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The Journal of Neurophysiology Vol. 85 No. 5 May 2001, pp. 2047-2062
Copyright ©2001 by the American Physiological Society
Laboratory of Neural Control, National Institute of Neurological Disorders and Stroke, National Institutes of Health, Bethesda, Maryland 20892-4455
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ABSTRACT |
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Li, Yan and
R. E. Burke.
Short-Term Synaptic Depression in the Neonatal Mouse Spinal Cord:
Effects of Calcium and Temperature.
J. Neurophysiol. 85: 2047-2062, 2001.
We have studied short-term
synaptic depression of excitatory postsynaptic potentials (EPSPs) in
lumbosacral motoneurons in the isolated, in vitro spinal cord of
neonatal mice at 2-4 days postnatal age. We used
2-amino-5-phosphonovaleric acid (AP5; 100 µM) to suppress spontaneous
and stimulus-evoked polysynaptic activity. Monosynaptic EPSPs were
generated by trains of 10 pulses stimuli delivered to a dorsal root at
eight frequencies between 0.125 and 16 Hz. The amplitudes of the second
(R2), third (R3), and the average of R8, R9, and R10 (tail) EPSPs,
normalized by the first EPSP (R1), defined the shapes of synaptic
depression curves. Tail responses were increasingly depressed as
stimulation frequency increased but R2 and R3 exhibited relative
facilitation at frequencies >1 Hz. Control experiments indicated that
the depression curves were not explained by presynaptic activation
failure. Lowering external Ca2+ concentration
([Ca2+]o) from 2.0 to 0.8 mM without changing
[Mg2+]o reduced average
R1 amplitudes and R2 depression with little change in tail depression.
Conversely, increasing
[Ca2+]o to 4.0 mM
increased average R1 amplitude and R2 depression but again did not
change tail depression. Increasing the bath temperature from 24 to
32°C produced little change in R1 amplitudes but markedly reduced the
depression of all responses at most frequencies. We developed an
empirical model, based on mechanisms described in more accessible
synaptic systems, that assumes: transmitter is released from a constant
fraction, f, of release-ready elements in two presynaptic
compartments (N and S) that are subsequently renewed by independent processes with exponential time constants (
N and
S); an
activation-dependent facilitation of transmitter release with constant
increment and fast exponential decay; and a more slowly decaying,
activation-dependent augmentation of the rate of renewal
(
N) of N. The model gave
satisfactory fits to data from all
[Ca2+]o conditions and
implied that f and the increments of the facilitation and
augmentation processes were all changed in the same direction as
[Ca2+]o, without changing
the time constants. In contrast, model fits to the 32°C data implied
that the process time constants all decreased by 40-45% while the
presumably Ca2+-related weighting factors were
unchanged. The model also successfully matched the normalized
amplitudes of EPSPs during trains with irregular intervals.
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INTRODUCTION |
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Since the classic work of
Liley and North (1953)
at the neuromuscular junction
(NMJ), the responses of synapses to repetitive stimulation has been
studied intensively because they provide clues to the basic mechanisms
that control transmitter release (Magleby 1987
;
Zucker 1989
, 1999
). There has been a great deal of
recent work on short-term depression and facilitation of synaptic transmission in mammalian central synapses, particularly using in vitro
techniques applied to junctions where the presynaptic elements are
accessible for direct electrical and/or optical recordings. A wealth of
data has become available from such studies that indicate the existence
of multiple mechanisms that can both depress and enhance synaptic
transmission (see reviews in MacDermott et al. 1999
;
Zucker 1989
, 1999
). These studies suggest ways in which transmission at less accessible synaptic systems can be examined.
Group Ia muscle spindle afferents make monosynaptic excitatory
connections to alpha motoneurons in the spinal cord, providing a
functionally defined synaptic system that has been used for decades as
a model system to study synaptic transmission in the mammalian CNS
(Burke and Rudomin 1977
; Eccles 1964
).
Mears and Frank (1997)
have shown that this system is
present in the neonatal mouse spinal cord. Using the isolated spinal
cord of neonatal rats in vitro, Lev-Tov and Pinco (Lev-Tov and
Pinco 1992
; Pinco and Lev-Tov 1993a
) have shown
that monosynaptic excitatory postsynaptic potentials (EPSPs) produced
by dorsal root stimulation in spinal motoneurons exhibit profound
synaptic depression at low frequencies. We have been interested in
studying the maturation of this synaptic system with postnatal age in
the mouse because of the growing importance of this animal for studies
of neurological mutants.
The present paper provides data on monosynaptic EPSPs in the neonatal
mouse spinal cord at 2-4 days of postnatal age (P2-P4) over a
stimulus frequency range within which the monosynaptic EPSPs display
relative facilitation as well as profound depression. We have examined
the effects of changes in extracellular Ca2+
concentration ([Ca2+]o)
and temperature on paired-pulse as well as steady-state depression, using short (10 pulse) trains at 0.125-8 Hz as well as EPSPs generated by irregular pulse patterns. These data have been compared with expectations from six empirical models of increasing complexity. The
model that best fit all of the observations suggests the co-existence of two separate mechanisms that enhance transmitter release,
superimposed on depression due to depletion of two independent,
presynaptic compartments. The models are described in some detail
because they are likely to be useful in codifying differences during
postnatal development. Preliminary results have appeared in abstract
form (Burke and Li 2000
; Li and Burke 1999
,
2000
).
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METHODS |
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Preparation
Experiments were performed on the isolated spinal cords of neonatal Swiss-Webster mice at 2-4 days postnatal (P2-P4). Animal care and use procedures were in accord with the "Principles of Laboratory Animal Care" (National Institutes of Health Publication 86-23) and were approved by the National Institute of Neurological Disorders and Stroke Committee on Animal Care and Use.
Neonatal mouse pups were anesthetized by inhalation of methoxyflourane (Metofane) in a small chamber and then quickly decapitated, eviscerated, and transferred into a dissection chamber circulated with cold (4°C) artificial cerebrospinal fluid (ACSF) bubbled with 95% O2-5% CO2. The composition of the normal ACSF was (in mM) 128 NaCl, 4 KCl, 2 CaCl2, 1 MgSO4, 1 NaH2PO4, 25 NaHCO3, and 30 glucose, bubbled with 95% O2-5% CO2 (pH 7.3). After ventral laminectomy, the spinal cord with intact dorsal (DR) and ventral roots (VR) was dissected free from DR ganglia. The dura and pia mater were removed carefully, and the spinal cord was hemisected longitudinally from T6 to the sacral segments with a tungsten needle. One hemicord was placed into a silicon elastomer (Sylgard)-based recording chamber that was continuously superfused with oxygenated ACSF flowing at 10-14 ml/min.
For testing the effects of low (0.8 mM) or high (4.0 mM) Ca2+ ACSF, only Ca2+ concentration was changed while Mg2+ remained constant at 1 mM. The temperature of bath solution was monitored with a thermistor and controlled by passing inflowing ACSF through a servo-controlled heater (TC-324B, Warner Instrument). The bathing solution was recirculated at all times except when drugs were added or washed out.
Dorsal and ventral rootlets of the L4 and
L5 segments were drawn into the polyethylene
suction electrodes for either stimulation or recording. Micropipettes
for intracellular recording were made from 1.2-mm filament glass (WPI)
drawn to produce DC electrode resistance between 40 and 90 M
(Sutter
Instruments Model P-87). Micropipettes were filled with 2 M K-acetate
and 100 mM QX-314 (Alamone Labs, Jerusalem, Israel) to suppress
Na+ action potentials (Frazier et al.
1970
). In some experiments, the electrode solution also
contained 2% biocytin to label the recorded cells. Motoneurons were
impaled from the lateral aspect of the hemisected cord and identified
by antidromic invasion after VR stimulation. In some experiments,
extracellular recordings in the ventral horn were obtained with
broken-tip electrode filled with 2 M NaCl (DC resistance, 5-7 M
).
Stimulation and recordings
Mono- and polysynaptic EPSPs were produced by stimulating a DR
filament with trains of 10 pulses (duration, 0.5 ms) at eight equally
spaced frequencies from 16 Hz down to 0.125 Hz (intervals of 0.0625, 0.125, 0.25, 0.5, 1.0, 2.0, 4.0, and 8.0 s). Trains were separated
by 2-min intervals (Fig. 1), which were
sufficiently long such that the first EPSPs in each train remained
constant, indicating full recovery of evoked synaptic release (see
Lev-Tov and Pinco 1992
). Changing the ordering of train
frequencies produced no changes in response patterns. Stimulus
amplitudes were adjusted to be just supramaximal for monosynaptic EPSPs
tested at 1 Hz.
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Spinal cord viability was shortened by high (>30°C) bath temperatures, so baseline observations were made at room temperature (23-24°C). Experiments to examine the effect of increased temperature (n = 18 cells) were done by transiently raising the bath temperature to 32°C only for periods of time needed for equilibration (~20 min) and to collect the required data (another 20 min). It proved to be difficult to maintain stable intracellular penetrations during temperature changes, but this was accomplished in some cases (n = 12; see Fig. 4C). The stability of DR-evoked reflexes and motoneuron population responses recorded from VRs served as indices of preparation viability. Most preparations remained stable for 8-12 h.
Data acquisition and measurements
Signals from suction electrodes on DRs and VRs were amplified with Cyberamp 380 amplifiers (Axon Instruments; band-pass 10-10 kHz). Intracellular potentials were amplified with an AXOCLAMP-2A (Axon Instruments) in current-clamp (bridge) mode. Intracellular signals were low-pass filtered at 10 kHz and digitized at 10 kHz (16-bit resolution) by a multichannel A/D converter (National Instruments NBIO-16). Custom-designed software (LabVIEW programming language; National Instruments, Austin, TX) was used to acquire and save the data in a Power Macintosh computer. Intracellular potentials and responses in VRs were also continuously recorded on a digital videotape record (VR-100 B, Instrutech, Great Neck, NY). Data analysis was done off-line using commercial software packages.
Electrotonic potentials generated by DR afferent volleys and recorded by a suction electrode on a DR filament immediately adjacent to the stimulated rootlet were monitored to ensure that the afferent volleys produced by each stimulus pulse in the train was constant (Fig. 3C, top). The amplitudes of monosynaptic EPSPs were measured before the inflections that signaled the onset of polysynaptic evoked PSPs (Fig. 3A, middle, arrows). Reflex responses in the VR (Fig. 3A, bottom) were rectified and integrated for analysis. These usually exhibited parallel changes with monosynaptic EPSPs but will not be considered further in this paper.
Pharmacological substances
Drugs were introduced into the ACSF bathing solution via a gravity-fed line (flow rate: 10-14 ml/min) to a recording chamber with total volume of 7.0 ml for minimum of 10 min before next tests were made, to allow equilibration. Drugs used were: (±)2-amino-5-phosphonovaleric acid (AP5), 6-cyano-7-nitroquinoxaline-2,3-dione disodium (CNQX), cyclothiazide (CTZ) obtained from RBI (Natick, MA), bicuculline methiodide and 2-hydroxysaclofen obtained from Sigma (St. Louis, MO), and EGTA-tetra(acetoxymethyl ester) (EGTA-AM) and BAPTA-tetra(acetoxymethyl ester) (BAPTA-AM) from Molecular Probes (Eugene, OR). AP-5 and CNQX disodium were prepared as stock solutions of 30 and 10 mM, respectively, in distilled water, stored at 4°C. Bicuculline and 2-hydroxysaclofen were freshly made in distilled water. CTZ was prepared as a 60 mM stock solution in methanol and frozen until use. EGTA-AM and BAPTA-AM were prepared as 100 and 10 mM stock solutions, respectively, in dimethyl sulfoxide. Solvent concentrations were <0.1% in the final ACSF.
Computer modeling
A variety of assumptions that might "explain" various aspects of the experimental observations formed the basis for equations that were embodied in spreadsheet programs (Microsoft Excel) that permitted comparisons between calculated and actual responses. The behavior of the response profiles with different parameter combinations were heuristically useful, but as the number of free parameters increased, it became impossible to fit the data by hand. Therefore a computer program was written in PASCAL (CodeWarrior, Metrowerks; Macintosh G3 computer) to determine the set of parameters that minimized the error between the calculated responses and experimental depression curves (e.g., Fig. 8). The organization of the program is discussed in the APPENDIX. Despite the large number of iterations, a complete parameter search with 105 iterations took <10 s on a G3 Macintosh computer. The source code is available on request.
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RESULTS |
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This description is based on observations in a total of 87 motoneurons recorded in the isolated, hemisected spinal cord of neonatal Swiss-Webster mice at postnatal ages of 2-4 days (P2-P4). Cells accepted for analysis had stable membrane potentials less than
50 mV for the 30 min period required for data collection (see
METHODS). Some cells had stable membrane potentials for 2 h.
Suppression of background activity
When recorded in normal ACSF at room temperature (23-24°C), the
isolated spinal cord of P2-P4 mice usually exhibited considerable spontaneous background activity with paroxysmal depolarizations in
motoneuron membrane potential and associated VR discharges. DR
stimulation was set at strengths slightly larger than required to
produce the largest intracellularly recorded EPSPs (e.g., Figs. 4A and 5A). These stimuli produced additional
long-lasting depolarizations superimposed on the falling phase of
monosynaptic EPSPs and often outlasted the stimulus trains (Fig.
1A). Preliminary experiments showed that addition of
mephenesin (1 mM) (see Lev-Tov and Pinco 1992
) largely
blocked this activity but also reduced monosynaptic EPSP amplitudes
(see also Seebach and Mendell 1996
;
Ziskind-Conhaim 1990
). However, the addition of the
N-methyl-D-aspartate (NMDA) receptor blocker AP5
(100 µM) to the ACSF eliminated the both spontaneous activity and
long-lasting stimulus-evoked polysynaptic depolarizations in almost all
preparations (Fig. 1B) (see also Pinco and Lev-Tov
1993a
). Accordingly, all of the synaptic depression data
discussed in the following text were obtained in the presence of 100 µM AP5. The peak amplitudes of the monosynaptic components were
reduced by an average of ~9% when studied in the same motoneurons before and after addition of AP5, irrespective of their amplitudes (Fig. 2). An additional advantage of
using AP5 is that it removes a potential source of nonlinear
amplification that could distort the peak amplitudes of large DR EPSPs.
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Latency of DR-evoked EPSPs in motoneurons
Figure 3 illustrates the
timing of DR afferent volleys as they entered the spinal cord
(top, DR) (see also Seebach and Mendell 1996
), and as they arrived in the ventral horn (VH) as a
"terminal potential" (middle, VH) (see Lev-Tov
and Pinco 1992
). In normal ACSF (2.0 mM
Ca2+; Fig. 3, A and C), the
averaged afferent volleys produced by 50 pulses at 1- and 8-s
inter-pulse intervals were superimposable, demonstrating that fiber
activation was reliable at both stimulus frequencies used (see also
Kudo and Yamada 1985
; Seebach and Mendell 1996
). On the other hand, the terminal potentials in the
ventral horn were different at the two frequencies, apparently because they were distorted by the onset of extracellular synaptic potentials at ~4 ms after the stimulus onset (Fig. 3, A and
C, VH) (see also Lev-Tov and Pinco 1992
).
Removing Ca2+ from the ACSF blocked the synaptic
field potentials, revealing that the terminal potentials were in fact
the same at 0.125 and 1 Hz (Fig. 3B). The records in Fig.
3C show the traces in Fig. 3A on an expanded time
base to emphasize that the VR record contains an electrotonically
conducted representation of the earliest EPSP in the motoneurons
(arrow) coincident with the terminal potential distortion (Fig.
3A).
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The latency changes in DR volleys and EPSP onsets in the same
motoneurons at room temperature and after raising bath temperature to
32°C are shown in Fig. 4. In the
example shown (Fig. 4A), increased temperature shortened the
delay of first reversal for the DR volley by ~0.6 ms but produced
even more dramatic shortening of the delay between the afferent volleys
and EPSP onsets (from 3.2 to 2.0 ms). The population data for EPSP
latencies measured from DR stimulus onset are given in the histogram in
Fig. 4B. All of these observations support the conclusion
that the earliest DR EPSPs are in fact monosynaptic (Mears and
Frank 1997
).
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Short-duration, low-frequency synaptic depression
The records in Fig. 5 illustrate an
example of the EPSP depression found in this work. Figure 5,
A-D, shows single sweep intracellular records of the first
(R1), second (R2), and the average of the final three EPSPs in the
sequence of 10 ("tail" response) during 10 pulse trains at 8 (A and B), 2 (C), and 0.125 Hz
(D). The R2 response data represent paired-pulse depression,
and the later tail responses provide an estimate of the steady-state
depression at a constant input frequency. Figure 5A,
inset, shows that the incoming afferent volleys recorded
from an adjacent DR were unchanged during the 8-Hz train; DR volleys in
the other trains were essentially identical (not shown). Figure
5B shows that the latency of R2 and tail responses were,
despite their appearance in A, the same as R1 after
adjusting them to match R1. The EPSP amplitudes were measured at the
time denoted by the vertical dashed line, prior to the inflections that
signal the onset of polysynaptic components (Mears and Frank
1997
; Pinco and Lev-Tov 1993b
;
Ziskind-Conhaim 1990
). Despite the presence of some
polysynaptic components, the potential returned to the baseline
between stimuli in the presence of AP5.
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Figure 5E illustrates the complete curves of EPSP amplitudes
for the 10 pulses in each frequency trial, normalized by the amplitude
of R1 in each train. Randomizing the order to frequency presentation
did not affect the depression curves. The tail average represented a
stable plateau of depression for each frequency (see also Pinco
and Lev-Tov 1992
; von Gersdorff et al. 1998
), while the amplitudes of R2 and R3 captured the shapes of the initial depression curves. A semi-logarithmic plot of the three normalized response values against stimulus frequency (Fig. 5F)
provided a convenient summary of the curves for different stimulation
frequencies. The curve for the tail responses exhibited a relatively
smooth decline with increasing frequency while those for the R2 and R3 were more irregular, presumably because they were from single measurements.
The three EPSP depression curves for individual motoneurons for P2-P4
mice exhibited relatively narrow ranges of variation, consistent with
the relatively narrow ranges in postsynaptic motoneuron properties
found in this age range in the rat (Seebach and Mendell 1996
). Therefore we averaged the normalized EPSP data for 29 cells collected under the baseline conditions
([Ca2+]o = 2.0 mM;
temperature 23 to 24°C). These averaged curves in Fig.
6 show that R2, R3, and tail responses
all declined similarly as stimulation frequency increased but R2
diverged upward at frequencies >1 Hz. In all cases, the afferent
volleys were constant across frequencies (not shown; see Fig. 3),
indicating that changes in the numbers of afferents stimulated could
not account for these observations. Data from trials at 16 Hz (0.0625-s
intervals; see METHODS) were sometimes contaminated by
residual polysynaptic PSPs evoked by successive stimuli and were
therefore not included in the following analysis.
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Effect of altered [Ca2+]o
We examined the effect of changing the Ca2+
concentration in the bathing solution,
[Ca2+]o, on the amplitude
of monosynaptic DR EPSPs and on the depression curves. Decreasing
[Ca2+]o from the normal
of 2.0 to 0.8 mM without changing
[Mg2+]o, reduced the
average EPSP amplitude to 6.9 ± 2.6 (SD) mV (n = 8) from the average of 12.7 ± 5.3 mV (n = 29) at
2.0 mM. When compared with the EPSPs at normal
Ca2+ in the same motoneurons (n = 8), lowering [Ca2+]o to
0.8 mM reduced their amplitude by ~50%. In contrast, increasing [Ca2+]o to 4.0 mM
increased the average EPSP amplitude to 15.3 ± 6.3 mV
(n = 8) or ~19% in the individual cells examined.
The averages were significantly different only for the comparison of
low with normal and high
[Ca2+]o
(P < 0.05; 1-way ANOVA with Scheffe post hoc test) and
are comparable in magnitude with observations in P1-P3 neonatal rats (Seebach and Mendell 1996
).
Figure 7, A and B, illustrates that R2 and tail depression curves changed as [Ca2+]o was altered. The R2 at [Ca2+]o = 0.8 mM showed considerably less overall depression at all frequencies, while [Ca2+]o = 4.0 mM produced less R2 depression. Shifts in the R3 curves (not shown for clarity) were shifted in the same directions but less so. The tail response curves were much less changed by [Ca2+]o. Analysis of variance showed that the differences in R2 depression between normal and both altered [Ca2+]o concentrations were significant (P < 0.01), while only that between 0.8 and 2.0 mM [Ca2+]o was significant for the tail responses (Scheffe post hoc test).
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We attempted to alter presynaptic intraterminal
Ca2+ kinetics by applying membrane-permeable
forms of the low- and high-affinity calcium chelators, EGTA-AM (50-100
µM, n = 10 cells) and BAPTA-AM (10-100 µM,
n = 3 cells), respectively, to test whether the
relative facilitation of R2 and R3 responses with higher frequencies
might be produced by residual free Ca2+
(Chen and Regehr 1999
; Ouanounou et al.
1996
). Neither drug produced changes in R1 DR EPSP amplitudes
nor did they change the synaptic depression curves. We could not
interpret this negative result because we had no independent evidence
that the drugs penetrated the hemisected spinal cord.
Effect of increased temperature
Increasing bath temperature from 24 to 32°C produced no significant change the average amplitude of monosynaptic EPSPs (average at 32°C =10.7 ± 2.6 mV, n = 12; P > 0.1, 2-tailed t-test). It proved to be difficult to retain acceptable intracellular penetrations in the same cell as the bath temperature was increased but when this was accomplished, the EPSPs were on average 8% smaller compared with EPSPs at 24°C (n = 5). However, the average depression curves at 32°C were quite different from those at 24°C (Fig. 7, C and D), and this was also true when comparing the curves in the few individual neurons that were satisfactory at both temperatures. There was less depression of R2 responses than at 24°C for frequencies <0.2 Hz but at higher frequencies the curves converged. In particular, the region in which the R2 response began to show relative facilitation was shifted toward higher frequencies than at 24°C. In contrast, the tail responses showed less depression at all frequencies. All of these curve differences were significant by two-way ANOVA (P < 0.01).
Effect of GABAergic synaptic blockade
Because DR stimulation was used to elicit monosynaptic EPSPs, it
is possible that activation of presynaptic inhibitory pathways could
affect the observed synaptic depression curves. In the neonatal mouse
cord, we found that addition of even small concentrations of the
GABAA receptor blocker bicuculline (1-2 µM) to
the ACSF with 100 µM AP-5 produced marked increases in spontaneous
polysynaptic activity that prevented data collection (Fig.
1A) (see also Seebach and Mendell 1996
).
However, although we had elected not to use mephenesin for most of
these experiments (see preceding text), ACSF containing AP-5 (100 µM)
and mephenesin (1 mM) blocked paroxysmal discharges and allowed
addition of bicuculline (10-20 µM) to the bath. Bicuculline under
these conditions did not alter the depression curves (n = 5 cells in 2 animals; not shown). Furthermore, the addition of the
GABAB blocker 2-hydroxysaclofen (100 µM) also produced no changes in depression curves (n = 6 cells
in 3 animals). We conclude that GABA-related presynaptic inhibition
played little or no role in producing the observed EPSP depression curves.
Attempts to use CTZ to test whether AMPA glutamate receptor (GluR)
desensitization (Raman and Trussell 1995
) might be
involved in the present observations were inconclusive because bath
application of conventional doses (50-100 µM) produced marked
paroxysmal background activity even in the presence of 100 µM AP5. A
maximum dose of 15 µM CTZ produced no changes in the depression
curves in three cells tested.
Effect of EPSP amplitude on depression curves
There was a fivefold range in the amplitude of initial EPSPs
(i.e., R1) in different motoneurons in all of the conditions reported
above. However, a two-way ANOVA showed that there was no relation
between the shape or magnitude of the depression curves in relation to
R1 amplitudes. As expected from earlier work (Jahr and Yoshioka
1986
; Pinco and Lev-Tov 1993b
), the DR EPSPs in
P2-P4 mice were quite sensitive to blockade by the AMPA-receptor
blocker, CNQX. We added graded doses of CNQX (1-8 µM) to the ACSF to
reduce the amplitude of DR EPSPs and found that the depression curves in individual neurons were essentially unchanged when R1 amplitudes were varied over a four- to fivefold range (n = 8 cells; not shown). This suggests that voltage-sensitive postsynaptic
factors are probably not important in producing the observed synaptic
depression curves.
Modeling short-term depression
The systematic changes in synaptic depression with stimulation
frequency are difficult to interpret without a consideration of
possible underlying mechanisms. For example, the relative facilitation of R2 and R3 EPSPs observed at higher frequencies (Fig. 6) cannot be
explained by a simple depletion model (Liley and North
1953
; see also Magleby 1987
) but requires at
least one superimposed process that enhances transmitter output (e.g.,
Dittman and Regehr 1996
; Dittman et al.
2000
; Varela et al. 1997
; Weis et al.
1999
).
We assumed that composite monosynaptic EPSPs in the neonatal mouse
motoneurons are produced by multiple group Ia synaptic contacts with
wide postsynaptic dispersion, as in the adult cat (e.g., Burke
and Glenn 1996
). We treated the observed composite EPSPs as if
produced by a lumped "virtual synapse" that is reliably activated
by each afferent impulse. The latter assumption seems reasonable in
view of the constancy of terminal field potentials recorded in the VH
(Fig. 3). Because of the relative inaccessibility of this synaptic
system, we explored a series of six phenomenological models of
increasing complexity. The equations that define the system, Eqs.
A1-A9, are given in the APPENDIX. These recurrence
relations were used to define the state of the system at selected time
points,
t, to calculate the normalized amplitude of each
response in pulse trains at different frequencies. Three models use a
single compartment, called N, representing a pool (perhaps
readily releasable synaptic vesicles) that is depleted by transmitter
release, while the other three models used two depleting compartments,
N and S (where S is perhaps a pool of
activation-ready synaptic release sites).
After activation, the N and S pools are refilled
by exponential processes with time constants
N and
S, respectively. One- or two-compartment models had no additional processes (simple depletion); a process P that modulates the
proportion of release-ready elements that release transmitter; or
process P plus a second process M that alters the
rate at which pool N is refilled. At each activation process
P receives a constant increment,
P, that, when
positive, increases transmitter release (see Eqs. A6 and A7 in the APPENDIX), an effect that decays
exponentially, with time constant
P. Process M is somewhat
more complex, in that it introduces a time-dependent modification of
N (see Eqs. A8 and A9
in APPENDIX). Each activation produces a constant increment,
M, that when positive, reduces
N,i (see Eq. A4a in
APPENDIX). The effect of process M decays
exponentially, with time constant
M.
The full model thus has four time-dependent variables that are defined
at the ith activation, Ni,
Si, Pi, and
N,i, by a maximum of seven parameters.
Model assessment: baseline data
A parameter search program was developed that minimized the error between simulated and experimental responses for each of the six models under test (see the 2nd section in the APPENDIX). The relative amplitudes of simulated second (R2), third (R3), and average plateau (tail) EPSPs were compared with the averaged, normalized responses obtained from 29 motoneurons and recorded at 24°C with [Ca2+]o = 2.0 mM (Fig. 6). The inclusion of R3 in the fitting procedures proved to be essential to produce simulated full depression curves that matched observed records (i.e., Fig. 5E).
When matched against the baseline data set, the best fitting simple
depletion model with one compartment (i.e.,
Ri = Ni · f; 2 free parameters:
N and
f; see Eq. A6 in the APPENDIX) produced a large RMS error (6.5%; Table
1). The two-compartment simple depletion
model (Ri = Ni · Si · f; 3 free parameters:
N,
S, and f) produced a smaller
RMS error (4.8%; Table 1). Neither model reproduced the observed
relative facilitation of R2 and R3 at higher frequencies (Fig. 6),
which requires a process to enhance transmitter output at relatively
high frequencies.
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We therefore assumed a process, P, in which each activation
produces an increment,
P, that enhances transmitter
release and decays exponentially with time constant
P (Eq. A7). This effect is
presumably due to residual effect of Ca2+ entry
(Dittman and Regehr 1996
; Dittman et al.
2000
; reviews in Magleby 1987
; Zucker
1989
, 1999
). Data fit with one- and two-compartment models that
included P process (4 and 5 free parameters, respectively) exhibited the relative facilitation of R2 but were still not
satisfactory (Table 1). Using double-exponential time courses for the
decay of the P process actually worsened these fits.
It appeared that a process qualitatively different from release
facilitation was needed. We therefore added a second process, M, that modulates the rate of restoration of the
N compartment (
N) because of
evidence that repetitive synaptic activation can speed the reformation
of releasable transmitter (Stevens and Wessling 1998
;
Wang and Kaczmarek 1998
; Weis et al.
1999
). Each activation generates an increment,
M,
that decays exponentially with time (time constant
M; Eqs. A8 and A9). One- and two-compartment models that included both
P and M processes (6 and 7 free parameters,
respectively) markedly improved the fit, especially with the
two-compartment model (Fig. 8, Table 1). The parameter extraction program continued to exhibit robust
convergence despite the additional free parameters. It should be noted
that
S is not modified by the M
process, which enables the program to distinguish its effects on
simulated EPSPs from those produced by
N. The two-compartment model including
both P and M processes, referred to below as the
full model, was taken as the best fit to the baseline experimental
observations. This model includes elements similar to those in other
recent formulations (Dittman and Regehr 1998
;
Dittman et al. 2000
; Weis et al. 1999
).
|
Clearly the biological relevance of a model system with seven free parameters is debatable unless it can predict system behavior under a variety of conditions. We therefore tested the full model against data sets obtained with altered [Ca2+]o and temperature (Fig. 7) as well as with irregular stimulation intervals (Fig. 12).
Effect of [Ca2+]o on model parameters
Because it is likely that the fractional release, f,
and the increments
P and
M are dependent on
Ca2+ entry during synaptic activation (see
DISCUSSION), we predicted that these parameters would
exhibit the largest alterations with changes in
[Ca2+]o. Table
2 gives the results when the parameter
extraction program was run with each
[Ca2+]o data set under
two conditions: with all parameters free to vary ("free" columns)
and with all time constants fixed to their values found for
[Ca2+]o = 2.0 mM
("constr." columns). The last column in Table 2 gives the relative
reliability of the parameter values extracted by the program with noisy
input data (see APPENDIX).
|
The data from both low and high
[Ca2+]o conditions
yielded parameter sets that differed from the baseline set (Table 2).
However, except for
M and
M
under the low [Ca2+]o
condition, which are least reliable in the presence of input noise
("sensitivity" column in Table 2; see APPENDIX), most
of the time constants extracted from the two data sets changed little in comparison to the values for f,
P, and
M extracted when all parameters were free to vary. When
all four time constants were fixed to their baseline values (Table 2,
"constr."; Fig. 9), the extracted
values for f,
P, and
M changed
only slightly (with the exception of
M in the low
[Ca2+]o condition) and
all were decreased in low
[Ca2+]o and increased in
high [Ca2+]o (Fig.
11A).
|
Effect of temperature on model parameters
We expected that increased bath temperature should mainly affect
the time constants of the renewal processes,
N and
S and
possibly those of the P and M processes
(
P and
M). When all
parameters were free to find their best fit values, the system recovery
time constants,
N and
S, showed marked decreases as compared
with the 24°C values, while f was approximately the same,
again except for the problematic
M (Table
3, "free"). We therefore examined the
time constants that best fit the data when the values of f,
P, and
M were fixed to the values found at
24°C. The fit to the data was almost as close as when all parameters
were free (RMS error, 2.0 and 2.2%, respectively; Fig.
10). All four time constants had values
that were 40-45% smaller than the values obtained at 24°C (Fig.
11B), implying that the
relevant processes have a Q10 of ~2. The
decrease in
P accounts for the rightwards shift of the R2 inflection point in the observed data at
32°C (Fig. 7C).
|
|
|
Fitting EPSPs produced by pseudorandom interval sequences
There has been considerable recent interest in examining
short-term synaptic modulation during random interval activation sequences (Abbott et al. 1997
; Dittman and Regehr
1998
; Dobrunz and Stevens 1999
; Markram
et al. 1998
). As a final test of the present model, we recorded
EPSP amplitudes during activation sequences in which 17 pseudorandom
intervals (Fig. 12A) were
repeated for six cycles. This approach allows averaging of EPSPs that
follow identical stimulus intervals to improve signal to noise ratios. Such data sets were collected from five motoneurons in two P3 mice with
[Ca2+]o = 2.0 mM and
temperature 24°C. The first cycle of 17 EPSPs, during which the
system stabilized, were discarded except for the initial EPSP, which
was used to normalize the later responses. The normalized EPSPs in the
subsequent five cycles were averaged for individual animals, and
these averages were combined to give the normalized EPSPs shown in Fig.
12B (
± SE).
|
The parameter extraction program was modified to accommodate the
irregular stimulation data to assess whether the parameters of the full
model could be extracted from this short sequence of responses. We were
surprised to find that some runs of the extraction program generated a
parameter set that produced an excellent fit to the input data (Fig.
12B,
; Table 4), although a
majority of runs led to several other local minima that produced parameter sets with larger RMS errors. Tests with artificial data sets
suggested that irregular sequences of EPSPs contain less information
than the R2, R3, and tail data but nevertheless have enough content to
constrain the parameter extraction process (see APPENDIX).
|
| |
DISCUSSION |
|---|
|
|
|---|
A great deal of recent work on these mechanisms in CNS synapses
has been done using in vitro slice preparations that offer particular
structural advantages, such as the calyx of Held (e.g., Bellingham et al. 1998
; Borst and Sakmann
1998
; Forsythe et al. 1998
; Wu and Borst
1999
), the parallel fiber synapses on cerebellar Purkinje cells
(e.g., Atluri and Regehr 1996
; Dittman and Regehr 1998
), and the climbing fiber synapses on cerebellar Purkinje cells (Silver et al. 1998
). We chose to study the less
accessible spinal cord system for several reasons. Monosynaptic
contacts from group Ia muscle spindle afferents onto spinal motoneurons represent a functionally well-defined synaptic system that has been
intensively studied in adult mammals (Burke and Rudomin
1977
; Eccles 1964
; Redman 1990
).
This system exhibits functional immaturity at birth in comparison to
propriospinal excitatory systems that are formed earlier in embryonic
life (Pinco and Lev-Tov 1994
) but changes rapidly during
the first 2 wk of postnatal life (Seebach and Mendell
1996
), making it a potentially useful model of synaptic maturation. We hoped to be able to use information that has been developed in more accessible synaptic systems to understand this process. Finally, the mouse is rapidly becoming an important model system for neuroscience research because of the availability of neurological mutant animals. Baseline information about normal development of synapses and circuits in the mouse is essential to
elucidate functional abnormalities in such animal models.
Initial DR EPSPs are monosynaptic
We assume that DR EPSPs are produced by group Ia muscle spindle
afferents that project directly to motoneurons as in the adult cat
(Burke and Glenn 1996
; Burke and Rudomin
1977
; Eccles 1964
). DR afferents reach the
ventral horn by day E17 in embryonic rats and mice, produce functional
excitation of motoneurons shortly thereafter, and are well established
by postnatal day two (Kudo and Yamada 1985
, 1987
;
Mears and Frank 1997
; Ziskind-Conhaim
1990
). Much of the relatively long latency exhibited by the
EPSPs produced by these afferents at room temperature appears to be due
to slow conduction along intraspinal collaterals (Fig. 3C)
(see also Lev-Tov and Pinco 1992
). As measured from VH
terminal potentials in the neonatal mouse, local synaptic delay is
1.0 ms (Fig. 3, A and B) (see also
Lev-Tov and Pinco 1992
). Moreover, increasing the bath
temperature to 32°C produced marked decreases in these latencies, without changes in the initial EPSP rising phases (Fig. 4). We conclude
that the initial DR EPSP in the mouse spinal cord are monosynaptic.
As expected from earlier studies (Jahr and Yoshioka
1986
; Konnerth et al. 1990
; Pinco and
Lev-Tov 1993b
; Ziskind-Conhaim 1990
), the DR
EPSPs are markedly sensitive to blockade by the AMPA-receptor blocker
CNQX but also exhibit a relatively minor component that is reduced by
the NMDA receptor blocker, AP5 (Fig. 2). Pinco and Lev-Tov
(1993b)
have presented evidence that both types of glutamate receptor are co-activated by release from the same monosynaptic synapses (see also Konnerth et al. 1990
; von
Gersdorff et al. 1997
). Therefore we assume that
interpretations of the present observations are unlikely to be
distorted by the use of AP5 to reduce background activity.
EPSP depression is not due to failure of afferent activation or presynaptic inhibition
The constancy of afferent volleys entering the spinal cord (e.g.,
Fig. 3) confirmed the findings of others that the range of stimulation
frequencies do not change the number of DR afferents activated
(Kudo and Yamada 1985
; Seebach and Mendell
1996
). The extracellular VH terminal potentials recorded in the
ventral horn at different stimulation frequencies are constant (Fig.
3B), suggesting that conduction in intraspinal collaterals
is also secure at the stimulus frequencies used in this work
(Lev-Tov and Pinco 1992
). The relative facilitation of
R2 and R3 responses at higher stimulus frequencies fits this conclusion
because propagation failures would be expected to increase as frequency
rises (Streit et al. 1992
).
It is possible that DR stimulation can activate pathways that produce
presynaptic inhibition, which could complicate interpretation of
depression curves. Indeed, low-frequency depression of monosynaptic transmission in the adult rat has been attributed mainly to presynaptic inhibition (e.g., Seburn and Cope 1997
). In the present
work, addition the GABAA receptor blocker
bicuculline produced no changes in observed depression curves when
mephenesin plus AP5 was used to suppress paroxysmal and stimulus-evoked
polysynaptic activity. Similarly, addition of 2-hydroxysaclofen to
depress GABAB receptors also produced depression
curves that were essentially identical to control curves in the same
motoneurons. We conclude that presynaptic inhibition, if it exists in
the neonatal mouse cord, does not contribute to the present
observations. It is unknown whether the recently described
non-GABA-related PAD, attributed to increases in extracellular
[K+]0 (Kremer and
Lev-Tov 1998
), can modulate synaptic transmission.
Presynaptic metabotropic glutamate receptors can produce powerful
modulation of synaptic transmission (reviewed in MacDermott et
al. 1999
). Preliminary experiments with group II/III
metabotropic GluR (mGluR) agonists exhibited strong reductions of DR
EPSPs and concomitant reduction in synaptic depression in the mouse cord (unpublished data). Although activation of presynaptic mGluRs appear to play only a minor role in short-term synaptic depression at
the calyx of Held (von Gersdorff et al. 1999
), further
experiments are underway to examine this possibility in the neonatal
mouse cord.
We were unable to evaluate the possibility that GluR desensitization
plays a role in the depression observed in the mouse cord because CTZ,
which is customarily used to block this effect, produced marked
paroxysmal discharges in the mouse cord when doses larger than 15 µM
were applied. Interpretation of CTZ effects were also complicated by
recent evidence that CTZ can also affect presynaptic transmitter
release mechanisms (Bellingham and Walmsley 1999
).
However the inter-stimulus intervals employed in this study were all
considerably longer than the reported duration of GluR desensitization
(Raman and Trussell 1995
; Turecek and Trussell 2000
), so it seems unlikely that this factor distorted the
present results.
On the basis of the preceding observations, we have attributed the observed modulation of monosynaptic DR EPSP amplitudes during repetitive stimulation to presynaptic mechanisms involved in transmitter mobilization and release. We developed quantitative phenomenological models of the system because the complex effects of stimulation frequency, and changes in [Ca2+]o and temperature, on DR EPSP amplitudes were difficult to understand intuitively.
Nature of model elements
In the adult cat, composite monosynaptic group Ia EPSPs are
produced by multiple afferents, each having multiple synaptic boutons
on an individual motoneuron (Burke and Glenn 1996
;
Redman and Walmsley 1983
). The synaptic potentials
produced by an individual group Ia afferent exhibit all-or-none quantal
increments (Burke 1967
; Kuno 1964
;
Redman 1990
; Redman and Walmsley 1983
),
which may or may not represent saturating actions at individual
boutons. For simplicity, the present empirical model treated the
anatomically and functionally complex system as if it were a single
synaptic entity. We assume that the N compartment represents
the net behavior of readily releasable transmitter vesicles while the
S compartment presumably reflects the net behavior of
release sites in the synaptic boutons. This two-compartment system
provided better fits to the experimental data than single-compartment
models (Table 1) (see Varela et al. 1997
).
There is no doubt that the entry of Ca2+ into
synaptic terminals is the major factor that initiates evoked
transmitter release (Magleby 1987
; Zucker 1989
,
1999
). The rapidly decaying P process that produces
overt facilitation of R2 and R3 only at higher frequencies is
compatible with the notion of "residual calcium," in which the
effect of voltage-sensitive Ca2+ entry decays
over a finite time, producing paired-pulse facilitation (Dittman
and Regehr 1998
; Pinco and Lev-Tov 1993a
;
reviewed in Magleby 1987
and Zucker
1999
). In the present results, the covert facilitation of R2
and R3 at higher stimulus frequencies was only evident in relation to
the amplitudes of those responses at lower frequencies (Figs. 5-7).
The estimated time constant for the short-term facilitatory
P process at 24°C (
P = 140 ms; Fig. 8) is compatible with the rapid decay of paired-pulse
facilitation in synapses from cerebellar granule cells to Purkinje
cells (100-200 ms) (Atluri and Regehr 1996
;
Dittman and Regehr 1998
). Directly visualized free
intra-terminal Ca2+ decays more rapidly than this
paired-pulse facilitation, implying the operation of an indirect
Ca2+-activated mechanism rather than simply
amplifying low-affinity triggered release (Atluri and Regehr
1996
; Zucker 1999
). Whatever Ca2+-related molecular events result in residual
Ca2+ facilitation, it seems reasonable to
attribute the present P process to this mechanism.
We interpret the parameter f as the proportion of
release-capable sites that do in fact liberate readily releasable
transmitter rather than a probability associated with individual
release sites. The distinction is important here because, with
P = 2.1 (Fig. 8), f · (1 + Pi) more than triples as
t
approaches zero. Although f during synaptic activity need
not be constant (Silver et al. 1998
), a value >1.0
would be meaningless for a probability. However, if we interpret
Si · f · (1 + Pi) as the proportion of release-ready sites at a given time, values >1 could signify an increase in the
total number of release-ready sites (i.e.,
Smax, used to normalize Si) above its original value (for example,
see Wang and Zucker 1998
). In other words, if
f is assumed to be constant, a value of
Pi > 1 could indicate that the number of
release-ready sites is larger than the original absolute
Smax in the baseline state. Of course,
the present model cannot differentiate between changes in f
versus Smax and/or
Nmax, any or all of which may be
altered by repetitive activation (e.g., Schneggenburger et al.
1999
; Wu and Borst 1999
). One possible
interpretation of a change in Smax is
that repetitive activation may reveal the existence of synapses that do
not release transmitter in the baseline state (i.e., "silent" synapses).
The relatively subtle effects added by the M process fit
with the classical distinction between a rapidly decaying
"facilitation" and a more slowly decaying "augmentation" during
repetitive synaptic activation (Magleby 1987
;
Zucker 1989
). There is evidence that repetitive
activation increases the rate of renewal of readily-releasable transmitter in some synaptic systems (Stevens and Wesseling
1998
; Wang and Kaczmarek 1998
; Wang and
Zucker 1998
). This effect was implemented by modifying
N that governs the rate of transmitter
renewal by a saturating process that grows during stimulus trains and
decays exponentially after each stimulus (Eqs. A4a, A8, and A9). It should be noted that the time constant for renewal of release sites
S was assumed to be
constant, which enabled the parameter extraction program to
differentiate between
N and
S, despite their analogous effects on the
calculated responses (Eq. A6).
Effect of altered [Ca2+]o on synaptic transmission
The relief of synaptic depression that occurs when
[Ca2+]o is lowered is
usually attributed to reduction in transmitter depletion (Betz
1970
; Lev-Tov and Pinco 1992
). As found by
Pinco and Lev-Tov (1993a)
, lowering
[Ca2+]o from 2.0 to 0.8 mM, without changing
[Mg2+]o, reduced the
average amplitude of R1 EPSPs by ~50% and significantly reduced the
paired-pulse depression of R2 (Fig. 7A). On the other hand,
the depression of tail responses was little changed by either low or
high [Ca2+]o (Fig.
7B). This differs from the observations of Lev-Tov and Pinco
(Lev-Tov and Pinco 1992
; Pinco and Lev-Tov
1993a
), who used older rat pups (P6-P10) and low
[Ca2+]o ACSF (0.75 mM)
with high Mg2+ (6-7 mM) and mephenesin. Under
these conditions, they found markedly decreased steady-state (i.e.,
tail) depression, accompanied by a much larger (about fourfold)
decrease in absolute R1 amplitudes than was observed in our
experiments. The composition of our normal bathing solution was
virtually identical to theirs, except that we did not change the
Mg2+ concentration when
[Ca2+]o was altered nor
did we use mephenesin in these experiments. Such differences presumably
account for the divergent observations.
The empirical model provided clues to the mechanisms that may underlie
these complex changes. The R2 depression curves in the three
[Ca2+]o conditions (Fig.
7A) were offset in response amplitude but were similar in
shape. This fits with model analysis (Fig. 11A), which
suggested that changing Ca2+ entry alters the
release fraction f and the increments of the P
and M processes (
P and
M), all
of which affect EPSP amplitudes, rather than the system time constants
(Table 2). Interactions between these factors in the initial EPSPs in
each train produced fractional depletions of the N and
S compartments that were roughly similar in all three conditions.
Effect of increased temperature
It has long been known that temperature markedly affects synaptic
transmission as well as the intrinsic properties of neurons (Katz and Miledi 1965
; Pierau et al.
1976
). In the present work, increasing bath temperature from 24 to 32°C produced considerable decreases in central latencies of
monosynaptic DR EPSPs (Fig. 4), presumably because of increased
conduction velocities in afferent collaterals and perhaps also by
shortening synaptic delay (Katz and Miledi 1965
).
Although the average amplitudes of DR-evoked composite EPSPs were about
the same at 24 and 32°C, the R2 and tail depression curves showed
less relative depression at the higher temperature except for R2
responses at frequencies >4 Hz (Fig. 7, C and
D).
In contrast to the results with altered
[Ca2+]o, temperature
increase changed the shape of the depression curves (Fig. 7,
C and D), notably introducing a convergence in
the R2 depression curves for higher frequencies at different
temperatures (Fig. 7C). The model suggests that the major
factor producing this convergence is the marked shortening of
P from 140 to 80 ms (Table 3), which limits
facilitation to interpulse intervals <0.250 ms (4 Hz) at 32°C. This
would be difficult to explain by changes in the postsynaptic
motoneurons (e.g., see Hardingham and Larkman 1998
). The
reduction in
P with increased temperature is
compatible with the faster decay of paired-pulse facilitation and free
[Ca2+]o found by
Atluri and Regehr (1996
, their Fig. 3) in cerebellar granule cell synapses with a similar temperature increase. The more
rapid restoration of the N and S pools, coupled
with the apparent lack of change in f (Table 3), produced
the smaller relative synaptic depression of all EPSPs.
Concluding comment
Although the participation of other factors cannot be ruled out,
the relative success of the present model formulation suggests that
short-term synaptic depression of monosynaptic (presumably group Ia)
EPSPs in the P2-P4 mouse spinal cord results primarily from mechanisms
operating within presynaptic terminals. The present results are
consistent with the view that short-term synaptic depression results
mainly from depletion of independent pools of readily releasable
transmitter and competent release sites, plus a release fraction that
is relatively high (Zucker 1989
, 1999
; but cf.
Markram et al. 1998
). The results also suggest the existence of rapidly decaying facilitation and more slowly decaying augmentation processes with stimulus-evoked increments that depend on
Ca2+ entry (Zucker 1999
). Because
of the complex interactions between these processes, these conclusions
are not intuitively obvious from inspection of the data, but they are
all compatible with findings in more accessible systems. The present
results provide a framework for examination of the postnatal maturation
of group Ia synaptic transmission in the neonatal mouse.
| |
APPENDIX |
|---|
|
|
|---|
Model assumptions and components
Although the models used in this work progressed from simple to more complex, it is more convenient to describe the full model used for parameter searches and then show how it can be reduced to test all six formulations tested.
1) The full model includes two independent pools of Nmax and Smax release-ready elements with unknown absolute values, which are both required for transmitter liberation. The release-ready populations are expressed as fractional populations, so that N1 = N/Nmax = 1 and S1 = S/Smax = 1 in the baseline state. The product Ni · Si represents the fractional population that is capable of releasing transmitter at the ith activation.
2) A constant proportion, f, of release-ready
Ni · Si
elements actually release transmitter at each ith
activation. When the Ni and
Si elements release transmitter to give an
EPSP, Ri, they are depleted, or
become refractory (N*i and
S*i). Thus the first
response, R1, in a train is simply
|
(A1) |
|
(A2) |
|
(A3) |
t, by independent, saturating, exponential processes
|
(A4) |
|
(A5) |
5) The relative facilitation of R2 and R3 at higher
frequencies (Fig. 6) is produced by a saturating process P
in which each activation adds an increment
P that changes
transmitter release from competent Ni or
Ni · Si
elements, so that the ith EPSP amplitude Eq. A1
becomes
|
(A6) |
|
(A7) |
P = 0.
6) Based on evidence that repetitive synaptic activation can
increase the availability of readily-releasable transmitter during repetitive stimulation (see DISCUSSION). This effect is
simulation by a saturating process, M, with increment
M and exponential decay time constant
M, by which synaptic activation can
change the initial time constant
N,0 in
Eq. A4
|
(A8) |
N as
|
(A9) |
M,
N,i+1 decreases during repetitive
activation, effectively increasing the renewal rate of
Ni, so that Eq. A4 becomes
|
(A4a) |
M = 0.
7) The amplitudes of all simulated responses in a given train were normalized by that of the first EPSP, R1, as done with the observed data (Fig. 6).
Model assessment
The behavior of this system of equations was explored using a
spreadsheet with graphics (Microsoft Excel). One-compartment simulations were obtained by setting Si = 1.0 in Eq. A6. Setting
P to zero in Eq. A7 removes the facilitating P process, while setting
M to zero in Eq. A8 removes the augmenting
M process. The parameters exhibited complex interactions in
their effects of the shapes of the R2, R3, and tail depression curves.
To extract the parameter set that best fit each elaboration of the
model, Eqs. A1-A9 were embodied in a computer program
written in PASCAL (CodeWarrior, Metrowerks; Macintosh G3 computer). The
program used an iterative search algorithm to find the set of
parameters that minimized the RMS error between simulated and
experimental R2, R3, and tail responses at all frequencies tested
(e.g., Fig. 8). The program began with randomly chosen values for the
free parameters in the selected model type and used these to generate
10 responses, R1-R10, with
t values of 0.125, 0.25, 0.5, 1, 2, 4, and 8 s. The summed differences between all observed
(Vobs,i) and simulated (Vcalc,i) responses gave the
root mean square (RMS) error for each test parameter set
|
Despite the large number of iterations, a complete parameter search with 105 iterations took <10 s on a G3 Macintosh computer. The source code is available on request.
Sensitivity tests
Tests of the full model's sensitivity to changes in each of the
seven parameters were done in two ways. First, we generated R2, R3, and
tail responses using the baseline parameter set (Fig. 8), but with the
individual parameters perturbed up to ±20% from the baseline values,
one at a time. The resulting RMS errors were slightly asymmetrical with
positive versus negative perturbations but were almost linearly related
to perturbation magnitude. Changing the release fraction, f,
produced the largest total errors while equivalent changes in
M produced the smallest. For 20% perturbation, the
relative total RMS errors varied in the following descending sequence:
f,
N,
P,
S,
P,
M, and
M, with ratios of
13.2:4.5:2.4:2.0:1.8:1.0:1.0, respectively.
It was also important to determine the error in parameter that are
extracted from test data created with a known parameter set. This was
done by using the program repeatedly to extract parameters from the
test data with different levels of added random noise (0, 5, 10, 20, or
30% random noise, with 10 trials on each set). Test data with
20%
added random noise converged to similar parameter sets. Convergence to
more than one parameter set was sometimes encountered with 30% noise,
although the majority of runs still converged to a set that exhibited
similar minimum RMS error. Percent parameter error was defined as 1 - (test/target) · 100. Without added noise, the average error was
<1.0% for f,
N,
P,
and
P, ~2% for
S, and 5 and 6.6% for
M and
M, respectively. As
expected, adding
20% random noise increased the average error
introduced with were larger for all extracted parameters, but still
largest for
M and
M.
The variability in each parameter during repeated extractions was
assessed by the percentage coefficients of variation (CV = SD · 100/mean) of the extracted parameter errors during repeated trials with
noisy input. The error and CV values were all dimensionless ratios. To
encapsulate both average error and its variability in repeated trials,
we took the average of the dimensionless error and CV ratios with and
without noisy input data as a combined figure of merit. By this
measure, f is the most reliable parameter and
M is the least reliable. This ordering of noise
sensitivity was similar to that found for the first test: f,
N,
P,
P,
S,
M, and
M, with ratios of
1:1.5:4.0:4.5:6.1:9.1:24.4, respectively (included in Tables 2 and 3).
Responses at the limits
The final model formulation includes one equation (Eq. A7) that introduced an unbounded term (P) into the
calculation of the normalized responses (Eq. A4a), which
produced the upward curvature of R2 depression at higher frequencies.
Equations 2-7 can be compressed into a single expression
for normalized R2
|
|
t
0, this equation reduces
to
|
t
approaches zero.
We also used the final model equations to develop a single closed-form
equation to calculate the steady-state normalized response, R
. The calculated
R
values were within 1% of those of the model responses to the tenth pulse (i.e., R10) at frequencies
1 Hz but, as expected, deviated at the higher frequencies because the
system requires 10 pulses to reach equilibrium at those frequencies.
| |
ACKNOWLEDGMENTS |
|---|
The authors are grateful to Dr. William B. Marks for many discussions on the model formulation and to Dr. Michael O'Donovan for comments on an earlier draft of the manuscript.
| |
FOOTNOTES |
|---|
Address for reprint requests: R. E. Burke, Bldg. 49, Rm. 3A51, National Institutes of Health, Bethesda, MD 20892-4455 (E-mail: reburke{at}helix.nih.gov).
Received 4 December 2000; accepted in final form 5 January 2001.
| |
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K. E. Personius, Q. Chang, G. Z. Mentis, M. J. O'Donovan, and R. J. Balice-Gordon Reduced gap junctional coupling leads to uncorrelated motor neuron firing and precocious neuromuscular synapse elimination PNAS, July 10, 2007; 104(28): 11808 - 11813. [Abstract] [Full Text] [PDF] |
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E. Zaporozhets, K. C. Cowley, and B. J. Schmidt Propriospinal neurons contribute to bulbospinal transmission of the locomotor command signal in the neonatal rat spinal cord J. Physiol., April 15, 2006; 572(2): 443 - 458. [Abstract] [Full Text] [PDF] |
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L. Vila, E. F Barrett, and J. N Barrett Stimulation-induced mitochondrial [Ca2+] elevations in mouse motor terminals: comparison of wild-type with SOD1-G93A J. Physiol., June 15, 2003; 549(3): 719 - 728. [Abstract] [Full Text] [PDF] |
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Y. Li and R. E. Burke Developmental Changes in Short-Term Synaptic Depression in the Neonatal Mouse Spinal Cord J Neurophysiol, December 1, 2002; 88(6): 3218 - 3231. [Abstract] [Full Text] [PDF] |
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