Department of Physiology and Biophysics, State University of New
York (SUNY) at Stony Brook, and Department of Anesthesiology, Health
Sciences Center at SUNY Stony Brook, Stony Brook, New York
Competitive antagonists to nicotinic acetylcholine receptors are
clinically used as muscle relaxants. Previously, we reported the
kinetics of inhibition (in the absence of acetylcholine) by (+)-tubocurarine and pancuronium on embryonic receptors. Here, we
examine cisatracurium, a commonly used muscle relaxant.
Outside-out patches were equilibrated with cisatracurium before
application of 300 µM acetylcholine. cisatracurium inhibited the
initial peak current, but the decay of these currents displayed a
pronounced biphasic behavior. The IC50 value was 54 ± 2 nM and 115 ± 4 nM for adult and embryonic receptors,
respectively. We designed a rapid perfusion system to apply or remove
cisatracurium for various times before application of acetylcholine. We
determined the association (embryonic, 3.4 ± 0.4 × 108 M
1 s
1; adult, 1.8 ± 0.3 × 108 M
1 s
1) and
dissociation (embryonic, 34 ± 6/s; adult: 13 ± 5/s) rates for cisatracurium. Association was 2.9- and 1.3-fold greater than that
of (+)-tubocurarine and pancuronium, respectively. Dissociation was 6- and 16-fold higher than (+)-tubocurarine and pancuronium, respectively.
These measurements correspond to dissociation of cisatracurium from
receptors in the absence of acetylcholine. Physiologically,
acetylcholine interacts with receptors equilibrated with antagonist. We
developed a mathematical technique that removes the effect of
desensitization and determined dissociation (embryonic, 52 ± 9/s;
adult, 33 ± 5/s) in the presence of acetylcholine. These data
suggest that presence of acetylcholine on one binding site of the
receptor increases the dissociation rate of antagonist from the other
binding site. We incorporated all of these rates into a computer
simulation of a comprehensive 11-state Markov model. There was
excellent agreement (without curve fitting) between simulated and
experimental currents.
 |
Introduction |
The
nicotinic acetylcholine receptor (nAChR), found on neurons in the
central and peripheral nervous system and muscle cells at the
neuromuscular junction, is the prototypical ionotropic ligand-gated ion
channel (Dilger, 1997
). There are two isoforms of muscle-type nAChR.
The embryonic isoform differs from the adult by one subunit (
instead of
) of five and has a conductance of 40 pS (in the adult,
60 pS) and a mean open-time three times longer than in the adult
isoform. Muscles that are not innervated (i.e., during development)
express only embryonic nAChR that are uniformly distributed at moderate
density in the synapse. During innervation, the embryonic isoform is
replaced by the adult isoform at the synapse; the embryonic isoform is
still present but aggregates around the periphery of the synapse.
Functionally, rapid synaptic transmission is achieved partly because
nAChR is a single protein containing both the ligand-receptor and
ion-channel. Action potentials propagate in the presynaptic nerve
terminal, and ACh is exocytosed into the synapse. ACh diffuses across
the synaptic cleft (~0.2 ms) and binds to sites on muscle-type nAChR
at the
-
(high-affinity) and
-
(low-affinity) subunit interfaces. The channels open for an average of 1 ms and allow the
entry of sodium ions that depolarize the postsynaptic terminal. Under
normal circumstances, the depolarization reaches threshold and the
muscle fiber fires an action potential that results in muscle
contraction. After the channel closes, ACh dissociates and is
hydrolyzed within ~0.2 ms by acetylcholinesterase; the entire
synaptic event is complete within a few milliseconds. The continued
presence of ACh induces nAChR to enter a nonconducting conformation, or
desensitization, with a higher affinity for ACh.
Competitive antagonists to nAChR are clinically used to
immobilize patients during surgery. Several studies have shown they have a higher affinity (as much as 100-fold) for
-
/
site
compared with the
-
site (Arias, 2000
; Fletcher and Steinbach,
1996
). They have little or no efficacy for channel gating, and the
occupancy of only one site is necessary to prevent normal activation by ACh. The binding affinities for several antagonists have been measured,
including (+)-tubocurarine, the prototypical antagonist. Several
studies attempted to determine the kinetics of inhibition for
(+)-tubocurarine but there was little agreement among their findings
(Colquhoun and Sheridan, 1982
; Le Dain et al., 1991
; Aoshima et al.,
1992
; Bufler et al., 1996
). This controversy was recently re-examined
in experiments from our laboratory (Wenningmann and Dilger, 2001
).
From a physiological point of view, determining the association and
dissociation rate constants of competitive antagonists is important
because the free concentration of ACh and the degree of ACh occupancy
on the receptors do not reach equilibrium during a synaptic event.
Moreover, the rates may provide insight into the clinical effects of
competitive antagonists. For example, it may be possible for an
antagonist with a high dissociation rate to dissociate from nAChR
during a synaptic event, thereby allowing ACh to activate these
receptors. Such an antagonist would probably have a lower clinical
potency (compared with an antagonist with a lower dissociation rate).
It might also have a faster clinical onset of action because its
diffusion will be buffered to a lesser extent by the embryonic
(extrajunctional) receptors (Glavinovic et al., 1993
). Finally, these
rates are necessary for the incorporation of antagonists into any model
of the neuromuscular junction.
Here, we examined the kinetics of competitive antagonism by
cisatracurium (cisatr), a commonly-used muscle relaxant with a clinical
potency 10-fold greater than that of (+)-tubocurarine (Savarese et al., 2000
). We made electrophysiological measurements from
outside-out patches containing embryonic or adult wild-type nAChR. In
equilibrium experiments, the patch was preincubated with cisatr before
application of 300 µM ACh. Interestingly, the decay of these
currents displayed a biphasic behavior (secondary increase in current
at high concentrations of cisatr). This biphasic behavior was also
observed for (+)-tubocurarine, albeit to a lesser extent
(Wenningmann and Dilger, 2001
), and it was predicted by others (Aoshima
et al., 1992
). To further investigate this phenomenon, we developed a
rapid perfusion system allowing measurement of the degree of nAChR
inhibition after brief exposure (< 1 ms) or washout of antagonist.
With this system, we determined the association and dissociation rate
constants for cisatr. These measurements correspond to the kinetics of
cisatr antagonism in the absence of ACh. During a synaptic event, ACh
interacts with receptors equilibrated with antagonist. To investigate
this condition, we developed a technique that reveals the time course
of dissociation of antagonist in the presence of ACh. We incorporated
all of these rates into a computer simulation of a comprehensive
11-state Markov model that describes competitive antagonism of cisatr
on embryonic and adult nAChR.
 |
Materials and Methods |
General Methods.
Clonal BC3H1 cells
that express mouse embryonic (
2

)
nAChR (Schubert et al., 1974
) were cultured as described previously (Sine and Steinbach, 1984
). HEK-293 cells were transfected with the
calcium-phosphate precipitation method to express adult
(
2

) nAChR (Prince and Sine, 1996
). At
the time of electrophysiological experiment, the culture medium was
replaced with extracellular solution (ECS) and patch electrodes were
filled with intracellular solution, as described in Wenningmann and
Dilger (2001)
. The three-tube perfusion system used here (Fig.
1) differs from that of Wenningmann and
Dilger (2001)
in that the minimum solution exposure time was 0.5 rather
than 10 ms. The improvement in time resolution was due to a steeper
angle and better alignment between tubes, and uniform high-precision
orifice edges that produced a more laminar flow.

View larger version (34K):
[in this window]
[in a new window]
|
Fig. 1.
Schematic of the 3-tube rapid perfusion system. The
pinch valves controlled the flow of solution through the tubes such
that only one solution was flowing to the patch at any time. The
perfusion system allowed rapid solution exchange (0.1-0.2 ms) between
tubes and a minimum solution exposure time of 0.5 ms. Only two tubes
were used for the equilibrium measurements.
|
|
The currents were measured with a patch clamp amplifier (EPC-9; List
Electronic, Darmstadt, Germany), sampled at 50 µs per point, filtered
at 6.7 kHz, digitized and stored on the hard disk drive of a laboratory
computer (Pentium II 266 MHz, 20 GB hard disk drive). Data were
analyzed with routines (specifically written for each protocol) in
WaveMetrics Igor Pro macro language and imported into Microsoft Excel
for presentation purposes. All data values are expressed as mean ± S.D.
Equilibrium Measurements.
The outside-out patch was
voltage-clamped at
50 or + 50 mV. Only two tubes were used for these
experiments. For the control series, the patch was equilibrated with
ECS for at least 5 s, and then perfused with ECS + ACh for 200 ms.
For the drug series, the patch was equilibrated with ECS + cisatr for
at least 5 s and then perfused with ECS + cisatr + ACh for 200 ms.
These procedures were performed at least 10 times per series per drug
concentration per patch. Control series were performed before and after
all other series on each patch. Data were accepted only when the
recovery was >95%. The ensemble mean current for each series was
calculated from the 10 or more individual current traces.
For control series, the decay of the mean current after the rapid onset
was fit to a one-exponential function: I(t) = I
+ I1
exp(
t/
1),
1 ranging
from 20 to 85 ms. For drug series, a one- or two-exponential function:
I(t) = I
+ I1 exp
(
t/
1) + I2
exp(
t/
2) was used to fit the mean current
decay because the current traces displayed a biphasic behavior in the
presence of high cisatr concentrations. The peak current of the rapid
onset phase reflects the number of channels that were not inhibited by
cisatr during the 5-s exposure to ECS + cisatr, assuming there was no
dissociation of cisatr during the onset phase; this assumption was
justified by results from the kinetic measurements. The ratio of this
current to the peak current from control series
(IDRUG/I0) represents the
fractional inhibition of nAChR by cisatr. The fractional inhibition
values for all patches were plotted as a function of cisatr
concentration and the data were fit to the Hill and two-site binding
model equations [see equations 1 and 2 in Wenningmann and Dilger
(2001)
]. Comparison between two data sets was performed by fitting the
Hill and two-site binding model equations to the fractional inhibition
data for each patch, and the mean IC50, L1, and L2 values were
tested for statistical significance using an unpaired two-tailed
t test.
Measurement of Cisatr Kinetics in the Absence of ACh.
All
three tubes were used for "onset" and "recovery" protocols. The
outside-out patch was voltage-clamped at
50 or + 50 mV. For the onset
protocol, the patch was equilibrated with ECS for at least 5 s
from tube 1, then perfused with ECS + cisatr for varying intervals of
time (0-600 ms) from tube 2, and finally perfused with ECS + cisatr + ACh for 200 ms from tube 3. For the recovery protocol, the patch was
equilibrated with ECS + cisatr for at least 5 s from tube 1, then
perfused with ECS for varying intervals of time (0-600 ms) from tube
2, and finally perfused with ECS + ACh for 200 ms from tube 3. These
procedures were performed for 20 different time intervals per protocol.
Each protocol was repeated at least five times at each concentration of
cisatr per patch (n = 3 per concentration per
protocol). A control series was also performed before and after each
onset and recovery protocol and data were accepted only when the
recovery was >95%. At the end of each experiment, the patch was blown
off the electrode and solution exposure times were ascertained by using
the onset and recovery protocols on the open-electrode using solutions
with different NaCl concentrations. The data analysis was similar to equilibrium experiments. Fractional inhibition was plotted as a
function of cisatr exposure or washout time for onset and recovery protocols, respectively. The data were fit to a one-exponential function.
We often observed a marked, albeit inconsistent, slowing of the onset
and recovery kinetics for cisatr on patches from the HEK-293 cells
transfected with the adult receptor. For example, in the recovery
protocol, even after 600 ms of washout of cisatr (concentrations
ranging from 50 to 3000 nM), the peak currents were only 80 ± 18% (n = 19; ranging from 24 to 100%) of control values. In contrast, after 300 ms of washout of cisatr from patches from BC3H1 cells, peak currents were 101 ± 5% (n = 15) of control values. We observed the same
phenomenon when we transfected the HEK-293 cells with embryonic nAChR,
suggesting that it is specific for this cell line. We considered the
possibility that the HEK-293 cells contain an endogenous binding site
for cisatr. Endogenous muscarinic acetylcholine receptors (mAChR) have
been reported in intact HEK-293 cells using a radiolabeled binding
assay with N-[3H]methylscopolamine
(Zhu et al., 1998
). To our knowledge, the binding affinity of cisatr
for mAChR has not been measured. An in vivo study in cats has reported
that high concentrations of cisatr inhibit the response to vagal
(parasympathetic) nerve stimulation (Wastila et al., 1996
). Moreover,
recent studies using radiolabeled binding assays have shown that
several competitive antagonists to nAChR (including
(+)-tubocurarine) bind to mAChR with affinities in the
micromolar range (Waelbroeck, 1994
; Hou et al., 1998
). More
specifically, the binding affinity of atracurium [consisting of 15%
cisatr in a mixture of nine other isomers (Savarese et al., 2000
)] for
the M2 and M3 subtypes of
mAChR was determined to be 5 and 1.4 µM, respectively (Hou et al.,
1998
). Based on these findings, we hypothesized that the diffusion of
cisatr was buffered by the endogenous mAChR expressed in HEK-293 cells,
thereby affecting our kinetic measurements in the onset and recovery
protocols. Subsequently, we added 1 µM atropine (mAChR antagonist) to
our solutions and the currents recovered to 101 ± 4%
(n = 12) of control values within 600 ms of washout of
cisatr from patches from HEK-293 cells with adult receptors. We note
that 1 µM atropine was used in another study to isolate neuronal
nAChR from mAChR currents in HEK-293 cells (Buisson and Bertrand,
1998
). This concentration of atropine did not affect the peak amplitude
or time course of the currents from our control and drug series. Thus,
we conclude that cisatr inhibition of nAChR is not sensitive to 1 µM
atropine, consistent with the binding affinity of 150 µM measured for
atropine on embryonic nAChR (Amitai et al., 1987
). All data reported
here for adult receptors were obtained in the presence of 1 µM atropine.
Measurement of Cisatr Kinetics in the Presence of ACh.
In
the control series, the decay of the ensemble mean current after the
rapid onset was fit to a one-exponential function: I(t) = I
+ I1
exp(
t/
1); the onset
(k+D) and recovery (k
D) rates of desensitization were
determined from the fit, assuming a simple two-state model (open state
or desensitized state), using the following two equations:
|
(1a)
|
|
(1b)
|
Data were collected using a two-tube perfusion protocol (similar
to that in the drug series) in which the patch was equilibrated with
ECS + cisatr (25, 50, 150, 300, 900, or 3000 nM) for at least 5 s,
and then perfused with ECS + ACh. Using numerical analysis, we
calculated (time step = 50 µs;
t) the fraction of receptors in the desensitized state (OD) as a function of time (t):
|
(2)
|
By adding the fraction of receptors in the open state (O) to OD,
we removed the effects of desensitization with the assumption that the
rates of desensitization are not affected by cisatr. Because activation
of receptors by 300 µM ACh is rapid, the rate-limiting step is the
dissociation of cisatr. Thus, the result of O + OD represents the
apparent time course of cisatr dissociation. By fitting O + OD to a
one-exponential function, the time constant revealed the dissociation
rate constant in the presence of ACh (
'
1;
see Fig. 2). We divided this rate by the
IC50 value (determined from equilibrium
experiments) to calculate the association rate constant in the presence
of ACh (
'+1). The kinetics of cisatr measured
with the O + OD technique from adult receptors were not changed by the
presence of 1 µM atropine. Here, we report the combined data
collected in the absence and presence of 1 µM atropine.

View larger version (17K):
[in this window]
[in a new window]
|
Fig. 2.
11-state model. The model assumes there are two
distinct binding sites for agonist (low-affinity, AR;
high-affinity, RA) and competitive antagonists
(low-affinity, RC; high-affinity, CR), no
single-liganded or hetero-liganded openings, and that the channel opens
(O) before it desensitizes (OD). Rate constants for cisatr in the
absence ( +1 and  1)
and presence ( '+1 and
' 1) of ACh were determined for the
high-affinity binding site in this study. We tested several values for
rates of the low affinity site ( +2,
 2, '+2, and
' 2) consistent with the difference in
affinity between the two binding sites (see Results). We
used rate constants published previously (Zhang et al., 1995 ; Auerbach
and Akk, 1998 ) for ACh binding (k+1,
k 1, k+2, and
k 2) and gating ( and ).
Rate-constants for desensitization (k+D and
k D) were calculated for each patch.
|
|
Measurement of Hetero-Liganded Openings at Low Concentrations of
ACh.
We measured single channel currents from embryonic receptors
with 200 nM ACh in the absence or presence of 300 nM cisatr. We
calculated the number of openings and the mean open and shut times
using the SCAN software
(http://www.ucl.ac.uk/Pharmacology/dcpr95.html). We also measured
current responses to 1 µM ACh with various concentrations of cisatr
and calculated the ensemble mean average. We modified the 11-state
model (Fig. 2) to incorporate a hetero-liganded open state
(one-ACh-bound + one-antagonist-bound open state, where both ligands
are bound to their high affinity site; CRA in Fig. 2), and simulated
currents with 1 µM ACh. We varied the hetero-liganded opening rate
until the simulation matched experimental responses.
Computer Simulation.
Experimental currents were simulated
using Euler's method of numerical integration on a set of equations
from an 11-state model (Fig. 2). The model assumes there are two
distinct binding sites for agonist (low-affinity, AR;
high-affinity, RA) and competitive antagonists
(low-affinity, RC; high-affinity, CR), no
single-liganded or hetero-liganded openings, and that the channel opens
(O) before it desensitizes (OD). The entire model consisted of 10 differential equations and an additional one-exponential equation
describing the time course of solution exchange. Some simulations were
performed assuming a single hetero-liganded open state from CRA in Fig.
2. Rate constants for cisatr in the absence
(
+1 and 
1) and
presence (
'+1 and
'
1) of ACh were determined for the
high-affinity binding site in the previous sections. We tested several
values for rates of the low-affinity site (
+2,

2,
'+2, and
'
2), consistent with the difference in
affinity between the two binding sites determined from equilibrium
measurements. We used rate constants published previously (Zhang et
al., 1995
; Auerbach and Akk, 1998
) for ACh binding
(k+1, k
1,
k+2, and k
2) and gating (
and
). Rate constants for desensitization
(k+D and k
D)
were calculated for each patch as described in the previous section.
Solution of the model involved specifying initial steady-state
conditions (R, CR, RC, CRC; calculated using the two-site binding model
equation) for the differential equations, with subsequent integration
of the equations as a function of time.
The consistency of the relationship between currents generated by the
11-state model simulation and those measured experimentally was
assessed using R2, the coefficient of
determination:
|
(3)
|
The "goodness of fit" between a current measured
experimentally and currents generated by the 11-state model simulation
with varying parameters was assessed using a
2
method:
|
(4)
|
A lower
2 value denotes a better fit.
Differences between
2 values were assessed for
statistical significance using a variance ratio test (Zar, 1999
).
 |
Results |
Equilibrium Measurements.
Representative traces from control
and drug series on embryonic receptors are shown in Fig.
3. For the control series, exposure to
300 µM ACh produced a rapid onset and the peak current represents approximately 95% open channels (Dilger and Brett, 1990
). The current
decays with a time constant of approximately 30 ms as receptors
desensitize in the continued presence of ACh. For the drug series, the
patch was equilibrated with ECS + cisatr, and perfused with ECS + cisatr + ACh for 200 ms. The peak current of the rapid onset phase
represents channels activated by ACh within 100 to 200 µs. The peak
current is reduced with increasing cisatr concentrations (as expected
for a competitive antagonist) because cisatr occupies the ACh-binding
site on nAChR and prevents activation by ACh. However, at high cisatr
concentrations (>50 nM), the currents display a biphasic time course
(after the rapid onset). This biphasic behavior becomes more pronounced
with increasing concentrations of cisatr.

View larger version (25K):
[in this window]
[in a new window]
|
Fig. 3.
Representative traces (alternating black and gray)
from control and drug series on embryonic receptors at 50 mV. For the
control series (0 nM), exposure to 300 µM ACh produced a rapid onset
and the current decays with a time constant of approximately 30 ms as
the receptors desensitize in the continued presence of ACh. For the
drug series, the patch was equilibrated with cisatr, and perfused with
cisatr + ACh for 200 ms. The peak current of the rapid onset phase
represents channels activated by ACh within 100 to 200 µs. The
corresponding cisatr concentrations for each drug series is labeled at
the peak of the rapid onset. The peak current is reduced with
increasing cisatr concentrations. At high cisatr concentrations (>50
nM), the currents display a biphasic time course (after the rapid
onset). This biphasic behavior becomes more pronounced with increasing
concentrations of cisatr. Current jumps seen at 15 and 60 ms are
artifacts caused by activation/deactivation of the solenoid-driven
pinch valves. The inset displays the traces at a higher time resolution
(1-ms separation between tick marks).
|
|
The fractional inhibition (mean ± S.D. for each cisatr
concentration) of embryonic and adult receptors is plotted as a
function of cisatr concentration in Fig.
4. The original data (before averaging for each concentration) were fit to the Hill and two-site binding model
equations; the results are listed in Table
1. The IC50 value
was similar to L1 for both embryonic and adult
receptors. The IC50 (115 ± 4 nM) and
L1 (120 ± 6 nM) values for embryonic receptors are not voltage dependent and are 2-fold larger than those
for adult receptors. The L2 values were 33-, 17- and 8-fold greater than those of L1 for embryonic
(
50 mV), embryonic (+50 mV), and adult receptors, respectively. The
significantly (p < 0.0001) larger S.D. values of
L2 compared with L1 were
related to the lower precision of the data at higher cisatr
concentrations.

View larger version (18K):
[in this window]
[in a new window]
|
Fig. 4.
Concentration-response curve for embryonic ( ) and
adult ( ) receptors at 50 mV. The ratio of the peak current from
drug series to that from control series represents the fractional
inhibition of nAChR by cisatr. They were fit to the Hill equation
(black line) and 2-site binding model (gray line); the fitting
parameters are given in Table 1.
|
|
View this table:
[in this window]
[in a new window]
|
TABLE 1
Results of fitting the Equilibrium concentration-response curves (Fig.
4) to the Hill and two-site binding equations [see Wenningmann and
Dilger (2001) ]
The total number of drug series (n) data for adult, embryonic ( 50
mV), and embryonic (+50 mV) receptors were collected from 20, 6, and 11 patches, respectively. Best fit values are given as mean ± S.D.
The IC50, L1, and L2 values of data from
embryonic receptors ( 50 mV) were tested for statistical significance
(see Materials and Methods) with the corresponding data from
adult and embryonic (+50 mV) receptors. Values for adult receptors were
significantly smaller than those for embryonic receptors
(*p < 0.001). Values for embryonic receptors were not
significantly different at 50 and +50 mV.
|
|
Measurement of cisatr Kinetics Using Onset and Recovery
Protocols.
The three-tube perfusion system (Fig. 1) was used to
measure the kinetics of embryonic and adult nAChR inhibition by cisatr. Results from a typical onset protocol using 300 nM cisatr on embryonic receptors are shown in Fig. 5. With
increasing exposure times, the peak current of the rapid onset phase is
reduced and the rest of the current trace manifests a biphasic
behavior. Even after only 1.4 ms of exposure time, cisatr has occupied
a significant fraction of nAChR such that the current is reduced by
15%. The IDRUG/I0 values
were plotted as a function of cisatr exposure time and fit to a
one-exponential function. The recovery protocol was similar to the
onset protocol; the patch was equilibrated with ECS + cisatr, then
cisatr was washed-off with ECS for various intervals of time (0-600
ms), then the patch was perfused with ECS + ACh for 200 ms. Figure
6 shows an example of an
exposure-response curve from onset and recovery protocols using 300 nM
cisatr on embryonic receptors. The values of
+1 and 
1 were determined by fitting each exposure-response curve to a one-exponential function, assuming a single (high-affinity) site binding model (Fletcher and Steinbach, 1996
):
|
(5)
|
Because ACh is not present, there are no open channels. The time
constant of the one-exponential function is given by:
|
(6)
|
Plots of the reciprocal of the time constant versus cisatr
concentrations from onset and recovery protocols in embryonic and adult
receptors are shown in Fig. 7. The slope
of the plot from onset protocols represents
+1, and the ordinate-intercept represents

1. A more precise estimate of

1 was obtained (average of all points) from
the recovery protocol, and this result was consistent with the

1 measured independently from the onset
protocol. The values of 
1 and
+1 were tested for statistical significance
between adult and embryonic receptors using an unpaired, two-tailed
t test. The results are listed in Table
2. In embryonic receptors,

1 was not significantly different at V = +50 and
50 mV and was 3-fold greater than that for adult receptors.
The
+1 value of embryonic receptors was 2-fold
greater than that of adult receptors. For both adult and embryonic
receptors, 
1/
+1 was
not significantly different from the IC50 value
(Welch-corrected unpaired, two-tailed t test).

View larger version (41K):
[in this window]
[in a new window]
|
Fig. 5.
Results from a representative onset protocol using
300 nM cisatr on embryonic nAChR at 50 mV. The cisatr exposure times
were: 0, 1.4, 2.2, 2.4, 3.0, 3.2, 3.5, 4.3, 4.6, 5.1, 5.9, 6.7, 7.7, 9.1, 10.4, 12.8, 15.4, 18.8, 23.5, 30.0, and 37.7 ms. The
bold-faced exposure times correspond to the black traces. With
increasing exposure times, the peak current of the rapid onset phase is
reduced and the rest of the current trace manifests a biphasic
behavior. The inset displays the traces at a higher time resolution
(1-ms separation between tick marks).
|
|

View larger version (18K):
[in this window]
[in a new window]
|
Fig. 6.
Exposure-response curves for onset ( , data from
Fig. 5) and recovery ( ) experiments on a single patch using 300 nM
cisatr on embryonic receptors at 50 mV. The fractional inhibition of
nAChR by cisatr was plotted as a function of cisatr exposure or washout
time. Each curve was fit (gray line) to a one-exponential function and
the reciprocal of the time-constant was used to determine the
association and dissociation rate constants.
|
|

View larger version (22K):
[in this window]
[in a new window]
|
Fig. 7.
The reciprocal of the time constant measured from
exposure-response curves of onset and recovery protocols in embryonic
(solid gray markers) and adult (open markers) receptors at 50 mV
plotted as a function of cisatr concentration (three patches per cisatr
concentration). The slope of the plot from onset protocols (circles)
represents the association rate constant and the ordinate-intercept
represents the dissociation rate constant. A more precise estimate of
the dissociation rate constant was obtained (average of all points)
from the recovery (squares) protocol.
|
|
View this table:
[in this window]
[in a new window]
|
TABLE 2
Results of kinetic experiments obtained from fitting the data in Figs.
5, 6, 7, and 8
The association ( +1 Onset) and dissociation ( 1
Onset) rate constants in the absence of ACh determined with the onset
protocol, dissociation rate constant in the absence of ACh
( 1 Recovery) determined with the recovery protocol, the
calculated equilibrium constant in the absence of ACh ( 1
Recovery/ +1 Onset), and the dissociation rate constant in
the presence of ACh ( ' 1 O + OD) determined with the
O + OD protocol for cisatr on embryonic and adult receptors are
reported as mean ± S.D.; the number of data points are included
within parentheses. The last two rows refer to the kinetics of
(+)-tubocurarine and pancuronium in the absence of ACh from Wenningmann
and Dilger (2001) .
|
|
Measurement of cisatr Kinetics in the Presence of ACh Using
Numerical Analysis.
In the absence of desensitization, it would be
relatively easy to determine the dissociation rate of a competitive
antagonist in the presence of ACh. If the patch is equilibrated with
ECS + cisatr, and then perfused with ECS + ACh, there will be a rapid onset (representing activation by ACh of nAChR not occupied by cisatr)
followed by a secondary increase in current on a slower time scale
(representing activation by ACh as cisatr dissociates from nAChR). This
slower second component would increase until all cisatr molecules had
dissociated from nAChR and the current reached the same steady-state
level as control. The time constant of an exponential fit to the second
component would represent the dissociation rate constant. The fast time
course of desensitization precludes such a simple measurement. It
should be possible, however, to remove the effects of desensitization
and extract the kinetic information from experimental data.
A two-tube perfusion protocol was used to equilibrate the patch with
cisatr and then simultaneously (within 200 µs) remove cisatr and
activate channels with ACh. An example with 300 nM cisatr is shown in
Fig. 8b. We transformed the current using
numerical integration (see Materials and Methods) to
calculate the time course of the sum of the number of open and
desensitized channels (O + OD). We fit O + OD to a one-exponential
function and the reciprocal of the time constant revealed
'
1, the dissociation rate constant for
cisatr in the presence of ACh. The value of
'
1 was tested for statistical significance
between embryonic and adult receptors and compared with the
corresponding 
1 (dissociation rate constant
in the absence of ACh) from embryonic and adult receptors using an
unpaired, two-tailed t test. The results are listed in Table
2. The value of
'
1 was 2.6- and 1.5-fold
greater than that of 
1 for adult and
embryonic receptors, respectively. The value of
'
1 for embryonic receptors was 1.6-fold
higher than that of adult receptors.

View larger version (13K):
[in this window]
[in a new window]
|
Fig. 8.
Results from a representative O + OD protocol using
300 nM cisatr on embryonic nAChR at 50 mV. A, a control current (gray
trace) and the corresponding O + OD calculation (black trace), which
was a linear horizontal trace (with negligible slope) after the peak
rapid onset, suggesting that before desensitizing, most channels are in
the open state with 300 µM ACh. B, a 300 nM cisatr washoff current
(gray trace). A two-tube perfusion protocol was used to equilibrate the
patch with cisatr and then simultaneously (within 200 µs) remove
cisatr and activate channels with ACh. The corresponding O + OD
calculation (black trace) was fit (superimposed gray trace) to a
one-exponential function and the reciprocal of the time constant (20 ms) revealed the dissociation rate constant for cisatr in the presence
of ACh.
|
|
We also calculated O + OD for control currents (Fig. 8a); these yielded
a linear horizontal trace (with negligible slope) after the peak rapid
onset, suggesting that before desensitizing, most channels are in the
open state at 300 µM ACh.
Another two-tube perfusion protocol was used in which the patch was
equilibrated with ECS and then perfused with ECS + cisatr + ACh. The
peak amplitude and time course of the currents (including rates of
desensitization) were the same as control, suggesting that cisatr does
not produce any noncompetitive effects at the concentrations used in
our study.
Measurement of Hetero-Liganded Openings at Low Concentrations of
ACh.
Several competitive antagonists, including atracurium,
activate a one-ACh-bound + one-antagonist-bound (hetero-liganded) open state in embryonic receptors (Fletcher and Steinbach, 1996
). To determine whether this is also true for cisatr, we performed
single-channel experiments at low concentrations of ACh. cisatr did not
activate any channels by itself. There were fewer openings (65 ± 8% of control; n = 3) with 0.2 µM ACh and 300 nM
cisatr than with 0.2 µM ACh alone. However, based on macroscopic
current measurements with 300 µM ACh and 300 nM cisatr
(n = 4), we expected the number of openings to be
26 ± 3.5% of control. The greater number of openings at 0.2 µM
ACh suggested the activation of a hetero-liganded open state.
Consistent with the number of openings, the mean shut time was 2-fold
greater in the absence than in the presence of cisatr. The mean open
time (~2 ms) was similar under both conditions, suggesting that the
closing rate of the hetero-liganded open state was ~500/s. Next, we
measured currents at 1 µM ACh with various concentrations of cisatr.
Again, there was less inhibition by cisatr than predicted by the
IC50 value. By comparing these currents with
simulated currents using a 12-state model (Fig. 2 with a second open
state from CRA), we estimated the hetero-liganded opening rate to be
~25/s. The efficacy of cisatr hetero-liganded openings (25/s /
500/s = 0.05) is similar to that reported for atracurium (Fletcher
and Steinbach, 1996
).
Computer Simulation.
The purpose of performing computer
simulations using the 11-state model was to try to reproduce the
experimental results, using rate constants for cisatr determined in the
previous sections, without implementing any optimization or
curve-fitting routines. We used rate constants published previously for
ACh binding and gating for embryonic (Zhang et al., 1995
) and adult
receptors (Auerbach and Akk, 1998
). Rate constants for desensitization
were determined for each patch; the values of
k+D and k
D ranged from 65 to 10/s and 5.5 to 0.064/s, respectively. First, we
examined the agreement between experimental currents from equilibrium measurements and simulated currents using the mean values of the rates
determined experimentally. The simulated currents accurately reproduced
the peak amplitude and time course of experimental currents
(R2 ranging from 0.95 to 1.00). The
results of six representative simulations compared with experimental
data from the same patch containing embryonic receptors are illustrated
in Fig. 9. The agreement between
simulated and experimental currents deteriorated with an increase in
cisatr concentration. This slight deterioration in
R2 may be attributable, in part, to the smaller
(noisier) currents at high cisatr concentrations. The agreement could
be further improved by varying 
1 or
'
1 around the mean measured value, but
without exceeding 1 S.D.

View larger version (21K):
[in this window]
[in a new window]
|
Fig. 9.
Comparison between 11-state-model simulation using
experimentally-measured mean values (black trace) and drug series (gray
trace) from embryonic receptors at 50 mV. The
R2 (eq. 3) between simulated currents and
experimental traces for 0, 25, 50, 150, 300, and 900 nM cisatr was
0.998, 0.997, 0.995, 0.986, and 0.984, respectively. The rate constants
used for this simulation were (in micromolar 1
s 1 or s 1): +1 = 340;
 1 = 34; +2 = 340;
 2 = 1122; '+1 = 440;
' 1 = 52; '+2 = 440;
' 2 = 1716; k+1 = 39; k 1 = 1241;
k+2 = 91;
k 2 = 5649; = 27000; = 376; k+D = 41; and
k D = 0.53.
|
|
Next, we examined the contribution of some states and kinetic
components to the overall shape of the current. For example, we could
not directly measure
'+1 and the kinetics of
cisatr binding to the low-affinity site. Even when we increased or
decreased
'+1 by 4-fold, the simulation was
not sensitive to this parameter. However, the time course of the
simulated currents deviated from experimental currents when the
L2 < 10 · L1,
suggesting that there is at least a 10-fold difference in affinity
between the two cisatr binding sites. Because our calculation of
+1 and 
1 assumed a
single (high-affinity) site binding model (eq. 5), we simulated onset
and recovery protocols and varied the dissociation rates for the two
sites from unity to a 1000-fold difference. The kinetics measured from
the simulated currents were not sensitive to the difference in binding
affinity between the two sites and whether the low-affinity site had a
slower association or faster dissociation rate. In addition, the
simulation was not sensitive to whether or not the high-affinity
binding site for ACh and cisatr were the same. To determine the
validity of the O + OD technique, we performed simulations using
different values for
'
1 and

1 and calculated O + OD for the simulated currents. By fitting O + OD to a one-exponential function, the reciprocal of the time constant was equal to the
'
1 that we used to simulate the currents. We
also performed simulations by modifying the 11-state model to
incorporate the hetero-liganded open state. This increased the
simulated currents by 6% or less and, in some cases, improved the
agreement with experimental data from embryonic receptors.
Finally, we investigated the different roles of

1 and
'
1 by
comparing our previous results with simulations using

1 =
'
1 or
'
1 = 
1. The
accuracy of the simulated currents deteriorated at high cisatr
concentrations, suggesting that a distinct difference in the rates
(
1 and
'
1) is
necessary to accurately describe the experimental currents. A
comparison at 900 nM cisatr is shown with adult receptors in Fig.
10. In this example, the simulation
using 
1 and
'
1
produced a current-trace that matched the experimental current
significantly better than the simulation using
'
1 = 
1.

View larger version (16K):
[in this window]
[in a new window]
|
Fig. 10.
Comparison between 11-state-model simulation using
experimentally-measured mean values (black trace) and drug series using
900 nM cisatr (gray trace) from adult receptors at 50 mV. The
simulated current ( 2 = 1.41;
R2 = 0.974) using distinct rates for
 1 and ' 1 agreed significantly better
(p < 0.0001) with the experimental trace than
simulated currents ( 2 = 1845.3;
R2 = 0.598) using the same rate for
 1 and ' 1. The rate constants used for
this simulation were (in micromolar 1 s 1 or
s 1): +1 = 180;
 1 = 12.6; +2 = 180;
 2 = 113; '+1 = 429;
' 1 = 32.9; '+2 = 429;
' 2 = 296; k+1 = 220; k 1 = 18000;
k+2 = 110;
k 2 = 36000; = 50000;
= 1200; k+D = 26; and
k D = 0.13.
|
|
 |
Discussion |
cisatr is one (R-cis, R'-cis) of a
mixture of 10 isomers that constitutes atracurium. Fletcher and
Steinbach (1996)
, using radiolabeled binding experiments, predicted the
IC50 value of atracurium to be 270 and 135 nM for
embryonic and adult receptors, respectively. Consistent with their
findings, we found that the IC50 value of cisatr
for embryonic receptors is 2-fold higher than that for adult receptors.
Although we did not directly measure binding, it was possible to
estimate binding affinities because the kinetics of cisatr are
rate-limiting in the presence of 300 µM ACh. Cisatr has a 2- to
3-fold higher affinity than atracurium, consistent with the difference
in their clinical potencies (Bryson and Faulds, 1997
). Cisatr has no
appreciable voltage-dependence for competitive inhibition, as reported
for (+)-tubocurarine (Colquhoun et al., 1979
). In embryonic
receptors, there was about a 33-fold difference in affinity between the
two binding sites. Consistent with this result, the Hill coefficient of
1.0 suggests that cisatr is interacting primarily with one site (Sine
and Taylor, 1981
). For adult receptors, there is a difference between
the two affinities of
8-fold. This is greater than that reported
for atracurium but is consistent with the lower Hill coefficient of
cisatr compared with that of atracurium (Fletcher and Steinbach, 1996
).
It was necessary to incorporate the low-affinity site into the 11-state model simulations to accurately simulate experimental traces from adult
receptors, but not embryonic receptors, at cisatr concentrations
150 nM.
In the equilibrium measurements, ACh was applied to an outside-out
patch in the constant presence of cisatr. Cisatr inhibited the initial
peak inward currents in a concentration-dependent manner. At low
concentrations (<50 nM), the decay time course was similar to that of
control. However, at higher concentrations, after the initial rapid
activation, the decay exhibited a slow secondary increase in current
before desensitizing. A similar, albeit smaller, biphasic behavior was
also observed for (+)-tubocurarine (Wenningmann and Dilger,
2001
). To further investigate this phenomenon, we first considered the
possibility that a hetero-liganded open conformation of the channel was
being activated. We incorporated the kinetics of this state into our
simulations. However, the opening rate was too small to account for the
observed currents. Moreover, the biphasic behavior was also present in
adult receptors, which do not exhibit hetero-liganded openings
(Fletcher and Steinbach, 1996
). Our next hypothesis was that cisatr
dissociates from the receptors on the millisecond time scale and, as
cisatr dissociates, ACh (present at saturating concentrations) binds to
the receptors and activates the channels. To test this hypothesis, it
was necessary to determine the kinetics of inhibition.
Using the onset and recovery protocols, we determined the association
and dissociation rate constants for cisatr. Because ACh is not present
during the interval when cisatr is being added or removed, these rates
represent transitions between states CR
R in Fig. 2. There is
excellent agreement between the antagonist affinity determined from
these kinetic experiments (Table 2) and that obtained from equilibrium
experiments (Table 1). The association rate is 20-fold greater than
that reported for ACh in embryonic receptors (Zhang et al., 1995
) and
comparable with that reported for ACh in adult receptors (Auerbach and
Akk, 1998
). Because cisatr is about 10-fold larger than ACh, its high
association rate suggests that it may not compete with ACh for the
putative agonist-binding site (Miyazawa et al., 1999
). Instead, it may bind at or near the tunnel entrance and sterically hinder the entrance
of ACh into the tunnel, as suggested by Wenningmann and Dilger (2001)
.
The association rate is probably not diffusion-limited; it is
antagonist-specific: cisatr has a significantly larger association rate
than pancuronium (1.3-fold) and (+)-tubocurarine (2.9-fold). The association rate of cisatr for embryonic receptors is 2-fold greater than that for adult receptors, suggesting that the
-subunit contributes additional diffusion barriers to cisatr than the
-subunit.
The dissociation rate of cisatr is markedly higher than that of
(+)-tubocurarine (6-fold) and pancuronium (16-fold). The
rapid dissociation rate is consistent with our hypothesis: in an
equilibrium measurement, cisatr dissociates at a rate faster than or
comparable with the rate of desensitization and allows ACh to bind to
and activate additional receptors. The excellent agreement between equilibrium measurements and the 11-state model simulation provided a
quantitative demonstration that the biphasic time course is caused by
antagonist dissociation. Moreover, it helped to establish the accuracy
of the rates measured experimentally and provided a quantitative
assessment of the contribution (or lack of) for each state and kinetic
component. Finally, it demonstrated that an 11-state model is
sufficient to describe competitive antagonism of nAChR.
At a synapse, antagonists interact with the receptor both in the
presence (CRA 171 RA in Fig. 2) and absence (CR
R) of ACh. Thus, we
developed a mathematical technique that removes the effect of
desensitization to determine the dissociation rate of an antagonist in
the presence of ACh. For both adult and embryonic receptors, we found
that the dissociation rate of cisatr in the presence of ACh was
significantly larger than that in the absence of ACh. These distinct
rates were necessary for the 11-state model simulation to describe
accurately the experimental currents (Fig. 10). These findings suggest
that the presence of ACh on one site decreases the affinity of cisatr
for the other site, at least by increasing its dissociation rate.
Consistent with this concept, a study using fluorescence binding assays
reported that the binding of ACh or antagonist to one site on
Torpedo californica nAChR causes a conformational change that alters the affinity of the other site (Covarrubias et al.,
1986
). More recently, it has been shown the binding of ACh to the
receptor causes a "conformational wave" to spread throughout the
whole receptor, and a low-to-high affinity change for ACh at the
transmitter-binding sites precedes the complete opening of the pore
(Grosman et al., 2000
). Because single-liganded openings have been
observed in embryonic receptors (Sine and Steinbach, 1986
; Parzefall et
al., 1998
), it is plausible that the binding of ACh to a single site
causes a global conformation change that alters the affinity of the
other site.
There is a large margin of safety (~80%) for competitive antagonism
of nAChR at the neuromuscular junction (Paton and Waud, 1967
). More
than 95% of the receptors are occupied during clinical administration
of cisatr. Because cisatr dissociates at a rate of 52/s in the presence
of ACh at room temperature, during synaptic transmission (~2 ms),
about 10% of the receptors [Free R = 1
exp(
0.002 × 52)], may become unoccupied (possibly more at
37°C). In the presence of saturating concentrations of ACh, the
kinetics of cisatr is determined by the dissociation rate rather than
the association rate (see simulation results). This should reduce the
potency of cisatr during synaptic transmission. The direct clinical
implications of this are not clear. Monte Carlo simulations are
required to provide further insight.
Our results show that cisatr has a markedly higher
IC50 value than (+)-tubocurarine or
pancuronium, primarily because of its high dissociation rate. An
antagonist with a higher dissociation rate should have a faster
clinical onset time for muscle relaxation because it will equilibrate
faster with junctional receptors (Rang, 1974
) and its diffusion will be
buffered to a lesser extent by extrajunctional receptors (Glavinovic et
al., 1993
). However, our results are not consistent with clinical
observations that cisatr has a significantly slower clinical onset time
than pancuronium (1.2-fold) and (+)-tubocurarine (1.7-fold)
(Kopman, 1989
; Kopman et al., 1999
). Moreover, the clinical potency of
cisatr is 1.3- and 10-fold greater than that of pancuronium and
(+)-tubocurarine, respectively (Savarese et al., 2000
). The
disparity may be related to temperature. For pancuronium, there was a
2-fold decrease in potency from 29 to 38°C in cats (Miller et al.,
1978
), in contrast to an increase in potency for
(+)-tubocurarine (Ham et al., 1978
). In denervated rat
hemidiaphragm, there was a 10-fold increase in the apparent binding
affinity of (+)-tubocurarine from 22 to 30°C (Banerjee and
Ganguly, 1996
). However, this finding was obtained using muscle
contraction, a very indirect indicator of antagonist activity.
Nevertheless, a study using a radiolabeled binding assay on T. californica electric organ membranes, reported a 10-fold increase
in the binding affinity of (+)-tubocurarine (for open-channel block) from 22 to 37°C (Shaker et al., 1982
). To our knowledge, the
temperature-dependence of cisatr has not been studied. Studies with
other competitive antagonists suggest that they are selectively sensitive to temperature and have varying degrees of responses (Yoneda
et al., 1991
). Therefore, it is necessary to conduct direct kinetic
measurements at 37°C to increase our understanding of the clinical condition.
We thank Ms. Claire Mettiwie for help with tissue culture and
transfection; Dr. David Colquhoun for insightful suggestions; Drs. Leon
Moore and Chris Clausen for advice on statistical analyses; Dr. Cesar
Labarca for providing the
,
, and
cDNA; and Dr. Steven Sine
for providing the
cDNA.
This research was supported in part by a grant from the
National Institute of General Medical Sciences (GM42095), and the Department of Anesthesiology, State University of New York at Stony
Brook. These data were presented at the 44th and 45th Annual Meetings
of Biophysical Society: Biophys J 78:359,
2000; Biophys J 80:463, 2001; and Biophys
J 80:462, 2001.
James P. Dilger, Ph.D.,
Department of Anesthesiology, Health Sciences Center L4, SUNY at Stony
Brook, Stony Brook, NY 11794-8282. E-mail:
jdilger{at}epo.som.sunysb.edu
nAChR, nicotinic acetylcholine receptor;
ACh, acetylcholine;
cisatr, cisatracurium;
HEK, human embryonic kidney;
ECS, extracellular solution;
mAChR, muscarinic acetylcholine receptor;
OD, desensitized state;
O, open state.