Quinidine and 4AP are two nonspecific K channel blockers. Both block
voltage-gated K channels from the intracellular side of the membrane
and, in most cases, binding is facilitated by channel activation.
However, there are distinct differences between quinidine and 4AP in
the time- and voltage-dependencies of drug-channel interaction. To
learn about the molecular basis underlying the similarities as well as
differences in drug actions between quinidine and 4AP, we used rKv1.4
(rat isoform of Kv1.4) as a model and studied: 1) Is there an overlap
between the binding sites of quinidine and 4AP? and 2) What factors are
involved in determining the binding affinity and kinetics of
drug-channel interaction? Our data show that mutations at a position in
the S6 domain of rKv1.4 (position 529) can cause dramatic and often
opposite effects on quinidine and 4AP binding. For quinidine, the
degree of steric hindrance imposed by side chain at position 529 is an
important factor in determining binding affinity. For 4AP, 529 mutations that slow the rate of deactivation reduce binding affinity,
probably due to a low binding affinity in the open state. This, in
conjunction with the observations that 4AP binding is facilitated by
channel activation, suggests that optimal 4AP binding may occur in a
transitional state between fully-closed and fully-open states. In
addition, hydrophobic interactions between blocker molecules and
residues at 529 tend to stabilize the binding of both quinidine and
4AP. Because the S6 amino acid sequences are well conserved among many voltage-gated K channels, our findings have general implications in
understanding the structural determinants of quinidine and 4AP binding
to different K channels.
 |
Introduction |
The
structures of quinidine and 4AP are shown in figure 1. They share the
general feature of having a hydrophobic aromatic moiety (quinoline in
quinidine and pyridine in 4AP) and a tertiary amine. The two are
markedly different in size, with quinidine being much bulkier than 4AP,
especially in the quinuclidine structure surrounding the tertiary
amine. Their effects on native K channels have been extensively
characterized (Fedida et al., 1993
; Campbell et
al., 1993
; Furukawa et al., 1989
; Roden et
al., 1988
; Balser et al., 1991
; Imaizumi and Giles,
1987
). Studies using various K channel clones further provide
structural information about their actions (Tseng et al.,
1996a
; Yao and Tseng, 1994
; Kirsch and Drewe, 1993
; Yao et
al., 1996
; Tseng et al., 1996b
; Yatani et
al., 1993
; Yeola et al., 1996
). In a few cases,
quinidine and 4AP binding preferentially occurs in the "rested"
state and channel activation induces drug dissociation (Campbell
et al., 1993
; Tseng et al., 1996a
; Roden et
al., 1988
; Yao et al., 1996
). This type of drug-channel
interaction will not be discussed here. The focus of our study is on a
more general type of drug-channel interaction in which drug binding is
facilitated by channel activation.
Studies on the effects of quinidine and 4AP on voltage-gated K channel
clones indicate that both agents block the channels from the
intracellular side of the membrane and, in most cases, binding is
facilitated by channel activation. For channels that have a fast N-type
inactivation process (Yao and Tseng, 1994
; Yatani et al.,
1993
), binding of quinidine or 4AP and the closure of the inactivation
gate (occlusion of the inner mouth by the N-terminal domain) interfere
with each other. This points to the inner mouth region of the pore as a
candidate for binding sites of both quinidine and 4AP. Indeed,
site-directed mutagenesis of several K channel clones reveal important
roles of residues lining the putative inner mouth region in determining
the blocking potency of both quinidine (Zhang et al., 1995
;
Yeola et al., 1996
) and 4AP (Shieh and Kirsch, 1994
).
However, there are important differences between quinidine and 4AP in
the voltage- and time-dependencies of action (see "Results"). These
differences raise two questions: 1) Do the binding sites of quinidine
and 4AP overlap with each other? 2) What controls the binding site
affinity and the kinetics of drug-channel interaction?
We used a K channel clone, rKv1.4, as a model to compare the actions of
quinidine and 4AP. To avoid interference from the fast N-type
inactivation process in the measurement of drug effects, a deletion
mutant (rKv1.4
3-25) was used in which the N-type inactivation process was disrupted (Tseng-Crank et al., 1993
). In search
for a common or overlapping site involved in quinidine and 4AP binding, our focus was on the sixth transmembrane (S6) domain of rKv1.4. It has
been widely recognized that the S6 domains of Na, Ca and K channels
play important roles in channel gating (Hoshi et al., 1991
;
Zuhlke et al., 1994
; Zhang et al., 1994
; McPhee
et al., 1995
) and in drug binding (Yeola et al.,
1996
; Baukrowitz and Yellen, 1996
; Hockerman et al., 1995
;
Ragsdale et al., 1996
). With respect to the role of S6 in
drug binding, a general theme has emerged from studies on Na, Ca and K
channels: drug binding is stabilized by hydrophobic interactions
between drug molecules and hydrophobic residues in the S6 domains
(Yeola et al., 1996
; Baukrowitz and Yellen, 1996
; Hockerman
et al., 1995
; Ragsdale et al., 1996
). For
voltage-gated K channels, one position in the S6 domain seems to play
an especially important role in drug binding: residue at the 13th
position in the S6 sequence. In rKv1.4
3-25 this is threonine at
position 529, T529 (fig. 1). The
equivalent residue in the Shaker channel, T469, has been shown to play
a key role in determining the blocking potency of a series of pore blockers (Baukrowitz and Yellen, 1996
). The equivalent position in
hKv1.5, T505, also affects the binding affinity of quinidine and
bupivacaine (Vicente et al., 1997
; Yeola et al.,
1996
). According to the current model of voltage-gated K channels
(Durell and Guy, 1996
), the S6 domain consists of two
-helices due
to a proline residue(s) in this region (fig. 1). The N-terminal half of
S6 (5'S6) is juxtaposed with the P-region. The P-region lines the outer
portion of the pore and determines ion selectivity. The C-terminal half
of S6 (3'S6), together with the S4-S5 linker and the N-terminal half of
the S5 domain (5'S5), lines the wide inner vestibule of the pore (Shieh
and Kirsch, 1994
; Slesinger et al., 1993
; Lopez et
al., 1994
). T529 may be located in the intersection between the
narrowest part of the pore and the opening into the wide inner
vestibule, a "strategic" position for binding of an efficient pore
blocker. Therefore, we mutated T529 of rKv1.4
3-25 to different
residues and studied the effects of mutations on the binding of
quinidine and 4AP.

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Fig. 1.
Top, Cartoon of transmembrane topology of one subunit
of a generic voltage-gated K channel. The structures between the end of
S4 and the end of S6 are highlighted here. The linker between the S4
and S5 domains (S4-S5) is shown as a short -helix (Holmgren et
al., 1996 ). The pore sequence is divided into 5' half (P1, shown
as a short -helix) and 3' half (P2, shown as an elongated structure)
(Lu and Miller, 1995 ). The S6 domain is divided into two -helices
due to proline(s) in the sequence (Durell and Guy, 1996 ). The inner
vestibule of the pore is lined by the S4-S5 linker (Slesinger et
al., 1993 ), 5'S5 (Shieh and Kirsch, 1994 ) and 3'S6 domains (Lopez
et al., 1994 ). The amino acid sequence of S6 in
rKv1.4 3-25 is listed below, with threonine at position 529 highlighted. Bottom, Structures of quinidine and 4AP.
|
|
 |
Materials and Methods |
In vitro mutagenesis and oocyte preparation.
Oligonucleotide-directed mutagenesis was carried out on the
rKv1.4
3-25 background (Tseng-Crank et al., 1993
) using a
commercial mutagenesis kit according to the manufacturer's
instructions (Altered Sites System, Promega, Madison, WI). Mutations
were confirmed by DNA sequencing using the dideoxy-mediated chain
termination method.
cDNAs encoding the rKv1.4
3-25 and all the mutant channels were
linearized with appropriate restriction enzymes and used as templates
for cRNA synthesis. In vitro transcription reactions were
carried out using a commercial kit and T7 RNA polymerase according to
the manufacturer's instruction (mMessage mMachine, Ambion, Austin,
TX). The quality and quantity of cRNA product of each transcription
reaction were checked by denaturing agarose gel electrophoresis.
Preparation of Xenopus oocytes and injection of cRNA have
been described previously (Tseng-Crank et al., 1993
). Four
to 6 hr after isolation, each oocyte was microinjected with 20 to 40 nl
of a cRNA solution. The oocytes were then incubated at 16°C in the
following medium for 2 to 4 days before voltage clamp studies (in mM):
NaCl 96, KCl 2, CaCl2 1.8, MgCl2 1, HEPES 5, Na-pyruvate 2.5, pH 7.5 with NaOH, supplemented with penicillin (50 U/ml), streptomycin (50 µg/ml), gentamycin (10 µg/ml) and horse
serum (4%).
Electrophysiological experiments.
Whole cell currents were
recorded using a modified two-microelectrode voltage clamp method. The
voltage-sensing electrodes had a tip resistance of 1 to 2 M
, and the
current-passing pipettes had a tip resistance of 0.1 to 0.3 M
("cushion-pipettes," with tips filled with 1% agarose in 3 M KCl
to prevent 3 M KCl leakage). An Oocyte Clamp (OC-725B) amplifier was
used (Warner Instruments, Hamden, CT). During current recordings, the
oocytes were superfused with a Cl-free solution to minimize
interference from endogenous Cl channel currents. The composition of
this solution was as follows unless otherwise stated (in mM): NaOH 96, KOH 2, Ca(OH)2 1.8, MgSO4 1, HEPES 5, Na-pyruvate 2.5, pH 7.5 with methanesulfonic acid. The bath temperature
was 23 to 25°C, unless otherwise denoted. In some experiments the
extracellular [K] was raised to 98 mM. This solution was made by
replacing NaOH with equimolar KOH.
Quinidine-gluconate and 4AP stock solutions (100 mM, replacing NaOH
with drugs) was made in a Cl-free solution with pH adjusted to 7.5. These solutions were diluted to the desired final concentrations before
experiments.
Data acquisition and analysis.
Voltage clamp protocol
generation and data acquisition were controlled by a 486 IBM computer
via pClamp software and a Digidata 1200 interface (Axon Instruments).
Currents were digitized at a sampling interval of 0.1 to 0.5 msec. Data
analysis were performed using Clampfit (version 6.1 of pClamp), Excel
(Microsoft Corporation, Redmond, WA) and PeakFit (Jandel Scientific,
Corte Madera, CA) programs. Data are presented as means and S.E.s.
Statistical significance was tested by unpaired t test
(SigmaStat 2.0, Jandel Scientific).
 |
Results |
Comparison of Effects of Quinidine and 4AP on rKv1.4
The effects of quinidine on the wild-type rKv1.4 channel has been
well characterized (Yatani et al., 1993
). It was concluded that quinidine blocks the channel from the intracellular side of the
membrane and binding preferentially occurs in the open state. Quinidine
shortens the single channel open time and prolongs the closed time,
indicating that the binding and unbinding kinetics are rapid. The
effects of quinidine on the deletion mutant, rKv1.4
3-25, are shown
in figure 2A. Deleting amino acids 3 to
25 from the N-terminus disrupted the fast N-type inactivation process
(Tseng-Crank et al., 1993
). rKv1.4
3-25 decayed slowly
during depolarization, probably due to a slow C-type inactivation
process (Hoshi et al., 1991
). Quinidine slightly accelerated
the decay of rKv1.4
3-25. However, it was difficult to dissect out a
clear phase of block development. The current trace induced by the
first pulse after quinidine application was similar to that recorded
after repetitive pulses (upper panel of fig. 2A). This indicates that
quinidine blockade of rKv1.4
3-25 developed rapidly and reached a
steady-state during a 1-sec depolarization pulse. Unblock occurred
during the interpulse interval when the membrane was repolarized to
80 mV, and blockade redeveloped during the next depolarization pulse. This is consistent with the fast binding and unbinding kinetics of
quinidine described for the wild-type rKv1.4 channel (Yatani et
al., 1993
), and was confirmed in our single channel recordings of
rKv1.4
3-25 (data not shown). Quinidine slowed the decay of tail
current of rKv1.4
3-25, and induced a "cross-over" with the control tail current (data not shown). This is indicative of drug unblock upon repolarization prior to the closure of the activation gate
(Yeola et al., 1996
).

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Fig. 2.
Quinidine and 4AP suppressed rKv1.4 3-25 with
different time and voltage dependencies. A, Effects of quinidine (50 µM) on rKv1.4 3-25. Top, Quinidine slightly accelerated the decay
of rKv1.4 3-25 but there was no clear phase of block development.
Currents were recorded during 1-sec depolarization pulses from
Vh 80 mV to Vt +40 mV before and after drug
application. Bottom, Effect of quinidine on rKv1.4 3-25 was enhanced
by membrane depolarization. Drug effect was quantified by the ratio of
current amplitude recorded in the presence of quinidine to control
(Id/Ic, right ordinate). Currents were measured
at the end of 1-sec depolarization pulses from Vh 80 mV
to different test voltages applied once every 15 sec. Data were average
from three experiments. Data of Id/Ic were
compared with the activation curve of rKv1.4 3-25, that was
constructed in the following manner. In 98 mM [K]o, the
membrane was depolarized from Vh 80 mV to different
Vt (from 55 to +60 mV in 5 mV increments) for 100 msec,
followed by repolarization to 65 mV. Peak inward tail currents were
measured 2 msec after return to 65 mV, and then normalized to the
maximal tail current following Vt to +60 mV. The
relationship between Vt and the normalized tail current (as
an estimate of the fraction of channels activated at Vt,
right ordinate) was fit with a double Boltzmann function
|
(1)
|
where A1 and (1 A1) are
fractions of the two Boltzmann components, V1 and
V2 are the corresponding half-maximum activation voltages
and k1 and k2 are the slope factors. The curve
was calculated using equation (1) and mean parameter values averaged
from 11 experiments: A1 = 0.64 ± 0.02, V1 = 39.7 ± 2.0 mV, k1 = 4.3 ± 0.5 mV,
V2 = 6.7 ± 4.5 mV, k2 = 13.5 ± 1.1 mV. B, Effects of 4AP (0.5 mM) on rKv1.4 3-25. Top, 4AP
suppressed rKv1.4 3-25 during depolarization with a clear phase of
block development, and there was no unblock between depolarization
pulses. Currents were recorded during 1-sec depolarization pulses from
Vh 80 mV to Vt 20 mV under the control
conditions and during the first to third pulses (labeled 1, 2 and 3)
after 4AP application. Between the control and the first pulse after
4AP application, the cell was superfused with the 4AP-containing
solution for 5 min during which the membrane was held at 80 mV. The
interpulse interval in the presence of 4AP was 1 min. Bottom, Effect of
4AP on rKv1.4 3-25 was reduced by membrane depolarization. The drug
effect was quantified by the current ratio
(Id/Ic, left ordinate). Currents were measured
at the end of 5-sec depolarization pulses from Vh 80 mV
to different Vt applied once every 15 sec (control) or
every 60 sec (in the presence of 4AP). Data were average from three
experiments. Data of Id/Ic are superimposed on
the activation curve of rKv1.4 3-25 (right ordinate).
|
|
In the lower panel of figure 2A, the ratios of current amplitudes
measured at the end of 1-sec pulses in the presence of quinidine to
control (Id/Ic) are plotted against the test
pulse voltage. The suppressing effect of quinidine on rKv1.4
3-25
was enhanced by membrane depolarization. The voltage-dependence of drug
effect was analyzed using the Woodhull formalism and data points in the voltage range of +30 to +70 mV, when channel activation
approached a plateau (Woodhull, 1973
). The analysis suggests that the
quinidine binding site in rKv1.4
3-25 lies within the membrane
electrical field and has an equivalent electrical distance of 0.30 ± 0.01 from the intracellular surface of the membrane
(n = 10).
The effects of 4AP on the wild-type and the deletion mutant of rKv1.4
have been described previously (Yao and Tseng, 1994
). It was concluded
that 4AP blocks rKv1.4 from the intracellular side of the membrane and
binding is facilitated by channel activation. Figure 2B illustrates the
key features of 4AP actions on rKv1.4
3-25 to contrast them with
those of quinidine's actions. When the membrane was held at
80 mV
during wash-in of 4AP (0.5 mM) for 5 min, modest block developed as
suggested by the change in the peak current amplitude during the first
pulse after 4AP application. In contrast to the modest degree of block
that had developed at
80 mV for 5 min, marked block developed rapidly
during depolarization to
20 mV, as reflected by the accelerated decay
of rKv1.4
3-25 during the first pulse after 4AP application. The
apparent separation between channel activation and block development
indicates that the rate of 4AP blockade of rKv1.4
3-25 is slow
relative to the rate of channel activation. This is consistent with the
effects of 4AP on single channel currents of rKv1.4
3-25: 4AP does
not alter the single channel open time but shortens the burst duration (Yao and Tseng, 1994
). 4AP did not unblock from rKv1.4
3-25 during the interpulse interval when the membrane was repolarized to
80 mV,
as reflected by the marked reduction of peak current amplitudes during
the second and the third pulses after 4AP application. Therefore, data
in figure 2 indicate two differences between quinidine and 4AP in their
actions on rKv1.4
3-25: 1) the kinetics of drug-channel interaction
is much slower for 4AP than for quinidine and 2) upon repolarization
the bound 4AP molecule is trapped inside the channel by the closure of
the activation gate, although quinidine leaves the channel followed by
deactivation.
Another important difference between 4AP and quinidine is the
voltage-dependence of drug action. In contrast to quinidine, the
suppressing effect of 4AP on rKv1.4
3-25 was reduced by membrane depolarization in the voltage range from
40 to +60 mV (fig. 2B, lower
panel). One possible explanation for such a voltage-dependence is that,
although 4AP binding to rKv1.4
3-25 was facilitated by channel
activation, membrane depolarization actually induced 4AP unblock by
reducing the binding site affinity. This was tested by the experiments
shown in figure 3. In these experiments,
the membrane was held at
45 mV during wash-in of 4AP and during
interpulse intervals. This holding voltage was 5 to 10 mV above the
threshold of channel activation and therefore would allow 4AP binding
to occur (evidenced by a 4AP-induced reduction in the outward holding current level, data not shown). Under these conditions, currents induced by depolarization pulses in the presence of 4AP had completely different time courses than those shown in figure 2B: the initial current amplitude was small but the current level gradually increased during depolarization. Therefore, consistent with the prediction based
on figure 2B, a depolarization pulse could induce 4AP unblock if 4AP
blockade had already occurred. The rate and extent of 4AP unblock were
enhanced by stronger depolarization (fig. 3A). As shown in figure 3B,
the voltage-dependence of the rate and extent of 4AP unblock from
rKv1.4
3-25 tracked the voltage-dependence of channel activation,
suggesting that channel activation induced 4AP unblock.

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Fig. 3.
4AP dissociated from rKv1.4 3-25 in the open
state. A, Superimposed rKv1.4 3-25 current traces recorded during
2-sec depolarization pulses from Vh 45 to Vt
30 mV (left) or to +50 mV (right) before (control) and after 4AP (0.5 mM) application. The interpulse interval was 15 sec under the control
conditions and 60 sec in the presence of 4AP. B, Comparison of
voltage-dependence of rate and extent of 4AP unblock from
rKv1.4 3-25 and voltage-dependence of channel activation. The degree
of 4AP unblock was evaluated by the ratio
(Id/Ic, solid circles and left ordinate) of
currents measured at the end of 2-sec depolarization pulses from
Vh 45 mV to different Vt. The rate of 4AP
unblock was the reciprocal of time constant of single exponential fit
to the rising phase of current traces in the presence of 4AP (open
circles, right ordinate, n = 3). The activation curve
of rKv1.4 3-25 (fraction activated, left ordinate) was calculated as
described for figure 2.
|
|
Data presented in figure 3 support the notion that activation-induced
4AP unblock is an important factor in determining the voltage-dependence of 4AP action on rKv1.4
3-25 (fig. 2B). However, these data do not allow us to determine whether 4AP bound within the
channel could experience the membrane electrical field or not. We
addressed this issue by examining the effects of elevating [K]o on drug actions. Elevating [K]o will
impede drug binding by an electrostatic repulsion and reduce the
apparent blocking potency if: 1) the binding site is within the pore
and 2) drug binds in the positively charged form (as is the case for
quinidine binding to rKv1.4
3-25). This was verified by the
experiments shown in figure 4. On
average, elevating [K]o from 2 to 98 mM increased
quinidine's Kd value (at +40 mV) from
117.2 ± 27.3 µM (n = 15) to 663.1 ± 107.1 µM (n = 6), i.e., a 5.7-fold increase in
the Kd value (P < .001). In contrast,
elevating [K]o from 2 to 98 mM had much lesser effects on
the apparent blocking potency of 4AP on rKv1.4
3-25. This can be
seen from the similar degree of current reduction at the end of the
pulses shown in figure 5A. However,
elevating [K]o slowed the development of 4AP blockade. In
the experiment shown in figure 5A,
of 4AP block was 203 msec in 2 mM [K]o and 500 msec in 98 mM [K]o. The
apparent rate of 4AP block development (reciprocal of
of block) is
plotted against 4AP concentration in figure 5B. Linear regression was
used to estimate the apparent binding (Kon) and unbinding
(Koff) rate constants based on equation (3) (fig. 5,
legend). In 2 mM [K]o, Kon was 3.35 mM
1sec
1 and Koff was 3.65 sec
1. In 98 mM [K]o both rate constants
were reduced (Kon = 1.96 mM
1sec
1, Koff = 2.92 sec
1). The Kd value estimated from
Kon/Koff was 1.09 vs. 1.49 mM in 2 vs. 98 mM [K]o. Therefore, elevating
[K]o from 2 to 98 mM caused only a 50% increase in
4AP's Kd value. This is much less than the
5.7-fold increase in quinidine's Kd value
caused by the same degree of [K]o elevation. There are
two possible explanations for such a low [K]o sensitivity
in 4AP's blocking potency: 1) the 4AP binding site is outside the pore
or 2) 4AP's charge is not exposed once bound inside the channel.
Results from our mutagenesis experiments to be presented below can help
resolve this issue.

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Fig. 4.
Elevating [K]o from 2 to 98 mM reduced
the apparent potency of quinidine suppression of rKv1.4 3-25. A,
Superimposed current traces before and after quinidine (200 µM)
application in 2 (left) and 98 (right) mM [K]o. Currents
were recorded during 1-sec depolarization pulses from Vh
80 mV to Vt +80 mV. Data were obtained from the same
cell. B, Summary of quinidine's Kd values
measured in 2 and 98 mM [K]o, with numbers of
measurements in parentheses. The Kd values were
estimated using current ratio (Id/Ic) of
currents measured at the end of 1-sec depolarization pulses to +40 mV,
based on
|
(2)
|
|
|

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Fig. 5.
Elevating [K]o from 2 to 98 mM slowed
4AP suppression of rKv1.4 3-25 with little effects on the apparent
blocking potency. A, Superimposed current traces recorded under the
control conditions (thin traces) and during the first pulses after 4AP
(0.5 mM) application (open circles). Currents were recorded during
2-sec depolarization pulses from Vh 80 mV to
Vt 20. Between the "control" and "4AP" traces the
cell was superfused with the 4AP solution for 5 min while the membrane
was held at 80 mV. Currents recorded in 98 mM [K]o were
inward. The current traces are inverted to facilitate comparison with
current traces in 2 mM [K]o. The data points of open
circles are superimposed on curves calculated from a single exponential
function with best-fit time constants (203 and 500 msec in 2 and 98 mM
[K]o, respectively). B, Summary of the apparent rates of
4AP block development at different 4AP concentrations in 2 and 98 mM
[K]o. The reciprocal of of 4AP block development
(determined as described for A) is plotted against [4AP]. Each data
point was average from four to eight measurements. Linear regression
was applied to estimate the apparent 4AP binding (Kon) and
unbinding (Koff) rate constants according to
|
(3)
|
The superimposed lines were calculated from equation
(3) with best-fit parameter values: 2 mM [K]o,
Kon = 3.35 mM 1sec 1,
Koff = 3.65 sec 1; 98 mM [K]o,
Kon = 1.96 mM 1sec 1,
Koff = 2.92 sec 1.
|
|
The slow kinetics of 4AP binding and unbinding suggest that
drug-channel interaction may not be a simple, diffusion-limited process. Instead, 4AP binding and unbinding may involve or require conformational changes in the channel protein. If this is the case, the
kinetics of 4AP actions should display a temperature-sensitivity higher
than that of a diffusion-limited event (Hille, 1992
). This was tested
in the experiments shown in figure 6. The
time constants of 4AP blockade were estimated by fitting a single
exponential function to the decay phase of current traces induced by
the first pulses after 4AP application at Vh
80 mV (fig.
6A, left panels). Elevating the bath temperature from 23 to 35°C
markedly shortened
of block development (241.3 ± 20.5 vs. 80.2 ± 7.3 msec at 23 and 35°C, fig. 6A, right
panel). This difference in the rate of 4AP block had a Q10
of 2.5. The
values of 4AP unblock were estimated by fitting a
single exponential function to the rising phase of current traces
induced by the first pulse after 4AP application at Vh
45
mV (fig. 6B, left panels). The average
of 4AP unblock was
489.3 ± 37.0 vs. 187.8 ± 17.0 msec at 23 vs. 35°C (Q10 = 2.2, fig. 6B, right panel).
Therefore, the Q10 values of 4AP block and unblock are
higher than the expected value of diffusion-limited events
(Q10
1.5), but are similar to the reported values of Q10 for channel gating processes (Hille, 1992
). This
supports the notion that 4AP interaction with rKv1.4
3-25 involves
or requires conformational changes in the channel protein.

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Fig. 6.
Temperature-sensitivity of kinetics of interactions
between 4AP and rKv1.4 3-25. A, Rates of 4AP (0.5 mM) blockade at 23 and 35°C. Left, Superimposed current traces recorded during 1-sec
depolarization pulses from Vh 80 mV to Vt
20 mV before (thin traces) and during the first pulses after 4AP
application (open circles). 4AP was applied for 5 min during which the
membrane was held at 80 mV before the first pulses were applied. The
data points of open circles are superimposed on curves calculated from
a single exponential function with best-fit time constants (254 msec at
23°C and 89 msec at 35°C). Right, Summary of of 4AP block
development at 23 and 35°C. The voltage clamp protocol and data
analysis were as described for the left panel. Numbers in parentheses
are numbers of measurements. The estimated Q10 value for
the rate of 4AP blockade is 2.5. B, Rate of 4AP unblock from
rKv1.4 3-25 at 23°C and 35°C. Left, Superimposed current traces
recorded during 2-sec depolarization pulses from Vh 45 to
Vt 20 mV before (thin traces) and during the first pulses
after 4AP (0.5 mM) application (open circles). 4AP was applied for 5 min during which the membrane was held at 45 mV before the first
pulses were applied. The data points of open circles are superimposed
on curves calculated from a single exponential function with best-fit
time constants (512 msec at 23°C and 177 msec at 35°C). Right,
Summary of of 4AP unblock at 23 and 35°C. The voltage clamp
protocol and data analysis were as described for the left panel.
Q10 of 4AP unblock is 2.2.
|
|
The above data indicate that although both quinidine and 4AP bind to
rKv1.4
3-25 from inside the cell membrane and binding is facilitated
by channel activation, the kinetics and voltage-dependence of
drug-channel interaction are distinctly different. The differential effects of elevating [K]o on the blocking potency of
quinidine and 4AP suggest that these two blockers experience different
degrees of electrostatic effects of K ions from the opposite end of the pore. We then examined whether the binding sites of quinidine and 4AP
in rKv1.4
3-25 overlap and what controls the affinity of their
binding sites. Our focus was on the S6 domain and in particular,
threonine at position 529 (T529).
Effects of T529 Mutations on the Blocking Potency of Quinidine and
4AP
T529 was mutated to 13 other residues. Five of them (T529D, T529K,
T529Q, T529N and T529Y) did not produce currents. Currents through a
sixth mutant, T529W, were very small. The remaining seven mutants
(T529G, T529S, T529A, T529V, T529I, T529L and T529F) produced robust
currents and were used to test the effects of T529 mutations on drug
binding.
The effects of quinidine on WT (=rKv1.4
3-25) and T529 mutant
channels were quantified by Kd values at +40 mV.
At this voltage, the degrees of channel activation reached or
approached a plateau in all cases, avoiding possible alterations in the
apparent blocking potency among channels introduced by different
degrees of channel activation. Figure 7
illustrates current traces of WT and T529 mutants recorded during 1-sec
depolarization pulses to +40 mV before and after quinidine (100 µM)
application. Quinidine reduced current amplitudes in all cases. There
was no clear phase of block development in any of the channels.
Quinidine's effects approached a steady-state at the end of the 1-sec
pulses. The current ratios (Id/Ic) measured at
the end of the pulses were used to construct concentration-response
relationships.

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Fig. 7.
Effects of 100 µM quinidine on rKv1.4 3-25 (WT)
and mutants in which threonine at position 529 was replaced by
different residues. The mutants were designated as T529X, with X = substituting residue using the one-letter code. Currents were recorded
during 1-sec depolarization pulses from Vh 80 mV to
Vt +40 mV applied once every 15 sec.
|
|
Figure 8 shows the mean values of
Id/Ic plotted against the quinidine
concentration for WT and T529 mutant channels. The data points are
superimposed on curves calculated from equation (2) with mean
Kd values averaged from 4 to 11 measurements
each (listed in fig. 11 legend). Replacing T529 with phenylalanine
(T529F) reduced quinidine's blocking potency, although all the other
mutant channels displayed a higher sensitivity to quinidine compared to
that of the WT channel.

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Fig. 8.
Concentration-response relationships of quinidine
suppression of rKv1.4 3-25 (WT) and T529 mutants. Each cell was
exposed to increasing concentrations of quinidine (from 5 to 1000 or
2000 µM) and the current amplitude was monitored by 1-sec
depolarization pulses from Vh 80 mV to Vt +40
mV applied once every 15 sec. The relationship between current ratio
(Id/Ic) and [quinidine] was fit with equation
(2) to estimate the Kd value. Shown are data
points (mean values from 4 to 11 measurements, S.E. bars omitted for
the sake of clarity) superimposed on curves calculated from equation
(2) with mean Kd values listed in figure 11
legend.
|
|
The Kd values of 4AP were determined using the
voltage clamp protocol illustrated in figure
9 (except for T529L and T529I): the
current amplitude was monitored by 40-msec depolarization pulses from
Vh
80 mV to Vt
20 mV applied once every 15 or 30 sec. The cell was exposed to increasing concentrations of 4AP and
the current ratio (Id/Ic) measured at the
steady-state of 4AP's effect at each concentration was used to
construct the concentration-response relationship. The rationale for
this voltage clamp protocol is the following. 4AP's blocking potency
is reduced by membrane depolarization due to blocker dissociation from
an activated channel (figs. 2B and 3). Because T529 mutations alter the
voltage-dependence of channel activation (authors' unpublished data),
we needed to avoid the interference from differences in the degree of
channel activation when measuring 4AP's blocking potency. Therefore,
short (40 msec) depolarization pulses to a low voltage (
20 mV) were
used to monitor the progression of drug effects without inducing
significant 4AP dissociation. Because once bound 4AP molecules were
trapped inside the channel by the closure of the activation gate at
Vh (
80 mV), the degree of 4AP blockade would accumulate
over a train of such short pulses. Figure 9 shows that, under the
conditions described above, 4AP blocked the WT channel with a
Kd of 126 µM.

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Fig. 9.
Concentration-response relationship for 4AP
suppression of rKv1.4 3-25 (WT). The main plot illustrates the time
course of changes in current ratio (Id/Ic) when
the cell was exposed to increasing concentrations of 4AP (in µM,
marked on top). The current amplitudes were monitored by 40-msec
depolarization pulses from Vh 80 mV to Vt
20 mV applied once every 30 sec. Inset on right, Superimposed
original current traces recorded before 4AP application and at the
steady-state of 4AP effect (concentrations marked to the right). Inset
on left, Concentration-response relationship
(Id/Ic vs. [4AP]) from the same
experiment. The superimposed curve was calculated from equation (2)
with Kd = 126 µM.
|
|
Data from representative experiments on T529F and T529L are shown in
figure 10. 4AP blocked T529F with a
much higher potency (Kd = 14.3 µM) than its
effect on the WT channel. As for the WT channel, the 4AP's effect on
T529F was partially reversible after washing out of 4AP. In contrast,
T529L was insensitive to 1 or 2 mM 4AP. In the experiment shown in
figure 10B, the current amplitude was even slightly increased in 10 mM
4AP. Elevating the 4AP concentration to 20, 50 and 100 mM caused a
rapid reduction in the current amplitude and, at 100 mM 4AP, this was
followed by a secondary decrease in current amplitude along with an
increase in the membrane "leak" conductance. Washing out 4AP caused
a rapid but incomplete reversal of blocker effects. The low 4AP
sensitivity of T529L made it difficult to construct a complete
concentration-response relationship. The secondary reduction in current
amplitude seen in high 4AP concentrations might be due to effects
unrelated to pore blockade. Therefore, the Kd
value for T529L was estimated from the initial current ratio in the
presence of 100 mM 4AP (arrow in fig. 10B) by equation (2). For T529I
that also had a low sensitivity to 4AP, the Kd value was similarly estimated by current ratio in 10 mM 4AP.

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Fig. 10.
Comparison of effects of 4AP on T529F (A) and T529L
(B). Each panel shows the time course of changes in current ratio
(Id/Ic) when the cell was exposed to increasing
concentrations of 4AP (marked on top) and after washout. The current
amplitudes were monitored using the same voltage clamp protocol as
described for figure 9. Insets, Superimposed current traces recorded
before and after 4AP application (concentrations marked to the right).
The concentration-response relationship of 4AP's effect on T529F was
fit with equation (2) to estimate Kd (14.3 µM). The initial Id/Ic value of T529L in the
presence of 100 mM 4AP (arrow) was used to calculate
Kd from equation (2) (Kd = 67 mM).
|
|
Figure 11 shows a summary of
Kd values of quinidine and 4AP in blocking the
WT and T529 mutant channels. The Kd values are listed in figure 11 legend. For T529G, T529S, T529V, T529I and T529L,
the quinidine's Kd values were reduced
(blocking potency enhanced) while the 4AP's Kd
values were increased relative to those of the WT channel. T529F had
the opposite effects: quinidine's Kd value was
increased while 4AP's Kd value was reduced.
Finally, for T529A the Kd values of both
quinidine and 4AP were reduced.

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Fig. 11.
Comparison of effects of T529 mutations on the
blocking potency of quinidine and 4AP. The voltage clamp protocols and
methods of Kd estimation were as described in
figures 7 to 10. The Kd values of quinidine
(left ordinate) and those of 4AP (right ordinate) are plotted on a
logarithmic scale against channel types along the abscissa (WT = rKv1.4 3-25). The following are the Kd values
(n = number of measurements):
|
|
Quinidine (µM) |
n |
4AP
(µM) |
n |
|
| WT |
63.2
± 5.4 |
10 |
124.2 ± 6.7 |
3
|
| T529G |
6.9 ± 0.9a |
6 |
192.1 ± 27.9 |
5
|
| T529S |
31.6 ± 6.4a |
10 |
311.9 ± 86.9 |
4
|
| T529A |
20.4 ± 3.4a |
8 |
33.2
± 7.5a |
3 |
| T529V |
13.0
± 3.8a |
4 |
195.6 ± 41.5 |
6 |
| T529I |
12.3
± 3.4a |
6 |
10000 |
1
|
| T529L |
18.6 ± 3.1a |
6 |
190000
± 64799a |
5 |
| T529F |
479.6
± 109.8a |
5 |
18.4 ± 1.9a |
6 |
|
|
a
P < .05 vs. WT.
|
|
|
Data in figure 11 indicate that position 529 is an important
determinant of blocking potency of both quinidine and 4AP. This, in
turn, suggests that the binding sites of quinidine and 4AP in rKv1.4 at
least partially overlap with each other. Replacing T529 with G, S, V,
I, L and F had opposite effects on quinidine and 4AP binding,
indicating that different factors are involved in determining the
binding sites' affinity for the two blockers.
Correlating Effects of T529 Mutations on Quinidine and 4AP Blocking
Potency with Side Chain Properties or with Changes in Channel Gating
Factors affecting quinidine's binding affinity.
To elucidate
the factors involved in determining the effects of T529 mutations on
quinidine binding, we tried to correlate changes in quinidine's
blocking potency with side chain properties at position 529. Two
factors were considered: side chain polarity and residue volume (fig.
12). It has been suggested, based on a limited mutagenesis study of quinidine's effect on hKv1.5, that the
primary factor in determining drug binding affinity is the hydrophobicity of side chain at position 505 (equivalent to 529 of
rKv1.4) (Yeola et al., 1996
). However, when examined with
more extensive mutations and with the side chain hydrophobicity
evaluated quantitatively, we could not identify a clear correlation
between quinidine's Kd value and side chain
polarity at 529. This is shown in figure 12A: the
Kd values of quinidine are plotted on a
logarithmic scale against 529 side chain polarity. The side chain
polarity was estimated by the free energy (kcal/mol) needed to transfer the side chain from an aqueous phase to octanol (Guy, 1985
).

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Fig. 12.
Correlating side chain properties of residues at
position 529 with quinidine's blocking potency. Quinidine's
Kd values from figure 11 are plotted on a
logarithmic scale against 529 side chain polarity [(Guy, 1985 ) with
the direction of increasing hydrophobicity or increasing hydrophilicity
marked] (A) or 529 residue volume (Zamyatnin, 1972 ) (B). The line in B
was a linear regression of data points from WT, T529G, T529S, T529A and
T529F.
|
|
Quinidine is a bulky molecule and steric hindrance can be an important
factor in affecting its ability to bind to the narrow part of the inner
vestibule. As discussed previously, position 529 may be situated in the
intersection between the narrow part of the pore and the opening into
the wide inner vestibule. This is supported by a mutagenesis study of
the 529 equivalent in the Shaker channel (T469): a cysteine residue
introduced into this position (T469C) is not accessible to
intracellular thiol-modifying MTS reagents, although a cysteine at the
immediate downstream position (I470C) is accessible (Liu et
al., 1997
). One possible explanation for this difference in
accessibility is steric hindrance for MTS reagents to approach position
469 in the Shaker channel. Quinidine's Kd
values are plotted against the estimated residue volume at position 529 (Zamyatnin, 1972
). The Kd value was the highest
(lowest quinidine blocking potency) when position 529 was occupied by
the bulkiest residue examined here (T529F). The Kd value was the lowest when 529 was occupied by
glycine (T529G) that does not have a side chain. The
Kd values for WT, T529S, and T529A fell between
these two extremes, and these three data points along with those of
T529G and T529F could be described by a linear relationship between
log(Kd) and residue volumes at 529. However,
when 529 was occupied by a highly hydrophobic residue (V, I or L), the
Kd value was lower (blocking potency higher) than that expected based on the linear relationship between
log(Kd) and residue volume. Therefore, quinidine
binding to rKv1.4 is favored by a hydrophobic residue at position 529. However, steric hindrance seems to be a more important factor in
determining quinidine's blocking potency. Therefore, although
phenylalanine in T529F is the most hydrophobic residue among the
residues examined (fig. 12A), it conferred the lowest sensitivity to
quinidine due to its bulky side chain (fig. 12B). Along with a decrease
in the blocking potency, the voltage-sensitivity of quinidine binding
to T529F was reduced: the equivalent electrical distance was 0.30 ± 0.01 for WT (n = 10) but 0.12 ± 0.04 for
T529F (n = 7, P < .05). This is consistent with
the notion that the bulky side chain of T529F prevented quinidine from
penetrating deep into the pore.
Factors affecting 4AP's binding affinity.
Plotting 4AP's
Kd value against the side chain polarity or
residue volume at position 529 did not reveal any clear pattern (data
not shown). Therefore we needed to consider other factor(s) that might
affect 4AP binding. It has been shown for 4AP's effects on chimeric
channels of Kv2.1 and Kv3.1 that there is an empirical linear
relationship between 4AP's Kd value and the
rate of channel deactivation: a slower deactivation is coupled with a
lower 4AP sensitivity (Shieh and Kirsch, 1994
). A slower rate of
deactivation reflects a longer dwell time in the open state. The above
relationship therefore is consistent with the notion that 4AP tends to
dissociate from channels in the open state that have a low binding
affinity. We tested whether a relationship between 4AP's
Kd value and the rate of channel deactivation
could be identified among WT and T529 mutant channels.
Relative to the WT channel, the activation curves of the mutant
channels (except T529S) were shifted in the hyperpolarizing direction
by different degrees (authors' unpublished data). This shift in the
voltage-dependence of channel activation was accompanied by a slowing
of channel deactivation. Figure 13A
compares tail current kinetics between WT and T529 mutant channels. The
mean values of
of deactivation are listed in figure 13 legend.
Replacing T529 by G, A, V, I, L or F slowed the deactivation rate. In
figure 13B, the 4AP's Kd values are plotted
against
of deactivation on a double logarithmic scale. When
position 529 was occupied by a hydrophobic residue (T529F, T529A,
T529V, T529L and T529I), a larger value of
of deactivation is
accompanied by a higher Kd value. Therefore,
indeed there is a correlation between the apparent 4AP binding affinity
and the rate of channel deactivation. However, when 529 was occupied by
a hydrophilic residue (WT and T529S) or by glycine that does not have a
side chain (T529G), 4AP's Kd value was higher
than that expected based on the other data points. This suggests that a
hydrophobic residue at 529 is still a contributing factor in
stabilizing 4AP binding. Removing this factor destabilized 4AP binding
even though the open state is short-lived (short
of deactivation).

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Fig. 13.
A, Effects of T529 mutations on the rate of
deactivation at 80 mV. Recordings were made in 98 mM
[K]o using the voltage clamp protocol shown on top left:
the membrane was depolarized to +60 mV for 100 msec followed by
repolarization to 80 mV. Inward tail currents at 80 mV are shown.
In each panel, the tail current from one of the T529 mutants (depicted
by the thick trace) is superimposed on the WT tail current (thin
trace). To facilitate comparison, the gain of display is adjusted so
that the tail current amplitudes match each other. Note the differences
in the time calibration. B, Correlating effects of T529 mutations on
4AP's blocking potency with effects on the rate of deactivation.
4AP's Kd values from figure 11 are plotted
against of deactivation at 80 mV on a double logarithmic scale.
The dotted lines are drawn by eye. The following are values of of
deactivation (in msec, numbers of measurements in parentheses):
|
| WT |
5.7 ± 1.1 |
(4) |
| T529G |
7.1
± 0.9 |
(3) |
| T529S |
3.8 ± 0.6 |
(6) |
| T529A |
21.3
± 1.7a |
(7) |
| T529V |
70.0 ± 7.9a |
(7)
|
| T529I |
300.0 ± 52.8a |
(5) |
| T529L |
403.2
± 135.3a |
(3) |
| T529F |
12.1 ± 3.5 |
(3) |
|
|
a
P < .05.
|
|
|
 |
Discussion |
Our data suggest that both quinidine and 4AP can bind deep in the
pore, and position 529 in the middle of the S6 domain is an important
determinant for their binding affinity. This may be somewhat surprising
for 4AP, for which a more superficial binding site has been assigned
based on mutagenesis work on chimeric channels of Kv2.1 and Kv3.1
(Durell and Guy, 1996
; Shieh and Kirsch, 1994
). In our study, replacing
T529 with leucine practically abolished the 4AP sensitivity. Such a
dramatic effect argues that T529 indeed directly interacts with 4AP.
Does residue at position 529 face the lumen of the pore?
It
has been shown that the S6 segments of Na, Ca and K channels can play
important roles in channel gating (Hoshi et al., 1991
;
Zuhlke et al., 1994
; Zhang et al., 1994
; McPhee
et al., 1995
). This suggests that the S6 segments do not
simply serve a "packing" function in stabilizing the protein
structure, but can actively engage in conformational changes in the
channel gating processes. Our data from T529 mutations are consistent
with such a role of the S6 segment in rKv1.4 (authors' unpublished
data).
Replacing T529 with positively or negatively charged residues (T529K
and T529D), highly hydrophilic residues (T529Q and T529N), or bulky
residues (T529Y and T529W) reduces or abolishes current expression.
These observations suggest that position 529 may participate in
interactions with residues from other transmembrane
-helices of the
channel, and thus cannot tolerate charged, highly hydrophilic or very
bulky residues here (Durell and Guy, 1996
; Guy, 1985
). However,
replacing T529 with glycine that does not have a side chain (T529G), a
similar residue (T529S) or more hydrophobic residues (T529A, T529V,
T529I, T529L and T529F) leads to robust current expression. When a
hydrophobic residue occupies position 529, there is a negative shift in
the voltage-dependence of channel activation and a slowing of
deactivation. The degree of slowing in the deactivation rate correlates
with the degree of increase in side chain hydrophobicity at 529 (authors' unpublished data). This correlation suggests that the open
state of rKv1.4 is stabilized by a hydrophobic residue at position 529, possibly because this residue interacts with hydrophobic residues in
other transmembrane
-helices when channel opens. The implication
then is that the residue at 529 may face away from the lumen in the
open state. If this is the case, hydrophobic interactions between pore
blockers and residues 529 proposed here [and suggested by others
studying the Shaker and hKv1.5 channels (Yeola et al., 1996
;
Baukrowitz and Yellen, 1996
)] may involve an intercalation of the
hydrophobic moiety of a drug molecule into the protein interior.
Steric hindrance influences quinidine, but not 4AP, binding.
For a bulky molecule like quinidine, steric hindrance is an important
factor in determining the apparent binding affinity. It is possible
that quinidine binds to the narrow part of the inner vestibule between
T529 and the ion selectivity filter (fig. 1) and causes a deformation
of this part of the pore. Mutations that reduce side chain volume here
can relieve the steric constraint and stabilize quinidine binding. This
is supported by data presented here (fig. 12). Furthermore, we have
shown that mutating the threonine at position 501 [in the middle of
the P-region and adjacent to the ion selectivity filter (Durell and
Guy, 1996
)] to serine and thus reducing side chain volume enhances
quinidine binding (Kd at +40 mV: 63.2 ± 5.4 to 29.2 ± 3.4 µM, P < .05) (Zhang et al., 1995
). The mechanism is probably also a relief of steric constraint around the quinidine binding site.
The bulky size of the quinidine molecule may explain the phenomenon of
"cross-over" of tail currents: the size of quinidine does not allow
the activation gate to close when quinidine is within the pore.
Therefore when the membrane is repolarized, quinidine needs to leave
the channel before the activation gate can close ("foot-in-the-door" behavior). However, 4AP is a much smaller molecule and can stay inside the inner vestibule when the activation gate is closed. A similar phenomenon has been described recently for
the Shaker channel. The wild-type Shaker channel can not trap QA
blockers (e.g., TEA or decyltriethylammonium) within the
inner vestibule when the activation gate is closed. However, mutating the residue at position 470 (immediate downstream from the Shaker equivalent of 529) from isoleucine to cysteine and thus reducing the
side chain volume here allows QA blockers to be trapped by the closure
of the activation gate (Holmgren et al., 1997
). Furthermore, the QA-bound I470C channel can still gate similar to a blocker-free channel, reflecting that a QA molecule trapped within the inner vestibule does not compromise the opening and closing of the activation gate. These observations indicate that the inner vestibule of a
channel's pore does not collapse when the channel is in the closed
state. Instead, there remains a space that can accommodate a blocker
molecule such as tetraethylammonium or decyltriethylammonium in the
Shaker I470C mutant channel or 4AP in rKv1.4 and other K channels.
Channel activation increases the accessibility but reduces the
affinity of 4AP binding site.
Our data suggest that activation of
the rKv1.4
3-25 channel has two effects on 4AP binding: increasing
the accessibility of the binding site (fig. 2B) and reducing the
binding site affinity (fig. 2B and 3). The correlation between 4AP's
Kd value and
of deactivation shown in figure
13B lends further support to the latter contention. Therefore, 4AP
binding is hindered when the rKv1.4
3-25 channel is fully-closed or
when the channel is fully-open, and optimal 4AP binding probably occurs
in a "transitional" state between these two extremes.
S6 as an important determinant of drug binding to voltage-gated ion
channels.
Our data are consistent with a common theme of
drug-channel interactions that has emerged from studies of drug binding
to Na, Ca and K channels: the S6 segment plays an important role in
drug binding, and hydrophobic interactions between drug molecules and
S6 residues stabilize drug binding (Baukrowitz and Yellen, 1996
;
Hockerman et al., 1995
; Ragsdale et al., 1996
).
Furthermore, our data show that T529 in rKv1.4 plays a key role in
determining the binding affinity of pore blockers. This is similar to
the situation in the Shaker (Baukrowitz and Yellen, 1996
) and hKv1.5 (Yeola et al., 1996
) channels.
A possible scenario of drug-channel interaction is the following. The
hydrophobic domains of quinidine (quinoline) and 4AP (pyridine) anchor
the blocker molecules inside the pores. For quinidine, the bulky
quinuclidine moiety plugs the pore, while its protonated (positively
charged) tertiary amine is capable of sensing an electrostatic
repulsion by K ions from the other end of the pore. It is not clear
whether 4AP physically plugs the pore by its tertiary amine, or
occludes the pore by stabilizing the channel in a closed state. Several
observations suggest that the latter may be more likely. First, our
data suggest that optimal 4AP binding may occur in a "transitional"
state between fully-closed and fully-open states. Second, the
temperature sensitivity of rates of 4AP binding and unbinding
(Q10 = 2.2 to 2.5) suggests that 4AP's actions may involve
or require conformational changes of the channel protein (Hille, 1992
).
Third, gating current measurements indicate that 4AP suppresses a
component of the "ON" gating current that may be directly involved
in the process of pore opening (McCormack et al., 1994
).
Therefore, 4AP may hinder charge movements and prevent pore opening by
binding to a transitional state. On the other hand, quinidine as a
simple pore blocker does not affect the "ON" gating current
(although the "OFF" gating current kinetics is slowed due to the
"foot-in-the-door" phenomenon) (Fedida, 1997
). Fourth, 4AP's
blocking potency was little affected by electrostatic repulsion by K
ions from the other end of the pore, suggesting that the tertiary amine
of 4AP may not be exposed. The major effect of elevating
[K]o was a slowing of the apparent rates of 4AP binding and unbinding. This may be secondary to a stabilizing effect of external K ions on the open state of the channel (Pardo et
al., 1992
), that hinders 4AP binding to a transitional state.
The difference between quinidine and 4AP in their interaction with
rKv1.4 can be better described by the following schemes. Quinidine is a
classical open-channel blocker that blocks and unblocks in the open
state. Quinidine binding prevents the closure of the activation gate
(scheme 1):
where C, C*, O and OB denote closed, transitional, open and
open/blocked states, respectively. 4AP preferentially binds to rKv1.4
in the transitional state. 4AP binding prevents channel from opening,
but does not affect the closure of the activation gate. Scheme 2 can be
applied to 4AP-rKv1.4 interaction, with C*B denotes the
transitional/blocked state:
In conclusion, our data suggest that the binding sites for quinidine
and 4AP in rKv1.4 overlap with each other. For both, hydrophobic
interactions between blocker molecules and a residue in the S6 domain
(position 529) stabilize drug binding. In addition, quinidine binding
may be limited by steric constraints due to the bulky size of the
molecule, while 4AP binding depends on the gating state of the channel
with optimal binding occurring in a transitional state between the
fully-closed and fully-open states. Because the channel structure and
especially the amino acid sequences of the S6 domains are well
conserved in many voltage-gated K channels, our results may be
applicable to understanding the structural determinants of quinidine
and 4AP binding to other voltage-gated K channels.
Accepted for publication April 30, 1998.
Received for publication December 9, 1997.