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The Rammelkamp Center, MetroHealth System, Cleveland, Ohio 44109 (A.E.L. and M.-L.R.), Nippon Hoechst Marion Roussel, Tokyo 107, Japan (E.W.L.), and Hoechst Marion Roussel, Inc., Cincinnati, Ohio 45215 (D.R.)
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Summary |
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The use of nonsedating antihistamines may, on rare occasions, be
associated with cardiac arrhythmias. This could be due to blockade of
voltage-dependent K+ channels in the heart, leading to a
prolongation in repolarization in the human myocardium. For this
reason, we examined the effects of the nonsedating antihistamine
loratadine on a rapidly activating delayed-rectifier K+
channel (Kv1.5) cloned from human heart and stably expressed in HEK 293 cells or mouse Ltk
cells. Using patch-clamp
electrophysiology, we found that loratadine blocked Kv1.5 current
measured from inside-out membrane patches at concentrations of
100
nM, resulting in an IC50 value of 808 nM at +50 mV. The drug enhanced the rate of Kv1.5 current
decay, and block was enhanced at membrane potentials near threshold
relative to higher potentials. Loratadine did not alter the kinetics of Kv1.5 current activation or deactivation. Unitary Kv1.5 currents were
recorded in cell-attached patches. At the single-channel level, the
main effect of loratadine was to reduce the mean probability of opening
of Kv1.5. This effect of loratadine was achieved by a reduced number of
openings in bursts and burst duration. Finally, loratadine (10 µM) failed to inhibit HERG K+ channel
currents expressed in Xenopus laevis oocytes. It is
concluded that loratadine is an effective blocker of Kv1.5 that
interacts with an activated state or states of the channel. This
interaction suggests a potential for loratadine to alter cardiac
excitability in vivo.
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Introduction |
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Voltage-dependent K+ channels play an important role in determining the length of the cardiac action potential. Many different types of K+ channels exist in the human myocardium and contribute to its electrical activity (1, 2). Recent advances in molecular biology have led to the cloning of a variety of cardiac K+ channel cDNAs. For example, the rapid component of the delayed-rectifier K+ current is thought to be subserved by the protein encoded by HERG (3). A number of voltage-dependent K+ channels belonging to the Shaker superfamily have also been cloned from the heart (4, 5). One of these Shaker channels, Kv1.5, is thought to underlie the ultrarapidly activating delayed-rectifier K+ current found in human atrial myocytes (6, 7). In addition, both Kv1.5 transcripts (6) and Kv1.5 protein (8) have been detected in human ventricular tissue, in which they may form heteromultimeric K+ channels in combination with other Shaker-like subunits (8).
Pharmacological blockade of voltage-dependent K+ channels in the heart can be associated with untoward cardiac toxicity. Such an activity may underlie the prolongation in cardiac repolarization, which has been observed with the nonsedating antihistamines terfenadine (Seldane) and astemizole (Hismanal). Under certain clinical settings, such as cases of overdose, both terfenadine and astemizole may be associated with a prolongation of the QT interval, sometimes leading to the ventricular arrhythmia torsades de pointes (9, 10). In vitro, both terfenadine and astemizole have been shown to block cardiac K+ channel currents, including Kv1.5 (11-14). Another nonsedating antihistamine, loratadine (Claritin), is clinically available. Although loratadine is generally believed not to cause cardiac arrhythmias (15), reports of such arrhythmias have recently begun to appear (16, 17). To date, little is known about the interaction of loratadine with human cardiac K+ channels; therefore, the current study was undertaken to detail the effects of loratadine on the cloned human cardiac K+ channel Kv1.5.
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Materials and Methods |
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Cell culture.
The HEK 293 and mouse Ltk
cell
lines (American Type Culture Collection, Rockville, MD) were
transfected with the human cardiac Kv1.5 K+ channel
complementary DNA as previously described (6). Cells were grown in
Dulbecco's modified Eagle's medium supplemented with 10% fetal
bovine serum (GIBCO BRL, Grand Island, NY) in an atmosphere of 95%
air/5% CO2. This media also contained
penicillin/streptomycin/fungizone and G418 (0.5 mg/ml, GIBCO BRL).
Electrophysiology.
For whole-cell and cell-free inside-out
macropatch recordings (18), HEK 293 cells were seeded onto glass
coverslips 24-72 hr before use. Electrodes (1.5-3-M
resistance)
were fashioned from TW150 glass capillary tubes (World Precision
Instruments, New Haven, CT). For inside-out patches, the electrodes
were filled with a solution containing 130 mM NaCl, 5.0 mM KCl, 2.8 mM sodium acetate, 1.0 mM MgCl2, 10 mM HEPES, 10 mM glucose, and 1.0 mM CaCl2, pH
7.4, with 1 N NaOH. This solution served as the external solution for whole-cell recordings. The external recording solution used for inside-out patches contained 120 mM potassium
aspartate, 20 mM KCl, 4.0 mM Na2ATP, 5.0 mM HEPES, and 1.0 mM MgCl2, pH 7.2, with KOH. This served as the internal solution for whole-cell experiments. Currents were recorded at room temperature using an
Axopatch-1 D amplifier (Axon Instruments, Burlingame, CA) and were
conditioned by a four-pole low-pass filter with a cutoff frequency of
500 Hz. Currents were stored and analyzed using a Compaq Deskpro
computer and pCLAMP software (Axon Instruments). Linear leakage and
capacity currents were corrected on-line by using the P/4 subtraction
method unless stated otherwise. For steady state inactivation curves,
peak currents were normalized to the first pulse in each series and fit
to the Boltzmann equation 1 + exp[(V0.5
V)/k]
1, where V is the membrane voltage,
V0.5 is the midpotential of the curve, and k is
the slope factor. The IC50 value of loratadine was obtained
by nonlinear least-squares fit of the data (GraphPAD Software, San
Diego, CA). To obtain the apparent association and dissociation rates
of loratadine, we plotted the fast, drug-induced time constants
(
drug) versus drug concentration, [D], according to
the equation 1/
drug = k[D] + L, where
k and L are the apparent association and dissociation
constants, respectively.
cells were seeded onto
glass coverslips 24-48 hr before use, and the cell-attached mode of
the patch-clamp technique (18) was used to record unitary Kv1.5 channel
currents. Pipettes were fashioned from 7052 glass, and the tips were
coated with Sylgard 184 (Dow Corning, Midland, MI) and fire-polished
before use. The bath solution consisted of 140 mM potassium
aspartate, 5 mM EGTA, 10 mM HEPES, 1.0 mM MgCl2, and 10 mM glucose; pH 7.4 with KOH. Pipettes were filled with 137 mM NaCl, 5.4 mM KCl, 1.0 mM MgCl2, 1.8 mM CaCl2, 5 mM HEPES, and 10 mM glucose, pH 7.4 with NaOH. An Axopatch 200A and pCLAMP
software (Axon Instruments) were used for recording unitary current
from cell-attached patches. Data were analog-filtered with an
eight-pole low-pass Bessel response filter at one fifth the sampling
frequency and subsequently digitally filtered to a final cutoff
frequency of 1000 Hz. Single-channel currents were corrected for leak
and capacity currents by subtracting the average of records with no
openings from each record in an experiment and idealized with the
TRANSIT algorithm (19). Parameter estimates for single-channel
probability distributions were obtained with the maximum likelihood
method. For burst analysis, we used a critical closed criterion that
results in equal proportions of misclassified short and long dwell
times (20). This condition is satisfied for values of
crit that satisfy the relation
exp(
crit/
f) = 1
exp(
crit/
s), where
f and
s are the time constants for fast and slow components,
respectively, of the closed time distribution. The probability of
observing a dwell time from the long closed dwell time component with
duration of 
crit is 1
exp(
crit/
s), and the probability for
observing a dwell time from the short closed dwell time component
longer than
crit is
exp(
crit/
f). The value of
crit is obtained by using a modified Newton-Raphson root
search algorithm implemented in Turbo Pascal to numerically solve for
the value (
crit) that satisfies this equation. In two of
three patches, a very rapid closed time component with time constant of
<350 µsec was detected. These events are poorly resolved at the
filter frequency (1 kHz) used for analysis and were not further
analyzed. Values for
crit used to define bursts in data from three patches presented in the study were (control/loratadine) 2.665/6.449, 6.263/7.132, and 3.118/3.187 msec.
For oocyte recordings, the cRNA encoding the HERG K+
channel was microinjected into Xenopus laevis oocytes as
previously described (14). Whole-cell currents were recorded from
X. laevis oocytes by use of the conventional
two-microelectrode voltage-clamp technique. Beveled microelectrodes
were filled with a solution of 3 mol/liter KCl, 10 mmol/liter HEPES,
and 10 mmol/liter EGTA, pH 7.4 (Tris), to give a low tip resistance of
0.2 to 0.5 M
. Oocytes were placed in a
chamber and perfused with Ringer's solution containing 120 mmol/liter
NaCl, 2.5 mmol/liter KCl, 1.1 mmol/liter CaCl2, 1.0 mmol/liter EGTA, and 10 mmol/liter HEPES-acid, pH 7.2 (NaOH). A stock
solution of loratadine (50 mmol/liter) was prepared in dimethylsulfoxide and diluted to the desired test concentrations with
bath solution. To avoid artifacts, the portion of dimethylsulfoxide in
the perfusing solution was never allowed to exceed 0.2% (v/v).
Current records were amplified with the use of a Warner oocyte clamp
(OC-725A) and low-pass filtered at 3 kHz (
3 dB, four-pole Bessel
filter, Wavetech model 432; Hamdem, CT). Data were stored on the hard
disk of a 486 IBM-compatible computer for off-line analysis. All data
acquisition and analysis were done with pCLAMP software (Axon
Instruments). Currents were recorded at room temperature, and
experiments in which the holding current was >
0.2 µA at a holding
level of
90 mV were excluded from analysis. For all
electrophysiological measurements, statistical significance was
accepted at the p < 0.05 level.
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Results |
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Fig. 1 shows the effects of
loratadine on human cardiac Kv1.5 current recorded from an HEK 293 cell
in the inside-out membrane patch configuration. Under these conditions,
we found loratadine to be an effective blocker of this channel. At a
concentration of 100 nM, loratadine produced a small but
significant (16 ± 2% inhibition, n = 7;
p < 0.05 paired t test) inhibition of Kv1.5 current (Fig. 1A). At higher concentrations, a more robust inhibition of Kv1.5 current was apparent, which was reversible on washing the
patch with drug-free solution (Fig. 1B). The IC50 value for loratadine blockade of Kv1.5 was 8.08 × 10
7
M (Fig. 1C). The main effect of loratadine was to
accelerate the rate of Kv1.5 current decay during a step
depolarization. In the absence of drug, Kv1.5 current decay was well
fitted to a single exponential function with a time constant of
~400-500 msec (Fig. 2A) (13, 21). In
the presence of loratadine, a new component of rapid inactivation was
added (Fig. 2B). This rapid component of inactivation ranged from 54.4 msec at a loratadine concentration of 300 nM to 11.0 msec
at 10 µM. These fast, drug-induced time constants are
plotted as a function of loratadine concentration in Fig. 2C. A plot of
the reciprocal of these time constants versus loratadine concentration
(Fig. 3) yielded an apparent association rate constant of 7.5 × 106
M
1sec
1 and an apparent
dissociation rate constant of 16.5 sec
1. The apparent
KD value was 2.2 × 10
6 M, which is in good agreement with
the IC50 value obtained in Fig. 1C.
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After oral administration, loratadine is extensively metabolized, with
descarboethoxyloratadine as the major metabolic product (22). Fig.
4 illustrates the effects of this
metabolite on Kv1.5. Descarboethoxyloratadine was ~7-fold less potent
at blocking Kv1.5 than the parent compound, displaying an
IC50 value of 5.60 × 10
6 M
(Fig. 4B). Also, unlike loratadine, descarboethoxyloratadine reduced
Kv1.5 current amplitude with no apparent effect on the rate of current
decay (Fig. 4A).
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Fig. 5 illustrates the effects of loratadine on Kv1.5 current recorded over a wide range of test potentials. Currents in the absence and presence of 1 µM loratadine are shown in Fig. 5, A and B, respectively. The resultant steady state I-V relationships for these data are shown in Fig. 5C. Interestingly, we found that the blocking effects of loratadine on Kv1.5 were more potent at lower membrane potentials relative to higher ones. This was true even over potentials in which channel conductance is saturated (+20 to +50 mV, Ref. 6, slope significantly different from zero, p < 0.05, t test). This inverse relationship between Kv1.5 current blockade and test potential is plotted in Fig. 5D.
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Fig. 6 shows the effects of loratadine on
Kv1.5 current deactivation. Using the whole-cell configuration of the
patch-clamp, outward tail currents were recorded at a potential of
45
mV after a 100-msec step depolarization to +30 mV (Fig. 6A). In the
absence of drug, Kv1.5 currents deactivated with a time constant of
10.83 ± 1.56 msec (five experiments). In the presence of 3 µM loratadine, this value was 9.85 ± 1.19 msec
(five experiments), which was not significantly different from the
control value (p > 0.05, paired t
test). Loratadine also failed to alter the time course of Kv1.5 current
activation. In the absence of drug, Kv1.5 current activated at +30 mV
with a time constant of 3.24±0.25 msec (five experiments). In the
presence of 3 µM loratadine, this value was not
significantly different and was 3.49±0.49 msec (five experiments).
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Fig. 7 illustrates the effects of
loratadine on the steady state inactivation properties of Kv1.5.
Inactivation was determined by measuring current evoked by depolarizing
pulses to +50 mV while the holding potential (20-sec duration) was
increased in 7-mV increments from
70 to 7 mV. In the absence of drug,
the midpotential (V0.5) and slope value (k) of
the steady state inactivation curve was
21.5 ± 1.9 mV and
8.2 ± 0.4 mV, respectively (four experiments). In the presence of 3 µM loratadine, the slope value was not significantly changed and was
9.0 ± 0.5 mV, whereas a small but significant (p < 0.05, paired t test)
hyperpolarizing shift in the midpotential (
27.5 ± 1.4 mV, four
experiments) was observed.
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We next examined the effects of loratadine on Kv1.5 at the
single-channel level. Because the very high channel density in the HEK
293 cell line made single-channel experiments difficult, we used a
mouse Ltk
cell line expressing a lower density
of Kv1.5 channels for single-channel recordings. This system has
previously been used for recording Kv1.5 currents (23). Fig.
8 shows typical Kv1.5 channel activity recorded at a test potential of +60 mV. In the absence of drug, Kv1.5
channel openings appeared throughout the duration of a 190-msec test
pulse (Fig. 8, A and B). In the presence of 3 µM
loratadine (Fig. 8B), channel openings were largely confined to an
abbreviated burst at the beginning of each test depolarization,
followed by longer closed times relative to control (Fig. 8A). This
resulted in an acceleration of Kv1.5 current decay when these
single-channel sweeps were summed (Fig. 8C), similar to that found for
the macroscopic currents.
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Because the time dependence of loratadine block resembles the kinetics of open-channel block we examined the open time distribution for evidence of a reduction in channel open time. Fig. 9 illustrates the lack of effect of loratadine on the open time distribution of Kv1.5 unitary currents. Mean values are 2.56 ± 0.38 msec for control and 2.71 ± 0.66 msec for loratadine (mean ± standard error, three experiments; p > 0.05, Student's paired t test). The probability of open state occupancy at the end of the voltage step was reduced significantly by loratadine. The ratio of the mean to the peak probability of open state occupancy was 0.73 ± 0.05 in control and was significantly reduced to 0.43 ± 0.06 in the presence of loratadine (mean ± standard error, three experiments; p < 0.05, Student's paired t test).
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Comparison of burst duration in control and in the presence of 3 µM loratadine revealed a statistically significant reduction: 52 ± 3 msec for control and 27 ± 3 msec for loratadine (mean ± standard error, three experiments; p < 0.05, Student's paired t test). The shorter burst duration was due to a reduction in the number of openings in a burst: 14 ± 2 for control and 7 ± 2 for loratadine (mean ± standard deviation, three experiments; p < 0.05, Student's paired t test), whereas closed times within bursts were unchanged.
We next examined the effects of loratadine on the HERG cardiac
K+ channel with a protocol previously used to examine the
blocking effects of terfenadine on this channel (14). Briefly, HERG
current was activated at a potential of >
40 mV by an 800-msec
depolarizing pulse from a holding potential of
80 mV. The steady
state I-V relationship had a typical bell-shaped wave form that peaked
at 0 mV and revealed large outward tail currents at
50 mV due to fast
recovery from inactivation and slow deactivation characteristic of this
channel (3, 14). Fig. 10 shows the
effects of 10 µM loratadine on whole-cell HERG channel
currents recorded from a X. laevis oocyte over a wide range
of test potentials. Under these conditions, loratadine failed to
significantly alter HERG currents. Conversely, using the same
experimental protocol, the nonsedating antihistamine terfenadine has
previously been shown to block HERG currents with an IC50
value of 350 nM (14).
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Discussion |
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We previously used the Kv1.5 channel as a model to explore the interactions of another nonsedating antihistamine, terfenadine, with human cardiac K+ channels (13). We have shown that terfenadine blocks Kv1.5 channel current in a time-dependent manner with an IC50 value of ~400 nM (13). Like terfenadine, loratadine blocked Kv1.5 currents in a time-dependent fashion with approximately equal affinity. Also like terfenadine, the major metabolite of loratadine was far less potent at inhibiting Kv1.5 compared with the parent compound. However, we noted some important differences in the apparent mode of action of these two drugs. Terfenadine, which is mainly positively charged at physiological pH (pKa = 8.6), slows Kv1.5 deactivation and displays a greater block at more depolarized potentials, including potentials in which channel conductance is saturated. This presumably reflects blockade of the open channel state of Kv1.5 from the intracellular face of the channel (13, 24) and that the channel must wait for the drug to unbind before closing. Loratadine, on the other hand, showed no appreciable effect on Kv1.5 current deactivation, suggesting that the channels can close with the drug bound. Furthermore, the blocking effects of loratadine displayed an inverse relationship to voltage, with significantly less inhibition occurring at depolarized potentials relative to membrane potentials closer to the threshold of activation of Kv1.5. We found this type of voltage-dependent behavior especially interesting in light of the fact that loratadine is uncharged at physiological pH (pKa = 5.0). Finally, we found that loratadine had little effect on the cardiac HERG channel, whereas terfenadine blocks this channel with an IC50 value of 350 nM (14).
We used single-channel analysis to further explore the mechanism of
action of loratadine on Kv1.5 and found the main effect of loratadine
was to decrease the probability of opening of Kv1.5. However, even at a
near-maximal inhibitory concentration, loratadine failed to alter the
mean open time of Kv1.5. Furthermore, we found that loratadine
significantly reduced Kv1.5 burst duration. Taken together with the
macroscopic currents, the data suggest an interaction of loratadine
with an activated state of the Kv1.5 channel. This could take the form
of an interaction with the open state of Kv1.5. Our single-channel data
rule out a simple open-channel block mechanism in which loratadine
interacts with the open state of the channel at a rate sufficient to
reduce the open time of individual openings because no change in mean
open time was observed with exposure to loratadine. From the
concentration dependence of the kinetics of channel block, we
calculated an on-rate for loratadine of 7.5 × 103
M1sec1, and at a concentration of 3 µM, the channel-blocking rate becomes 0.0225 msec
1. Channel open time is defined kinetically as the
reciprocal of the sum of transitions leaving the open state and
measured 2.56 msec in control and 2.71 msec in the presence of
loratadine. The expected value for the open time in the presence of
loratadine can be calculated from the closing rate determined in
control conditions (
o = 1/
o), and the
additional closing transition introduced by loratadine interaction with
the open state can be calculated as
o,loratadine = 1/(
o
kon,loratadine · [loratadine concentration]). Using the estimated value for the
loratadine blocking rate at 3 µM (0.0225 msec
1), the expected open time for a simple open-channel
block mechanism with a 2.56-msec open time in control is (0.390 msec
1 + 0.0225 msec
1)
1, or
2.42 msec in the presence of 3 µM loratadine (25). This small reduction in open time is below the precision of our open time
measurements; consequently, we observed no significant difference in
open times between measurements in control and after exposure to
loratadine. Although changes in mean open time were negligible, our
data predict the interaction of loratadine with Kv1.5 to be sufficiently fast and of a duration to alter burst kinetics. The mean
sum of individual open state dwell times occurring within single bursts
(mean total open time in a burst) is much longer than an individual
dwell time in the open state for Kv1.5. Similar to the relation for
individual open times, the reciprocal of the mean total open time in a
burst gives an estimate for the mean exit rate from the open state
within a burst. This rate is similar in magnitude to the calculated
blocking rate for loratadine and should be observable. In our case, the
calculated off-rate for loratadine (16.5 sec
1; see above)
predicts a mean shut interval (61 msec) much longer than the critical
closed time used to distinguish bursts (<5 msec in all cases), so
essentially all blocking events will terminate a burst and be reflected
in the data as a reduction in the mean total open time in a burst. The
mean total open time in a burst obtained as the product of the mean
open dwell time (2.56 and 2.71 msec for control and in the presence of
loratadine, respectively) and the mean number of openings in a burst
(14 and 7 for control and in the presence of loratadine, respectively)
were 35.84 msec in control and 18.97 msec in the presence of 3 µM loratadine. Using the calculated blocking rate
constant for 3 µM loratadine and the reciprocal of the
experimentally determined mean total open time in a burst in control
conditions, the predicted mean total open time in a burst for the case
in which all loratadine blocking events terminate a burst is (35.84 msec
1 + 0.0225 msec
1)
1, or
19.84 msec, which compares favorably to our experimentally observed
value of 18.97 msec. The mechanism for this block would be similar to
that proposed for open-channel block of Kv1.5 by clofilium (26).
However, the inverse voltage dependence of block produced by the
uncharged loratadine molecule is difficult to reconcile with blockade
of only the open state. Thus, we cannot exclude a secondary interaction
of loratadine with another nonconducting state of Kv1.5 that may be
favored at potentials near threshold.
Use of the nonsedating antihistamines terfenadine and astemizole may,
on occasion, be associated with a prolongation of cardiac repolarization (9, 10). Presumably, this reflects an interaction of
these drugs with one or more voltage-dependent K+ channels
in the human myocardium (11-14). After the normal therapeutic dose of
loratadine (10 mg), peak serum plasma levels of the drug average ~12
nM (22, 27). However, after a dose of 40 mg, peak serum
levels of loratadine can reach ~150 nM in normal
volunteers and >200 nM in the elderly (22, 28). One case
report has linked loratadine use with QT prolongation and ventricular
tachycardia in a patient with a history of such arrhythmias (16, but
see also 29). More recently, a cluster of adverse drug reactions
involving palpitations and arrhythmias after loratadine administration
was reported to the Australian ADR Advisory Committee (17). In the United States, a number of adverse drug reactions associating loratadine use with various supraventricular tachycardias are on file
with the Food and Drug Administration (30), and some adverse drug
reactions involving loratadine overdoses of
40 mg have been
accompanied by tachycardias or other cardiac electrical disturbances.
Presently, it is unclear whether any of these adverse reactions involve
loratadine blockade of voltage-dependent K+ channels in the
human myocardium. However, the results of the current study show that
although loratadine has little affinity for HERG, it can block the
human cardiac Kv1.5 channel at concentrations similar to those reported
for terfenadine. Such concentrations can be achieved in humans with
relatively small overdoses of the drug. Furthermore, due to its inverse
voltage dependence, the affinity of loratadine for Kv1.5 may be
enhanced near its threshold of activation. Because Kv1.5 is an
important repolarizing current in the human atria (6, 7), such an
interaction could lead to altered repolarization in this tissue. Future
studies using human atrial tissue should prove useful in exploration of
this possibility.
In summary, we described the interaction of the nonsedating
antihistamine loratadine on the human cardiac K+ channel
Kv1.5. The blocking effects of loratadine on Kv1.5 occurred at
concentrations of
100 nM. Loratadine enhanced the rate of Kv1.5 current decay and was more potent at membrane potentials near the
threshold of channel activation. At the single-channel level,
loratadine reduced the probability of opening of Kv1.5 and decreased
the number of openings in a burst and the burst duration. Loratadine
failed to alter the mean open time of Kv1.5. The results show that like
terfenadine and astemizole, loratadine can block at least one type of
cardiac K+ channel at submicromolar concentrations. It is
possible that such an interaction could contribute to altered cardiac
repolarization in vivo.
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Acknowledgments |
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We thank Dr. Barbara Wible (The Rammel Kamp Center, Cleveland, OH) for the cloning and transfection of the Kv1.5 cDNA and Dr. Glenn Kirsch for helpful discussions regarding the manuscript.
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Note Added in Proof |
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After this article was accepted for publication, we obtained a mammalian cell line expressing HERG and found the IC50 value of lovatadine to be 2.8 mM.
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Footnotes |
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Received September 17, 1996; Accepted April 17, 1997
Send reprint requests to: David Rampe, Ph.D., Hoechst Marion Roussel, Inc., 2110 E. Galbraith Road, Cincinnati, OH 45215. E-mail: davidrampe{at}hmri.com
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Abbreviations |
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HEK, human embryonic kidney;
HERG, human
ether-a-go-go-related gene;
EGTA, ethylene glycol bis(
-aminoethyl
ether)-N,N,N
,N
-tetraacetic
acid;
HEPES, 4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid;
I-V, current-voltage.
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