Preclinical assessment of drug-induced proarrhythmicity is typically evaluated by the potency of the drug to block the potassium human ether-à-go-go-related gene (hERG) channels, which is currently quantified by the IC50. However, channel block depends on the experimental conditions. Our aim is to improve the evaluation of the blocking potency of drugs by designing experimental stimulation protocols to measure the IC50 that will help to decide whether the IC50 is representative enough. We used the state-of-the-art mathematical models of the cardiac electrophysiological activity to design three stimulation protocols that enhance the differences in the probabilities to occupy a certain conformational state of the channel and, therefore, the potential differences in the blocking effects of a compound. We simulated an extensive set of 144 in silico IKr blockers with different kinetics and affinities to conformational states of the channel and we also experimentally validated our key predictions. Our results show that the IC50 protocol dependency relied on the tested compounds. Some of them showed no differences or small differences on the IC50 value, which suggests that the IC50 could be a good indicator of the blocking potency in these cases. However, others provided highly protocol dependent IC50 values, which could differ by even 2 orders of magnitude. Moreover, the protocols yielding the maximum IC50 and minimum IC50 depended on the drug, which complicates the definition of a "standard" protocol to minimize the influence of the stimulation protocol on the IC50 measurement in safety pharmacology. As a conclusion, we propose the adoption of our three-protocol IC50 assay to estimate the potency to block hERG in vitro. If the IC50 values obtained for a compound are similar, then the IC50 could be used as an indicator of its blocking potency, otherwise kinetics and state-dependent binding properties should be accounted.
Preclinical assessment of drug-induced proarrhythmicity is typically evaluated by the potency of the drug to block the potassiumhuman ether-à-go-go-related gene (hERG) channels, which is currently quantified by the IC50. However, channel block depends on the experimental conditions. Our aim is to improve the evaluation of the blocking potency of drugs by designing experimental stimulation protocols to measure the IC50 that will help to decide whether the IC50 is representative enough. We used the state-of-the-art mathematical models of the cardiac electrophysiological activity to design three stimulation protocols that enhance the differences in the probabilities to occupy a certain conformational state of the channel and, therefore, the potential differences in the blocking effects of a compound. We simulated an extensive set of 144 in silico IKr blockers with different kinetics and affinities to conformational states of the channel and we also experimentally validated our key predictions. Our results show that the IC50 protocol dependency relied on the tested compounds. Some of them showed no differences or small differences on the IC50 value, which suggests that the IC50 could be a good indicator of the blocking potency in these cases. However, others provided highly protocol dependent IC50 values, which could differ by even 2 orders of magnitude. Moreover, the protocols yielding the maximum IC50 and minimum IC50 depended on the drug, which complicates the definition of a "standard" protocol to minimize the influence of the stimulation protocol on the IC50 measurement in safety pharmacology. As a conclusion, we propose the adoption of our three-protocol IC50 assay to estimate the potency to block hERG in vitro. If the IC50 values obtained for a compound are similar, then the IC50 could be used as an indicator of its blocking potency, otherwise kinetics and state-dependent binding properties should be accounted.
The rapid component of delayed rectifier current (IKr), which is encoded by the human ether-à-go-go-related
gene (hERG), plays an important role on the cardiac action potential
(AP) duration. This current is a well-known promiscuous drug target,
and many drugs associated with torsade de pointes inhibit the IKr and hERG channels.[1] Therefore, a key test of the current cardiac safety assessment of
pharmacological compounds consists of the observed in vitro block
of these channels.[2] This is typically quantified
by the IC50, which is the drug concentration that blocks
50% of the current. There is experimental evidence of the IC50 dependency on the experimental conditions, such as voltage stimulus
protocol, temperature, and expression system.[3−7] Indeed, hERG channel blockers can inhibit the channel
by means of different mechanisms, which may exhibit time, voltage,
and state dependence.[5,8,9] However,
there is no standardization of these assays at present, which favors
the existence of a high variability of the IC50 values
reported in the literature and databases, such as FDA drug labels,
PubChem,[10] and DrugBank.[11] A few experimental works have compared the IC50 values using different voltage protocols and have reported variations
in the IC50 values up to 10-fold when only changing the
voltage protocol.[4−6,12] However, the number
of drugs used in these studies was reduced. A very recent investigation
of the factors that contribute to the IC50 differences
has been performed using a in silico drug binding and unbinding to
the open and inactivated states not allowing drug-bound channels to
change their conformational state.[13] With
these simple drug–channel interactions, the authors have elegantly
shown that state dependence of drug binding is a major determinant
of the protocol dependence of IKr IC50. However, that study only considered in silico drug binding
and unbinding in the open and/or inactivated states, not in the closed
state, despite the existence of compounds, such as ketoconazole and
BeKm-1, that preferentially block the channel in the closed state.[5,8,9] In addition, drug-bound channels
in that study were not allowed to change their conformational state,
which avoids simulation of drug trapping, a very well-known phenomenon
that takes place in the presence of certain drugs.[14,15]Here, we attempt to shed light on the relevance of the IC50 as an indicator of the IKr blocking
potency of a compound and to improve the characterization of its blocking
effects using a highly detailed Markov model considering a wide range
of drug–channel interactions. We hypothesize that, as the drug–channel
interaction may depend on the conformational state of the channel,
stimulation at certain voltages where the probability of these states
is very different will provide more information about the blocking
potency than a unique voltage clamp protocol. In this work, we designed
voltage protocols that could unmask distinct state-dependent potencies
of block. Then, we systematically carried out “in silico drug
genesis” by creating a wide range of virtual drugs with different
kinetics and affinities to the conformational states of the IKr channel. In silico drugs are able to bind
and unbind to any conformational state of the channel: closed, open,
and/or inactivated. Moreover, two kinds of drug-bound channels were
simulated: those that do not change their conformational state and
those that do it, which allows the simulation of drug trapping. Next,
we obtained the Hill-plots for each virtual drug using our new protocols
as well as other existing protocols and calculated the IC50s. Finally, we performed some experiments to support our simulation
results.
Materials and Methods
Drug
Models
The human ventricular IKr was simulated using the five-state Markov
chain proposed by Fink et al.[16] This model
has five states: three closed states (C3, C2, and C1), an open state
(O), and an inactivated state (I). In order to simulate drug interactions
with IKr, we included the new states the
channel can occupy in the presence of the drug, namely, C3d, C2d, C1d, Od, and Id. Figure shows the
simulated IKr Markov model for multiple
drug-bound configurations together with the corresponding type drug–channel
interaction label. As the ion channel targeting drugs display complex
properties determined by preferential binding to distinct conformational
states and/or distinct affinity to discrete states, we simulated a
wide variety of likely drug–channel interactions: drugs that
exclusively interact in the closed (Figure A,B), open (Figure C,D), or inactivated (Figure E,F) states, drugs binding simultaneously
to both the closed and open states (Figure G,H), or to both the open and inactivated
states (Figure I,J)
and drugs binding simultaneously to all states (Figure K,L). We allowed drug-bound channels to change
their conformational state (Figures A,C,E,G,I,K) as in our previous work,[17] and we labeled them unstuck, but we also considered the
possibility that the drug-bound channels do not change their conformational
state unless unbinding occurs, and we labeled them stuck (Figures B,D,F,H,J,L). Microscopic
reversibility was ensured by equaling the product of the rates going
clockwise to the product going anticlockwise in closed loops.[18] As drug-bound channels are electrically silent,
which precludes the assessment of the transition rates between states,
we modified the transition rates from Id to Od and from Od to C1d when appropriate. Drug
kinetics were also analyzed in detail by testing a range of diffusion
(k) and dissociation rates (r) for
the various drug configurations. Dissociation rates ranged from 0.001
to 1000 s–1 using logarithmic or half-logarithmic
increments, in line with other simulation works,[19,20] and the diffusion was the same in all the states, where the drug
binds. A total of 144 prototypical drugs were simulated, and their
names were generated depending on the states the drug binds and unbinds
to and the speed of the dissociation rates. We called Closed, Open,
and Inactivated drugs to those binding exclusively to the closed,
open, or inactivated states, respectively. We labeled ClosedO, OpenC,
and CO the drug binding simultaneously to both the open and closed
states with higher affinity to the closed state, to the open state,
and with the same affinity, respectively. We labeled OpenI, InactivO,
and IO the drugs binding simultaneously to both the open and inactivated
states with higher affinity to the open state, to the inactivated
state, and with the same affinity, respectively. Finally, we labeled
COI, ClosedOI, OpenCI, and InactivOC the drug binding simultaneously
all states with the same affinity, with higher affinity to the closed,
to the open, and to the inactivated state, respectively. We added
the suffixes sss, ss, s, m, f, and ff, depending on the slowest dissociation
rate of the drug, which corresponded to 0.001, 0.003, 0.01, 0.1, 1
and 10 s–1, respectively. Diffusion (k) and dissociation (r) rate constants for each drug–IKr interaction as tested in the model are included
in the Supporting Information (Tables S1
and S2). Drug doses ranging from 10–11.7 to 10–2.7 mol/L (M) with 100.1 M steps were simulated
for each virtual drug in order to build their respective Hill plots.
The temperature was set to 22 or 37 °C and intracellular and
extracellular potassiumconcentrations were fixed to 130 and 4 mM,
respectively.
Figure 1
Simulated Markov drug–IKr interaction
models with nondrug-bound (C3, C2, C1, O, and I) and drug-bound (C3d, C2d, C1d, Od, and Id) states considering unstuck
(A,C,E,G,I, and K) and stuck (B,D,F,H,J, and L) drug-bound channels. D is the drug concentration, and its product with kC, kO, and kI corresponds to the association rates constants
in the closed, open, and inactivated states, respectively, and rC, rO, and rI are the dissociation rate constants in the
closed, open, and inactivated states, respectively. Binding states
are red colored. First column indicates the corresponding type of
the drug–channel interaction and first row specifies the state
of the channel when the drug is bound.
Simulated Markov drug–IKr interaction
models with nondrug-bound (C3, C2, C1, O, and I) and drug-bound (C3d, C2d, C1d, Od, and Id) states considering unstuck
(A,C,E,G,I, and K) and stuck (B,D,F,H,J, and L) drug-bound channels. D is the drug concentration, and its product with kC, kO, and kI corresponds to the association rates constants
in the closed, open, and inactivated states, respectively, and rC, rO, and rI are the dissociation rate constants in the
closed, open, and inactivated states, respectively. Binding states
are red colored. First column indicates the corresponding type of
the drug–channel interaction and first row specifies the state
of the channel when the drug is bound.
Simulation of the Pseudo-ECG
Pseudo-ECGs
were computed using a one-dimensional (1D) tissue model of a transmural
wedge preparation, as in our previous work.[21] The 1D model was composed by 60 endocardial cells, 45 midmyocardial
cells, and 60 epicardial cells, each cell being 100 μm long,
as defined in the O’Hara et al. model[22] and it was paced at 1 Hz. The propagation of the AP was described
by the following nonlinear reaction diffusion equationwhere Cm stands
for the membrane capacitance, a is the radius of
the fiber, ∑Iion is the sum of
all the ionic currents flowing through the cellular membrane, and Ri represents the intracellular resistivity.
Drug blocking effect on IKr was formulated
using the standard sigmoid dose–response curve, parameterized
using the half-maximal response dose (IC50), and considering
a Hill coefficient of 1 as in previous studies[21,23−26]where D is the drug concentration
and “1 – b” is the fraction
of unblocked channels.
Experimental Methods
All experiments
were conducted manually with an EPC-10 amplifier (HEKA, Lambrecht/Pfalz,
Germany) at room temperature in the whole-cell mode of the patch-clamp
technique. HEK-293 cells stably expressing hKv11.1 (hERG) under G418
selection were a generous gift from Craig January (University of Wisconsin,
Madison). Cells were cultured in Dulbecco’s modified Eagle’s
medium containing fetal bovine serum 10%, glutamine 2 mM, Na + pyruvate
1 mM, penicillin 100 U/L, streptomycin 171.94 μM (100 μg/mL),
and G418 1 M (500 mg/mL). Before experiments, cells were lifted using
TrypLE and plated onto poly-l-lysine-coated coverslips, patch
pipettes were pulled from soda lime glass (micro-hematocrit tubes)
and had resistances of 2–4 MΩ. We used normal sodium
Ringer for the external solution (in mM: NaCl 160, KCl 4.5, CaCl2 2, MgCl2 1, HEPES 10 (adjusted to pH 7.4, using
HCl and NaOH, and 290–310 mOsm). The internal solution contained
(in mM) CaCl2 5.375, MgCl2 1.75, EGTA 10, HEPES
10, KCl 120, and NaATP 4 (adjusted to pH 7.2, using HCl and NaOH,
and 300–320 mOsm). For all experiments, solutions of dofetilide
and moxifloxacin were always freshly prepared from 1, 10, or 100 mM
stock solutions in dimethyl sulfoxide (DMSO) during the experiment.
The final DMSOconcentration never exceeded 1%.
Stimulation Protocols
Three different
sets of voltage clamp protocols were used. The first and third sets
were designed in this work while the second was adopted from the literature.
The first set was composed of our new stimulation voltage clamp protocols,
which consisted of a 5 s variable voltage conditioning step (at −80,
0, and 40 mV) followed by a 0.2 s test pulse at −60 mV repeated
at 5.4 s intervals, from a holding potential of −80 mV (Figure , top). When the
5 s variable voltage was fixed at −80 mV, a 0.5 ms prepulse
at 20 mV was included and the 0.2 s test pulse was applied at −50
mV. These protocols were called P-80, P0, and P40, respectively. The
second set was composed of Protocol-O, Protocol-C, and the standard
protocol (SP) defined by Yao et al. 2005.[5] Protocol-O consisted of a 4.8 s conditioning step at 20 mV followed
by a 0.5 s test pulse at −50 mV repeated at 6 s intervals,
from a holding potential of −80 mV. Protocol-C consisted of
a 1 s conditioning step at 20 mV followed by a 5 s test pulse at −50
mV repeated at 60 s intervals, from a holding potential of −80
mV. The SP consisted of a 4.8 s conditioning step at 20 mV followed
by a 5 s test pulse at −50 mV repeated at 15 s intervals, from
a holding potential of −80 mV. The third set of protocols consisted
of two AP clamp protocols, P_AP1 and P_AP2, which were generated using
a version of the mid-myocardial O’Hara et al. AP model[22] whose IKr is reduced
to 40% at 0.5 and 2 Hz, respectively.
Figure 2
Simulated influence of the voltage of
the stimulation protocol
on the probabilities of the states of the IKr channel at 22 °C. Stimulation protocol (top), averages (A)
of the simulated probabilities of the closed states (CAVG, solid line), the open state (OAVG, dashed line) and the inactivated state (IAVG, dotted line) for the whole protocol duration as a
function of the voltage of the conditioning step (Vm) and the difference between the average of the simulated
probabilities of the closed states and the open state [CAVG – OAVG, (B)] and
the difference between the average of the probabilities of the inactivated
state and the open state [IAVG – OAVG, (C)].
Simulated influence of the voltage of
the stimulation protocol
on the probabilities of the states of the IKr channel at 22 °C. Stimulation protocol (top), averages (A)
of the simulated probabilities of the closed states (CAVG, solid line), the open state (OAVG, dashed line) and the inactivated state (IAVG, dotted line) for the whole protocol duration as a
function of the voltage of the conditioning step (Vm) and the difference between the average of the simulated
probabilities of the closed states and the open state [CAVG – OAVG, (B)] and
the difference between the average of the probabilities of the inactivated
state and the open state [IAVG – OAVG, (C)].IKr and hERG channels were stimulated
repeatedly until reaching the steady state at pretreatment control
and under drug application. Peak tail current amplitudes were measured
at steady state and Hill plots were constructed by plotting the steady-state
tail peak current normalized to control for each concentration versus
the decimal logarithm of the drug concentration, as in previous studies.[5,6,25,27]
Results
Design of Voltage Protocols
As a
drug–channel interaction may depend on the conformational state
of the channel, and it depends on the membrane voltage, we studied
the influence of the voltage of the conditioning step of the stimulation
protocol on the probability of the IKr channel to occupy a specific conformational state using computer
simulations. For this purpose, we considered a stimulation voltage
clamp that consisted of a 5 s variable voltage (Vm) conditioning step followed by a 0.2 s test pulse at
−60 mV repeated at 5.4 s intervals from a holding potential
of −80 mV (Figure , top). This protocol was applied in control (absence of drug)
at different conditioning step voltages. Then, the average of the
probabilities of the three closed states (CAVG, solid line), the open state (OAVG,
dashed line), and the inactivated state (IAVG, dotted line) for the whole protocol duration were computed as a
function of the conditioning step voltage (Figure A). Moreover, the differences CAVG – OAVG (Figure B) and IAVG – OAVG (Figure C) were also calculated,
as these differences will be key to select the conditioning step voltages
that will provide more information about the blocking potency of the
drug. Indeed, unstuck OpenC drugs are expected to produce the highest
block when the stimulation protocol is such that it maximizes the
probability of the open state (close to 0 mV, Figure A, long dashed line) while the probability
of the closed state is low. It would occur when the CAVG – OAVG is small
and OAVG is relatively high, which would
correspond to a conditioning pulse close to 0 mV (Figure B). In addition, the lowest
inhibition of the channels would occur when the CAVG – OAVG is maximum,
which takes place for conditioning pulses at low voltages (Figure B). Therefore, the
maximum and minimum IC50 of unstuck OpenC will be expected
when applying this protocol with conditioning pulses close to −80
and 0 mV, respectively. For conditioning pulses at higher voltages,
such as 40 mV the IC50 would be expected to be closer to
the value obtained with the conditioning pulse at 0 mV. In the case
of unstuck ClosedO drugs, the opposite behavior is expected. Regarding
drugs with different affinities to the open and inactivated states,
as IAVG – OAVG is maximum at 40 mV (Figure C), adoption of this voltage for the conditioning pulse
would yield high inhibition for unstuck InactivO drugs. Therefore,
the application of this protocol with conditioning steps at −80,
0, and 40 mV would highlight the differences in the potency of the
block with the voltage. As conditioning steps at −80 mV raised
very small currents to be measured in the experiments, we modified
this protocol to include a prepulse at 20 mV for 0.5 s to open the
channels. These protocols were labeled P-80, P0, and P40, respectively,
as indicated in the Materials and Methods section. Figure A shows a representation of
each protocol.
Figure 3
Simulated effects of voltage clamp protocols on IC50. Voltage clamp protocols (A) and the corresponding steady-state
current traces before and after the application of selected virtual
drugs: unstuck Inactivated_s (B), stuck Inactivated_s (C), and stuck
ClosedO_s (D) at 22 °C. First column represents the Markovian
schemes of the simulated drug–IKr interactions. Second, third, and fourth columns correspond to the
steady-state currents traces elicited for each protocol and arrows
indicate peak tail current amplitudes at marked concentrations. Last
column illustrates the corresponding Hill plots.
Simulated effects of voltage clamp protocols on IC50. Voltage clamp protocols (A) and the corresponding steady-state
current traces before and after the application of selected virtual
drugs: unstuck Inactivated_s (B), stuck Inactivated_s (C), and stuck
ClosedO_s (D) at 22 °C. First column represents the Markovian
schemes of the simulated drug–IKr interactions. Second, third, and fourth columns correspond to the
steady-state currents traces elicited for each protocol and arrows
indicate peak tail current amplitudes at marked concentrations. Last
column illustrates the corresponding Hill plots.
Simulated Effects of the Voltage Protocol
on the IC50
Once the stimulation protocols were
designed, IKr inhibition produced by all
the prototypical drugs was examined using P-80, P0, and P40.Figure summarizes
the results obtained for three selected drugs: unstuck Inactivated_s
(Figure B), stuck
Inactivated_s (Figure C), and stuck ClosedO_s (Figure D). The voltage clamp protocols are represented at
the top panel (Figure A). The Markovian schemes of the simulated drug–IKr interactions are illustrated in the first column, the
steady-state currents traces elicited for each protocol, namely, P-80,
P0, and P40, are depicted in the second, third, and fourth column,
respectively, and the corresponding Hill plots are constructed in
the last column. Unstuck Inactivated_s (Figure B) produced similar inhibition of IKr tail currents with P-80, P0, and P40, so
the resulting Hill plot curves are superimposed and the IC50s values are the same. Indeed, in the case of unstuck drugs that
only bind and unbind to one state, the IC50 values do not
depend on the stimulation protocol, as it is determined by the ratio
between the diffusion (k) and the “off”
rate (r). Although the steady-state block is the
same for each protocol, the time needed to reach it depends on the
voltage protocol as it determines the mean probabilities of the channel
of being on each state, and, therefore the average of the time during
the cycle to be on the state where the drug can bind and unbind. However,
stuck Inactivated_s (Figure C) had higher inhibitory effects with protocols P0 (second
column) and P40 (third column) than with P-80 (first column), which
is consistent with the fact that IAVG is high for P0 and
P40 and almost zero for P-80 (Figure A, Vm = 0, 40 and −80
mV, respectively). For example, 10 nM stuck Inactivated_s inhibited
tail currents by approximately 50% with P0 and P40, whereas it only
reached approximately 20% with P-80. Subsequently, the Hill plot curves
and the IC50 values corresponding to P0 (red) and P40 (green)
are similar while the one corresponding to P-80 (blue) is shifted
to the left. Therefore, Hill plots of drugs binding just to one state
of the channel were highly dependent on the state of the drug-bound
channel. Unstuck variants had the same IC50 with the three
protocols while the stuck ones exhibited the smallest IC50 with the protocol that enhanced the probability of the state where
the drug binds and unbinds; P40, P0, and P-80 for Inactivated (Figure C), Open, and Closed
drugs, respectively (not shown). Finally, stuck ClosedO_s (Figure D) revealed higher
potency to block IKr with P-80, followed
by P0, than with P40, so the Hill plot curves as well as the IC50 values are different. It is in close agreement with the
inverse dependency of CAVG and CAVG – OAVG with Vm (Figure A,B). These results indicate that unstuck
Inactivated_s (Figure B) produces voltage independent IKr steady-state
blocks. On the contrary, stuck Inactivated_s (Figure C) produces smaller IKr inhibition at low voltages, as it binds and unbinds to the
inactivated state, and stuck ClosedO_s (Figure D) at high voltages, as it has a preferential
affinity to the closed states. Therefore, the dissimilar effects produced
by the drugs when applying our set of voltage clamp protocols manifest
the differences in drug–channel interactions.Figure illustrates
the simulated Hill plots for each type of the prototypical drug binding
to two states with state-dependent affinities using the proposed protocols:
P-80 (blue), P0 (red), and P40 (green) at 22 °C. Both variants
of ClosedO_s (Figure A) have the minimum IC50 with P-80, as expected, as more
channels are closed at −80 mV, while the maximum IC50 is registered with P0 or P40. In the case of OpenC_s drugs, the
maximum IC50 is registered with P-80, which maximizes the
time the channels are closed and tends to reveal the drug’s
affinity to this state. OpenI_s drugs only showed small differences
of IC50, P0 being the protocol showing the smallest IC50, as it is the one that enhances the most the probability
of the open state. Finally, the maximum IC50 of InactivO_s
(Figure D) is registered
with P-80 as this protocol minimizes the probability of the inactivated
state, when the affinity of the drug is higher. Drugs with similar
state preferences and drug-bound states exhibited similar Hill plot
patterns although the maximum IC50 ratio depended on the
value of the slowest dissociation rate of the drug. For example, the
maximum IC50 of InactivO_m also corresponded to P-80 and
the IC50s obtained with P0 and P40 were very similar, like
InactivO_s. However, the maximum IC50 ratio was 13.0 instead
of 23.2, which was the corresponding to InactivO_s (Figure D). These results suggest that
the influence of the voltage clamp protocol on the estimation of the
inhibitory effects of a compound depends on the specific interaction
with the channel.
Figure 4
Simulated Hill plots for each type of the prototypical
drugs binding
to two states with state-dependent affinities using the proposed protocols:
P-80 (blue), P0 (red) and P40 (green) at 22 °C. Unstuck (top)
and stuck (bottom) variants of ClosedO_s (A), OpenC_s (B), OpenI_s
(C), and InactivO_s (D). The maximum IC50 ratio for each
drug is also indicated in each panel.
Simulated Hill plots for each type of the prototypical
drugs binding
to two states with state-dependent affinities using the proposed protocols:
P-80 (blue), P0 (red) and P40 (green) at 22 °C. Unstuck (top)
and stuck (bottom) variants of ClosedO_s (A), OpenC_s (B), OpenI_s
(C), and InactivO_s (D). The maximum IC50 ratio for each
drug is also indicated in each panel.As this study was extended to the 144 in silico drugs, Hill plots
for every prototypical drug were constructed using our proposed protocols
(P0, P40, and P-80) and IC50 values were extracted. Figure summarizes the maximum
IC50 ratios for each drug–channel interaction. Unstuck
and stuck variants are represented with nonfilled and filled bars,
respectively. The highest IC50 ratios were observed for
the stuck variants of Closed, ClosedO, and ClosedOI drugs, and some
unstuck variants of InactivOC, InactivO, ClosedO, ClosedOI, and OpenC
drugs. The highest, mean, and median values of the maximum IC50 ratio were 51.2, 8.7, and 2.7, respectively. Moreover, 13.9%
of the prototypical drugs exhibited a ratio above 20-fold and the
34% yielded a ratio above 10-fold. On the contrary, unstuck drug binding
and unbinding to one state (Closed, Open, and Inactivated), two states
(CO and IO) or all states with the same affinity (COI) exhibited voltage
independent IC50s. IC50s of stuck drugs whose
preferential state for binding and unbinding are the open state (Open,
OpenC, OpenI, and OpenCI) showed a very small dependence on the voltage
protocol, followed by the unstuck variant of Open_I and both unstuck
and stuck variants of InactivO_f, InactivO_ff, and OpenC_ff. Stuck
drugs tended to register higher IC50 ratios than unstuck
drugs, the mean maximum IC50 ratio for stuck drugs being
11.2 while for unstuck drugs being 6.2. However, most unstuck variants
of OpenC, OpenI, and InactivO displayed higher IC50 ratios
than the corresponding stuck variants. Finally, the speed of the association
and dissociation rates played a relevant role, although their effects
were highly drug-dependent. For example, fast rates tended to increase
the maximum IC50 ratio in stuck drugs binding and unbinding
to the closed state. By contrast, fast dynamics decreased this ratio
in drugs binding simultaneously to both the inactivated and open states
with higher affinity to the inactivated state.
Figure 5
Maximum IC50 ratios obtained with our proposed protocols
(P0, P40, and P-80) at 22 °C. Filled (blue and green) and nonfilled
(black and red) bars for stuck and unstuck drugs, respectively.
Maximum IC50 ratios obtained with our proposed protocols
(P0, P40, and P-80) at 22 °C. Filled (blue and green) and nonfilled
(black and red) bars for stuck and unstuck drugs, respectively.IKr inhibition produced
by all the
prototypical drugs was also simulated using the Protocol-O, Protocol-C,
and the SP experimentally used by Yao, et al. 2005[5] (Figure C). Figure shows
the simulated Hill plots of stuck ClosedO_f obtained with ours (A)
and Yao and colleagues’ ones (B). In this case, our protocols
provided a maximum IC50 ratio of 51.5 while the Yao and
co-workers’ ones yielded 37.6. Maximum IC50 ratios
obtained with both sets of protocols for all prototypical drugs are
provided in the Supporting Information (Figure
S1). Maximum, mean, and median values of the maximum IC50 ratios obtained with Yao and co-workers’ protocols were 37.7,
6.5, and 3.1, respectively, which are smaller than those registered
with ours (51.2, 8.7, and 2.7, respectively). Therefore, our new protocols
could be more useful than those currently available in the literature
to detect those compounds that obstruct the channel to a different
extent depending on the stimulation voltage.
Figure 6
Simulated Hill plots
for stuck ClosedO_f using our proposed protocols
(A) and with Yao et al. (2005) protocols (B) at 22 °C. (A) P0
(red), P40 (green), and P-80 (blue). (B) Protocol-O (P-O, red), Protocol-C
(P-C, blue), and SP (green). (C) Yao et al. voltage clamp protocols.[5] The maximum IC50 ratio for each drug
is also indicated in each panel.
Simulated Hill plots
for stuck ClosedO_f using our proposed protocols
(A) and with Yao et al. (2005) protocols (B) at 22 °C. (A) P0
(red), P40 (green), and P-80 (blue). (B) Protocol-O (P-O, red), Protocol-C
(P-C, blue), and SP (green). (C) Yao et al. voltage clamp protocols.[5] The maximum IC50 ratio for each drug
is also indicated in each panel.Our protocols were also used to simulate Hill plots for every prototypical
drug at 35 °C. Although the effects of temperature on binding
and unbinding rates of the virtual drugs were not included, our results
were temperature-dependent as the formulation of the transition rates
between the channel states was temperature-dependent. Absolute and
relative to 22 °C maximum IC50 ratios at 35 °C
are provided in the Supporting Information (Figure S2). Maximum IC50 ratios at 35 °C exhibited
a similar tendency to those at 22 °C although important differences
were observed. The highest IC50 ratio at 35 °C was
105.1. The maximum IC50 ratio that increased the most with
the temperature belonged to unstuck ClosedO_s (Figure A) while the one that decreased the most
corresponded to stuck InactivO_sss (Figure B). Temperature-related differences for the
other virtual drugs were smaller than two-fold. Therefore, the impact
of the voltage protocol on the IC50 is influenced by temperature,
although to a small extent.
Figure 7
Simulated Hill plots for unstuck ClosedO_s (A)
and stuck InactivO_sss
(B) using the new protocols at 22 °C (top) and 35 °C (bottom).
The maximum IC50 ratio for each drug is also indicated
in each panel.
Simulated Hill plots for unstuck ClosedO_s (A)
and stuck InactivO_sss
(B) using the new protocols at 22 °C (top) and 35 °C (bottom).
The maximum IC50 ratio for each drug is also indicated
in each panel.
Experimental
Validation
In order
to provide an experimental validation to our results, our protocols
were applied to construct the experimental Hill plots of two well-known IKr blockers, moxifloxacin and dofetilide, at
22 °C. The moxifloxacin IC50 corresponding to P0,
P40, and P-80 was 373, 196, and 143 μM, respectively (Figure A, left panel), which
gives rise to a maximum ratio of 2.6. This ratio is in accordance
to the experiments of Alexandrou et al. 2006[28] performed at 22 °C, that provide a maximum ratio of 1.9. A
much more dilated influence of the stimulation protocol on dofetilide
IC50 was registered. Hill plots look completely different
(Figure B, left panel)
and disparate IC50 values are obtained: 57, 193, and 695
nM, which correspond to P0, P40, and P-80, respectively. It yields
a maximum ratio of 12.2, which is approximately 3-fold the one calculated
from studies, where the only factor that changed was the voltage protocol.[12] Moreover, our experiments support our finding
that no stimulation protocol can provide the maximum IC50 for every drug. Indeed, the P-80 protocol raised the maximummoxifloxacin
IC50 value while P0 provided the minimum, contrarily to
dofetilide.
Figure 8
Experimental Hill plots (left column) and simulated steady-state
AP of isolated endocardial cells (right columns) for moxifloxacin
(top row) and dofetilide (bottom row). Hill plots were obtained using
the proposed protocols: P-80 (blue), P0 (red), and P40 (green). Symbols
and vertical bars are presented as mean ± standard error of the
mean (n = 4 for all data points). An extra sum-of-squares F test with α set to 0.05 (GraphPad Prism 5; GraphPad
Software, La Jolla, CA) was performed to compare the curves to each
other (moxifloxacin: P40 vs P0 p = 0.0013, P40 vs
P-80 p = 0.1646, P0 vs P-80 p <
0.0001 and dofetilide: P40 vs P0 p = 0.0003, P40
vs P-80 p < 0.0001, P0 vs P-80 p < 0.0001). Simulated steady-state pseudo-ECG in control (black)
and in the presence of 196 μM of moxifloxacin and 193 nM of
dofetilide considering the IC50 obtained using the P-80
(blue), P0 (red), and P40 (green).
Experimental Hill plots (left column) and simulated steady-state
AP of isolated endocardial cells (right columns) for moxifloxacin
(top row) and dofetilide (bottom row). Hill plots were obtained using
the proposed protocols: P-80 (blue), P0 (red), and P40 (green). Symbols
and vertical bars are presented as mean ± standard error of the
mean (n = 4 for all data points). An extra sum-of-squares F test with α set to 0.05 (GraphPad Prism 5; GraphPad
Software, La Jolla, CA) was performed to compare the curves to each
other (moxifloxacin: P40 vs P0 p = 0.0013, P40 vs
P-80 p = 0.1646, P0 vs P-80 p <
0.0001 and dofetilide: P40 vs P0 p = 0.0003, P40
vs P-80 p < 0.0001, P0 vs P-80 p < 0.0001). Simulated steady-state pseudo-ECG in control (black)
and in the presence of 196 μM of moxifloxacin and 193 nM of
dofetilideconsidering the IC50 obtained using the P-80
(blue), P0 (red), and P40 (green).Therefore, our experiments support the potential use of our protocols
to discriminate drugs with a small protocol dependence of the drug
block, such as moxifloxacin, from drugs with an enormous dependence,
such as dofetilide. Our experiments also corroborate that the maximum
IC50 ratios obtained with our protocols are higher than
with previous protocols, and the difficulty to define a unique protocol
to assess the IKr IC50 for
all IKr blockers.
Simulated
Effects of IC50 Differences
on the QT Interval
In order to show how dissimilar estimates
for the IC50 would affect the prediction of drug-induced
QT interval prolongation, pseudo-ECGs were computed in the presence
of moxifloxacin and dofetilide. Concentrations of both drugs were
fixed to the IC50 values obtained with P40, as this protocol
provided an intermediate IC50 value for both drugs. Then,
the drug block was simulated using the simple pore equation without
considering the kinetics and conformational state preference, as done
in many previous works.[21,23−25]Figure shows that
when the estimate of the IC50 used in the simulations was
the one obtained with P40, a 106 ms QT prolongation—from 310
ms in control (black) to 416 ms (green)—was predicted in both
cases, as 50% of the channels are closed. However, different QT prolongations
were observed when considering the IC50 estimates obtained
with P-80 (blue) and P0 (red). The discrepancies were higher for dofetilide
(242 vs 34 ms, bottom row) than for moxifloxacin (134 vs 60 ms, top
row), as estimates of IC50 were more disparate. We also
simulated the pseudo-ECGs in the presence of the following therapeutic
concentrations: 6.23 μM moxifloxacin and 2 nM dofetilide (see
Figure S3 in the Supporting Information). The predicted QT intervals for moxifloxacin were 318, 319, and
323 ms when using the IC50s corresponding to P40, P0, and
P-80, respectively, and for dofetilide they were 326, 322, and 317
ms, respectively. Again, the discrepancies were higher for dofetilide
(9 ms) than for moxifloxacin (5 ms). Therefore, differences in estimates
for the IC50 involve variances in the prediction of the
QT interval.
Clinical Relevance of the
IC50s
Obtained with the Proposed Stimulation Protocols
The ultimate
objective of studying the blocking potency of drugs is to know the
effects of the drugs in vivo. As our proposed stimulation protocols
are far from the time courses of the membrane potentials in vivo,
we also aimed to investigate the drug effects when stimulating the
channels with AP waveforms to study whether the blocking effects observed
with our three proposed protocols are close to those estimated with
more realistic voltage waveforms. For this purpose, we simulated the
Hill plots for every prototypical drug with P_AP1 and P_AP2, which
correspond to the steady-state APs obtained using a version of the
mid-myocardial O’Hara et al. AP model[22] whose IKr is reduced to 40% at 0.5 and
2 Hz, respectively. Figure illustrates these AP clamp protocols (A and B) and shows
a comparison of the simulated Hill plots with these AP clamps (dotted)
and with our three proposed protocols (solid) for each type of the
prototypical drugs binding to two states with state-dependent affinities.
Our results showed that the curves obtained with P_AP1 were similar
to the ones corresponding to P80 while those registered with P_AP2
looked like those obtained with P0. This observation seems reasonable
as in P_AP1 the membrane voltage is −80 mV most of the time
with short intervals of positive potential and in P_AP2 the membrane
voltage is close to 0 mV for a long proportion of the time. These
results may lead to the conclusion that P-80 and P0 would be enough
to characterize the IKr block under realistic
conditions, P40 being less relevant. However, the IC50 obtained
with P40could be useful to study the IKr block in situations that promote channel inactivation. Our results
suggest that the blocking potencies observed with our three proposed
protocols are in line with the ones that will be exerted under realistic
voltage waveforms.
Figure 9
Comparison of the simulated Hill plots obtained with two
AP clamp
protocols, P_AP1 (dotted blue) and P_AP2 (dotted red), which are illustrated
in (A,B), and with our proposed protocols: P-80 (solid blue), P0 (solid
red), and P40 (solid green), at 22 °C. Each type of the prototypical
drugs binding to two states with state-dependent affinities are represented:
unstuck (top) and stuck (bottom) variants of ClosedO_s (C), OpenC_s
(D), OpenI_s (E), and InactivO_s (F).
Comparison of the simulated Hill plots obtained with two
AP clamp
protocols, P_AP1 (dotted blue) and P_AP2 (dotted red), which are illustrated
in (A,B), and with our proposed protocols: P-80 (solid blue), P0 (solid
red), and P40 (solid green), at 22 °C. Each type of the prototypical
drugs binding to two states with state-dependent affinities are represented:
unstuck (top) and stuck (bottom) variants of ClosedO_s (C), OpenC_s
(D), OpenI_s (E), and InactivO_s (F).
Discussion
Main Findings
We developed a computational
approach to investigate whether the IC50 values obtained
for a certain drug could be good estimators of the inhibitory effects
in vivo and to propose improvements in the assessment of the blocking
potency. First, we designed new experimental stimulation protocols
to detect different inhibitory potencies depending on the voltage.
Second, we simulated a wide variety of IKr–drug interactions with increasing drug concentrations using
the new stimulation protocols. Third, we extracted the IC50 values for each drug with the new protocols and with others from
the literature and calculated the maximum ratio of IC50 for each drug–protocol combination. Fourth, we performed
experiments to support our theoretical observations. Finally, we investigated
the drug effects when stimulating the channels with realistic AP waveforms
at different frequencies and they were in line with the effects observed
with our three new protocols.Our results revealed that our
proposed three-protocol IC50 assay improves the assessment
of the blocking potency of drugs and can be very useful to decide
whether the IC50 values accurately assess the inhibitory
effects of the drug in vivo. Our results suggest that when the IC50 values resulting from applying our three protocols to a
compound are similar, then, the IC50 could be a good indicator,
otherwise kinetics and preferential state biding properties should
be taken into account to predict the blocking potency of the drug
in vivo. Our results revealed a much more pronounced impact of the
stimulation protocol on the IC50 than previous experimental
studies. Indeed, the mean and the highest value of the maximum ratio
of IC50 were 8.9 and 105.1, respectively, much higher than
4.3 and 10.3, the corresponding values calculated from experimental
studies, where the voltage protocol was the only factor that changed.[5] Our experiments also support that our protocols
may yield higher IC50 differences than other protocols
available in the literature. This can be due to two important aspects.
First, our protocols were specifically designed to unmask the potential
differences in the blocking effects of a compound because of the existence
of dissimilarities in the affinities to each conformational state
of the hERG channel. In addition, the generation and simulation of
a wide variety of dynamic models of the IKr–drug interaction with very diverse kinetics and affinities
to the conformational states of the channel, which is to date hardly
possible to achieve experimentally. Importantly, our experiments confirmed
that the protocol providing the maximum IC50 value was
drug-specific. This suggests that the adoption of a standard stimulation
protocol would dramatically underestimate or overestimate the blocking
potency of certain drugs. In our opinion, the use of our three proposed
protocols is crucial to build a better picture of the inhibitory effects
and the possible clinical outcomes of a compound.
Impact of the Stimulation Protocol on Blocking
Potency Estimation
Some experimental studies have evidenced
that the blocking potencies of drugs may vary with the stimulus pattern.
Kirsch, et al. 2004[4] used several patch-clamp
voltage protocols to study hERG inhibition of 15 drugs. They found
differences in the IC50 for some drugs, the maximum IC50 ratio being 3.2. Later, Yao et al. in 2005[5] designed two voltage protocols, Protocol-O and Protocol-C,
and compared their results with the SP. BeKm-1, a compound that preferentially
blocks the channel in the closed, showed the biggest differences in
the concentration–response curves. This is in agreement with
our simulations, as most of the highest IC50 ratios correspond
to virtual drugs that exclusively or preferentially bind in the closed
state (see Figure ). However, the IC50 ratios obtained for these drugs in
our simulations are higher than 20 (up to 105.1) while the ratio registered
for BeKm-1 is 10.3. It corresponds to the ratio between the IC50 obtained with a SP over the IC50 obtained with
Protocol-O. Protocol-C revealed a smaller block but, unfortunately,
the concentration–response curve was incomplete and no IC50 was provided. Obtaining the full curve could have provided
a higher IC50 ratio.More recently, Milnes et al.
in 2010[12] studied the effects of the stimulation
protocol on hERG inhibition
for cisapride and dofetilide at 37 °C. They provided maximum
IC50 ratios of 10.3 and 3.75, respectively, when only changing
the voltage protocol. The maximum ratio in our experiments with dofetilide
is 12.8, which is higher than 3.75. This can be because of the differences
on the stimulation protocols and temperature.Our results also
reveal that protocols yielding the maximum IC50 and minimum
IC50 depend on the drug. Our experiments
provided the lowest IC50 value with P-80 in the case of
moxifloxacin and with P0 for dofetilide. Our observation that the
protocol revealing the maximum potency of the block is drug-dependent
is also supported by Yao et al. 2005.[5]Therefore, our study of the impact of the stimulation protocol
on the estimation of current inhibition is in accordance with previous
experiments, but it reveals a more critical role of the voltage protocol.
A very recent investigation has studied protocol-dependent differences
in IC50 and observed that state preferential binding, drug-binding
kinetics and trapping are key factors.[13] Their Markov models included a state-dependent block, but they did
not reproduce other important characteristics, such as closed-state
trapping.[13] Contrarily, our Markovian models
are very comprehensive as they reproduce a state-dependent block,
trapping as well as drug binding and unbinding to any state of the
channels. Moreover, our models can mimic drug-bound channels changing
its conformational state or remaining unchanged.In order to
know if our main results were highly dependent on the
ionic channel model, we repeated some key simulations using two additional
formulations of the hERG channel: Lee et al.[19] and Li et al.[29] models. These two Markovian
models have distinct structures and transition rates, which are also
different from the Fink et al. model. Figures S4 and S5 of the Supporting Information represent the Markovian
schemes (left column) and the simulated Hill plots for each type of
the prototypical drugs binding to two states with state-dependent
affinities using the proposed protocols: P-80 (blue), P0 (red), and
P40 (green) at 22 °C using Lee et al. and Li et al. hERG models,
respectively. These figures show the simulated Hill plots for each
type of the prototypical drug binding to the two states with state-dependent
affinities using the proposed protocols, as in Figure , where they were simulated using the Fink
et al. model.[16] The patterns of the Hill
plots obtained with the three models were very similar, although there
are quantitative differences that affect the values of the maximum
IC50 ratios. In the three cases, the IC50 protocol
dependency relied on the tested compounds and the protocols yielding
the maximum IC50 and minimum IC50 depended on
the drug with the three ionic models. Indeed, both variants of ClosedO_s
(Figures A, S4B and S5B) have the minimum IC50 with P-80 and the IC50 registered with P0 and P40 are
substantially higher. Also, in the case of OpenC_s drugs (Figures B, S4C and S5C), the maximum IC50 was registered with
P-80 and the minimum with P0, which is similar to the one obtained
with P40. In addition, OpenI_s drugs showed small differences of IC50 with the three models (Figures C, S4E and S5E), the minimum IC50 being obtained with P0, although it
could be very similar to the ones registered with the other protocols.
Moreover, the maximum IC50 of InactivO_s was registered
with P-80 with the three models (Figures D, S4F and S5F), and the IC50 values obtained with P0 and P40 were similar.
We have also obtained the Hill plots of unstuck and stuck Inactivated_s
with Lee et al. and Li et al. models (see middle and bottom rows of
Figure S6 of the Supporting Information) and they clearly resemble the ones obtained with the Fink et al.
model (top row of Figure S6 and right panels
of Figure B,C), the
unstuck variant having the same IC50 for the three protocols.
Therefore, there are also drugs that showed no differences or small
differences on the IC50 value when simulated with Lee et
al. and Li et al. models. Overall, the main conclusions of this work
hold when the ionic channel model is simulated with Lee et al. or
the Li et al. models, which have different structures and transition
rates from the Fink et al. model, which suggests that the main conclusions
of this work are not dependent of the ionic model used.
Implications for Drug Safety Assessment
Our work has
important implications for drug safety assessment.
Indeed, one of the most relevant cardiac safety tests of pharmacological
compounds consists of the measurement of hERG IC50 in vitro.[2] As previously explained, other authors have shown
differences on IC50 values, but they were smaller than
in our work, and some of these authors considered that the use of
a certain protocol could be enough for safety studies.[4,5] However, different protocols and temperatures are proposed. Kirsch
and co-workers propose a step-ramp protocol at near-physiological
temperatures,[4] while Yao and colleagues
propose the long-pulse step protocol at room temperature.[5] More recently, the comprehensive in vitro proarrhythmia
assay initiative, led by the FDA, has raised the need of a standardization
of the experiments used to obtain the IC50 values.[30] However, our results suggest that the existence
of a wide variety of drug–channel interactions impairs the
definition of a “standard” protocol to minimize the
influence of the stimulation protocol on the IC50 measurement.
In order to improve the assessment of drug safety, we suggest the
adoption of a three-protocol IC50 assay. Provided that
the differences in IC50 for a compound are small enough,
the IC50 could be used for the assessment of the inhibitory
effects of the compound. On the contrary, supposing the IC50s resulted in very different values, the IC50 would be
a poor indicator. Then, other characteristics, like kinetics and state-dependent
binding properties should be investigated to have a better picture
of the blocking effects of the compound.Although the proposed
protocols do not correspond to electrophysiological conditions, our
simulations with the AP clamp protocols have shown that the Hill plots
obtained with P-80 are close to those obtained with P_AP1 and P0 with
P_AP2 which come from voltage membrane time courses of cells with
a reduced repolarization reserve at slow and fast pacing, respectively.
Therefore, the IC50s obtained from our protocols would
be related to the blocking potencies of the drugs in vivo. However,
considering only these two
IC50 values would be an oversimplification, as electrical
activity is very different during arrhythmic episodes or in the presence
of pathologies, like hypo or hyperkalemia, ischemia, or heart failure.
In addition, the AP waveform is not uniform in the heart. There are
apico-basal and transmural differences. Purkinje AP time courses are
also different from ventricular AP time courses and there is a natural
intersubject variability. These reasons led us to try to design protocols
to infer the drug potency in each conformational state of the channel.
We designed P-80, P0, and P40 to investigate the drug block in the
closed, open, and inactivated states, respectively. Although at 0
mV not all channels are open, the open probability is relatively high
at that voltage. If the IC50s obtained with the three protocols
are similar, we can assume that the channel block that can occur in
any real situation will be similar. On the contrary, if the values
are disparate, the channel block produced by the drug may be extremely
dependent on the situation.Recent works propose alternative
methods to assess the proarrhythmic
risk of drugs by using the modeling and simulation of drug–channel
interactions and considering the kinetics of block.[31−33] Some authors
have even attempted to implement a standardized protocol for the measurement
of kinetics and potency of the hERG block. Unfortunately, their results
highlight the challenges in identifying it over a range of kinetics.[34] We also agree that drug safety assessment would
improve by considering the kinetics of the block, but, to the best
of our knowledge, most pharmaceutical companies are not constructing
mathematical models of drug–hERG interactions based on the
current block measured using a dynamic voltage protocol, which seems
to require a substantial time. Formulation of mathematical models
describing drug–channel interactions is not an easy work. Even
the authors proposing this method obtain different models depending
on the seed used to fit the model,[32] which
may lead to different predictions. In addition, drugs may bind and
unbind the channel by many mechanisms and, as far as we are concerned,
only a few possible types of drug–channel interactions are
being accounted for in these attempts. Indeed, their Markovian models
do not consider the possibility of the drug binding and unbinding
to any channel state and their simulated drug-bound channels have
less conformational states than the unbound channels. Therefore, only
a few types of drug–channel interactions are considered in
these attempts. The above-mentioned restrictions reduce the number
of parameters to be fitted in the process of drug model development
and simplify it. However, it can also lead to a misunderstanding of
the mechanism of drug–channel interaction, which can result
in unrealistic predictions of the effects of the compounds. Therefore,
we suggest the application in the industry of the protocols designed
here. If the three IC50 values are similar, then IC50 is a good indicator of the blocking effects of the compound
and it can be used to predict its proarrhythmic risk, by using the
Tx index[21] for example. Otherwise, the
study of the kinetics and state-dependent binding would be needed
to better characterize it, and the formulation of mathematical models
describing drug–channel interactions would be worthy.
Limitations
Our work suggests the
use of three voltage protocols instead of one when assessing the blocking
potential of drugs. We have applied them to a wide range of virtual
drugs and to two off-the-shelf drugs. Although it is not possible
to experimentally reproduce our simulations, our work would also benefit
from experiments with more types of drugs.We have accounted
for the effect of the temperature on the transition rates between
the channel states. However, the influence of temperature on binding
and unbinding rates of the virtual drugs has not been included as
there is not a universal dependence followed by all compounds.It is to mention that there are factors affecting data interpretation
in ligand binding assays under equilibrium conditions that must be
considered when designing and performing experiments to obtain Hill
plot curves, such as ligand depletion, nonattainment of equilibrium,
buffer composition, and the temperature at which the assay is conducted.[35]All in all, we believe that our three-protocol
hERG-IC50 assay would improve the evaluation of the proarrhythmic
risk of
drugs in the early stages of drug development.
Conclusions
Our work reveals that the evaluation of the
blocking potency of
drugs in the early stages of drug development could be improved by
the use of our three-protocol hERG-IC50 assay, which was
designed to reveal the dissimilarities in the affinity of the drug
to the different conformational states of the channel. Our results
show that the influence of the stimulation protocol on IC50 evaluation depends on the specific IKr–drug interaction. In some cases, the three IC50 values registered for a compound are the same or very similar, then,
the IC50 could be used as an estimator of the inhibitory
potency. However, in other cases, the IC50 estimated by
two different protocols could vary as much as 2 orders of magnitude.
Then, kinetics and state-dependent properties would also be necessary
to predict drug effects. Importantly, as the protocol that provided
the maximum IC50 was specific to the drug, the design of
a “standard” protocol that provides a representative
IC50 value for any compound becomes pointless. To sum up,
adoption of our hERG-IC50 assay on the methods of routinely
evaluating the effects of a drug on hERG channels on safety pharmacology
would ultimately result in more accurate clinical predictions.
Authors: James T Milnes; Christopher E Dempsey; John M Ridley; Olivia Crociani; Annarosa Arcangeli; Jules C Hancox; Harry J Witchel Journal: FEBS Lett Date: 2003-07-17 Impact factor: 4.124
Authors: Jian-An Yao; Xiaoyi Du; Daniel Lu; Robert L Baker; Eric Daharsh; Philip Atterson Journal: J Pharmacol Toxicol Methods Date: 2005 Jul-Aug Impact factor: 1.950
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Authors: Gary R Mirams; Yi Cui; Anna Sher; Martin Fink; Jonathan Cooper; Bronagh M Heath; Nick C McMahon; David J Gavaghan; Denis Noble Journal: Cardiovasc Res Date: 2011-02-07 Impact factor: 10.787
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