF

Propagation of action potentials between parallel chains of cardiac muscle cells was simulated using the PSpice program. Excitation was transmitted from cell to cell along a strand of three or four cells not connected by low-resistance tunnels (gap-junction connexons) in parallel with one or two similar strands. Thus, two models were used: a 2 x 3 model (two parallel chains of three cells each) and a 3 x 4 model (three parallel chains of four cells each).

View Article and Find Full Text PDF

To evaluate the potency of levosimendan, a newly developed cardiotonic agent, as a phosphodiesterase-3 inhibitor, we examined its effects on the L-type Ca(2+) current (I(Ca,L)) in single human atrial cells using the whole-cell voltage-clamp method. Levosimendan significantly increased I(Ca,L) in a concentration-dependent manner (E(max), 139.0 +/- 1.

View Article and Find Full Text PDF

Tyrosine protein kinase (Tyr-PK) regulation of L-type Ca2+ channel (CaL) current was studied in COS-7 cells expressing vascular smooth muscle-type alpha1C-b with no auxiliary subunit by using a whole-cell voltage clamp. The averaged peak amplitude of CaL currents was -0.33 +/- 0.

View Article and Find Full Text PDF

To investigate the possible regulation of large-conductance Ca2+-activated K+ channels (BKCa) by tyrosine phosphatases (Tyr-PPs), single-channel currents of myocytes from rat mesenteric artery were recorded in open cell-attached patches. Two structurally different Tyr-PP inhibitors, sodium orthovanadate (Na3VO4) and dephostatin, were used. The channels (236 pS) evoked at +40 mV and pCa 6, were significantly inhibited by 1 mM Na3VO4 (-81+/-3%, n = 10; P < 0.

View Article and Find Full Text PDF

To clarify interactions between the cytoskeleton and activity of L-type Ca(2+) (Ca(L)) channels in vascular smooth muscle (VSM) cells, we investigated the effect of disruption of actin filaments and microtubules on the L-type Ca(2+) current [I(Ba(L))] of cultured VSM cells (A7r5 cell line) using whole cell voltage clamp. The cells were exposed to each disrupter for 1 h and then examined electrophysiologically and morphologically. Results of immunostaining using anti-alpha-actin and anti-alpha-tubulin antibodies showed that colchicine disrupted both actin filaments and microtubules, cytochalasin D disrupted only actin filaments, and nocodazole disrupted only microtubules.

View Article and Find Full Text PDF

We investigated the role of K(+) channels in the regulation of vascular tone in de-endothelialized porcine coronary artery. Isometric force and intracellular Ca(2+) ([Ca(2+)](i)) under resting conditions were increased by treatment with 4-aminopyridine (4-AP, 1 mM), an inhibitor of voltage-dependent K(+) (K(v)) channels, but not by tetraethylammonium chloride (TEA, 1 mM) or charybdotoxin (100 nM), both inhibitors of Ca(2+)-activated K(+) (K(Ca)) channels, or glibenclamide (10 microM), an inhibitor of ATP-sensitive K(+) channels. Under stimulated conditions with 9,11-dideoxy-11alpha, 9alpha-epoxymethano-prostaglandin F(2alpha) (U46619), 4-AP as well as TEA or charybdotoxin increased isometric force and [Ca(2+)](i), but not glibenclamide.

View Article and Find Full Text PDF

We investigated the action of calmidazolium (CMZ), an inhibitor of calmodulin (CaM), on the L-type Ca2+ currents (ICa(L)) of cultured vascular smooth muscle (VSM) cells (A7r5 cell line), by using the whole-cell voltage-clamp method. All experiments were conducted at room temperature (24-25 degrees C). The peak IBa (Ca2+ channel current with 5 mM Ba2+ as charge carrier) was evoked every 15 s by a test potential to +10 mV from a holding potential of -60 mV.

View Article and Find Full Text PDF