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NeuroSearch A/S, Ballerup, Denmark (R.S.H., T.G.D., S.-P.O., M.G.); Danish National Research Foundation Centre for Cardiac Arrhythmia, University of Copenhagen, Copenhagen, Denmark (R.S.H., T.G.D., S.-P.O., M.G.); and Department of Pharmacology and Toxicology, Medical Faculty, Dresden University of Technology, Dresden, Germany (T.C., E.W., U.R.)
Received May 16, 2006; accepted July 5, 2006
| Abstract |
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| Materials and Methods |
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cRNA preparation and capping were performed by in vitro transcription using the mCAP mRNA capping kit (Stratagene, La Jolla, CA) or Ambion T7 mMessage mMachine kit (Ambion, Austin, TX) according to the manufacturer's instructions. mRNA was phenol/chloroform-extracted, ethanol-precipitated, and dissolved in Tris-EDTA buffer to approximate concentrations of 1 µg/µl. For proof of purity and integrity, mRNA was inspected by gel electrophoresis, and concentrations were determined photometrically. mRNA was stored at -80°C until injection.
Expression in X. laevis Oocytes. X. laevis surgery and oocyte treatment were done as described previously (Grunnet et al., 2001
). Oocytes were collected under anesthesia (Tricain 2 g/l, Sigma A-5040; Sigma-Aldrich, St. Louis, MO) using guidelines approved by the Danish National Committee for Animal Studies. Before injection of 50 nl of mRNA (approximately 50 ng), oocytes were kept for 24 h at 19°C in Kulori medium consisting of 90 mM NaCl, 1 mM KCl, 1 mM MgCl2, 1 mM CaCl2, and 5 mM HEPES, pH 7.4. Injection of mRNA was accomplished using a Nanoject microinjector from Drummond (Drummond Scientific, Broomall, PA). Oocytes were kept at 19°C for 2 to 5 days before measurements were performed.
Expression and Recording in Mammalian Cells. Heterologous expression of HERG1 in mammalian HEK 293 cells and wholecell patch-clamp recordings were performed as described previously (Hansen et al., 2006
).
Isolation of Native Cardiomyocytes. Cells were isolated and incubated as described previously (Hansen et al., 2006
).
Native Cardiomyocytes for Recordings of Ca2+ and Na+ Current. Currents were measured with the single electrode voltageclamp method as described in detail elsewhere (Christ et al., 2005
). The pipette solution had the following composition: 90 mM cesium methanesulfonate, 20 mM CsCl, 10 mM HEPES, 4 mM Mg-ATP, 0.4 mM Tris-GTP, 10 mM EGTA, and 3 mM CaCl2, with a calculated free Ca2+ concentration of
60 nM (computer program EQCAL; Bio soft, Cambridge, UK; pH 7.2). Ca2+ currents were measured with the following Na+-free superfusion solution: 120 mM tetraethylammonium chloride, 10 mM CsCl, 10 mM HEPES, 2 mM CaCl2, 1 mM MgCl2, and 20 mM glucose, pH 7.4 (adjusted with CsOH). ICa,L was measured from a holding potential of -80 mV with test steps (200 ms) between -70 and +65 mV in 5-mV increments at 37°C. For measuring INa, NaCl (5 mM) was added to the superfusion solution, and CaCl2 was reduced to 0.5 mM. Contaminating ICa,L was blocked by nisoldipine (1 µM). INa was measured at room temperature from a holding potential of -100 mV, with test steps (100 ms) between -80 and +5 mV in 5-mV increments. ICa,L and INa amplitudes were determined as the difference between peak inward current and current at the end of the depolarizing test step. A system for rapid solution changes allowed application of drugs in the close vicinity of the cells (Cell Micro Controls, Virginia Beach, VA; ALA Scientific Instruments, Long Island, NY).
Papillary Muscle Preparation. Animal handling was performed in accordance with the Helsinki convention. Male Dunkin Hartley Crl: (HA) guinea pigs (Charles River, Sulzfeld, Germany) of 280 to 350 g were sacrificed under light CO anesthesia. Hearts were excised, and thin papillary muscles were removed from the right ventricles. The muscles were mounted in an organ bath continuously perfused with carbogenated Tyrode's solution: 126.7 mM NaCl, 5.4 mM KCl, 1.8 mM CaCl2, 1.05 mM MgCl2, 22 mM NaHCO3, 0.42 mM NaPO4, and 5 mM glucose, pH 7.4, at 37°C. One end of the muscle was pinned to the floor of the chamber, and the free end was connected to a force transducer (AE 801; SensoNor, Dasing, Germany) with silk thread. The muscle was stimulated via Ag/AgCl electrodes at a regular frequency of 1 Hz. After at least 90 min of equilibration, intracellular action potentials were recorded with conventional glass pipettes filled with 2 M KCl (tip resistance 10-20 M
). Drugs were added to the superfusion solution. Action potentials from stable impalements were recorded 30 to 45 min after drug addition before the drug concentration was increased. Action potentials were recorded, and the following parameters were analyzed offline: resting membrane potential, action potential amplitude, APD at 20, 50, and 90% of repolarization (APD20, APD50, and APD90), and maximum upstroke velocity (dV/dtmax). All the data acquisition and analysis were carried out with the ISO 2 system (MFK, Niedernhausen, Germany).
Analysis of Data. Data analysis and drawings were performed using IGOR software (WaveMetrics, Lake Oswego, OR) or GraphPad Prism software (GraphPad Software, San Diego, CA). All the deviations of calculated mean averages are given as S.E.M. values. EC50 values were calculated from equilibrium concentration-response experiments. Data were fitted with a sigmoidal dose-response equation: Y = Bottom + (Top-Bottom)/{1 + 10[(LogEC50-X) · HillSlope]}, where X is the logarithm of concentration, and Y is the response. Similar activation and inactivation data were fitted with Boltzmann equations. The applied equations were for activation data: I = Imax/{1 + exp[(V50 - Vt)/k]} and for inactivation data: I = Imax/{1 + exp[(Vt - V50)/k]}, where I is the current, V50 is the voltage required for half-activation, Vt is the test membrane potential, and k is the slope factor. To avoid transient capacitance, current values for release from inactivation (Fig. 5) were calculated as the average current amplitude recorded from 10 to 20 ms after the second depolarization step to +20 mV. Time constants for deactivation were calculated by fitting with the double exponential equation Itail = K0 + Kfast · exp[-(t/
fast)] + Kslow · exp [-(t/
slow)], where t is the time in seconds, and the fast and slow deactivation constants are given by
fast and
slow, respectively. Finally, the time constant for inactivation was calculated by fitting to the single exponential equation Itail = K0 + K · exp[-(t/
)], where t is the time in seconds, and
is the time constant for inactivation. Capacitative current was subtracted before fitting.
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| Results |
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The following experiments were designed to obtain detailed information about the effect of NS3623 on cloned HERG1 channels expressed in X. laevis oocytes. Figure 2 shows the effect of NS3623 on HERG1-expressing oocytes challenged with the outlined step protocol, where the HERG1 channels were activated by 1-s voltage increments ranging from -80 to +40 mV. These changes in membrane potential evoke a slow voltage-dependent activation of the HERG1 channel followed by strong inactivation, a feature that is reflected in a bell-shaped current-voltage (I-V) relationship (Fig. 2, A and C). The potentials were increased with 10-mV steps, and the tail current was elicited by clamping at -60 mV for 4 s. Summarized I-V relationship for tail currents are shown in Fig. 2D. When a stable control current was obtained, 30 µM NS3623 was added to the bath. In the presence of the compound, both the steady-state and the tail HERG1 currents were increased to a level significantly different from initial control measurements (Fig. 2, B-D). The Boltzmann fits to the activation currents resulted in almost identical V50, where half-maximal activation was -20.0 ± 2mVin control experiments and -20.0 ± 3 mV in the presence of NS3623. These experiments were repeated with similar results after coexpression of HERG1 and the β-subunit KCNE2 (data not shown). Finally, data were reproduced with HERG1 channels heterologously expressed in mammalian HEK 293 cells (data not shown). To determine the concentration response of NS3623 on heterologously expressed HERG1 channels, oocytes were repeatedly activated by clamping 1 s at +20 mV followed by3sat -60 mV. Between steps, cells were kept at -80 mV for 3 s. Oocytes were exposed to a series of seven concentrations of NS3623 ranging from 300 nM to 300 µM. Between application of drugs, the oocytes were washed with Kulori solution until a baseline comparable with the initial control values was obtained. The concentration-response relationship with normalized current as a function of drug concentration is depicted in Fig. 3. These currents were sigmoidally fit, and the increase in HERG1 channel activity as a function of concentration was found to have an EC50 value of 79.4 ± 14.9 µM.
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To further investigate how NS3623 could affect the inactivation properties of HERG1 channels, a protocol designed to examine the time course of the inactivation was applied. This protocol was initially described by Smith et al. (1996
) and Spector et al. (1996
) and is outlined in Fig. 6. Channels were first activated and then inactivated by a 1-s pulse to +40 mV. Thereafter, the channels were subjected to a 10-ms pulse at -120 mV to allow full recovery from inactivation. The 10-ms time span at -120 mV is at the same time sufficiently short to prevent the channels from initiating deactivation. The third part of this pulse was a stepwise increment in the potential from -40 to +50 mV lasting for 1 s, to elicit a re-onset of channel inactivation. The currents representing this re-onset of inactivation were then fitted with a monoexponential function. When comparing the resulting time constants from NS3623-treated oocytes with control experiments, it was revealed that time constants were significantly and immensely increased at all the measured potentials in the presence of 30 µM NS3623 (Fig. 6).
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The selectivity of NS3623 for HERG1 over other important cardiac potassium ion channels was examined, and representative traces are presented in Fig. 11. Measurements were performed from oocytes expressing either KCNQ1 (Fig. 11A), Kv1.5 (Fig. 11B), or Kv4.3 channels (Fig. 11C). KCNQ1 participates in cardiac IKs current, Kv1.5 in IKur current, and Kv4.3 in Ito current. The protocols outlined in the figure legend were used to elicit the respective currents. KCNQ1, Kv1.5, and Kv4.3 channels were unaffected by the presence of 30 µM NS3623. We then further examined the effect of NS3623 on native calcium and sodium currents measured from isolated guinea pig cardiomyocytes. The results obtained for 10 µM of the compound are shown in Fig. 12, A and B (calcium current) and C and D (sodium current). Effect of NS3623 on inward currents ICa in guinea pig ventricular myocytes showed a substantial and variable run-down over time. Five minutes after establishing access, the cells were exposed to 10 µM NS3623. ICa,L density was 20.1 ± 3.4 pA/pF before and 19.1 ± 3.7 pA/pF after drug exposure (n = 7). This decline was not different compared with spontaneous rundown in time-matched controls (data not shown). NS3623 also did not affect ICa,T (Fig. 12A). However, a small block of 20% of the L-type calcium currents was observed in the presence of 30 µM of the compound, whereas 100 µM inhibited the current by 40%. INa was stable over time, and INa density 2 min after exposure to NS3623 was not different from the control values (46.5 ± 7.3 versus 46.8 ± 7.5 pA/pF, n = 5). The small Na+ current was unaffected by 30 and 100 µM NS3623 (data not shown). We then examined the effect of activating HERG1 channels by NS3623 in isolated papillary muscle (Fig. 13). Under control conditions, APD20, APD50, and APD90 were 80 ± 3, 133 ± 4, and 154 ± 5 ms, respectively (n = 5), and remained stable in time-matched control experiments. Exposure to 10 µM NS3623 decreased APD20, APD50, and APD90 to 67 ± 3, 112 ± 6, and 131 ± 8 ms, respectively (p < 0.05). Moreover, NS3623 (10 µM) reduced force of contraction when compared with the time-matched control (from 122 ± 45 to 53 ± 23 µN in NS3623 versus from 118 ± 12 to 78 ± 10 µN in TMC, n = 5 each group). Resting membrane potential, dV/dtmax, and action potential amplitude were not affected by NS3623. Control values were -87 ± 0.5 mV, 238 ± 13 V/s, and 125 ± 1 mV, respectively (n = 5).
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| Discussion |
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Until very recently, no activators of the HERG1 channel have been known, and understanding how compounds can increase the current through this important cardiac channel is crucial because it can be speculated that such a drug is beneficial in the treatment of certain kinds of arrhythmias. An overall increase of HERG1 channel current may stem from an increase in channel protein insertion in the cell membrane, and/or an increase in the open probability of the channel, and/or a change in single-channel conductance. In the present experiments, the increase of current was immediate as the drug was added to the perfusion solution, which makes it highly unlikely that NS3623 induces a higher expression of HERG1 channel in the oocyte. NS3623 was found to predominantly increase HERG1 current by affecting channel inactivation. When investigating the voltage-dependent release from inactivation, we observed a rightward shift of 17.7 mV of the half-inactivation voltage; i.e., channels will more easily be released from inactivation at any given membrane potential during repolarization and at the resting membrane potential in the cardiac diastole. Therefore, it follows that in the presence of NS3623 more channels are expected to be available at physiological relevant potentials compared with controls (Fig. 5C). We also found that the onset of inactivation was dramatically slowed at all the measured potentials (Fig. 6B). The profound influence of NS3623 on the inactivation kinetics of the HERG1 channel may fully account for the observed increase in current. Because inactivation holds channels in a nonconducting conformation, rightward shifting the voltage at which half of the channels are inactive makes more channels available at most physiologically relevant membrane potentials. Therefore, it can be hypothesized that during the action potential, exposure of the cardiomyocyte to NS3623 will increase the repolarizing reserve.
We also investigated the effect of NS3623 on channel activation, and although there was an overall increase in the steady-state and tail current in the drug-treated oocytes, we found no significant difference in the voltage dependence of activation (Fig. 2). When deactivation time course was investigated, we did not find any significant changes in the presence of NS3623 compared with control (Fig. 4). However, NS3623 induced a shift in the voltage that induced the largest tail current (4, C and D). Under control conditions, the largest current was induced at -50 mV, whereas application of NS3623 resulted in a 10-mV shift toward a more negative potential. Such a shift may be speculated to increase the repolarizing reserve and the diastolic HERG1 current of cardiac myocytes exposed to drugs like NS3623 because the larger tail current will appear later in the repolarizing phase of the action potential.
In mutant channels where the inactivation ability was compromised (HERG1 S620T and HERG1 S631A) or where the blocking site was eliminated (HERG1 F656M), the mechanism of action of NS3623 was further revealed. When the compound was examined by application to the noninactivating HERG1 mutant S620T, no significant increase in current was observed (Fig. 7C). Neither did NS3623 significantly increase currents measured from the S631A mutated channel (Fig. 7C), a channel that has been reported to possess a slight inactivation (Zou et al., 1998
). This is consistent with the finding that NS3623 most dominantly affects the rapid C-type inactivation that occurs during normal HERG1 channel activation. Addition of NS3623 to channels mutated in one of two amino acids necessary for high-affinity HERG1 channel inhibition (F565M) resulted in a
5-fold increase of the steady-state current at 0 mV and a
5-fold increase in the tail current likewise measured at 0 mV (Fig. 8). When these data are compared with results obtained after NS3623 application to wild-type HERG1 channels (Fig. 2), it is obvious that NS3623 is a far more potent HERG1 channel activator when part of the high-affinity HERG1 channel inhibitor site is mutated. Therefore, it can be concluded that NS3623 must have a dual mode of action with a combined inhibitory and activating function. It should be emphasized that the overall mode of action of NS3623 is to increase wild-type HERG1 current, showing that the activating function of NS3623 is superior to the inhibitory activity of the compound. Finally, it was shown that NS3623 can bind to and activate closed HERG1 channels. This indicates that the binding site for NS3623 may be at the extracellular part of the channel.
Recently, attention has been drawn to the short QT syndrome, where an apparent gain-of function mutation of the HERG1 channels gives rise to lethal cardiac arrhythmias. Gussak et al. (2000
) first described that short QT intervals on the electrocardiogram increase the risk of sudden cardiac death to the same extent as the long QT, and it can be speculated whether drugs that increase the HERG1 current and thereby decrease the APD will be proarrhythmic. It has been shown that the short LQT1 syndrome is caused by a gain-of-function mutation in the HERG1 channel by an N588K (asparagine to lysine) mutation that is located in the S5-pore linker region and gives rise to a HERG1 current with a large steady-state current but a very small tail current (Zou et al., 1998
; Brugada et al., 2004
; Cordeiro et al., 2005
; McPate et al., 2005
). The small tail current will result in less repolarization reserve in the myocardium. Therefore, it can be argued that even though HERG1 N588K is reported as a gain-of-function in the steady-state current, it can equally well be revealed as a loss of function when it comes to participation in cardiac action potential repolarization. Moreover, this mutation affects the recovery of inactivation, extensively resulting in an almost 100-mV rightward shift in the voltage-dependence HERG1 channel availability. We observed a rightward shift of 17 mV, which means that NS3623 induces a shift in the potential where half of the channels will be inactivated toward more depolarized potentials, resulting in a larger steady-state current. However, HERG1 channels exposed to NS3623 will still be expected to inactivate during the plateau phase of the action potential, considering the moderate shift in the estimated half-point of mid-inactivation. Furthermore, McPate et al. (2005
) and Cordeiro et al. (2005
) reported that the N588K mutation resulted in a HERG1 current that monotonously followed the action potential wave form when such a protocol was applied, which is in contrast to the wild-type HERG1 current where the steady state reaches a peak current during the plateau phase. When we applied an action potential wave form to elicit HERG1 current, we observed that the shape of the current did not change when the oocytes were exposed to NS3623, although the current did increase in magnitude as seen on Fig. 10. Therefore, it is highly likely that HERG1 channel activation by NS3623 is incomparable with the HERG1 N588K gain-of-function mutation.
In the isolated papillary muscle from guinea pigs, we observed a shortening of the action potential (Fig. 13). In the presence of 10 µM NS3623, APD90, APD50, and APD20 decreased to the same extent, indicating a uniform abbreviation of repolarization. In the studies of selectivity for NS3623 for HERG1 channels over other relevant cardiac channels, we did not observe any significant changes in the native sodium and calcium currents (Fig. 12), a finding that is consistent with the maintenance of "normal" action potential appearance. Neither did NS3623 significantly affect KCNQ1, Kv1.5, or Kv4.3, indicating that the abbreviation of the APD is mainly through activation of the HERG1 channel.
We conclude that NS3623 can be seen as a selective HERG1 channel opener when applied in cardiac tissue. Furthermore, NS3623 activation of HERG1 channels is fundamentally different from currents recorded from gain-of-function HERG1 N588K mutations. Having the good solubility profile of NS3623 in mind, we therefore believe that a proper tool compound has been obtained to address questions regarding HERG1 opening in intact tissue and after in vivo applications. These approaches will be addressed in future studies.
| Acknowledgements |
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| Footnotes |
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ABBREVIATIONS: HERG, human ether-a-go-go-related gene; APD, action potential duration; NS1643, 1,3-bis-(2-hydroxy-5-trifluoromethylphenyl)-urea; NS3623, N-(4-bromo-2-(1H-tetrazol-5-yl)-phenyl)-N'-(3'-trifluoromethylphenyl)urea; HEK, human embryonic kidney.
Address correspondence to: Morten Grunnet, NeuroSearch A/S, Pederstrupvej 93, DK-2750 Ballerup, Denmark. E-mail: mgr{at}neurosearch.dk
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