Single-Channel Kinetics,Inactivation, and Spatial Distribution of Inositol Trisphosphate (IP3) Receptors in Xenopus Oocyte Nucleus

Single-channel properties of the Xenopus inositol trisphosphate receptor (IP₃R) ion channel were examined by patch clamp electrophysiology of the outer nuclear membrane of isolated oocyte nuclei. With 140 mM K⁺ as the charge carrier (cytoplasmic [IP₃] = 10 μM, free [Ca²⁺] = 200 nM), the IP₃R exhibited four and possibly five conductance states. The conductance of the most-frequently observed state M was 113 pS around 0 mV and ∼300 pS at 60 mV. The channel was frequently observed with high open probability (mean P _o = 0.4 at 20 mV). Dwell time distribution analysis revealed at least two kinetic states of M with time constants τ < 5 ms and ∼20 ms; and at least three closed states with τ ∼1 ms, ∼10 ms, and >1 s. Higher cytoplasmic potential increased the relative frequency and τ of the longest closed state. A novel “flicker” kinetic mode was observed, in which the channel alternated rapidly between two new conductance states: F₁ and F₂. The relative occupation probability of the flicker states exhibited voltage dependence described by a Boltzmann distribution corresponding to 1.33 electron charges moving across the entire electric field during F₁ to F₂ transitions. Channel run-down or inactivation (τ ∼ 30 s) was consistently observed in the continuous presence of IP₃ and the absence of change in [Ca²⁺]. Some (∼10%) channel disappearances could be reversed by an increase in voltage before irreversible inactivation. A model for voltage-dependent channel gating is proposed in which one mechanism controls channel opening in both the normal and flicker modes, whereas a separate independent mechanism generates flicker activity and voltage- reversible inactivation. Mapping of functional channels indicates that the IP₃R tends to aggregate into microscopic (<1 μm) as well as macroscopic (∼10 μm) clusters. Ca²⁺-independent inactivation of IP₃R and channel clustering may contribute to complex [Ca²⁺] signals in cells.     

Ryanoids and imperatoxin affect the modulation of cardiac ryanodine receptors by dihydropyridine receptor Peptide A

Ca²⁺-entry via L-type Ca²⁺ channels (DHPR) is known to trigger ryanodine receptor (RyR)-mediated Ca²⁺-release from sarcoplasmic reticulum (SR). The mechanism that terminates SR Ca²⁺ release is still unknown. Previous reports showed evidence of Ca²⁺-entry independent inhibition of Ca²⁺ sparks by DHPR in cardiomyocytes. A peptide from the DHPR loop II-III (PepA) was reported to modulate isolated RyRs. We found that PepA induced voltage-dependent “flicker block” and transition to substates of fully-activated cardiac RyRs in planar bilayers. Substates had less voltage-dependence than block and did not represent occupancy of a ryanoid site. However, ryanoids stabilized PepA-induced events while PepA increased RyR2 affinity for ryanodol, which suggests cooperative interactions. Ryanodol stabilized Imperatoxin A (IpTx_A) binding but when IpTx_A bound first, it prevented ryanodol binding. Moreover, IpTx_A and PepA excluded each other from their sites. This suggests that IpTx_A generates a vestibular gate (either sterically or allosterically) that prevents access to the peptides and ryanodol binding sites. Inactivating gate moieties (“ball peptides”) from K⁺ and Na⁺ channels (ShakerB and KIFMK, respectively) induced well resolved slow block and substates, which were sensitive to ryanoids and IpTx_A and allowed, by comparison, better understanding of PepA action. The RyR2 appears to interact with PepA or ball peptides through a two-step mechanism, reminiscent of the inactivation of voltage-gated channels, which includes binding to outer (substates) and inner (block) vestibular regions in the channel conduction pathway. Our results open the possibility that “ball peptide-like” moieties in RyR2-interacting proteins could modulate SR Ca²⁺ release in cells.     

Unitary Ca2+ Current through Cardiac Ryanodine Receptor Channels under Quasi-Physiological Ionic Conditions

Single canine cardiac ryanodine receptor channels were incorporated into planar lipid bilayers. Single-channel currents were sampled at 1–5 kHz and filtered at 0.2–1.0 kHz. Channel incorporations were obtained in symmetrical solutions (20 mM HEPES-Tris, pH 7.4, and pCa 5). Unitary Ca²⁺ currents were monitored when 2–30 mM Ca²⁺ was added to the lumenal side of the channel. The relationship between the amplitude of unitary Ca²⁺ current (at 0 mV holding potential) and lumenal [Ca²⁺] was hyperbolic and saturated at ∼4 pA. This relationship was then defined in the presence of different symmetrical CsCH₃SO₃ concentrations (5, 50, and 150 mM). Under these conditions, unitary current amplitude was 1.2 ± 0.1, 0.65 ± 0.1, and 0.35 ± 0.1 pA in 2 mM lumenal Ca²⁺; and 3.3 ± 0.4, 2.4 ± 0.2, and 1.63 ± 0.2 pA in 10 mM lumenal Ca²⁺ (n > 6). Unitary Ca²⁺ current was also defined in the presence of symmetrical [Mg²⁺] (1 mM) and low [Cs⁺] (5 mM). Under these conditions, unitary Ca²⁺ current in 2 and 10 mM lumenal Ca²⁺ was 0.66 ± 0.1 and 1.52 ± 0.06 pA, respectively. In the presence of higher symmetrical [Cs⁺] (50 mM), Mg²⁺ (1 mM), and lumenal [Ca²⁺] (10 mM), unitary Ca²⁺ current exhibited an amplitude of 0.9 ± 0.2 pA (n = 3). This result indicates that the actions of Cs⁺ and Mg²⁺ on unitary Ca²⁺ current were additive. These data demonstrate that physiological levels of monovalent cation and Mg²⁺ effectively compete with Ca²⁺ as charge carrier in cardiac ryanodine receptor channels. If lumenal free Ca²⁺ is 2 mM, then our results indicate that unitary Ca²⁺ current under physiological conditions should be <0.6 pA.     

Functional Coupling of Ryanodine Receptors to KCa Channels in Smooth Muscle Cells from Rat Cerebral Arteries

The relationship between Ca²⁺ release (“Ca²⁺ sparks”) through ryanodine-sensitive Ca²⁺ release channels in the sarcoplasmic reticulum and K_Ca channels was examined in smooth muscle cells from rat cerebral arteries. Whole cell potassium currents at physiological membrane potentials (−40 mV) and intracellular Ca²⁺ were measured simultaneously, using the perforated patch clamp technique and a laser two-dimensional (x–y) scanning confocal microscope and the fluorescent Ca²⁺ indicator, fluo-3. Virtually all (96%) detectable Ca²⁺ sparks were associated with the activation of a spontaneous transient outward current (STOC) through K_Ca channels. A small number of sparks (5 of 128) were associated with currents smaller than 6 pA (mean amplitude, 4.7 pA, at −40 mV). Approximately 41% of STOCs occurred without a detectable Ca²⁺ spark. The amplitudes of the Ca²⁺ sparks correlated with the amplitudes of the STOCs (regression coefficient 0.8; P < 0.05). The half time of decay of Ca²⁺ sparks (56 ms) was longer than the associated STOCs (9 ms). The mean amplitude of the STOCs, which were associated with Ca²⁺ sparks, was 33 pA at −40 mV. The mean amplitude of the “sparkless” STOCs was smaller, 16 pA. The very significant increase in K_Ca channel open probability (>10⁴-fold) during a Ca²⁺ spark is consistent with local Ca²⁺ during a spark being in the order of 1–100 μM. Therefore, the increase in fractional fluorescence (F/F_o) measured during a Ca²⁺ spark (mean 2.04 F/F_o or ∼310 nM Ca²⁺) appears to significantly underestimate the local Ca²⁺ that activates K_Ca channels. These results indicate that the majority of ryanodine receptors that cause Ca²⁺ sparks are functionally coupled to K_Ca channels in the surface membrane, providing direct support for the idea that Ca²⁺ sparks cause STOCs.     

Phe-Met-Arg-Phe-amide Activates a Novel Voltage-dependent K+ Current through a Lipoxygenase Pathway in Molluscan Neurones

The neuropeptide Phe-Met-Arg-Phe-amide (FMRFa) dose dependently (ED₅₀ = 23 nM) activated a K⁺ current in the peptidergic caudodorsal neurones that regulate egg laying in the mollusc Lymnaea stagnalis. Under standard conditions ([K⁺]_o = 1.7 mM), only outward current responses occurred. In high K⁺ salines ([K⁺]_o = 20 or 57 mM), current reversal occurred close to the theoretical reversal potential for K⁺. In both salines, no responses were measured below −120 mV. Between −120 mV and the K⁺ reversal potential, currents were inward with maximal amplitudes at ∼−60 mV. Thus, U-shaped current–voltage relations were obtained, implying that the response is voltage dependent. The conductance depended both on membrane potential and extracellular K⁺ concentration. The voltage sensitivity was characterized by an e-fold change in conductance per ∼14 mV at all [K⁺]_o. Since this result was also obtained in nearly symmetrical K⁺ conditions, it is concluded that channel gating is voltage dependent. In addition, outward rectification occurs in asymmetric K⁺ concentrations. Onset kinetics of the response were slow (rise time ∼650 ms at −40 mV). However, when FMRFa was applied while holding the cell at −120 mV, to prevent activation of the current but allow activation of the signal transduction pathway, a subsequent step to −40 mV revealed a much more rapid current onset. Thus, onset kinetics are largely determined by steps preceding channel activation. With FMRFa applied at −120 mV, the time constant of activation during the subsequent test pulse decreased from ∼36 ms at −60 mV to ∼13 ms at −30 mV, confirming that channel opening is voltage dependent. The current inactivated voltage dependently. The rate and degree of inactivation progressively increased from −120 to −50 mV. The current is blocked by internal tetraethylammonium and by bath- applied 4-aminopyridine, tetraethylammonium, Ba²⁺, and, partially, Cd²⁺ and Cs⁺. The response to FMRFa was affected by intracellular GTPγS. The response was inhibited by blockers of phospholipase A₂ and lipoxygenases, but not by a cyclo-oxygenase blocker. Bath-applied arachidonic acid induced a slow outward current and occluded the response to FMRFa. These results suggest that the FMRFa receptor couples via a G-protein to the lipoxygenase pathway of arachidonic acid metabolism. The biophysical and pharmacological properties of this transmitter operated, but voltage-dependent K⁺ current distinguish it from other receptor-driven K⁺ currents such as the S-current- and G-protein-dependent inward rectifiers.     

Time-dependent Outward Currents through the Inward Rectifier Potassium Channel IRK1 : The Role of Weak Blocking Molecules

Outward currents through the inward rectifier K⁺ channel contribute to repolarization of the cardiac action potential. The properties of the IRK1 channel expressed in murine fibroblast (L) cells closely resemble those of the native cardiac inward rectifier. In this study, we added Mg²⁺ (0.44–1.1 mM) or putrescine (∼0.4 mM) to the intracellular milieu where endogenous polyamines remained, and then examined outward IRK1 currents using the whole-cell patch-clamp method at 5.4 mM external K⁺. Without internal Mg²⁺, small outward currents flowed only at potentials between −80 (the reversal potential) and ∼−40 mV during voltage steps applied from −110 mV. The strong inward rectification was mainly caused by the closed state of the activation gating, which was recently reinterpreted as the endogenous-spermine blocked state. With internal Mg²⁺, small outward currents flowed over a wider range of potentials during the voltage steps. The outward currents at potentials between −40 and 0 mV were concurrent with the contribution of Mg²⁺ to blocking channels at these potentials, judging from instantaneous inward currents in the following hyperpolarization. Furthermore, when the membrane was repolarized to −50 mV after short depolarizing steps (>0 mV), a transient increase appeared in outward currents at −50 mV. Since the peak amplitude depended on the fraction of Mg²⁺-blocked channels in the preceding depolarization, the transient increase was attributed to the relief of Mg²⁺ block, followed by a re-block of channels by spermine. Shift in the holding potential (−110 to −80 mV), or prolongation of depolarization, increased the number of spermine-blocked channels and decreased that of Mg²⁺-blocked channels in depolarization, which in turn decreased outward currents in the subsequent repolarization. Putrescine caused the same effects as Mg²⁺. When both spermine (1 μM, an estimated free spermine level during whole-cell recordings) and putrescine (300 μM) were applied to the inside-out patch membrane, the findings in whole-cell IRK1 were reproduced. Our study indicates that blockage of IRK1 by molecules with distinct affinities, spermine and Mg²⁺ (putrescine), elicits a transient increase in the outward IRK1, which may contribute to repolarization of the cardiac action potential.     

Voltage Gating of Shaker K+ Channels : The Effect of Temperature on Ionic and Gating Currents

Ionic (I_i) and gating currents (I_g) from noninactivating Shaker H4 K⁺ channels were recorded with the cut-open oocyte voltage clamp and macropatch techniques. Steady state and kinetic properties were studied in the temperature range 2–22°C. The time course of I_i elicited by large depolarizations consists of an initial delay followed by an exponential rise with two kinetic components. The main I_i component is highly temperature dependent (Q₁₀ > 4) and mildly voltage dependent, having a valence times the fraction of electric field (z) of 0.2–0.3 e_o. The I_g On response obtained between −60 and 20 mV consists of a rising phase followed by a decay with fast and slow kinetic components. The main I_g component of decay is highly temperature dependent (Q₁₀ > 4) and has a z between 1.6 and 2.8 e_o in the voltage range from −60 to −10 mV, and ∼0.45 e_o at more depolarized potentials. After a pulse to 0 mV, a variable recovery period at −50 mV reactivates the gating charge with a high temperature dependence (Q₁₀ > 4). In contrast, the reactivation occurring between −90 and −50 mV has a Q₁₀ = 1.2. Fluctuation analysis of ionic currents reveals that the open probability decreases 20% between 18 and 8°C and the unitary conductance has a low temperature dependence with a Q₁₀ of 1.44. Plots of conductance and gating charge displacement are displaced to the left along the voltage axis when the temperature is decreased. The temperature data suggests that activation consists of a series of early steps with low enthalpic and negative entropic changes, followed by at least one step with high enthalpic and positive entropic changes, leading to final transition to the open state, which has a negative entropic change.     

Extracellular Zinc Ion Inhibits ClC-0 Chloride Channels by Facilitating Slow Gating

Extracellular Zn²⁺ was found to reversibly inhibit the ClC-0 Cl⁻ channel. The apparent on and off rates of the inhibition were highly temperature sensitive, suggesting an effect of Zn²⁺ on the slow gating (or inactivation) of ClC-0. In the absence of Zn²⁺, the rate of the slow-gating relaxation increased with temperature, with a Q₁₀ of ∼37. Extracellular Zn²⁺ facilitated the slow-gating process at all temperatures, but the Q₁₀ did not change. Further analysis of the rate constants of the slow-gating process indicates that the effect of Zn²⁺ is mostly on the forward rate (the rate of inactivation) rather than the backward rate (the rate of recovery from inactivation) of the slow gating. When ClC-0 is bound with Zn²⁺, the equilibrium constant of the slow-gating process is increased by ∼30-fold, reflecting a 30-fold higher Zn²⁺ affinity in the inactivated channel than in the open-state channel. As examined through a wide range of membrane potentials, Zn²⁺ inhibits the opening of the slow gate with equal potency at all voltages, suggesting that a two-state model is inadequate to describe the slow-gating transition. Following a model originally proposed by Pusch and co-workers (Pusch, M., U. Ludewig, and T.J. Jentsch. 1997. J. Gen. Physiol. 109:105–116), the effect of Zn²⁺ on the activation curve of the slow gate can be well described by adding two constraints: (a) the dissociation constant for Zn²⁺ binding to the open channel is 30 μM, and (b) the difference in entropy between the open state and the transition state of the slow-gating process is increased by 27 J/ mol/°K for the Zn²⁺-bound channel. These results together indicate that extracellular Zn²⁺ inhibits ClC-0 by facilitating the slow-gating process.     

Voltage-Dependent Modulation of Cardiac Ryanodine Receptors (RyR2) by Protamine

It has been reported that protamine (>10 µg/ml) blocks single skeletal RyR1 channels and inhibits RyR1-mediated Ca²⁺ release from sarcoplasmic reticulum microsomes. We extended these studies to cardiac RyR2 reconstituted into planar lipid bilayers. We found that protamine (0.02–20 µg/ml) added to the cytosolic surface of fully activated RyR2 affected channel activity in a voltage-dependent manner. At membrane voltage (V_m; SR lumen - cytosol) = 0 mV, protamine induced conductance transitions to several intermediate states (substates) as well as full block of RyR2. At V_m>10 mV, the substate with the highest level of conductance was predominant. Increasing V_m from 0 to +80 mV, decreased the number of transitions and residence of the channel in this substate. The drop in current amplitude (full opening to substate) had the same magnitude at 0 and +80 mV despite the ∼3-fold increase in amplitude of the full opening. This is more similar to rectification of channel conductance induced by other polycations than to the action of selective conductance modifiers (ryanoids, imperatoxin). A distinctive effect of protamine (which might be shared with polylysines and histones but not with non-peptidic polycations) is the activation of RyR2 in the presence of nanomolar cytosolic Ca²⁺ and millimolar Mg²⁺ levels. Our results suggest that RyRs would be subject to dual modulation (activation and block) by polycationic domains of neighboring proteins via electrostatic interactions. Understanding these interactions could be important as such anomalies may be associated with the increased RyR2-mediated Ca²⁺ leak observed in cardiac diseases.     

Blockade of cardiac outwardly rectifying K+ channels by TEA and class III antiarrhythmics — evidence against a single drug-sensitive channel site

Elementary K⁺ currents through cardiac outwardly rectifying K⁺ channels were recorded in insideout patches excised from cultured neonatal rat cardiocytes at 19 °C and at 9 °C. By studying the inhibitory effects of tetraethylammonium (TEA), quinidine and verapamil, the properties of this novel type of K⁺ channel were further characterized. Internal TEA (50 mmol/1) evoked a reversible decline of i_unit to 62.7 + 2.7% of control (at –7 mV), without significant changes of open state kinetics, indicating a blockade of the open K⁺ pore with kinetics too fast to be resolvable at 1 kHz. This TEA blockade was e-fold voltage-dependent, with a decrease of the apparent K_{D( TEA)} from 102 mmol/1 at –37 mV to 65 mmol/1 at +33 mV and, furthermore, became accentuated on lowering the internal K⁺ concentration. Thus, TEA competes with the permeant K⁺ for a site located in some distance from the cytoplasmic margin, within the K⁺ pore. Quinidine (100 mol/l), like verapamil (40 mol/1) reversibly depressed i_unit to about 80% of the control value (at –7 mV), but drug-induced fast flicker blockade proved voltage-insensitive between –27 mV and +23 mV These drugs gain access to a portion of the pore distinct from the TEA binding site whose occupancy by drugs likewise blocks K⁺ permeation. Both drugs showed a greater potency to depress P_o which, with quinidine,decreased reversibly to38.6 ± 11.1% (at –7 mV) and, with verapamil to 24.9 ± 9.1%(at –7 mV), mainly by an increase of the prolonged closed state (C,). This alteration of the gating process also includes a sometimes dramatic shortening of the open state. Most probably, cardiac K_{(outw.-rect.)} ⁺K⁺ _outw.-rect. channels possess a second drug-sensitive site whose occupancy by quinidine or verapamil may directly or allosterically stabilize their non-conducting configuration. Correspondence to: M. Kohlhardt     

Sodium and Calcium Inward Currents in Freshly Dissociated Smooth Myocytes of Rat Uterus

Freshly dissociated myocytes from nonpregnant, pregnant, and postpartum rat uteri have been studied with the tight-seal patch-clamp method. The inward current contains both I_Na and I_Ca that are vastly different from those in tissue-cultured material. I_Na is abolished by Na⁺-free medium and by 1 μM tetrodotoxin. It first appears at ∼−40 mV, reaches maximum at 0 mV, and reverses at 84 mV. It activates with a voltage-dependent τ of 0.2 ms at 20 mV, and inactivates as a single exponential with a τ of 0.4 ms. Na⁺ conductance is half activated at −21.5 mV, and half inactivated at −59 mV. I_Na reactivates with a τ of 20 ms. I_Ca is abolished by Ca²⁺-free medium, Co²⁺ (5 mM), or nisoldipine (2 μM), and enhanced in 30 mM Ca²⁺, Ba²⁺, or BAY-K 8644. It first appears at ∼−30 mV and reaches maximum at +10 mV. It activates with a voltage-dependent τ of 1.5 ms at 20 mV, and inactivates in two exponential phases, with τ''s of 33 and 133 ms. Ca²⁺ conductance is half activated at −7.4 mV, and half inactivated at −34 mV. I_Ca reactivates with τ''s of 27 and 374 ms. I_Na and I_Ca are seen in myocytes from nonpregnant estrus uteri and throughout pregnancy, exhibiting complex changes. The ratio of densities of peak I_Na/I_Ca changes from 0.5 in the nonpregnant state to 1.6 at term. The enhanced role of I_Na, with faster kinetics, allows more frequent repetitive spike discharges to facilitate simultaneous excitation of the parturient uterus. In postpartum, both currents decrease markedly, with I_Na vanishing from most myocytes. Estrogen-enhanced genomic influences may account for the emergence of I_Na, and increased densities of I_Na and I_Ca as pregnancy progresses. Other influences may regulate varied channel expression at different stages of pregnancy.     

Intrinsic Voltage Dependence and Ca2+ Regulation of mslo Large Conductance Ca-activated K+ Channels

The kinetic and steady-state properties of macroscopic mslo Ca-activated K⁺ currents were studied in excised patches from Xenopus oocytes. In response to voltage steps, the timecourse of both activation and deactivation, but for a brief delay in activation, could be approximated by a single exponential function over a wide range of voltages and internal Ca²⁺ concentrations ([Ca]_i). Activation rates increased with voltage and with [Ca]_i, and approached saturation at high [Ca]_i. Deactivation rates generally decreased with [Ca]_i and voltage, and approached saturation at high [Ca]_i. Plots of the macroscopic conductance as a function of voltage (G-V) and the time constant of activation and deactivation shifted leftward along the voltage axis with increasing [Ca]_i. G-V relations could be approximated by a Boltzmann function with an equivalent gating charge which ranged between 1.1 and 1.8 e as [Ca]_i varied between 0.84 and 1,000 μM. Hill analysis indicates that at least three Ca²⁺ binding sites can contribute to channel activation. Three lines of evidence indicate that there is at least one voltage-dependent unimolecular conformational change associated with mslo gating that is separate from Ca²⁺ binding. (a) The position of the mslo G-V relation does not vary logarithmically with [Ca]_i. (b) The macroscopic rate constant of activation approaches saturation at high [Ca]_i but remains voltage dependent. (c) With strong depolarizations mslo currents can be nearly maximally activated without binding Ca²⁺. These results can be understood in terms of a channel which must undergo a central voltage-dependent rate limiting conformational change in order to move from closed to open, with rapid Ca²⁺ binding to both open and closed states modulating this central step.     

Ca2+-induced Ca2+ Release in Chinese Hamster Ovary (CHO) Cells Co-expressing Dihydropyridine and Ryanodine Receptors

Combined patch-clamp and Fura-2 measurements were performed on chinese hamster ovary (CHO) cells co-expressing two channel proteins involved in skeletal muscle excitation-contraction (E-C) coupling, the ryanodine receptor (RyR)-Ca²⁺ release channel (in the membrane of internal Ca²⁺ stores) and the dihydropyridine receptor (DHPR)-Ca²⁺ channel (in the plasma membrane). To ensure expression of functional L-type Ca²⁺ channels, we expressed α₂, β, and γ DHPR subunits and a chimeric DHPR α₁ subunit in which the putative cytoplasmic loop between repeats II and III is of skeletal origin and the remainder is cardiac. There was no clear indication of skeletal-type coupling between the DHPR and the RyR; depolarization failed to induce a Ca²⁺ transient (CaT) in the absence of extracellular Ca²⁺ ([Ca²⁺]_o). However, in the presence of [Ca²⁺]_o, depolarization evoked CaTs with a bell-shaped voltage dependence. About 30% of the cells tested exhibited two kinetic components: a fast transient increase in intracellular Ca²⁺ concentration ([Ca²⁺]_i) (the first component; reaching 95% of its peak <0.6 s after depolarization) followed by a second increase in [Ca²⁺]_i which lasted for 5–10 s (the second component). Our results suggest that the first component primarily reflected Ca²⁺ influx through Ca²⁺ channels, whereas the second component resulted from Ca²⁺ release through the RyR expressed in the membrane of internal Ca²⁺ stores. However, the onset and the rate of Ca²⁺ release appeared to be much slower than in native cardiac myocytes, despite a similar activation rate of Ca²⁺ current. These results suggest that the skeletal muscle RyR isoform supports Ca²⁺-induced Ca²⁺ release but that the distance between the DHPRs and the RyRs is, on average, much larger in the cotransfected CHO cells than in cardiac myocytes. We conclude that morphological properties of T-tubules and/or proteins other than the DHPR and the RyR are required for functional “close coupling” like that observed in skeletal or cardiac muscle. Nevertheless, some of our results imply that these two channels are potentially able to directly interact with each other.     

Amino Acid Residues 489–503 of Dihydropyridine Receptor (DHPR) β1a Subunit Are Critical for Structural Communication between the Skeletal Muscle DHPR Complex and Type 1 Ryanodine Receptor

The β_1a subunit is a cytoplasmic component of the dihydropyridine receptor (DHPR) complex that plays an essential role in skeletal muscle excitation-contraction (EC) coupling. Here we investigate the role of the C-terminal end of this auxiliary subunit in the functional and structural communication between the DHPR and the Ca²⁺ release channel (RyR1). Progressive truncation of the β_1a C terminus showed that deletion of amino acid residues Gln⁴⁸⁹ to Trp⁵⁰³ resulted in a loss of depolarization-induced Ca²⁺ release, a severe reduction of L-type Ca²⁺ currents, and a lack of tetrad formation as evaluated by freeze-fracture analysis. However, deletion of this domain did not affect expression/targeting or density (Q_max) of the DHPR-α_1S subunit to the plasma membrane. Within this motif, triple alanine substitution of residues Leu⁴⁹⁶, Leu⁵⁰⁰, and Trp⁵⁰³, which are thought to mediate direct β_1a-RyR1 interactions, weakened EC coupling but did not replicate the truncated phenotype. Therefore, these data demonstrate that an amino acid segment encompassing sequence ⁴⁸⁹QVQVLTSLRRNLSFW⁵⁰³ of β_1a contains critical determinant(s) for the physical link of DHPR and RyR1, further confirming a direct correspondence between DHPR positioning and DHPR/RyR functional interactions. In addition, our data strongly suggest that the motif Leu⁴⁹⁶-Leu⁵⁰⁰-Trp⁵⁰³ within the β_1a C-terminal tail plays a nonessential role in the bidirectional DHPR/RyR1 signaling that supports skeletal-type EC coupling.     

Diversity of Channels Generated by Different Combinations of Epithelial Sodium Channel Subunits

The epithelial sodium channel is a multimeric protein formed by three homologous subunits: α, β, and γ; each subunit contains only two transmembrane domains. The level of expression of each of the subunits is markedly different in various Na⁺ absorbing epithelia raising the possibility that channels with different subunit composition can function in vivo. We have examined the functional properties of channels formed by the association of α with β and of α with γ in the Xenopus oocyte expression system using two-microelectrode voltage clamp and patch-clamp techniques. We found that αβ channels differ from αγ channels in the following functional properties: (a) αβ channels expressed larger Na⁺ than Li⁺ currents (I_Na+/I_Li+ 1.2) whereas αγ channels expressed smaller Na⁺ than Li⁺ currents (I_Na+/I_Li+ 0.55); (b) the Michaelis Menten constants (K _m) of activation of current by increasing concentrations of external Na⁺ and Li⁺ of αβ channels were larger (K _m > 180 mM) than those of αγ channels (K _m of 35 and 50 mM, respectively); (c) single channel conductances of αβ channels (5.1 pS for Na⁺ and 4.2 pS for Li⁺) were smaller than those of αγ channels (6.5 pS for Na⁺ and 10.8 pS for Li⁺); (d) the half-inhibition constant (K _i) of amiloride was 20-fold larger for αβ channels than for αγ channels whereas the K _i of guanidinium was equal for both αβ and αγ. To identify the domains in the channel subunits involved in amiloride binding, we constructed several chimeras that contained the amino terminus of the γ subunit and the carboxy terminus of the β subunit. A stretch of 15 amino acids, immediately before the second transmembrane domain of the β subunit, was identified as the domain conferring lower amiloride affinity to the αβ channels. We provide evidence for the existence of two distinct binding sites for the amiloride molecule: one for the guanidium moiety and another for the pyrazine ring. At least two subunits α with β or γ contribute to these binding sites. Finally, we show that the most likely stoichiometry of αβ and αγ channels is 1α:1β and 1α:1γ, respectively.     

Potassium Currents in Freshly Dissociated Uterine Myocytes from Nonpregnant and Late-Pregnant Rats

In freshly dissociated uterine myocytes, the outward current is carried by K⁺ through channels highly selective for K⁺. Typically, nonpregnant myocytes have rather noisy K⁺ currents; half of them also have a fast-inactivating transient outward current (I_TO). In contrast, the current records are not noisy in late pregnant myocytes, and I_TO densities are low. The whole-cell I_K of nonpregnant myocytes respond strongly to changes in [Ca²⁺]_o or changes in [Ca²⁺]_i caused by photolysis of caged Ca²⁺ compounds, nitr 5 or DM-nitrophene, but that of late-pregnant myocytes respond weakly or not at all. The Ca²⁺ insensitivity of the latter is present before any exposure to dissociating enzymes. By holding at −80, −40, or 0 mV and digital subtractions, the whole-cell I_K of each type of myocyte can be separated into one noninactivating and two inactivating components with half-inactivation at approximately −61 and −22 mV. The noninactivating components, which consist mainly of iberiotoxin-susceptible large-conductance Ca²⁺-activated K⁺ currents, are half-activated at 39 mV in nonpregnant myocytes, but at 63 mV in late-pregnant myocytes. In detached membrane patches from the latter, identified 139 pS, Ca²⁺-sensitive K⁺ channels also have a half-open probability at 68 mV, and are less sensitive to Ca²⁺ than similar channels in taenia coli myocytes. Ca²⁺-activated K⁺ currents, susceptible to tetraethylammonium, charybdotoxin, and iberiotoxin contribute 30–35% of the total I_K in nonpregnant myocytes, but <20% in late-pregnant myocytes. Dendrotoxin-susceptible, small-conductance delayed rectifier currents are not seen in nonpregnant myocytes, but contribute ∼20% of total I_K in late-pregnant myocytes. Thus, in late-pregnancy, myometrial excitability is increased by changes in K⁺ currents that include a suppression of the I_TO, a redistribution of I_K expression from large-conductance Ca²⁺-activated channels to smaller-conductance delayed rectifier channels, a lowered Ca²⁺ sensitivity, and a positive shift of the activation of some large-conductance Ca²⁺-activated channels.     

The Effect of Ionic Strength and Specific Anions on Substrate Binding and Hydrolytic Activities of Na,K-ATPase

The physiological ligands for Na,K-ATPase (the Na,K-pump) are ions, and electrostatic forces, that could be revealed by their ionic strength dependence, are therefore expected to be important for their reaction with the enzyme. We found that the affinities for ADP³⁻, eosin²⁻, p-nitrophenylphosphate, and V_max for Na,K-ATPase and K⁺-activated p-nitrophenylphosphatase activity, were all decreased by increasing salt concentration and by specific anions. Equilibrium binding of ADP was measured at 0–0.5 M of NaCl, Na₂SO₄, and NaNO₃ and in 0.1 M Na-acetate, NaSCN, and NaClO₄. The apparent affinity for ADP decreased up to 30 times. At equal ionic strength, I, the ranking of the salt effect was NaCl ≈ Na₂SO₄ ≈ Na-acetate < NaNO₃ < NaSCN < NaClO₄. We treated the influence of NaCl and Na₂SO₄ on K _diss for E·ADP as a “pure” ionic strength effect. It is quantitatively simulated by a model where the binding site and ADP are point charges, and where their activity coefficients are related to I by the limiting law of Debye and Hückel. The estimated net charge at the binding site of the enzyme was about +1. Eosin binding followed the same model. The NO₃ ⁻ effect was compatible with competitive binding of NO₃ ⁻ and ADP in addition to the general I-effect. K _diss for E·NO₃ was ∼32 mM. Analysis of V_max/K _m for Na,K-ATPase and K⁺-p-nitrophenylphosphatase activity shows that electrostatic forces are important for the binding of p-nitrophenylphosphate but not for the catalytic effect of ATP on the low affinity site. The net charge at the p-nitrophenylphosphate-binding site was also about +1. The results reported here indicate that the reversible interactions between ions and Na,K-ATPase can be grouped according to either simple Debye-Hückel behavior or to specific anion or cation interactions with the enzyme.     

Interactions of a Reversible Ryanoid (21-Amino-9α-Hydroxy-Ryanodine) with Single Sheep Cardiac Ryanodine Receptor Channels

The binding of ryanodine to a high affinity site on the sarcoplasmic reticulum Ca²⁺-release channel results in a dramatic alteration in both gating and ion handling; the channel enters a high open probability, reduced-conductance state. Once bound, ryanodine does not dissociate from its site within the time frame of a single channel experiment. In this report, we describe the interactions of a synthetic ryanoid, 21-amino-9α-hydroxy-ryanodine, with the high affinity ryanodine binding site on the sheep cardiac sarcoplasmic reticulum Ca²⁺-release channel. The interaction of 21-amino-9α-hydroxy-ryanodine with the channel induces the occurrence of a characteristic high open probability, reduced-conductance state; however, in contrast to ryanodine, the interaction of this ryanoid with the channel is reversible under steady state conditions, with dwell times in the modified state lasting seconds. By monitoring the reversible interaction of this ryanoid with single channels under voltage clamp conditions, we have established a number of novel features of the ryanoid binding reaction. (a) Modification of channel function occurs when a single molecule of ryanoid binds to the channel protein. (b) The ryanoid has access to its binding site only from the cytosolic side of the channel and the site is available only when the channel is open. (c) The interaction of 21-amino-9α-hydroxy-ryanodine with its binding site is influenced strongly by transmembrane voltage. We suggest that this voltage dependence is derived from a voltage-driven conformational alteration of the channel protein that changes the affinity of the binding site, rather than the translocation of the ryanoid into the voltage drop across the channel.     

Electrophysiological Characterization of the Rat Epithelial Na+ Channel (rENaC) Expressed in MDCK Cells : Effects of Na+ and Ca2+

The epithelial Na⁺ channel (ENaC), composed of three subunits (α, β, and γ), is expressed in several epithelia and plays a critical role in salt and water balance and in the regulation of blood pressure. Little is known, however, about the electrophysiological properties of this cloned channel when expressed in epithelial cells. Using whole-cell and single channel current recording techniques, we have now characterized the rat αβγENaC (rENaC) stably transfected and expressed in Madin-Darby canine kidney (MDCK) cells. Under whole-cell patch-clamp configuration, the αβγrENaC-expressing MDCK cells exhibited greater whole cell Na⁺ current at −143 mV (−1,466.2 ± 297.5 pA) than did untransfected cells (−47.6 ± 10.7 pA). This conductance was completely and reversibly inhibited by 10 μM amiloride, with a Ki of 20 nM at a membrane potential of −103 mV; the amiloride inhibition was slightly voltage dependent. Amiloride-sensitive whole-cell current of MDCK cells expressing αβ or αγ subunits alone was −115.2 ± 41.4 pA and −52.1 ± 24.5 pA at −143 mV, respectively, similar to the whole-cell Na⁺ current of untransfected cells. Relaxation analysis of the amiloride-sensitive current after voltage steps suggested that the channels were activated by membrane hyperpolarization. Ion selectivity sequence of the Na⁺ conductance was Li⁺ > Na⁺ >> K⁺ = N-methyl-d-glucamine⁺ (NMDG⁺). Using excised outside-out patches, amiloride-sensitive single channel conductance, likely responsible for the macroscopic Na⁺ channel current, was found to be ∼5 and 8 pS when Na⁺ and Li⁺ were used as a charge carrier, respectively. K⁺ conductance through the channel was undetectable. The channel activity, defined as a product of the number of active channel (n) and open probability (P _o), was increased by membrane hyperpolarization. Both whole-cell Na⁺ current and conductance were saturated with increased extracellular Na⁺ concentrations, which likely resulted from saturation of the single channel conductance. The channel activity (nP _o) was significantly decreased when cytosolic Na⁺ concentration was increased from 0 to 50 mM in inside-out patches. Whole-cell Na⁺ conductance (with Li⁺ as a charge carrier) was inhibited by the addition of ionomycin (1 μM) and Ca²⁺ (1 mM) to the bath. Dialysis of the cells with a pipette solution containing 1 μM Ca²⁺ caused a biphasic inhibition, with time constants of 1.7 ± 0.3 min (n = 3) and 128.4 ± 33.4 min (n = 3). An increase in cytosolic Ca²⁺ concentration from <1 nM to 1 μM was accompanied by a decrease in channel activity. Increasing cytosolic Ca²⁺ to 10 μM exhibited a pronounced inhibitory effect. Single channel conductance, however, was unchanged by increasing free Ca²⁺ concentrations from <1 nM to 10 μM. Collectively, these results provide the first characterization of rENaC heterologously expressed in a mammalian epithelial cell line, and provide evidence for channel regulation by cytosolic Na⁺ and Ca²⁺.     

Back to the future with the AGP–Ca2+ flux capacitor

Background

Arabinogalactan proteins (AGPs) are ubiquitous in green plants. AGPs comprise a widely varied group of hydroxyproline (Hyp)-rich cell surface glycoproteins (HRGPs). However, the more narrowly defined classical AGPs massively predominate and cover the plasma membrane. Extensive glycosylation by pendant polysaccharides O-linked to numerous Hyp residues like beads of a necklace creates a unique ionic compartment essential to a wide range of physiological processes including germination, cell extension and fertilization. The vital clue to a precise molecular function remained elusive until the recent isolation of small Hyp–arabinogalactan polysaccharide subunits; their structural elucidation by nuclear magentic resonance imaging, molecular simulations and direct experiment identified a 15-residue consensus subunit as a β-1,3-linked galactose trisaccharide with two short branched sidechains each with a single glucuronic acid residue that binds Ca²⁺ when paired with its adjacent sidechain.

Scope

AGPs bind Ca²⁺ (K_d ∼ 6 μm) at the plasma membrane (PM) at pH ∼5·5 but release it when auxin-dependent PM H⁺-ATPase generates a low periplasmic pH that dissociates AGP–Ca²⁺ carboxylates (pk_a ∼3); the consequential large increase in free Ca²⁺ drives entry into the cytosol via Ca²⁺ channels that may be voltage gated. AGPs are thus arguably the primary source of cytosolic oscillatory Ca²⁺ waves. This differs markedly from animals, in which cytosolic Ca²⁺ originates mostly from internal stores such as the sarcoplasmic reticulum. In contrast, we propose that external dynamic Ca²⁺ storage by a periplasmic AGP capacitor co-ordinates plant growth, typically involving exocytosis of AGPs and recycled Ca²⁺, hence an AGP–Ca²⁺ oscillator.

Conclusions

The novel concept of dynamic Ca²⁺ recycling by an AGP–Ca²⁺ oscillator solves the long-standing problem of a molecular-level function for classical AGPs and thus integrates three fields: AGPs, Ca²⁺ signalling and auxin. This accounts for the involvement of AGPs in plant morphogenesis, including tropic and nastic movements.