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The Journal of Neuroscience, March 1, 2001, 21(5):1473-1480
Kv2 Channels Form Delayed-Rectifier Potassium Channels In
Situ
Judith T.
Blaine and
Angeles B.
Ribera
Department of Physiology and Biophysics, Medical Scientist Training
Program, University of Colorado Health Sciences Center, Denver,
Colorado 80262
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ABSTRACT |
A non inactivating potassium current known as the delayed rectifier
plays a major role in membrane repolarization during an action
potential. Whereas several candidate genes exist that code for
potassium current, the identities of the molecular isotypes that are
responsible in situ for membrane repolarization remain unidentified. We report that Kv2 channels play a major role in action
potential repolarization. Kv2 channel elimination resulted in a
reduction of the density of noninactivating potassium current and a
prolonged impulse duration. In contrast, suppression of noninactivating
current carried by Kv1 channels was much less effective in increasing
action potential durations. Thus, whereas different potassium channels
encode sustained potassium current, their contributions to action
potential repolarization vary and require direct examination in
situ. Our results indicate that Kv2 subunits function as
classic delayed-rectifier channels in vertebrate neurons.
Key words:
Kv2 channels; potassium current; delayed rectifier; spinal neurons; Xenopus embryo; action potential
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INTRODUCTION |
Voltage-gated potassium channels
determine key signaling properties in the adult nervous system (Adams
et al., 1980 ; Rudy, 1988 ; Storm, 1990 ; Hille, 1992 ; Levitan and
Rogawski, 1996 ). In addition, potassium currents undergo developmental
modulation and dynamically regulate excitability as it emerges in the
embryonic nervous system (Barish, 1986 ; O'Dowd et al., 1988 ; Spitzer
and Ribera, 1998 ). In vivo, various types of voltage-gated
potassium currents, such as noninactivating delayed-rectifier and
inactivating "A" currents, are distinguishable on the basis of
voltage-dependent properties (Hodgkin and Huxley, 1952 ; Connor and
Stevens, 1971 ; Adams et al., 1980 ; Hille, 1992 ). Numerous potassium
channel genes have been identified that might serve as structural
determinants of these different currents (Butler et al., 1989 ; Coetzee
et al., 1999 ). However, progress in matching cloned vertebrate genes to in situ identified currents has met significant obstacles,
including the large number of candidate potassium channel genes, lack
of specific pharmacological tools, and difficulties in establishing a
preparation that allows appropriate genetic manipulation, especially in
the embryonic nervous system.
Kv2 (Shab) potassium channel genes code for molecular
determinants of sustained potassium currents in several species ranging from flies to mammals (Butler et al., 1989 ; Frech et al., 1989 ; Pak et
al., 1991 ; Hwang et al., 1992 ; Burger and Ribera, 1996 ; Patton et al.,
1997 ; Coetzee et al., 1999 ) (but see Quattrocki et al., 1994 ). Although
it is clear the Kv2 channels generate sustained potassium currents, so
do other molecular species of potassium channels (e.g., Kv1, Kv3;
Butler et al., 1989 ; Tsunoda and Salkoff, 1995 ; Rosenthal et al., 1996 ;
Coetzee et al., 1999 ).
Here, we investigate the functional contributions of Kv2 channels to
voltage-dependent potassium current
(IKv) and membrane repolarization of
embryonic spinal neurons. We focus on
IKv because of the pivotal role it
plays in maturation of excitability (Barish, 1986 ; O'Dowd et al.,
1988 ; Spitzer and Ribera, 1998 ). In Xenopus, Kv2.2
transcripts are present in the spinal cord during the period when
action potentials mature from long-duration calcium-dependent impulses
to brief sodium-driven spikes (Gurantz et al., 1996 ; Ribera and Burger,
1996 ). Kv2.2 channels are thus candidate structural determinants of
IKv. However, levels of channel
transcripts do not always reflect the amount of protein or current
produced (Xu et al., 1996 ). Thus, the contribution of each individual
Kv channel isotype to current generation requires direct functional
analysis in situ.
We reduced Kv2 channel function by overexpressing a dominant-negative
Kv2 subunit in embryonic neurons at early stages of differentiation;
this dominant-negative subunit coassembles with either Kv2.1 or Kv2.2
subunits to produce nonfunctional channels (Blaine and Ribera, 1998 ).
In a subpopulation of neurons, IKv was
partially suppressed. Furthermore, action potential durations were
dramatically prolonged. In contrast, functional elimination of another
Kv subfamily that also codes for sustained potassium current (Kv1) had
only subtle effects on action potential duration despite pronounced
effects on IKv density (Ribera, 1996 ).
Finally, mathematical modeling accounted well for the effects of
elimination of Kv1 but not Kv2 channel function.
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MATERIALS AND METHODS |
RNA synthesis. Plasmids were linearized and capped,
and sense RNAs were generated in vitro. RNA concentrations
and integrity were determined spectrophotometrically and by gel electrophoresis.
Embryos and microinjection protocols. In vitro fertilization
and embryo injections were performed as described previously (Jones and
Ribera, 1994 ; Ribera, 1996 ) with the following modifications. Each
blastomere of a two-cell stage Xenopus embryo was injected, with either green fluorescent protein (GFP) and mutant Kv2.2
RNAs or RNase-free rhodamine-conjugated dextran; Kv1.1 RNA was
coinjected with dextran as described previously (Ribera, 1996 ). GFP and
mutant Kv1.1 RNAs were injected at a concentration of 60-80 pg/nl,
whereas dominant-negative Kv2.2 RNA was used at 100-150 pg/nl. The
dominant-negative Kv2.2 subunit is expected to coassemble with either
Kv2.1 or Kv2.2 subunits. However, Kv2.1 mRNA has not been detected in
Xenopus spinal neurons using either in situ
hybridization or single-cell RT-PCR (Burger and Ribera, 1996 ; Gurantz
et al., 1996 ).
Spinal neuron cultures. Stage 18-19 embryos (Nieuwkoop and
Faber, 1967 ) were viewed under epifluorescence to identify embryos expressing GFP and rhodamine fluorescence on opposite sides of the
neural tube. Isolated cell cultures were prepared as described previously (Spitzer and Lamborghini, 1976 ; Blair, 1983 ; Ribera and
Spitzer, 1989 ). A 10-15 min incubation in divalent cation solution,
without enzymatic treatment, sufficed for cell dissociation (Spitzer
and Lamborghini, 1976 ). Neurons were studied within 27 hr of plating.
The acute nonenzymatic dissociation of neurons and brief time in
culture combines advantages of both in vivo (e.g., normal
development) and in vitro (e.g., spatially compact, isolated
cells) model systems. Neurons in culture were identified as either
control (rhodamine-positive) or +Mutant (GFP-positive).
Electrophysiological methods. Tight-seal, whole-cell
recordings (Hamill et al., 1981 ) were made from immature (3-7 hr in
culture) or mature (15-27 hr in culture) neurons. Whole-cell currents
were recorded with an Axopatch 1-D amplifier (Axon Instruments, Foster City, CA) in conjunction with a TL-1 data interface and pClamp6. Recordings were obtained at room temperature only from neurons with
short processes (<50 µm). Electrodes were pulled from borosilicate glass and had resistances ranging from 2 to 3.9 M when filled with
the standard pipette solution (in mM: 100 KCl, 10 EGTA, and 10 HEPES, pH 7.4).
Cell capacitance was used to determine membrane surface area (1 µF/cm2) and normalization of current
amplitudes to densities. Recordings were excluded if the access
resistance changed during a recording or if the input resistance was
<0.5 G . The neuronal membrane was held at 80 mV and stepped for
60 msec in 10 mV increments to voltages ranging between 60 and +90
mV. Currents were filtered at 5 kHz and digitized at 25 kHz. Leak
subtraction was achieved using a modified P/4 protocol (pClamp6).
For IKv, the bath solution contained
80 mM NaCl, 3 mM KCl, 5 mM MgCl2, 10 mM CoCl2, 5 mM HEPES, pH 7.4, and 1 µM tetrodotoxin (TTX; Calbiochem, La Jolla,
CA). Steady-state IKv amplitudes were measured by averaging values during a 7 msec interval at the end of the pulse. ICa was recorded using a
bath solution containing 40 mM NaCl, 40 mM TEA, 3 mM KCl, 10 mM CaCl2, 5 mM HEPES, pH 7.4, and 1 µM TTX. Electrodes were filled with 100 mM CsCl, 10 mM
tetraethylammonium-Cl, 10 mM EGTA, and 10 mM HEPES, pH 7.4, with CsOH.
Conductance densities were obtained by dividing current densities by
driving force using a calculated potassium equilibrium potential of
91.6 mV. Conductance-voltage (G-V) data were fit with the Boltzmann equation (G = Gmax/{1
+exp[(V1/2 V)/k]}) to
obtain the maximal Gmax,
V1/2, and slope factor (k).
Similar values were obtained when G-V curves were
constructed by measuring the amplitude of tail currents when the
membrane was returned to 40 rather than 80 mV, suggesting that
single-channel current-voltage relationships were linear over the
voltage range examined. Furthermore, there was no correlation between
current amplitude-density and the reversal potential of the current,
suggesting that Ek was constant during
the 60 msec depolarization. Current and conductance-density plots were
not corrected for the voltage error introduced by the series
resistance, which ranged between 3 and 9 M . Time to half-maximum current (t1/2) was measured using
Axograph 3. For examination of t1/2
and Gmax values for
IKv of individual neurons, we binned values and then plotted the percentage of neurons having the value in a
particular bin (histograms of Figs. 3, 4).
Action potentials were recorded in the current-clamp mode. The neuronal
membrane potential was set to 80 mV by steady-state current
injection, and depolarizing current (2.5 msec) was injected to elicit
an impulse. The bath solution contained (in mM): 125 NaCl,
3 KCl, 10 CaCl2, and 5 HEPES, pH 7.4. Analysis of
action potentials entailed measurement of the following parameters:
overshoot, amplitude, maximum rate of rise, time to peak, and time to
half-decay from the peak. We refer to the time to half-decay as the
duration of the action potential, because we are interested primarily
in repolarization of the action potential.
Data analysis. Mean values ± SEM are presented.
Differences between means were analyzed using the nonparametric
Mann-Whitney U test (two-tailed), and p
values 0.05 indicated statistical significance.
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RESULTS |
If Kv2 channels contribute to the endogenous
IKv, neurons containing exogenous
mutant Kv2 transcripts (+Mutant) would be expected to
display alterations in IKv such as a
reduction in density. Indeed, mean IKv
densities in +Mutant neurons were 40 and 26% smaller than
those in corresponding controls at immature and mature times in culture
(p < 0.04; +30 mV; Fig.
1). These data indicate that Kv2 channels
contribute to the endogenous IKv at
both early and mature times. In control neurons,
IKv showed its normal developmental threefold increase in density (Fig. 1). Similarly, in
+Mutant neurons, IKv
displayed an approximately threefold increase in density during the
same developmental period, suggesting that upregulation of other Kv
channels persists.

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Figure 1.
Elimination of Kv2 channel function led to a
reduction in IKv density. A,
IKv was recorded from control
(top) or +Mutant (bottom)
neurons at either immature (left) or mature
(right) stages. The neuronal membrane was held at 80
mV and stepped to potentials ranging between 60 and +90 mV. Currents
elicited for steps to 60, 40, 20, 0, +20, and +40 mV are shown.
B, Current density-voltage (I-V)
plots for IKv recorded from immature
(left) or mature (right) neurons. At both
stages, the dominant-negative Kv2 mutant led to a reduction in current
density over a range of voltages.
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The reduction in IKv density is
consistent with the known expression pattern of Kv2.2 mRNA and the
documented effects of the dominant-negative subunit on Kv2 channel
function (Burger and Ribera 1996 ; Gurantz et al., 1996 ; Blaine and
Ribera, 1998 ). Nonetheless, we examined the possibility that the mutant
subunit might have additional or nonspecific actions that would lead
indirectly to a reduction in IKv.
Measures of passive membrane properties were similar in Control and
+Mutant neurons (Table 1),
suggesting a lack of nonspecific effects. Furthermore, heterologous
coexpression of dominant-negative Kv2.2 with Kv1.1 subunits did not
reduce current amplitudes compared with those induced by the same dose of Kv1.1 RNA injected alone (n = 32; data not shown).
In addition, we examined another voltage-dependent current, calcium
current (ICa).
ICa did not differ between Control and
+Mutant neurons, further demonstrating the specificity of
the mutant Kv2 subunit (Fig. 2).

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Figure 2.
Elimination of Kv2 channel function did not affect
calcium current (ICa).
A, Representative ICa traces
recorded from mature control (left) and
+Mutant (right) neurons are similar. The
neuronal membrane was held at 80 mV, and currents were elicited by
stepping the membrane to potentials ranging between 60 and +90 mV.
Currents elicited by steps to 30, 20, +20, +30, +40, and +50 mV are
shown. B, Peak density and voltage dependence were
similar for control and +Mutant neurons.
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In contrast to effects on current density, overexpression of the
dominant-negative Kv2 subunit did not affect the kinetics of activation
of IKv. There was no significant
difference in mean t1/2 values for
IKv recorded from immature or mature
+Mutant neurons compared with age-matched controls (Fig.
3A,B).
Spinal neurons represent a heterogeneous population of neurons, and it
is possible that the mean results could obscure effects in
subpopulations of neurons. However, examination of histograms of
t1/2 values for
IKv recorded from individual neurons
revealed similar distributions (Fig. 3C,D).

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Figure 3.
Elimination of Kv2 channel function had minimal
effect on activation kinetics of IKv.
A, B, Time to half maximum
(t1/2) of
IKv recorded from either immature
(A) or mature (B) neurons.
At either stage in culture, overexpression of the dominant-negative
subunit led to minimal if any difference in the average
t1/2. C, D, Distribution of
t1/2 values in individual neurons also
revealed little difference between control and +Mutant
neurons at either immature (C) or mature
(D) stages. The histograms present data obtained
+0 mV, a voltage at which the average values showed a small,
nonsignificant difference (A, B).
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Examination of the effects of the mutant Kv2 subunit on current density
were evident over a broad range of voltages (Fig. 1B), suggesting a decrease in the number of
functional channels. To examine this possibility more directly, we
constructed conductance density versus voltage (G-V)
plots. Control neurons showed the normal developmental increase in
conductance density (Fig.
4A,B). Similarly, conductance density was developmentally upregulated in
+Mutant neurons. However, both immature and mature
+Mutant neurons demonstrated a decrease in conductance
density compared with stage-matched controls. Maximal conductance
density (Gmax) values for immature
+Mutant and Control neurons were 3.9 ± 0.5 and
6.5 ± 0.9 pS/µm2, respectively
(p < 0.05), indicating that overexpression of
the mutant subunit produced a 40% reduction in
Gmax. In mature +Mutant and
Control neurons, Gmax values were
13.7 ± 1.0 and 21.5 ± 1.5 pS/µm2 (p < 0.0002), indicating that overexpression of the mutant subunit reduced
Gmax to the same extent in immature
and mature neurons. Because the reduction in
Gmax obtained at immature and mature times did not vary (40 and 36%, respectively), the inferred
proportions of Kv2 channels are similar. The mutant subunit may have
produced this effect by decreasing either the number of functional
channels, the single-channel conductance, or
Popen. These results suggest that functional Kv2
channels are not selectively upregulated during development.

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Figure 4.
Elimination of Kv2 channel function reduced the
maximum conductance density (Gmax).
A, C, Conductance density-voltage plots for
IKv recorded from either control or
+Mutant neurons at immature (A)
and mature (C) stages. Overexpression of the Kv2
mutant subunit led to a ~40% reduction in the average conductance
density at both stages. B, D, Histograms
for Gmax of IKv
recorded from individual immature (B) and mature
(D) neurons. The distribution was shifted to
smaller values of Gmax for
+Mutant neurons at both immature
(B) and mature (D) stages.
E, At mature stages, overexpression of the
dominant-negative subunit shifted V1/2
by approximately 4 mV, as determined by fits to the Boltzmann
equation (see Materials and Methods); in this panel, the lines through
the data are the Boltzmann fit. F, Results for data that
were either not corrected ( Comp) or corrected (+Comp)
electronically for the series resistance are shown;
*p < 0.005, **p < 0.002 (control vs +Mutant).
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At early times, reductions in current densities (+30 mV; Fig. 2) and
Gmax were similar (40 vs 36%).
However, these values differed at late times (26 vs 36%). This
difference might arise if the voltage dependence of steady-state
activation is altered by elimination of Kv2 channels in mature but not
immature neurons. In immature Control or +Mutant neurons,
V1/2 was the same (18.9 ± 1.9, Control; 18.9 ± 1.8, +Mutant). In contrast, there was
a significant, albeit small (~4 mV), leftward shift in the average V1/2 of currents recorded from mature
+Mutant neurons compared with controls (Fig.
4B, inset). The shift in
V1/2 may arise from the series resistance
and a larger voltage error when current amplitudes are increased, as in
mature neurons. However, in a subset of neurons (n = 18), series resistance was electronically compensated, and a
significant leftward shift in V1/2 was
still observed (Fig. 4E,F).
Examination of conductance densities in individual neurons revealed
that the mutant subunit did not result in complete elimination of
IKv in any neuron (Fig.
4B,D). Similar results were
obtained when the dose of mutant RNA used was either 100 or 150 pg/nl, suggesting that the concentrations of RNA used were saturating. Furthermore, this dose was higher than that used previously for overexpression of dominant-negative Kv1 subunits (80 pg/nl; Ribera, 1996 ). These data are consistent with the possibilities that non-Kv2 channels carry the residual IKv
remaining after elimination of Kv2 channels and that multiple molecular
species of potassium channels contribute to the total
IKv.
The mutant Kv2 subunit dramatically decreased current density without
inducing obvious effects on activation kinetics. In contrast, antisense
suppression of Kv3.1 subunits in Xenopus spinal neurons led
simultaneously to a slowing of the activation kinetics and a reduction
in current density (Vincent et al., 2000 ). To enhance detection of
subtle effects of the Kv2 mutant on activation kinetics, we examined
simultaneously activation kinetics and conductance density in
individual neurons (Fig. 5). Whereas
Gmax was clearly reduced in a large
proportion of +Mutant neurons,
t1/2 values in these neurons were
not different from controls. In sum, the results indicate
that elimination of Kv2 channels ledto a reduction in
Gmax, a small negative shift in
V1/2 but no change in
t1/2.

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Figure 5.
Elimination of Kv2 channels led to reduction in
Gmax without effects on activation kinetics.
Plots for Gmax as a function of
t1/2 for IKv
recorded from individual immature and mature neurons reveal that the
principal effect of the Kv2 mutant subunit was on conductance rather
than activation kinetics.
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Given the pivotal role IKv plays in
maturation of the action potential, alterations in its properties would
be expected to alter the waveform of the action potential (Barish,
1986 ; O'Dowd et al., 1988 ; Lockery and Spitzer, 1992 ). We incorporated
the observed changes in Gmax and
V1/2 of
IKv into a mathematical model of the
action potential to calculate effects on the impulse (Lockery and
Spitzer, 1992 ). We also simulated action potentials produced by
reducing Gmax alone, a condition
modeling suppression of Kv1 channels which was previously found to
reduce current density (Ribera, 1996 ). Reduction of current density by
itself (i.e., suppression of Kv1 channels) resulted in a slightly more
prolonged action potential than did reduction of current density
combined with a negative shift in V1/2
(simulation of Kv2 channel elimination). The durations of the simulated
impulses were prolonged by factors of 1.25 and 1.11, respectively.
We compared simulated action potentials to ones recorded from mature
control and +Kv1 or +Kv2 Mutant neurons. Suppression of Kv1
channel function led to an average 1.5-fold (but statistically not
significant) prolongation of the impulse duration, which closely matched the mathematical prediction (1.25-fold increase; see Fig. 7A, Table 2). Elimination of
Kv2 channel function resulted in an average fourfold increase in action
potential duration in +Mutant neurons compared with controls
(see Fig. 7A, Table 2). This finding contrasts dramatically
with the simulated impulse, which was prolonged by a factor of only
1.11 (Fig. 6). In individual neurons,
dominant-negative Kv1 subunits increased the duration by at most a
factor of 4, whereas mutant Kv2 subunits produced up to a 35-fold
increase (Fig. 7B,
inset). Surprisingly, Kv2 currents played a major role in
sculpting the waveform of the impulse, a result not predicted by the
mathematical model.

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Figure 6.
Mathematical simulation of action potentials
incorporating observed effects of elimination of Kv1 versus Kv2 channel
function elimination. The mathematical model derived by Lockery and
Spitzer (1992) was run under control (thick dotted line)
and variant IKv conditions for mature
neurons. Gmax was reduced by 33% alone (Kv1
elimination, thin dotted line) or in combination with a
5 mV shift in V1/2 (Kv2 elimination,
solid line). The horizontal dashed line
indicates the value of half-repolarization, the voltage at which the
impulse duration is determined; its leftmost position is at the time to
peak. A simulated action potential produced by reducing
Gmax by 82% ("observed", thick
dashed line) had a fourfold increase in its duration. The
duration of the impulse is defined here as the time between the peak
and half-repolarization and was 1.12, 1.25, and 4-fold that of control
for Kv2 elimination, Kv1 elimination, and "observed",
respectively.
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Figure 7.
Elimination of Kv2, but not Kv1, channels led to
significant prolongation of the duration of the action potential.
A, Action potentials were recorded from mature neurons
using the current-clamp mode of the patch-clamp amplifier. A steady
level of current was injected to hold the neuronal membrane at
approximately 80 mV. Impulses were elicited by a 2.5 msec
depolarizing current pulse. Examples representing the "average"
impulse recorded from control (left), +Kv1
Mutant (middle), and +Kv2 Mutant
(right) neurons are presented. B,
Histogram presenting the distributions of durations of the action
potential recorded from control, +Kv1 Mutant, and
+Kv2 Mutant neurons. All mature control neurons had
impulse durations of <3 msec. Elimination of Kv2 channels shifted the
distribution to much larger values than did suppression of Kv1
channels. The duration of the impulse is defined as the time between
peak and half-repolarization. Inset, In one +Kv2
Mutant neuron, the action potential had an unusually long
duration, and repolarization was not observed during the recording
sweep. One neuron (*) fired an action potential with an unusually long
duration, as shown in the inset (*).
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Nonspecific effects are unlikely to account for the increased duration
of the impulse because passive membrane properties and
ICa were unaffected (Fig. 2, Table 1).
Furthermore, there was no significant difference in the overshoot of
action potentials recorded from +Mutant or control neurons
(Table 2). The maximum rates of rise did not differ significantly
between control and +Kv2 Mutant neurons or between
+Kv1 and +Kv2 Mutant neurons; however, there was
a difference between control and +Kv1 Mutant neurons (Table
2). Overall, these latter findings suggest that sodium current
densities were unaffected by the Kv2 dominant-negative subunit,
although there may have been effects of the Kv1 dominant-negative subunit. Resting membrane potentials recorded from +Kv1 or
+Kv2 Mutant neurons appeared more depolarized than those
recorded from controls (Table 2), but the differences were not
statistically significant. Furthermore, there was no correlation
between resting membrane potential and impulse duration (data not
shown). Moreover, for recording of action potentials, the holding
potential of the neuronal membrane was forced to 80 mV by injection
of steady current.
The mathematical model accounted well for the observed effects of
elimination of Kv1 but not Kv2 channels (compare Figs. 6, 7). An 82%
reduction in Gmax was required to
simulate the average fourfold increase of the impulse duration observed
after elimination of Kv2 channel function (Fig. 6). Such a dramatic
reduction in channel number is much larger than that produced by Kv2
channel elimination (Fig. 4A,B).
Taken together, the results indicate that ventral spinal neurons
provide an appropriate environment for Kv2 channels to function
in situ as efficient delayed-rectifier channels.
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DISCUSSION |
Our results demonstrate that efficient membrane repolarization
during an action potential requires Kv2 channel function in some
Xenopus spinal neurons. These data are consistent with the restricted expression pattern of Kv2.2 gene in the Xenopus
spinal cord (Burger and Ribera, 1996 ). In addition,
IKv was not completely eliminated in
any neuron, and some neurons appeared resistant to the mutant Kv2
subunit (Figs. 1, 4). One possible scenario is that Kv2 channels are
found in a subset of spinal neurons in combination with other Kv
channels. A similar conclusion has been reached for mammalian CNS
neurons by comparison of the properties of whole-cell potassium current
to the Kv gene expression profile of individual cells (Martina et al.,
1998 ; Baranauskas et al., 1999 ). In contrast, Kv2 (Shab)
channels are the sole determinant of sustained potassium current in
Drosophila neurons (Tsunoda and Salkoff, 1995 ).
Interpretation of our data warrants caution because the exact dose of
dominant-negative Kv2 RNA delivered to any individual neuron was
unknown. However, we obtained similar results with two different
concentrations of dominant-negative Kv2 RNA, suggesting that saturating
dosages were used.
Overexpression of the dominant-negative Kv2 subunit resulted in slower
activation kinetics of IKv. These data
were surprising in light of the slow activation of heterologously
expressed Kv2 channels (Burger and Ribera, 1996 ; Blaine and Ribera,
1998 ). It is possible that Kv2 subunits in situ
contribute to channels that activate more rapidly than do homomeric
channels expressed heterologously. Whereas the molecular mechanism is
not yet known, Kv2 subunits in situ might form heteromeric
complexes with members of the Kv5-Kv9 subfamilies; the latter
coassemble with and modify the properties of the resultant channel in
heterologous systems (Hugnot et al., 1996 ; Post et al., 1996 ; Salinas
et al., 1997a ,b ). In addition, Kv2 channel function has been shown to
be modified by RNA editing and channel subunit phosphorylation
(Murakoshi et al., 1997 ; Patton et al., 1997 ).
We also observed a small but significant shift in the
V1/2 of steady-state activation. It is
possible that a negative shift could be produced by voltage errors
arising from the series resistance. However, our test of this
possibility indicated otherwise. An alternative explanation for the
negative shift in V1/2 is that neuronal
Kv2 currents have uniquely positive voltage dependencies, consistent
with the relatively depolarized activation properties (V1/2 = 25-35 mV) of heterologously
expressed Kv2 channels (Burger and Ribera, 1996 ; Blaine and Ribera,
1998 ). If the voltage dependencies of activation of Kv2 neuronal and
oocyte currents are similar, suppression of endogenous neuronal Kv2
currents by the dominant-negative mutant should result in a leftward
shift in the V1/2 of residual IKv, as we observed. These data
suggest that the voltage dependence of the steady-state activation
properties (i.e., V1/2) of Kv2 currents in
their native location versus a heterologous system are similar, whereas
the kinetics of activation differ in these two environments (Fig.
3).
Gene expression profiling of mammalian CNS neurons suggested that
native Kv2 currents vary greatly in their voltage sensitivities, with
inferred V1/2 values ranging between 18
and 3 mV (Martina et al., 1998 ; Baranauskas et al., 1999 ). Direct
examination of Kv2.1 currents in hippocampal neurons using blocking
antibodies revealed a higher threshold current with a more positive
value for V1/2 (15 mV; Murakoshi and
Trimmer, 1999 ), similar to what is observed after heterologous
expression of recombinant Kv2 channels. In contrast, antisense
elimination of Kv2.1 channels in hippocampal neurons suggested that
endogenous Kv2 currents were low-threshold and had a more negative
V1/2 (Du et al., 2000 ). The disparate values for V1/2 may reflect cell- and
activity-dependent modifications of Kv2 channels that occur in
situ. Consistent with this possibility, target cells modify the
voltage sensitivity of the native IKv in Xenopus motoneurons (Nick and Ribera, 2000 ). In the
present study, we restricted analysis to neurons that did not contact other cells to exclude effects of contact-dependent activity on IKv activation properties.
In Xenopus, cloned genes that might encode the non-Kv2
residual IKv include several Kv1
isotypes, Kv3.1, and Kv4.3 (Ribera, 1990 ; Ribera and Nguyen, 1993 ;
Lautermilch and Spitzer, 1997 ; Gurantz et al., 2000 ). Their
contribution to IKv, although not essential for membrane repolarization, might determine firing frequencies and subthreshold behavior. The Kv1.1 gene has a dorsal expression pattern, whereas that of the Kv1.3 gene is more widespread (Ribera and Nguyen, 1993 ) (A. D. Hofmann and A. B. Ribera,
unpublished observations). Kv3.1 mRNA localizes to interneurons
initially and to other spinal neurons at mature stages (Gurantz et al., 2000 ). Antisense elimination of Kv3.1 gene products results in partial
suppression of IKv and almost a
doubling of the duration of the action potential in ~40% of spinal
neurons (Vincent et al., 2000 ).
Mathematical modeling of the effects of elimination of Kv1 or Kv3.1 or
channels on IKv predicted well the
observed consequences on the action potential (Vincent et al., 2000 ;
this study). However, the model underestimated the effects of Kv2
channel elimination. The model was based on whole-cell currents and did
not consider the effects of channel distribution. Immunocytochemical
data indicate that Kv2.2 channels form clusters, whereas Kv2.2 channels
are more diffusely localized in mammalian neurons (Hwang et al.,
1992 ; Maletic-Savetic et al., 1995 ; Rhodes et al.,
1995 ). In addition, neurons expressing Kv2 channels may possess
a unique repertoire of ion channels not well represented by the
computer model. This hypothesized ensemble of ion channels may provide
the appropriate environment for Kv2 channels to function in
situ as the primary determinants of action potential
repolarization. Consistent with this possibility, Kv2.2 mRNA localizes
to the ventral but not dorsal spinal cord; in contrast, the gene coding
for calcium-activated potassium current (xSlo) is expressed by dorsal
but not ventral spinal neurons (Chouinard et al., 1994 ; Burger and
Ribera, 1996 ).
Key output neurons of the nervous systems of flies, squid, amphibia,
and mammals express Kv2 channels (Butler et al., 1989 ; Frech et al.,
1989 ; Pak et al., 1991 ; Hwang et al., 1992 ; Quattrocki et al., 1994 ;
Burger and Ribera, 1996 ; Patton et al., 1997 ; Coetzee et al., 1999 ). In
the mammalian CNS, virtually every neuron expresses Kv2 mRNA
(Murakoshi and Trimmer, 1999 ). Thus, firing properties of
several different types of neurons depend on Kv2 channel function in situ. Physiological studies have demonstrated that
specific functional components of a current are dynamically modified in response to changes in input or development (Barish, 1986 ; O'Dowd et
al., 1988 ; Turrigiano et al., 1994 ; Desai et al., 1999 ; Golowosch et
al., 1999 ; Spitzer, 1999 ; Nick and Ribera, 2000 ). Matching functional
current components in situ to their structural counterparts provides essential information for identification of molecular mechanisms underlying development and plasticity of neuronal signaling.
 |
FOOTNOTES |
Received Sept. 7, 2000; revised Nov. 21, 2000; accepted Dec. 21, 2000.
This work was supported by National Institutes of Health Grants MH11349
(J.T.B.), T32-NS07083, and NS25217 (A.B.R.). We thank M. Klymkowsky for
the Ultra-GFP vector, I. Hsieh, S. Lockery, and N. C. Spitzer for
assistance with mathematical modeling, A. Hofmann, M. Lazaroff, A. Linares, T. Nick, and K. Svoboda for discussion, and W. J. Betz
for comments on this manuscript.
Correspondence should be addressed to Angeles B. Ribera, Department of
Physiology and Biophysics, C-240, University of Colorado Health
Sciences Center, Denver, CO 80262. E-mail: Angie.Ribera{at}UCHSC.edu.
 |
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