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The Journal of Neuroscience, February 15, 1998, 18(4):1602-1612
The Pharmacology and Roles of two K+ Channels in
Motor Pattern Generation in the Xenopus Embryo
Frederick M.
Kuenzi and
Nicholas
Dale
School of Biomedical Sciences, University of St. Andrews, St.
Andrews, Fife KY16 9TS, United Kingdom
 |
ABSTRACT |
The spinal neurons of the Xenopus embryo that
participate in the swimming motor pattern possess two kinetically
distinct sets of potassium currents: the fast
IKf and sodium-dependent
IKNa, which together constitute
~80% of the outward current; and the slow
IKs, which constitutes the remainder.
To study their respective roles in cell excitability and the swimming
pattern, we have characterized their pharmacological properties.
Catechol selectively blocked the fast potassium currents
(IC50, ~10 µM). The block was
voltage-dependent, with partial unblocking occurring at positive
voltages.
-Dendrotoxin and dendrotoxin-I selectively blocked the
slow potassium current. Catechol and the dendrotoxins had different
effects on membrane excitability: catechol caused spike broadening but
had little effect on repetitive firing, whereas both dendrotoxins
markedly increased repetitive firing without affecting spike width. By applying these agents to the whole embryo, we tested the role of the
fast and slow currents in motor pattern generation. Catechol had little
effect on fictive swimming, suggesting that the fast K+ currents are not critical to circuit operation.
However, dendrotoxin disrupted swimming early in the episode and
increased the duration of ventral root bursts. The slow
K+ current, which is a minor component of the total
outward current, thus appears to play an important role in motor
pattern generation.
Key words:
potassium channels; catechol; dendrotoxin; 4-aminopyridine; Xenopus; central pattern generator; neural
model; repetitive firing
 |
INTRODUCTION |
The pattern of neural output
produced by a circuit of interconnected neurons depends on the
biophysical properties of the constituent neurons, the pattern of
synaptic interconnections, the transmitter-receptor systems of those
synapses, and the neurohumoral environment. The roles of individual
voltage- and ion-gated ion channels have been studied in shaping reflex
responses (Byrne, 1979
), and recently this analysis has been extended
to more complex circuits (e.g., Golowasch and Marder, 1992
; El Manira
et al., 1994
; Dale, 1995b
; Nadim et al., 1995
; Olsen et al., 1995
;
Tegner et al., 1997
). These channels determine how the synaptic
currents are integrated into a pattern of action potentials. They may
also be targets for neuromodulators that alter the outputs of the
neural circuit (Harris-Warrick et al., 1995a
,b
; Dale and Gilday, 1996
; Nadim and Calabrese, 1997
). Potassium channels, in particular, are very
diverse and control aspects of membrane excitability such as the delay
in spiking in response to sustained synaptic input, the frequency of
action potentials, and the degree of accommodation within a burst
(e.g., Connor, 1975
; Byrne, 1980a
,b
; McCormick and Huguenard, 1992
;
Brew and Forsythe, 1995
). Testing the roles of potassium currents
experimentally requires selective pharmacological tools. However,
because few potassium channel blockers are specific, appreciation of
the roles of these channels may also depend on computer simulations
that incorporate quantitative models of the circuit and the known
conductances.
The Xenopus embryo is a preparation in which detailed
understanding of how ion channels contribute to motor behavior is
possible. The embryonic neurons that control swimming fire a single
spike on each cycle. Discharge on either side of the body alternates, causing flexions that drive the animal forward. The spinal circuitry that generates swimming has been well characterized (Arshavsky et al.,
1993
; Roberts, 1990
), and through voltage-clamp analysis of acutely
dissociated neurons, quantitative kinetic descriptions of the principal
voltage- and ion-dependent channels are available (Dale, 1991
, 1993
,
1995a
; Wall and Dale, 1995
). Three potassium channels can play a role
in the cycle by cycle pattern: the fast-activating IKf, the slow-activating
IKs, and the sodium-dependent potassium current IKNa, which is kinetically
similar to IKf. Through a physiologically based
model of the swimming circuit, Dale (1995b)
hypothesised that the
IKf and IKs play distinct
roles in producing the swimming motor pattern. The effects on swimming
of nonspecific potassium channel blockers, such as tetraethylammonium
and 3,4-diaminopyridine, give some support to these predictions (Wall
and Dale, 1994
).
We have identified pharmacological agents that selectively block the
fast and slow potassium currents in Xenopus spinal neurons; catechol specifically inhibited IKf and
IKNa in a voltage-dependent manner, whereas both
dendrotoxin-I (DTX-I) and
-dendrotoxin (
-DTX) preferentially
blocked the slow current. The effects of catechol and dendrotoxins on
cell firing properties were very similar to the predictions of the
model. Furthermore catechol, at doses that blocked up to 50% of the
fast currents, had no effect on fictive swimming in the intact embryo,
but the dendrotoxins significantly altered the motor pattern.
 |
MATERIALS AND METHODS |
Dissociation of spinal neurons. Spinal neurons
of stage 37/38 Xenopus laevis (Nieuwkoop and Faber, 1956
)
embryos were dissociated as described previously (Dale, 1991
) with
slight modifications. Embryos were anesthetized in tricaine methane
sulfonate (MS-222, 0.5 mg/ml; Sigma, St. Louis, MO), and, using
sharpened tungsten needles, a section of spinal cord extending from the
obex of the hindbrain to the level of the anus was removed. The cords
from three embryos were incubated for at least 3 min in "normal"
saline [in mM: 115 NaCl, 3 KCl, 1 MgCl2, 2 CaCl2, 2.4 NaHCO3, 10 HEPES (Sigma), 10 glucose, and 0.13 mg/ml
DNase I (Boehringer Mannheim, Indianapolis, IN), pH 7.6]. The tissue
was then incubated for 1 min with Pronase E (1.5 mg/ml, type XIV;
Sigma) in "trituration" saline, which was the same as normal
saline, except that NaCl was substituted by sodium methane sulfonate.
The tissue was then washed in a low-divalent saline [in
mM: 115 sodium methane sulfonate, 3 KCl, 2 EDTA (Sigma), 10 1,4-piperazinediethanesulfonic acid (PIPES; Sigma), and 10 glucose, pH
7.0] for 1 min and in a second solution (containing in mM:
115 sodium methane sulfonate, 3 KCl, 0.1 MgCl2, 0.1 CaCl2, 10 PIPES, 20 glucose, and 0.13 mg/ml DNase, pH 7.0). The cords were then gently triturated in trituration saline
and DNase (4 mg/ml) to yield isolated cells. These were spread on
polylysine-coated plastic culture dishes containing O2-saturated normal saline.
Cell identification. Neurons that had been acutely
dissociated in this way retained much of their morphology and could be identified by the criteria of Dale (1991)
. The cells that make up the
swimming central pattern generator (CPG) neurons fall into three
classes: "commissural" cells (monopolar cells with pear-shaped somata and initial segments), monopolar cells with circular somata, and
multipolar cells. Approximately 90% of cells in the commissural class
are glycinergic commissural cells of the spinal circuit, and ~70% of
the monopolar class are also commissural interneurons. The remainder of
these and the multipolar classes include mainly descending excitatory
interneurons and motor neurons (Dale, 1991
; Roberts and Clarke, 1982
).
Dorsolateral commissural cells are relatively rare in the spinal cord
and were presumably included in the CPG class, although they are not
part of the central pattern generator per se (Roberts and Sillar,
1990
). Rohon Beard (RB) sensory neurons were identified by their large,
circular somata containing a large nucleus and prominent nucleolus.
Patch recording in isolated cells. For making whole-cell
patch recordings the normal solution bathing the cells was exchanged for a "control" recording medium that contained (in mM)
115 NaCl, 3 KCl, 1 MgCl2, 10 CaCl2, 2.4 NaHCO3, and 10 HEPES.
The pH was adjusted to 7.4, and the osmolarity was ~260 mOsm. The
intracellular solution contained (in mM) 100 potassium
methane sulfonate, 5 KCl, 6 MgCl2, 5 ATP (sodium
salt), 2 1,2-bis(2-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid (Molecular Probes, Eugene, OR), and 20 HEPES. The pH was adjusted
to 7.4 with KOH, and the osmolarity was adjusted to 240 mOsm, usually
by increasing the volume by 10%. Both of these solutions were
sterile-filtered before use. In the dendrotoxin experiments we found
that the block was more reliable if the extracellular calcium was
reduced to 5 mM and the osmolarity was adjusted with glucose. The Ag/AgCl2 ground electrode was separated from
the bath by an agar bridge containing control saline. Drugs were
applied through a nine-barrel microperfusion apparatus with the nozzle positioned within 150 µm of the cell. Adequate flow was judged by the
movement of cells and debris within the field of the microscope when
the flow was turned on and off. In voltage-clamp experiments all
solutions contained 150 nM tetrodotoxin to block sodium
channels and 100 µM CdCl2 to block calcium
currents (both from Sigma), and in all experiments the holding
potential was
50 mV. In some experiments the sodium-dependent
potassium current was blocked by replacing the sodium in the control
medium with equimolar N-methyl-D-glucamine (Sigma). To measure INa we modified the external
saline by replacing half of the NaCl with TEA-Cl and adding 100 µM CdCl2 and 1 mM 4-aminopyridine
(4-AP). The internal saline contained (in mM) 100 cesium
methane sulfonate, 1 CaCl2, 10 EGTA, 20 HEPES, 5 ATP, and 6 MgCl2, pH 7.4.
Recordings were made with a List Biologic (Campbell, CA) L/M EPC7
patch-clamp amplifier with the stimulus input and data acquisition controlled by an IBM-compatible computer and a Data Translation DT2831
data acquisition board. When filled with intracellular recording saline
the electrode resistance was 4-10 M
in the bath. After breaking
through to whole-cell configuration the series conductance was
0.1
µS, and in voltage clamp the series resistance compensation was
typically between 75 and 80%.
Patch recording in the intact spinal cord. Although
many neurons fired repetitively in cell culture, we found that
repetitive firing was more reliable when making patch recordings
in situ. In accordance with the United Kingdom Animals
(Scientific Procedures) Act of 1986, embryos were anesthetized with
MS-222, and their dorsal fins were slit open using fine tungsten
needles. They were incubated in 0.077 mg/ml
-bungarotoxin (Sigma)
for 20 min or until they stopped swimming in response to a tactile
stimulus. The skin and muscles on the side and overlying the spinal
cord were removed. The embryo was pinned with two tungsten needles through the notochord in a recording chamber that had a volume of 200 µl. A "blind" recording technique was used in which the recording
electrode was positioned by course adjustment to just touch the spinal
cord, and then it was slowly advanced into the cord to a depth of ~20
µm. Swimming was initiated by dimming the lights. All recordings
included in this study were from neurons that received a rhythmic
synaptic drive and were active during swimming and therefore had a high
probability of being part of the CPG (Arshavsky et al., 1993
).
Drugs. DTX-I and
-DTX were obtained from Alomone Labs
(Jerusalem, Israel). Stock solutions of 20 µM were made
in control saline and kept refrigerated but used within 2 weeks.
Catechol (1,2-benzenediol) and 4-aminopyridine were from Sigma.
Catechol is light-sensitive, so refrigerated stock solutions (100 mM) were discarded after 1 week.
Fictive swimming. For convenience, in this paper fictive
swimming recorded from the ventral roots of a paralyzed embryo will be
referred to simply as "swimming." The preparation for extracellular recording of ventral root activity was similar to that described for
in situ patch recording, except that the embryo was
spinalized at the level of the first or second postotic myotome. The
embryo was held upright between two pairs of tungsten pins so that
glass suction electrodes could be pressed against the intermyotomal clefts to make ventral root recordings. Swimming was started by a brief
electrical stimulus to the skin of the tail. At least 3 min elapsed
between the end of the last swim episode and the next stimulus. Data
were recorded on a cassette tape for later analysis.
To measure burst duration and cycle period, episodes of swimming were
acquired with a Data Translation DT31EZ board onto a computer disk. The
ventral root records were rectified and integrated over a 2 msec
interval. Cycle period was calculated from the midpoints of the ventral
root bursts, and the duration of a burst was measured as the time
between the first crossing above a threshold and the last crossing
below the threshold per burst. Thirty cycles were also averaged,
triggered from the leading edge of the burst. The area under the
averaged record was a measure of the number of spikes contributing to
the bursts.
Statistical analysis. Results are presented as mean ± SEM. In dose-response curves the error bars are 1 SD. Exponential
curves were fitted to experimental data using the Simplex algorithm, and concentration-response curves were fitted by the
Levenburg-Marquardt method of least squares fitting (Press et al.,
1988
). Tests of significance are described in Results.
 |
RESULTS |
Central pattern generator neurons and Rohon Beard neurons
have different K+ currents
All of the cell types in this study possessed
K+ currents that were not inactivated at a holding
potential of
50 mV and that activated at potentials between
20 mV
and +20 mV. The tail currents were well fitted by sum of two
exponentials, indicating the presence of two kinetically distinct
currents, but the activation phase of the current records proved
difficult to fit reliably, because most cells displayed some
K+ current inactivation. To measure the fast and
slow components separately, we evoked tail currents by first stepping
the cell from a
50 mV holding potential to +10 or +20 mV and then
repolarizing the cell to
30 mV (Fig.
1A).

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Figure 1.
The potassium currents of CPG neurons are faster
than RB sensory neurons. A1, From a holding
potential of 50 mV a CPG (commissural) neuron was depolarized to 10 mV for 20 msec and repolarized to 30 mV (traces are averages of 7 leak-subtracted sweeps). The inset shows the current
during the step. The tail current (bottom left) was
fitted by the equation I = 22 + 1320(exp( t/0.9)) + 317(exp( t/12.1)).
Solid lines show the exponential fits of the fast, slow,
and total currents. A2, Same as
A1 for an RB neuron. The tail current
I = 119 + 321(exp( t/3.8)) + 174(exp( t/24.9)). B, C, Summary of
fitted time constants for the fast and slow components, respectively,
for the different cell types (Co, commissural;
Mo, monopolar; Mu, multipolar). Error bars indicate 1 SEM in this and, unless otherwise specified, subsequent figures. The sample size for each class is indicated. Significance levels of comparisons in this and subsequent figures:
*p < 0.05; **p < 0.01;
***p < 0.001.
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The channel kinetics were similar across cell types that make up
the central pattern generator for swimming but were slower in the Rohon
Beard sensory neurons. We separated the time constants from fits of a
sample of 71 cells according to cell morphology (Fig.
1B,C; see Materials and Methods, Cell
identification). An ANOVA including all cell types was highly
significant (F(3,67) = 22.89 fast and 18.24 slow; p < 0.001 for both). In the planned comparison
of time constants from the different (CPG) cell classes (Fig.
1B,C, Co, Mo, Mu) there was no difference for either
the fast components or IKs between the different
morphological types (F(2,46) = 0.06 fast and
0.42 slow). However, when the CPG groups were pooled and compared with
RB neurons, the RB neurons were significantly slower for both
components (F(1,69) = 70.57 fast and 55.27 slow;
p < 0.001 for both).
A second difference between the cell types is in the fraction of the
total outward current carried by IKs. By
extrapolating the curves fitted to the tail currents back to the moment
of repolarization, the amplitudes of the fast
(IKf and IKNa) and
slow (IKs) components could be estimated.
Using this protocol 22 ± 2% of the tail current was
IKs in CPG neurons compared with 40 ± 2%
in RB cells (n = 49 CPG and 38 RB cells;
p < 0.001). The similarity of the potassium currents
across the CPG classes suggests that they are a homogeneous population
and are quite distinct from the RB neurons. In addition, the
pharmacological properties of RB K+ channels
differed from those of CPG neurons (F. M. Kuenzi and N. Dale,
unpublished results). Thus, we will not consider the RB neurons further
in this paper. Only the properties of K+ currents in
CPG neurons will be described.
Catechol specifically blocks the fast potassium currents
Catechol caused a rapid and reversible block of the
K+ current at voltages lower than +20 mV. At
voltages more positive than +20 mV the block partially reversed with a
slow time course relative to channel opening.
During test steps to +10 or +20 mV the greatest block of the
total current occurred early in the voltage step (Fig.
2A). The dose-response
relationship for the percent block of the peak current early in the
step (Fig. 2B, measured at the arrowhead
in Fig. 2A) was well fitted by the Hill equation with
an IC50 of 9.1 ± 1.9 µM and assuming a
one-to-one binding (Hill coefficient = 1). When the Hill
coefficient was allowed to vary, the best fit was 0.793 ± 0.162, which was not significantly different from 1, and the IC50
was not significantly different from the result using the simpler
equation. The maximum block was 85.0 ± 3.6%, which corresponds
well with the relative amount of fast current in these cells. The
activation of the current became slower between 10 and 100 µM, which again suggested that the slow component was resistant to catechol. The current appeared to reach equilibrium faster
in 1 mM than in 100 µM, which may be
attributable to voltage-dependent unblocking at the lower
concentrations (see below).

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Figure 2.
Catechol selectively blocked the fast
voltage-gated potassium currents. A, Effect of catechol
on currents during the step recorded in control saline and the
concentrations of catechol indicated. The voltage (top
trace) was stepped from a holding potential of 50 mV to 20 mV. B, Summary of the concentration dependence of block
for the current early in the pulse (measured at the
arrowhead in A). Each
point represents the mean of 5-14 cells except that at
500 µM (n = 2). Error bars indicate 1 SD. The points are fitted by the Hill equation,
(Imax I)/Imax × 100 = A/(1 + (IC50/[Cat])h),
where Imax is the peak current in control,
I is the current at this time in different
concentrations of catechol ([Cat]), IC50 is the
concentration that reduces the current by 50%, and h is
the Hill coefficient, here assumed to be 1. C, Catechol
selectively blocks the fast tail current. The dotted
line shows the steady-state current at 30 mV. Tail currents
were measured as described in Figure 1. D, Summary of
the catechol block of the fast (open bars) and slow
(filled bars) tail currents. Sample size is
indicated for each concentration. The significance level of the paired
comparison between fast and slow is indicated (see legend of Fig.
1).
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We examined the tail currents to see whether catechol specifically
blocked the fast component. Increasing the concentration of catechol to
100 and 1000 µM reduced the fast component but had little
effect on the slow component (Fig. 2C,D). Paired comparisons of the percent block at each concentration of catechol showed that the
fast component was blocked significantly more than the slow component
at all concentrations. The dose response for the fast tail current was
very similar to that of the total current (Fig. 2B).
Again, the values in Figure 2D include partial
unblocking during the test pulse (see Fig.
3B).

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Figure 3.
Voltage dependence of catechol- resistant and
-sensitive current. Example of total current in control
(A1) and 100 µM catechol
(A2). A3, Difference
currents, obtained by subtracting traces in A2
from the corresponding ones in A1, show a decay
in the catechol-sensitive current at positive voltages. Test voltages
ranged from 40 to 40 mV in intervals of 10 mV. B, C,
The catechol block of the fast currents partially reverses at positive
voltages. The activation of the fast and slow currents was measured
from the tail currents of a representative cell. B, In
100 µM catechol (filled circles) the activation of the fast current was shifted positive compared with
control (open circles), whereas the shift of the slow
current was small (C). The solid
lines are the best fit of the equation: I
= Imax/(1 + exp[(V V1/2)/slope]) to the data. For the fast current the
values for V1/2 and slope were 8.9 and 7.6 in
control and 30.9 and 8.7 in catechol. The corresponding values for
the slow current were 1.9 and 8.2 (control) and 0.6 and 6.8 (catechol).
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The near total blockade of the fast component suggested that both
IKf and IKNa are
sensitive to catechol. We tested this directly by applying catechol in
the presence and absence of external sodium. Replacing sodium in the
control medium with N-methyl-D-glucamine reduced
the total current by 31 ± 3%. This was the percentage of
IKNa in these cells (Dale, 1993
).
N-Methyl-D-glucamine reduced the block by
catechol by 23 ± 3% (n = 4), which is consistent with an equal block of IKf and
IKNa.
In keeping with the effect on tail currents, the current that remained
in 100 µM catechol activated with a slow time course across the physiological range of voltages (Fig.
3A2). Difference currents obtained by subtracting
the current in 100 µM catechol from the control current
(Fig. 3A1) at each voltage step showed a
fast-activating, partially inactivating current (Fig.
3A3). At voltages of +20 mV and more, the current in
catechol was greater than expected from the dose-response curve
measured at lower voltages; it increased to ~50% of control rather
than 20-30% predicted from Figure 2. This suggested that the block
was voltage-dependent.
We constructed voltage-activation curves from tail currents after long
voltage pulses. The fast and slow components were estimated by
extrapolating the fitted curves back to the end of the test pulse as
before. These curves showed that catechol appeared to shift the
activation of the fast current toward more positive voltages (Fig.
3B). In six CPG cells the voltage for half-activation was
6.9 ± 1.6 mV in control and 26.4 ± 3.4 mV in 100 µM catechol (pairwise p < 0.01). In the
four cells with a measurable slow component the voltage-activation
curve was not shifted significantly (Fig. 3C).
Time dependence of catechol block
We explored the time and voltage dependence of catechol block
further. The process of unblocking was studied by delivering a positive
prepulse of varying duration and measuring the tail currents when the
membrane was returned to
30 mV. In the example in Figure
4A1 the control
current reached its maximum within 3 msec. The fast component of the
tail reached near maximum after 1 msec and decayed slightly with longer
pulses (Fig. 4B). In 100 µM catechol,
however, the fast component increased slowly over several milliseconds
(Fig. 4A2,B). There was no change
in the time course of fast deactivation in the tail current compared
with control, so we interpret this slow "activation" of the fast
component as an unblocking reaction; depolarization causes some of the
blocked channels to become unblocked and pass current during the step,
after which they close according to the normal channel kinetics. Note
that unblocking was never complete; here it recovered to ~50% block.
We measured the time constant for unblocking in three cells to be
3.3 ± 0.4 msec in 100 µM catechol and at +20 mV. In
contrast, the tail currents of IKs increased at
the same rate in control and catechol, as would be expected from the
insensitivity of IKs to catechol (
= 6.3 ± 1.1 and 5.5 ± 0.8 msec in control and catechol, respectively;
n = 3) (Fig. 4C).

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Figure 4.
The fast current showed time-dependent unblocking
and reblocking. A, The pulse length of a voltage step to
20 mV was increased from 1 to 15 msec in control
(A1) and 100 µM catechol (A2). The tail current was fitted with a double
exponential to measure the fast (B) and slow
(C) components in the two conditions (symbols as in A). Points
were fitted by the equation I =
Imax[1 exp( (t/ )]. For
the fast current in this example = 0.3 msec in control (although
there were not enough points for an accurate fit) and 2.7 msec in
catechol, and for the slow current the corresponding values were 4.9 and 4.6 msec. D, Reblocking was measured with twin
pulses to 20 mV separated by a variable interval at 50 mV. The
example shows six pairs of pulses, with the first pulse of each
aligned. In 100 µM catechol, the current during the first pulse activated slowly, but with a short latency the current during the
second pulse activated more rapidly. With longer latencies between
pulses the activation rate slowed. E, The amount of
current that could be blocked was the difference in current between the second (I2) and first
(I1) pulses measured 10 msec after the start of
the pulse (arrows 2 and 1 in
D, respectively). As the interval increased this
difference decreased, and the block approached its steady-state level
(n = 3 cells; the set of intervals was different
for one cell). The fitted curve was (I1 I2) = 0.003 + 0.296exp( t/142 msec).
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Returning the cell to a negative voltage reverses this process and
favors the reblocking reaction. We therefore measured the time
dependence of reblocking by using a twin-pulse protocol (Fig. 4D). In the control, the activation of the current
was the same in both pulses at all interpulse intervals, but in 100 µM catechol (Fig. 4D) the current
during the second pulse activated much faster than the first at short
interpulse intervals. As the interval increased the activation of the
second pulse slowed and became more like the first, indicating a
recovery of block. This recovery of block was examined in three cells
by measuring the current 10 msec after the start of both pulses. The
difference between the current during the first and second pulses at
this point indicates the amount of unblocked current under these
conditions (Fig. 4E). The points were well fitted by
a single exponential, giving a time constant for reblocking of 141 ± 10.1 msec. Thus, IKf and IKNa undergo rapid, partial unblocking during
the voltage step (Fig. 4B) followed by slow
reblocking at the holding potential.
4-Aminopyridine preferentially blocks the fast current
In many types of neuron 4-AP specifically blocks the transient
potassium current IA; however, we found
that in embryonic Xenopus spinal neurons it blocked the
sustained currents at low concentrations. With repeated pulses the
block developed slowly, requiring >20 sec to reach a steady state, and
it was only partially reversible. Like catechol, 4-AP slowed the
activation of the current during the step (Fig.
5A). The concentration
dependence of block for the current early in the pulse was also similar
to that of the block by catechol (Fig. 5B). Assuming a
single binding site, the data were well fitted by the Hill equation,
with an IC50 of 15 ± 12 µM and maximum
block of 82 ± 10%. There was a wide range of responses, with 100 µM causing near complete block (>80%) in some cells and
<50% block in others.

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Figure 5.
4-Aminopyridine blocked both fast and slow
potassium currents. A, During the voltage step the
current during the beginning of the pulse is blocked more than the end.
B, Concentration-response curve for the current early
in the step (arrowhead in A). Error bars
indicate 1 SD (n = 4-17 cells for each point).
C, Tail currents at 30 mV show complete block of the
fast and partial block of the slow component at 100 µM.
The dotted line indicates the steady-state current.
D, Summary of block of the fast (open
bars) and slow (filled bars) tail
currents in 13 cells. The sample size for each concentration is
indicated. Asterisks are as in Figure 1.
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Analysis of the tail currents showed that 4-AP preferentially blocked
the fast component (Fig. 5C). In contrast to the effect of
catechol, these concentrations also significantly reduced the slow
component (p < 0.01 at 100 µM and
p < 0.05 at 1 mM). Nevertheless, at every
concentration the mean block of the fast component was greater than
that of the slow component, and the pairwise differences in block were
significant (Fig. 5D). The poor selectivity of 4-AP rendered
it of limited value for functional studies, so it was not considered
further.
Dendrotoxin-I and
-Dendrotoxin specifically block
IKs
DTX-I blocked the slow component of tail currents by ~40% at
0.5 µM (Fig.
6A,B). The slow
component was blocked more than the fast component in a pairwise
comparison (Fig. 6B), although the fast component was
reduced by a small, but significant, amount. There was no measurable
increase in the block of IKs at the highest concentration tested, 4 µM, nor was the selectivity less.
In keeping with the relative size of IKs,
the current during the step was reduced by only 10-15%.
-DTX
presented a similar picture in the concentration range of 0.5-2
µM (Fig. 6C,D). When tested, the block of
IKs was slowly and only partially reversible
with washing.

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Figure 6.
Dendrotoxin-I and -dendrotoxin block slow
current selectively. A, C, Tail currents
are shown at the bottom left in control and either
dendrotoxin-I (A) or -dendrotoxin
(C). The dotted line shows the
steady-state current. The insets show the current during
the step in control and dendrotoxin as indicated. Traces are averages
of three to four leak-subtracted sweeps. B, D, Summary of changes in the fast and slow tail currents caused by 500 nM DTX-I and 2 µM -DTX, respectively
(n as indicated, and asterisks are as in
Fig. 1). Both toxins caused a significant block of both fast and slow
components. Also, for both toxins the amount of block did not increase
with concentrations >500 nM (data not shown).
|
|
Dendrotoxin causes a small reduction in the sodium current
DTX has been found to modulate INa as well
as blocking Ik in some preparations (Li and
McArdle, 1993
; Schauf, 1987
) but not in others (Halliwell et al.,
1986
). We found that 1 µM DTX-I reversibly reduced the
peak sodium current (stepping from a holding potential of
50 to +10
mV) by 8.8 ± 1.7% (p < 0.01;
n = 6). This was accompanied by a small but significant
shift in the V1/2 for steady-state inactivation of
3.7 ± 0.6 mV (p < 0.01;
n = 5), but there was no change in either the steepness
of the voltage dependence or the time course of inactivation.
Catechol broadens the action potential
The specificity of catechol and DTX allowed us to test the
control that the fast and slow potassium currents have over neuronal firing properties. Whole-cell recordings were made under current clamp
to measure changes in action potential duration and repetitive firing.
To study the repolarizing phase of the action potential, a brief
outward current pulse was delivered to a cell to initiate an action
potential near the end of the pulse (Fig.
7A). We measured spike width
as the time required for the voltage to return from the peak to
one-third of the spike amplitude (resting potential to peak). In the
control, spike width was 1.3 ± 0.1 msec; catechol increased this
to 2.7 ± 0.6 msec at 100 µM (n = 10) and 4.1 ± 0.8 msec at 1 mM (n = 10; Fig. 7A). Both increases were significant at the 5%
level. In a similar protocol and in repetitive firing studies (see
below) the dendrotoxins caused no change in the spike width (mean width
at 0 mV, 1.3 ± 0.1 and 1.2 ± 0.1 msec in control and 1 µM DTX, respectively; n = 5 (Fig.
8A-C).

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Figure 7.
Catechol broadened spikes and slightly inhibited
repetitive firing. A, In current-clamp recordings from a
dissociated neuron a brief outward current pulse triggered a spike
(bottom traces, voltage). One hundred micromolar and 1 mM catechol progressively slowed the repolarizing phase,
broadening the spike compared with control. B,
Repetitive firing of a cell that was depolarized by 80 pA to elicit a
train of spikes in control saline. Ten micromolar and 100 µM catechol reduced the average frequency of firing and thus the number of spikes during the pulse. In this cell the initial frequency was also slightly reduced, but across all cells the change
was not significant. Similar results were seen in cells that exhibited
stronger accommodation.
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Figure 8.
Dendrotoxin has little effect on spike width and
increases repetitive firing. A, B, Current-clamp
recordings from a dissociated cell (A) and a cell
recorded in situ in control (A1, B1) and 1 µM DTX-I
(A2, B2). After perfusing
with 1 µM DTX-I the cells increased their firing, and the
first spike was the same width as in control. C, A
series of pulses of increasing magnitude were delivered to the cell in B to show changes in threshold and repetitive firing
properties in DTX. DTX-I (filled circles)
increased the number of spikes fired at each level of current.
D, For three cells with similar thresholds the initial
firing frequency (1/first interspike interval) is plotted against the
current normalized to the control threshold current. At every current
level the frequency in DTX (filled circles) was
higher than in control (open circles).
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|
Repetitive firing is slightly depressed by catechol but enhanced
by dendrotoxins
Repetitive firing was examined by injecting a series of long
outward current pulses of increasing amplitude, the highest of which
was strong enough to activate multiple action potentials in most cells
(Figs. 7B, 8B). In this study we found
that the firing properties of cells ranged from those that had a graded response (number of spikes and frequency) to the amount of current injected to those that showed moderate or strong accommodation. Despite
this variability in control conditions, the changes in firing caused by
catechol and DTX were similar across cells. We considered changes in
the total number of spikes and the threshold. Because the activity of
cells during swimming suggested that the firing of the first two spikes
was the most functionally relevant repetitive firing characteristic, we
also measured the initial frequency (inverse of first interspike
interval) at the current level that evoked at least two spikes in
control. Both 10 and 100 µM reduced the total number of
spikes during the train, but the change was only significant in 100 µM (p < 0.05; n = 7) (Fig. 7B). Catechol also lowered the threshold for firing
spikes by 20 ± 8% at 10 µM
(p < 0.05). The initial frequency, however, was not affected significantly by either concentration (n = 8 for 10 µM; n = 7 for 100 µM).
Dendrotoxins increased the repetitive firing capabilities of the cells.
One micromolar DTX-I reduced the membrane accommodation, and neurons
became capable of firing many more spikes in response to the same
current injection (n = 10 of 12; Fig.
8A,B). An example of the relationship between current
injected and the number of spikes evoked is shown in Figure
8C, and a similar trend was evident in five of six cells
tested with graded steps. The threshold current decreased in 1 µM DTX-I to 57 ± 9% of control
(p < 0.01; n = 6). In DTX the
cells fired at higher frequencies at each current level. This is shown
for three cells that had very similar thresholds (between 10 and 40 pA)
in Figure 8D. At twice threshold current the
frequency in control corresponded to an interspike interval of 20 ± 1 msec, which was significantly longer than the interspike interval
in DTX-I (17 ± 1 msec; p < 0.05;
n = 3). There were no noticeable differences between
the effects of DTX-I and
-DTX or between isolated neurons and
recordings made from the intact spinal cord, although in the intact
cord repetitive firing was much more reliable in control, and the
membrane potential was much more stable.
The swimming pattern generator is very sensitive to changes in the
slow current
We tested whether catechol block of the fast K+
currents could disrupt the basic pattern of swimming recorded in the
ventral roots of the spinal cord. In control, the swimming pattern is characterized by brief bursts of activity that alternate on the two
sides of the body; a burst on the right occurs midcycle of the burst on
the left (Fig. 9A). The cycle
period ranges from ~50 msec at the beginning of an episode to ~100
msec just before swimming stops. In the presence of 10 µM
catechol, the basic pattern (cycle period, burst duration, and
alternation) was unchanged (Fig. 9A, Table
1). After blocking at least 70% of the
fast current with 100 µM, the embryo was surprisingly
still capable of generating an alternating rhythm with a normal cycle
period and burst duration. However, abnormalities were present, such as
periods during which the ventral root discharge was missing on one side
of the embryo (Fig. 9B). To examine the effects on burst
duration more closely, the rectified and integrated extracellular
record was averaged over 30 cycles in control (Fig.
10, thick line) and in
catechol (Fig. 10, thin line). Ten and 100 µM
catechol did not significantly change the number of spikes fired by
motor neurons, as measured by the area under the curve (Fig. 10; change
in area,
13 ± 12%, n = 4 in 10 µM;
7 ± 16%, n = 4 in 100 µM). The averaging also confirmed that the burst duration
was also unchanged.

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Figure 9.
The swimming pattern is relatively insensitive to
catechol. Records of ventral root activity on the two sides of the
embryo (vrl, vrr, left and right ventral root records,
respectively) show that 10 µM catechol
(A), which is near the IC50 for block of the fast current, has little effect on swimming; 100 µM catechol (B) caused some
abnormalities in the pattern, with discharge absent on some cycles (*).
Segments illustrated are taken 8 sec from the electrical skin stimulus
that initiated the swimming episode.
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Figure 10.
Catechol has no effect, but DTX increases the
burst duration during swimming. Ventral root recordings were rectified,
integrated (2 msec steps), and averaged over the first 30 cycles. In
each panel the thick line is in control, and the
thin line is in the treatment indicated. Although
catechol had no consistent effect on burst shape, DTX increased burst
duration and increased the burst intensity (area under the
curves).
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In contrast to the relative insensitivity of motor pattern generation
to catechol, the spinal circuit was sensitive to both
-DTX and
DTX-I. We found that these abolished the alternating pattern of ventral
root bursts for up to several hundred milliseconds (Fig.
11A). The skin
stimulus evoked continuous and unpatterned activity on both sides,
which was sometimes followed by a period of quiescence before swimming
began. Once swimming had been established, the pattern of alternation
was preserved, but the duration of the ventral root bursts increased
from 9.4 msec in control to 16.2 msec in 1 µM DTX-I
(Table 1). Importantly, the area under the averaged extracellular
records increased by 89 ± 24% (p < 0.01;
n = 7), indicating that more motor neuron spikes
occurred during each cycle (Fig. 10; see Discussion). The effect of DTX on cycle period at both 100 nM and 1 µM was
rather variable, but overall the mean change was not significant (Table
1). In some cases (n = 2; Fig. 11B)
the swimming pattern failed to occur after the initial burst of
activity. In most preparations there was either full or partial
reversal of the prolonged initial ventral root burst with washing (Fig.
11B); however, the change in burst duration was
irreversible.

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Figure 11.
Dendrotoxins disrupt the swimming pattern.
A, Ventral root records from one side at the beginning
and near the end of a swimming episode in control saline and -DTX.
-DTX caused a prolonged burst of activity on both sides, followed by
swimming in which the duration of the ventral root bursts increased.
B, Example in which DTX increased burst duration and
then abolished swimming activity. The initial burst was reversed during
the wash, but the change in burst duration was not.
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DISCUSSION |
Pharmacological dissection of the fast and slow currents
Our results support the hypothesis that slow and fast potassium
channels are distinct at the molecular level. In addition to having
widely different opening and closing kinetics (Dale, 1995a
), the fast
and slow currents were blocked by different agents (catechol and
dendrotoxins, respectively), and they were expressed in different
proportions in nonsensory and Rohon Beard neurons. In light of the
in situ hybridization results of Ribera and colleagues, it
is possible that IKs is coded for (in part) by
Kv1.1, and IKf is coded for by Kv2.2.
IKs is more prominent in Rohon Beard neurons (Fig. 1), which co-localize with expression of a Kv1.1-like transcript (Ribera and Nguyen, 1993
), whereas a Kv2.2 transcript is expressed most
strongly ventrally (Burger and Ribera, 1996
), but
IKf is more prominent. Differences in the
kinetics of the respective channels between the Rohon Beard and the
other neurons could be attributable to other co-expressed
and
subunits in the native channels (Scott et al., 1994
).
For pharmacological agents to be useful in studying how ion channels
influence circuit operation, they must satisfy two criteria: specificity for blocking one or a restricted set of channels, and
maintenance of block during circuit operation. Catechol and DTX appear
to satisfy both of these criteria in the Xenopus embryo; catechol blocks the fast currents, whereas DTX blocks the slow currents. Although we have demonstrated specificity for these two types
of current, some stage 37/38 Xenopus neurons possess a small
IA (F. M. Kuenzi and N. Dale, unpublished
observations), and an "A" current is present in neurons grown in
culture (Ribera and Spitzer, 1990
). Catechol can block
IA in some preparations, but the
IC50 values of 0.5-5 mM (Ito and Maeno, 1986
;
Erdélyi and Such, 1988
; Kehl, 1991
; Sah and McLachlan, 1992
) are
much higher than for block of the fast Xenopus currents. In
the few Xenopus neurons tested, 100 µM
catechol blocked IA by 10-20% (Kuenzi and
Dale, unpublished observations). Such a small block of a rare current
may not be of functional significance at this stage of development. In
addition to blocking IKs, the
dendrotoxins also slightly blocked INa. However,
this is unlikely to complicate our interpretation of the changes in
cell firing or circuit operation, because block of
INa would tend to oppose the increases in
excitability we observed.
The second criterion, that the block is maintained during circuit
activity (swimming), depends on the level of depolarization during
activity within the circuit. During swimming the membrane potential is
tonically depolarized to approximately
30 mV, and cells fire a single
spike (~2 msec long and reaching +20 mV) per cycle (Roberts and Kahn,
1982
; Dale, 1995b
). Thus, although we found a voltage dependence to the
catechol block, most of the time is spent in the voltage range in which
unblocking is not a factor (Fig. 3B). During each action
potential, however, some unblocking would occur, and the total block
would decrease toward its equilibrium value of ~70% at +20 mV (Figs.
2D, 3B). With a cycle period of 70 msec
(Kahn and Roberts, 1982a
,b
) and with the rates of unblocking (during a
square pulse of half of the spike width) and reblocking given above,
this equilibrium will be reached within the first 50 cycles. Because
episodes tend to last a few minutes, the dose-response data of the
fast tail current in Figure 2D is a good measure of
the expected block for most of the episode. We did not see any changes
in swimming early in the episode in 10 µM catechol but
saw them throughout the episode in 100 µM, suggesting
that the sensitivity of the circuit lies between 50 and 70% block of
IKf and IKNa. A similar
argument holds for the DTX block, which has some voltage dependence
(Werkman et al., 1992
). The increase in burst duration occurred
throughout the swimming episodes, so any unblocking was not
functionally significant.
Kinetically distinct potassium currents play different roles in
neural circuit function
The model of the Xenopus swimming circuit produced by
Dale (1995b)
is based on the measured kinetics of the principal voltage and ligand gated channels in stage 37/38 neurons. It incorporated single-compartment neurons and a reduced representation of spinal circuitry. The model reproduced the basic pattern of neuron firing and
the dependence of cycle period on reciprocal inhibition. It also
predicted that IKf and
IKs would have very different roles both in the
control of membrane excitability and in circuit operation. In the
model, reducing IKf by 50% or eliminating it
caused spike broadening and a lowering of threshold. These effects
(Dale, 1995b
, his Fig. 2) are qualitatively very similar to the changes
in spike shape and repetitive firing caused by catechol (Fig. 7). By
contrast, the model predicted a different role for
IKs. Reductions of IKs by
50% in the model had no effect on threshold or spike width but greatly
increased the slope of the frequency-current relation. Like the model,
applications of DTX to real neurons increased the amount and frequency
of repetitive firing at all levels of current injection without
broadening the spike. DTX also greatly lowered the threshold, an effect
not seen in the model. Both IKf and
IKs undergo slow inactivation with long
depolarizing steps. This feature has not yet been included in the
model. With long current injections of the type used in these
experiments, the slow kinetics of IKs may be
important for compensating for inactivation of
IKf. Weakening IKs with
DTX may shift the balance of inward and outward currents late in a
previously subthreshold pulse to allow spiking. Interestingly,
injection of cesium either through sharp microelectrodes (Soffe, 1990
)
or patch electrodes containing low concentrations of cesium (Dale,
1991
) also enhances repetitive firing without affecting spike width.
The simplest explanation of these observations is that low
concentrations of internal cesium preferentially block
IKs.
The model predicts that the swimming circuit is not very sensitive to
changes in IKf but depends very strongly on
IKs. Our results with catechol and DTX support
this prediction; reducing the fast currents by 50% had no effect,
whereas the block of IKs by DTX significantly
altered the swimming pattern. In the model a 50% reduction of
IKs did not disrupt the alternation between the
two sides, but it did cause cells to fire a pair rather than a single
spike in each cycle. In real embryos after treatment with DTX the
alternation of ventral root activity on the two sides during swimming
was normal. However, the ventral root burst duration was greatly
increased. This increase could occur either through motor neurons
firing a second spike during the excitatory phase of the cycle or
through desynchronization of the motorneuron firing. Our data support
the first interpretation. DTX increased the area under the curve of the
averaged ventral root bursts (Fig. 10C). Because there was
no spike broadening, more motor neuron spikes must have occurred during
each cycle. This eliminates simple desynchronization, unless
recruitment from a large pool of previously silent motor neurons
occurred to provide extra spikes. This is unlikely because intracellular recordings from ventral neurons (primarily motor neurons)
suggest that most fire during every swimming cycle (Soffe, 1993
). Also,
recruitment of subthreshold CPG neurons (by application of glutamate)
did not increase burst duration (Soffe, 1996
). In contrast, dual
spiking by motor neurons is consistent with the observed changes in
ventral root activity; the increase in burst duration was ~16 msec,
which was very similar to the minimum interspike interval seen under
current clamp (Fig. 8D), and in some experiments the
averaged ventral root burst clearly showed a second hump (Fig. 10C), as would be expected if cells were firing twin spikes
rather than single ones. We therefore conclude that DTX, by inhibiting IKs, caused a fundamental change that
allowed neurons to fire repetitively during swimming cycles rather than
the single spike, which is characteristic of the embryonic pattern.
Taken together these results confirm the predictions from our earlier
model and suggest that IKs is a "strategic"
current in the Xenopus swimming circuit. It is small in
comparison with other outward currents (20% of the total) yet plays an
important role in the function of the circuit. As such, the slow
current could be a key target for modulation of the whole circuit. In vertebrate neurons some delayed rectifier currents are controlled by
neuromodulators (Rehm and Tempel, 1991
; Hille, 1992
; Grudt and
Williams, 1993
; Simmons and Chavkin, 1996
). The Xenopus
circuit is also regulated by adenosine triphosphate, which inhibits the potassium currents (Dale and Gilday, 1996
). The magnitude of this inhibition is within the range for a specific action on
IKs, and it will be important to
determine whether this is so.
Developmental changes in expression of IKs may
also underlie changes in the swimming motor pattern that occur in the
transition from embryo (stage 37/38) to larva (stage 41). During this
period the pattern matures from the short bursts of ventral root
activity in the embryo to much longer bursts in the larva (Sillar et
al., 1991
). The slow potassium current limits repetitive firing in the
model, and the similarity between the DTX-induced bursts in the embryo
and the 15-20 msec bursts in the larva suggests that downregulation of
IKs may indeed be a key step in the maturation of the motor pattern.
 |
FOOTNOTES |
Received Sept. 29, 1997; revised Nov. 25, 1997; accepted Dec. 2, 1997.
We thank the Biotechnology and Biological Sciences Research Council and
the Royal Society for their generous support. We also thank Dr. William
J. Heitler for his helpful comments on this manuscript.
Correspondence should be addressed to Nicholas Dale, Bute Medical
Building, Westburn Lane, St. Andrews, Fife KY16 9TS, UK.
 |
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