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The Journal of Neuroscience, September 1, 2000, 20(17):6734-6740
Adjustable Amplification of Synaptic Input in the Dendrites of
Spinal Motoneurons In Vivo
Robert H.
Lee and
C. J.
Heckman
Departments of Physiology and Physical Medicine and Rehabilitation,
Northwestern University Medical School, Chicago, Illinois 60611
 |
ABSTRACT |
The impact of neuromodulators on active dendritic conductances was
investigated by the use of intracellular recording techniques in spinal
motoneurons in the adult cat. The well known lack of voltage control of
dendritic regions during voltage clamp applied at the soma was used to
estimate dendritic amplification of a steady monosynaptic input
generated by muscle spindle Ia afferents. In preparations deeply
anesthetized with pentobarbital, Ia current either decreased with
depolarization or underwent a modest increase at membrane potentials
above
40 mV. In unanesthetized decerebrate preparations (which have
tonic activity in axons originating in the brainstem and releasing
serotonin or norepinephrine), active dendritic currents caused strong
amplification of Ia input. In the range of
50 to
40 mV, peak Ia
current was over four times as large as that in the
pentobarbital-anesthetized preparations. Exogenous administration of a
noradrenergic agonist in addition to the tonic activity further
enhanced amplification (sixfold increase). Amplification was not seen
in preparations with spinal transections. Overall, the dendritic
amplification with moderate or strong neuromodulatory drive was
estimated to be large enough to allow the motoneurons innervating slow
muscle fibers to be driven to their maximum force levels by remarkably
small synaptic inputs. In these cells, the main role of synaptic input
may be to control the activation of a highly excitable dendritic tree. The neuromodulatory control of synaptic amplification provides motor
commands with the potential to adjust the level of amplification to
suit the demands of different motor tasks.
Key words:
motoneuron; spinal cord; neuromodulation; electrophysiology; serotonin; norepinephrine; plateau potential; bistable; dendritic amplification
 |
INTRODUCTION |
Voltage-sensitive conductances
within the dendritic tree of the postsynaptic neuron play a major role
in synaptic integration (Johnston et al., 1996
; Yuste and Tank, 1996
).
Many types of voltage-sensitive conductances are under the control of
neuromodulatory inputs acting via second messenger systems. Thus, the
potential exists for the neuromodulatory inputs to control synaptic
integration by altering the activation of voltage-sensitive currents in
the dendrites of neurons.
The spinal motoneuron is subject to potent neuromodulatory control by
axons that originate in the brainstem and release either serotonin
(5-HT) or norepinephrine (NE) (Hounsgaard et al., 1988
; Takahashi and
Berger, 1990
; Wang and Dun, 1990
; White et al., 1991
; Binder et al.,
1996
). In the presence of these neuromodulators, motoneurons exhibit a
persistent inward current (Houns-gaard and Kiehn, 1989
; Svirskis
and Hounsgaard, 1998
; Lee and Heckman, 1999a
). The composition of this
current may vary in different types of motoneurons (Hounsgaard and
Kiehn, 1989
; Hsiao and Chandler, 1995
; Zhang et al., 1995
; Lee and
Heckman, 1998b
). In spinal motoneurons in the adult cat, the total
persistent inward current (IPIC) is exceedingly large (Lee and Heckman, 1998a
, 1999a
). Activation of
IPIC can produce prolonged
self-sustained firing or, when spikes are blocked, long-lasting plateau
potentials. Both of these phenomena can be subsequently deactivated by
a brief inhibitory input, allowing the motoneuron to act in a bistable
manner (Hounsgaard et al., 1988
; Lee and Heckman, 1998a
).
The dendritic tree of the spinal motoneuron is especially large,
consisting of multiple primary trunks each with branches extending as
far as 2 mm from the soma (for review, see Binder et al., 1996
).
Serotonergic receptors are densely distributed throughout this
extensive dendritic tree (Alvarez et al., 1998
). Similar data for
noradrenergic receptors are not yet available, but the high density of
these receptors in the ventral part of the spinal cord (Giroux et al.,
1999
) suggests that the noradrenergic input also has a potent impact on
the dendrites of spinal motoneurons. Most of
IPIC is generated in the dendritic
tree (Hounsgaard and Kiehn, 1993
; Lee and Heckman, 1998b
, 1999b
), where
it can be readily affected by dendritic neuromodulatory receptors and
where it may have a major impact on synaptic integration.
Our hypothesis was that the dendritic portion of
IPIC acts as a potent amplifier of
steady-state synaptic input to spinal motoneurons, allowing even a
small synaptic input to generate large currents at the soma of the
cell. We further hypothesized that changes in the level of
neuromodulatory drive to motoneurons would provide a control system for
this highly potent dendritic amplification. These hypotheses were
tested by the use of intracellular recordings in motoneurons in the
lumbar spinal cord of the cat. Amplification of synaptic current was
assessed with a single-electrode voltage-clamp technique that
controlled somatic voltage-sensitive conductances while assessing the
impact of an excitatory synaptic input on the dendritic component of
IPIC.
 |
MATERIALS AND METHODS |
Surgical preparation. A total of 19 experiments were
performed. Of these, 16 used an unanesthetized decerebrate preparation (3 of these were also spinalized), and 3 used a
pentobarbital-anesthetized preparation. All procedures were approved by
the animal care committee at Northwestern University. Full details are
available in previous publications (Heckman et al., 1994
; Lee and
Heckman, 1998a
). Briefly, all surgical preparations of the spinal cord
and hindlimb were done under deep gaseous anesthesia (1.5-3.0%
isoflurane in a 3:1 mixture of O2 and
N2O). The preparation included a laminectomy to
expose the L7 and S1 segments of the cord for intracellular recording
as well as isolation of the Achilles tendon and the nerves to the
medial gastrocnemius (MG) and lateral gastrocnemius-soleus (LGS)
muscles. In the decerebrate experiments, the gaseous anesthesia was
discontinued after a precollicular decerebration in which all forebrain
anterior to the colliculi was removed. In three of these experiments,
the spinal cord was fully transected at the thoracic level (T9-T10).
In three additional experiments, decerebration was not performed, and
instead the animal was switched to pentobarbital anesthesia via
intravenous administration of an initial dose of 65 mg/kg. All
preparations were then paralyzed with Flaxedil and artificially
respired. In addition, a bilateral pneumothorax was done to enhance
intracellular recording stability. In the pentobarbital-anesthetized
preparations, supplemental doses were given as needed to maintain a
stable blood pressure and to provide continued absence of withdrawal
reflexes, which were periodically tested by allowing the preparation to
recover from paralysis. At the end of the experiment, the animals were
killed with a lethal dose of pentobarbital.
Intracellular recordings of motoneurons. The nerves to the
MG and LGS muscles in the hindlimb were placed on hook
electrodes for stimulation. Intracellular recordings of motoneurons
antidromically activated by stimulation of the MG and LGS nerves were
obtained in the lumbar cord with sharp microelectrodes. Microelectrode tips were broken back under microscopic observation and control. Because of the large currents required for successful single-electrode voltage-clamp techniques in spinal motoneurons, resistances of the
electrodes were kept low
typically ~3-4 M
in saline before entering the cord. Electrodes were filled with a solution combining potassium citrate (0.5 M) and potassium chloride (1.5 M). Voltage clamp was achieved by the use of the
discontinuous, single-electrode voltage-clamp mode of our amplifier
(Axoclamp 2A amplifier; Axon Instruments) (Finkel and Redman, 1985
).
Switching rates typically varied between 8 and 11 kHz. Head stage
output was monitored at all times to assess settling of electrode
transients. Data with inadequate settling were rejected. The clamp
feedback gains ranged from 10 to 40 nA/mV. In addition, feedback gain
at low frequencies was increased to 100-400 nA/mV by adding an
external low-frequency feedback loop (
3 dB at 30 Hz; gain of 10),
which virtually eliminated steady-state errors in voltage (cf. Misgeld
et al., 1989
; Richter et al., 1996
). Details of the limitations for
this technique in motoneurons in vivo are in Lee and Heckman
(1998b)
.
Levels of neuromodulatory input. The experimental design
consisted of comparing three samples of cells obtained in three
different experimental preparations, each with a different level of
neuromodulatory drive. Within-cell analyses were not performed because
the agents used to alter the neuromodulatory state (the noradrenergic
1 agonist methoxamine and the anesthetic
pentobarbital) were found in preliminary experiments to be slow acting
and to produce small transient changes in blood pressure that
destabilized intracellular recordings. The standard
neuromodulatory state was defined as that existing in the decerebrate
cat preparation, which has tonic activity in axons descending from the
brainstem and releasing either 5-HT or NE (Jankowska, 1992
; Lee and
Heckman, 1998b
). IPIC is of moderate
amplitude in this preparation (Lee and Heckman, 1999a
). Administration
of the noradrenergic
1 agonist methoxamine to
the decerebrate preparation markedly increases the amplitude of
IPIC (Lee and Heckman, 1999a
). Thus,
we considered motoneurons in the decerebrate preparation with
methoxamine to be in an enhanced neuromodulatory state as
compared with the standard state for cells in the decerebrate without
methoxamine. A minimal neuromodulatory state was defined by
motoneurons from pentobarbital-anesthetized preparations, in which
IPIC is small or nonexistent (Schwindt and Crill, 1980
). In addition, a few motoneurons were recorded in fully
spinalized decerebrate preparations to assess whether the amplification
of synaptic input required descending input.
Synaptic input. Selective activation of muscle spindle Ia
afferents provided an excitatory synaptic input that was primarily monosynaptic (Heckman and Binder, 1988
) and widely distributed on
motoneuron dendrites (Burke et al., 1979
). It is likely that the Ia
input is primarily ionotropic, but this has not been decisively established (see Discussion). Additionally, the Ia input is modest in
amplitude, contributing perhaps 5% of the total excitatory input to
motoneurons (see Discussion), and in the adult cat, the Ia input is not
mediated by NMDA receptors (Brownstone et al., 1994
; Walmsley and
Bolton, 1994
; Miller et al., 1997
).
Selective activation of the Ia input was achieved by high-frequency,
low-amplitude sinusoidal vibration (180 Hz; 80 µm peak-to-peak) of
the combined MG and LGS tendons. The Ia synaptic current generated by
the tendon vibration remained remarkably constant for up to 10 sec
(Fig. 1).

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Figure 1.
The monosynaptic input from muscle spindle Ia
afferents generates prolonged and steady synaptic currents. Vibration
was applied for 10 sec while the cell was clamped at 60 mV.
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|
Protocols and analysis. In each cell, regardless of the
preparation, the standard protocol began with measurement of a spike antidromically evoked by single shocks to either the MG or LGS nerves.
The cell was tested for bistable behavior by applying a steady injected
current in bridge balance mode to bring the cell near threshold for
rhythmic firing. The bias level was monitored for 5-10 sec to verify
that synaptic noise did not generate any spikes. A 1.5 sec period of
vibration that evoked Ia input was applied on this bias, and bistable
behavior, if present, was manifest as self-sustained firing that
continued after the vibration ceased. We then switched to voltage-clamp
mode and applied a slow (6-8 mV/sec) ramp-shaped voltage command to
define the current-voltage (I-V) relationship of
the cell. We have shown previously that this slow rate of change of
voltage provides a good estimate of the cell's steady-state
I-V function (Lee and Heckman, 1998b
). The same ramp
voltage command was then repeated during a steady background of Ia
input. The vibration began 1 sec before the ramp to make sure that Ia
input reached its steady-state level (see Fig. 1). The onset of the
total IPIC was measured at the
point of zero slope at the beginning of the negative slope region of the I-V function (see Fig. 2A). The peak
amplitude of IPIC was measured as the
vertical distance from the peak downward deflection on the
I-V function to a line extrapolated from the
subthreshold region to define the leak current. The primary analysis of
the effect of Ia synaptic input on voltage-sensitive dendritic
conductances was based on the current generated by the voltage ramps
with and without the steady background of tendon vibration (see
Results). Statistical analyses consisted of comparisons of sample
averages using t tests and linear regression analyses to
assess the relationships between variables. The significance level
was set at p = 0.05. When multiple t tests
were performed, 0.05 was divided by the number of t tests.
 |
RESULTS |
Motoneurons were investigated under three preparations with
different levels of neuromodulatory drive (see Materials and Methods): enhanced (decerebrate plus a noradrenergic agonist; n = 14), standard (decerebrate with no drug; n = 12), and
minimal (pentobarbital anesthetized; n = 11). In
motoneurons in the standard state, application of a slow voltage ramp
reveals an I-V function with a region of negative
slope, caused by a persistent inward current,
IPIC (see Fig.
2A, top
trace). The applied ramp was slow enough to approximate steady-state conditions (Lee and Heckman, 1998b
).

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Figure 2.
Measurement of the effect of active dendritic
conductances on Ia synaptic input. The motoneuron illustrated is in the
standard neuromodulatory state (see Materials and Methods).
A, Top trace, The relationship between
current and voltage generated by the use of single-electrode voltage
clamp to apply a linearly rising voltage command that was slow enough
to approximate steady-state conditions (Lee and Heckman, 1998b ). The
onset of IPIC is evident as the start of a
negative slope region. Bottom trace, The effect of
applying a steady background of synaptic input from muscle spindle Ia
afferents throughout the duration of the voltage ramp. Note the shift
in onset of IPIC. B,
Subtraction of the current in the bottom trace in
A from that in the top trace revealing
the effective synaptic current generated at the soma by the Ia input
(Ia IN) as a function of voltage. In a
passive neuron, Ia IN would have declined
with voltage. Instead, Ia IN underwent
strong amplification because of dendritic voltage-dependent
conductances.
|
|
Assessment of dendritic amplification of synaptic input
To identify the influence of the Ia input on active dendritic
currents, we relied on the well known lack of control of dendritic regions during voltage clamp applied to the soma of a neuron (Rall and
Segev, 1985
). This poor space clamp allows synaptic currents, most of
which enter the cell via the dendrites, to alter the state of active
dendritic conductances while the voltage clamp holds constant the
behavior of somatic active conductances (Schwindt and Crill, 1995
; Lee
and Heckman, 1996
). If IPIC were
generated solely in the portion of the cell under good clamp control,
addition of a steady background of Ia synaptic input during the voltage ramp would simply shift the I-V function downward along the
current axis and slightly increase its overall slope. Instead, as
illustrated by the cell in the standard state in Figure
2A, bottom trace, the Ia input altered the
activation of voltage-sensitive dendritic currents and thus markedly
lowered the onset voltage of IPIC. The
difference between the top and bottom traces in
Figure 2A (which is shown in Fig.
2B) defines the total current generated at the soma
of the cell by the Ia input, including the contribution of active
dendritic currents. We refer to this total current as the Ia effective
synaptic current (Ia IN) (Binder et al.,
1996
). At hyperpolarized levels (
70 mV), Ia
IN was ~3.5 nA, but this increased to
over 11 nA as the cell was depolarized to approximately
42 mV. Thus,
active dendritic currents caused the Ia synaptic input to undergo a
strong, voltage-dependent amplification. Further depolarization
resulted in a sharp reduction in the magnitude of Ia
IN. Note also that the curvature of the
I-V function is increased in the presence of the Ia input
(Fig. 2A, bottom trace), resulting in a
gradual increase to the peak of amplification (Fig. 2B). This may reflect gradual activation of the
dendritic component of IPIC. This
pattern of a gradual increase to strong amplification followed by a
clear reduction was typical of all cells in the standard and enhanced
states (see below).
Control of amplification by neuromodulatory drive
Amplification of the Ia synaptic input was readily modified by the
strength of the neuromodulatory drive to the motoneurons. Ia
IN is plotted as a function of voltage for
motoneurons in the three different neuromodulatory states in Figure
3. Both high- and low-input conductance
cells are shown for each state, because spinal motoneurons exhibit
systematic differences in their electrical properties that correlate to
differences in the mechanical properties of the muscle fibers they
innervate (Binder et al., 1996
) (see Discussion). In the enhanced
neuromodulatory state (Fig. 3A), the peak Ia
IN at depolarized levels was especially
large. Further depolarization resulted in a precipitous decline that
caused Ia IN to fall to zero. This
suppression of Ia IN occurred well before the reversal potential of 0 mV for the Ia synapses and probably was
caused by activation of outward voltage-sensitive dendritic currents
(cf. Clements et al., 1986
; Hounsgaard and Kiehn, 1993
; Powers and
Binder, 2000
). Note also that the amplification and suppression
occurred at substantially more depolarized levels in the high-input
conductance cell. In the standard state (Fig. 3B), the same
amplification and suppression were still evident, but both were less
dramatic. Furthermore, the differences in voltage range for low- versus
high-input conductance cells remained well defined.

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Figure 3.
Changing neuromodulatory drive changed the
amplification of Ia synaptic input. Each panel of the
figure shows the changes in Ia IN as a
function of voltage in two cells, one with low input conductance
(thick line; Lo Gn) and one with high
input conductance (thin line; Hi Gn). See Materials and
Methods for techniques used to alter the neuromodulatory state of the
cells. A, Amplification is highest in the enhanced
neuromodulatory state. B, Amplification in the standard
state is shown. C, Amplification is reduced or absent in
the minimal state.
|
|
In the minimal state (Fig. 3C), the low-input conductance
cell exhibited some amplification, but at a much more depolarized level
than that for the low-input conductance cells in the enhanced and
standard states. In some low-input conductance cells in the minimal
state, the peak of amplification was not reached within the voltage
range we could successfully clamp (data not shown). In contrast, most
high-input conductance cells exhibited only voltage-dependent
suppression of Ia IN. In the example in
Figure 3C, Ia IN steadily
declined to become negative at approximately
37 mV, which, like the
suppression after amplification in Figure 3, A and
B, presumably occurred because of activation of outward dendritic currents.
Six cells were examined in decerebrate preparations with full
transections of the thoracic cord. Voltage-dependent amplification was
not apparent in any of these six cells, regardless of whether they had
high (n = 4) or low (n = 2) input
conductances. Thus, like bistability (Hounsgaard et al., 1988
),
amplification of Ia input is probably dependent on neuromodulatory
drive with a supraspinal origin.
Figure 4 shows the peak values of Ia
IN for each cell plotted as a function of
input conductance (in cells in the minimal state that lacked a clear
maximum in Ia IN, such as the one
illustrated by the thin line in Fig. 3C, the peak
value was defined as the average value of Ia
IN between
50 and
40 mV). The data for
all three levels of neuromodulatory drive are illustrated, as indicated by the symbols in the legend. In the minimal
state, Ia IN tended to decrease with input
conductance (cf. Heckman and Binder, 1988
), but this relationship was
not significant. In contrast, Ia IN tended
to increase with input conductance in both the standard and enhanced
states, but only the relation for the standard state was significant
(r = 0.75; p < 0.01). The reason for
the increase in amplification with input conductance is uncertain, but
the most striking aspect of this figure is the existence of large overall increases in amplitude of Ia IN in
the standard and enhanced states as compared with the minimal state.
There was some overlap in the range of values for the standard state
with those of the enhanced and minimal states. However, this overlap
was not caused by interexperiment variability because the overlapping
points were not all from the same experiment. Thus, in experiments in which three or more cells were included, the average within-experiment values for the minimal and enhanced states fell outside the range of
values for the standard state.

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Figure 4.
Peak Ia IN plotted as a
function of input conductance for each cell in each neuromodulatory
state (see legend symbols). Only the cells in the
control state (Standard) exhibited a statistically
significant relation between the two parameters (dashed line;
r = 0.75; p < 0.01). There were
however large differences in the values of peak Ia
IN across the different states.
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|
The average values for each neuromodulatory state are shown in Figure
5. The peak Ia
IN in the standard state (11.9 ± 2.4 nA) was approximately fourfold greater than that in the minimal state
(3.1 ± 3.0 nA), whereas in the enhanced state the increase was
approximately sixfold (17.0 ± 2.7 nA). All three averages were
significantly different (minimal vs both standard and enhanced, p < 0.00001; standard vs enhanced, p < 0.001). Thus, neuromodulatory state had an enormous impact on the
peak amplitude of Ia IN.

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Figure 5.
Comparison of peak Ia
IN, which occurs at depolarized levels
(typically 50 to 40 mV), with the Ia IN
recorded at hyperpolarized levels ( 65 to 75 mV). Averages and SDs
are given for the cells in each of the three neuromodulatory states
listed on the x-axis. The hyperpolarized Ia
IN reflected the influence of Ia input with
reduced activation of voltage-sensitive dendritic conductances. Thus
the difference between peak and hyperpolarized points, which increases
as neuromodulatory drive increases, gives an estimation of the
influence of active dendritic currents. See Results for statistical
comparisons.
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Magnitude of active dendritic currents
The depolarization-induced amplification of Ia
IN illustrated in Figures 2 and 3 was
caused by activation of the component of
IPIC in poorly clamped, presumably
dendritic, regions of the cell. To quantify the depolarization-induced
changes attributable to dendritic conductances, we compared the
amplitude of the Ia IN measured at the
most hyperpolarized level in each cell (typically
65 to
75 mV) with
the peak amplitude recorded at more depolarized levels. We assumed that
strong hyperpolarization at the soma would spread to the dendrites
sufficiently to reduce markedly the activation of the dendritic
component of IPIC by the Ia input (cf.
Schwindt and Crill, 1995
; Lee and Heckman, 1996
).
In the minimal state, peak Ia IN was, on
average, approximately the same as the hyperpolarized Ia
IN, with modest amplification in some
cells being counterbalanced by voltage-dependent suppression in other
cells. In cells in the standard state, the difference between peak and
hyperpolarized Ia IN was 7.8 ± 2.1 nA, whereas in the enhanced state, this difference was 12.2 ± 2.6 nA. Both values were significantly different from zero
(p < 0.00001). Because of these differences,
the peak Ia IN was ~3.2 times as large
as the hyperpolarized Ia IN in the
standard state and 3.5 times as large in the enhanced state.
However, Figure 5 also reveals a modest increase in the hyperpolarized
Ia IN with increasing neuromodulatory
drive (minimal, 2.8 ± 0.8 nA; standard, 4.0 ± 1.3 nA; and
enhanced, 4.8 ± 1.6 nA; only the difference between the minimal
and enhanced state was significant, p < 0.001). This
increase was unlikely to be caused by an excitatory effect of the
monoamines on Ia afferents via
motoneurons, because the preparation
was paralyzed. Presynaptic actions of monoamines on muscle afferents
are inhibitory and in any case appear to be absent on group I muscle
afferents (Bras et al., 1990
; Riddell et al., 1993
). Thus, the increase
probably occurred because the hyperpolarization was insufficient to
prevent the Ia synaptic input from partially activating the dendrites in the standard and enhanced states. This suggests that amplification of Ia IN by dendritic currents is slightly
larger than the estimates given above. Note also that the dendritic
currents achieved their strong amplification despite reductions in
synaptic driving force, which might have been quite large in dendritic regions.
It is interesting to note that the difference between peak Ia
IN and the hyperpolarized Ia
IN (i.e., the contribution from active
dendrites) is ~70% of the peak value of
IPIC as measured from the
I-V functions in both the standard and enhanced states (peak value for IPIC in the standard
state, 12.2 ± 6.4 nA; enhanced state, 18.4 ± 5.1 nA). The
reason that the amplification of Ia input was usually smaller than
IPIC may be that the synaptic input also activated voltage-sensitive outward currents in addition to
IPIC. However, in a few cells,
including the one shown in Figure 2, the contribution from active
dendrites was in fact larger than IPIC. Thus the balance of outward and
inward dendritic currents may well vary from cell to cell. These
results support previous work indicating that most of
IPIC is generated in dendritic
regions. Overall, it is clear that voltage-dependent amplification
attributable to dendritic voltage-sensitive currents greatly increased
Ia IN in both the standard and enhanced
neuromodulatory states.
Voltage range for amplification
In all cells, the peak amplification of Ia
IN occurred within the voltage range
traversed during the interspike intervals of rhythmic firing in
unclamped conditions in motoneurons (Schwindt and Crill, 1982
). Figure
6 shows the voltage at the peak Ia
IN plotted against input conductance for
both the standard and enhanced state cells (this analysis could not be
done for the minimal state as many cells lacked a clear peak). The
peaks for low-input conductance cells were close to the threshold for
spike initiation [typically approximately
50 mV (Lee and Heckman,
1998b
)], whereas those for high-input conductance cells were more
depolarized but still did not exceed the voltage range traversed during
higher rates of rhythmic firing. The relationship between voltage level
for peak amplification and input conductance was significant for both the enhanced and standard states, but the slightly increased slope for
the enhanced state was not significantly steeper than that for the
standard state. Thus, methoxamine mainly increased the potency of the
amplification without altering its voltage range, which is consistent
with our previous work showing that methoxamine did not alter the
voltage range for activation of IPIC
(Lee and Heckman, 1998b
).

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Figure 6.
The voltage for peak amplification of Ia synaptic
input varied systematically with the input conductance of the
motoneuron. In the sample of cells in the standard neuromodulatory
state, there was a statistically significant trend for amplification to
occur at more depolarized levels in high-input conductance cells
(r = 0.71; n = 12;
p < 0.05; slope, 8.15; intercept, 55.02). A
similar relationship was observed in the sample of cells in the
enhanced neuromodulatory state (r = 0.78;
n = 14; p < 0.01; slope,
11.54; intercept, 54.59). The difference between the slopes for the
standard and enhanced states was not significant
(p > 0.05, t tests for
slopes).
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Consistency of synaptic amplification
Only 3 of the 14 cells in the enhanced neuromodulatory state
exhibited strong bistable behavior. As in our previous study, these 3 cells had low input conductances (Lee and Heckman, 1998a
). None of the
12 cells in the standard state was bistable, which is again consistent
with our previous work (Lee and Heckman, 1999a
). However, every cell in
both the enhanced and standard states exhibited strong amplification of
Ia synaptic input. Thus, amplification of synaptic input may play a
wider role in normal motor outflow than bistable behavior.
Firing rates evoked by Ia synaptic input
We also measured the firing rate evoked during the Ia input in the
test for bistable firing. As expected from the strong amplification of
Ia IN seen in every cell in the standard
and enhanced states, Ia-evoked firing rates in all cells in these
states were remarkably high. In the standard state, the firing rate
averaged 31 ± 11 Hz, whereas in the enhanced state the average
was even higher at 60 ± 15 Hz. These rates are entirely
consistent with our previous work (Lee and Heckman, 1998a
).
 |
DISCUSSION |
The results shown here indicate that potent amplification of
maintained synaptic input can occur in the dendrites of motoneurons and
that this amplification scales with the level of neuromodulatory drive.
Previous studies have shown that the transient Ia EPSP evoked by a
single electrical shock does not undergo significant amplification with
depolarization in the decerebrate preparation (Brownstone et al.,
1994
). Polysynaptic transient inputs do undergo amplification, but
unlike the Ia input, these inputs are probably mediated by NMDA
receptors (Brownstone et al., 1994
). Transient inputs may be
insufficient to activate IPIC, which
appears to require a more sustained input for activation (Hounsgaard
and Kiehn, 1989
; Bennett et al., 1998b
; Lee and Heckman, 1998b
).
Voltage-dependent synaptic amplification has been observed previously
in response to sustained EPSPs from muscle stretch (Bennett et al.,
1998a
) and tendon vibration (Powers and Binder 2000
), followed by
suppression at more depolarized levels. However, in the present study,
the use of voltage clamp has allowed us to show that voltage-sensitive currents in the dendrites play a major role in generating this amplification and suppression of sustained inputs and that this dendritic amplification scaled with neuromodulatory drive.
Several roles for the effect of dendritic voltage-sensitive
conductances on synaptic integration have been advanced (Stuart and Sakmann, 1994
; Schwindt and Crill, 1997
; Cook and Johnston, 1999
;
Magee, 1999
). However, three aspects of our results suggest that
unusually large dendritic voltage-sensitive currents in motoneurons do
not just modify synaptic current but instead completely transform synaptic integration in these cells.
(1) Relatively small synaptic inputs were very effective in
activating the dendritic component of
IPIC. The Ia input constitutes perhaps
5% of the total excitatory synaptic input to spinal motoneurons [the
total number of excitatory synapses on spinal motoneurons in the cat is
~17,000-50,000 (Ornung et al., 1998
); the total number of Ia
synapses from MG and LGS spindles is ~1000 (estimated from Burke et
al., 1979
)]. Nonetheless, the dendritic voltage-sensitive currents
activated by the Ia input were large in comparison with the total
persistent inward current in motoneurons (i.e., the current added to Ia
IN by depolarization-induced amplification was 60-70% of IPIC).
(2) The peak Ia IN was several times
larger than the Ia IN at the most
hyperpolarized levels. Thus, the current generated by dendritic
voltage-sensitive conductances was several times larger than the
current generated by the Ia synaptic input on its own.
(3) The amplified Ia IN generated very
high firing rates. In the minimal state, Ia
IN is only large enough to increase
motoneuron rates by 5-8 Hz (Powers and Binder, 1995
). In contrast,
firing rates to Ia input reached >30 Hz in the standard state and >50 Hz in the enhanced state. These rates are compared with those required
for maximum force generation in the next section.
Differences in synaptic integration between low- and high-input
conductance motoneurons
Slow-twitch (type S) muscle fibers require firing rates of 20-30
Hz to reach their maximum force (Binder et al., 1996
). The current
required to bring type S motoneurons to threshold in the standard and
enhanced states is small because the monoamines also produce
significant steady depolarization (Binder et al., 1996
; Lee and
Heckman, 1998a
). Therefore the firing rates during Ia input in
low-input conductance cells usually required no bias current or, in the
enhanced state, a negative bias because the cell fired tonically in the
resting state (Lee and Heckman, 1998a
). Thus, a single synaptic input
system becomes capable of driving type S motoneurons to their maximum
functional firing rates (standard state) or beyond (enhanced state).
Therefore, it appears that type S motoneurons in both the standard and
enhanced states have a unique form of synaptic integration. Ionotropic
synaptic inputs are primarily relieved of the burden of supplying
sufficient current to drive rhythmic firing. Instead, these inputs
activate a highly excitable dendritic tree, which is then the primary
source of current to generate firing. This new form of synaptic
integration stands in sharp contrast to the classical picture for
motoneurons, which was developed from studies in the minimal state and
postulated that simultaneous activation of many synaptic inputs was
required to achieve high firing rates (Binder et al., 1996
).
High-input conductance motoneurons tend to innervate fast-twitch (type
F) muscle fibers. Because of their higher input conductances, type F
motoneurons are recruited after type S motoneurons
this is Henneman's
size principle (Henneman and Mendell, 1981
; Binder et al., 1996
). Type
F fibers require much higher rates than do S fibers to reach maximum,
often 70 Hz or more (Binder et al., 1996
). Furthermore, although
voltage thresholds for spike initiation are similar in all motoneurons
(Pinter et al., 1983
; Lee and Heckman, 1998b
), the higher input
conductance of the type F cells means that they require much more
current to reach threshold, as much as 10-20 nA compared with 3 nA or
less in type S cells in the standard state (Lee and Heckman, 1998a
). In
addition, in high-input conductance cells, amplification is shifted to
a more depolarized level than in S cells (Fig. 4). These considerations
suggest that the type F motoneurons with the highest input conductances
have a broad subthreshold and near-threshold range in which the
integration of multiple inputs is necessary to produce strong firing.
Overall these systematic differences in synaptic integration in types S
and F motoneurons further emphasize the importance of Henneman's size
principle (Henneman and Mendell, 1981
; Binder et al., 1996
) in
understanding motor outflow.
Neuromodulatory control of amplification in motoneurons
The large differences between synaptic amplification in the
different neuromodulatory states could provide descending motor commands with the capacity to adjust amplification of ionotropic inputs
for different motor tasks (cf. Svirskis and Hounsgaard, 1998
). The Ia
input does appear to be ionotropic (Binder et al., 1996
), but we cannot
exclude the possibility that it activates some metabotropic glutamate
receptors or that Ia afferents colocalize neuromodulatory transmitters.
However, amplification was not present in the spinalized state, so that
any neuromodulatory actions of Ia afferents on their own must be
ineffective without descending monoaminergic input. Thus, the
descending monoaminergic input can potentially be used to control
amplification in motoneurons during normal motor behaviors. For
example, one might expect that highly precise tasks might benefit from
reduced amplification to avoid overemphasis of small errors in the
descending commands. Tasks requiring moderate force like posture might
have moderate amplification, whereas tasks requiring high forces might
require as much amplification as possible.
Limitations and further studies
In the simple combination of voltage-clamp and synaptic input used
in this study, a full range description of the influence of dendritic
voltage-sensitive currents on synaptic integration was achieved with a
compact protocol. This technique makes efficient use of what was
considered previously a serious limitation of voltage-clamp methods in
neurons, namely, the lack of space clamp in dendritic regions. However,
there is a clear limitation with this method, which is the uncertainty
regarding what portion of the cell was under good clamp control. The
finding that amplification of Ia IN was
large relative to the total IPIC
suggests that the controlled portion was rather small, perhaps not even
including the proximal dendrites. Nor is it clear to what degree the
monoamines actually increase the amplitude of persistent inward
currents in the dendrites as compared with decreasing outward currents. Blocking K+ currents with intracellularly
injected agents increases the amplitude of both transient and sustained
Ia EPSPs (Clements et al., 1986
; Powers and Binder, 2000
). One
possibility may be that reduction of a proximally located outward
current markedly facilitates transfer of current to the soma. However,
a localized proximal reduction does not appear to be consistent with
the lack of effect of methoxamine on both the voltage for peak
amplification (Fig. 6) and the voltage for onset of
IPIC (Lee and Heckman, 1998b
), because
improved current transfer should aid the somatically applied clamp
currents in depolarizing the dendrites. Perhaps a distributed reduction
of outward currents allows the persistent inward current to dominate the dendrites. These issues require further study with in
vitro preparations and computer simulations (cf. Booth et al.,
1997
).
There are however many additional questions that need to be pursued
in vivo. The time course of amplification may be important, because IPIC tends to decay slowly in
type F but not in type S cells (Lee and Heckman, 1998b
). Closely linked
to the question of whether synaptic amplification is gradable is the
question of how amplification impacts the summation of several
different synaptic inputs. Preliminary data indicate in fact that
summation of amplified inputs is linear (Prather et al., 1998
). Further work is needed on inputs mediated by metabotropic or NMDA glutamate receptors and, especially, on inhibitory inputs. The complex interplay among various inputs should allow descending motor commands ample scope
for controlling the potent amplification of synaptic inputs mediated by
voltage-sensitive conductances in the dendrites of motoneurons.
 |
FOOTNOTES |
Received May 2, 2000; revised June 13, 2000; accepted June 23, 2000.
This work was supported by National Institutes of Health Grants NS
34382 and NS 28076.
Correspondence should be addressed to Dr. C. J. Heckman,
Department of Physiology M211, Northwestern University Medical School, 303 East Chicago Avenue, Chicago, IL 60611. E-mail: c-heckman{at}nwu.edu.
 |
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