Mechanisms Underlying the Antifibrillatory Action of Hyperkalemia in Guinea Pig Hearts

Hyperkalemia increases the organization of ventricular fibrillation (VF) and may also terminate it by mechanisms that remain unclear. We previously showed that the left-to-right heterogeneity of excitation and wave fragmentation present in fibrillating guinea pig hearts is mediated by chamber-specific outward conductance differences in the inward rectifier potassium current (I_K1). We hypothesized that hyperkalemia-mediated depolarization of the reversal potential of I_K1 (E_K1) would reduce excitability and thereby reduce VF excitation frequencies and left-to-right heterogeneity. We induced VF in Langendroff-perfused guinea pig hearts and increased the extracellular K⁺ concentration ([K⁺]_o) from control (4 mM) to 7 mM (n = 5) or 10 mM (n = 7). Optical mapping enabled spatial characterization of excitation dominant frequencies (DFs) and wavebreaks, and identification of sustained rotors (>4 cycles). During VF, hyperkalemia reduced the maximum DF of the left ventricle (LV) from 31.5 ± 4.7 Hz (control) to 23.0 ± 4.7 Hz (7.0 mM) or 19.5 ± 3.6 Hz (10.0 mM; p < 0.006), the left-to-right DF gradient from 14.7 ± 3.6 Hz (control) to 4.4 ± 1.3 Hz (7 mM) and 3.2 ± 1.4 Hz (10 mM), the number of DF domains, and the incidence of wavebreak in the LV and interventricular regions. During 10 mM [K⁺]_o, the rotation period and core area of sustained rotors in the LV increased, and VF often terminated. Two-dimensional computer simulations mimicking experimental VF predicted that clamping E_K1 to normokalemic values during simulated hyperkalemia prevented all of the hyperkalemia-induced VF changes. During hyperkalemia, despite the shortening of the action potential duration, depolarization of E_K1 increased refractoriness, leading to a slowing of VF, which effectively superseded the influence of I_K1 conductance differences on VF organization. This reduced the left-to-right excitation gradients and heterogeneous wavebreak formation. Overall, these results provide, to our knowledge, the first direct mechanistic insight into the organization and/or termination of VF by hyperkalemia.     

The relationship between single-channel and whole-cell conductance in the T-type Ca2+ channel CaV3.1

In T-type Ca²⁺ channels, macroscopic I_Ba is usually smaller than I_Ca, but at high Ca²⁺ and Ba²⁺, single-channel conductance (γ) is equal. We investigated γ as a function of divalent concentration and compared it to macroscopic currents using Ca_V3.1 channels studied under similar experimental conditions (TEA_o and K_i). Single-channel current-voltage relationships were nonlinear in a way similar to macroscopic open-channel I/Vs, so divalent γ was underestimated at depolarized voltages. To estimate divalent γ, concentration dependence, i_Div, was measured at voltages <−50 mV. Data were well described by Langmuir isotherms with γ_max(Ca²⁺) of 9.5 ± 0.4 pS and γ_max(Ba²⁺) of 10.3 ± 0.5 pS. Apparent K_M was lower for Ca²⁺ (2.3 ± 0.7 mM) than for Ba²⁺ (7.9 ± 1.3 mM). A subconductance state with an amplitude 70% that of the main state was observed, the relative occupancy of which increased with increasing Ca²⁺. As predicted by γ, macroscopic G_maxCa was larger than G_maxBa at 5 mM (G_maxCa²⁺/Ba:²⁺1.43 ± 0.14) and similar at 60 mM (G_maxCa²⁺/Ba:²⁺1.10 ± 0.02). However, over the range of activation, I_Ca was larger than I_Ba under both conditions. This was a consequence of the fact that V_rev was more negative for I_Ba than for I_Ca, so that the driving force determining I_Ba was smaller than that determining I_Ca over the range of potentials in standard current-voltage relationships.     

Characteristics of L-Type Ca2+ Channels in the Membrane of Mesenteric Artery Myocytes from Genetically Hypertensive Rats

Using the standard voltage-clamp technique in the whole-cell mode, we studied the characteristics of barium currents (I _Ba; Ba²⁺ concentration in the external solution was 5 mM) carried through L-type Ca²⁺ channels in the membrane of myocytes of the resistive mesenteric artery from normotensive and genetically hypertensive rats (NR and GHR, respectively). To perforate the membrane, we used amphotericin B. The arbitrary density of I _Ba through the plasma membrane of GHR myocytes significantly exceeded this parameter in the NR group. For both animal groups, activation curves plotted as the dependence of the membrane conductance (G _Ba) on the membrane potential were not significantly different: the membrane potential for half activation (V _0.5) of I _Ba in the NR myocytes was equal to 1.0 ± 0.3 mV with slope factor k = 6.3 ± 0.4 mV, whereas in the GHR myocytes V _0.5 = -1.6 ± 0.2 mV and k = 6.2 ± 0.5 mV. The stationary inactivation curves for I _Ba differed significantly: in the NR myocytes, V _0.5 = -24.2 ± 0.4 mV and k = 8.3 ± 0.2 mV, whereas in the GHR myocytes such parameters were, respectively, -21.4 ± 0.4 and 8.7 ± 0.3 mV. The pattern of intersection of stationary activation and stationary inactivation curves for I _Ba was indicative of the existence of a window current, i.e., the non-inactivating component of I _Ba within the -40 to ±20 mV range; the phenomenon was clearly pronounced in the GHR myocytes. Differences in the arbitrary density of integral I _Ba and window current were observed. These differences can cause an increased tone of the blood vessels in hypertensive animals.     

Short-term exposure to waterborne free silver has acute effects on membrane current of Xenopus oocytes

Waterborne free silver can cause osmo- and ionoregulatory disturbances in freshwater organisms. The effects of a short-term exposure to extracellular Ag⁺ ions on membrane currents were investigated in voltage-clamped defolliculated Xenopus oocytes. At a holding potential of − 60 mV, ionic silver (1 μM Ag⁺) increased inward currents (=I_Ag) from − 8 ± 2 nA to − 665 ± 41 nA (n = 74; N = 27). I_Ag activated within 2 min of silver exposure and then rose impetuously. This current was largely reversible by washout and repeatable. I_Ag reversed around − 30 mV and rectified slightly at more positive potentials. Na⁺-free bath conditions reduced the silver-induced current to a smaller but sustained current. The response to silver was abolished by the Cl⁻ channel blockers DIDS and SITS, whereas niflumic acid strongly potentiated I_Ag. Intraoocyte injection of AgNO₃ to about 1 mM [Ag]_i strongly potentiated I_Ag. Extracellular application of either dithiothreitol (DTT), a compound known to reduce disulfide bridges, or l-cysteine abolished Ag⁺-activated increase of membrane current. In contrast, n-ethylmaleimide (NEM) which oxidizes SH-groups potentiated I_Ag. Hypoosmotic bath solution significantly increased I_Ag whereas hyperosmolar conditions attenuated I_Ag. The activation of I_Ag was largely preserved after chelation of cytosolic Ca²⁺ ions with BAPTA/AM. Taken together, these data suggest that Xenopus oocytes are sensitive to short-term exposure to waterborne Ag⁺ ions and that the elicited membrane currents result from extra- and intracellular action of Ag⁺ ions on peptide moieties at the oocyte membrane but may also affect conductances after internalization.     

Ni2+ Slows the Activation Kinetics of High-Voltage-Activated Ca2+ Currents in Cortical Neurons: Evidence for a Mechanism of Action Independent of Channel-Pore Block

The effects of Ni²⁺ were evaluated on slowly-decaying, high-voltage-activated (HVA) Ca²⁺ currents expressed by pyramidal neurons acutely dissociated from guinea-pig piriform cortex. Whole-cell, patch-clamp recordings were performed with Ba²⁺ as the charge carrier. Ni²⁺ blocked HVA Ba²⁺ currents (I _Bas) with an EC₅₀ of approximately 60 μm. Additionally, after application of nonsaturating Ni²⁺ concentrations, residual currents activated with substantially slower kinetics than both total and Ni²⁺-sensitive I _Bas. None of the pharmacological components of slowly decaying, HVA currents activated with kinetics significantly different from that of total currents, indicating that the effect of Ni²⁺ on I _Bas kinetics cannot be attributed to the preferential inhibition of a fast-activating component. The effect of Ni²⁺ on I _Ba amplitude was voltage-independent over the potential range normally explored in our experiments (−60 to +20 mV), hence the Ni²⁺-dependent decrease of I _Ba activation rate is not due to a voltage- and time-dependent relief from block. Moreover, Ni²⁺ significantly reduced I _Ba deactivation speed upon repolarization, which also is not compatible with a depolarization-dependent unblocking mechanism. The dependence on Ni²⁺ concentration of the I _Ba activation-rate reduction was remarkably different from that found for I _Ba block, with an EC₅₀ of ∼20 μm and a Hill coefficient of ∼1.73 vs.∼1.10. These results demonstrate that Ni²⁺, besides inhibiting the I _Bas under study probably by exerting a blocking action on the pore of the underlying Ca²⁺ channels, also interferes with Ca²⁺-channel gating kinetics, and strongly suggest that the two effects depend on Ni²⁺ occupancy of binding sites at least partly distinct. Received: 13 July 2000/Revised: 9 November 2000     

Ion-dependent Inactivation of Barium Current through L-type Calcium Channels

It is widely believed that Ba²⁺ currents carried through L-type Ca²⁺ channels inactivate by a voltage- dependent mechanism similar to that described for other voltage-dependent channels. Studying ionic and gating currents of rabbit cardiac Ca²⁺ channels expressed in different subunit combinations in tsA201 cells, we found a phase of Ba²⁺ current decay with characteristics of ion-dependent inactivation. Upon a long duration (20 s) depolarizing pulse, I_Ba decayed as the sum of two exponentials. The slow phase (τ ≈ 6 s, 21°C) was parallel to a reduction of gating charge mobile at positive voltages, which was determined in the same cells. The fast phase of current decay (τ ≈ 600 ms), involving about 50% of total decay, was not accompanied by decrease of gating currents. Its amplitude depended on voltage with a characteristic U-shape, reflecting reduction of inactivation at positive voltages. When Na⁺ was used as the charge carrier, decay of ionic current followed a single exponential, of rate similar to that of the slow decay of Ba²⁺ current. The reduction of Ba²⁺ current during a depolarizing pulse was not due to changes in the concentration gradients driving ion movement, because Ba²⁺ entry during the pulse did not change the reversal potential for Ba²⁺. A simple model of Ca²⁺-dependent inactivation (Shirokov, R., R. Levis, N. Shirokova, and E. Ríos. 1993. J. Gen. Physiol. 102:1005–1030) robustly accounts for fast Ba²⁺ current decay assuming the affinity of the inactivation site on the α₁ subunit to be 100 times lower for Ba²⁺ than Ca²⁺.     

Barium inhibition of sodium ion transport in toad bladder

The effect of Ba²⁺ on Na⁺ transport and electrical characteristics of toad bladder was determined from change produced in short circuit current (I_sc, epithelial, apical and basal-lateral potentials (ψ_t, ψ_a, ψ_b), epithelial and membrane resistances (R_t, R_a, R_b) and shunt resistance (R_s). Mucosal Ba²⁺ had no effect. Serosal Ba²⁺ reduced I_sc, ψ_t, ψ_a, and ψ_b, but had no effect on R_t, R_a, R_b and R_s. Minimal effective Ba²⁺ concentration was 5 · 10^?5 M. The phenomenon was reversed by Ba²⁺ removal, but not by 86 mM serosal K⁺. Ba²⁺ inhibition of I_sc did not impair the response to vasopressin which was quantitatively the same as controls. ψ_a with Ba²⁺ equalled ψ_b. After Ba²⁺ inhibition, ouabain produced no further decrease in ψ_t and I_sc. Ba²⁺ exposure after ouabain did not decrease ψ_t and I_sc. The results suggest that Ba²⁺ inhibits the basal-lateral electrogenic Na⁺ pump.     

External Ba2+ block of human Kv1.5 at neutral and acidic pH: evidence for Ho+-induced constriction of the outer pore mouth at rest

Previous studies have shown that low pH_o accelerates depolarization-induced inactivation and decreases the macroscopic conductance by reducing channel availability. To test the hypothesis that outer pore constriction underlies the decreased conductance at low pH_o, external Ba²⁺ was used to examine the accessibility of the channel pore at rest under neutral and acidic conditions. At pH_o 7.4, Ba²⁺ block of closed channels follows a monoexponential time course and involves a low-affinity superficial site (K_D ≅ 1 mM, −80 mV, 0 mM ) and a high-affinity site (K_D ≅ 4 μM) deeper in the pore. Depolarization promotes Ba²⁺ dissociation and an analytical model incorporating state-dependent changes of Ba²⁺ affinity is presented that replicates the frequency dependence of the time course and the extent of block. Open-channel block by Ba²⁺ is weak. At pH_o 5.5, both the access to and exit from the deep site is inhibited. These results are consistent with a low-pH_o-induced conformational change in the outer pore that prevents Ba²⁺ binding at rest or unbinding during depolarization. If a pore constriction is involved, similar to that proposed to occur during P/C-type inactivation, this would imply that closed-state inactivation in Kv1.5 occurs under acidic conditions.     

Speeding the Recovery from Ultraslow Inactivation of Voltage-Gated Na+ Channels by Metal Ion Binding to the Selectivity Filter: A Foot-on-the-Door?

Slow inactivated states in voltage-gated ion channels can be modulated by binding molecules both to the outside and to the inside of the pore. Thus, external K⁺ inhibits C-type inactivation in Shaker K⁺ channels by a “foot-in-the-door” mechanism. Here, we explore the modulation of a very long-lived inactivated state, ultraslow inactivation (I_US), by ligand binding to the outer vestibule in voltage-gated Na⁺ channels. Blocking the outer vestibule by a mutant μ-conotoxin GIIIA substantially accelerated recovery from I_US. A similar effect was observed if Cd²⁺ was bound to a cysteine engineered to the selectivity filter (K1237C). In K1237C channels, exposed to 30 μM Cd²⁺, the time constant of recovery from I_US was decreased from 145.0 ± 10.2 s to 32.5 ± 3.3 s (P < 0.001). Recovery from I_US was only accelerated if Cd²⁺ was added to the bath solution during recovery (V = −120 mV) from I_US, but not when the channels were selectively exposed to Cd²⁺ during the development of I_US (−20 mV). These data could be explained by a kinetic model in which Cd²⁺ binds with high affinity to a slow inactivated state (I_S), which is transiently occupied during recovery from I_US. A total of 50 μM Cd²⁺ produced an ∼8 mV hyperpolarizing shift of the steady-state inactivation curve of I_S, supporting this kinetic model. Binding of lidocaine to the internal vestibule significantly reduced the number of channels entering I_US, suggesting that I_US is associated with a conformational change of the internal vestibule of the channel. We propose a molecular model in which slow inactivation (I_S) occurs by a closure of the outer vestibule, whereas I_US arises from a constriction of the internal vestibule produced by a widening of the selectivity filter region. Binding of Cd²⁺ to C1237 promotes the closure of the selectivity filter region, thereby hastening recovery from I_US. Thus, Cd²⁺ ions may act like a foot-on-the-door, kicking the I_S gate to close.     

Kinetics of the cis-to-planar interconversion of cis-diaqua(1,4,7,11-tetraazacyclotetradecane)nickel(II) ion

In order to examine the effects of coordinated hydroxide ion and free hydroxide ion in configurational conversion of a tetraamine macrocyclic ligand complex, the kinetics of the cis-to-planar interconversion of cis-[Ni(isocyclam)(H₂O)₂]²⁺ (isocyclam, 1,4,7,11-tetraazacyclotetradecane) has been studied spectrophotometrically in basic aqueous solution. The interconversion requires the inversion of one sec-NH center of the folded cis-complex to have the planar species. Kinetic data are satisfactorily fitted by the rate law, R = k_OH[OH⁻][cis-[Ni(isocyclam)(H₂O)₂]²⁺], where k_OH = 3.84 × 10³ dm³ mol⁻¹ s⁻¹ at 25.0 ± 0.1 °C with I = 0.10 mol dm⁻³ (NaClO₄). The large ΔH^≠, 61.7 ± 3.2 kJ mol⁻¹, and the large positive ΔS^≠, 30.2 ± 10.8 J K⁻¹ mol⁻¹, strongly support a free-base-catalyzed mechanism for the reaction.     

Complexation study of europium(III) and curium(III) with urea in aqueous solution investigated by time-resolved laser-induced fluorescence spectroscopy

The complex formation of europium(III) and curium(III) with urea in aqueous solution has been studied at I = 0.1 M (NaClO₄), room temperature and trace metal concentrations in the pH-range of 1-8 at various ligand concentrations using time-resolved laser-fluorescence spectroscopy. While for curium(III) the luminescence maximum is red shifted upon complexation, in case of europium(III) emission wavelengths remain unaltered but a significant change in peak splitting occurs. Both heavy metals form weak complexes of the formulae ML³⁺ and MLOH²⁺ with urea. Stability constants were determined to be log β₁₁₀ = −0.12 ± 0.05 and log β_11-1 = −6.86 ± 0.15 for europium(III) and log β₁₁₀ = −0.28 ± 0.12 and log β_11-1 = −7.01 ± 0.15 for curium(III).     

Structural and spectroscopic characterisation of the holmium double-decker partially oxidised and bi-radical phthalocyanine complexes with iodine

Two crystals of holmium(III) double-decker iodine doped phthalocyanines, HoPc₂I_5/3 (I) and HoPc₂I (II), were grown directly in the reaction of holmium chips with 1,2-dicyanobenzene under versatile quantity of iodine at 180-160 °C. The complex I crystallises in the P4/mcc space group of tetragonal system, while the complex II crystallises in the P2/c space group of monoclinic system. The space group of P4/mcc and z = 1 requires that the Ho(III) atom is statistically disordered in the HoPc₂I_5/3 structure. The iodine atoms form linear symmetrical triiodide ions in I, while the I⁻ ions in II. Assignment of iodine species as in the HoPc₂I_5/3 and I⁻ in HoPc₂I complexes point to the +5/9 and +1 oxidation state of the HoPc₂ unit in these complexes. Thus one Pc macrocycle of the double-decker HoPc₂ units has a non-integer oxidation state of −1.222 in I, while both Pc-rings are one-electron oxidised radical Pc⁻ in II. Magnetic susceptibilities of HoPc₂I_5/3 and HoPcI at room temperature are 4.56 × 10⁻² and 5.12 × 10⁻² emu/mol and the calculated magnetic moments are 10.46 and 11.08 μ_B, respectively. UV-Vis spectroscopic measurement of I and II in benzene solution were carried out and discussed.     

Ecology of aquatic Ranunculus communities under the Mediterranean climate

The Iberian Peninsula encompasses more than 80% of the species richness of European aquatic ranunculi. The floristic diversity of the phytocoenosis characterised by aquatic Ranunculus and the main physical–chemical factors of the water were studied in 43 localities of the central Iberian Peninsula. Four aquatic Ranunculus communities are found in most of the aquatic environments. These are species-poor and have an uneven distribution: three species of Batrachium are heterophyllous and their communities are distributed in different aquatic ecosystems on silicated substrates; one species is homophyllous and its community occurs in various aquatic ecosystems with carbonated waters. In the Mediterranean climate, Ranunculus species are present in different habitats, as shown by the results of all the statistical analyses. Ranunculus trichophyllus communities occur in base-rich waters with a high buffering capacity (2273.44 ± 794.57 mg CaCO₃ L⁻¹) and a high concentration of cations (Ca²⁺, 121 ± 33.12 mg L⁻¹; Mg²⁺, 71.64 ± 82.77 mg L⁻¹), nitrates (2.89 ± 4.80 mg L⁻¹), ammonium (2.19 ± 1.36 mg L⁻¹) and sulphates (216.25 ± 218.54 mg L⁻¹). Ranunculus penicillatus communities are found in flowing waters with a high concentration of phosphates (0.48 ± 0.6 mg L⁻¹) and intermediate buffering capacity (683.66 ± 446.76 mg CaCO₃ L⁻¹). Both Ranunculus pseudofluitans and Ranunculus peltatus communities grow in waters with low buffering capacity (R. pseudofluitans, 385.91 ± 209.2 mg CaCO₃ L⁻¹; R. peltatus, 263.3 ± 180.36 mg CaCO₃ L⁻¹), and a low concentration of cations (R. pseudofluitans: Ca²⁺, 12.57 ± 9.42 mg L⁻¹; Mg²⁺, 3.42 ± 1.67 mg L⁻¹; R. peltatus: Ca²⁺, 15 ± 18.26 mg L⁻¹; Mg²⁺, 6.26 ± 8.89 mg L⁻¹) and nutrients (R. pseudofluitans: nitrates, 0.23 ± 0.2 mg L⁻¹; phosphates, 0.09 ± 0.1 mg L⁻¹; R. peltatus: nitrates, 0.19 ± 0.21 mg L⁻¹; phosphates, 0.09 ± 0.12 mg L⁻¹); the first in flowing waters, the latter in still waters.     

Effect of zooplankton availability on the rates of photosynthesis, and tissue and skeletal growth in the scleractinian coral Stylophora pistillata

This work investigated the effect of light and feeding on tissue composition as well as on rates of photosynthesis and calcification in the zooxanthellae (zoox) scleractinian coral, Stylophora pistillata. Microcolonies were maintained at three different light levels (80, 200, 300 μmol m⁻² s⁻¹) and subjected to two feeding regimes (starved and fed) over 9 weeks. Corals were fed both natural plankton and Artemia salina nauplii four times a weeks and samplings were made after 2, 5, and 9 weeks. Results confirmed that feeding enhances coral growth rate and increases both the dark and light calcification rates. These rates were 50-75% higher in fed corals (FC; 60±20 and 200±40 nmol Ca²⁺ cm⁻² h⁻¹ for dark and light calcification, respectively) compared to control corals (CC; 30±9 and 124±23 nmol Ca²⁺ cm⁻² h⁻¹). The dark calcification rates, however, were four times lower than the rates of light calcification (independent of trophic status). After 5 weeks, chlorophyll a (chl-a) concentrations were four to seven times higher in fed corals (7-21 μg cm⁻²) than in control corals (2-5 μg cm⁻²). The amount of protein was also significantly higher in fed corals (2.11-2.50 mg cm⁻²) than in control corals (1.08-1.52 mg cm⁻²). Rates of photosynthesis in fed corals were 2-10 times higher (1.24±0.75 μmol O₂ h⁻¹ cm⁻²) than those measured in control corals (0.20±0.08 μmol O₂ h⁻¹ cm⁻²).     

Multinuclear NMR study and crystal structures of complexes of the types cis- and trans-Pt(amine)2I2

Complexes of the types cis- and trans-Pt(amine)₂I₂ were studied by spectroscopic methods, especially by multinuclear NMR spectroscopy. In ¹⁹⁵Pt NMR, the cis diiodo compounds with primary amines were observed between −3342 and −3357 ppm in acetone, while the trans compounds were found between −3336 and −3372 ppm. For the secondary amines, the chemical shifts were observed at lower fields. In ¹H NMR, the trans complexes were observed at higher fields than the cis compounds, while in ¹³C NMR, the reverse was observed. The ²J(¹⁹⁵Pt-¹H) and ³J(¹⁹⁵Pt-¹H) coupling constants are larger for the cis compounds (ave. 67 and 45 Hz, respectively) than for the trans isomers (ave. 59 and 38 Hz). In ¹³C NMR, the values of ²J(¹⁹⁵Pt-¹³C) and ³J(¹⁹⁵Pt-¹³C) were also found to be larger for the cis complexes (ave. 17 and 39 Hz versus 11 and 28 Hz). There seems to be a slight dependence of the pK_a values of the protonated amines or the proton affinity in the gas phase with the δ(Pt) chemical shifts. The crystal structures of eight diiodo complexes were determined. These compounds are cis-Pt(CH₃NH₂)₂I₂, cis-Pt(n-C₄H₉NH₂)₂I₂, cis-Pt(Et₂NH)₂I₂, trans-Pt(n-C₃H₇NH₂)₂I₂, trans-Pt(iso-C₃H₇NH₂)₂I₂, trans-Pt(n-C₄H₉NH₂)₂I₂, trans-Pt(t-C₄H₉NH₂)₂I₂ and trans-Pt(Me₂NH)₂I₂. The Pt-N bond distances located in trans position to the iodo ligands were compared to those located in trans position to the amines. The Pt-N bond in cis-Pt(Et₂NH)₂I₂ are much longer than the others, probably caused by the steric hindrance of the two very bulky ligands located in cis positions.     

Cardiac ion channel current modulation by the CFTR inhibitor GlyH-101

The role in the heart of the cardiac isoform of the cystic fibrosis transmembrane conductance regulator (CFTR), which underlies a protein kinase A-dependent Cl⁻ current (I_Cl.PKA) in cardiomyocytes, remains unclear. The identification of a CFTR-selective inhibitor would provide an important tool for the investigation of the contribution of CFTR to cardiac electrophysiology. GlyH-101 is a glycine hydrazide that has recently been shown to block CFTR channels but its effects on cardiomyocytes are unknown. Here the action of GlyH-101 on cardiac I_Cl.PKA and on other ion currents has been established. Whole-cell patch-clamp recordings were made from rabbit isolated ventricular myocytes. GlyH-101 blocked I_Cl.PKA in a concentration- and voltage-dependent fashion (IC₅₀ at +100 mV = 0.3 ± 1.5 μM and at −100 mV = 5.1 ± 1.3 μM). Woodhull analysis suggested that GlyH-101 blocks the open pore of cardiac CFTR channels at an electrical distance of 0.15 ± 0.03 from the external membrane surface. A concentration of GlyH-101 maximally effective against I_Cl.PKA (30 μM) was tested on other cardiac ion currents. Inward current at −120 mV, comprised predominantly of the inward-rectifier background K⁺ current, I_K1, was reduced by ∼43% (n = 5). Under selective recording conditions, the Na⁺ current (I_Na) was markedly inhibited by GlyH-101 over the entire voltage range (with a fractional block at −40 mV of ∼82%; n = 8). GlyH-101 also produced a voltage-dependent inhibition of L-type Ca²⁺ channel current (I_Ca,L); fractional block at +10 mV of ∼49% and of ∼28% at −10 mV; n = 11, with a ∼−3 mV shift in the voltage-dependence of I_Ca,L activation. Thus, this study demonstrates for the first time that GlyH-101 blocks cardiac I_Cl.PKA channels in a similar fashion to that reported for recombinant CFTR. However, inhibition of other cardiac conductances may limit its use as a CFTR-selective blocker in the heart.     

Cyanide and chloride exchange on homoleptic gold(III) square-planar complexes: variable pressure kinetic investigation by heteronuclear NMR

Kinetic studies of X⁻ exchange on [AuX₄]⁻ square-planar complexes (where X=Cl⁻ and CN⁻) were performed at acidic pH in the case of chloride system and as a function of pH for the cyanide one. Chloride NMR study (330-365 K) gives a second-order rate law on [AuCl₄]⁻ with the kinetic parameters: (k₂^Au,Cl)²⁹⁸=0.56±0.03 s⁻¹ mol⁻¹ kg; ΔH₂^‡ Au,Cl=65.1±1 kJ mol⁻¹; ΔS₂^‡ Au,Cl=−31.3±3 J mol⁻¹ K⁻¹ and ΔV₂^‡ Au,Cl=−14±2 cm³ mol⁻¹. The variable pressure data clearly indicate the operation of an I_a or A mechanism for this exchange pathway. The proton exchange on HCN was determined by ¹³C NMR as a function of pH and the rate constant of the three reaction pathways involving H₂O, OH⁻ and CN⁻ were determined: k₀^HCN,H=113±17 s⁻¹, k₁^HCN,H=(2.9±0.7)×10⁹ s⁻¹ mol⁻¹ kg and k₂^HCN,H=(0.6±0.2)×10⁶ s⁻¹ mol⁻¹ kg at 298.1 K. The rate law of the cyanide exchange on [Au(CN)₄]⁻ was found to be second order with the following kinetic parameters: (k₂^Au,CN)²⁹⁸=6240±85 s⁻¹ mol⁻¹ kg, ΔH₂^‡ Au,CN=40.0±0.8 kJ mol⁻¹, ΔS₂^‡ Au,CN=−37.8±3 J mol⁻¹ K⁻¹ and ΔV₂^‡ Au,CN=+2±1 cm³ mol⁻¹. The rate constant observed varies about nine orders of magnitude depending on the pH and HCN does not act as a nucleophile. The observed rate constant of X⁻ exchange on [AuX₄]⁻ are two or three orders of magnitude faster than the Pt(II) analogue.     

Multinuclear NMR and molecular modelling investigations on the structure and equilibria of complexes that form in aqueous solutions of Ca and gluconate

Complexation of d-gluconate (Gluc⁻) with Ca²⁺ has been investigated via ¹H, ¹³C and ⁴³Ca NMR spectroscopy in aqueous solutions in the presence of high concentration background electrolytes (1 M ? I ? 4 M (NaCl) ionic strength). From the ionic strength dependence of its formation constant, the stability constant at 6 ? pH ? 11 and at I → 0 M has been derived (). The protonation constant of Gluc⁻ at I = 1 M (NaCl) ionic strength was also determined and was found to be log K_a = 3.24 ± 0.01 (¹³C NMR) and log K_a = 3.23 ± 0.01 (¹H NMR). It was found that ¹H and ¹³C NMR chemical shifts upon complexation (both with H⁺ and with Ca²⁺) do not vary in an unchanging way with the distance from the Ca²⁺/H⁺ binding site. From 2D ¹H-⁴³Ca NMR spectra, simultaneous binding of Ca²⁺ to the alcoholic OH on C2 and C3 was deduced. Molecular modelling results modulated this picture by revealing structures in which the Gluc⁻ behaves as a multidentate ligand. The five-membered chelated initial structure was found to be thermodynamically more stable than that derived from a six-membered chelated initial structure.     

Spatially Discordant Alternans and Arrhythmias in Tachypacing-Induced Cardiac Myopathy in Transgenic LQT1 Rabbits: The Importance of IKs and Ca2+ Cycling

BackgroundRemodeling of cardiac repolarizing currents, such as the downregulation of slowly activating K⁺ channels (I_Ks), could underlie ventricular fibrillation (VF) in heart failure (HF). We evaluated the role of I_ks remodeling in VF susceptibility using a tachypacing HF model of transgenic rabbits with Long QT Type 1 (LQT1) syndrome.ConclusionsCompared with LMC-TICM, LQT1-TICM rabbits exhibit steepened APD restitution and complex DA modulated by Ca²⁺. Our results strongly support the contention that the downregulation of I_Ks in HF increases Ca²⁺ dependent alternans and thereby the risk of VF.