State-dependent hyperpolarization of voltage threshold enhances motoneurone excitability during fictive locomotion in the cat
Article first published online: 5 AUG 2004
The Journal of Physiology
Volume 532, Issue 1, pages 271–281, April 2001
How to Cite
Krawitz, S., Fedirchuk, B., Dai, Y., Jordan, L. M. and McCrea, D. A. (2001), State-dependent hyperpolarization of voltage threshold enhances motoneurone excitability during fictive locomotion in the cat. The Journal of Physiology, 532: 271–281. doi: 10.1111/j.1469-7793.2001.0271g.x
- Issue published online: 5 AUG 2004
- Article first published online: 5 AUG 2004
- (Received 17 April 2000; accepted after revision 22 November 2000)
- 1Experiments were conducted on decerebrate adult cats to examine the effect of brainstem-evoked fictive locomotion on the threshold voltage (Vth) at which action potentials were initiated in hindlimb motoneurones. Measurements of the voltage threshold of the first spike evoked by intracellular injection of depolarizing ramp currents or square pulses were compared during control and fictive locomotor conditions. The sample of motoneurones included flexor and extensor motoneurones, and motoneurones with low and high rheobase currents.
- 2In all 38 motoneurones examined, action potentials were initiated at more hyperpolarized membrane potentials during fictive locomotion than in control conditions (mean hyperpolarization -8.0 ± 5.5 mV; range -1.8 to -26.6 mV). Hyperpolarization of Vth occurred immediately at the onset of fictive locomotion and recovered in seconds (typically < 60 s) following the termination of locomotor activity.
- 3The Vth of spikes occurring spontaneously without intracellular current injection was also reduced during locomotion.
- 4Superimposition of rhythmic depolarizing current pulses on current ramps in the absence of locomotion did not lower Vth to the extent seen during fictive locomotion. We suggest that Vth hyperpolarization results from an as yet undetermined neuromodulatory process operating during locomotion and is not simply the result of the oscillations in membrane potential occurring during locomotion.The hyperpolarization of Vth for action potential initiation during locomotion is a state-dependent increase in motoneurone excitability. This Vth hyperpolarization may be a fundamental process in the generation of motoneurone activity during locomotion and perhaps other motor tasks.
Electrical stimulation of the brainstem in paralysed decerebrate cats evokes a centrally generated pattern of motor output (fictive locomotion) that has many of the characteristics of overground locomotion in adult quadripedal mammals (see Rossignol, 1996). During fictive locomotion, motoneurones innervating limb muscles receive alternating excitatory and inhibitory synaptic currents from the central pattern generator (CPG) for locomotion (Jordan, 1983). These result in the rhythmic fluctuations of membrane potential (locomotor drive potentials, LDPs) that underlie the patterned activation of motoneurones during locomotion. The transformation of rhythmic excitatory drive into trains of action potentials is governed by the passive and active membrane properties of motoneurones. It is now known that some of these properties are altered during locomotion. For example, the post-spike afterhyperpolarization (AHP) is reduced in motoneurones during fictive locomotion (Brownstone et al. 1992; Schmidt, 1994) and there is the appearance of a voltage-dependent excitatory current (Brownstone et al. 1994). This voltage-dependent excitation results in non-linear responses of motoneurones to depolarizing currents, which may facilitate the recruitment of motoneurones, or augment motoneuronal output evoked by reflex or central excitation (Brownstone et al. 1994; McCrea et al. 1997; Bennett et al. 1998). These changes in motoneurone membrane properties result in increased motoneuronal firing in response to intracellular current injection during fictive locomotion (Brownstone et al. 1992; Fedirchuk et al. 1998). The fictive locomotor state thus appears to include processes that increase the excitability of hindlimb motoneurones.
The membrane potential at which action potentials are initiated in response to sufficient depolarizing currents (the voltage threshold, Vth) is not a fixed value in motoneurones. For example, Vth tends to be higher (more depolarized) in higher rheobase motoneurones (Gustafsson & Pinter, 1984) and the Vth of action potentials occurring later in a train during repetitive firing increases (accommodation) (Kolmodin & Skoglund, 1958). The present study sought to determine whether the Vth of hindlimb motoneurones was altered during fictive locomotion. To this end Vth was measured in motoneurones recorded in decerebrate and paralysed adult cats during control conditions and during brainstem-evoked fictive locomotion. A comparison of the Vth threshold in each motoneurone during these two states revealed a locomotor-related decrease (i.e. hyperpolarization) in motoneuronal Vth during fictive locomotion. We suggest that Vth hyperpolarization is another means by which motoneurone properties are re-configured to enhance motoneuronal output in the locomotor state. Parts of these data have been presented in abstract form (Krawitz et al. 1997).
Data were obtained from six cats of either sex weighing 2.0-3.1 kg. All surgical and experimental protocols were in compliance with the guidelines set out by the Canadian Council on Animal Care and the University of Manitoba. Anaesthesia was induced and maintained with halothane (5 % and 0.8-1.8 %, respectively) delivered in an oxygen/nitrous oxide mixture (40 %/60 %). A surgical plane of anaesthesia was confirmed by continuous monitoring of the arterial blood pressure via a carotid artery cannula and by repeatedly testing for the lack of pedal withdrawal and corneal reflexes as well as muscle tone. A glucose sodium bicarbonate buffer (5 g glucose, 0.84 g NaHCO3 per 100 ml) was infused intravenously (5-10 ml h−1) throughout the experiment.
The peripheral nerves innervating the following muscles of the left hindlimb were dissected and cut: sartorius (Sart), the posterior biceps mounted with semitendinosus, semimembranosus-anterior biceps (SmAB), lateral gastrocnemius-soleus (LGS), medial gastrocnemius (MG), plantaris (Pl), flexor digitorum or hallucis longus (FDHL), the remaining mixed posterior tibial nerve (Tib) as it enters the foot, and tibialis anterior (TA). The common peroneal nerve could be stimulated to test for antidromic activation, and the nerve innervating the right anterior biceps was dissected to monitor extensor activity of the contralateral hindlimb. Remaining ipsilateral and contralateral branches of the femoral, sciatic and common peroneal nerves, and the tendons attached around the hip joint, were cut.
A dorsal laminectomy of the L4-L6 vertebrae exposed the lower lumbar spinal cord, and the animal was fixed in a stereotaxic recording frame. Mineral oil pools were fashioned for the spinal cord and both hindlimbs, and the dissected nerves were placed on conventional silver hook bipolar electrodes for stimulation or recording. A craniotomy was performed and a mechanical precollicular/postmammillary decerebration was completed. All tissue rostral to the plane of decerebration was removed rendering the animal totally insentient and allowing the anaesthetic to be discontinued. The animal was injected with the neuromuscular blocker Pavulon (pancuronium bromide; 1.2 mg, supplemented with 0.6 mg every 45 min) and artificially ventilated to maintain expired CO2 at 3-5 %. Decreases in blood pressure were countered by the intravenous administration of a blood volume expander (6 % Gentran 70). At the termination of the experiments, the animals were killed by the intravenous administration of potassium chloride.
Electrical stimulation (50-220 μA, 0.5 ms pulses at 15-27 Hz) of the mesencephalic locomotor region (MLR) was used to evoke rhythmic and alternating activity in hindlimb flexor and extensor motoneurones. Monopolar stimulating electrodes were placed bilaterally in the brainstem and their positions adjusted to optimize the production of fictive locomotion. Unilateral stimulation was usually sufficient to evoke locomotion but occasionally bilateral stimulation was required. Fictive locomotion was monitored from amplified, rectified and filtered records from peripheral nerves (electroneurograms, ENGs), which were displayed continuously.
Intracellular recordings from lumbar motoneurones were obtained using glass microelectrodes filled with 2 m potassium acetate solution (3-8 MΩ). The primary aim of this study was to compare the membrane potential at which action potentials were initiated (Vth) during control and locomotor conditions. Use of the discontinuous current clamp (DCC) mode of an Axoclamp-2A amplifier (Axon Instruments) permitted reliable measurements of membrane potential during injection of large intracellular currents. The ability of the electrode to pass the current without rectification was continuously assessed using a high speed, high gain oscilloscope trace of the electrode voltage (i.e. the unswitched ‘monitor’ output). Only data where comparisons between control and locomotor conditions were made using the same DCC switching rate are reported. The intracellular recording and a monitor of injected current were digitized (membrane potential at 10 kHz; monitor of injected current at 3.3 kHz), as well as rectified-integrated ENG and cord dorsum recordings (500 Hz and 5 kHz, respectively), and stored on a computer for subsequent analysis using software developed within our group (details at www.scrc.umanitoba.ca/doccc).
Immediately after impalement motoneurones were identified by antidromic activation from one of the peripheral nerves. For the 12 motoneurones not antidromically activated by any of the peripheral nerves available, the presumptive motoneurone was classified as flexor or extensor based on its pattern of activity during fictive locomotion. Hyperpolarizing 50 ms current pulses (typically 2 nA), were injected to determine the motoneuronal input resistance, although in four motoneurones input resistance was estimated from depolarizing current injections of < 5 nA. Rheobase was defined as the minimum amplitude of a depolarizing (50 ms duration) current pulse that evoked an action potential. In two cells rheobase was estimated using a slowly rising current ramp (see Table 1). The intracellular amplifier was then placed in DCC mode and the switching rate for current injection adjusted while monitoring electrode voltage. Under control conditions without MLR stimulation and fictive locomotion, injection of a triangular ramp or pulses of depolarizing current were used to initiate an action potential(s) in the motoneurone. Fictive locomotion was evoked later in the same trial, and the intracellular current injection was repeated (see Fig. 1A). The extracellular DC potential recorded immediately after withdrawing the microelectrode was measured and subtracted from the intracellular potential. Recordings in which the intracellular or extracellular DC values were suspected of drifting were discarded.
|Motoneurone (n= 38)||Rheobase (nA)||Rin (MΩ)||Vm control (mV)||Vth|
|Control (mV)||Locomotion (mV)||Difference (mV)|
|Mean =−8.0 S.D.= 5.5|
Voltage threshold measurement
Voltage threshold (Vth) was measured for the first spike elicited either from 50 ms depolarizing square pulses or, more commonly, from slow (5-15 s) triangular ramps of intracellularly injected depolarizing current (as in Fig. 1). Measurements are reported only for the first spike evoked to avoid the potential for previous spikes to influence Vth by either spike accommodation or inter-spike trajectory. In order to standardize measurements, Vth was defined as the membrane potential at which depolarization increased at ≈10 V s−1 (i.e. the initiation of the action potential; see Brownstone et al. 1992). At the 10 kHz sampling rate used, this Vth estimate corresponded to the voltage value of the first data point where the following data point was ≤ 1 mV depolarized. The Vth of each cell was measured in the same data file during control conditions (i.e. in the absence of brainstem stimulation) and brainstem-evoked fictive locomotion. Each cell thus served as its own control (see Fig. 1). In some cells, several ramps of current that varied in amplitude and/or duration were injected but comparisons between the individual Vth measurements during the locomotor and control states were usually made from identically shaped current injections (as in Fig. 1). In some cases a hyperpolarizing bias current was injected from which the depolarizing ramp was initiated. This procedure permitted measurement of the Vth of the first action potential during locomotion when locomotion-related firing would have interfered with the measurement (e.g. Fig. 5).
Locomotor-related changes in Vth were assessed in 38 motoneurones innervating a variety of hindlimb muscles and having action potential amplitudes in control conditions ranging from 50 to 97 mV (mean 76 mV; 36/38 had spikes of ≤ 65 mV; 22/38 had spikes of ≤ 75 mV). Control rheobase and input resistance values are reported in columns 2 and 3 of Table 1. The range of rheobases (2-31 nA) indicates that both motoneurones innervating slow twitch muscle fibres (low rheobase) and those innervating fast twitch muscle fibres were represented in the sample (see Burke, 1981). The 38 motoneurones examined included both flexors and extensors.
The principle aim of the study was to determine the minimum level of membrane depolarization required to evoke an action potential during control and locomotor conditions. Early experiments in this series revealed that the current required to evoke spikes during locomotion was often much less than that required during control conditions. Because of the unpredictability of the change in threshold current during locomotion, Vth measurements were most often made from slowly rising current ramps that began at levels well below threshold. A comparison of the Vth of motoneurone spikes elicited from pulse and ramp current injections was made during control (non-locomotor) conditions. In 9 of the 11 motoneurones examined, the Vth of the spike evoked by the current ramp was more depolarized than that obtained from the pulse; however, the mean values of Vth obtained by the two techniques were not statistically different (Student's paired t test, P = 0.08; Wilcoxon signed rank test, P = 0.07). All comparisons of Vth during locomotor and control conditions are from measurements made using the same technique.
Figure 1A shows an intracellular recording from a SmAB motoneurone in which two identical triangular-shaped current injections were delivered. Each went from 0 nA to +50 nA to 0 nA over an 18 s period. The first current injection was delivered in the absence of MLR stimulation and locomotion (control). It evoked an action potential as the current reached 36 nA (marked by a +; see expanded time scale in Fig. 1B). The Vth was -46.5 mV, as determined by the point at which the change in membrane potential was ≤ 10 V s−1. The second current injection was initiated about 25 s after the onset of electrical stimulation of the MLR (1 ms pulses, 26 Hz). MLR stimulation produced fictive locomotion with a characteristic rhythmic alternation between flexor (not illustrated) and extensor (SmAB illustrated) ENG activity. In this example the rhythmic locomotor-induced depolarizations (i.e. LDPs) were small and well below the amplitude required for recruitment. As can be seen on the expanded time scale of Fig. 1C, the current required to initiate an action potential (marked with a +) was reduced during fictive locomotion from the control value of 36 nA to 10 nA. During fictive locomotion the Vth was -55.2 mV, an 8.7 mV hyperpolarization compared to control. Note the increase in the motoneurone firing rate (from 29 to 59 Hz) during fictive locomotion at the same membrane potential (Fig. 1B and C).
Figure 2 shows a recording from another SmAB motoneurone where the Vth was -32.7 mV in the control (Fig. 2A1 and B1), and -42.2 mV during fictive locomotion (Fig. 2A2 and B2; i.e. hyperpolarized by 11.5 mV). Note that like the example in Fig. 1, during fictive locomotion less current was needed to evoke an action potential and the motoneurone fired faster (32 vs. 20 Hz) at comparable membrane potentials (see Fig. 2A1 and 2). A third ramp current injection delivered about 60 s after the cessation of fictive locomotion (Fig. 2A3) shows that the Vth had returned to -31.8 mV by this time.
The Vth of all 38 motoneurones examined during control and locomotor conditions is shown in Table 1. The right-most column shows that the Vth of all 38 hyperpolarized during locomotion (mean -8.0 ± 5.5 mV; median -6.7 mV). Hyperpolarization of Vth was not accompanied by a consistent change in the spike overshoot (see Fig. 1) or obvious changes in spike duration (not illustrated). This hyperpolarization of Vth was striking both in its incidence (i.e. occurrence in all cells examined) and in the wide range of threshold changes seen during locomotion (-1.8 to -26.6 mV). At present we have no explanation for the differing degrees of threshold lowering in different motoneurones during locomotion. There was no correlation between motoneurone membrane potential recorded before fictive locomotion and Vth hyperpolarization during locomotion (linear regression coefficient r2= 0.01; Pearson product moment correlation, P = 0.5). The amount of threshold change was not a function of the particular experiment. In one experiment Vth hyperpolarization during fictive locomotion ranged from -1.8 to -19.1 mV in different motoneurones. Figure 3 plots the amount of change in Vth against motoneurone rheobase. There was no relationship between motoneurone rheobase and Vth hyperpolarization during fictive locomotion (linear regression coefficient r2= 0.01; Pearson product moment correlation, P = 0.6). Thus both high and low rheobase neurones displayed large and small changes in Vth during locomotion.
Recovery of Vth to within 1 mV of the control value was followed in seven motoneurones. Recovery occurred in three cells in < 30 s, and in 30-145 s in the remaining four cells (see Fig. 2). The use of long duration ramps (typically about 20 s) and the need to wait until all peripheral nerve activity ceased following MLR stimulation precluded an accurate assessment of the minimum time to Vth recovery. Nevertheless it is clear that in some cells Vth remained hyperpolarized in the period immediately following the bout of fictive locomotion and when rhythmic fluctuations of the membrane potential had ceased.
Figures 1 and 2 show a reduction in the amount of intracellular current needed to evoke an action potential during fictive locomotion compared to control. This increase in motoneurone excitability is, however, difficult to quantify since the depolarization produced by the locomotor circuitry (the depolarizing portion of the LDP) will add to the depolarization produced by current injection. Similarly, estimating changes in the minimum current required to evoke spikes during the hyperpolarizing portion of the LDP is complicated by both the hyperpolarization itself and the synaptic conductances that occur during the hyperpolarizing phase of locomotion. As a result, changes in rheobase current during locomotion are not reported.
Figure 4 illustrates an extensor motoneurone in which the LDPs were large enough to produce rhythmic activation during locomotion in the absence of intracellular current injection. In this cell the control Vth was -50 mV (not shown). During locomotion the membrane potential at which spikes were produced on the LDP was -53 mV; i.e. Vth became hyperpolarized by 3.0 mV. Current pulses of 4 nA, 50 ms duration were injected into this motoneurone at about 1 Hz with three of these pulse injections shown in the portion of data illustrated in Fig. 4. Since the delivery of current pulses was not synchronized with the fictive step cycle, these pulses occurred at random with respect to the rhythmic depolarization and hyperpolarization of the motoneurone. When these pulses occurred during the hyperpolarized portion of the step cycle it was possible to determine the Vth (see the spike produced by the third current pulse injection from the left). The Vth of this spike was -53 mV; the same as that produced by locomotor depolarization without current injection. A similar observation was made in one other cell. Despite the small sample size, these observations are important because they indicate that (1) Vth does not vary rhythmically with membrane potential fluctuations during locomotion and (2) Vth is reduced to the same extent for spikes produced by the locomotor circuitry and intracellular current injection. The examples in Fig. 1 and 2 show a lowering of Vth in two motoneurones with small LDPs that were not recruited during fictive locomotion without the addition of intracellular depolarizing current. Thus, the hyperpolarization of Vth in these cells during locomotion was not a consequence of motoneurone recruitment.
Vth hyperpolarization during locomotion is not the result of rhythmic changes in motoneurone membrane potential
Figure 4 shows that spikes occurring either spontaneously during locomotion or as a result of current injection do so at a hyperpolarized Vth. One of the features of locomotion is the rhythmic LDPs in motoneurones. To determine whether rhythmic depolarizations and hyperpolarizations reduce Vth in the absence of locomotion, current pulses were superimposed on top of current ramps during control conditions in eight motoneurones. Voltage thresholds were measured for action potentials produced by a current ramp alone (control), those produced by a ramp current with superimposed current pulses without locomotion, and for those occurring on the current ramp during fictive locomotion (as in Fig. 1 and 2). Figure 5 illustrates the data from one of these cells. The Vth of the first spike produced by ramp current injection alone was -48.2 mV (Fig. 5A1 and B1). Current pulses (10 nA, ≈300 ms) superimposed on the ramp depolarization resulted in ≈10 mV membrane potential oscillations (Fig. 5A2). The Vth of spikes evoked by the combination of ramp and pulse current injection was somewhat hyperpolarized (by 2.3 mV) compared to the spike evoked by ramp current injection alone (Fig. 5A2 and B2). During locomotion, this motoneurone displayed LDPs with about a 10 mV peak-to-peak amplitude (Fig. 5A3). Hyperpolarizing bias current was needed to prevent firing on the LDP during locomotion. During locomotion, the Vth of the first spike evoked on the current ramp was -57.9 mV (Fig. 5A3 and B3). This was a hyperpolarization of 9.7 mV compared to the spike evoked by ramp current during control and a hyperpolarization of 7.4 mV compared to the spike evoked by the combination of ramp and pulse current injection during control conditions. In all eight cells examined in this manner the hyperpolarization of Vth during locomotion (9.3 to 26.6 mV) was larger than that produced by the combination of pulse and ramp current injection during control conditions (1.9 to 11.4 mV). The mean Vth hyperpolarization during locomotion (14.3 ± 2.1 mV) was significantly larger than the Vth hyperpolarization for firing evoked by combining current pulses and ramps (4.7 ± 1.4 mV; paired t test, P = 0.013).
The use of hyperpolarizing bias current in some cells to prevent rhythmic action potential generation during locomotion is potentially a further complication in determining the extent to which Vth changes during locomotion. To address the extent of this possible complication, the amount of constant hyperpolarizing current preceding the ramp was varied in six cells in the absence of locomotion. In five cells, changing the hyperpolarizing bias current by 10-20 nA altered Vth by ≤ 2.2 mV. In one cell the change was 7.0 mV. In three of these six cells, Vth was increased (i.e. depolarized) by increases in hyperpolarizing bias current, in two cells Vth was hyperpolarized with increasing hyperpolarizing bias current, and one cell showed no change in Vth. Constant hyperpolarization of the motoneurone preceding the ramp therefore might have small effects on the measured Vth. Since this effect is small and often opposite to the hyperpolarization of Vth seen during fictive locomotion, it is unlikely to account for the locomotor-related Vth hyperpolarization that we have described. In some cases, it may have caused us to underestimate the amount of Vth hyperpolarization occurring during locomotion.
Further evidence that the hyperpolarization of Vth seen during fictive locomotion is not simply the result of rhythmic fluctuations in membrane potential is presented in Fig. 6. This MG motoneurone was recorded under three conditions. Figure 6A shows firing evoked by 15 nA, 250 ms current pulses in the absence of fictive locomotion. The Vth during this control condition was -31.0 mV. Fictive locomotion began soon after MLR stimulation commenced (Fig. 6B) but LDPs in this motoneurone were not well developed. The threshold of the spikes evoked by the CPG, without any intracellular current injection, was -37.1 mV (-6.1 mV compared to control). As is common in these preparations, fictive locomotion may change with constant MLR stimulation. After about 3 min prominent LDPs were evident in the motoneurone (Fig. 6C). Despite the clear increase in rhythmic drive to this motoneurone, the Vth for the LDP-evoked firing (-37.4 mV) was similar to that recorded in Fig. 6B. This example illustrates that the extent of threshold lowering in this motoneurone was not related to the size of the LDP. This observation and the prolonged recovery of Vth following locomotion suggest that Vth is associated with the locomotor state and not the rhythmic changes in motoneurone membrane potential per se.
This study demonstrates that action potentials in motoneurones are initiated at more negative membrane potentials during fictive locomotion than in the absence of locomotor activity. This locomotor-related hyperpolarization of Vth (i.e. lowering of Vth) occurred in all 38 motoneurones examined. These included flexors and extensors and motoneurones with either high or low rheobases (see Table 1). Because each motoneurone served as its own control, we could see that Vth hyperpolarization occurred immediately at the onset of, and recovered in seconds following, fictive locomotion. Threshold hyperpolarization occurred for spikes recruited during fictive locomotion in the absence of current injection (e.g. Fig. 4 and 6), as well for spikes evoked by injection of intracellular depolarizing current (e.g. Fig. 1 and 2). In addition, the Vth seemed not to be phasically modulated during the depolarizing and hyperpolarizing parts of the fictive step cycle, and the Vth hyperpolarization during locomotion was not dependent on the presence of well-developed LDPs. We suggest that Vth hyperpolarization is a ‘state-dependent’ phenomenon associated with the fictive locomotor process.
The present study is the first to demonstrate a reduction in motoneurone Vth during locomotion, but not the first report of modulation of neuronal Vth. For example, following a classical conditioning paradigm to decrease the amplitude of the H-reflex in monkeys, the mean Vth of spinal motoneurones became depolarized (Carp & Wolpaw, 1994). Mean motoneurone threshold potential is also depolarized in chronic spinal cats compared to spinal-intact animals (Hochman & McCrea, 1994). Cleary et al. (1998) have shown that the median Vth from their sample of motoneurone recordings in Aplysia was hyperpolarized the day following long-term sensitization of the siphon withdrawal reflex. Thus the hyperpolarization of Vth that we have observed during locomotion may reflect a general means of neuromodulatory control of neuronal excitability in a manner appropriate for a particular behavioural state. The present observations that Vth can change within seconds of the onset of brainstem stimulation and before the induction of repetitive firing in motoneurones as well as its recovery following locomotion are consistent with a mechanism that involves release of a neuromodulatory substance. The nature of this neuromodulator and whether spinal or supraspinal sources are involved remains to be determined. It also remains to be determined whether Vth hyperpolarization is a feature of other behaviours or whether different mechanisms contribute to threshold lowering in different species or under different conditions.
Many studies have noted the increase (depolarization) of voltage threshold that occurs during repetitive firing in cat motoneurones. Thus the Vth becomes more depolarized for successive action potentials of a spike train induced either by synaptic activation (Kolmodin & Skoglund, 1958) or by intracellular current injection (Granit et al. 1963; Barrett et al. 1980). This Vth depolarization may contribute to the decrease in firing rates seen during long trains of repetitive firing and is thought to be caused by accommodation of sodium channels (Schwindt & Crill, 1982). The locomotor-dependent hyperpolarization of Vth described here occurred for the first action potential evoked during fictive locomotion (see Fig. 1 and 2) and is, therefore, not a consequence of previous action potentials. This state-dependent hyperpolarization of Vth would tend to counter accommodation and the accompanying late adaptation during repetitive firing. The reduction of late adaptation during brainstem-evoked fictive locomotion (Krawitz et al. 1996) is consistent with this suggestion. It is also known that motoneurones have biophysical properties related to the type of muscle that they innervate (i.e. slow or fast twitch; see Burke, 1981). In non-locomoting preparations motoneurones innervating fast-type muscle are more likely to show accommodation to current ramps than those innervating slow twitch muscle (Burke & Nelson, 1971). In contrast, the locomotor-related Vth hyperpolarization is unrelated to motoneurone type, since large hyperpolarizations of Vth occurred in both low and high rheobase motoneurones (Fig. 3 and Table 1).
The hyperpolarization of Vth during fictive locomotion is not caused by oscillations of the motoneurone membrane potential underlying the LDPs. Vth hyperpolarization produced by superimposing square current pulses on top of current ramps in the absence of locomotion was always smaller than that occurring during locomotion. This is despite the fact that the current pulses caused an even more rapid change in the membrane potential trajectory than the LDPs. Furthermore, the Vth hyperpolarization could be large in the absence of substantial LDPs (see Fig. 6B) and persisted for seconds after fictive locomotion, when LDPs were absent. Therefore, while the motoneurone membrane potential trajectory during fictive locomotion might contribute to Vth hyperpolarization, our results suggest that Vth hyperpolarization is caused by a locomotor-dependent modulation of the threshold properties of motoneurones.
To our knowledge, the rapid modulation of Vth as a means of enhancing motoneuronal excitability during a motor task has not previously been described in any preparation. Its occurrence in every motoneurone examined indicates that Vth lowering, like AHP reduction and the release of voltage-dependent excitation (see Introduction) is another motoneurone membrane property that is regulated during locomotion. Interestingly, these changes in membrane properties would enhance motoneuronal excitability during locomotion and tend to counter the decrease in excitability that could result from the increase in motoneurone conductance that occurs during fictive locomotion (Shefchyk & Jordan, 1985; Gosgnach et al. 2000). The large reduction in the current required to evoke firing during locomotion (eg. Fig. 1 and 2) suggests that overall the excitability of motoneurones increases during fictive locomotion. This increased excitability would have large ramifications for motoneuronal recruitment and firing since less depolarization from either central or reflex pathways would be required to recruit any given motoneurone. Furthermore, because motoneurone firing properties are different during locomotion from those at rest, predictions of motoneurone firing during locomotion based on their firing properties in the non-locomoting state should be made with caution.
The present study did not examine the mechanism(s) underlying the hyperpolarization of motoneuronal Vth during fictive locomotion, nor the direct consequences on repetitive firing. In addition, we have no satisfactory explanation for the wide variation in the degree of Vth hyperpolarization seen in different motoneurones (see Table 1). Currently, both physiological studies and computer simulations are being utilized to examine how modulation of motoneuronal sodium and/or potassium conductances might contribute to this phenomenon (Dai et al. 1998a,b, 2000). In addition, a large scale simulation of spinal cord circuitry has been used to show that Vth hyperpolarization results in increased output of motoneurone pools in response to an excitatory synaptic input (Dai et al. 1999).
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The authors gratefully acknowledge the excellent technical assistance provided by Kim Madec, Maria Setterbom and Matt Ellis, and the participation of Dr Kelvin Jones in some of these experiments. S.K. was the recipient of a Medical Research Council (MRC) of Canada Studentship; B.F. thanks the Manitoba Division of the Canadian Paraplegic Association for salary support. This work was funded by a MRC of Canada program grant to L.M.J. and D.A.M.