Abstract
The role of voltage-dependent (IKv) and large conductance Ca2+-activated (BKCa) K+ currents in the function of the rat aorta was investigated using specific BKCa and KV channel inhibitors in single rat aortic myocytes (RAMs) with patch-clamp technique and in endothelium-denuded aortic rings with isometric tension measurements.
The whole-cell K+ currents were recorded in RAMs dialysed with 200 and 444 nM Ca2+ and in perforated-patch configuration. Electrophysiological analysis demonstrated that IKv appeared at ⩾−40 mV, while BKCa (isolated using 1 μM paxilline) were seen positive to −20 mV in all conditions.
Voltage-dependent characteristics, but not maximal conductance, of IKv was significantly altered in increased [Ca2+]i. Correolide (1 μM) (a KV1 channel blocker) did not inhibit the IKv, whereas millimolar concentration of TEA (IC50=3.1±0.6 mM, n=5) and 4-aminopyridine (4-AP, IC50=5.9±1.9 mM, n=7) suppressed IKv. These results and immunocytochemical analysis suggest the KV2.1 channel to be a molecular correlate for IKv.
In nonstimulated aortic rings 1–5 mM TEA and 4-AP (inhibitors of IKv), but not paxilline (1 μM), caused contraction. The frequency of contractile responses to TEA and 4-AP was increased in the presence of 10 mM KCl, which itself did not significantly affect the aortic basal tone.
Phenylephrine (15–40 nM) induced sustained tension with superimposed slow oscillatory contractions (termed OWs). OWs were blocked by diltiazem, ryanodine and cyclopiazonic acid, suggesting the involvement of L-type Ca2+ channels and ryanodine-sensitive Ca2+ stores in this process.
TEA and 4-AP, but not IbTX, paxilline or correolide, increased the duration and amplitude of OWs, indicating that IKv is involved in the control of oscillatory activity.
In conclusion, our findings suggest that the KV2.1-mediated IKv, and not BKCa, plays an important role in the regulation of the excitability and contractility of rat aorta.
Keywords: Vascular smooth muscle cells, potassium channels, single smooth muscle cells, patch-clamp technique, rhythmic contraction, thoracic aorta, rat, Ca2+-activated K+ channels, voltage-gated K+ channels, KV2.1 channel
Introduction
Potassium (K+) channels play an important role in the regulation of the resting membrane potential and vascular contractility. Stimulation of vascular smooth muscle cells (VSMCs) with high K+ or α1-adrenoreceptor agonists causes membrane depolarisation and elevation of intracellular Ca2+ concentration ([Ca2+]i), resulting in contraction and a reduction of vessel diameter. Ca2+ entry via L-type voltage-dependent Ca2+ channels (L-VDCCs), activated by membrane depolarisation, and Ca2+ release from inositol-1,4,5-trisphosphate (IP3) and ryanodine-sensitive intracellular Ca2+ stores are the major contributors to increased [Ca2+]i (Nelson et al., 1990). Membrane hyperpolarisation, caused by the activation of K+ channels leading to the closure of L-VDCCs, and Ca2+ removal from the cytoplasm due to the activity of sarcoplasmic/endoplasmic reticulum Ca2+-ATPase (SERCA) and plasmalemmal Ca2+-ATPase represent the main factors responsible for vessel relaxation. Both large conductance Ca2+ (BKCa) and voltage-gated (KV) K+ channels could be activated under these conditions, thereby hyperpolarising the cell membrane (Nelson & Quayle, 1995).
A selective inhibitor of BKCa channels, iberiotoxin (IbTX), caused contraction of human saphenous arteries (Milesi et al., 1999), and an increase in [Ca2+]i and vasoconstriction of cerebral arteries from adult but not neonatal rats (Gollasch et al., 1998). IbTX also inhibited vasodilatation to nitric oxide and its donors in human coronary artery preconstricted with serotonin (Bychkov et al., 1998). Additionally, IbTX potentiated phenylephrine- (PE) induced contraction in rat small mesenteric arteries (Dora et al., 2000) and increased noradrenaline-dependent contraction and [Ca2+]i in fetal and adult arteries of the sheep (Long et al., 2000) and hamster cremasteric arterioles (Jackson & Blair, 1998). Charybdotoxin (ChTX), another potent inhibitor of BKCa channels, contracted blood vessels isolated from rat mesenteric, femoral and carotid arteries (Asano & Nomura, 2002). An important role of BKCa channels in cerebral vascular reactivity was further supported by experiments with mice lacking the BKCaβ subunit, showing reduced BKCa activity associated with elevated blood pressure and reduced sensitivity of arteries to IbTX (Brenner et al., 2000; Plüger et al., 2000). These findings lead to the conclusion that a transient Ca2+ release from the ryanodine-sensitive Ca2+ stores (Ca2+ sparks) causes a local increase in [Ca2+]i sufficient to activate BKCa and may therefore represent a common mechanism by which the BKCa channels contribute to the regulation of basal vascular tone (Jaggar et al., 1998).
The role of KV channels in pulmonary circulation is well documented (Coppock et al., 2001). Also, it has been previously demonstrated that application of nonselective inhibitors of KV channels such as 4-aminopyridine (4-AP) or 3,4-diaminopyridine caused or augmented agonist- and KCl- induced contractions of arteries and arterioles from various vascular beds of different animal species (Uchida et al., 1986; Knot & Nelson, 1995; Doi et al., 2000; Shimizu et al., 2000; Cheong et al., 2001b; 2002), including humans (Uchida et al., 1986). In rabbit coronary and middle cerebral arteries, the effect of aminopyridines was mimicked by IbTX or ChTX and low (⩽1 mM) concentrations of TEA (Knot & Nelson, 1995; Shimizu et al., 2000), suggesting that KV channels act in concert with BKCa to regulate vascular tone in some blood vessels. However, in rabbit cerebral arterioles preconstricted with endothelin-1, penitrem A (another specific BKCa channel inhibitor) had no effect on vascular tone (Cheong et al., 2002). In this study, patch-clamp observations of K+ currents in single myocytes (recorded under conditions when pipette Ca2+ buffering was minimised) showed that KV currents appeared at more negative voltages than BKCa (Cheong et al., 2002), suggesting a greater contribution of the KV (compared to the BKCa) channels in the control of the resting membrane potential in small blood vessels.
The rat aorta is widely used as an experimental model to study various aspects of electro- and pharmacomechanical coupling in physiological and pathophysiological states (Shimamura et al., 1999). However, very little is known about the relative contribution of the KV channel currents (IKv), compared to BKCa currents, in the control of smooth muscle excitability in this artery. It is also unknown whether an augmentation of [Ca2+]i, which occurs in the presence of vasoconstrictors would alter the IKv properties in this tissue, for example, by inhibiting the current favouring membrane depolarisation as proposed in Gelband & Hume (1995). Therefore, we investigated the functional role and properties of the whole-cell IKv in single RAMs dialysed with an elevated free Ca2+ (200 and 444 nM) pipette solution to mimic an increased [Ca2+]i in stimulated arteries (Chen & Rembold, 1995; Aalkjær et al., 1998; Knot & Nelson, 1998) including aortas (Bruschi et al., 1988; Bova et al., 1990; Papageorgiou & Morgan, 1991), and compared these with whole-cell BKCa current characteristics. The pharmacological profile of the IKv and the BKCa current was then used to assess the relative contribution of each conductance to both resting tone and PE-induced contraction in endothelium-denuded aortic preparations. Our findings suggest that IKv (which is likely to be mediated by K+ efflux predominantly via KV2.1 channels), and not the BKCa current, is the main K+ conductance activated in both resting and stimulated aortic SMCs. In addition, an increased [Ca2+]i altered the voltage-dependent characteristics or the IKv resulting in the augmentation of the current in the physiological range of membrane potentials.
Methods
Male Wistar rats (weight 225–300 g) were killed by cervical dislocation in accordance with U.K. Home Office guidelines, and the midpart of the thoracic aorta was removed, cleaned of connective tissue and cut into rings, which were then either used for enzymatic cell isolation or tension measurements.
Cell isolation for electrophysiology
Aortic rings (width ∼1–1.5 mm) bathed in normal physio-logical salt solution (PSS) were left on ice for 30 min followed by an incubation in Ca2+-free PSS for 10 min at 37°C. Tissue was then transferred into prewarmed nominally Ca2+-free PSS (3 ml) containing 1 mg ml−1 collagenase (Type XI) and incubated for 10 min at 37°C. After gentle trituration, pieces of tissue were placed in a fresh Ca2+-free PSS with 1 mg ml−1 of papain and 1 mM dithiothreitol and incubated for another 10 min at 37°C. The tissue pieces were triturated in enzyme- and Ca2+-free PSS and the papain treatment was repeated two more times. The resulting three volumes of Ca2+-free PSS containing dispersed cells were combined, filtered through 95 μm nylon mesh and centrifuged (1100 × g) for 5 min. The pellet was initially resuspended in 0.5 ml of Ca2+-free PSS and then adjusted to a final volume of 1.5 ml with normal PSS. Cells were stored at +4°C and used on the same day.
Composition of solutions and materials
Composition of PSS was (in mM): 130 NaCl, 5 KCl, 1.5 CaCl2, 1.2 MgCl2, 10 HEPES and 10 glucose; pH was adjusted to 7.2 with NaOH. Nominally Ca2+-free PSS had the same composition as PSS, but CaCl2 was omitted. The pipette solution containing 200 nM free [Ca2+] (Maxchelator, Stanford University, U.S.A.) had the following composition (in mM): 110 KCl, 10 NaCl, 5 MgCl2, 10 HEPES, 10 EGTA and 5 mM CaCl2; pH was adjusted to 7.2 with KOH. Calculated 8 or 444 nM free [Ca2+] in the pipette solution was achieved by adding 0.5 or 7 mM instead of 5 mM CaCl2, respectively. Also, the 8 nM Ca2+-containing pipette solution included 5 mM MgATP (Belevych et al., 2002; Smirnov et al., 2002) and the 444 nM solution had 4 mM MgCl2 instead of 5 mM MgCl2. The pipette solution for perforated patch (PP) recordings contained (in mM): 110 KCl, 10 NaCl, 10 HEPES, 10 EGTA, 0.5 mM CaCl2 and 100 μg ml−1 amphotericin B (Sigma, U.K.). The composition of Krebs solution used for tension measurements was (in mM): 118 NaCl, 25 NaHCO3, 4.9 KCl, 1.2 KH2SO4, 2.5 CaCl2, 1.2 MgSO4, 11.7 glucose. 10 mM K+-containing Krebs was made by equimolar replacement of 4.1 mM NaCl with KCl. Appropriate volumes of TEA (2 M stock) or 4-AP (0.5 M stock solution, pH adjusted to 7.4) were added directly to the organ bath to achieve a required final concentration of the drug.
Basic chemicals were purchased from BDH Merck (U.K.) or Fisher (U.K.). Enzymes for cell isolation, PE, ryanodine, cyclopiazonic acid (CPA) and K+ channel inhibitors, except IbTX (Latoxan), were purchased from Sigma (U.K.). Correolide was obtained as a gift from Merck (U.S.A.).
Electrophysiological experiments
Cells were placed in a chamber with a volume of 100–200 μl and were continually superfused (∼1 ml min−1) with PSS or the test solution via a 5-barrel pipette. Whole-cell membrane currents were recorded using the standard patch-clamp technique at room temperature as described previously (Belevych et al., 2002; Smirnov et al., 2002). Briefly, currents were recorded using an Axopatch-200B amplifier, Digidata 1200 A/D interface and pCLAMP 8.02 software (Axon Instruments, CA, U.S.A.) at a sample rate of 10 kHz and filtered at 2 kHz. The pipette resistance was 2–5 MΩ when filled with the standard pipette solution. Capacitance transients elicited by a 10 mV hyperpolarising step (filtered at 50 kHz and sampled at 200 kHz) were routinely measured after rupture of the cell membrane. The area under the capacitance transient was used to calculate cell membrane capacitance (Cm). To allow for equilibration of the pipette solution with the cell interior, all recordings were started 5 min after establishing the whole-cell configuration. To analyse adequately changes in key characteristics of K+ currents (such as activation and inactivation) under variety of experimental conditions, whole-cell currents were measured between −100 and +80 or +100 mV using either a voltage step or ramp membrane depolarisation, respectively. Holding potential was maintained at −80 mV in all experiments.
Isometric tension recordings
Isolated aortic rings (∼2–2.5 mm width) were mounted at 37°C in an organ bath under 1 g resting tension and equilibrated for 60 min in Krebs solution bubbled with 95% O2/5% CO2. Tissue was stimulated with three consecutive applications of 2.5 μM PE followed by washing with Krebs solution before the start of an experimental protocol. Tension was measured using a Biegestab K30 isometric force transducer (Hugo Sack Elektronics, Germany), MacLab/4 s recording unit and Chart v3.6/s software (ADI Instruments, U.K.), and expressed in grams of tension. Data were sampled at 40 Hz. Endothelium was removed by gentle rubbing of the vessel lumen with horse hair and successful removal was verified by the absence of relaxation to 10 μM acetylcholine in arteries precontracted with 2.5 μM PE. Each experimental protocol was repeated in preparations from at least three animals.
Immunocytochemistry
A drop of cell suspension was placed on a glass coverslip and left for 30 min to allow cells to attach to the glass surface. Cells were then fixed with 4% paraformaldehyde and incubated with anti-Kv antibodies (Alomone, Israel) for 3 h. The binding of the primary antibody was detected using goat anti-rabbit IgG secondary antibodies labelled with Alexa Fluor 488 (Molecular Probes) (1 : 500) and examined under a confocal microscope (FV500, v.3.2, Olympus, U.K.). Negative controls were routinely performed in the absence of primary antibodies and showed no significant nonspecific staining under these conditions.
Curve fitting, statistical analysis and data presentation
Electrophysiological data analysis and curve fitting were performed using pCLAMP 8.2 and Origin 6.02 (Microcal Software, Northampton, MA, U.S.A.) software. The results are expressed as mean±s.e.m. Data were analysed by Student's unpaired t-test and P<0.05 was considered to be statistically significant unless otherwise stated.
Results
Effect of BKCa channel inhibitors on whole-cell K+ currents
To evaluate the relative contribution of IKv and BKCa to the net outward current in the presence of 200 nM [Ca2+]i, the effect of specific BKCa channel inhibitors, IbTX and paxilline, and the nonselective inhibitor TEA, which blocks BKCa at concentrations below 1 mM, were studied. Whole-cell currents were recorded in response to a 2 s voltage ramp from −100 to +100 mV applied every 10 s. K+ channel inhibitors were applied cumulatively for 150–200 s, sufficient to allow a new steady-state level to be reached in the presence of each concentration of the blocker. IbTX at concentrations between 1 and 100 nM progressively suppressed the whole-cell current (Figure 1a). It is worth noting that, in the concentration range between 100 and 300 nM, the effect of IbTX saturated and no significant block was further developed (Figure 1a). The mean IC50 for IbTX, calculated as described in the legend to Figure 1, was 12±5 nM (n=5, Figure 1d). Paxilline, another potent inhibitor of BKCa currents (Li & Cheung, 1999), suppressed the whole-cell current in a similar manner reaching a saturation level between 0.5 and 1 μM (Figure 1b). The overall potency of paxilline was ∼8 times less than that of IbTX (mean IC50=97±19 nM, n=7, P<0.006, Figure 1d). TEA blocked the current with a mean IC50=273±37 μM (n=6, Figure 1c and d), which is similar to the values reported for BKCa channels elsewhere (Langton et al., 1991; Khan et al., 1997). The residual whole-cell K+ current was not blocked by the highest concentration of IbTX and paxilline (16±6 and 11±3% of the net current, respectively, P>0.4, Figure 1a and b), suggesting that both drugs selectively inhibit the BKCa current. Therefore, to eliminate the BKCa component, 1 μM paxilline was used in all subsequent experiments. Based on pharmacological evidence we considered the fraction of the whole-cell current, which was blocked by 1 μM paxilline, as the BKCa current, while the paxilline-resistant component was assumed to be the IKv.
Figure 1.
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Comparison of the KV and BKCa currents in elevated [Ca2+]i
IKv and BKCa were compared under three different conditions: cell dialysis with high free [Ca2+] of 200 and 444 nM in the pipette solution and by using PP recordings. This range of Ca2+ concentrations is similar to the previously measured global changes in [Ca2+]i in nonstimulated (∼150–200 nM) and stimulated intact aortic preparations and single myocytes (Bruschi et al., 1988; Bova et al., 1990; Papageorgiou & Morgan, 1991; England et al., 1993), thus allowing changes in properties of K+ currents to be analysed under conditions that mimic a stimulated RAM. Comparison of the whole-cell currents in cells dialysed with 200 and 444 nM [Ca2+]i showed that the current was increased to a greater extent at positive potentials (by 200–300% between +30 and +100 mV) than in the negative voltage range (by 15–50% between −30 and 0 mV) (Figure 2a). The BKCa channel inhibitor paxilline also reduced the current more potently at positive than at negative potentials in the same cell; however, the relative degree of the block was similar in both 200 and 444 nM [Ca2+]i. For example, at +100 mV paxilline blocked 92.7±1.3 and 90.8±1.9% of the whole-cell current, whereas only 35.4±4.7 and 41.2±3.4% of the current was inhibited by the drug at 0 mV in 200 (n=15) and 444 (n=13) nM [Ca2+]i, respectively. No evidence for a discernible activation of Ca2+-dependent chloride or nonselective conductances was found, since the slope resistance measured in the linear range (between −90 and −60 mV) of the current–voltage (I–V) relationship was not significantly different in cells dialysed with 200 nM (7.9±1.1 GΩ, n=15) and 444 nM (10.6±1.8 GΩ, n=13) free Ca2+.
Figure 2.
Comparison of KV and BKCa currents in RAMs dialysed with different [Ca2+]i and recorded using the perforated patch mode (as indicated at the top of each panel). (a) Whole-cell currents measured before (open symbols) and after addition of 1 μM paxilline (filled symbols). (b) Comparison of the paxilline sensitive (BKCa, open circles) and paxilline insensitive (KV, filled circles) currents. Currents were corrected for a residual leak calculated from the slope resistance measured in the linear range of the I–V (between −100 and −60 mV) in each cell and then normalised to that at +100 mV for each component. (c) Shows the same normalised currents as in (b) but at an expanded scale. Data presented as mean±s.e.m. for 15 (200 nM), 13 (444 nM) and 19 (perforated patch) RAMs.
To compare the effect of paxilline on the whole-cell current in RAMs in which [Ca2+]i was not influenced by the pipette Ca2+ buffer, PP recordings were performed (Figure 2a, right panel). As can be seen from the figure, a significant component of the paxilline-insensitive current was present over a wide range of membrane potentials, suggesting that the activation of the BKCa current is relatively small under resting conditions.
To analyse the relative contribution of the BKCa and IKv recorded in two pipette [Ca2+] and in the perforated patch mode, the I–V's of the paxilline-sensitive and -insensitive currents were leak corrected, normalised to the current at +100 mV and compared over the whole range of membrane potential tested (Figure 2b), and also at the expanded scale in Figure 2c. This comparison clearly shows that the paxilline-insensitive KV channel current was activated at more negative potentials than the paxilline-sensitive BKCa current under all three experimental conditions. These results strongly suggest that, despite the increased [Ca2+]i, the IKv is the predominant K+ current activated close to the resting membrane potential measured in rat aortic smooth muscle preparations (Chen & Suzuki, 1989).
Steady-state activation and availability of IKv in elevated [Ca2+]i
It has been previously suggested that elevation of intracellular Ca2+ concentration can inhibit IKv in VSMCs (Gelband & Hume, 1995). We therefore compared the maximal conductance for the IKv measured under the three experimental conditions described above. Since the current amplitude is significantly underestimated when measured with the ramp protocol (data not shown), I–V relationships for the peak IKv were derived from currents measured using a 300 ms test pulse applied between −100 and +80 mV. The peak amplitude of the IKv was derived as an asymptotic value of a single exponential fit of the current activation kinetic (as previously described Belevych et al., 2002; Smirnov et al., 2002). The peak IKv was converted into conductance assuming the K+ equilibrium potential to be equal to −83 mV, plotted against membrane voltage and fitted with the standard Boltzmann function in order to attain the maximal conductance (Gmax), the half-activation (Va) and the slope factor (ka) values. Figure 3a compares the averaged conductance–voltage relationships obtained in 200 and 444 nM [Ca2+]i and in the PP mode. The mean Gmax was similar for IKv measured in 444 nM [Ca2+] (87±12 pS/pF, n=15) and with the PP technique 86±8 pS/pF, n=9). Although Gmax was increased in 200 nM [Ca2+] (114±20 pS/pF, n=15), this value was not significant compared to the other two conditions. Interestingly, no significant differences in Va and ka values were found in 200 nM [Ca2+]i (−4.9±2 and 14.7±0.7 mV, respectively, n=15) compared to those obtained with PP recordings (−4.7±4.1 and 14.1±1.4 mV, respectively, n=9). However, cell dialysis with [Ca2+]i=444 nM shifted the steady-state activation dependency to the right by ∼8 mV (Va=3±2.1 mV, P<0.011 when compared with 200 nM Ca2+ and P<0.037 when compared with the PP using one-tailed t-test). Also, the ka value (which represents the maximum exponential slope of the activation curve) was significantly increased to 18.6±1.1 mV (n=15, 0.007<P<0.023).
Figure 3.
Comparison of the voltage-dependent characteristics of the IKv recorded in different [Ca2+]i. (a) Steady-state activation of the IKv measured with 300 ms step protocol. Currents in each cell were leak subtracted, converted into conductance densities (gKv), averaged and plotted against membrane potential (Vm). gKv measured in 15, 15 and 9 RAMs using 200 and 444 nM pipette Ca2+ and PP, respectively, were averaged and fitted with the standard Boltzmann function (solid lines) with the mean parameters described in the text. (b) IKv availabilities measured at the test potential +60 mV followed 10 s conditioning membrane depolarisations between −100 and 0 mV. The interval between two pulses was 10 ms. Current amplitude measured during the test step was normalised to the maximal current recorded at a conditioning potential of −90 or −100 mV. The averaged normalised IKv was then fitted to the Boltzmann function with inactivation parameters described in the text. Dashed lines indicate half-inactivation potentials. Solid triangles show availability of the BKCa current measured at the test potential of +100 mV in the absence of paxilline (n=6). All experiments were performed in the presence of 1 μM paxilline unless otherwise indicated. Holding potential −80 mV.
The effect of [Ca2+]i on the IKv inactivation was assessed using a two-step voltage protocol as described in the legend to Figure 3b. The standard Boltzmann equation was used to compare statistically the effect of increased [Ca2+]i on the availability of IKv in RAMs. The IKv inactivation dependence was shifted by ∼10 mV to more negative membrane voltages in RAMs dialysed with 200 nM free Ca2+ (the half-inactivation potential, Vh, was −58.2±2.1 mV, n=15) or 444 nM free Ca2+ (Vh=−56.5±1.9 mV, n=15) in comparison to nondialysed cells (Vh=−47.2±3.3 mV, n=6, 0.008<P<0.012). In elevated [Ca2+]i, a small but significant increase in the slope factor, kh, (10.22±0.41 mV, n=15) and in the noninactivating component (0.15±0.03, n=15) was observed in comparison to those obtained with the 200 nM Ca2+ in the pipette solution (8.96±0.38 and 0.08±0.01 mV, respectively, n=15, 0.01<P<0.022). In perforated patch recordings, although no significant change in the mean kh was found (9.77±1.34 mV, n=6) compared to dialysed RAMs, the IKv inactivated to a significantly smaller degree (0.19±0.02, P<0.0001) than that in 200 nM Ca2+.
It is worth noting that the BKCa was not significantly inactivated in this range of membrane potentials (Figure 3b). Thus, when the two-pulse voltage protocol was applied in the absence of paxilline, the overall suppression of the current amplitude measured at the test pulse to +100 mV (mainly the BKCa) by conditioning depolarisation between −40 and 0 mV was only 11–23%.
Pharmacological characterisation of IKv and immunocytochemical detection of KVα-isoforms
Expression of multiple types of KV1 α-genes has previously been detected in rat aorta (Cox et al., 2001). We have also shown protein expression of KV1.2, KV1.5 and KV2.1 α-subunits in adult rat aortic smooth muscle (Belevych et al., 2002). To verify whether members of the Kv1 subfamily contribute to the IKv in RAMs, 1 μM correolide, a nortriterpene purified from the tree Spachea correae that blocks all KV1 channels in the nM range (Felix et al., 1999; Hanner et al., 1999), was used. Cells were stimulated every 10 s with a 300 ms voltage step to +60 mV and correolide was applied at time point 0. No significant inhibition of the current was observed in six RAMs studied (Figure 4a (left) and b (open circles)). In contrast, in rat conduit pulmonary arterial KV1 cells (which were used as a positive control since the IKv1 is thought to be mediated predominantly by KV1 α-subunits (Smirnov et al., 2002)), the current was blocked by 61±5% within the same period of time (n=3, Figure 4a (right panel) and b (filled circles)).
Figure 4.
Pharmacological characterisation of IKv. (a) Effect of 1 μM correolide on IKv recorded in representative RA cells (left, Cm=13.5 pF) and IK1 cell from rat conduit pulmonary artery (RPA, right, Cm=6.6 pF) in the absence and 5 min after application of the inhibitor (shown by arrows). (b) Time dependence of the effect of correolide (applied at time 0) on the IKv in six RAMs and three RPA cells (P>0.22, paired t-test). Current was normalised to the mean current recorded in the absence of the inhibitor. RPA cells were isolated and IKv1 current was defined in a manner previously described in (Smirnov et al., 2002). (c) Effect of TEA and 4-AP on IKv. Cells were dialysed with either 200 nM (n=5) or 8 nM (TEA, n=3, 4-AP, n=7) free Ca2+ and IKv was measured with a 300 ms step to +60 mV applied every 10 s. Inhibitors were added cumulatively and the current amplitude, in the presence of each concentration of the drug, was normalised to that in the absence of TEA. Solid lines were drawn according to the equation described in the legend to Figure 1 with the mean IC50 and A values described in the text.
The lack of effect of the selective KV1 α-subunit inhibitor correolide on IKv in RAMs suggests that IKv is likely to be mediated by either the Kv2.1 or the Kv3.1 delayed rectifier channels previously found in vascular SMCs (Coppock et al., 2001). One of the most distinguished pharmacological features of both channels is an approximate 30 times difference in their sensitivity to TEA; the KV2.1 is blocked by millimolar, concentrations, while the KV3.1b by 100 μM concentrations of TEA (Post et al., 1996). Therefore, the TEA sensitivity of the IKv recorded using the same protocol as for correolide was investigated in RAMs dialysed with 200 nM Ca2+. Cumulative addition of TEA blocked IKv in a concentration-dependent manner with a mean IC50 of 3.1±0.6 mM and a residual component A=0.1±0.02 (n=5, Figure 4c). A similar effect of TEA (IC50=3.2±0.7 mM, A=0.1±0.01, n=3) was also observed under conditions when the pipette solution contained 8 nM free Ca2+ in the presence of both 1 μM paxilline and 10 μM glibenclamide in the external PSS (Figure 4c). Cumulative addition of 4-AP also blocked the IKv (recorded with high buffered pipette Ca2+) in the millimolar concentration range with a mean IC50=5.9±1.9 mM and A=0.5±0.08 (n=7, Figure 4c).
Immunostaining of single rat aortic SMCs with anti-KV1.2, anti-KV1.5 and anti-KV2.1 antibodies clearly demonstrated a strong labelling for the KV2.1 α-protein using both lower and higher antibody dilutions, while only weak staining was detected for anti-KV1.2 and anti-KV1.5 antibodies (Figure 5).
Figure 5.
Immunocytochemical detection of KV channels in RAMs. Localisation of KV subunits in rat aortic SMCs which were fixed, permeabilised and stained with corresponding anti-KV2.1, anti-KV1.2 and anti-KV1.5 antibodies at dilutions indicated within parentheses. Confocal images and superimposed confocal and transmitted light images are shown on the left and right in each panel, respectively. Horizontal bars 10 μM.
Effect of changes in [Ca2+]i on the whole-cell steady-state IKv current in RAMs
Changes in the voltage-dependent characteristics of IKv caused by increased [Ca2+]i (Figure 2) can affect the number of channels open in the physiological range of membrane potential (Nelson & Quayle, 1995). To evaluate this possibility, we calculated the steady-state IKv as a product of activation and inactivation functions, using the mean activation and inactivation parameters described in the text. Figure 6 compares the predicted whole-cell steady-state IKv (also referred to as the ‘window current') calculated for [Ca2+]i equal to 200 nM (black line) and 444 nM (grey line) and for that in nondialysed RAMs (dashed line). Although the steady-state IKv was reduced in dialysed cells compared to nondialysed RAMs, the comparison of the ‘window' IKv under controlled [Ca2+]i showed an approximately two-fold increase in the [Ca2+]i augmented the steady-state IKv over the physiological range of membrane potentials. For example, at −60 and −30 mV the whole-cell open state probability of IKv increased from 0.013 to 0.019 and from 0.006 to 0.01, respectively. Such an increase in IKv could assist membrane repolarisation and lead to relaxation of the aorta during agonist-induced elevation of [Ca2+]i.
Figure 6.
Comparison of the whole-cell steady-state IKv. The predicted steady-state IKv (expressed as a fraction of 1) was derived from the product of the steady-state activation and availability dependences with the mean half-activation and half-inactivation potentials and slope factor values recorded in the presence of PP (dotted line), 200 (solid line) and 444 (grey line) nM free Ca2+ in the pipette solution as described in the text. The noninactivating component of the current has not been taken into account in this analysis.
Contribution of IKv to the control of resting tension in rat aorta
To investigate the contribution of Kv currents to the resting tension, the effects of K+ channel inhibitors were evaluated in the presence of 10 mM K+ in order to depolarise the cell membrane and enhance the K+ channel activity. Application of similar concentrations of K+ produced ∼5 mV membrane depolarisation in rat conduit pulmonary arteries (Chen & Suzuki, 1989), but generally did not cause a significant effect on the basal tension (Auer & Ward, 1998; Andersen et al., 1999; Doi et al., 2000). Under our experimental conditions, no significant difference in the basal tension measured in Krebs and 10 mM K+ solutions (0.57±0.02 versus 0.58±0.02 g, respectively, n=30) was found. Cumulative addition of TEA between 1 and 5 mM induced contractions with superimposed twitch-like oscillations (Figure 7a). An increase in the TEA concentration up to 10–20 mM caused only a slight further increase in the tonic component. In normal Krebs solution (5.9 mM K+), contractions to the same concentrations of TEA were observed less frequently than in elevated 10 mM K+ (Figure 7c). For example, only 3/34 and 5/34 preparations contracted in response to 1 and 5 mM TEA, respectively, in comparison to 3/13 and 8/17 aortic rings maintained in the presence of 10 mM K+. It is worth noting that responses to low concentrations of TEA were nearly maximal and tended to decrease spontaneously despite the presence of the inhibitor, which made analysis of the TEA concentration-dependent relationship difficult. Therefore, the frequency of occurrence of the TEA-induced response, measured as the presence of contraction and/or oscillations normalised to the total number of experiments performed with each dose of TEA, was measured instead. The frequency response demonstrates that TEA-induced contractions are facilitated by higher doses of the drug and in the presence of 10 mM K+ (Figure 7c).
Figure 7.
The effect of TEA and paxilline on the basal tone in the endothelium-denuded rat aorta in the presence of 10 mM K+. (a) Effect of cumulative addition of TEA. (b) Effect of 1 μM paxilline. (c) Comparison of the percentage of preparations eliciting TEA-induced contraction in normal Krebs and 10 mM K+ solutions. Frequency response was measured as a percentage ratio of contractions evoked by each concentration of TEA to the total number of applications of the inhibitor in normal Krebs solution (open bars, total attempts=34) and in the presence of 10 mM K+ (solid bars, total attempts=17, except 1 mM where n=13).
Application of 5 and 10 mM 4-AP also induced contractions similar to those induced by TEA (data not shown). 4-AP (5 mM) triggered contraction in 1/5 and 2/4 preparations in the absence and presence of 10 mM K+ solution, respectively, whereas 10 mM 4-AP constricted all aortic rings tested (n=6). A lower dose of 4-AP (1 mM), however, did not cause contraction either in the absence (n=5) or in the presence of 10 mM K+ (n=4).
In the presence of 10 mM K+, the addition of 1 μM paxilline (Figure 7b, n=7) or 10 μM glibenclamide (n=5), a selective inhibitor of ATP-sensitive K+ (KATP) channels, or combination of both drugs (n=3) applied for 30 min did not produce a contraction.
Role of IKv in agonist-induced contraction in rat aorta
To investigate which type of K+ current was activated in rat aorta stimulated with an agonist, the effects of the K+ channel inhibitors (TEA, 4-AP, paxilline, IbTX and correolide) were studied on PE-induced contractions. Aortic rings were stimulated with concentrations of PE between 15 and 40 nM, close to the half-maximal response for PE in endothelium-denuded rat aorta (EC50=31±5 nM, n=13, our unpublished observation). Application of submaximal PE concentrations produced a complex response causing an initial increase in the basal tension, followed by superimposed slow waves of contractions (termed oscillatory waves or OWs) (Figures 8 and 9). Each OW was characterised by a marked plateau with superimposed periodic fluctuations probably representing the summation of several shorter twitch-like contractions (Figures 8 and 9, insets). OWs were consistently evoked by low PE concentrations (including two preparations which required 50 and 80 nM) in 65/73 aortic rings obtained from 25 animals. In the remaining eight preparations, four showed only periodical twitch-like contractions and four produced sustained tension with superimposed fluctuations of small amplitude.
Figure 8.
Effect of diltiazem, ryanodine and CPA on PE-induced rhythmic contractions in the endothelium-denuded rat aorta. (a) Effect of 200 nM and 1 μM of diltiazem (DILT). Inset: two superimposed OWs before (trace 1) and after addition of 200 nM diltiazem (trace 2). Traces were aligned at the beginning of each OW to aid comparison. (b) Effect of 1 and 3 μM ryanodine (Rya) on PE-induced OWs. Inset: superimposed traces before (1) and in the presence of 1 μM ryanodine (2 and 3). The baseline in traces 2 and 3 was adjusted by 10 and 40 mg, respectively, for better alignment with trace 1. Note that neither diltiazem nor ryanodine affected the PE-induced sustained contraction. (c) Effect of 5 and 10 μM CPA. Traces in (a–c) were recorded from three different preparations.
Figure 9.
The effect of K+ channel blockers on PE-induced rhythmic activity in endothelium-denuded rat aorta. (a–d) show the effect of various concentrations of TEA, 4-AP, paxilline and IbTX on OWs, respectively. Insets: superimposed OWs marked by letters in the absence and presence of the K+ channel inhibitors. In order to facilitate a comparison, the baseline was adjusted by 96 (trace 2), 59 (trace 3) and 21 (trace 4) mg in panel (a), by 90 mg (trace 3) in panel (b), and by 19 (trace 2) and 43 (trace 3) mg in panel (d).
Since, as described below, the K+ channels inhibitors affected only rhythmic activity but not sustained contraction, OWs were characterised quantitatively by measuring the amplitude, as the difference between the maximal and the minimal amplitudes, and the duration at 50% of the maximal amplitude of OWs. Each measurement was calculated as an average of at least three OWs, giving a mean OW duration of 113±5 s (n=65, range 21–252 s). Variations in both the amplitude (range 133–720 mg with a mean value of 359±15 mg) and the frequency (range 0.13–1.32 waves/min with a mean of 0.29±0.02 waves/min) of OWs were also observed (n=65). The mean sustained tension (measured as the difference between the minimum active tension achieved for a given dose of a drug and the resting tension measured in the absence of any stimulants) developed at these concentrations of PE was 0.34±0.02 g (n=65). No correlation between the magnitude of sustained contraction and the amplitude, the frequency or the duration of OWs was found (correlation coefficient was between 0.02 and 0.36).
OWs were suppressed by 0.2–1 μM diltiazem, a selective inhibitor of L-VDCC, and by 1–2 μM ryanodine, which inhibits Ca2+ release from ryanodine-sensitive stores, (Figure 8a and b, respectively). Both agents blocked OWs in a similar manner, causing an initial shortening of OWs by decreasing the number of individual twitch-like contractions within OWs, followed by complete cessation of OWs (Figure 8a and b, insets). In addition, OWs were rapidly inhibited by 5–10 μM CPA (a SERCA inhibitor). The effect of CPA was also associated with a gradual increase in the sustained tension (Figure 8c), whereas no significant inhibition of PE-induced sustained contraction was found in the presence of diltiazem or ryanodine (Figure 8a and b). It is worth mentioning that OWs were not blocked by 50 μM niflumic acid, an inhibitor of Ca2+-activated Cl− channels, suggesting that activation of this conductance was not essential for the generation of rhythmic activity under our experimental conditions (data not shown).
The addition of increasing concentrations of TEA caused a progressive increase in the amplitude and duration of OWs (Figure 9a), as expected from the inhibition of TEA-sensitive K+ channels participating in the OW relaxation process. Application of 4-AP caused two effects: an initial transient decrease in the PE-induced sustained contraction and a significant increase in both the amplitude and duration of OWs (Figure 9b). Although the reason for the 4-AP-dependent decrease in tension is not clear, we did not observe any relaxant effect of 4-AP on the basal tension measured both in Krebs and 10 mM K+ solutions, indicating that the development of some tone is required for this to be observed. Nevertheless, the effect of 4-AP on the duration and amplitude of OWs was very similar to that of TEA, suggesting that the K+ conductance involved in the regulation of rhythmic activity is also 4-AP sensitive. A marked reduction in the frequency of OWs usually observed in the presence of 4-AP could be partially due to a decreased level of sustained contraction in the presence of the drug. For example, the sustained tension was decreased by 8±2% (n=7) and 12±2% (n=5) in the presence of 1 and 5 mM 4-AP, respectively. It is worth noting that with time a slow decrease in the PE-induced sustained tension, observed in some preparations, caused a reduction in the frequency of OWs. This was also associated with a decrease in the duration and amplitude of OWs; effects which are opposite to those observed in the presence of 4-AP. In contrast to TEA and 4-AP, addition of the BKCa channel inhibitors paxilline (Figure 9c) or IbTX (Figure 9d) had no significant effect on the amplitude and duration of OWs, nor the sustained tension, suggesting that BKCa currents are not involved in the regulation of PE-induced contraction of rat aortic smooth muscle.
To compare quantitatively the effect of K+ channel inhibitors on OWs in all preparations, relative changes in the amplitude and duration of OWs observed in the presence of K+ channel inhibitors were averaged expressed as a percentage, and plotted against the corresponding concentration of the drug (Figure 10). The mean changes in both the amplitude and duration of OWs observed in the presence of TEA or 4-AP (both at 5 mM) were significantly different from those measured in the presence of the maximal concentration of the BKCa channel inhibitors (0.008<P<0.03). In addition to this, application of 1 μM correolide for at least 30 min did not significantly affect either the amplitude (1.6±6.1%) or the duration (−5.9±9.1%) of OWs in six aortic rings tested, suggesting that KVα1 channels are not active in SMCs in the intact preparation.
Figure 10.
Comparison of the effect of K+ channel inhibitors. (a–d) summarise the effect of TEA (a), 4-AP (b), paxilline (c) and IbTX (d) on the amplitude and duration of OWs. The amplitude and duration of OWs were measured in the presence of each concentration of a K+ blocker, normalised to that in the absence of the drug and expressed as percentage of relative change. The control value was measured as the mean of three OWs just before the inhibitor was added to the organ bath and set as 100%. Statistical analysis is given in the text.
Discussion
Our primary findings demonstrate that KV currents (via channels formed mainly by KV2.1 α-subunits), and not BKCa currents, are responsible not only for maintaining the resting tension of rat aorta but also for the regulation of induced rhythmic activity of this tissue. The characterisation of the IKv in cells dialysed with 200 and 444 nM free Ca2+ demonstrated significant changes in the voltage-dependent properties, but not in the maximal conductance, of the KV current. This can lead to the enhancement of the IKv in the physiological range of membrane potentials, thereby promoting membrane hyperpolarisation.
IKv is the predominant K+ conductance in rat aortic myocytes
To differentiate between the KV and BKCa channel currents, we used 1 μM paxilline in most of our experiments. Despite being several times less potent than IbTX, paxilline selectively blocked BKCa currents with an IC50=97 nM (Figure 1), which was similar to that reported previously for BKCa currents in rat mesenteric arterial myocytes (IC50=37.5 nM) (Li & Cheung, 1999). Based on the sensitivity to paxilline, we considered the paxilline-sensitive component of the whole-cell current as BKCa, while the paxilline-resistant component was assumed to predominantly be the KV current.
In perforated patch recordings (Figure 2a), the amplitude of the BKCa current was significantly smaller than that in cells dialysed with 200 or 444 nM [Ca2+], indicating that in nondialysed RAMs [Ca2+]i is maintained at low levels close to the plasmalemmal membrane. An increase in [Ca2+]i from 200 to 444 nM (assuming that 5 min was sufficient for equilibration between the pipette solution and the cytosol) resulted in a significant augmentation of the BKCa current in the positive, and not the negative (<0 mV), voltage range. A comparison of the apparent activation threshold of BKCa and KV currents in elevated [Ca2+]i (Figure 2) clearly demonstrates that the appearance of IKv was shifted by ∼20–30 mV to more negative membrane potentials than that of the BKCa. These findings echo the results obtained in rabbit cerebral arterioles, where IKv (recorded with a low Ca2+-buffered pipette solution containing 0.2 mM EGTA) was activated by ∼20 mV more negative than BKCa currents (Cheong et al., 2002), and in rat intrapulmonary arterial SMCs, where cell dialysis with ∼0.5 μM [Ca2+]i only caused a small (16–30%) increase in the amplitude of the TEA-sensitive (BKCa) current at membrane potentials positive to −10 mV (Smirnov & Aaronson, 1994; Smirnov et al., 1994). Furthermore, practically no BKCa single channel activity was observed below −20 mV in inside–out patches from freshly isolated RAMs or myocytes maintained in primary culture and superfused with 0.1 μM Ca2+, and only a ∼10% increase in the channel open probability at −20 mV was observed at 1 μM [Ca2+]i (Sadoshima et al., 1988; England et al., 1993). Interestingly, a relatively low Ca2+ sensitivity of single BKCa channels, requiring >1 μM Ca2+ for the channel to be active at negative voltages, was observed in both rat small cerebral arteries and hamster cremasteric arterioles (Jackson & Blair, 1998), correlating with a low (Liu et al., 1998) or complete absence (Jackson & Blair, 1998) of contractile response of intact vessels to IbTX. Conversely, perfusion of single SMCs isolated from human saphenous veins with a pipette solution containing only 0.1 mM EGTA resulted in a marked activation of BKCa currents in the negative voltage range and application of 50 nM IbTX caused contraction of the intact preparation (Milesi et al., 1999). Although the exact reason for the differential Ca2+ sensitivity of BKCa currents in some VSMCs is not clear, possible explanations could include the existence of BKCa splice variants with a different Ca2+ sensitivity (Sansom & Stockand, 1994); differences in the functional expression the BKCa β-subunits (Brenner et al., 2000; Plüger et al., 2000) and/or interaction between α and β subunits (Tanaka et al., 1997); a spatial distribution of BKCa channels in VSMCs (e.g. their colocalization with ryanodine receptors allowing a rapid and large increase in [Ca2+]i in the channel vicinity (Jaggar et al., 1998)) or a combination of these and maybe other yet to be identified factors.
Effect of elevated [Ca2+]i on IKv
It has been previously suggested that the enhancement of intracellular Ca2+ can directly inhibit IKv in some types of VSMCs (Gelband & Hume, 1995). In rat aortic SMCs, the comparison of conductance–potential relationships of IKv studied under three different experimental conditions did not reveal significant changes in the maximal conductance of the KV current (Figure 3a), suggesting that IKv is not directly blocked by the rise in intracellular Ca2+ at least up to ∼0.4 μM in this preparation. Nevertheless, the voltage-dependent characteristics of the IKv were markedly altered in cells dialysed with increasing [Ca2+]i. The most significant effect was on the IKv steady-state activation dependence shifting it rightward and decreasing its voltage sensitivity (via an increase in the slope factor) by ∼30%. In addition, a small decrease in the slope of the IKv availability was also observed at [Ca2+]i=444 nM. Ca2+-dependent changes in the steady-state voltage-dependent characteristics of the IKv in RAMs produced an increase in the open state probability of the current (Figure 6) that may be important in membrane hyperpolarisation in agonist-stimulated intact tissue as discussed below. Although differences in the activation and inactivation of the IKv were observed between dialysed and nondialysed RAMs, a direct comparison of voltage-dependent parameters is complicated by the fact that these characteristics of IKv in RAMs also depend on the phosphorylation state of the channel (Tammaro et al., 2001), as well as on the presence of intracellular magnesium ions (Tammaro & Smirnov, 2003), which may differentially alter the IKv properties depending on the composition of the pipette solution. This is further supported by a comparison of the IKv activation and inactivation obtained in the present study with those we previously reported in RAMs dialysed with low [Ca2+]i (8 nM) and 5 mM MgATP (Belevych et al., 2002). Both the activation (mean Va=5.2 mV) and the availability (mean Vh=−39.6 mV) of IKv was shifted to more positive membrane potentials, which differ from those in RAMs dialysed with 200 nM Ca2+ despite the fact that the sensitivity of the IKv to TEA was virtually the same under both conditions (Figure 4c).
Molecular identity of IKv in rat aortic SMCs
The molecular identity of delayed rectifier currents in different types of VSMCs is largely unknown, although the gene expression of most KV isoforms has been demonstrated in various types of blood vessels (Davies & Kozlowski, 2001; Cheong et al., 2001b). Recent evidence suggests that, depending on the vessel size and probably animal species, different KV channel isoforms can be responsible for KV currents. Thus, in cerebral circulation, KV1.2/KV1.5 heteromultimers are likely to form IKv in rat small cerebral arteries (Albarwani et al., 2003), whereas different KVα1 isoforms are more important in rabbit (KV1.6 and KV1.5 homo- and/or heteromultimeric complexes; Cheong et al., 2001a) and in murine (KV1.3 and KV1.6 homo- and/or hetero-tetramers; Cheong et al., 2001b) cerebral arterioles. The members of the KVα1 subfamily (KV1.2/KV1.5 heteromultimers) together with the KV2.1/KV9.3 heterotetramers and KV3.1b homotetramers were also proposed to compose IKv in pulmonary SMCs (Coppock et al., 2001). In rat aorta, the expression of multiple KVα1 and KVα2 genes (Roberds & Tamkun, 1991; Cox et al., 2001; Thorne et al., 2002) and proteins (Belevych et al., 2002; Thorne et al., 2002) have been demonstrated previously. However, the analysis of gene and protein expression does not answer the question as to whether the whole-cell IKv is composed of a single or multiple KV component in intact RAMs. To address this question, we used a selective KVα1 inhibitor correolide (Felix et al., 1999; Hanner et al., 1999). Application of 1 μM correolide had no effect on the IKv in RAMs, despite the significantly suppressed KV1-mediated current in rat main pulmonary SMCs (Figure 4a and b). These results support our previous findings that IKv in RAMs was not blocked by 200 nM α-dendrotoxin and 300 nM ChTX (Belevych et al., 2002), suggesting that KV1 α-subunits are unlikely to contribute to the native IKv in this tissue. The KV3.1b channel is sensitive to both TEA and 4-AP in the micromolar range (Grissmer et al., 1994; Post et al., 1996). On the other hand, a relatively slow kinetic of activation of IKv and millimolar sensitivity to 4-AP (Belevych et al., 2002) and TEA (this paper) are characteristic features of the cloned KV2.1 channels (Post et al., 1996), pointing towards the KV2.1 α-subunit as the main component of the KV channel in rat aortic SMCs. The results of the immunocytochemical analysis of the expression of KV α-subunits also support this conclusion.
Role of KV channels in the regulation of contraction of rat aorta
The electrophysiological data in single RAMs suggests that IKv is activated at more negative membrane potentials than BKCa currents (Figure 2), and could therefore be one of the major currents in this tissue to control membrane potential at rest. To assess whether KV channels are also active in the intact nonstimulated aorta at rest (i.e. without the development of contraction), the effect of 1–5 mM TEA and 4-AP (K+ channel inhibitors which block IKv in RAMs) was studied. Both inhibitors caused a marked contraction of endothelium-denuded rat aortic rings in normal Krebs. Notably, stimulatory effects of 4-AP and TEA were enhanced in the presence of 10 mM K+, which depolarises large arteries by ∼5 mV (Chen & Suzuki, 1989) without significant effects on the basal tension (Auer & Ward, 1998; Andersen et al., 1999; Doi et al., 2000). Such a small depolarisation should significantly increase the activation of voltage-dependent K+ channels, such as KV and BKCa, in the negative voltage range (Nelson & Quayle, 1995). However, the specific BKCa inhibitor paxilline did not mimic the effects of TEA and 4-AP under this condition (Figure 7b), which suggests that BKCa currents are not active at rest in the intact aorta, thus supporting the electrophysiological data obtained in single cells. The lack of effect by the selective KATP channel inhibitor glibenclamide also rules out a significant contribution of KATP currents to the regulation of the basal tone in this tissue. Interestingly, potentiation of agonist- and KCl-induced contraction by mM concentrations of 4-AP and TEA was also observed in mouse (Jiang et al., 1999) and rabbit (Cook, 1989) aortas, indicating that activation of a similar type of K+ conductance might contribute to the control of aortic contractility in other species.
Since activation of BKCa currents can be significantly increased in the stimulated tissue by local increases in [Ca2+]i (Pérez et al., 2001), the effect of TEA, 4-AP, correolide, paxilline and IbTX on contraction induced by the α1-adrenoreceptor agonist PE was investigated. The effect of K+ channel blockers on the KCl-induced contraction has not been studied in detail because a decrease in the K+ conductance resulting from a reduction in the driving force for potassium ions could make the interpretation of their effects ambiguous, as was demonstrated with the effect of the K+ channel activator cromakalim on KCl contraction in rat conduit pulmonary arteries (Seiden et al., 2000). Application of PE at concentrations close to the EC50-induced slow rhythmic contractions (termed OWs) superimposed on the sustained tension in endothelium-denuded aortic rings. It is worth noting that although shorter twitch-like contractions have been reported in rat aorta (Freeman et al., 1995), the type of oscillatory contraction described in this paper has not previously been characterised. Neither IbTX and paxilline (the BKCa channel inhibitors) nor correolide (which blocks KVα1 channels) caused any significant effect either on the basal tension or OWs. On the other hand, TEA and 4-AP, which blocked IKv in RAMs, significantly increased both the amplitude and duration of PE-induced OWs, suggesting that TEA- and 4-AP-sensitive IKv is the predominant K+ conductance, which operates during α1-adrenergic stimulation of rat aortic SMCs.
It should be noted that although TEA and 4-AP had a significant effect on PE-induced rhythmic activity, they did not cause an appreciable increase in the sustained tension, suggesting that sustained contraction and OWs could be initiated by different mechanisms. It has been previously shown that stimulation of α1-adrenoreceptors, in addition to release of Ca2+ from IP3-sensitive stores, also causes membrane depolarisation of VSMCs (Mulvany et al., 1982; Chen & Rembold, 1995). Therefore, it is possible that the sustained tension is maintained by IP3-mediated release from intracellular Ca2+ stores, whereas OWs are triggered by membrane depolarisation. The stimulatory effect of the IKv blockers and the inhibitory effect of the L-VDCC inhibitor diltiazem on OWs, but not on the sustained tension (Figures 8a, 9 and 10), support the involvement of both types of voltage-dependent ion channels in the initiation of OWs. Additional sensitivity of OWs to ryanodine (Figure 8b), as well as CPA (Figure 8c), indicates the participation of Ca2+ release from ryanodine-sensitive Ca2+ stores triggered by Ca2+ entry via L-VDCCs in the generation of OWs. Similar effects of the L-VDCCs inhibitors (such as nifedipine or nicardipine), ryanodine and CPA on endothelium-independent rhythmic contractions were reported in rat pulmonary arteries from animals exposed to chronic hypoxia (Bonnet et al., 2001) and treated with monocrotaline (Kiyoshi et al., 2003) to induce hypertension. An increase in sustained tension in the presence of CPA is expected, since CPA constricts arteries by releasing Ca2+ from both ryanodine- and IP3-sensitive stores (Shima & Blaustein, 1992; Noguera et al., 1998; Tosun et al., 1998).
In order to maintain any rhythmic activity, the presence of a negative feedback mechanism is required (Berridge & Galione, 1988; Gustafsson, 1993). If membrane depolarisation is essential to trigger OWs in rat aortic SMCs, then a mechanism capable of hyperpolarising the cell membrane should also be present. In other preparations the BKCa, activated by the rise of [Ca2+]i in addition to an increase in the membrane potential, has been proposed to be the main hyperpolarising K+ conductance. This hypothesis has been supported by the stimulatory effects of IbTX and/or ChTX on rhythmic activity in intact preparations (Gokina et al., 1996; Wesselman et al., 1997; Jiang et al., 1999).
Our experimental evidence entails the involvement of two voltage-dependent conductances in the initiation of rhythmic contraction in rat aorta: L-VDCCs (as the main depolarising conductance) and the delayed rectifier IKv (as the main hyperpolarising K+ conductance), which should act as a pure voltage-dependent oscillator coupled to ryanodine-sensitive stores. If this is the case, then changes in the voltage-dependent characteristics of both channel types should be important in providing a negative feedback loop required for oscillatory behaviour. Ca2+-dependent inactivation, a characteristic feature of L-VDCCs in SMCs, can be responsible for the initial reduction of the Ca2+ entry via L-VDCCs. A subsequent increase in the IKv activation (as a result of membrane depolarisation caused by L-VDCCs) could progressively hyperpolarise the cell membrane.
Potentiation of the steady-state IKv at elevated [Ca2+]i can also contribute to membrane hyperpolarisation in RAMs. In various vascular preparations (Gokina et al., 1996; Peng et al., 1998; Oishi et al., 2002) including rat aortas (Hayashida et al., 1986), the amplitude of oscillations in membrane potential ranged between 5 and 20 mV. Although membrane potential was not measured in this study, it is possible to estimate the degree of cell membrane hyperpolarisation caused by an increased [Ca2+]i using the approach described previously by Nelson and Quayle (1995). Assuming an input resistance of 8 GΩ, which corresponds to a conductance of 125 pS, the total K+ conductance at −60 mV would be equal to ∼90 pS. The estimated number of KV channels per a single RAM is equal to 116, assuming the maximal conductance to the equal to 95 pF/pS (Figure 3a), a mean cell capacitance of 12 pF and a single channel conductance of ∼10 pS (Pascual et al., 1997; Kramer et al., 1998). Taking into account the Ca2+-dependent changes in the open state probability (Figure 6), an increase in the steady-state IKv conductance at −60 and −30 mV should be equal to 7.5 and 4.3 pS yielding membrane hyperpolarisation of 1.1 and 0.5 mV, respectively, which is comparable to oscillatory changes in membrane potential measured with intracellular microelectrodes (Hayashida et al., 1986; Gokina et al., 1996; Peng et al., 1998; Oishi et al., 2002). The Ca2+i-dependent increase in the steady-state IKv is unlikely to be due to differences in the pipette Mg2+ concentration since a similar effect was also observed in RAMs dialysed with 200 nM compared to 10 nM free Ca2+ in the pipette solution containing 0.5 mM MgCl2 (our unpublished observations). Although the precise mechanism of modulation of IKv by intracellular Ca2+ remains unclear and necessitates further experimental evidence, the involvement of Ca2+-dependent protein kinase C (PKC) isoform (e.g. PKCα) in this process is possible (Tammaro et al., 2002; Tammaro & Smirnov, 2002).
In conclusion, our findings suggest that the voltage-dependent K+ current through KV2.1 channels plays a key role in the regulation of contractile activity of rat aorta. Modulation of the voltage-dependent characteristics of IKv by various intracellular factors including calcium and/or calcium-dependent processes could be important in maintaining the function of KV channels in the physiological range of membrane potential.
Acknowledgments
We are grateful to Mr Barry Crowley for technical assistance and Dr G Kaczorowski (Merck, U.S.A.) for the gift of correolide. This work was supported by the British Heart Foundation Grant FS/2000013.
Abbreviations
- 4-AP
4-aminopyridine
- BKCa
large conductance Ca2+-activated K+ current
- ChTX
charybdotoxin
- Cm
cell membrane capacitance
- CPA
cyclopiazonic acid
- IbTX
iberiotoxin
- IKv
voltage-dependent K+ current
- IP3
inositol-1,4,5-triphosphate
- ka
slope factor of activation
- kh
slope factor of inactivation
- KV
voltage-dependent K+ channel
- L-VDCC
L-type voltage-dependent Ca2+ channel
- OW
oscillatory wave of contraction
- PE
phenylephrine
- PP
perforated patch
- PSS
physiological salt solution
- RAM
rat aortic myocyte
- SERCA
sarcoplasmic/endoplasmic reticulum Ca2+-ATPase
- TEA
tetraethylammonium
- Va
half-activation potential
- Vh
half-inactivation potential
- VSMC
vascular smooth muscle cell
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