Transverse propagation in an expanded PSpice model for cardiac muscle with gap-junction ion channels

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. Transverse velocity increased with increase in model size. The present study was performed to examine boundary effects on transverse propagation velocity when the length of the chains was held constant at 10 cells and the number of parallel chains was varied from 3 to 5, to 7, to 10, and to 20. The number of g-j channels was either zero, both longitudinally and transversely (0/0), or 100/100. Some experiments were also made at 100/0, 1/1, and 10/10. Transverse velocity and overall velocity (both longitudinal and transverse components) was calculated from the measured total propagation time (TPT), i.e., the elapsed time between when the first action potential (AP) and the last AP crossed the zero potential level. The transverse g-j channels were placed only at the ends of each chain, such that propagation would occur in a zigzag pattern. Electrical stimulation was applied intracellularly between cells A1 and A2. It was found that, with no g-j channels (0/0), overall velocity increased almost linearly when more and more chains were placed in parallel. In contrast, with many g-j channels (100/100), there was a much flatter relationship between overall velocity and number of parallel chains. The difference in velocities with 0/0 channels and 100/100 channels was reduced as the number of chains was increased. In conclusion, edges have important effects on propagation velocity (overall and transverse) in cardiac muscle simulations.     

Electrical impedance tomography imaging using a priori ultrasound data

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. Transverse velocity increased with increase in model size. The present study was performed to examine boundary effects on transverse propagation velocity when the length of the chains was held constant at 10 cells and the number of parallel chains was varied from 3 to 5, to 7, to 10, and to 20. The number of g-j channels was either zero, both longitudinally and transversely (0/0), or 100/100. Some experiments were also made at 100/0, 1/1, and 10/10. Transverse velocity and overall velocity (both longitudinal and transverse components) was calculated from the measured total propagation time (TPT), i.e., the elapsed time between when the first action potential (AP) and the last AP crossed the zero potential level. The transverse g-j channels were placed only at the ends of each chain, such that propagation would occur in a zigzag pattern. Electrical stimulation was applied intracellularly between cells A1 and A2. It was found that, with no g-j channels (0/0), overall velocity increased almost linearly when more and more chains were placed in parallel. In contrast, with many g-j channels (100/100), there was a much flatter relationship between overall velocity and number of parallel chains. The difference in velocities with 0/0 channels and 100/100 channels was reduced as the number of chains was increased. In conclusion, edges have important effects on propagation velocity (overall and transverse) in cardiac muscle simulations.     

Boundary effects influence velocity of transverse propagation of simulated cardiac action potentials

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 × 3, 3 × 4, and 5 × 5 models (where the first number is the number of parallel chains and the second is the number of cells in each chain). The purpose of the present study was to enlarge the model size to 7 × 7, thus enabling the transverse velocities to be compared in models of different sizes (where all circuit parameters are identical in all models). This procedure should enable the significance of the role of edge (boundary) effects in transverse propagation to be determined.     

Transverse propagation of action potentials between parallel chains of cardiac muscle and smooth muscle cells in PSpice simulations

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).     

Activation of intestinal smooth muscle cells by interstitial cells of Cajal in simulation studies

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. The ICC cell was connected to cell E5 of the network [5th cell of the 5th (E) chain] via a high-resistance junction. The stimulating current, applied to the ICC cell interior, was made to resemble the endogenous undershooting slow wave (I(SW)). An I(SW) of 2.4 nA (over a rise time of 4 ms) took the ICC cell from a resting potential (RP) of -80 mV to a membrane potential of -41 mV. The slow wave produced a large negative cleft potential in the JC (V(JC); ICC-E5). The V(jc) brought the postjunctional membrane of E5 to threshold, causing this cell to fire an AP. This, in turn, propagated throughout the SMC network. If the ICC cell was given an RP of -55 mV (like SMC) and a slow wave of 40 mV amplitude (I(SW) of 1.8 nA), it still activated the SMC network. This was also true when the ICC cell was made excitable (developing an overshooting, fast-rising AP). In summary, one ICC cell displaying a slow wave was capable of activating a network of SMC in the absence of gap junctions.     

Effect of transverse gap-junction channels on transverse propagation in an enlarged PSpice model of cardiac muscle

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.     

Propagation of action potentials between parallel chains of cardiac muscle cells in PSpice simulation

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). The entire surface membrane of each cell fired nearly simultaneously, and nearly all the propagation time was spent at the cell junctions, thus giving a staircase-shaped propagation profile. The junctional delay time between contiguous cells in a chain was about 0.2-0.5 ms. A significant negative cleft potential develops in the narrow junctional clefts, whose magnitude depends on several factors, including the radial cleft resistance (Rjc). The cleft potential (Vjc) depolarizes the postjunctional membrane to threshold by a patch-clamp action. Therefore, one mechanism for the transfer of excitation from one cell to the next is by the electric field (EF) that is generated in the junctional cleft when the prejunctional membrane fires. Propagation velocity increased with elevation of Rjc. With electrical stimulation of the first cell of the first strand (cell A1), propagation rapidly spread down that chain and then jumped to the second strand (B chain), followed by jumping to the third strand (C chain) when present. The rapidity by which the parallel chains became activated depended on the longitudinal resistance of the narrow extracellular cleft between the parallel strands (Rol2). The higher the Rol2 resistance, the faster the propagation (lower propagation time) over the cardiac muscle sheet (2-dimensional). The transverse resistance of the cleft had no effect. When the first cell of the second strand (cell B1) was stimulated, propagation spread down the B chain and jumped to the other two strands (A and C) nearly simultaneously. When cell C1 was stimulated, propagation traveled down the C chain and jumped to the B chain, followed by excitation of the A chain. Thus, there was transverse propagation of excitation as longitudinal propagation was occurring. Therefore, transmission of excitation by the EF mechanism can occur between myocardial cells lying closely parallel to one another without the requirement of a specialized junction.     

The intrinsic electrophysiological characteristics of fly lobula plate tangential cells: I. Passive membrane properties

The passive membrane properties of the tangential cells in the fly lobula plate (CH, HS, and VS cells, Fig. 1) were determined by combining compartmental modeling and current injection experiments. As a prerequisite, we built a digital base of the cells by 3D-reconstructing individual tangential cells from cobalt-stained material including both CH cells (VCH and DCH cells), all three HS cells (HSN, HSE, and HSS cells) and most members of the VS cell family (Figs. 2, 3). In a first series of experiments, hyperpolarizing and depolarizing currents were injected to determine steady-state I-V curves (Fig. 4). At potentials more negative than resting, a linear relationship holds, whereas at potentials more positive than resting, an outward rectification is observed. Therefore, in all subsequent experiments, when a sinusoidal current of variable frequency was injected, a negative DC current was superimposed to keep the neurons in a hyperpolarized state. The resulting amplitude and phase spectra revealed an average steady-state input resistance of 4 to 5 M and a cut-off frequency between 40 and 80 Hz (Fig. 5). To determine the passive membrane parameters R _m (specific membrane resistance), R _i (specific internal resistivity), and C _m (specific membrane capacitance), the experiments were repeated in computer simulations on compartmental models of the cells (Fig. 6). Good fits between experimental and simulation data were obtained for the following values: R _m = 2.5 kcm², R _i = 60 cm, and C _m = 1.5 F/cm² for CH cells; R _m = 2.0 kcm², R _i = 40 cm, and C _m = 0.9 F/cm² for HS cells; R _m = 2.0 kcm², R _i = 40 cm, and C _m = 0.8 F/cm² for VS cells. An error analysis of the fitting procedure revealed an area of confidence in the R _m -R _i plane within which the R _m -R _i value pairs are still compatible with the experimental data given the statistical fluctuations inherent in the experiments (Figs. 7, 8). We also investigated whether there exist characteristic differences between different members of the same cell class and how much the exact placement of the electrode (within ±100 m along the axon) influences the result of the simulation (Fig. 9). The membrane parameters were further examined by injection of a hyperpolarizing current pulse (Fig. 10). The resulting compartmental models (Fig. 11) based on the passive membrane parameters determined in this way form the basis of forthcoming studies on dendritic integration and signal propagation in the fly tangential cells (Haag et al., 1997; Haag and Borst, 1997).     

Retention of basic electrophysiologic properties by human sweat duct cells in primary culture

Summary The present investigation was undertaken to examine the usefulness of cultured human sweat duct cells for ion transport and related studies in the genetic disease, cystic fibrosis. Electrical properties of cultured duct (CD) cells were compared with electrical properties of microperfused duct (MPD) cells. The resting apical membrane potential (V _a ) of the CD cells was −26.4±0.9 mV,n=158 cells as compared to −24.3±0.6 mV,n=105 of MPD cells. The Na⁺−K⁺ pump inhibitor ouabain, when applied to the apical surface of the CD cells and basolateral surface of MPD cells, depolarized both CD cells (from −28.6±3.6 to −16.8±2.4 mV,n=5) and MPD cells (from −23.8±0.5 mV to −19.5±1.8 mV,n=6). The Na⁺ conductance inhibitor amiloride applied to the apical surface hyperpolarized the apical membrane potentials (V_a) of CD cells and MPD cells by −13.2±1.4 mV,n=43 and −34.3±3.1 mV,n=19), respectively, indicating the presence of amiloride sensitive Na⁺ channels in both groups of cells. However, the amiloride sensitivity of CD cells was dependent on the age of the culture. Cl⁻ substitution at the apical side by the impermeant anion gluconate depolarized the V _a of CD cells and MPD cells by 12.2±0.9 mV,n=32 and 37.9±4.3 mV,n=12, respectively. The effect of β-adrenergic agonist isoproterenol (IPR), was inconsistent. In CD cells, IPR either hyperpolarized (ΔV _a =−8.3±1.2mV,n=5) or depolarized (ΔV _a =8.2±2.3 mV,n=4) or had no effect,n=2. In contrast, most of the MPD cells did not respond to IPR, but three cells had a varied response to IPR. Our results suggest that CD cells, like MPD cells, retain significant Na⁺ and Cl⁻ conductances. CD cells seem to have developed a higher sensitivity to β-adrenergic stimulation in tissue culture as compared to MPD cells. This work was supported by grants from the National Institutes of Health, Bethesda, MD, DK26547, Getty Oil Co., the Gillette Co., Cystic Fibrosis Research Inc., and the U.S. National Cystic Fibrosis Foundation.     

BK Ca Channels Activating at Resting Potential without Calcium in LNCaP Prostate Cancer Cells

Large-conductance Ca²⁺-dependent K⁺ (BK_Ca) channels are activated by intracellular Ca²⁺ and membrane depolarization in an allosteric manner. We investigated the pharmacological and biophysical characteristics of a BK_Ca-type K⁺ channel in androgen-dependent LNCaP (lymph node carcinoma of the prostate) cells with novel functional properties, here termed BK_L. K⁺ selectivity, high conductance, activation by Mg²⁺ or NS1619, and inhibition by paxilline and penitrem A largely resembled the properties of recombinant BK_Ca channels. However, unlike conventional BK_Ca channels, BK_L channels activated in the absence of free cytosolic Ca²⁺ at physiological membrane potentials; the half-maximal activation voltage was shifted by about −100 mV compared with BK_Ca channels. Half-maximal Ca²⁺-dependent activation was observed at 0.4 μM for BK_L (at −20 mV) and at 4.1 μM for BK_Ca channels (at +50 mV). Heterologous expression of hSlo1 in LNCaP cells increased the BK_L conductance. Expression of hSlo-β1 in LNCaP cells shifted voltage-dependent activation to values between that of BK_L and BK_Ca channels and reduced the slope of the P_open (open probability)-voltage curve. We propose that LNCaP cells harbor a so far unknown type of BK_Ca subunit, which is responsible for the BK_L phenotype in a dominant manner. BK_L-like channels are also expressed in the human breast cancer cell line T47D. In addition, functional expression of BK_L in LNCaP cells is regulated by serum-derived factors, however not by androgens.     

Microbial fuel cells for energy self-sufficient domestic wastewater treatment—a review and discussion from energetic consideration

As the microbial fuel cell (MFC) technology is getting nearer to practical applications such as wastewater treatment, it is crucial to consider the different aspects that will make this technology viable in the future. In this paper, we provide information about the specifications of an energy self-sufficient MFC system as a basis to extrapolate on the potential benefits and limits of a future MFC-based wastewater treatment plant. We particularly emphasize on the importance of two crucial parameters that characterize an MFC: its electromotive force (E _emf) and its internal resistance (R _int). A numerical projection using state-of-art values (E _emf = 0.8 V and R _int = 5 Ω) emphasized on the difficulty at this moment to reach self-sufficiency using a reasonable number of MFCs at the laboratory scale. We found that a realistic number of MFCs to provide enough voltage (=5 V) at a sufficient current (=0.8 A) to power a pump requiring 4 W would be of 13 MFCs in series and 10 stacks of MFCs in parallel, resulting in a total number of 130 MFCs. That would result in a treatment capacity of 144 L of domestic wastewater (0.5 g-COD L⁻¹) per day. The total MFC system would be characterized by an internal resistance of 6.5 Ω.     

One reason for increased seizure susceptibility of hippocampus compared with neocortex

In this study we compared the membrane resting potential and action potential (AP) activation thresholds of neocortical layer 2/3 and CA1 hippocampal pyramidal cells in brain slices from 6–8-day old mice. The activation threshold was −37 ± 2 mV in the neocortical pyramids (5 cells), and −50 ± 1 mV in the CA1 ones (5 cells). The observed difference in the AP activation thresholds may account for a higher excitability of hippocampus as compared to neocortex. The article is submitted by the author in English.     

The Sensitivity of the Human Kv1.3 (hKv1.3) Lymphocyte K+ Channel to Regulation by PKA and PKC is Partially Lost in HEK 293 Host Cells

cDNA encoding the full-length hKv1.3 lymphocyte channel and a C-terminal truncated (Δ459-523) form that lacks the putative PKA Ser⁴⁶⁸ phosphorylation site were stably transfected in human embryonic kidney (HEK) 293 cells. Immunostaining of the transfected cells revealed a distribution at the plasma membrane that was uniform in the case of the full-length channel whereas clustering was observed in the case of the truncated channel. Some staining within the cell cytoplasm was found in both instances, suggesting an active process of biosynthesis. Analyses of the K⁺ current by the patch-clamp technique in the whole cell configuration showed that depolarizing steps to 40 mV from a holding potential (HP) of −80 mV elicited an outward current of 2 to 10 nA. The current threshold was positive to −40 mV and the current amplitude increased in a voltage-dependent manner. The parameters of activation were −5.7 and −9.9 mV (slope factor) and −35 mV (half activation, V _0.5) in the case of the full-length and truncated channels, respectively. The characteristics of the inactivation were 14.2 and 24.6 mV (slope factor) and −17.3 and −39.0 mV (V _0.5) for the full-length and truncated channels, respectively. The activation time constant of the full-length channel for potentials ranging from −30 to 40 mV decreased from 18 to 12 msec whereas the inactivation time constant decreased from 6600 msec at −30 mV to 1800 msec at 40 mV. The unit current amplitude measured in cells bathing in 140 mm KCl was 1.3 ± 0.1 pA at 40 mV, the unit conductance, 34.5 pS and the zero current voltage, 0 mV. Both forms of the channels were inhibited by TEA, 4-AP, Ni²⁺ and charybdotoxin. In contrast to the native (Jurkat) lymphocyte Kv1.3 channel that is fully inhibited by PKA and PKC, the addition of TPA resulted in 34.6 ± 7.3% and 38.7 ± 9.4% inhibition of the full-length and the truncated channels, respectively. 8-BrcAMP induced a 39.4 ± 5.4% inhibition of the full-length channel but had no effect (8.6 ± 8.3%) on the truncated channel. Cell dialysis with alkaline phosphatase had no effects, suggesting that the decreased sensitivity of the transfected channels to PKA and PKC was not due to an already phosphorylated channel. Patch extract experiments suggested that the hKv1.3 channel was partially sensitive to PKA and PKC. Cotransfecting the Kvβ1.2 subunit resulted in a decrease in the value of the time constant of inactivation of the full-length channel but did not modify its sensitivity to PKA and PKC. The cotransfected Kvβ2 subunit had no effects. Our results indicate that the hKv1.3 lymphocyte channel retains its electrophysiological characteristics when transfected in the Kvβ-negative HEK 293 cell line but its sensitivity to modulation by PKA and PKC is significantly reduced. Received: 18 June 1997/Revised: 7 October 1997     

P2Y(2) receptor-mediated inhibition of amiloride-sensitive short circuit current in M-1 mouse cortical collecting duct cells

Extracellular nucleotides modulate renal ion transport. Our previous results in M-1 cortical collecting duct cells indicate that luminal and basolateral ATP via P2Y₂ receptors stimulate luminal Ca²⁺-activated Cl⁻ channels and inhibit Na⁺ transport. Here we address the mechanism of ATP-mediated inhibition of Na⁺ transport. M-1 cells had a transepithelial voltage (V _te ) of −31.4 ± 1.3 mV and a transepithelial resistance (R _te ) of 1151 ± 28 Ωcm². The amiloride-sensitive short circuit current (I _sc ) was −28.0 ± 1.1 μA/cm². The ATP-mediated activation of Cl⁻ channels was inhibited when cytosolic Ca²⁺ increases were blocked with cyclopiazonic acid (CPA). Without CPA the ATP-induced [Ca²⁺]_i increase was paralleled by a rapid and transient R _te decrease (297 ± 51 Ωcm²). In the presence of CPA, basolateral ATP led to an R _te increase by 144 ± 17 Ωcm² and decreased V _te from −31 ± 2.6 to −26.6 ± 2.5 mV. I _sc dropped from −28.6 ± 2.4 to −21.6 ± 1.9 μA/cm². Similar effects were observed with luminal ATP. In the presence of amiloride, ATP was without effect. This reflects ATP-mediated inhibition of Na⁺ absorption. Lowering [Ca²⁺]_i by removal of extracellular Ca²⁺ did not alter the ATP effect. PKC inhibition or activation were without effect. Na⁺ absorption was activated by pH_i alkalinization and inhibited by pH_i acidification. ATP slightly acidified M-1 cells by 0.05 ± 0.005 pH units, quantitatively not explaining the ATP-induced effect. In summary this indicates that extracellular ATP via luminal and basolateral P2Y₂ receptors inhibits Na⁺ absorption. This effect is not mediated via [Ca²⁺]_i, does not involve PKC and is to a small part mediated via intracellular acidification. Received: 9 February 2001/Revised: 17 May 2001     

Electrophysiological characterization of murine HL-5 atrial cardiomyocytes

HL-5 cells are cultured murine atrial cardiomyocytes and have been used in studies to address important cellular and molecular questions. However, electrophysiological features of HL-5 cells have not been characterized. In this study, we examined such properties using whole cell patch-clamp techniques. Membrane capacitance of the HL-5 cells was from 8 to 62 pF. The resting membrane potential was –57.8 ± 1.4 mV (n = 51). Intracellular injection of depolarizing currents evoked action potentials (APs) with variable morphologies in 71% of the patched cells. Interestingly, the incidence of successful, current-induced APs positively correlated with the hyperpolarizing degrees of resting membrane potentials (r = 0.99, P < 0.001). Only a few of the patched cells (4 of 51, 7.8%) exhibited spontaneous APs. The muscarinic agonist carbachol activated the acetylcholine-activated K⁺ current and significantly shortened the duration of APs. Immunostaining confirmed the presence of the muscarinic receptor type 2 in HL-5 cells. The hyperpolarization-activated cation current (I_f) was detected in 39% of the patched cells. The voltage to activate 50% of I_f channels was –73.4 ± 1.2 mV (n = 12). Voltage-gated Na⁺, Ca²⁺, and K⁺ currents were observed in the HL-5 cells with variable incidences. Compared with the adult mouse cardiomyocytes, the HL-5 cells had prolonged APs and small outward K⁺ currents. Our data indicate that HL-5 cells display significant electrophysiological heterogeneity of morphological appearance of APs and expression of functional ion channels. Compared with adult murine cardiomyocytes, HL-5 cells show an immature phenotype of cardiac AP morphology. action potential; ion channel; muscarinic receptor     

Suppressive effect of an activator of ATP-dependent potassium channels, flocalin, on electrical and contractile activities of smooth muscles of the guinea-pig ureter

In experiments on isolated segments or strips obtained from the guinea-pig ureter, we showed, using a sucrose-gap technique, that application of an activator of ATP-dependent potassium channels (K_ATP), (flocalin (PF-5), suppresses generation of action potentials (APs) by ureter smooth muscle cells (SMCs). Pre-incubation of the ureter preparations under study in Krebs solution containing 1 to 10 μM PF-5 results initially in a decrease in the frequency of oscillations preceding an AP plateau, shortening of this plateau, and, later on, complete inhibition of AP generation. In the presence of PF-5, spikes induced by hyperpotassium depolarization were also inhibited, while a tonic component of such depolarization underwent a mild decrease. The data obtained indicate that PF-5 modulates the entry of Ca²⁺ ions through L-type voltage-dependent channels in the SMC membrane. Shortening of the plateau and suppression of the spikes initiated by application of an activator of voltage-dependent L-type potassium channels, Bay K 8644, can be considered a confirmation of the modulatory influence of PF-5 on voltage-dependent L-type potassium channels. It seems possible that Bay K 8644 can be used under experimental conditions for initiation and long-lasting modulation of APs generated by the ureter SMC instead of corresponding neurotransmitters. We hypothesize that voltage-dependent entry of Ca²⁺ ions into SMCs depends significantly on the PF-5-induced activation of K_ATP channels of the ureter SMCs. Neirofiziologiya/Neurophysiology, Vol. 37, Nos. 5/6, pp. 403–409, September–December, 2005.     

Theoretical characterization of SOME amides and esters DERIVATIVES of valproic acid

The equilibrium structures, the planarity of the C(=O)X linkage and the nature of the chemical bond in the Y−C(=O)−XR₁R₂ [where: Y= −CH−(CH₂−CH₂−CH₃)₂, X=N,O and R₁, R₂= H; alkyl and aryl groups and lone pair electrons (lp)] molecular fragment of derivates of Valproic acid (Vpa) with antiepileptic activity were studied systematically by means of B3LYP calculations and topological analysis of the electron localization function (ELF). The covariance parameter cov[Ω_i, Ω_j] reveals a dominating delocalization effect between the lone pair V(O₁), V(X) and the electron density of the H−C and H−X₁ bonds resulting from the existence of not only non-conventional intramolecular hydrogen bonding patterns as C−H...O/N but also a weak closed-shell stabilizing interaction type arising from a dihydrogen bonding as C−H...H−N, where H...H contacts at a significantly shorter distance than twice the hydrogen atom van der Waals radius. The analyzed data derived from ELF domains were found to be in agreement with the known features and properties of the hydrogen bonding interactions discussed in this work.     

Composition and distribution of internal resistance in three types of microbial fuel cells

High internal resistance is a key problem limiting the power output of the microbial fuel cell (MFC). Therefore, more knowledge about the internal resistance is essential to enhance the performance of the MFC. However, different methods are used to determine the internal resistance, which makes the comparison difficult. In this study, three different types of MFCs were constructed to study the composition and distribution of internal resistance. The internal resistance (R _i) is partitioned into anodic resistance (R _a), cathodic resistance (R _c), and ohmic resistance () according to their origin and the design of the MFCs. These three resistances were then evaluated by the “current interrupt” method and the “steady discharging” method based on the proposed equivalent circuits for MFCs. In MFC-A, MFC-B, and MFC-C, the R _i values were 3.17, 0.35, and 0.076 Ω m², the values were 2.65, 0.085, and 0.008 Ω m², the R _a values were 0.055, 0.115, and 0.034 Ω m², and the R _c values were 0.466, 0.15, and 0.033 Ω m², respectively. For MFC-B and MFC-C, the remarkable decrease in R _i compared with the two-chamber MFC was mainly ascribed to the decline in and R _c. In MFC-C, the membrane electrodes’ assembly lowered the ohmic resistance and facilitated the mass transport through the anode and cathode electrodes, resulting in the lowest R _i among the three types.     

Fish Gill Respiratory Cells in Culture: A New Model for Cl−-secreting Epithelia

Primary cultures of sea bass gill cells grown on permeable membranes form a confluent, polarized, functional tight epithelium as characterized by electron microscopy and electrophysiological and ion transport studies. Cultured with normal fetal bovine serum (FBS) and mounted in an Ussing chamber, the epithelium presents a small short-circuit current (I _sc : 1.4 ± 0.3 μA/cm²), a transepithelial voltage (V _t ) of 12.7 ± 2.7 mV (serosal positive) and a high transepithelial resistance (R _t : 12302 ± 2477 Ω× cm²). A higher degree of differentiation and increased ion transport capacities are observed with cells cultured with sea bass serum: numerous, organized microridges characteristic of respiratory cells are present on the apical cell surface and there are increased I _sc (11.9 ± 2.5 μA/cm²) and V _t (25.9 ± 1.7 mV) and reduced R _t (4271 ± 568 Ω× cm²) as compared with FBS-treated cells. Apical amiloride addition (up to 100 μm) had no effect on I _sc . The I _sc , correlated with an active Cl⁻ secretion measured as the difference between ³⁶Cl⁻ unidirectional fluxes, was partly blocked by serosal ouabain, bumetanide, DIDS or apical DPC or NPPB and stimulated by serosal dB-cAMP. It is concluded that the chloride secretion is mediated by a Na⁺/K⁺/2Cl⁻ cotransport and a Cl⁻/HCO₃ ⁻ exchanger both responsible for Cl⁻ entry through the basolateral membrane and by apical cAMP-sensitive Cl⁻ channels. This study gives evidence of a functional, highly differentiated epithelium in cultures composed of fish gill respiratorylike cells, which could provide a useful preparation for studies on ion transport and their regulation. Furthermore, the chloride secretion through these cultures of respiratorylike cells makes it necessary to reconsider the previously accepted sea water model in which the chloride cells are given the unique role of ion transport through fish gills. Received: 12 July 1996/Revised: 5 November 1996     

Synthesis, structures, and magnetic properties of one-dimensional Fe-M (M = Ni, Cu) coordination polymers bridged by nitroprusside

Self-assembling [Fe(CN)₅(NO)]²⁻ and [M(L)]²⁺ (M = Ni, Cu; L = macrocycles) led to one-dimensional coordination polymers, [Ni(L1)][Fe(CN)₅(NO)] · 2H₂O (1) with parallel chains and [Cu(L2)][Fe(CN)₅(NO)] · 3H₂O (2) exhibiting a slanted chain structure. Compound 1 contains a planar macrocycle L1 coordinated to a slightly distorted octahedral Ni(II) ion in which the planarity of L1 gives rise to piling up chains in parallel. In contrast, a more flexible macrocyclic ligand L2 in 2 that surrounds a Cu center with a tetragonal elongation has bulky cyclohexyl groups together with pendant methyl side groups. The presence of the methyl groups on L2 in a chain makes the cyclohexyl groups in an adjacent chain tilted against the CuN₄ basal plane with the methyl groups, eventually resulting in the slanted chain structure. Magnetic data demonstrate that antiferromagnetic interactions (J ≈ −0.13 cm⁻¹) are operating although the paramagnetic centers are linked by the long diamagnetic [Fe(CN)₅(NO)]²⁻ anion.