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J Physiol Volume 556, Number 2, 401-413, April 15, 2004 DOI: 10.1113/jphysiol.2003.059303
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Single-channel recordings of a rapid delayed rectifier current in adult mouse ventricular myocytes: basic properties and effects of divalent cations

Gong Xin Liu1, Jun Zhou1, Stanley Nattel2 and Gideon Koren1

1 Bioelectricity Laboratory, Cardiovascular Division, Brigham and Women's Hospital, Harvard Medical School, Boston, MA 02115, USA2 Department of Medicine and Research Center, Montreal Heart Institute and University of Montreal, 5000 Belanger Street, Montreal, Quebec H1T 1C8, Canada


    Abstract
 Top
 Abstract
 Introduction
 Methods
 Results
 Discussion
 References
 
The rapidly delayed rectifier current (IKr) has been described in ventricular myocytes isolated from many species, as well as from neonatal mice. However, whether IKr is present in the adult mouse heart remains controversial. We used cell-attached patch-clamp recording in symmetrical K+ solutions to assess the presence and behaviour of single IKr channels in adult mouse cardiomyocytes (mIKr). Of 314 patches, 158 (50.1%) demonstrated mIKr currents as compared with 131 (42.3%) for the IK1 channel. Single mIKr channel activity was rarely observed at potentials positive to –10 mV. The slope conductance at negative potentials was 12 pS. Upon repolarization, ensemble-averaged mIKr showed slow deactivation with a biexponential time course. A selective IKr blocker, E-4031 (1 µM), completely blocked mIKr channel activity. Extracellular Ca2+ and Mg2+ at physiological concentrations shifted the activation by ~30 mV, accelerated deactivation kinetics, prolonged long-closed time, and reduced open probability without affecting single-channel conductance, suggesting a direct channel-blocking effect in addition to well-recognized voltage shifts. HERG subunits expressed in Chinese hamster ovary cells produced channels with properties similar to those of mIKr, except for the more-negative activation of the HERG channels. Despite the abundant expression of mIKr, single-channel events were rarely observed during action-potential clamp and 5 µM E-4031 had no detectable effect on the action potential parameters, confirming that mIKr plays at best a minor role in repolarization of adult mouse cardiomyocytes, probably because the modulatory effects of divalent cations prevent significant mIKr opening under physiological conditions.

(Received 10 December 2003; accepted after revision 6 January 2004; first published online 23 January 2004)
Corresponding author G. Koren: Bioelectricity Laboratory, Cardiovascular Division, Brigham and Women's Hospital, 75 Francis St, Boston, MA 02115, USA. Email: gkoren{at}rics.bwh.harvard.edu


    Introduction
 Top
 Abstract
 Introduction
 Methods
 Results
 Discussion
 References
 
Voltage-gated outward K+ currents control the shape and duration of the action potential (AP) in cardiac myocytes (Tristan-Firouzi et al. 2001). Classically, time-dependent K+-channels are divided into two types: a transient outward current (Ito) that underlies the first phase (phase 1) of AP repolarization; and ultrarapid, rapid, and slow delayed rectifier currents (IKur, IKr, and IKs) that determine the middle and late phases of repolarization (Nerbonne, 2000). Expression of the rapidly activating delayed rectifier current (IKr) in the hearts of humans (Wang et al. 1993; Li et al. 1996; Veldkamp et al. 1995), dogs (Liu & Antzelevitch, 1995; Gintant, 1996), rabbits (Shibasaki, 1987; Veldkamp et al. 1993; Clay et al. 1995; Mitcheson & Hancox, 1999), and guinea-pigs (Sanguinetti & Jurkiewicz, 1990,1991; Horie et al. 1990) has been well documented. Recent molecular biological and electrophysiological studies have shown that the pore-forming {alpha} subunit of the IKr channel is encoded by the human ether-á-go-go-related gene (HERG) (Sanguinetti et al. 1995), which may coassemble with an accessory protein, MiRP1, to form the native IKr channel (Abott et al. 1999). Because of its critical functional role in determining the duration of the action potential and its promiscuous propensity to drug blockade, IKr has become a focal point of research interest. Various mutations in HERG have been linked to abnormal repolarization and long-QT syndromes (LQTs) in humans (Curran et al. 1995). A number of non-cardiac drugs are reported to cause QT prolongation through IKr inhibition (Vandenberg et al. 2001) and are associated with an increased risk of a potentially fatal cardiac arrhythmia known as torsades de pointes, which has resulted in withdrawal from the market of drugs such as grepafloxacin, terfenadine, astemizole and cisapride.

In the adult mouse heart, the major delayed rectifier potassium currents involved in repolarization appear to be of different molecular identities. In addition to the prominent transient outward current, a Kv1.5-like current, IK,slow1, and a Kv2.1-like current, IK,slow2, are reported to play important roles (Zhou et al. 1998, 2003; Xu et al. 1999). Of the IKr blockers, E-4031 and dofetilide (Zhou et al. 1998; Wang et al. 1996) are reported to have minimal effects on AP durations of adult mouse ventricular myocytes, and the expression of a dominant negative transgene directed against HERG does not produce prolongation in the QT interval in adult mice (Nerbonne et al. 2001; Babij et al. 1998). Since there is evidence for a key role of IKr in repolarizing the embryonic and neonatal mouse heart (Wang et al. 1996), it has been thought that IKr is minimal or absent in adult mouse cardiomyocytes. Here we report that single IKr channels are abundantly expressed in adult mouse ventricular myocytes. The single-channel properties are characterized and compared with those of channels encoded by HERG in a mammalian cell line. Single-channel analyses reveal that divalent cations modify the voltage dependence of activation as well as the open probability and the rate of deactivation of the channel such that channel openings are minimal under physiological conditions in the mouse heart.


    Methods
 Top
 Abstract
 Introduction
 Methods
 Results
 Discussion
 References
 
Preparation of mouse ventricular myocytes and Chinese hamster ovary (CHO) cells

Ventricular myocytes were isolated from the hearts of adult FVB mice (12–16 weeks, 25–35 g) by standard enzymatic techniques. After the mouse was anaesthetized with enflurane, its heart was removed and perfused for 4–5 min with a nominally calcium-free solution containing (mM): 130 NaCl, 5 KCl, 1.5 MgCl2, 0.33 NaH2PO4, 8 taurine, 5 Hepes, 5 pyruvic acid and 5 glucose. The flow rate was maintained at 2–3 ml min–1 with a peristaltic pump. Subsequently, the heart was perfused for 3–4 min with the same solution to which 0.05% collagenase (Type 1, Sigma), 20–40 µM CaCl2 and 0.1% BSA had been added. The heart was then minced, and cells were dispersed with a glass pipette for 3–5 min in a solution containing (mM): 45 KCl, 70 potassium glutamate, 3 MgSO4, 15 KH2PO4, 16 taurine, 10 Hepes, 0.5 EGTA and 10 glucose (pH 7.38). The cell suspension was filtered through a 100-µm nylon mesh, kept at room temperature for 1 h before transfer to Eagle's minimum essential medium containing 1 mM Ca2+, and used within 6–8 h.

Chinese hamster ovary (CHO-K1) cells stably transfected with HERG channel were cultured in a 35-mm dish with F-12 nutrient mixture (Gibco BRL, no. 1765-047). Recordings were made 48 h after passage.

Electrophysiological recording and data analysis

Whole-cell and single-channel recordings were obtained with an Axopatch-200B amplifier (Axon Instruments, Union City, CA, USA) with standard patch-clamp techniques. Currents were recorded at room temperature (21–23°C). Capacitance and 60–80% of series resistance were routinely compensated. The sampling frequency was 2.5 or 5 kHz; the –3 dB cut-off frequency was 1 kHz. Detailed recording protocols are specified in the text.

For whole-cell recording, pipette resistances were 2–4 M{Omega} when filled with (mM): 130 KCl, 5 Mg2-ATP, 5 EGTA, 10 Hepes and 0.5 Tris-GTP; pH was adjusted to 7.2 with KOH. For cell-attached single-channel recording, the pipette resistance was in the range of 8–10 M{Omega} for pipettes filled with a solution containing (mM): 150 KCl, 1 CaCl2, 1 MgCl2 and 5 Hepes, pH 7.4. In some experiments, divalent cation salts (Ca2+ and Mg2+) were excluded and 10 mM EGTA was added (‘divalent-free solution’). Tyrode solution was used as a standard bath solution and contained (mM): 140 NaCl, 5.4 KCl, 0.33 NaH2PO4, 1 MgCl2, 1 CaCl2, 5 Hepes and 7.5 glucose, pH 7.4. The bath solution for single-channel recording in cardiomyocytes contained (mM): 150 KCl, 10 EGTA, 5 Hepes, 2 K2-ATP and 10 glucose, pH 7.4; for recording in CHO cells, the solution contained 150 KCl, 5 Hepes, 2 MgCl2 and 1 glucose, pH 7.4.

Data were evaluated using pCLAMP8.3 (Axon Instruments) and Origin7.0 (OriginLab Corp.) software, and results are given as means ±S.E.M.


    Results
 Top
 Abstract
 Introduction
 Methods
 Results
 Discussion
 References
 
Characterization of single-channel mouse IKr and effect of extracellular divalent cations

To analyse the properties of native potassium channels in cardiac myocytes, we carried out cell-attached single-channel recordings in isolated mouse cardiomyocytes. As shown in Fig. 1, two types of potassium channels were typically seen in our recordings. The first channel showed a typical inward rectifier property (IK1), opened at negative but not positive potentials, and had a slope conductance of ~30 pS. The other type of channel was more readily elicited at negative potentials after a positive depolarization and showed a much smaller conductance. As illustrated later, this small channel demonstrated properties closely resembling those of IKr reported in rabbit (Shibasaki, 1987; Veldkamp et al. 1993), guinea-pig (Sanguinetti & Jurkiewicz, 1990) and human (Veldkamp et al. 1995) myocytes and the HERG channel in Xenopus oocytes (Zou et al. 1997). Therefore, we will refer to it as mouse IKr (mIKr). To our surprise, mIKr channels were observed very frequently, appearing in 158 (50.1%) of 314 patches as compared with Kir channels, which were seen in 131 (41.7%) of 314 patches.



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Figure 1.  Single-channel recordings of inward rectifier (IK1) and the rapidly activating delayed mIKr
Recordings of a single IK1 channel that opened at negative, but not positive, potentials, under symmetrical potassium conditions. Upon repolarization to –60 mV from potentials positive to –10 mV, small-amplitude channel openings were frequently seen to overlap IK1 channel activity. The recording protocol is shown on the top of the current traces. Holding potential is at –80 mV; the test potentials are from –110 mV to +70 mV for 2 s followed by –60 mV for 2 s. Dashed lines mark the closed level.

 
Figure 2 demonstrates a single mIKr channel recorded at a series of repolarizing potentials ranging from,. –20 mV to –10 mV following a 400 ms prepulse to +60 mV. Following repolarization, channel openings terminated more rapidly at more-negative potentials, in agreement with the accelerated deactivation kinetics at more-negative potentials found with macroscopic IKr/HERG current (Ho et al. 1996, 1998; Paquette et al. 1998; Johnson et al. 1999). Unlike many other voltage-gated K+ channels, IKr is considerably modulated by extracellular divalent cations such as Ca2+ and Mg2+ under physiological conditions (Ho et al. 1996, 1998; Paquette et al. 1998; Johnson et al. 1999). However, to our knowledge, there are no studies of the effect of divalent cations on IKr single-channel behaviour. Therefore, we evaluated the effect of the presence of divalent cations on the properties of single mIKr channels. Figure 2A and B illustrates typical recordings with (1 mM Ca2+ and 1 mM Mg2+, Fig. 2A) or without (Fig. 2B) divalent cations in the pipette solution. The presence of divalent cations in the extracellular solution significantly reduced channel activity at each voltage. However, the single-channel slope conductance was not affected by the presence of divalent cations (Fig. 2C) (12.16 ± 0.31 pS, n= 30 with divalent cations versus 12.38 ± 0.22 pS, n= 27 without). The time course of deactivation of the ensemble-averaged IKr current could be best fitted with a two-exponential function (Fig. 3): at –80 mV in the presence of divalent cations, {tau}fast and {tau}slow were 37.1 ± 3.5 ms (n= 5) and 326.1 ± 36.7 ms (n= 5), respectively. In the absence of divalent cations, the mean {tau}fast and {tau}slow were slower: 70.8 ± 8.7 ms (n= 3) and 969.3 ± 207.2 ms (n= 3), respectively. Of note, the ensemble-averaged currents in six patches could not be fitted because the currents persisted for several minutes.



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Figure 2.  Repolarization-induced single mIKr channel
A and B, recordings with and without divalent cations in the pipette solution. Voltage protocol shown in lower panel of A. Holding potential was at –80 mV; the test potentials from –20 to –110 mV were preceded by a 400-ms prepulse to +60 mV. A 200-ms pulse to –120 mV was applied after test pulses to terminate channel activity rapidly (see inset in Fig. 4). Single-channel current–voltage relationship of mouse IKr channel in the range of negative potentials was shown in the lower panel of B. With divalent cations (•, n= 30); without divalent cations ({circ}, n= 27).

 


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Figure 3.  Ensemble-averaged mIKr single channel current
Ensemble-averaged currents were acquired by averaging 50–100 sweeps recorded at –80 mV preceded by +60 mV. A, recording with divalent cations in the pipette solution. B, recording without divalent cations in the pipette. Slowed deactivation resulted in a sustained current at the end of 1 s in the absence of divalent cations. Ensemble-averaged current was best fitted by a two-exponential function.

 
IKr/HERG current activates at depolarized voltages, but the outward currents are increasingly reduced at potentials positive to ~0 mV due to fast voltage-dependent inactivation that results in a negative slope conductance at positive voltages (Sanguinetti & Jurkiewicz 1990, 1991; Trudeau et al. 1995; Smith et al. 1996; Spector et al. 1996). Figure 4 shows IKr channel activity following steps from a holding potential of –80 mV to a series of test potentials between –110 mV and +70 mV, followed by a step to –60 mV. In the presence of divalent cations, depolarization-induced channel openings were first observed at –30 mV (Fig. 4A), while in divalent-free solution they were evident even at –70 mV (Fig. 4B). These results indicate that the addition of divalent cations shifted the threshold of mIKr activation to a more positive potential. Upon stepping to –60 mV, channel activity was observed following all the prepulses between –110 and +70 mV in the absence of divalent cations but were evident only after potentials positive to –10 mV in the presence of divalent cations (Fig. 4A). The NPo of the ‘tail currents’ at –60 mV was voltage-dependent and was shifted to more-positive potentials in the presence of divalent cations in the pipette solution. The mean half-activation voltage (V1/2) was –14.8 mV in the presence of divalent cations, and the slope factor is 8.0 mV; in the absence of divalent cations the V1/2 and slope factor were –43.1 mV and 25.6 mV, respectively.



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Figure 4.  Depolarization-induced activation of mIKr
Currents were recorded using the voltage protocol shown in the lower part of A. Membrane was held at –80 mV. Test potentials ranging from –110 to +70 mV at an increment of 20 mV were followed by a repolarization to –60 mV to elicit the tail current. A 200 ms pulse of –120 mV was applied to terminate channel activity quickly before returning to the holding potential. A, recording with divalent cations in the pipette solution. B, recording without divalent cations in the pipette. NPo of tail current as a function of potential is shown in the lower part of B. NPo was measured in the first second of the tail current at –60 mV in A and B with divalent cations (•, n= 20) and without divalent cations ({circ}, n= 18). The data points were fitted with a Boltzmann function: NPo=NPmax/(1 + exp((V – V1/2)/k)), where NPmax represents the maximum NPo, V is the membrane potential, V1/2 is the membrane potential at half-maximal activation, and k is the slope factor. In the presence of divalent cations, the V1/2 and k are –14.86 ± 0.71 mV and 8.03 ± 0.62 mV, respectively; and are –43.15 ± 1.75 mV and 25.56 ± 1.46 mV, respectively, in the absence of divalent cations.

 
Frequently, we found that the channel opened during depolarization with a very long latency; therefore, we conducted prolonged recordings to further investigate the activation and the recovery properties of mIKr. Figure 5 demonstrates that the presence of divalent cations shifts the latency of activation during both depolarization and repolarization. Figure 5A is a recording in the absence of divalent cations, in which we observed no single-channel activities at +60 mV, but observed single channel activities upon both repolarization and depolarization to –60 mV, though with a much short latency upon repolarization (0.21 s) than depolarization (1.5 s). Since the depolarization- and repolarization-activated currents have the same pattern and have the same amplitude of single-channel current (0.59 pA at –60 mV), we assumed that these currents are from the same channel. In the presence of divalent cations, the most negative membrane potential at which we observed single-channel activities during depolarization was –40 mV (Fig. 5B). This dramatically contrasted with recordings without divalent cations, for which single-channel activities during depolarization could be observed as negative as –70 mV. At –40 mV the latency of activation upon depolarization and repolarization in the presence of extracellular divalent cations was much longer than that without divalent cations (Fig. 5C). The effect of the extracellular divalent cations on the gating properties of mIKr at the single-channel level was further examined by analysing the open probability as a function of voltage. An all-events histogram from continuous single-channel recording during depolarization fitted with Gaussian distributions at –60 mV is shown in Fig. 6A. The open probabilities at –70 mV, –60 mV, –50 mV and –40 mV in the absence of divalent cations were 0.17 ± 0.01 (n= 4), 0.16 ± 0.01 (n= 8), 0.15 ± 0.01 (n= 10) and 0.14 ± 0.01 (n= 4), respectively (Fig. 6B). In contrast, the presence of divalent cations significantly inhibited the open probability at –40 mV (NPo 0.08 ± 0.01, n= 7, P < 0.05) as compared with that obtained under divalent-free conditions at the same potential. Only at this potential could the channel activity be analysed accurately, because at more positive potentials the current amplitude was too small to be differentiated from the recording noise.



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Figure 5.  Divalent cations prolong latency of activation
A is a recording in the absence of divalent cations. The channel activated upon repolarization to –60 mV from +60 mV with latency of 0.21 s, but with 1.5 s latency upon depolarization to –60 mV from –20 mV. a and b demonstrate enlarged depolarization- and repolarization-activated channel currents, respectively, and both currents have an amplitude of 0.59 pA. B, is a recording in the presence of divalent cations. The channel opened 25 s later upon depolarization to –40 mV. However, channel opening was seen within 0.87 s during repolarization. Expanded parts c and d show depolarization- and repolarization-induced currents, and both currents have amplitude of 0.32 pA. C, histogram demonstrates the latency of activation during depolarization (left) and repolarization (right). Note the different scale of Y-axis at left and right. Latency of activation was determined by gap-free recordings holding at each potential for 1 min, and latency of recovery was determined upon –60 mV (without divalent cations) or –40 mV (with divalent cations) from 20-s preceding potential of +60 mV. Filled bar is with divalent cations, and open bar is without.

 


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Figure 6.  Open probability and dwell time of a single mIKr channel
A, histogram of mIKr current amplitude at –60 mV. Histogram was constructed from a 20 s gap-free recording in steady-state during depolarization (see inset). Both open and closed domains were fitted with a Gaussian function, and the proportion of the area under the curve was used to estimate the open probability of the channel. B, open probability at different membrane potentials in the absence of divalent cations (open bars) and in the presence of divalent cations (filled bars, only at –40 mV). C and D, open and closed time at –40 mV in the absence of divalent cations. Open time could be best fitted with one exponential function; closed-time clearly shows two peaks and could be best fitted with two exponential functions. E and F, open and closed time at –40 mV in the presence of divalent cations.

 
Dwell-time kinetics of the mIKr channel was analysed from 1–3 min continuous recordings. The open time could be well-fitted with one exponential function, whereas the closed time needed two exponentials to fit. The open-time histograms at –40 mV are demonstrated in Fig. 6C and E (without and with divalent cations, respectively), and the closed-time histograms are shown in Fig. 6D and F (without and with divalent cations, respectively). The mean open time with and without divalent cations at –40 mV was 3.53 ± 0.54 ms (n= 6) and 4.06 ± 0.82 ms (n= 4), respectively, and no difference was found between the two groups (P > 0.05). Two exponential fittings of the closed time revealed a short mean closed time (tc1) and a long closed time (tc2) with relative amplitudes of 0.7 and 0.3, respectively. Under divalent-free conditions, the resulting tc1 and tc2 were 1.72 ± 0.41 and 110.68 ± 17.24 ms (n= 4), respectively, as compared with 1.69 ± 0.33 and 175.63 ± 17.85 ms (n= 6), respectively, with the extracellular divalent cations. Therefore, the existence of divalent cations in the extracellular solution prolonged the long closed-time tc2 (P < 0.05) without affecting the short closed-time tc1 (P > 0.05). This may explain the reduced open probability as demonstrated in Fig. 6B.

Thus far, we have described a single channel in mice that possesses biophysical properties resembling those of IKr channels recorded in other species and have explored the effect of extracellular divalent cations on its single-channel behaviour. To further verify that the channel we observed was indeed IKr, we examined the effect of E-4031, a specific blocker of IKr, on the single-channel activity. As shown in Fig. 7, E-4031 inhibited channel events during both depolarization and repolarization. Complete blockade by 1 µM E-4031 was seen within 1 min of application. In 2 of 15 patches, channel activities partially recovered after a 5-min washout period. In the other 13 patches that could be followed for 5–10-min washout periods, the effect of E-4031 was irreversible.



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Figure 7.  Effect of E-4031 on mIKr
A depicts a continuous recording at different potentials (mV) in the absence of divalent cations. At least three channels were included in this patch; a shows an enlarged recording. B, 1 µM of E-4031 blocked the channel activities during both depolarization and repolarization. C, after washout of E-4031, the channel activities could be partially recovered; b is an expanded recording.

 
The abundance of single mIKr channels on membranes of adult mouse ventricular myocytes suggests that mIKr might participate in regulating mouse cardiac repolarization. However, under physiological conditions, the whole-cell current of mIKr confirmed that its density is small, with a maximal E-4031-sensitive tail current of 0.23 pA pF–1 measured at +50 mV (Fig. 8D). Furthermore, 5 µM E-4031 failed to affect the shape of the action potential of the adult cardiomyocyte (Fig. 8E). AP durations at 50% and 90% repolarization were 7.77 ± 1.45 and 19.85 ± 5.1 ms, respectively, before E-4031 application versus 7.50 ± 1.20 and 19.17 ± 4.60 ms after E-4031 application (n= 7, P > 0.05). We also applied an AP waveform recorded in the whole-cell mode to examine single-channel activity during the course of the AP. APs were applied at a frequency of 400 b.p.m. (comparable to the resting heart rate of a conscious mouse). Single-channel events were rarely observed in the presence of divalent cations but could be observed in 16.5% of the sweeps (258/1560 sweeps, from 7 patches) when divalent cations were removed from pipette solution (Fig. 8F). These observations suggest that, despite the abundant expression of functional mIKr channels, their physiological role in mouse cardiac repolarization might be attenuated by the presence of divalent cations.



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Figure 8.  E-4031-sensitive whole-cell current and effect of E-4031 on action potential
A and B, a family of whole-cell currents before and after 5 µM E-4031 recorded in normal Tyrode solution with 1 mM 4-AP and 4 mM TEA. Inset is the voltage protocol. C, The E-4031 difference currents obtained by off-line subtracting recording B from recording A. D, current–voltage relationship of E-4031-sensitive tail current. E, representative action potentials recorded before (continuous line) and after (dashed line) 5 µM E-403. F, single mouse IKr current recorded during AP stimulation (pipette solution without divalent cations).

 
Single HERG channel expressed in CHO cells

Previous results from other laboratories demonstrated single-channel activities (IKr/HERG) could only be observed during repolarization after the channel had been activated at high voltages (Veldkamp et al. 1995) even under divalent-free conditions (Veldkamp et al. 1993; Zou et al. 1997). This contrasts with our observations of mIKr openings following both depolarization and repolarization. We therefore examined the single-channel activity of HERG stably expressed in a CHO cell line under similar recording conditions to compare its properties with those of mIKr. As shown in Fig. 9 (comparable format to Fig. 2), single HERG channel events were observed at all repolarizing potentials (–120 to ~–20 mV) following the +60 mV prepulse. As for mIKr channels, the presence of divalent cations did not affect the slope conductance of the HERG channel (13.44 ± 0.34 pS, n= 9, with divalent versus 13.39 ± 0.50 pS, n= 15, divalent-free). With the standard protocol shown in Fig. 4, we also observed that the HERG channel could be activated during depolarization and repolarization, a phenomenon like that observed in the mIKr channel, but activated at more negative potentials than mIKr channels (Fig. 10). The mean half-activation voltage (V1/2) was –33.82 mV in the presence of divalent cations, and the slop factor is 7.14 mV; in the absence of divalent cation the V1/2 and slop factor are –65.93 mV and 12.18 mV, respectively. Again, effects of divalent cations on HERG channels were similar to those on mIKr; i.e. positively shifted by ~30 mV. Further continuous recordings proved that HERG channels could be activated as far negative as –110 mV (found in 50% patches, n= 21). In Fig. 11, we first held the membrane at –120 mV for at least 20 s and then gradually stepped to less negative potentials. The channel opened after a 16 s delay following the potential change to –110 mV. After the channel was closed at –110 mV, the membrane potential was stepped to –100 mV, which triggered second openings after a 12.5 s latency. At +60 mV, the channel opened sparsely, but multiple channels were seen upon repolarization to –110 mV. Similar to the activation of mIKr channel, activation of the HERG channel was also slow upon depolarization, but fast upon repolarization.



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Figure 9.  Deactivation of HERG channel as a function of membrane potential
A and B, recordings with and without divalent cations in the pipette solution. Voltage protocol is shown in the lower panel of A. Holding potential is –120 mV (without divalent cations) or –80 mV (with divalent cations); test pulses to potentials from –20 to –120 mV were preceded by a 400 ms prepulse to +60 mV. A 200 ms postpulse of –160 mV was applied after test potentials to quickly terminate channel activity. Single-channel current amplitude measured in various membrane potentials was used to construct the current-voltage relationship shown in the lower part of column B, with divalent cations (•, n= 9); without divalent cations ({circ}, n= 15).

 


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Figure 10.  Depolarization-induced activation of HERG channel
Currents were recorded using the voltage protocol shown in lower part of A. Membrane was held at –80 mV (with divalent cations) or –120 mV (without divalent cations). Test potentials ranging from –110 to +50 mV at an increment of 20 mV were followed by a repolarization to –60 mV (with divalent cations) or –80 mV (without divalent cations) to elicit the tail currents. A 200 ms step depolarization to –160 mV was applied to terminate channel activity before returning to the holding potential. A, recording with divalent cations in the pipette solution. B, recording without divalent cations in the pipette. NPo of tail current as a function of potential is shown in the lower panel of B. NPo was measured in the first second of the tail current in the presence of divalent cations (•, n= 9); or in their absence ({circ}, n= 9). These data were well fitted with a Boltzmann function. In the presence of divalent cations; the V1/2 and k are –33.82 ± 0.63 mV and 7.14 ± 0.61 mV, respectively, and in the absence of divalent cations, they are –65.92 ± 2.42 mV and 12.18 ± 2.09 m, respectively.

 


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Figure 11.  HERG channel activity during depolarization and repolarization
A–F is a continuous recording, truncated for clarity. No channel opening was observed while membrane potential was held at –120 mV for 20 s (A); Channel opening was observed when the voltage was stepped to –110 mV, with a 15.8 s latency (B and C). After being closed for 37.5 s at10 –1mV, the channel re-opened at –100 mV after a latency of 12.5 s. D, channel activity observed at –90 mV (E). At +60 mV, channels opened only occasionally, and multiple channels quickly deactivated upon repolarization to –110 mV. a, b, c and d are enlarged recordings.

 

    Discussion
 Top
 Abstract
 Introduction
 Methods
 Results
 Discussion
 References
 
We report for the first time the recording of single-channel current (mIKr) from membranes of adult mouse ventricular myocytes and our finding that this current has properties resembling those of the HERG channel (Zou et al. 1997; Kiehn et al. 1999) and IKr channels in rabbit and guinea-pig ventricular myocytes (Veldkamp et al. 1996, 1993; Shibasaki, 1987; Horie et al. 1991). Like IKr channels in other species, mIKr is inwardly rectifying. Single-channel openings are barely detected at positive potentials but are easily recorded upon repolarization from a positive to a negative potential. Ensemble-averaged current showed rapid recovery from inactivation followed by slow deactivation, and the time course of deactivation could be best fitted with two exponential functions. Single-channel conductance at negative potentials is 12 pS; the steady-state open probability at negative potentials is around 0.16. The open-state dwell time could be fitted with one exponential function, while the closed-state dwell time could be fitted with two exponential functions. In addition, single-channel activity could be blocked by E-4031, a specific blocker of IKr. Thus, mIKr is similar to IKr in other species (Veldkamp et al. 1995, 1993; Shibasaki, 1987; Horie et al. 1991) in terms of inward rectification, single-channel conductance, gating properties, and response to the selective blocker E-4031.

Whole-cell experiments examining the properties of IKr/HERG have demonstrated that extracellular divalent cations reduce the current's amplitude, shifted its activation, and slowed its inactivation (Ho et al. 1996, 1998, 1999; Paquette et al. 1998; Johnson et al. 1999; Song et al. 1999). Our single-channel data are consistent with the findings of macroscopic studies and further characterize the effect of Ca2+/Mg2+ on the IKr/HERG channel. We found that physiological concentrations of extracellular Ca2+/Mg2+ caused ~30 mV positive shift in activation. Moreover, extracellular Ca2+ and Mg2+ reduced the open probability through prolongation of a long closed time but did not affect the conductance of the IKr/HERG channel. These results indicate that extracellular divalent cations may exert a direct effect on the voltage sensor of the channel. However, it is worth noting that Ca2+ and Mg2+ may not necessarily exert their effects on the IKr channel in the same manner, either quantitatively or qualitatively, and thus further studies investigating their individual effects are warranted.

When HERG channels were expressed in CHO cell, they showed similar behaviour to mIKr channels in conductance, activation and deactivation. However, HERG channels activated at more negative potential than mIKr channels. These results suggest that, in native myocytes, the IKr channel may be regulated by additional subunits (e.g. MiRP1 and/or minK) that modify the threshold of activation. Alternatively, PiP2 might play a role in determining the threshold, since it shifts activation and increases open probability (Bian et al. 2001).

Previous single-channel studies of IKr in rabbit and human ventricular myocytes (Veldkamp et al. 1993, 1995) or the HERG channel in Xenopus oocytes (Zou et al. 1997; Kiehn et al. 1999) indicated that IKr/HERG is a repolarization-activated channel, since no single-channel openings were observed while the potentials were held at values more negative than –70 mV. However, we find that single-channel openings of mIKr and HERG can be seen at quite negative holding potentials, especially after divalent cations are removed from the extracellular solution. This notion is consistent with the whole-cell recording of the IKr/HERG current. The failure of the former studies to observe single-channel openings at negative holding potentials might be attributable in part to the presence of divalent cations in the pipette solution, since the addition of Ca2+/Mg2+ dramatically shifts activation. Another potential explanation could be the short holding time, since the activation latency was sometimes quite long at negative potentials. Alternatively, the difference could also be attributed to the presence of species-specific subunits, or differences in expression systems (Abbott et al. 1999; McDonald et al. 1997).

Contrary to the early dofetilide-binding findings of an absence of IKr on the membrane of adult mouse ventricular myocytes (Wang et al. 1996), we found that IKr was expressed abundantly in single-channel recordings. Our data correlate well with recent observations documenting robust expression of mERG transcript and polypeptide in the mouse heart (London et al. 1997; Lees-Miller et al. 1997; Pond et al. 2000; Pond & Nerbonne, 2001). However, at the whole-cell level when physiological concentrations of Ca2+ and Mg2+ are present, mIKr appears to play a minimal role in cardiac repolarization, as confirmed by pharmacological studies with dofetilide (Wang et al. 1996) and E-4031 (Fig. 8E). Indeed, the current density of mIKr (~0.23 pA pF–1 at +50 mV for 1 s) was 50- to ~100-fold less than those of the dominant Ito (25–35 pA pF–1) and IK,slow (15–20 pA pF–1) (Zhou et al. 1998,2003; Xu et al. 1999; Guo et al. 1999). It is highly possible that the effects of extracellular Ca2+/Mg2+ (e.g. shifting the activation and reducing the open probability) have made activation of mIKr so difficult as to prevent its playing a role in repolarization during the extremely short action-potential duration above its activation threshold. Supporting this notion is our failure to observe any single-channel activity using an action potential waveform to stimulate the membrane patch in the presence of Ca2+/Mg2+ but our ability to detect channel events when extracellular Ca2+/Mg2+ was removed (see Fig. 8F).

Since single-channel opening of the IKr/HERG channel could be seen at negative potentials close to the K+ equilibrium potential, IKr/HERG might also contribute to maintenance of the resting membrane potential. Although this may not be important to ventricular myocytes, in which resting potential is dominated by IK1 (Kir channel), it might be important for maintenance of maximal resting membrane potential of pacemaker cells, such as sino-atrial node pacemaker cells, which are thought to be rich in the IKr channel (Ito & Ono, 1995; Matsuura et al. 2002; Noma et al. 1984) but lacking in the Kir channel (Noma et al. 1984; Nathan, 1986). Interestingly, a recent study demonstrated episodes of sinus bradycardia related to functional deficiency of IKr channels in pacemaker cells in ERG1 B knock-out mice (Lees-Miller et al. 2003). Additionally, we speculate that mIKr may serve as a divalent cation sensor in cardiomyocytes and that depletion of cations in microdomains outside the cell may result in the activation of mIKr at negative potentials and influence membrane potential.


    References
 Top
 Abstract
 Introduction
 Methods
 Results
 Discussion
 References
 
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    Acknowledgements
 
We thank Dr Günter Schlichthörl for the data evaluation and figures. This work was supported by NIH grants to G.K. and by the Canadian Institutes of Health Research and the Quebec Heart and Stroke Foundation.




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