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From the Vanderbilt University School of Medicine, Departments of Medicine and Pharmacology, Nashville, Tenn.
Correspondence to Dan M. Roden, MD, Director, Division of Clinical Pharmacology, Vanderbilt University School of Medicine, 532C Medical Research Building I, Nashville, TN 37232-6602.
| Abstract |
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inactivated and
inactivated
open transitions. Thus, in these cardiac
myocytes, as with heterologously expressed HERG,
IKr undergoes fast inactivation that determines
its characteristic inward rectification. These studies demonstrate that
the mechanism underlying decreased activating current observed at low
[K+]o is more extensive fast inactivation.
Key Words: K+ current delayed rectifier extracellular K+ fast inactivation heart
| Introduction |
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A second mechanism, proposed in 1987 by Shibasaki2 during
studies of a current strongly resembling IKr in
rabbit AV nodal cells, is that rectification is determined by very fast
inactivation from the open state. In the simplest model,
closed
open
inactivated, it was suggested that more
channels entered the inactivated state with stronger
depolarizations, thus producing apparent rectification. With
repolarizing pulses, inactivated channels would rapidly
enter the open state, from which channels would close slowly, thereby
accounting for the experimentally observed hooks. Recent studies of
currents resulting from expression of the human ether-à-go-go
(HERG) gene, thought to be a major
IKr subunit, have provided strong evidence in
support of this mechanism.12 13 14 15 16
In AT-1 cells, derived from the atrial tumors arising in mice carrying a transgene in which expression of the simian virus 40 large-T antigen is driven by the atrial natriuretic factor promoter,17 IKr is the sole delayed rectifier observed.18 19 We have shown that IKr in these cells is very similar to that recorded in other mammalian cardiac myocytes, making AT-1 cells a convenient system in which to study the physiology and pharmacology of this current.18 The goals of the present study were to determine if lowering intracellular Mg2+ influenced IKr rectification or drug block and to determine the role of rapid inactivation in IKr rectification and in the anomalous response of IKr to changes in [K+]o. Portions of this study have been reported previously.20 21
| Materials and Methods |
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Electrophysiological Recording
Recordings were performed using an Axopatch-1A or 200A
patch-clamp amplifier (Axon Instruments, Inc) in the whole-cell
configuration of patch-clamp technique.22 Experiments were
conducted at room temperature (20°C to 22°C). After the whole-cell
configuration was established, the capacitive transients elicited by
symmetrical 10-mV voltage-clamp steps from -80 mV were recorded at
50 kHz (filtered at a bandwidth of 10 kHz, -3 dB) for calculation of
capacitive surface area. Thereafter, capacitance and series resistance
compensation were optimized; 80% compensation was usually obtained.
The extracellular solution was normal Tyrode's that contained (in
mmol/L) CaCl2 1.8, MgCl2 1, HEPES 10, and
glucose 10; for the experiments studying changes in
[Mg2+]i, 4 mmol/L KCl and 130
mmol/L NaCl were used, whereas for experiments studying changes in
[K+]o, equimolar NaCl was substituted or
added for KCl. The pH of the solution was adjusted to 7.35 with NaOH.
The intracellular pipette filling solution contained (mmol/L) KCl 110,
K4BAPTA 5, K2ATP 5, MgCl2 1, and
HEPES 10, and the solution was adjusted to pH 7.2 with KOH, yielding a
final [K+ ]i of
145 mmol/L. In all
experiments, L-type Ca2+ current, Na+ current,
and T-type Ca2+ current were eliminated by adding 1
µmol/L nisoldipine, 30 µmol/L tetrodotoxin, and 200
µmol/L NiCl2 to the extracellular solution. To study the
effect of nominal [Mg2+]o
([Mg2+]o=0), MgCl2 was omitted
from the filling solution. To assess drug block as a function of
[Mg2+]o, tail current after a 1-second test
pulse to 20 mV was monitored during drug washin; once steady state was
established (usually within 10 to 15 minutes), tail currents were
measured at a range of test potentials. A higher drug concentration was
then washed in; a maximum of baseline and three sequentially increasing
drug concentrations were assessed in this fashion. To study the
inactivating behavior of IKr as a function of
[K+]o, currents were recorded before and
during exposure to a high concentration (1 µmol/L) of the
IKr-specific blocker dofetilide.
Analysis of current amplitudes and calculation of time
constants was then performed on dofetilide difference currents,
obtained by digital subtraction. Salts and quinidine were purchased
from Sigma Chemical Co. Nisoldipine was obtained from Miles
Pharmaceutical, Inc, and dofetilide was provided by Pfizer Central
Research. Stock solutions were stored at 4°C, and the final
concentrations in the bath were obtained by diluting the stock
solutions in the external solution during experiments.
Voltage-Clamp Protocols and Data Analysis
The specific protocols used are described in "Results." To
compare current densities among cells, currents are reported as current
per unit capacitance (pA/pF) after linear leak subtraction and
normalization relative to cell surface area, determined by measurement
of capacitance, as described above. The drug concentration blocking
50% of current, IC50, was determined using a Hill
function, ie, block=1/{1+(IC50/[D])n},
where [D] is the drug concentration. Results are expressed as mean±1
SE.
| Results |
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The lack of effect of altering intracellular constituents on
IKr rectification suggests that fast
inactivation may play a role. Fig 2
shows voltage
dependence of deactivation and preceding hooks after a depolarizing
pulse to +40 mV. Deactivation (transitions from open to closed states)
proceeded relatively slowly (eg,
=165 ms at -30 mV). In contrast,
the time course of the hooks (transitions from inactivated
to open states) was much faster and accelerated (as shown in Fig 2B
) at
hyperpolarized potentials. For example, at -120 mV, the time constant
of the hook was 2.4 ms; summary data are presented below.
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This difference in time courses was exploited to dissect
inactivated
open from open
closed transitions, as shown
in Fig 3
. Both tracings presented in Fig 3
represent different currents after exposure to the
IKr blocker dofetilide. Fig 3A
shows activating
IKr and deactivating tail current (with a
preceding hook) elicited by a 1520-ms pulse to +40 mV, with
repolarization back to -40 mV. At the end of the depolarizing pulse,
channels would be in the open (activating current) and
inactivated states. Fig 3B
shows the identical
600-pA
current elicited in the same cell by a pulse to +40 mV. Instead of a
1520-ms pulse, however, the pulse was interrupted after 1 s by a
brief (20-ms) hyperpolarizing step to -120 mV. Upon return to +40 mV,
a very large (
3900 pA) current that then decayed rapidly (
=18 ms)
back to the 600-pA baseline was observed. Repolarization back to -40
mV then elicited the same hook, followed by a slowly (
=219 ms)
deactivating tail current, as in the left panel. This provides direct
evidence that IKr in these cells behaves in a
fashion similar to that reported for expressed HERG: during
strong depolarizations, the channel undergoes rapid and extensive
inactivation that can be relieved by a short hyperpolarizing pulse.
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Further evidence in support of this concept is shown in Fig 4
. Here, the duration of the hyperpolarizing pulse from
+40 to -120 mV was varied. The effect of 20- and 200-ms
hyperpolarizing pulses is shown in Fig 4A
. With the short
hyperpolarizing pulse, a large current was observed with the pulse back
to +40 mV (dotted line), as in Fig 3B
. With the longer 200-ms
hyperpolarizing pulse, channel deactivation was observed at -120 mV.
Thus, just before the pulse back to +40 mV, fewer channels remain in
the inactivated state, and most of the open channels had
closed. Indeed, with the pulse back to +40 mV, the large rapidly
inactivating current was not observed; rather, channel reopening
occurred. Fig 4B
shows the effect of varying the hyperpolarizing pulse
from 20 to 200 ms. The amplitude of the currents elicited immediately
after the subsequent steps back to +40 mV is shown, along with the time
course of the current recorded during a long step (200 ms) to -120
mV. Fig 4C
shows that the two time courses are similar, with time
constants of 32 to 33 ms. Moreover, the ratio of tail current at -120
mV to instantaneous current at +40 mV was
0.33 and was independent
of the duration of the hyperpolarizing pulse (Fig 4D
); ie, an envelope
test was satisfied. These data demonstrate that with longer
hyperpolarizing pulses, not only do inactivated channels
open, but open channels begin to close. The fact that the envelope test
is satisfied indicates that both recovery from inactivation (with short
pulses) and channel closing (with longer pulses) at -120 mV determine
the availability of channels to open during a subsequent pulse to +40
mV. If a K+ reversal potential of
-80 mV is assumed,
the ratio of tail current at -120 mV to instantaneous current at +40
mV should be [-80-(-120)]/[40-(-80)], or 0.33. Thus, the
result of the experiment also indicates that contamination by other
conductances is minimal.
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The experiment shown in Fig 3
was repeated at a range of
depolarizing potentials in two different ways. In the first, a 1-s
pulse to a range of activating potentials was followed by a 20-ms
hyperpolarizing pulse to -120 mV and a third 500-ms pulse to the same
potential as the first (Fig 5
). In the second, a 1-s
pulse to +50 mV and a subsequent 20-ms pulse to -120 mV were followed
by pulses to a range of potentials (Fig 6
). In both
approaches, dofetilide difference currents were used, as described in
"Materials and Methods." Fig 5
demonstrates that relief of
inactivation by a hyperpolarizing pulse augmented the outward current
to a small extent at negative test potentials (eg, -10 mV); the
augmentation was considerably greater at more positive potentials (eg,
+40 mV), indicating greater inactivation at positive potentials. I-V
curves for activating current and for total current immediately after
the hyperpolarizing pulse are presented in Fig 5B
. It is
apparent that the brief hyperpolarizing pulse completely relieved the
inward rectification shown with the activating current.
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When IKr was first fully activated
and the effect of brief hyperpolarization was
studied (Fig 6
), a similar result was observed: the I-V curve for total
current just after the hyperpolarizing pulse (instantaneous current,
Fig 6D
) displayed slight apparent outward rectification. This approach
was then used to test the hypothesis that the decrease in activating
IKr observed with low
[K+]o is due to
[K+]o enhancement of fast inactivation. The
results of one such experiment are shown in Fig 7
. As
previously reported,3 4 activating current was smaller at
low [K+]o: activating current in this
experiment after 1 s at +40 mV was 2.2 pA/pF with 1 mmol/L
[K+]o, 3.3 pA/pF with 4 mmol/L
[K+]o, and 4.9 pA/pF with 20 mmol/L
[K+]o. However, with relief of inactivation
by a short hyperpolarizing pulse, it is evident that total
(instantaneous) current was largest at 1 mmol/L
[K+]o and smallest at 20 mmol/L
(arrows).
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Fig 8
shows I-V curves for activating
IKr at [K+]o at 1, 4,
and 20 mmol/L. With step depolarizations, prominent inward
rectification was evident, and the currents were larger at 20 than at
1 mmol/L. In contrast, using the approach shown in Figs 6
and 7
to
remove IKr inactivation, near-ohmic I-V curves
are apparent. Furthermore, the curves were parallel, differing only in
their x intercepts (reversal potentials), indicating that
the rectification of IKr can be attributed
virtually exclusively to rapid inactivation. The reversal potentials
were consistently slightly positive to those predicted by the
Nernst equation: -109±3 (observed) versus -127 mV (predicted) at
1 mmol/L, -80±1 versus -91 mV at 4 mmol/L, and -49±2
versus -50 mV at 20 mmol/L.
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The experiment shown in Fig 7
indicates not only that the distribution
of channel states during depolarizing pulses is
[K+]o dependent but also suggests that the
transition rates between the states, reflected by the time constants
indicated, are similarly [K+]o dependent. Fig 9
shows that with elevated
[K+]o, both the
inactivated
open (Fig 2
) and
open
inactivated (Figs 6
and 7
) state transitions were
markedly slower. However, even at 20 mmol/L
[K+]o, the rate of recovery from fast
inactivation at -120 mV was still rapid enough that the process was
still essentially complete within the 20-ms hyperpolarizing pulse. At
potentials <0 mV, inactivation may be contaminated by deactivation
(eg, see Fig 6A
and 6C
), making measured inactivation rate slower than
the actual rate. For this reason, points negative to 0 mV are indicated
by open symbols in Fig 9B
.
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| Discussion |
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A number of groups have reported that when HERG is expressed in oocytes10 14 15 16 or in noncardiac mammalian cells,12 13 the observed current displays IKr-like rectification that can be relieved using brief hyperpolarizations. Thus, the present experiments indicate that the mechanism underlying rectification of IKr in cardiac myocytes is very similar to that found with heterologous expression of HERG. Liu et al31 have reported that the delayed rectifier in ferret atrial myocytes also displays this behavior. Moreover, the present data, as well as previous studies involving guinea pig myocytes (where a prominent IKs is present)10 and, more recently, expressed HERG confirm the suggestion that intracellular Mg2+ does not mediate IKr rectification.11 An important new finding in the present studies (previously suggested in studies of HERG expressed in Xenopus oocytes14 ) is that rapid inactivation is also the mechanism that determines another important physiological characteristic of IKr, its unusual sensitivity to changes in [K+]o.
The approach we and others have used assumes that recovery of
inactivated channels to the open state takes place much
faster than open-channel deactivation, thereby allowing separation of
the two processes. Indeed, if the duration of the hyperpolarizing pulse
is prolonged, we did observe a decrease in the subsequent
activated current (Fig 4
). The finding that the time course of
the outward peak currents following the hyperpolarizing pulse
paralleled that of the current observed during a long
hyperpolarization (ie, an envelope test is
satisfied) indicates that channel recovery from inactivation during a
hyperpolarizing pulse does determine the availability of open channels
during the subsequent repolarizing pulse. We also make the simplifying
assumption of a three-state model to provide a framework within which
to conceptualize the relationship between inactivation and
rectification. The sigmoid nature of activation with some depolarizing
pulses speaks to the fact that this must be a simplification.
Similarly, this model does not explain the very slow inactivation we
and others have observed both in AT-1 cells18 and in human
myocytes.29 30 When HERG was expressed in
Xenopus oocytes, the voltage dependence of the time
constants for inactivation and for recovery from fast inactivation was
similar to that observed here.10 However, the actual rates
were somewhat faster, raising the possibility of a species difference
or of a difference between HERG (expressed in
Xenopus oocytes) and IKr (in cardiac
myocytes). Such a difference is further suggested by the recent cloning
of a "cardiac-specific" ERG isoform from mouse32 and
the report of altered IKr deactivation kinetics
with coexpression of the cardiac and other ERG
isoforms.33 As discussed above, it is also possible that
at negative potentials, the measured inactivation rate is contaminated
by channel deactivation. Liu et al31 have
presented evidence that modeling IKr in
ferret cells requires at least four states. In their studies, fast
inactivation was relatively insensitive to voltage (as in our Fig 9B
),
and activation was dependent on at least two processes, one voltage
dependent and one voltage independent. The same group has more recently
reported that when HERG is expressed in Xenopus
oocytes, the rate of recovery from fast inactivation was decreased when
[K+]o was increased from 2 to 98
mmol/L.34 However, the rates of recovery from fast
inactivation that would occur over the lower range of
[K+]o used in the present study have not
been studied.
Multiple mechanisms are thought to underlie inactivation in
voltage-gated ion channels.35 With N-type inactivation, a
"ball-and-chain" mechanism has been proposed.36 37
With C-type inactivation, on the other hand, a direct effect of channel
protein conformational transitions on the conducting pore is
envisioned.37 Smith et al12 have now shown
that inactivation is entirely removed by mutations on the extracellular
face near the pore-S6 junction, indicating similarity to a C-type
inactivation mechanism. Presumably, K+ ions interact with
this site to affect C-type inactivation. Indeed, slowing of
inactivation by elevation of [K+]o has been
reported for expressed HERG,14 for rapidly
inactivating members of the Shaker family,38 39
and now for IKr (Figs 7
and 9
); as discussed
below, this slowing may contribute to the greater amplitude of
activating IKr at elevated
[K+]o. Interestingly, preliminary studies
indicate that the methanesulfonanilide E4031 (a compound with
structural and pharmacological features similar to dofetilide) probably
blocks the channel from the intracellular side.40 Thus,
the effect of changing [K+]o to modulate drug
block may not be determined at a single-channel protein domain. For
example, conformational changes induced by
[K+]o effects at extracellular sites may make
intracellular binding drug domain(s) more or less accessible. Another
possibility is that competition between drug block and fast
inactivation may change the apparent time course of block and possibly
the apparent affinity, as suggested previously.13 The
observed [K+]o-induced changes in the rate
constants for fast inactivation could then indirectly modulate
observable block. The mechanism(s) underlying modulation of drug block
by changing [Mg2+]i remains to be determined,
but in this case, a direct interaction between
[Mg2+]i and drug at a distinct binding site
in the channel protein is one possibility.
The magnitude of macroscopic current during a depolarizing pulse will
be determined by partitioning between open and inactivated
channel states and by the time courses of the closed
open and
open
inactivated transitions. Even though faithful
recapitulation of IKr may require models with
multiple closed, open, or inactivated states, the smaller
activating current in low [K+]o suggests
decreased open-channel probability at steady state.
Shibasaki2 demonstrated that single-channel conductance
was dependent on [K+]o, which was studied at
values of >50 mmol/L; for example, increasing
[K+]o from 100 to 300 mmol/L increased
conductance from 8 to 15 pS. However, it is not known whether such an
effect contributes at all at the lower more
physiological [K+]o
values we studied. For "conventional" inactivating channels,
channel opening is much faster than inactivation, and a characteristic
transient current signature results. For IKr, it
is now apparent that the reverse is the case: the
open
inactivated transition occurs much more rapidly than
does the closed
open one.2 It has been suggested that
hyperpolarization-mediated fast recovery from
inactivation might result in a dramatic increase in
IKr during repolarization, in analogy to the
experiment shown in Fig 3B
, and that this increase in
IKr might thus be antiarrhythmic by inhibiting
early afterdepolarizations.41 However, our data indicate
that entry and exit from inactivated state(s) is very
rapid, even at room temperature. Given the slow time course of
repolarization in cardiac cells, it becomes difficult to conceive of
the conditions under which the relief of inactivation by brief
hyperpolarization (an entirely
unphysiological event) might play such a direct
antiarrhythmic role. However, mutations in HERG or the use
of IKr-blocking drugs are both associated with
torsade de pointes, which is thought to arise from early
afterdepolarizations. If the mechanisms underlying reduced
IKr under these circumstances were to involve
sequestration of channels in the inactivated, rather than
open, states during depolarization, a direct role of fast inactivation
in arrhythmogenesis (and of normal inactivation in arrhythmia
suppression) might be inferred. Generically, any augmentation of
outward current during repolarization would shift the balance between
inward and outward current during repolarization and might therefore
inhibit the development of the inward current(s), such as L-type
Ca2+ current reactivating through a window mechanism,
responsible for early afterdepolarizations.42 Thus, a
major role for IKr in normal physiology may be
to repolarize cells sufficiently rapidly to avoid such arrhythmogenic
mechanisms.
We have previously pointed out that the greater sensitivity of IKr to drug block at low [K+]o may explain the well-recognized effect that hypokalemia promotes torsades de pointes.4 Moreover, this finding suggested that interventions (such as administration of K+) to increase [K+]o should prove antiarrhythmic in torsade de pointes related to decreased IKr; indeed, clinical studies lend some support to this concept.43 44 The present data further suggest that drugs whose major effect is to prevent or delay IKr inactivation might also reverse torsades de pointes. In addition, the decreased sensitivity at high [K+]o may provide an explanation for the "reverse use-dependent" effect of blocking drugs on action potential duration4 and raises the possibility of diminished drug effect during ischemia, which is frequently accompanied by elevations in [K+]o. Our findings demonstrating inhibition of block by low intracellular [Mg2+]i have similar implications: we speculate that with chronic hypomagnesemia (that may decrease [Mg2+]i), drug block will be diminished. Moreover, since these changes are frequently inhomogeneous, they would be expected to exaggerate dispersion of action potential durations, a potentially arrhythmogenic effect. Thus, the further elucidation of the mechanisms underlying modulation of drug block by changes in intracellular and extracellular cations may provide clues to the development of safer ion channel blocking drugs.
| Selected Abbreviations and Acronyms |
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| Acknowledgments |
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| Footnotes |
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Received December 19, 1996; accepted March 4, 1997.
| References |
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