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The Journal of Neuroscience, December 15, 1999, 19(24):10635-10646
The General Anesthetic Propofol Slows Deactivation and
Desensitization of GABAA Receptors
Donglin
Bai1,
Peter S.
Pennefather2,
John F.
MacDonald1, and
Beverley A.
Orser1, 3, 4
1 Departments of Physiology, 2 Faculty of
Pharmacy, 3 Department of Anaesthesia, University of
Toronto, Toronto, Ontario, Canada M5S 1A8, and 4 Sunnybrook
Health Science Centre, Toronto, Ontario, Canada M4N 3M5
 |
ABSTRACT |
Propofol (2,6-di-isopropylphenol) has multiple actions on
GABAA receptor function that act in concert to potentiate
GABA-evoked currents. To understand how propofol influences inhibitory
IPSCs, we examined the effects of propofol on responses to brief
applications of saturating concentrations of GABA (1-30
mM). GABA was applied using a fast perfusion system to
nucleated patches excised from hippocampal neurons. In this
preparation, propofol (10 µM) had no detectable agonist
effect but slowed the decay, increased the charge transfer (62%), and
enhanced the peak amplitude (8%) of currents induced by brief pulses
(3 msec) of GABA. Longer pulses (500 msec) of GABA induced responses
that desensitized with fast (
f = 1.5-4.5 msec) and
slow (
s = 1-3 sec) components and, after the
removal of GABA, deactivated exponentially (
d = 151 msec). Propofol prolonged this deactivation (
d = 255 msec) and reduced the development of both fast and slow
desensitization. Recovery from fast desensitization, assessed using
pairs of brief pulses of GABA, paralleled the time course of
deactivation, indicating that fast desensitization traps GABA on the
receptor. With repetitive applications of pulses of GABA (0.33 Hz), the
charge transfer per pulse declined exponentially (
15 sec)
to a steady-state value equal to ~40% of the initial response.
Despite the increased charge transfer per pulse with propofol, the time
course of the decline was unchanged. These experimental data were
interpreted using computer simulations and a kinetic model that assumed
fast and slow desensitization, as well as channel opening developed in
parallel from a pre-open state. Our results suggest that propofol stabilizes the doubly liganded pre-open state without affecting the
isomerization rate constants to and from the open state. Also, the rate
constants for agonist dissociation and entry into the fast and slow
desensitization states were reduced by propofol. The recovery rate
constant from fast desensitization was slowed, whereas that from slow
desensitization appeared to be unchanged. Taken together, the effects
of propofol on GABAA receptors enhance channel opening,
particularly under conditions that promote desensitization.
Key words:
propofol; GABAA receptors; desensitization; kinetics; nucleated patch; hippocampal neurons; patch clamp; anesthetics
 |
INTRODUCTION |
Many general anesthetics, including
propofol (2,6-di-isopropylphenol), prolong the duration of GABAergic
IPSCs, and this action is thought to contribute to the behavioral
properties of these drugs (MacIver et al., 1991
; Orser et al., 1994
).
Previous studies using conventional multibarrel perfusion systems and
whole-cell recordings indicate that propofol has multiple distinct
effects on GABAA receptor (GABAAR) function,
including the potentiation of GABA-evoked currents, direct activation
of the receptor, and modulation of desensitization (Hales and Lambert,
1991
; Hara et al., 1993
; Orser et al., 1994
). In those studies,
concentration-response relationships were constructed to reflect the
interaction between the drug and receptor under near-equilibrium
conditions. However, synaptic currents are generated by transient
pulses of high concentrations of GABA, and at no time during the
response is there equilibrium. It is not certain how the multiple
actions of propofol will combine under nonstationary conditions to
modify IPSCs.
The shape of IPSCs is determined by several factors, including the
concentration and temporal profiles of the neurotransmitter in the
synaptic cleft, as well as the kinetic properties of postsynaptic receptors. It is generally believed that a saturating concentration of
GABA is released into the synaptic cleft from the presynaptic terminal
(Maconochie et al., 1994
; Jones and Westbrook, 1995
) (but see Frerking
et al., 1995
). Most of the free GABA is likely cleared from the cleft
by the time the IPSC reaches its peak (Jones and Westbrook, 1996
;
Uteshev and Pennefather, 1996a
). Thus, the slow decay of IPSCs
primarily reflects receptor gating and the unbinding of agonist rather
than diffusion of transmitter within the cleft.
To investigate the physiological and pharmacological properties of the
GABAAR under non-equilibrium conditions (as might occur in
the synaptic cleft), several groups have applied high concentrations of
agonist (>500 µM) to excised outside-out and nucleated
membrane patches (Celentano and Wong, 1994
; Maconochie et al., 1994
;
Jones and Westbrook, 1995
; Galarreta and Hestrin, 1997
). In these
studies, GABAARs display a complex pattern of
desensitization, which includes a fast component of desensitization
(
f, <100 msec) that is evident when GABA is
applied using fast perfusion systems (open tip exchange time <2 msec).
This form of desensitization appears to buffer the channel in an
agonist-bound conformation that permits the channel to reopen long
after free GABA has been removed. Recovery of the receptor from the
desensitized state, through a ligand-bound pre-open state with the
opportunity for reopening, contributes to the slow decay of IPSCs
(Jones and Westbrook, 1995
; Jones et al., 1998
). In addition, a slower
desensitization process (
~ 3 sec) is evident during longer
applications of GABA (Orser et al., 1994
; McClellan and Twyman,
1999
).
We previously demonstrated, using conventional perfusion systems and
whole-cell recording methods, that propofol decreases the rate and
extent of slow desensitization (Orser et al., 1994
). Here we studied
the effects of propofol on GABAARs using fast applications
of high GABA concentrations to nucleated patches. We discovered that
fast desensitization and deactivation are also slowed. To assist with
the interpretation of the experimental data, computer simulation was
undertaken using a simple kinetic model of GABAAR gating
similar to that proposed by Celentano and Wong (1994)
. This kinetic
model assumes that fast and slow desensitization, as well as channel
opening, develop in parallel as absorbing states from a pre-open state.
An equal decrease by propofol in the rate of dissociation of GABA from
the pre-open state and the rate constants of entry into fast and slow
desensitization states adequately accounts for our experimental data.
Additionally, propofol reduced the rate of recovery from fast
desensitization. Otherwise, the other kinetic parameters can remain
unchanged. The slowing of fast desensitization accounts for the
observed increase in the amplitudes of the peak and early plateau of
the response. Because fast desensitization is slowed but is not greatly
reduced, the pronounced effect of propofol on deactivation indicates
that propofol must also reduce the rate of dissociation of GABA. In
summary, our results suggests that propofol prolongs IPSCs by
stabilizing the fully liganded pre-open state of the receptor.
 |
MATERIALS AND METHODS |
Cell culture. Cultures of embryonic hippocampal
neurons were prepared from Swiss white mice as described previously
(MacDonald et al., 1989
). Briefly, fetal hippocampi were obtained from
mice killed by cervical dislocation. Neurons were dissociated using mechanical trituration and plated on 35 mm collagen-coated culture dishes. Monolayers of cells were formed after 12-16 d in
vitro. Before recording, cells were rinsed with a standard
extracellular recording solution containing (in mM): 140 NaCl, 1.3 CaCl2, 5.4 KCl, 2 MgCl2, 25 HEPES, and 33 glucose, with the pH
adjusted to 7.4 with 1 M NaOH. All experiments were
conducted at room temperature (22-25°C).
Electrophysiology. Recording pipettes were prepared from
borosilicate glass capillaries containing an inner filament (World Precision Instruments, Sarasota, Florida). Electrodes were pulled in
two stages using a vertical puller (Narishige PP-83) and had a
resistance of 4-7 M
when filled with a solution containing (in
mM): 120 CsCl, 30 HEPES, 11 EGTA, 2 MgCl2, 1 CaCl2, and 4 MgATP, with
the pH adjusted to 7.3 with CsOH. The osmolarity of the pipette
solution was adjusted to 300-315 mOsm. Voltage-clamp (VH =
60 mV) whole-cell currents were
recorded using a patch-clamp amplifier (Axopatch 1-D, Axon Instruments,
Foster City, CA). Currents were recorded simultaneously on a chart
recorder (Astro-Med MT8800, West Warwick, RI), a video tape recorder
through a converter (VR10, Instrutech, Elmont, NY), and a PC computer
using pClamp Software (Axon Instruments).
GABA-induced currents were recorded from nucleated patches formed from
cultured hippocampal neurons as described previously (Sather et al.,
1992
). A double-barrel perfusion pipette made from theta tubing (R&D
Scientific Glass Co., Spencerville, MD) was attached to a
piezo-electric translator (PZS-100, driven by PZ-150; Burleigh,
Fishers, NY). This assembly permitted the rapid switching of the
solutions bathing the patches. The open tip solution exchange time was
determined by examining the current produced by a change to a dilute
extracellular solution (10-20% with water). Under optimum conditions,
the open tip exchange time was ~0.2 msec. The exchange time for
solutions bathing the nucleated patch was also determined by measuring
the rise time (10-90%) of current associated with an increase in the
extracellular concentration of K+. The recording
electrode was filled with a solution containing (in mM):
140 CsF, 35 CsOH, 10 HEPES, 2 MgCl2, 1 CaCl2, 11 EGTA, 2 tetraethylammonium (TEA), and 4 KATP. The pH was adjusted to 7.3 using CsOH. The extracellular
concentration of K+ was increased from 5 to 50 mM, and the Na+ concentration was
reduced by 50 mM. The osmolality of the solutions was
unchanged. At a holding potential of 0 mV, the inward current associated with the switch to the high K+ solution
had a rise time (10-90%) of 1.9 ± 0.5 msec (n = 6 patches).
The time interval between the 3 and 500 msec applications of GABA was
at least 30 and 120 sec, respectively. Under these conditions, little
"rundown" (diminished peak responses with time) was observed for
GABA-induced current responses. Patches that displayed a rundown greater than ~2% per agonist application were discarded.
Propofol was prepared on the day of experiment from Diprivan (Zeneca
Pharma, Mississauga, Canada). The effects of propofol on GABA-evoked
currents were studied after control recordings were obtained. Propofol
was allowed to pre-equilibrate for at least 2 min, and the vehicle
Intralipid (KabiVitrium Canada, Toronto, Canada) was included in the
control solutions.
Data were expressed as the mean ± SEM, and a paired Student's
t test was used to examine the statistical significance of
differences between the groups. For multiple groups of data, a two-way
ANOVA was used (GraphPad Software, San Diego, CA). A p value
<0.01 was considered to be significant.
Simulation. A general simulator program Axon Engineer (Aeon
Software, Minneapolis, MN; http://userpages.itis.com/aeonsoft/) was
used to simulate the data. This program allows kinetic states to be
defined and linked together by rate constants that can be a function of
voltage, ion, and drug concentration. The differential equations
implicit in the kinetic scheme are then integrated and driven by
user-defined stimuli. The distribution of states in time is converted
to open probability by assigning conductance weights to the individual
states and summating the system at each time point. Given the
difficulty in obtaining results with nucleated patches and the
relatively high degree of variability of responses between patches, we
did not feel that there was sufficient data to warrant an exhaustive
parameter optimization effort. Rather, a range of rate constants was
deduced by the analysis of a three-state approximation of our kinetic
model (see Appendix).
 |
RESULTS |
Kinetics of GABA-induced current recorded from
nucleated patches
To investigate the mechanisms underlying propofol-induced changes
in postsynaptic GABAA receptor function, currents were
activated by rapid applications of GABA (1-30 mM) to
nucleated patches. The method used for rapid exchange of extracellular
bathing solutions is illustrated in Figure
1A. Responses evoked from a
single nucleated patch by applications of 1 mM GABA for 3, 30, 300, and 1000 msec are shown (Fig. 1B). Brief pulses of
GABA (3 msec) induced transient currents that peaked with a rapid onset
[10-90% rise time (RT) = 2.0 ± 0.2 msec,
n = 26], then declined to baseline in a biphasic manner. The time-to-peak for GABA-evoked currents has previously been
reported to be
1 msec (Maconochie et al., 1994
; Puia et al., 1994
).
We attribute the slower time course observed in our experiments to the
slower speed of the agonist application to nucleated patches. The rise
time for GABA-evoked responses in nucleated patches was similar to that
of the currents associated with an increase in the extracellular
concentration of K+ (see Materials and Methods).
This observation suggests that the binding of GABA to the receptor is
fast, and in this preparation the rate of current onset is limited by
the rate of solution exchange. The fast component of the decay with the
brief 3 msec application of GABA was generally complete within 10 msec
(Fig. 1B, inset). The slow component of the decay had
a time constant ranging in different cells from 99 to 265 msec.

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Figure 1.
Experimental setup and GABA-induced currents
recorded from nucleated patch excised from cultured hippocampal neuron.
A, The drawing illustrates the rapid solution switching
system. The theta tubing with control and GABA-containing solutions
flowing through the barrels is rapidly moved in front of the nucleated
patch. A rapid step-like change in the concentration of GABA (within 2 msec) occurs as the interface of the solutions is moved across the
patch. B, The bottom traces represent
superimposed currents recorded from the same nucleated patch. GABA (1 mM) was applied for the various time intervals indicated by
the top traces. A brief pulse of GABA (1 mM, 3 msec) induced a transient inward current that increased rapidly, then
decayed with a fast and a slow time course (as indicated by the
arrow in the inset). The slower component
declined monoexponentially with a time constant of 106 msec
(smooth line). Longer applications of GABA (30, 300, 1000 msec) induced currents with a similar rising phase and peak amplitude.
However, in the continued presence of GABA, currents desensitized with
two distinct components that we refer to as fast and slow
desensitization (see inset). After the removal of GABA, the
responses declined to baseline (defined as deactivation). The major
component of deactivation was adequately described by a single
exponential function, and the smooth lines superimposed on
the experimental data represent an exponential function fit to the
data. The time constants are shown. A small slow component is evident
but is ignored in our analysis. The inset provides a
temporal expansion of the onset and initial decay of the currents
activated by brief and longer pulses of GABA. The lines
above the recordings indicate the duration of the agonist application.
The transient upward deflection illustrates the junctional current
measured after the membrane patch was disrupted.
|
|
Longer pulse applications of GABA (30-1000 msec) activated currents
that decreased in amplitude during the continued presence of agonist.
Fast and slow desensitization processes could be clearly discriminated
in most recordings as illustrated in Figure 1. The fast and slow
components had time constants estimated to be in the 1.5-4.5 msec and
1-3 sec range, respectively. After the removal of GABA, the currents
deactivated with a time course dominated by a single exponential
process (
d = 151 ± 12 msec, n = 12) (Fig. 1B). Although an additional slower component
of deactivation was evident in some records, it represented only a
small component of the decay and was not included in the present analysis.
Effects of propofol on responses to brief (3 msec) application
of GABA
Propofol (10 µM) was added to both control and
agonist-containing solutions after stable currents were observed. At
this concentration, propofol did not induce any detectable current when
applied in the absence of GABA or alter the rise time of
GABA-induced currents (RTcontrol = 1.9 ± 0.2 msec to RTpropofol = 2.0 ± 0.2 msec; p > 0.01, n = 17). However, propofol
significantly increased the duration of GABA-induced current from
63 ± 7 to 115 ± 13 msec (measured at 50% of the peak,
n = 17, p < 0.01) (Fig.
2A). Similarly, the charge
transfer associated with the GABA-induced current was substantially
increased by 62 ± 5% (Fig. 2B) (n = 17, p < 0.01). Propofol also reversibly increased the peak amplitude of
currents (8 ± 2%, n = 17, p < 0.01)
activated by saturating concentrations of GABA (1-30 mM)
(Fig. 2B). No significant differences were observed in these
parameters with the different concentrations of GABA, so the data were
pooled together. Propofol prolonged both the fast and slow component of
the decay observed with the brief applications of GABA (Fig. 2A,
inset). Recordings that demonstrated a well defined fast
component of decay (10 of the 17 patches) were further analyzed by
fitting a single exponential function to the response, from the peak to
10 msec after the peak. The initial decay was slowed 1.5-fold by
propofol from
= 5.0 ± 0.7 to 7.2 ± 1 msec (n = 10, p < 0.01). The slow decay measured by
fitting an exponential to points 10 msec after the peak response was
also prolonged by propofol from
= 159 ± 17 to
= 231 ± 24 msec, n = 17 (p < 0.01).

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Figure 2.
Propofol prolonged the deactivation and
increased the peak amplitude of GABA-induced current. A,
Three superimposed responses to brief pulses of GABA (1 mM)
were recorded from the same patch in the absence and presence of 10 µM propofol. Each trace represents the average of two to
three individual traces. Propofol increased the peak amplitude and
charge transfer associated with the responses, an effect that was
reversed after the washout of propofol. The top trace shows
the open tip junctional current. The inset illustrates the
slowing of the fast decay by propofol. The time constant of the fast
component of a biexponential function was increased by propofol from
2.2 to 3.1 msec (solid lines). B, The bar
graph summarizes the effects of propofol on the peak amplitude
and the charge transfer of currents recorded from 17 patches. Values
were normalized to those obtained under control conditions. A
consistent increase in peak current amplitude (8 ± 2%,
n = 17, p < 0.01; filled bar) and in charge
transfer (62 ± 5%, n = 17, p < 0.01; open
bar) was observed. C, Superimposed traces of currents
activated by longer (500 msec) pulses of GABA (1 mM)
in the absence and presence of propofol (10 µM) are
shown. Note that the predominant effect of propofol is to prolong the
deactivation. Similar to the results obtained for brief pulses of GABA,
the peak current amplitude was increased (shown in inset). A
temporal expansion of the currents is shown in the inset.
Propofol slows the initial decay of the response. D, The
bar graph illustrates that the time constant of
deactivation ( d) was reversibly increased by
propofol.
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|
Propofol modulates GABAAR deactivation
and desensitization
Longer pulses (500 msec) of GABA were used to further investigate
the actions of propofol on receptor desensitization and deactivation.
As is shown in Figure 2C, clearly the most pronounced effect
of propofol (10 µM) was to slow deactivation as evidenced by a slowing of the decay after the removal of GABA. Fitting this decay
with a single exponential function revealed that propofol caused
1.7-fold increase in
d from 151 ± 14 to 255 ± 26 msec (Fig. 2D) (n = 7, p < 0.01).
Similar to the enhancement observed with the brief pulses of GABA, the
peak amplitude of the current activated by 500 msec pulses of GABA was
increased by 8 ± 4% (n = 7, p < 0.01). The increase in the peak was associated with a slowing of the decay of the
fast component. In five of seven patches in which a fast component was
well defined, the initial decline was fit using a single exponential
function. The time constant of the decay was slowed by propofol
1.7-fold, from 2.5 ± 0.4 to 4.3 ± 0.7 msec. In the
continued presence of agonist, currents decayed slowly, and propofol
appeared to reduce this slow desensitization (Fig. 2C).
It is evident in Figure 2C that the slow decline had not
reached a steady state by the end of the 500 msec pulse. Therefore, to
estimate the rate of onset of slow desensitization, we measured the
change in current amplitude from 100 msec (where fast desensitization is complete) to 500 msec (at the end of the agonist pulse). Provided that slow desensitization develops monoexponentially (Mierlak and Farb,
1988
; Oh and Dichter, 1992
; Orser et al., 1994
) and the steady-state
response is small, this initial rate of decline allows the time
constant of slow desensitization to be estimated. The ratio
(amp500msec/amp100msec)
was 0.75 ± 0.02 under control conditions, indicating a 25%
decrement in current over a 400 msec period. This value suggests that
the time constant for slow desensitization (
slow)
equals, at most, 1.4 sec. In the presence of 10 µM
propofol, the ratio
amp500msec/amp100msec was
significantly increased to 0.80 ± 0.02 (n = 11, p < 0.01). A 20% decrement in current amplitude over 400 msec in
the presence of propofol is consistent with
slow of, at
most, 1.8 sec.
Consistent with the 8% increase in the peak current in the
presence of propofol, the amplitude at 100 msec was increased 7 ± 4%. This observation suggests that the increase in peak current persisted after the development of fast desensitization. This increase
in peak amplitude (despite the application of saturating concentrations
of GABA) is consistent with propofol reducing the rate constant of
development of fast desensitization (see below). A small increase in
channel conductance could also produce a similar change in current
amplitude; however, single-channel studies indicate that propofol does
not influence channel conductance (Hales and Lambert, 1991
; Orser et
al., 1994
). It is noteworthy that the ratio of current amplitude at 100 msec and the peak amplitude (amp100msec/amppeak) was not
changed significantly by propofol compared with control (0.75 ± 0.03 and 0.77 ± 0.04, respectively; n = 11, p > 0.01).
Previous studies indicate that recovery from fast desensitization of
the GABAAR underlies the slow deactivation of GABA-induced currents (Jones and Westbrook, 1995
; Tia et al., 1996
; Galarreta and
Hestrin, 1997
; Mellor and Randall, 1997
; Jones et al., 1998
). Therefore, we next examined the relationship between the recovery from
fast desensitization and the change in deactivation produced by
propofol. Fast desensitization was studied using a previously described
double-pulse protocol (Jones and Westbrook, 1995
; Tia et al., 1996
).
With this method, a second test pulse of GABA delivered at various time
intervals after the conditioning pulse examines the recovery from
desensitization induced by the conditioning pulse.
As illustrated in Figure 3, the peak
current induced by a brief test pulse of GABA (3 mM for 3 msec) produced little additional current when applied 20 msec after the
conditioning pulse. As the interval between these pulses was increased,
the amplitude of the test response gradually increased to a level
similar but not quite equal to that of the conditioning pulse. The time
course of recovery from desensitization was examined by plotting the amplitude of the test response (P2) after
subtracting the amount of current remaining at the end of the first
pulse (On2). This value was normalized to
the control response (P1), i.e.,
(P2
On2)/P1. The normalized value was
then plotted against the time interval between
P1 and P2 (
T)
as illustrated in Figure 3B, and the time course was fit by
a single exponential function. Because saturating concentrations of
GABA were applied, (P2
On2)/P1 measures
the proportion of receptors that are no longer associated with GABA and
have returned to a resting and "activatable" state. If there was no
fast desensitization and the biexponential decay simply reflected two
modes of deactivation, P2 should be the same as
P1. Under these conditions, the measure
(P2
On2)/P1 would increase with a rate
constant equal to the deactivation time constant. However, if the
receptors desensitize and the process recovers through a pathway that
is different from that of deactivation, then this difference will be
apparent in the recovery time course. If there is a common state
through which both activated and desensitized receptors recover, the
measure should start at zero and approach 1 with a time constant that
is the same as the deactivation rate.

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Figure 3.
Recovery from fast desensitization was
slowed by propofol. A, Superimposed currents evoked by
paired pulses of GABA (3 mM, 3 msec) are illustrated.
Desensitization produced by the conditioning pulse was investigated by
applying a second test pulse. The test pulse produced negligible
additional current when the time interval between the pulses was 20 msec. As the interval between the pulses increased, the amplitude of
the test response gradually increased to a level that was similar but
not quite equal to that of the conditioning pulse. The reduction in the
amplitude of the test response was primarily caused by loss of the fast
component that occurred within the first 10 msec. The dashed
lines indicate that the slow component of the decay is relatively
stable. The time course of recovery from desensitization was slowed by
propofol (10 µM). B, The ratio of the
amplitude of test pulse and the conditioning pulse
[(P2 On2)/P1)] is plotted versus
the time interval between the two pulses ( t). To
control for rundown of the response during the recordings, the
amplitude of the conditioning response was normalized to the initial
value of P1. The data points
represent the average values for currents recorded from three
difference patches in the absence (filled circle) and
presence of propofol (open circles). The time course of the
recovery was best fit by a single exponential function
( control = 152 msec, propofol = 264 msec). C, The relationship between the fraction of
receptor population that has recovered from desensitization
(P2 On2)/P1 and the extent of
deactivation (P1 On2)/P1 is shown. Note that the
plots can be superimposed in the absence and presence of propofol,
suggesting that deactivation parallels desensitization and propofol
does not influence this relationship.
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We found that this measure of recovery appeared to follow a single
exponential process with a time constant
= 152 msec (Fig. 3B). When propofol (10 µM) was added to the
perfusion solution, the recovery from desensitization was slower:
= 264 msec (Fig. 3B). These values are similar to
the deactivation time constants in the presence and absence of propofol
(see above).
The reduction in peak amplitude of the test pulse primarily resulted
from a decrease in the fast component of decay. As the interval between
the two pulses was increased, the amplitude of the fast component
rapidly recovered, whereas the slower component remained relatively
unchanged (Fig. 3A, dashed line). When the fast
component of the second pulse (defined as P2
response at 10 msec after P2) was
plotted against
T, propofol slowed the time constant of this
recovery from 107 to 181 msec (data not shown).
The correlation between the recovery from desensitization and
deactivation is illustrated in Figure 3C. The parallel time course in the absence and presence of propofol is now illustrated by
plotting fast desensitization (P2
On2)/P1 as a function of extent of
deactivation (P1
On2)/P1. Note that
(P1
On2)/P1 = 1 when the current
is fully deactivated. These plots superimpose in the presence and
absence of propofol, indicating that the prolongation of deactivation
by propofol does not change the relationship between deactivation and
desensitization. These observations are consistent with a model whereby
fast desensitization leads to trapping of the agonist on the receptor,
enabling those receptors to reopen after the free GABA has been washed
away (Jones and Westbrook, 1995
; Jones et al., 1998
).
The onset but not recovery from slow desensitization is modulated
by propofol
The slow component of desensitization is difficult to characterize
accurately because it takes several seconds to reach a steady state
(Celentano and Wong, 1994
; McClellan and Twyman, 1999
). We observed
that it is technically difficult to produce stable currents with
prolonged (>500 msec) applications of agonist to nucleated patches.
Therefore, we adopted an approach of phasic stimulation to investigate
the slower kinetic processes (Jassar et al., 1993
). Thirty brief (3 msec) pulses of GABA were administered at a rate of 0.33 Hz (Fig.
4). The evoked charge transfer declined with each pulse of GABA until a new steady-state value was reached within 15 pulses (Fig. 4C).

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Figure 4.
Propofol reduces slow desensitization.
A, Current traces illustrate the response to repetitive
applications of brief (3 msec) pulses of GABA (30 pulses administered
at a rate of 1 per 3 sec). Under control conditions, the peak amplitude
of the current gradually declined to a steady-state level. Propofol
reversibly increased the duration of each response and also increased
the amplitude of each of the 30 responses to a similar extent.
B, A temporal expansion of currents evoked by the 1st and
30th application of GABA is shown. Responses are superimposed, and the
arrows indicate the peak amplitude of the 30th response.
Note that in the absence or presence of propofol, the decay of the 30th
response was accelerated compared with the initial response. This
effect is further illustrated in the panel to the
right where the peak amplitude is normalized to the maximum
response. C, The charge transfer associated with each
response during the repetitive applications of GABA is shown. Data
points are the average values obtained from seven different patches.
After the first two pulses, in the absence of propofol
(filled circle), the charge transfer declined
monoexponentially with a time constant of 14.4 sec to a steady-state
value 39% of the initial response. In the presence of propofol
(open circle), the time constant was 15.7 sec, and the
steady-state value was 38% of the initial value. The first two data
points were not included in the exponential fit. Propofol significantly
increased the charge transfer of all 30 pulses to a similar extent
(two-way ANOVA, p < 0.01). D, The decline in
ton (charge transfer/amplitude) for the 30 pulses activated by GABA is shown. Propofol increased
ton of GABA-evoked currents (two-way ANOVA,
p < 0.01). The straight line plotted
through the last 28 data points represents a linear regression with the
slope restricted to zero. The intercept of this line for
ton was 90 and 142 msec for currents recorded in
the absence and presence of propofol, respectively. The
inset illustrates the calculation of
ton.
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|
To analyze the build up of slow desensitization during the phasic
stimulation, we applied a previously described form of analysis (Starmer, 1986
; MacDonald et al., 1991
; Jassar et al., 1993
). The
assumptions implicit to this analysis have been previously summarized
(Jassar et al., 1993
; Starmer, 1986
). This analysis assumes that
receptors are saturated during the brief response and that the rate
constant of recovery from slow desensitization (rs) is slow relative to the time intervals
between pulses. Here, the transient currents are considered to be
equivalent to a theoretical square pulse of activated receptors (Fig.
4D, inset). Channels activated by the actual response
to a transient application of agonist have the same opportunity for
slow desensitization as a theoretical square pulse of activated
receptors with a duration of ton, where
ton = charge transfer (Q)/peak
amplitude of the response (P). A mathematically more
sophisticated analysis of phasic stimulation is also possible (Uteshev
and Pennefather, 1996b
) but provides little additional information in
the present case. It is evident in Figure 4D that
after the first several pulses, ton is constant.
The values for ton in the absence and presence
of propofol were 90 and 142 msec, respectively.
The apparent rate constant for the development of slow desensitization
(d's) during phasic stimulation can be
estimated using the calculated values for ton
and the fractional decrement of change transfer per pulse (
). The
actual rate constant (ds) will dependent on the
proportion of doubly liganded receptors in the state that lead to slow
desensitization. By defining the time during which receptors are not
activated as toff
(toff = pulse interval
ton), then one can demonstrate that
= d's * ton + rs * toff, and
the relative fractional amplitude of the steady-state response observed
during continued phasic stimulation is such that (1
Qsteady-state/Qinitial) = d's * ton/
and
Qsteady-state/Qinitial = rs * toff/
(Starmer, 1986
). A fraction of the available receptors enter the
desensitized state with each pulse, and the steady-state value reflects
the product of the rate of recovery from slow desensitization (Rs) and toff.
Using the data summarized in Figure 4 and considering the steady-state
response, we note that propofol decreases the rate of entry into the
slow desensitized state such that d's is
reduced from d's = 1.37 sec
1 under control conditions to
d's = 0.85 sec
1
in the presence of propofol. This decrease in
d's reflects the fact that
and the
steady-state response are relatively unchanged despite the increase in
ton by propofol. We also estimate that rs = 0.025 sec
1 in the
presence and 0.028 sec
1 in the absence of
propofol. These estimated values ignore the possibility of the multiple
desensitized states. Alternatively, multiple receptor subtypes with
different kinetic properties could account for the initial deviation of
the ton as well as the biphasic time course of
recovery from desensitization reported previously (Orser et al., 1994
).
Nevertheless, these values produce a reasonable simulation of our
experimental results when used in conjunction with our model (see below).
Propofol thus appears to slow the onset of slow desensitization to the
same extent that it reduces the deactivation rate. This observation
suggests that propofol slows both of these transitions out of the
pre-open state to the same extent. Our results are consistent with
previous data that indicate propofol slows the entry into the slowly
developing state of desensitization but has little effect on the
recovery process (Orser et al., 1994
). The results predict that
propofol will increase the steady-state response observed during a
prolonged application of saturating GABA, after slow desensitization
has been allowed to equilibrate (Orser et al., 1994
). Indeed, slow
desensitization will be decreased to the same extent as the response is
prolonged after a brief application of GABA (~1.85-fold).
Propofol's action is not voltage-dependent
We next tested whether the membrane potential influences the
action of propofol on deactivation of GABA-induced current. In the
absence of propofol, membrane hyperpolarization (+40 to
80 mV) was
associated with an increase in the rate of current decay (Fig.
5A). The rate of deactivation
(1/
d) decreased with increasing membrane
potentials at a rate of e-fold/420 mV. Propofol increased
d by ~60% at all holding potentials tested (Fig.
5B). Therefore, the slope of the linear regression line for
the relationship between log 1/
d and voltage was not
influenced by propofol. In addition, propofol did not alter the
reversal potential of GABA-induced current (data not shown).

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Figure 5.
Slowing of deactivation by propofol is
voltage-independent. A, Currents evoked by GABA (3 mM, 3 msec) at various holding potentials are superimposed.
The rate of decay (1/ d) was increased at
hyperpolarizing potentials. The inset illustrates the
superimposed currents obtained at holding potentials of +40 mV
(inverted) and 80 mV normalized to the peak amplitude for responses.
The decay was increased by propofol at all holding potentials.
B, Data obtained from five different patches were averaged
and plotted versus 1/ d (log scale). A linear
relationship was observed between 1/ d and holding
potential (voltage) under control conditions (filled
circle) and in the presence of propofol (open circles).
Propofol produced a similar decrease in the rate of current decay at
all holding potentials as indicated by the slope of the lines
(n = 5, two-way ANOVA, p < 0.01).
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Simulations
To simulate the actions of propofol, we consider a simple parallel
model (reproduced below) similar to that proposed by Celantano and Wong
(1994)
. However, only two components of desensitization are considered.
C represents the closed state, L depicts the agonist ligand, and D and
O represent the desensitized and open states, respectively.
This model assumes that there are two equivalent ligand binding sites
with the binding and unbinding rates kon and
koff, respectively. These rates (Table
1) are multiplied by statistical factors
that take into account that two equivalent agonist sites are available. Occupation of these two binding sites by agonist generates the pre-open
state, (L2C). The receptor can either rapidly isomerize into an open state (L2O) with a rate constant
or
rapidly convert into a desensitized state (L2Df
or L2Dfast) with a rate constant df. Closing of the channel occurs with a rate
, and recovery from L2Df occurs with a rate
constant rf. In this model, GABA cannot readily
dissociate from the L2Df or L2O
states, so after the removal of GABA, deactivation will be limited by
the unbinding of GABA from the closed but double-liganded receptor
state L2C. For simplicity we have allowed slow
desensitization to proceed only from the L2C state with a
rate constant ds. Recovery from slow
desensitization (L2Ds or L2Dslow)
occurs as the reverse of this process through the L2C state
with a rate constant rs.
Scheme 1 can be simplified to a three-state system for
which analytical solutions are possible. If we assume that binding is
fast, then after the application of a saturating concentration of GABA
all of the receptors will rapidly convert into L2C, and the
rising phase of the response is determined primarily by the isomerization to L2O and L2Df. Thus, at
time zero all of the receptors are in the L2C state (Scheme
2 in the Appendix). Using this assumption, we chose to
deduce the parameters by analysis of a three-state approximation of our
model rather than fit each of our recordings to the model using
optimization techniques.
In the Appendix we show how the kinetics of the response to GABA
observed here permit further simplifications of these analytical equations such that quite simple relations can be derived that relate
model rate constants to the observed kinetic components of the
response. For example in Equation A10a we show that if
and df are fast compared with
koff, then the deactivation rate
(1/
d) will be approximated by:
|
(1)
|
The denominator reflects the relative proportions of
L2C, L2O, and L2Dfast
present during the deactivation phase. Thus, the rate of deactivation
will be slowed to the extent that GABA is trapped on L2O
and L2Df. Likewise, it can be shown (Eq. A17) that under these conditions, the amplitude of the response after
fast desensitization has developed, but before extensive slow
desensitization has developed (the initial plateau response or ~10
msec after the peak) it will be:
|
(2)
|
|
(2a)
|
For situations where the rising phase is dominated by
and
where
/
is small, the initial fast decay time constant
f (Eq. A16) will be approximated by:
|
(3)
|
To assign parameters to our more complicated model (Scheme 1), we
first set
as large as was consistent with experimental observation
(6/msec) (Maconochie et al., 1994
). Previous measurements (Orser et
al., 1994
) constrain
at 0.4/msec. Thus,
/
= 15 and
/
is
1. On the basis of preliminary simulations, we decided to
consider the condition where
df/rf =
/
and therefore
(
/
)(df/rf) = 1. Thus, at the initial plateau phase the distribution between opening and fast desensitization will be 50:50 and
L2O(pl)/L2C(o) = 0.5. With long
pulses, we estimated that
f = 2.5 msec (see above).
Therefore, using Equation 3 and our estimate of
(
/
)(df/rf) = 1, we set rf = 0.20/msec and
df = 3/msec. Using Equation 1 we set
2koff = 31/151 msec = 0.206/msec. For
kon, we use the value of 1 mM/msec,
which gives an EC50 value for the peak response of 25 µM. However, because we are using saturating
concentrations of GABA, this value is not critical to our simulations.
For the slow desensitization parameters, we use a rough estimate of
rs = 2.7 × 10
5/msec that was derived from the analysis of
phasic activation with brief pulses (Fig. 4). If
ds is set at 0.026/msec, then Scheme 1
reproduces the results obtained with phasic activation for a two-state
scheme where d's = 1.37/sec,
rs = 2.7 × 10
5/msec, and ton = 90 msec
(see above).
Simulations of the brief pulses of GABA (Fig.
6A) indicate that the proposed
parameters generate a peak response where 59% of available receptors
are in the open state. All receptors are occupied, however, with 37%
of receptors in the fast desensitized state and 4% in the pre-open
state. Simulation of the longer pulses of GABA (Fig. 6B)
indicates that the fraction of activated receptors quickly declines to
a value of 49% as the equilibration between the L2O and
states L2Df gives rise to a pseudo-equilibrium
within a 10 msec period.

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Figure 6.
Simulations of the effects of propofol on
GABA-induced current and predesensitization of GABA currents.
A, Simulations of GABAAR-mediated activity after
the application of brief pulses of GABA (3 mM, 3 msec).
Popen represents fraction of channels in open
state. The solid declining line depicts the rapid decrease
in open probability. Superimposed is a plot of the probability of slow
desensitization (L2Dslow) in the absence (solid
line) or presence (dashed line) of propofol. The
slower buildup of the L2Dslow state under
control conditions is indicated by the solid inclining line
(arrow). Propofol causes an increase in the open probability
and a small decrease in slow desensitization as indicated by the
dotted lines. B, Simulations of the longer (500 msec) pulses of GABA is shown. Again, superimposed is a plot of
L2Dslow. Note the increase in open probability and
slower buildup of L2Dslow in the presence of
propofol (dashed lines). Propofol (10 µM)
increased the probability of channel opening and reduced slow
desensitization. C, Simulation of the application of 30 brief pulses of GABA at 30 pulses administered at a rate of 1 per 3 sec
in the absence and presence of propofol. The buildup of the
L2Dslow state was extensive in the absence and
presence of propofol. D, Simulation of the same experiment
as in C only now monitoring the level of unbound receptors
(C). E, Experimental data illustrate that the preapplication
of 3 µM GABA decreased the amplitude of current evoked by
a saturating concentration of GABA (1 mM), but this effect
is far from equilibrium even with longer applications. Increasing the
duration of the preapplication from 5 sec (arrow) to 10 sec
(double arrows) doubled the effect from an 8% decrease to a
17% decrease. However, our model parameters predict that at
equilibrium, 3 µM GABA will reduce the test response by
16 and 24% in the absence and presence of propofol, respectively.
Thus, a 10 sec predesensitization period will underestimate the
affinity of the slow desensitized state for GABA because the
IC50 for predesensitization is 3 µM at
equilibrium.
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|
Propofol reduces the rate of onset of fast desensitization ~1.7-fold,
whereas the initial plateau is only changed by 7%. Therefore, from
Equations 2a and 3 we can estimate that rf is
reduced 1.7-fold to 0.12/msec. The plateau is enhanced by propofol so
that df must be reduced by a slightly greater
extent than rf. The 7% increase in the
plateau is reproduced if df is reduced 1.85-fold
to 1.62/msec. If df is reduced to exactly the
same extent as rf, then Equation 2 would
predict that the response at 100 msec with long pulses would not be
changed at all by propofol because the ratio of
df/rf would remain
the same. These reductions in df and
rf predicts a 17% increase in the amplitude of
the response (Fig. 6A), whereas an increase of 8% was observed.
According to previous models (Jones and Westbrook, 1995
), the slight
reduction in the extent of fast desensitization, if anything, should
increase the rate of deactivation in the presence of propofol. Because
previous results suggest that propofol does not affect
and the rise
time is also unchanged by propofol, we conclude that propofol has
little effect on the opening/closing isomerization. Therefore, using
Equation 1 we can estimate that 2koff is reduced 1.85-fold by 10 µM propofol.
For slow desensitization, we accept that propofol has no effect on
recovery from slow desensitization (see above) and set rs at 0.027/sec. We then adjust
ds until Scheme 1 gives a steady-state level of
desensitization of 60% during phasic stimulation (Fig. 4). The
resulting value of ds = 0.014/msec is also
1.85-fold lower than the control value. Thus, our analysis suggests
that propofol stabilizes the pre-open state and increases the energy
barrier for transitions to fast and slow desensitized states as well as for agonist dissociation to similar extents.
Because saturating concentrations of GABA are used in the current
experiments, the time course of desensitization from the single
bound state (L1C) makes little difference to the
simulations. However, the assumption of equivalent binding sites in our
model means that with low agonist concentrations, as well as during deactivation, a significant fraction of receptors will be in the L1C state. Furthermore, with our model, propofol will
potentiate this state because it decreases
koff. In preliminary experiments, we
observed that slow desensitization requires minutes to develop at low
agonist concentrations in this preparation (Fig. 6E). This result is not consistent with the development of significant slow desensitization from L1C. This observation may also explain
the unexpected finding of Orser et al. (1994)
where the GABA
IC50 value for predesensitization was similar to the GABA
EC50 for activation of GABAA receptor. In the
previous study, GABA was applied for only 10 sec to predesensitize the
receptors. If slow desensitization can only develop from an
L2C state at the rates deduced here, a 10 sec time period
is inadequate to reach equilibrium at low agonist concentrations.
Our model parameters predict that at equilibrium, the IC50
for slow desensitization is 3 µM GABA, whereas the
EC50 for peak responses is ~25 µM. This
value could be confirmed using predesensitization protocols in which
sufficient time is allowed for a true equilibrium to develop. In our
previous model (Orser et al., 1994
) we included an additional binding
step for the induction of slow desensitization so that
predesensitization and activation could be allowed to occur over a
similar range of concentrations.
It is noteworthy that although the model predicts that propofol will
potentiate the GABA response and therefore reduce the EC50
value for GABA-evoked currents, the IC50 for
predesensitization will be changed to a lesser extent. Desensitization
is reduced by an amount similar to the enhancement of the response.
Thus, potentiation of background current (Bai et al., 1998
) will have a
smaller effect on resting desensitization and the concomitant reduction
in the amplitude of spontaneous miniature IPSCs (mIPSCs).
The process of slow desensitization is highlighted by the phasic
stimulation protocol. We simulated the experimental results as
illustrated in Figure 6C. However, the model did not predict the acceleration of deactivation observed during the first few responses in the train (Fig. 4B, right panel,
D). In our simulations, the time course of the first and
the last response can be superimposed once responses are normalized to
the peak amplitude (data not shown). This acceleration of the decay may
reflect the desensitization of two populations of GABAAR
that are present in the nucleated patches.
The effect of slowing recovery from fast desensitization is shown in
Figure 7. The model accurately reproduces
the results obtained with the paired-pulse protocol. Recovery from fast
desensitization and deactivation occurred in parallel, and the small
amount of slow desensitization that develops per pulse is reflected by
the incomplete recovery of the amplitude of the second pulse (Fig. 3).

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Figure 7.
Simulation of the recovery from desensitization.
Using our proposed model, we simulated the currents activated by paired
pulses of GABA. GABA (3 mM for 3 msec) was applied at
intervals of 20, 120, 220, 320, 420, 720, 1320, and 1920 msec. The
dotted line represents the fit of a monoexponential equation
to the peak amplitude of the second pulse. B, Simulated
currents for responses activated in the presence of propofol (10 µM).
|
|
 |
DISCUSSION |
We examined the actions of propofol on GABAergic currents under
nonequilibrium conditions. The most prominent effect of propofol on
responses to brief applications of GABA is to cause a
voltage-independent prolongation of deactivation. Consistent with an
earlier report (Orser et al., 1994
), propofol also reduces slow
desensitization, as evidenced by changes in the time course of
responses to 500 msec pulses of GABA. Slow desensitization was also
indicated by the decline in peak amplitude of currents evoked by
repeated brief applications of GABA. Propofol increased
ton by prolonging the deactivation of individual
responses. However, the fractional decline (
) in peak amplitude per
pulse in a train was unchanged despite this enhanced response,
suggesting that propofol must also reduce the rate of development of
slow desensitization.
A fast component of desensitization could be resolved using our fast
perfusion system with saturating concentrations of GABA. Propofol
increased the amplitude of the peak current, an effect that is
consistent with propofol causing a decrease in the kinetics of fast
desensitization. An increase in current amplitude attributable to a
redistribution of the receptors between activated and fast desensitized
states may explain how some compounds increase the amplitude of mIPSCs
despite receptor saturation. Hence, an increase in peak amplitude
cannot be used as evidence (Frerking et al., 1995
) that receptors
contributing to mIPSCs are not saturated.
The rise time of GABA-induced current in this study was ~2 msec
(10-90%). This value is similar to that reported by Jones and
Westbrook (1995)
for hippocampal neurons but slower than that reported
for cerebellar granule cells (Maconochie et al., 1994
; Zhu and Vicini,
1997
), cortical neurons (Galarreta and Hestrin, 1997
), or basket cells
of the dentate gyrus (Berger et al., 1998
). The slower rise time
reported in the present study could be attributed, in part, to the
accessibility of agonist to receptors present in the nucleated patch
because the exchange time for the K+ current
recorded under similar experimental conditions was 1.9 msec. The slower
rise time of GABA currents might also be determined by the subunit
composition of the receptor (Haas and Macdonald, 1999
; McClellan and
Twyman, 1999
).
Actions of propofol on GABA-evoked currents in nucleated
patches of hippocampal neurons mimic its effect on mIPSCs
The action of propofol to slow deactivation of GABA-evoked
currents qualitatively resembles the effects of propofol on mIPSCs (Orser et al., 1994
). Propofol causes a concentration-dependent increase in the duration of synaptic currents. However, the
decay of mIPSCs recorded in cultured hippocampal neurons is two to four times faster than deactivation of GABA-evoked responses (Jones and
Westbrook, 1997
; Mozrzymas et al., 1999
; our data). Using our kinetic
model, the rapid decay of mIPSCs could not be mimicked by simply
altering the duration or the concentration of GABA (data not shown).
However, a simple increase in the rate of dissociation of GABA
(koff) from synaptic receptors permits our model
to simulate the more rapid decay of mIPSCs. This observation is
consistent with the suggestion that the inherent binding and gating
properties of postsynaptic GABAAR differ from receptors
present in excised patches (Nusser et al., 1995
; Brickley et
al., 1999
). For example, synaptic GABAARs may not trap GABA
as extensively on the desensitized states. The subunit composition of
the receptors (Tia et al., 1996
; Haas and Macdonald, 1999
; McClellan
and Twyman, 1999
) or post-translational modification by second
messenger systems (Jones and Westbrook, 1997
; Mozrzymas and Cherubini,
1998
) or regulatory cytoskeletal proteins might also contribute to the
differences between synaptic receptors and those present in the excised
patches. Nevertheless, the action of propofol on the duration of IPSCs could be explained if propofol slows koff at
synaptic receptors to the same extent as it slows dissociation of GABA
from extrasynaptic receptors.
Alterations of GABAergic currents by pharmacological agents depend
on the time course and concentration of GABA
GABAARs undergo multiple conformational changes after
the binding of agonist, and the pharmacological properties of these conformational states can differ. Thus, the time course and magnitude of receptor activation by the GABA influences the pharmacological sensitivity of a population of receptors (Quastel and Pennefather, 1983
; Mozrzymas et al., 1999
). This may account, in part, for differences between drug modulation of synaptic currents and
GABA-evoked currents that have been demonstrated for various compounds,
including barbiturates (Hill et al., 1998
), benzodiazepines (Lavoie and Twyman, 1996
; Mellor and Randall, 1997
; Perrais and Ropert, 1999
), neurosteroids (Harrison et al., 1987
; Zhu and Vicini, 1997
),
phenothiazine (Mozrzymas et al., 1999
), and lanthanum (Zhu et al.,
1998
).
Recently, a tonic form of GABAergic inhibition has been described
whereby GABAARs are activated by persistent low ambient concentrations of transmitter (Valeyev et al., 1993
; Brickley et al.,
1996
). An important prediction of our kinetic model is that drugs such
as benzodiazepines and propofol that have different actions on slow
desensitization will have discordant effects on the tonic current and
IPSCs. For example, diazepam-like benzodiazepines increase the
frequency of single-channel opening (Rogers et al., 1994
) and prolong
deactivation (Orser et al., 1999
) but do not reduce the rate of onset
of slow desensitization. On the other hand, propofol increases the
frequency of channel opening (Orser et al., 1994
), slows deactivation
of macroscopic current, and decreases slow desensitization (this
study). According to our model, midazolam applied to receptors
persistently activated by low concentrations of GABA will facilitate
the accumulation of the receptors into the slow desensitized state.
Absorption of receptors into this nonconducting state will counter the
enhancement of current caused by slowed deactivation. In contrast, for
propofol our model predicts that for the same degree of prolongation of mIPSCs, there will be a larger effect on the sustained background response to ambient GABA. Consistent with these predictions,
preliminary evidence indicates that low concentrations of propofol
enhanced the tonic current recorded from cultured hippocampal neurons
to a greater extent than midazolam, whereas propofol and midzolam produced similar changes to the time course and charge transfer associated with mIPSCs (Bai et al., 1998
). Thus, our kinetic model predicts that drugs with differing actions on slow desensitization will
have different effects on the enhancement of currents activated by low
concentrations of GABA under near-equilibrium conditions compared with
currents evoked by saturating concentrations of agonist under
nonequilibrium conditions.
In summary, we demonstrate that the prominent effect of propofol on
GABA-evoked currents is to slow deactivation. We attribute this effect
to a stabilization of the ligand-bound pre-open state and suggest that
it accounts for the prolongation of synaptic currents by propofol. The
action of propofol to slow the onset of desensitization would not
contribute appreciably to changes in synaptic currents activated at a
low frequency but would enhance charge transfer during high-frequency
stimulation. Propofol would also reduce desensitization of GABAergic
currents activated by persistent low concentrations of agonist and
enhance the steady-state amplitude of that current.
 |
FOOTNOTES |
Received April 16, 1999; revised Sept. 27, 1999; accepted Sept. 30, 1999.
This work was supported by the Medical Research Council of Canada
(J.F.M., P.S.P.). B.A.O. was supported by the First Frontiers in
Anesthesia Research Award from the International Anesthesia Research
Society and a Career Scientist Award from the Ontario Ministry of
Health. We thank L. Brandes and E. Czerwinska for preparation of the
cell cultures.
Correspondence should be addressed to Dr. Beverley A. Orser, Department
of Physiology, Medical Science Building, Room 3318, University of
Toronto, Toronto, Ontario, Canada M5S 1A8. E-mail: beverley.orser{at}utoronto.ca.
 |
APPENDIX: ANALYSIS OF THREE-STATE SIMPLIFICATION OF SCHEME 1 |