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Department of Anesthesiology, Baylor College of Medicine, Houston, Texas 77030
Submitted 22 April 2003 ; accepted in final form 11 June 2003
| ABSTRACT |
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calcium; brain; purinergic; small conductance potassium channels; large conductance potassium channels; endothelium-derived hyperpolarizing factor
There are, however, a number of unifying hallmarks common among EDHF-mediated dilations. One in particular is the essential involvement of KCa [for review see Feletou and Vanhoutte (25)]. Although it was initially assumed that the KCa channels critical to EDHF-mediated dilations were large conductance KCa channels (BKCa) located on the smooth muscle (44), it is now generally believed that the KCa channels involved include intermediate conductance KCa (IKCa) alone or in combination with small conductance KCa (SKCa) located on the endothelium (3, 19, 20, 23, 30). The mechanism by which endothelial KCa channel activation translates into a smooth muscle hyperpolarization is still a matter of debate, but has been proposed to result from either 1) direct transfer of hyperpolarization from the endothelium via myoendothelial gap junctions (5, 6, 18, 20, 24, 45, 49) or 2) stimulation of smooth muscle inwardly rectifying K channels (KIR) channels or Na+-K+-ATPase by modest elevations in extracellular K+ concentration ([K+]o) in the intercellular space (20).
One additional role for endothelial KCa channels that is often assumed in intact arteries is to facilitate greater influx of extracellular Ca2+ into the endothelium. It is proposed that activated endothelial KCa channels hyperpolarize the endothelium, thus creating a greater electrical driving force for Ca2+ influx [for review, see Nilius and Droogmans (42)]. Given the essential roles for both Ca2+ and KCa channels in EDHF-mediated dilations, it is reasonable to speculate that endothelial KCa channels contribute to endothelial Ca2+ reaching or staying at the Ca2+ threshold required for EDHF-mediated dilations. However, it must be noted that, whereas a role for endothelial K channel activation on Ca2+ flux is widely supported from endothelial cell culture models (32, 3537, 46), there are little data available regarding endothelial intracellular Ca2+ concentration ([Ca2+]i) within the context of intact arteries. Furthermore, the data that exist from pressurized artery preparations appear to conflict regarding the relevance of membrane potential on endothelial Ca2+ handling (27, 33, 50).
In the present studies, experiments were designed to determine the role and subtype of endothelial KCa channels involved in EDHF-mediated dilations within pressurized cerebral arteries. Our use of an intact pressurized artery preparation is significant given that pressurized and nonpressurized vessel preparations differ in many respects, such as in resting membrane potential and [Ca2+]i (29, 34). We evaluated the following three hypotheses regarding the mechanism of EDHF-mediated dilations in pressurized middle cerebral arteries (MCAs): 1) IKCa channel activation and endothelial hyperpolarization is critical to the EDHF-dependent mechanism, 2) IKCa channel activation and endothelial hyperpolarization is sufficient for EDHF-mediated vasodilatation, and 3) IKCa channel-mediated hyperpolarization of the endothelium is required for endothelial [Ca2+]i to reach the threshold for initiating EDHF-mediated dilations.
| MATERIALS AND METHODS |
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Mounting of pressurized/perfused MCAs. MCAs were cannulated with two glass micropipettes as described in detail previously (39). In brief, MCAs were secured to the micropipettes with 12-0 nylon suture and verified to be free of leaks. Warmed (37°C) and gassed (20% O2-5% CO2-balance N2) Krebs was circulated through the chamber (abluminally) and perfused through the lumen of the artery (100 µl/min). Mean intraluminal pressure was set to 85 mmHg and monitored by two inline pressure transducers. After mounting of the MCA, the vessel chamber was placed on the stage of an inverted fluorescence microscope equipped for the simultaneous measurement of artery diameter and either endothelial [Ca2+]i or changes in endothelial membrane potential (
Vm).
Simultaneous measurement of endothelial [Ca2+]i and diameter in intact cerebral arteries. The method for selectively measuring endothelial [Ca2+]i and diameter in pressurized MCA has recently been described in detail (39). Briefly, the endothelium was selectively loaded with fura-2 AM by adding it to the luminal perfusate. Fura-2 AM (0.67 µM) was coadministered with pluronic F-127 (0.02%) to ensure a more even dispersion of fura-2 AM. The artery was perfused luminally with the fura-2 solution for 4 min before a washout period of 15 min. This short incubation with a low concentration of fura-2 AM ensured that the endogenous endothelial esterases were not overwhelmed, thus ensuring that the fura-2 free acid was contained to the endothelium.
Measurement of endothelial [Ca2+]i was performed by alternating between 340 and 380 nm bandpass excitation filters and measuring the fura-2 fluorescence at 510 nm (28, 39). The artery was transilluminated with a red light (>690 nm) for simultaneous measurement of diameter (Intracellular Imaging; Cincinnati, OH). Endothelial [Ca2+]i was determined from a series of in situ calibration curves on the basis of the following equation [Ca2+]i =
[(R Rmin)/(Rmax R)] Kd, where R is the ratio of 340 to 380 fluorescence, Rmin is the ratio in Ca2+-free conditions, Rmax is the ratio in saturating Ca2+ conditions,
is the ratio of the 380 fluorescence with Ca2+ unbound to bound, and Kd is the dissociation constant for fura-2 to Ca2+. An in situ calibration produced the following values: 1.52 (Rmax), 0.18 (Rmin), and 4.35 (
). The Kd was determined to be 282 nM (34).
Measurement of endothelial membrane potential in intact cerebral arteries. Endothelial membrane potential (Vm) changes were measured in pressurized MCA by using a voltage-sensitive dye, 4-{2-[6-(dioctylamino)-2-naphthalenyl]ethenyl}1-(3-sulfopropyl)-pyridinium (di-8-ANEPPS). This dye has previously been utilized to indicate changes in endothelial membrane potential in intact peripheral microvessels (1, 2, 10, 41). Selective endothelial loading of di-8-ANEPPS was achieved by delivering di-8-ANEPPS (10 µM/0.1% pluronic) luminally for 10 min followed by a 10-min washout period. During incubation, the dye becomes associated with the endothelial membrane. Confocal microscopy was utilized to ensure that the dye was confined to the endothelium (see Confocal microscopy of pressurized/perfused cerebral arteries). The ratio of the 560 and 620 emissions (excitation at 475 nm) changes with endothelial membrane potential such that a decrease in the ratio (560/620) indicates a hyperpolarization and an increase indicates a depolarization. The 560/620 ratios were acquired at a frequency of 12.5 Hz by using a fluorometer equipped with matched spinning excitation and emission filter wheels (C & L Instruments; Hummelstown, PA). Because changes in endothelial Vm result in relatively small changes in fluorescence intensity, we felt it was important to eliminate changes in fluorescence intensity due to vasodilatation. We therefore used an inhibitor of smooth muscle actin polymerization (10 µM cytochalasin D administered abluminally) (13) to dilate the arteries before administering the experimental drug. In some vessels, we used papaverine (300 µM, abluminally) as a vasodilator and obtained similar results as with cytochalasin D (not shown). Artery diameter was measured simultaneously with di-8-ANEPPS fluorescence by using an infrared light source and infrared-sensitive video camera. However, because the arteries were predilated, the reported diameter responses to the experimental drugs were obtained in a separate set of vessels.
Confocal microscopy of pressurized/perfused cerebral arteries. Nipkow-type confocal microscopy was used to confirm that the di-8-ANEPPS dye was confined to the endothelium. The vessel chamber containing pressurized/perfused arteries was mounted on the stage of a Nikon TE-2000 fluorescence microscope (Nikon Instruments) coupled with a CARV confocal module set up for detection of di-8-ANEPPS fluorescence (Atto Instruments, Rockville, MD). The di-8-ANEPPS dye was loaded as described above before imaging.
Delivery of pharmacological compounds to the artery. Luminal delivery of pharmacological compounds was achieved by adding the compound to one of the luminal reservoirs connected to the inflow pipette. A miniaturized manifold system was utilized to substantially reduce the dead volume in the connecting tubing and thus speed delivery of the compound to the luminal compartment of the perfused artery. Abluminal delivery of pharmacological compounds was achieved by adding the compound to the abluminal perfusate reservoir. Compounds reached the luminal or extraluminal surface of the artery with a <30-s lag time.
Chemicals and buffers. All drugs and chemicals were obtained from Sigma (St. Louis, MO) with the exceptions of fura-2 AM (TefLabs; Austin, TX), di-8-ANEPPS (Molecular Probes; Eugene, OR), 1-ethyl-2-benzimidazolinone (1-EBIO; Tocris; Ellisville, MO), and 1-[(2-chlorophenyl)diphenylmethyl]-1H-pyrazole (TRAM)-34 (a generous gift from Dr. Heike Wulff, University of California, Irvine). The standard Krebs buffer solution consisted of the following (in mM): 119 NaCl, 4.7 KCl, 21 NaHCO3, 1.18 KH2PO4, 1.17 MgSO4, 0.026 EDTA, 1.6 CaCl2, and 5.5 glucose. The high K+ buffers consisted of either 60 mM [K+] or 90 mM [K+] (calibration of di-8-ANEPPS) with the appropriate reduction in Na+ concentration to maintain an isotonic buffer; the remaining ingredients remained the same as the standard buffer. The Krebs buffer was gassed with a mixture of 20% O2-5% CO2-75% N2 to achieve a pH of 7.4 and a PCO2 of
35 mmHg.
Iberiotoxin (IbTx; 100 nM) selectively blocks BKCa channels, whereas charybdotoxin (ChTx; 70 nM) is a nonselective BKCa/IKCa channel blocker. ChTx has also been shown to block the delayed rectifier (Kv) channels Kv1.2 and Kv1.3 (4). TRAM-34 (10 µM) and clotrimazole (CTZ; 10 µM) are IKCa channel blockers (54). TRAM-34 is a recently developed structural analog of CTZ that is a potent IKCa channel blocker and lacks the cP450 inhibitory activity of CTZ (54). Apamin (Apa; 100 nM) is a selective SKCa channel blocker. High K+ (60 mM) Krebs buffer was used to nonselectively block all K channels.
Calculations and statistical methods. All data are presented as means ± SE. Percent tone is defined as %tone = [(Dmax Dt)/Dmax] x 100, where Dt is the vessel diameter after development of spontaneous tone and Dmax is the maximum diameter of the artery corresponding to the Ca2+-free diameter. Percent diameter change is defined as %diameter change = [(D Dbase)/(Dmax Dbase)] x 100, where D is the diameter in response to a given vasodilator and Dbase is the diameter before the addition of the vasodilator. Percent maximum diameter is defined as %max diameter = (AUCdrug/AUCmax) x 100, where AUCdrug is the baseline corrected area under the curve for 200 s of the response and AUCmax is the maximum possible area under the curve for that time period [(maximum diameter resting diameter) x 200 s].
For comparison of concentration-response curves, a two-way repeated-measures ANOVA was utilized followed by a Tukey's test for individual comparisons when appropriate. For comparison of multiple treatments within one group, a one-way repeated-measures ANOVA was used. Comparison of single treatments between two groups was performed by either paired or unpaired t-test. Significance was defined as P < 0.05.
| RESULTS |
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The ability to selectively deliver di-8-ANEPPS to the endothelium was evaluated for this isolated vessel preparation by confocal microscopy. In three separate vessels studied, di-8-ANEPPS fluorescence appeared uniformly along the lumen of the vessel and was clearly confined to the endothelium (data not shown). In a fourth vessel, the dye leaked from an open side branch and resulted in dye loading of the smooth muscle. The smooth muscle loading was evident as bright circumferential bands perpendicular to the direction of flow and was clearly evident by confocal or standard fluorescence microscopy.
The di-8-ANEPPS ratio changes were calibrated by using valinomycin (5 µM) and various [K+]o to voltage clamp endothelial Vm (52). Valinomycin is a K+ ionophore that serves to increase the conductance value for K+ and thus increase the contribution of inner/outer K+ concentrations to the overall membrane potential. Luminal valinomycin was delivered in the presence of both 5.9 and 90 mM [K+]o. From the Nernst equation, these concentrations of [K+]o should produce endothelial Vm values of 82 and 10 mV, respectively. The full range of the Vm change would be 72 mV. The measured corresponding range of the di-8-ANEPPS ratio change to 5.9 and 90 mM [K+]o was 5.6 ± 0.5% (n = 3). Therefore, the calculated relationship between millivolt and ratio change is 12.9 mV for each 1% change in the 560/620 ratio. This relationship compares well with what others have reported from peripheral vessels (1012 mV/1% ratio change) (2, 11).
Figure 1 shows a representative experiment in which endothelial
Vm was determined with di-8-ANEPPS. Cytochalasin D (10 µM) administered abluminally produced a rapid and near-maximal dilation that was sustained throughout the experiment (Fig. 1A). Fluorescence intensities (F560 and F620) both decreased on artery dilation (Fig. 1B). The drop in fluorescence resulted from the near and far portions of the vessel (from the objective) going beyond the depth of field of the objective. However, as the drops in intensities were equivalent for each wavelength, the 560/620 ratio remained essentially the same (Fig. 1C). The luminal addition of UTP (105 M) produced minimal further change in diameter, whereas the F560 (dotted line) and F620 (solid line) changed in opposite directions (F560 decreased and F620 increased; Fig. 1B). The 560/620 ratio decreased by
4%, thus indicating an endothelial hyperpolarization.
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Diameter and endothelial Vm responses to luminally delivered UTP (105 M) were evaluated in the absence and presence of ChTx (70 nM). Diameter responses are reported from a separate group of vessels, because cytochalasin D was used to predilate the endothelial Vm group vessels. Diameter responses to UTP are reported as the %maximum achievable area under the curve over a 200-s time period (see MATERIALS AND METHODS). The diameter and Vm results are summarized in Fig. 2. Luminal UTP produced significant vasodilatation (88 ± 3%) and endothelial hyperpolarization (42 ± 2 mV). The addition of ChTx to the bath virtually eliminated both the dilation (27 ± 14%) and endothelial hyperpolarization to UTP (5 ± 13 mV). These results indicate that the dilation and endothelial hyperpolarization are mediated primarily by ChTx-sensitive K channels.
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Because ChTx has been shown to inhibit both BKCa and IKCa channels as well as some voltage-sensitive K channels (Kv1.2 and Kv1.3) (4), we sought to determine which ChTx-sensitive channels were essential to the EDHF-mediated response. The %max diameter (Fig. 3) reflects the measured AUC in response to UTP as a percentage of theoretical maximum AUC over a 200-s period (see MATERIALS AND METHODS). Control responses to luminal 10 µM UTP produced significant artery vasodilatation (82 ± 2%) over the measurement period. Application of a selective BKCa channel blocker (IbTx 100 nM) had no significant effect on EDHF-mediated dilations to UTP (73 ± 11%). Similarly, application of a selective SKCa channel blocker (100 nM Apa) had no effect on dilations to UTP (88 ± 4%). However, application of a selective IKCa channel blocker (TRAM-34 10 µM) significantly reduced EDHF-mediated dilations to UTP (32 ± 4%). Combined inhibition of IKCa and Kv channels (TRAM-34 and 3 mM 4-aminopyridine) similarly reduced dilations to UTP (25 ± 6%), although the inhibition was not significantly different than with TRAM-34 alone (P = 0.84, two-way repeated-measures ANOVA). Thus it appears that IKCa channels by themselves contribute considerably to the EDHF-mediated dilation and likely reflect the critical K channel blocked by ChTx.
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If activation of IKCa channels is the critical down-stream event from elevated endothelial [Ca2+]i in the mechanism of EDHF-mediated vasodilatation, then direct activation of IKCa channels should produce a dilatation. We therefore utilized an IKCa channel opener (1-EBIO) to determine the effect of direct activation of endothelial IKCa channels on vessel diameter. Luminal administration of 1-EBIO (1 to 300 µM) produced concentration-dependent vasodilatation that was significantly inhibited by nonselective K channel inhibition with luminal 60 mM K+ (Fig. 4). Furthermore, when 1-EBIO was administered abluminally (smooth muscle side), responses were significantly attenuated compared with luminal administration.
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Although 1-EBIO has been demonstrated to be an effective activator of IKCa channels (15, 21, 31, 51), it was still incumbent on us to confirm that 1-EBIO acts specifically via stimulation of IKCa channels and produces the predicted hyperpolarization of the endothelium in this vessel preparation. Figure 5 summarizes diameter responses as a percentage of control dilations in response to luminal delivery of 1-EBIO (300 µM) with selected BKCa and IKCa channel blockers. Note that 1-EBIO produced a significant dilation that was unaffected by a selective BKCa channel blocker (IbTx 100 nM, n = 3) but was significantly attenuated by a BKCa/IKCa channel blocker (ChTx 70 nM, n = 3) or by an IKCa channel blocker (CTZ 10 µM, n = 4). In addition, Fig. 6 shows that luminal 1-EBIO resulted in significant hyperpolarization of the endothelium (26 ± 4 mV) that was significantly attenuated in the presence of 100 nM ChTx (9 ± 2 mV, P < 0.01). Taken as a whole, these data indicate that luminal 1-EBIO acts primarily by stimulating endothelial IKCa channels. Furthermore, the direct activation of endothelial IKCa channels is sufficient to produce significant endothelial hyperpolarization and subsequent vasodilatation.
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We then sought to determine whether 1-EBIO-mediated vasodilatation was a direct result of IKCa channel-mediated endothelial hyperpolarization or whether perhaps IKCa-mediated endothelial hyperpolarization was simply a means to increase endothelial [Ca2+]i. For instance, as the endothelial membrane potential has been shown to modulate Ca2+ influx, a possible indirect mechanism for 1-EBIO-dependent dilations could be to promote endothelial Ca2+ influx secondary to endothelial hyperpolarization. In this latter scenario, 1-EBIO-mediated hyperpolarization would promote an influx of Ca2+, thus activating some other pathway or enzyme in the EDHF-dependent mechanism. To evaluate these possible mechanisms of 1-EBIO-mediated vasodilatation, endothelial [Ca2+]i was measured in response to 1-EBIO. Endothelial [Ca2+]i was determined fluorometrically by selectively loading the endothelium with fura-2 as demonstrated previously (39, 40). The effect of luminal 1-EBIO on endothelial [Ca2+]i and diameter were determined simultaneously. Luminal UTP (105 M) was subsequently administered to the same vessel as a positive control. Figure 7A summarizes artery diameter in response to 300 µM 1-EBIO. The dilation to UTP (105 M) reflects a steady-state diameter equivalent to 99 ± 4% of maximum. Figure 7B summarizes the corresponding endothelial [Ca2+]i in response to 1-EBIO and to the subsequent addition of UTP. Note that 1-EBIO did not alter endothelial [Ca2+]i despite significant artery dilation. Importantly, the lack of increase in endothelial [Ca2+]i to 1-EBIO was not due to an inability of the endothelium to increase [Ca2+]i, as significant increases to luminal UTP were obtained from the same arteries. Thus it appears that 1-EBIO-mediated vasodilatation via stimulation of endothelial IKCa channels and endothelial hyperpolarization does not result from an increase in endothelial [Ca2+]i. Rather, it appears that vasodilatation results directly from IKCa channel activation and subsequent endothelial hyperpolarization.
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As EDHF-mediated dilations have been shown to critically depend on elevations in endothelial [Ca2+]i, we also sought to determine whether the endothelial hyperpolarization was required for the production of sufficient increases in endothelial [Ca2+]i to elicit EDHF-mediated dilations with an EDHF-dependent agonist. Artery diameter and endothelial [Ca2+]i were measured simultaneously after the addition of luminal UTP (107 to 105 M). Figure 8 shows responses for control, high luminal K+, and ChTx/Apa. The addition of either luminal K+ (nonselective neutralization of all endothelial K+ channels) or ChTx/Apa (inhibition of all KCa) resulted in complete elimination of EDHF-mediated dilations (Fig. 8A). However, peak endothelial Ca2+ responses were not at all attenuated by the inhibition of either KCa channels or all K+ channels (Fig. 8B). Furthermore, plateau [Ca2+]i (measured at 200 s from onset of Ca2+ increase) was not attenuated after K+ channel inhibition in either group (see Table 2). Thus in this intact artery preparation, neither peak [Ca2+]i nor plateau [Ca2+i] responses were sensitive to K channel activation. In fact, endothelial [Ca2+]i responses in the high K+ and ChTx/Apa groups easily exceeded the [Ca2+]i threshold (
340 nM) normally needed to elicit EDHF-mediated dilations (40). These data demonstrate that endothelial hyperpolarization does not significantly affect increases in endothelial [Ca2+]i in intact cerebral arteries. In addition, these data demonstrate that inhibition of EDHF-mediated dilations by K channel blockers is not due to a diminished capacity of the artery to elevate endothelial [Ca2+]i.
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| DISCUSSION |
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The first step in demonstrating that endothelial IKCa channel activation results in endothelial hyperpolarization and vasodilatation was to develop a method for measuring endothelial membrane potential in pressurized arteries. The gold standard for measuring cell membrane potential has traditionally been by microelectrode impalement. However, measurement of endothelial membrane potential in the pressurized MCA preparation is exceedingly difficult, as it would entail passing a microelectrode through two to three layers of smooth muscle and into a very thin endothelial cell. To our knowledge, measurement of endothelial membrane potential by microelectrode in a pressurized artery has only been reported by a single laboratory (24, 53). We therefore sought to apply a recently developed technique that utilizes a ratiometric voltage-sensitive fluorescent dye, di-8-ANEPPS, to measure changes in membrane potential. Di-8-ANEPPS has been used successfully for that purpose in a variety of tissues, including the endothelium from intact pressurized peripheral blood vessels (1, 2, 10, 11, 41). In the present study, we demonstrated that luminally applied di-8-ANEPPS could be confined to the endothelium and used to indicate changes in endothelial Vm in a pressurized cerebral artery preparation. We also performed an in vitro calibration of the dye and determined a relationship of 12.9 mV/1% ratio change. This relationship compares well with what others have reported from peripheral vessels (1012 mV/1% ratio change) and thus appears to be a reasonable approximation of actual membrane potential change (2, 11).
Luminal application of UTP produced significant hyperpolarization of the endothelium (
= 43 mV) as well as maximal EDHF-dependent dilations. Furthermore, the endothelial hyperpolarization to UTP was virtually abolished after the administration of ChTx. These data demonstrated that EDHF-mediated dilations to UTP involve significant endothelial hyperpolarization and that ChTx-sensitive channels were the primary effectors of that hyperpolarization (Fig. 2). The extent to which UTP hyperpolarized the endothelium falls within the upper range of agonist-mediated endothelial hyperpolarization (
= 20 to 45 mV) reported from nonpressurized peripheral tissues (3, 8, 12, 20, 21, 30, 32, 38). To our knowledge, only one previous study (53) has reported endothelial membrane potential in an EDHF-mediated response from a pressurized vessel. In that study, Welsh and Segal (53) demonstrated endothelial hyperpolarizations to ACh (
1532 mV) within hamster cheek pouch arterioles. Interestingly, the resting endothelial membrane potential that they report (30 mV) is notably depolarized from that of nonpressurized artery endothelium (42 to 65 mV) (14, 21, 22, 26, 38). Thus a more depolarized resting endothelial membrane potential in the pressurized artery would permit a greater possible hyperpolarization and might contribute to the reason that our hyperpolarization values fall at the upper end of the nonpressurized range.
Luminal 1-EBIO was used to determine the effect of activating endothelial IKCa channels directly. Activation of endothelial IKCa channels with 1-EBIO resulted in vasodilatation and endothelial hyperpolarization (
= 26 mV). Furthermore, both vasodilatation and hyperpolarization were significantly attenuated after the application of ChTx. It should be noted that, whereas 1-EBIO has been shown to be a good activator of IKCa channels and to possess good selectivity of IKCa channels over BKCa channels (15, 21, 31, 51), it may have additional effects that should be keep in mind. For instance, 1-EBIO has been shown to activate certain SKCa channels (43) as well as to promote relaxation of the smooth muscle through a mechanism not involving hyperpolarization (51). In our studies, 1-EBIO produced concentration-dependent dilations when delivered luminally (to the endothelium). When delivered abluminally (to the smooth muscle), however, the dilations were significantly attenuated. The significantly greater potency of 1-EBIO when delivered luminally versus abluminally suggests that the primary site of action is on the endothelium. The vasodilatation to luminal 1-EBIO was unaffected by the presence of a selective BKCa channel blocker, IbTx, demonstrating that BKCa channels are not involved in the 1-EBIO response (Fig. 5). However, vasodilatation was significantly attenuated when 1-EBIO was administered in the presence of either ChTx, CTZ, or high luminal K+ (Figs. 4 and 5). Our data indicate that SKCa channels do not play a significant role in the vasodilatation to 1-EBIO in this particular preparation, because the inhibition with ChTx or CTZ was not significantly different from that with nonspecific K channel inhibition (high luminal K+). Together, these data indicate that luminal 1-EBIO acts primarily on endothelial IKCa channels in the pressurized MCA preparation. Furthermore, endothelial IKCa channels are capable of promoting significant endothelial hyperpolarization when directly activated.
Although arteries dilated subsequently to 1-EBIO-mediated endothelial hyperpolarization, it was not clear where endothelial hyperpolarization fit into the mechanism. Because endothelial membrane potential has been shown to modulate Ca2+ influx, a possible indirect mechanism for 1-EBIO-dependent dilations could be to promote endothelial Ca2+ influx secondary to endothelial hyperpolarization. Therefore, whereas 1-EBIO produced significant endothelium-dependent dilations by activating endothelial IKCa channels, it was still necessary to determine whether the dilation resulted directly from IKCa channel activation and endothelial hyperpolarization or whether the resulting endothelial hyperpolarization triggered another Ca2+-dependent mechanism by promoting endothelial Ca2+ influx. For instance, if 1-EBIO resulted in an increase in endothelial [Ca2+]i, then the vasodilatation to 1-EBIO (or IKCa channel activation) could ultimately result from subsequent production of a Ca2+-dependent relaxing factor(s). However, the addition of 1-EBIO did not alter endothelial [Ca2+]i from resting values despite the significant vasodilatory effect of 1-EBIO (Fig. 7). Taken as a whole, these data indicate that 1-EBIO-dependent vasodilatation of cerebral arteries is mediated primarily by direct activation of endothelial IKCa channels, without an involvement of elevated endothelial [Ca2+]i. Furthermore, these data demonstrate that direct stimulation of endothelial IKCa channels alone is indeed sufficient to produce EDHF-like dilations. These findings are consistent with a model in which endothelial IKCa channels act downstream of endothelial Ca2+ as the critical effector of EDHF-mediated dilations.
From previous studies, we know that endothelial Ca2+ does play a critical role in EDHF-mediated dilations. For instance, an endothelial [Ca2+]i threshold (340 nM) has been demonstrated for the initiation of EDHF-mediated dilations (40). Additionally, influx of extracellular Ca2+ has been shown to be essential to sustain EDHF-mediated dilations (9, 48). The specific function of endothelial [Ca2+]i in EDHF-mediated dilations is still unclear, because elevated endothelial [Ca2+]i could activate any number of enzymes or pathways, including a hypothetical EDHF synthase. However, in light of this and other recent studies, one clear role for endothelial [Ca2+]i in the EDHF mechanism could simply be as the physiological activator of endothelial IKCa channels. In support of this conclusion, the reported EDHF-initiating [Ca2+]i threshold falls right within the range of [Ca2+]i required to produce significant activation of IKCa channels (250500 nM Ca2+) (42).
Whereas the primary role for IKCa channel activation in the EDHF mechanism thus appears to be down-stream of calcium, a secondary role might be to augment agonist-mediated endothelial [Ca2+]i responses. In cultured endothelial cells, Ca2+ influx has been shown to be dependent on membrane potential with hyperpolarization driving greater Ca2+ influx (32, 35, 46). Given the IKCa channel activation and endothelial hyperpolarization that results from EDHF-dependent agonists (Fig. 2), one would therefore presume that IKCa channel activation would augment agonist-mediated endothelial [Ca2+]i responses. Conversely, one would expect that interrupting that positive feedback system by inhibiting IKCa channels would result in reduced [Ca2+]i responses to EDHF-dependent agonists. Thus IKCa channel blockers might also be able to inhibit or modulate EDHF-mediated dilations by preventing endothelial [Ca2+]i from reaching the EDHF-initiating threshold. It must be noted, however, that such a scenario is reasonable only as long as one assumes that the relationship between membrane potential and Ca2+ flux applies beyond cultured endothelial cells. Although that assumption is often made in the literature, there are very few studies that provide data regarding the role of membrane potential on endothelial Ca2+ flux in intact arteries. The issue is further complicated given that endothelial Ca2+ responses from intact arteries are more complex to interpret given the likely contribution of smooth muscle to endothelial [Ca2+]i (17). In intact peripheral arteries, agonist-mediated Ca2+ flux has been shown to be reduced (27, 33) or unchanged (27, 50) in the presence of K channel blockers. Interestingly, the studies that reported reduced [Ca2+]i responses used high [K+]o to nonselectively block K channels (and presumably depolarize the endothelium and smooth muscle) (27, 33). In contrast, ChTx/Apa was without effect on endothelial [Ca2+]i, despite effectively blocking the agonist-mediated dilator response (27, 50). In the present study, neither ChTx/Apa nor high [K+]o reduced endothelial Ca2+ responses to UTP or prevented endothelial [Ca2+]i from attaining the [Ca2+]i threshold necessary for initiating EDHF-mediated dilations despite substantially reducing endothelial hyperpolarization (Figs. 2 and 8 and Table 2). It is not clear why these studies appear to conflict regarding the role of membrane potential in modulating endothelial [Ca2+]i. One possible explanation is that the relative role of membrane potential is dependent on the contribution of other modulating factors such as intracellular Ca2+ stores or Ca2+ flux from coupled smooth muscle cells (17). However, irrespective of the reason, our data demonstrate that endothelial hyperpolarization does not significantly affect endothelial [Ca2+]i in response to UTP in intact cerebral arteries. Furthermore, these data reinforce the conclusion that the critical role of endothelial IKCa channel activation is entirely down-stream of endothelial [Ca2+]i in the EDHF-dependent mechanism.
Taken as a whole, these data demonstrate that EDHF-mediated dilations in the cerebral circulation require activation of endothelial IKCa channels. In addition, direct activation of endothelial IKCa channels (1-EBIO) produces endothelial hyperpolarization and vasodilatation that mimic the EDHF-mediated response. Because the vasodilatory effect of direct IKCa channel activation does not involve an increase in endothelial [Ca2+]i, it appears that the critical role for endothelial IKCa channels is downstream of endothelial [Ca2+]i in the EDHF mechanism. Thus the present data support a model in which increased endothelial [Ca2+]i acts as the physiological activator of endothelial IKCa channels with IKCa channel activation and endothelial hyperpolarization being critical events in promoting the subsequent smooth muscle hyperpolarization. Further studies are required to determine the specific mechanism by which endothelial IKCa channel activation ultimately effects smooth muscle hyperpolarization and vasodilatation in cerebral arteries.
| DISCLOSURES |
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| FOOTNOTES |
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The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
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S. P. Marrelli, R. G. O'Neil, R. C. Brown, and R. M. Bryan Jr. PLA2 and TRPV4 channels regulate endothelial calcium in cerebral arteries Am J Physiol Heart Circ Physiol, March 1, 2007; 292(3): H1390 - H1397. [Abstract] [Full Text] [PDF] |
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E. M. Sokoya, A. R. Burns, C. T. Setiawan, H. A. Coleman, H. C. Parkington, and M. Tare Evidence for the involvement of myoendothelial gap junctions in EDHF-mediated relaxation in the rat middle cerebral artery Am J Physiol Heart Circ Physiol, July 1, 2006; 291(1): H385 - H393. [Abstract] [Full Text] [PDF] |
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J. Ledoux, M. E. Werner, J. E. Brayden, and M. T. Nelson Calcium-Activated Potassium Channels and the Regulation of Vascular Tone Physiology, February 1, 2006; 21(1): 69 - 78. [Abstract] [Full Text] [PDF] |
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J. Andresen, N. I. Shafi, and R. M. Bryan Jr. Endothelial influences on cerebrovascular tone J Appl Physiol, January 1, 2006; 100(1): 318 - 327. [Abstract] [Full Text] [PDF] |
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J. You, E. M. Golding, and R. M. Bryan Jr. Arachidonic acid metabolites, hydrogen peroxide, and EDHF in cerebral arteries Am J Physiol Heart Circ Physiol, September 1, 2005; 289(3): H1077 - H1083. [Abstract] [Full Text] [PDF] |
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L. J. Alvarez, A. C. Zamudio, and O. A. Candia Cl- secretory effects of EBIO in the rabbit conjunctival epithelium Am J Physiol Cell Physiol, July 1, 2005; 289(1): C138 - C147. [Abstract] [Full Text] [PDF] |
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F. M. Faraci, C. Lynch, and K. G. Lamping Responses of cerebral arterioles to ADP: eNOS-dependent and eNOS-independent mechanisms Am J Physiol Heart Circ Physiol, December 1, 2004; 287(6): H2871 - H2876. [Abstract] [Full Text] [PDF] |
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E. van Bavel Shear stress and intermediate-conductance calcium-activated potassium channels Cardiovasc Res, December 1, 2003; 60(3): 457 - 459. [Full Text] [PDF] |
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