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Volume 17, Number 17,
Issue of September 1, 1997
pp. 6647-6656
Copyright ©1997 Society for Neuroscience
Alteration of Ca2+ Dependence of Neurotransmitter
Release by Disruption of Ca2+ Channel/Syntaxin
Interaction
Jens Rettig1,
Christian Heinemann1,
Uri Ashery1,
Zu-Hang Sheng2,
Charles T. Yokoyama2,
William
A. Catterall2, and
Erwin Neher1
1 Department of Membrane Biophysics,
Max-Planck-Institute for Biophysical Chemistry, 37077 Göttingen,
Germany, and 2 Department of Pharmacology, University of
Washington, Seattle, Washington 98195-7280
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
DISCUSSION
FOOTNOTES
REFERENCES
ABSTRACT
Presynaptic N-type calcium channels interact with syntaxin and
synaptosome-associated protein of 25 kDa (SNAP-25) through a binding
site in the intracellular loop connecting domains II and III of the
1 subunit. This binding region was loaded into embryonic
spinal neurons of Xenopus by early blastomere injection. After culturing, synaptic transmission of peptide-loaded and control cells was compared by measuring postsynaptic responses under different external Ca2+ concentrations. The relative
transmitter release of injected neurons was reduced by ~25% at
physiological Ca2+ concentration, whereas injection
of the corresponding region of the L-type Ca2+
channel had virtually no effect. When applied to a theoretical model,
these results imply that 70% of the formerly linked vesicles have been
uncoupled after action of the peptide. Our data suggest that severing
the physical interaction between presynaptic calcium channels and
synaptic proteins will not prevent synaptic transmission at this
synapse but will make it less efficient by shifting its Ca2+ dependence to higher values.
Key words:
neuromuscular junction;
Ca2+
dependence;
synaptic transmission;
calcium channel;
synprint;
syntaxin
INTRODUCTION
Classic studies by Fatt and Katz
(1951)
at the frog neuromuscular junction revealed that
Ca2+ influx into the presynaptic terminal provides
the trigger for fast synaptic transmission in the vertebrate CNS.
Calcium ions enter the synaptic terminal through voltage-gated calcium
channels, which are clustered at specialized regions called active
zones (Heuser and Reese, 1981
; Robitaille et al., 1990
). The release of
neurotransmitter molecules is steeply dependent on the external calcium
concentration [Ca2+]e. Dodge and
Rahamimoff (1967)
estimated that the probability of acetylcholine
release at the frog neuromuscular junction increases as the fourth
power of [Ca2+]e.
The delay between Ca2+ influx and fusion of synaptic
vesicles is estimated to be in the range of 200-700 µsec (Llinas et
al., 1981
; Borst and Sakmann, 1996
; Yazejian et al., 1997
), leading to
the suggestion that there might be a physical link between presynaptic
channels and proteins of the docking and fusion machinery. Indeed,
coimmunoprecipitation studies indicated a close association between
-conotoxin GVIA-sensitive N-type calcium channels and syntaxin, a 35 kDa protein anchored by its C terminus in the presynaptic membrane and
a member of the synaptic core complex (Bennett et al., 1992
; Yoshida et
al., 1992
). An 87 amino acid region from the cytoplasmic loop between
homologous repeats II and III (LII-III) of the
channel is responsible for binding to syntaxin 1A (Sheng et al., 1994
).
A peptide containing this synaptic protein interaction (synprint) site
also blocks binding of native N-type channels to syntaxin and interacts
with synaptosome-associated protein of 25 kDa (SNAP-25) (Oyler et al.,
1989
), another presynaptic protein involved in docking and fusion of
synaptic vesicles. Binding of the peptide to syntaxin and SNAP-25
occurs in a Ca2+-dependent manner, being maximal in
the range of 10-30 µM [Ca2+] (Sheng
et al., 1996
), near the calcium threshold for secretion (for review,
see Burgoyne and Morgan, 1995
). Recently, it has been shown that
introduction of synprint peptide into presynaptic superior cervical
ganglion neurons reversibly inhibits synaptic transmission (Mochida et
al., 1996
), underscoring the physiological significance of this
interaction. This inhibition might be attributable to either
interference with the secretory machinery or changes in the calcium
dependence of transmission as the vesicle is separated from the calcium
channel.
To learn about the effect of synprint peptide on the calcium dependence
of synaptic transmission, we injected the purified syntaxin binding
site of N-type Ca2+ channels into one of the early
blastomeres of Xenopus laevis. Nerve-muscle cocultures
obtained from developing Xenopus embryos provide a powerful
system for the study of synaptic transmission. Synaptic transmission in
these cultured neurons is mainly dependent on N-type
Ca2+ channels (Yazejian et al., 1997
), thus making
it an ideal preparation for studying the possible interaction of the
N-type channels with proteins of the synaptic core complex. During the
first days of development, the embryos undergo cell divisions without
substantial growth. Injection of macromolecules into early blastomeres
therefore leads to efficient loading of all progeny cells, including
spinal cord neurons and muscle cells. The effect of the injected
macromolecules on synaptic transmission can be assayed at neuromuscular
junctions developed by these cells in culture (Tabti and Poo, 1991
),
and the presynaptic calcium concentration can be monitored with
fluorescent indicators. Our results show that synprint peptides reduce
the calcium sensitivity of synaptic transmission and support a model in
which the synprint peptides increase the distance between docked vesicles and calcium channels.
MATERIALS AND METHODS
Preparation of nerve-muscle cocultures.
Xenopus nerve-muscle cocultures were prepared from the
neural tube and associated myotomal tissue of stage 20-22 embryos as
described (Tabti and Poo, 1991
). After dissociation in
Ca2+-Mg2+-free solution (125 mM NaCl, 2 mM KCl, 1.2 mM EDTA, 5 mM HEPES, pH 7.6), cells were plated on glass coverslips
pretreated for ~60 min with ECL (entactin, collagen, and laminin;
Upstate Biotechnologies, Lake Placid, NY) and grown for ~24 hr at
22°C. The culture medium consisted of 70% Leibovitz L-15
supplemented with GMS-X and antibiotics (all components from Life
Technologies, Gaithersburg, MD). All electrophysiological experiments
were performed 1 d after plating.
Peptide injection and immunoblot analysis. Recombinant
His-fusion proteins containing the syntaxin/SNAP-25 binding site of N-type Ca2+ channel (LII-III 718-963)
and, as a negative control, the corresponding region of the L-type
calcium channel (LII-III 670-800), were purified as
described (Mochida et al., 1996
) and concentrated to a final concentration of 1 mg/ml. Peptides were mixed 1:1 with
rhodamine-dextran (molecular weight 10,000; 10 mg/ml) (Molecular
Probes, Eugene, OR), and ~10 nl of that mixture was injected into one
blastomere of embryos at the two- to four-cell stage by pressure
injection (Microinjector 5242) (Eppendorf, Hamburg, Germany). For
Western blotting, embryos at various stages were collected and
homogenized by trituration through Eppendorf tips with 20 µl of
extraction buffer (100 mM KCl, 0.1 mM
CaCl2, 1 mM MgCl2, 10 mM HEPES, pH 7.7). After centrifugation (14,000 rpm, 10 min), the supernatant of one embryo was loaded onto each lane,
separated by SDS-PAGE, and transferred overnight to nitrocellulose (0.2 µm) (Schleicher & Schuell, Dassel, Germany). Immunoblot analysis was
performed with Anti-T7.Tag monoclonal antibody (1:10,000) (Novagen,
Madison, WI), and the immunoreactive bands were visualized by enhanced chemoluminescence (ECL system) (Amersham, Arlington Heights, IL).
Electrophysiological recordings. Before recording,
spinal neurons were examined for rhodamine fluorescence (see optical
setup for details). Fluorescent nerve cells were considered
peptide-positive. Synaptic currents were recorded from innervated
muscle cells in the whole-cell configuration using a combination of
EPC-9 and EPC-7/EPC-8 amplifiers driven by the Pulse v8.06 software
package (Heka Elektronik, Lambrecht, Germany). The pipette solution for the muscle cells contained 107 mM CsCl, 1 mM
MgCl2, 1 mM NaCl, 10 mM
EGTA, 10 mM HEPES, pH 7.3. The bath solution contained
normal frog Ringer's solution (116 mM NaCl, 2 mM KCl, 1 mM MgCl2, 5 mM HEPES, pH 7.3), with varying calcium concentrations
(ranging from 0.3 to 10 mM) as indicated in the figures.
Solutions were changed by rapid perfusion with an estimated exchange
rate of 2-4 ml/min, the bath volume being 1 ml. To keep approximately
the same external divalent cation concentrations, external magnesium
concentrations were 2.5, 2.3, and 1.8 mM for 0.3, 0.5, and
1 mM [Ca2+]e,
respectively. For 1.8 and 10 mM
[Ca2+]e, the external magnesium
concentration was kept at 1 mM. The muscle cells were
routinely clamped at
50 mV holding potential. A 10 msec test pulse to
60 mV was given before each EPSC sweep to estimate the series
resistance for later offline series resistance compensation. Action
potentials were routinely elicited on external stimulation (0.3-0.5
msec, 0.2-2 µA) of the nerve cell soma, with frequencies between 0.2 and 1.0 Hz. In the case of fura-2 experiments, the whole-cell
configuration was established on the soma of the nerve cell. The nerve
cell was held at a potential between
45 and
70 mV in the current
clamp mode. Action potentials were elicited every 1-5 sec or as a
train of 10 action potentials (20 Hz) with 2 msec current injections of
700-900 pA. The pipette was filled with 114 mM potassium
gluconate, 10 mM KCl, 1 mM NaCl, 1 mM MgCl2, 10 mM HEPES, 2 mM MgATP, 0.3 mM GTP, 100 µM
fura-2, pH 7.3.
Data analysis. Amplitudes of EPSC were analyzed with locally
written software in IGOR (WaveMetrix, Lake Oswego, Oregon). Synaptic currents were counted as evoked currents when they occurred in a 6 msec
time window after the stimulus. Because of the large EPSC amplitudes
(up to 10 nA), there was sometimes a significant clamp error in our
measurements. The series resistance before each EPSC was estimated from
the peak of the capacitive current during the test pulse. We corrected
the EPSC amplitudes assuming a linear I-V
relation and a reversal potential of +2 mV (as measured independently).
Experiments with clamp errors larger than 30 mV were excluded from
further analysis.
Model calculations. Equilibrium calculations for the
Ca2+ dependence of transmitter release were also
performed in IGOR (WaveMetrix). We used a model scheme with four
sequential Ca2+ binding steps similar to those used
to describe the Ca2+ dependence of secretion in
neuroendocrine cells and bipolar nerve terminals (Heinemann et al.,
1994
; Heidelberger et al., 1994
). The equilibrium
Ca2+ binding is described in matrix notation by:
where X denotes
[Ca2+]i.
and
are rate
constants for binding and unbinding of Ca2+ to a
single Ca2+ binding site, and B = (B0, B1, B2,
B3, B4) is the vector of pool
sizes of vesicles that have bound zero, one, two, three, and four
Ca2+ ions, as denoted by the subscripts.
S0 is the total number of releasable vesicles.
We also implemented cooperative Ca2+ binding by the
factor b. Values for kinetic parameters
,
, and
b were taken from Heidelberger et al. (1994)
. The
dissociation constants for the four sequential Ca2+
binding steps were 143 µM, 57 µM, 23 µM, and 9 µM. The amount of transmitter
release was calculated for different
[Ca2+]i as the equilibrium filling
state of the pool B4
(B4([Ca2+]i)).
Optical setup. A monochromator-based illumination system
(T.I.L.L. Photonics, Planegg, Germany) was coupled into the
epifluorescence port of an inverted Axiovert 10 or IM 35 microscope
(Zeiss, Oberkochem, Germany). For fluorescence measurements we used an
Achrostigmat or Fluar objective (40×, 1.3 numerical aperture, oil
immersion; Zeiss). Rhodamine and fura-2 were excited at 530 nm or
350/380 nm, respectively. The filter sets for rhodamine were 565DCLP, LP580 (AHF Analysentechnik, Tübingen, Germany), and those for fura-2 were DC495, LP505 (T.I.L.L. Photonics). The illumination area
was reduced to a spot of ~15 µm diameter to reduce background fluorescence originating from dye-filled pipette and soma. The fluorescence detection area was adjusted by a "view finder system" (T.I.L.L. Photonics) to cover just the nerve terminal. Fluorescence light was detected with a photomultiplier tube (R928, Hamamatsu) and
acquired with the Pulse software package (Heka Elektronik).
RESULTS
Loading of synprint peptide into Xenopus embryos
Purified synprint peptide containing the syntaxin-binding region
of the N-type calcium channel was injected into one blastomere of a
Xenopus embryo at the two- to four-cell stage. To identify peptide-containing neurons in cell culture, rhodamine-dextran was
included as a fluorescent marker. After 24 hr of development (stage
19-22 according to Nieuwkoop and Faber, 1967
), the spinal cord was
dissected, and nerve-muscle cocultures were prepared. To determine
whether injected peptide was still present and intact, we performed
immunoblot analysis on pools of injected and noninjected embryos at
different developmental stages. As shown in Figure 1, the peptide could still be detected in
2- and 3-d-old embryos, indicating the presence of the peptide at times
when electrophysiological measurements were performed. As expected,
noninjected embryos showed no immunoreactivity. The presence of the
control peptide, which contained the corresponding region of an L-type
calcium channel, was also confirmed by immunoblot analysis (data not
shown).
Fig. 1.
Presence of exogenous synprint peptide after early
blastomere injection. Injected and noninjected embryos were collected
at the indicated days, and the soluble fraction of one embryo was loaded into each lane. As a control, 50 and 100 ng of purified synprint
peptide, respectively, were loaded into lanes 7 and 8. Numbers
on the right indicate positions of molecular weight markers (in
kDa). Two gels with identical probes were run in parallel. After
SDS-PAGE, one gel was stained with Coomassie blue to demonstrate even
loading (top panel), whereas the other was
subjected to immunoblotting. Detection of synprint peptide was
performed by enhanced chemoluminescence (bottom
panel). Note the persistence of the peptide 2 d
after injection, which is when all electrophysiological experiments were performed.
[View Larger Version of this Image (62K GIF file)]
Influence of synprint peptide on Ca2+ dependence
of synaptic transmission
Assuming that the injected synprint peptide binds to syntaxin and
SNAP-25 from Xenopus, it should exert its effect by
competing with the native N-type calcium channel. Thus, the fusion
machinery should be dissociated from the channel and therefore located
further away from the source of Ca2+ influx. The
uncoupled fusion complex should experience a lower calcium
concentration and have a lower release probability. To elucidate the
action of the synprint peptide, we studied the effect of different
external calcium concentrations
([Ca2+]e) on transmitter
release. For these experiments nerve cells were stimulated
extracellularly by a monopolar electrode to elicit action potentials,
and the resulting EPSC responses were monitored on muscle cells in the
whole-cell configuration. The influence of different
[Ca2+]e on synaptic transmission for a
control cell is illustrated in Figure 2.
In this experiment, a double pulse was applied every 2 sec with a 50 msec interval between the two pulses. Because of the high variability
of EPSC amplitudes, at least 50 responses were averaged in each calcium
concentration (Fig. 2A). Access resistance in the
muscle cell, which was monitored continuously, was stable throughout
the experiment (Fig. 2A, bottom trace). The amplitude histograms at the different external calcium
concentrations showed a typical Gaussian distribution (not shown),
which was taken as an indicator of a functional, mature synapse.
Fig. 2.
Representative experiment of a noninjected pair of
cells with double-pulse stimulation. A, The top
trace shows the different external calcium concentration
[Ca2+]e (in mM) during the
experiment. The nerve cell was stimulated at 0.5 Hz with a pulse
interval of 50 msec. In the two middle traces the
amplitudes of the EPSCs resulting from the first and second stimulus,
respectively, are displayed. The solid lines indicate
the averaged EPSC amplitude in each
[Ca2+]e. Because of the large
variability, at least 50 responses in each
[Ca2+]e were averaged. The
bottom trace shows the series resistance on the muscle
cell (Rs) throughout the experiment.
B (top), The average EPSCs (10 responses)
in the different external calcium concentrations are displayed.
[Ca2+]e are 0.5, 1.0, 1.8, and 10.0 mM (left to right). The graph below illustrates the dependence of the ratio of 2.EPSC to 1.EPSC on the
external calcium concentration. Note the constant decrease in the ratio
with increasing [Ca2+]e.
C, The dependence of the average EPSC amplitudes (
,
1.EPSC;
, 2.EPSC) on different
[Ca2+]e. Error bars represent
SEM.
[View Larger Version of this Image (28K GIF file)]
The double-pulse protocol also enabled us to examine the effect of
external calcium concentration on paired-pulse facilitation in this
preparation. This form of facilitation occurs when two stimuli are
given in rapid succession and is reflected in a larger amplitude of the
second EPSC, most likely attributable to elevated resting
[Ca2+]i remaining from the first
stimulus. In Figure 2B, the ratios of the amplitudes
of the second and first pulses are plotted against [Ca2+]e. Facilitation was observed in
external solution containing 0.5, 1.0, and 1.8 mM calcium,
being most pronounced in 0.5 mM [Ca2+]e (r = 1.47). In
1.0 and 1.8 mM
[Ca2+]e, the facilitation
declined with ratios of 1.32 and 1.16, respectively. In 10.0 mM [Ca2+]e, we
measured a slight depression with a ratio of 0.91, which is probably
attributable to depletion of the readily releasable pool after the
first stimulus. A qualitatively similar Ca2+
dependence of paired-pulse facilitation was observed for 25 msec pulse
intervals. These data are summarized in Table
1.
Table 1.
Summary of the Ca2+-dependence of relative
synaptic transmission, paired-pulse facilitation (25 msec pulse
interval), and coefficient of variation
|
[Ca2+]e in
mM
|
| 0.5 |
1.0 |
1.8 |
10.0
|
|
| % Transmitter release |
| Control
cells |
22.0 ± 5.4 (7) |
52.5
± 4.6 (8) |
77.3 ± 1.8 (12) |
100 (14)
|
| Synprint (N-type) |
11.6 ± 3.6 (3) |
28.0
± 3.8 (8) |
53.9 ± 3.4 (17) |
100 (19)
|
| LII-III670-800
(L-type) |
ND |
ND |
69.6
± 3.5 (14) |
100 (14) |
-conotoxin
GVIA |
15.5 (1) |
26.0 ± 0 (2) |
50.4
± 4.5 (6) |
100 (6) |
|
| Paired-pulse facilitation
|
| Control cells |
1.60 ± 0.26 (3) |
1.26
± 0.11 (7) |
1.05 ± 0.05 (5) |
0.87
± 0.06 (5) |
| Synprint
(N-type) |
ND |
1.29 ± 0.09 (7) |
1.06
± 0.05 (7) |
0.70 ± 0.05 (7) |
| LII-III670-800
(L-type) |
ND |
1.15 ± 0.08 (5) |
1.08
± 0.09 (5) |
0.72 ± 0.08 (4) |
|
| Coefficient of variation
|
| Control cells |
0.66 ± 0.07 (8) |
0.56
± 0.11 (7) |
0.40 ± 0.04 (14) |
0.35 ± 0.05 (14)
|
| Synprint (N-type) |
0.67 ± 0.06 (4) |
0.81
± 0.08 (8) |
0.54 ± 0.05 (17) |
0.35 ± 0.03 (18)
|
| LII-III670-800 (L-type) |
0.84
± 0.29 (3) |
0.67 ± 0.10 (10) |
0.38
± 0.07 (13) |
0.29 ± 0.05 (13) |
|
Data are presented for control cells (noninjected), cells
injected with synprint (N-type), and control (L-type) peptides and cells treated with -conotoxin GVIA. Errors are given as the SEM; numbers in parentheses indicate the number of experiments. ND, Not
determined.
|
|
An example of the dependence of the EPSC amplitude on
[Ca2+]e is shown in Figure
2C. These results show, as predicted from the classic
studies on the adult neuromuscular junction, that the release is
steeply dependent on [Ca2+]e in the
low calcium range up to 1 mM. When
[Ca2+]e was further elevated to 1.8 and 10.0 mM, saturation of the EPSC amplitude was observed.
A slightly different dependence on the calcium concentration was found
for the second EPSC, which reached its maximal amplitude at 1 mM [Ca2+]e. In 1.8 mM [Ca2+]e, the
amplitude remained at the same level, whereas there was a decrease in
EPSC amplitude in 10.0 mM
[Ca2+]e.
Analysis of 14 noninjected cells illustrated that the absolute EPSC
amplitudes were highly variable between cells (3.65 ± 2.45 nA for
10.0 mM [Ca2+]e).
This variability may reflect the difference in number of terminals
between each pair of cells; however, the dependence on
[Ca2+]e was comparable in all of these
cells. Therefore, to compare between different cells, we normalized the
average EPSC amplitudes to the value measured in 10.0 mM
[Ca2+]e. On average, our experiments
illustrate that for a control synapse the relative release for the
first EPSCs is already close to saturation at 1.8 mM
[Ca2+]e. Increasing the
[Ca2+]e by a factor of >5 (i.e., to
10.0 mM [Ca2+]e)
caused only a 22% increase in EPSC amplitudes (see Fig. 5B; Table 1).
Fig. 5.
Correlation of the action of synprint peptide with
a model of Ca2+-dependent synaptic transmission.
A, Schematic presentation of the assumptions implied in
the model. The Ca2+ concentration at the inner
surface of the membrane reaches its highest value at an open
Ca2+ channel. With increasing distance from a
channel the Ca2+ concentration declines, leading to
the formation of so-called Ca2+ domains. Two classes
of vesicles, linked (i) and nonlinked
(ii), can be distinguished. A linked vesicle senses the
sum of local and surrounding calcium, whereas a nonlinked vesicle
senses just the surrounding calcium. Note that the shape of the
Ca2+ domains is drawn schematically; for the model
calculations (see Results) we assumed a cylindrical shape. Also note
that the line, which indicates the value for the calcium
threshold of synaptic transmission, should be considered arbitrary.
B, Fit of the experimental data with model-derived
curves. Pooled control data (open circles) are best
described if one assumes that 95% of all releasable vesicles are
linked to a Ca2+ channel (solid
curve). For pooled data of cells containing the synprint
peptide (open squares), the model predicts that only 25% of all releasable vesicles remained linked to a
Ca2+ channel (dashed curve). Error
bars represent SEM.
[View Larger Version of this Image (26K GIF file)]
To examine the effect of the synprint peptide on transmitter release,
we used either a single- or a double-pulse protocol on neuromuscular
junctions, the nerve cells of which contained the synprint peptide (as
identified by rhodamine fluorescence). We chose the method of early
blastomere injection because large peptides are difficult to load
through the recording pipette, especially when the distance between
soma and terminal is highly variable (from 20 to 300 µm). A
representative example of a single-pulse experiment is shown in Figure
3. In 1.8 mM
[Ca2+]e, the average EPSC
amplitude was 0.33 nA. Perfusion of the bath with 10 mM
[Ca2+]e caused an increase in the
average EPSC amplitude to 1.1 nA. Again, perfusion with 1.8 [Ca2+]e resulted in a decrease in the
average EPSC amplitude to 0.51 nA, comparable to the initial value.
Changing the solution into low calcium concentration (i.e., 0.5 mM [Ca2+]e) caused
a sharp decrease to 0.2 nA and the appearance of many failures. EPSC
amplitudes recovered after perfusion with 1.8 mM [Ca2+]e. The amplitude histogram in
the different [Ca2+]e showed a typical
Gaussian distribution, like that of the control cell (not shown).
Fig. 3.
Representative experiment on a synapse that
contained the synprint peptide. A, EPSCs resulting from
stimulation of the nerve cell at 1 Hz. The top trace
shows the different external calcium concentration
[Ca2+]e (in mM); the
bottom trace shows the series resistance on the muscle
cell (Rs) during the experiment.
B, Examples of averaged EPSCs at the indicated external
calcium concentrations. C, Comparison of the dependence
of relative synaptic transmission on
[Ca2+]e for control cells and cells
that contained the synprint peptide. For control cells, averaged data
from 14 cells are displayed (for details, see Table 1). The curve for
the synprint peptide is derived from the data shown in A
(for averaged data of peptide-injected cells, see Fig.
5B and Table 1). Error bars represent SEM. Note the
decrease in relative transmitter release under physiological [Ca2+]e for the peptide-injected
cell.
[View Larger Version of this Image (29K GIF file)]
For comparison of the Ca2+ dependence of the
EPSC amplitudes of peptide-injected cells with that of control cells,
amplitudes were normalized to values measured in 10 mM
[Ca2+]e (Fig. 3C). When
[Ca2+]e is raised from 1.8 to 10.0 mM, the EPSC amplitudes increase ~2.5-fold compared with
only a 1.25-fold increase in noninjected cells. An average of 19 peptide-injected cells showed that the relative release in 1.8 mM [Ca2+]e was ~54% of
the values obtained in 10 mM
[Ca2+]e (3.02 ± 2.12 nA).
Double-pulse experiments with 25 msec pulse intervals indicated that
the peptide had no effect on paired-pulse facilitation (Table 1).
We also performed the identical protocol on neuromuscular junctions
injected with the corresponding region of an L-type calcium channel.
This peptide does not bind to syntaxin or SNAP-25 in binding assays,
which correlates well with the mostly postsynaptic localization of this
channel (Ahlijanian et al., 1990
). The relative release at different
external calcium concentrations in the presence of the L-type peptide
was comparable to that of control cells (Table 1), indicating that the
effect of the N-type synprint peptide is specific.
As shown in Figure 2C, the relative transmitter release in
control cells increases only ~20% when the
[Ca2+]e was raised from 1.8 to 10.0 mM. One possible explanation for this phenomenon might be
the saturation of the postsynaptic response. Therefore, we performed
experiments with tetraethylammonium (TEA) and 3,4-diaminopyridine
(3,4-DAP), which block voltage-gated potassium channels and
consequently prolong action potentials. After application of 10-20
mM TEA and 50-100 µM 3,4-DAP to the bath,
the EPSC amplitudes in injected and noninjected cells increased up to
twofold even in 10.0 mM
[Ca2+]e, demonstrating that the
postsynaptic response is not maximal under our experimental conditions
(data not shown). The increase was followed by a diminishing of EPSCs
attributable to blockade of acetylcholine receptors.
We also tested the possibility that the decline in relative release in
control cells is attributable to saturation of the Ca2+ influx through the presynaptic calcium
channels. Recording of single channel currents could prove this;
however, because of the small size of presynaptic terminals, this is
difficult to accomplish. Therefore, we used the calcium indicator dye
fura-2 (Grynkiewicz et al., 1985
) as a probe to measure relative
Ca2+ influx into control terminals with 1.8 mM and 10.0 mM
[Ca2+]e (Neher, 1995
). In addition, it
remained possible that the synprint peptide exerts its effect by
altering Ca2+ influx in 1.8 mM
[Ca2+]e and 10.0 mM
[Ca2+]e. Therefore, we also measured
the relative Ca2+ influx into peptide-loaded
terminals under these [Ca2+]e. A
representative trace of fura-2 measurements in a peptide-loaded terminal is shown in Figure 4. After
whole-cell configuration on the nerve cell soma was established, 100 µM fura-2 was loaded through the pipette and allowed to
equilibrate. This concentration might not fully overcome endogenous
buffer, but it should yield reliable estimates of the relative
Ca2+ influx under different external calcium
concentrations. Trains of ten action potentials at a frequency of 20 Hz
were given, and the resulting change of fluorescence amplitude at 380 nm was measured. The ratio of the changes in fluorescence in 10.0 and
1.8 mM external calcium [
F380 (10.0 mM)/
F380 (1.8 mM)] was 1.8 ± 0.4 (mean ± SD; n = 3) in peptide-injected
terminals, whereas it was 2.0 ± 0.1 (n = 2) in
control terminals. These values indicate that saturation of the
Ca2+ influx through the presynaptic calcium channels
is at least partially responsible for the saturation in relative
release in high [Ca2+]e. They also
show that the effect of the synprint peptide is not attributable to a
change in relative Ca2+ influx at 1.8 and 10.0 mM external calcium, suggesting an action of the peptide
downstream of the triggering event of synaptic transmission.
Fig. 4.
Measurement of the relative
Ca2+ influx in a nerve terminal that contained the
synprint peptide. Fura-2 (100 µM) was loaded through the
pipette on the nerve cell soma and allowed to equilibrate. A, Different external calcium concentrations used during
this experiment. B, C, Fluo-rescence values after
excitation at 350 nm (B, F350) and 380 nm (C,
F380). Shown traces start approximately 12 min after the
whole-cell configuration was established on the nerve cell soma. A
train of 10 action potentials was given at a frequency of 20 Hz. The
relative Ca2+ influx was calculated from the
reduction in fluorescence at 380 nm. For this experiment, the ratio of
F380 at 10 and 1.8 mM
[Ca2+]e was 1.8.
[View Larger Version of this Image (13K GIF file)]
These findings suggest that the synprint peptide exerts its effect by
reducing the efficiency of neurotransmitter release on the presynaptic
side without affecting the Ca2+ influx through the
channels.
Model calculations
We next tried to correlate the action of the synprint peptide with
a simple model of Ca2+-dependent synaptic
transmission. The assumptions included in our model are illustrated in
Figure 5A. We distinguish two
classes of releasable vesicles: (i) vesicles linked to a
Ca2+ channel through the synprint site and
(ii) vesicles that are not linked to a
Ca2+ channel. The first class senses the sum of
[Ca2+]i originating from
Ca2+ influx through the local channel (termed
[Ca2+]l) and through the
channels at some distance (termed
[Ca2+]s), whereas the second
class senses only [Ca2+]i from the
Ca2+ influx through the channels at some distance.
The values for "local calcium"
([Ca2+]l) and "surrounding
calcium" ([Ca2+]s) are given
by:
The factors al and
as scale the relative amplitude of local and
surrounding calcium, respectively. The dependence of the "relative
Ca2+ influx" i as a function of
[Ca2+]e is described by
i([Ca2+]e) = [Ca2+]i,max/(1 + Kd/[Ca2+]e),
with [Ca2+]i,max = 1.0 mM.
The product of [Ca2+]i,max × al determines the maximal
[Ca2+]i added by an open channel at
infinity [Ca2+]e. This value scales
linearly with the Kd of the secretion apparatus. From our fura-2 measurements we estimated a twofold increase of Ca2+ influx between 1.8 and 10.0 mM
[Ca2+]e. Because this is a rather
indirect measurement, we adapted the Kd
(Ca2+ current) of 5.6 mM from a single
channel study on L-type Ca2+ channels by Church and
Stanley (1996)
. This would result in a 2.6-fold increase in
Ca2+ influx between 1.8 and 10.0 mM
[Ca2+]e, which is comparable to
our estimates from fura-2 measurements.
If we assume further that synaptic transmission is proportional to the
quadruply bound state of a calcium binding site, we can now calculate
the amount of release from each class of vesicles by the following
equations:
with pl denoting the probability
of a docked vesicle being linked to a calcium channel.
In Figure 5B, a fit of our pooled experimental data
for control and peptide-injected cells with the model equations is
displayed. We assumed the same Kd values and
cooperativity as for the goldfish bipolar terminal (b = 0.4) (Heidelberger et al., 1994
). As mentioned above, the
Kd values scale linearly with the
[Ca2+]i. Because there are no
Kd values available for this preparation, we
adapted the ones measured from the bipolar nerve terminal. The sharp
saturation of the dose-response curve can be influenced by both the
cooperativity of the calcium binding to the secretion apparatus and the
calcium dependence of the Ca2+ influx. Use of only
one of these parameters results in rather extreme assumptions, whereas
reasonable values for cooperativity (b = 0.4) and the
calcium dependence of the Ca2+ influx (see above)
describe our measured data well. We fixed al and
as at 0.5 and 0.25, respectively, which assumes
that the linked channel contributes twice as much to the local
[Ca2+] as all the other channels together. The
resulting local calcium ([Ca2+]l) predicted by the
model is ~163 µM at 1.8 mM
[Ca2+]e. The best fit for control
cells could be obtained when 95% of the vesicles are linked to a
calcium channel, which correlates well with the reported in
vivo situation in the adult frog neuromuscular junction (Yoshikami
et al., 1989
). For the peptide-injected cells, the model predicts that
only 25% of the vesicles remain linked to a calcium channel after
action of the synprint peptide. The majority of vesicles (70%) has
been uncoupled from a single calcium channel but is still releasable by
increasing the Ca2+ influx through the channels at
some distance. A major assumption of our model is the ratio of calcium
concentrations sensed by linked and nonlinked vesicles. When changing
this ratio from 3:1 to 5:1, the estimate for the fraction of uncoupled
vesicles required for a proper fit is reduced from 70 to 60%. At the
same time, however, the accuracy of the fit is reduced. These
model-derived numbers may not correctly reflect the absolute numbers
in vivo, but they indicate that in peptide-injected cells
the fraction of uncoupled vesicles is larger than the measured
reduction in relative release (Fig. 3C, Table 1). These
results therefore support the conclusion that competition with the
binding region on N-type channel does not prevent synaptic
transmission, but it shifts its Ca2+ dependence to
higher values.
Mimicking the synprint peptide effect with
-conotoxin GVIA
An alternative approach that should mimic the action of the
synprint peptide is the irreversible blockade of a portion of the
calcium channels involved in transmitter release by toxin. In terms of
our model described above, blocking channels will have two effects. (1)
The fraction of blocked channels will no longer contribute to the
Ca2+ influx. This leads to a reduction in
surrounding calcium concentration. (2) A vesicle that is linked to a
blocked Ca2+ channel will be converted to the class
of nonlinked vesicles experiencing only the surrounding calcium.
A vesicle linked to a blocked channel will not be released, if we
assume that the surrounding calcium concentration is below the
threshold to stimulate release (Fig. 6,
bottom left panel). Increasing calcium influx through
the neighboring channels by elevating
[Ca2+]e (i.e., from 1.8 to 10.0 mM), however, will lead to a rise in calcium in the
vicinity of this vesicle and therefore increase its probability of
release (Fig. 6, bottom right panel). We used the
following experimental approach to examine this question.
-conotoxin
GVIA (200 nM), an irreversible blocker of the N-type calcium channel, was applied to the bath, and EPSCs were monitored before and after toxin application. EPSCs were evoked every 2 sec as
described for Figures 2 and 3. Shortly after application of the toxin,
EPSC amplitudes started to decline from 6 to <1 nA (Fig.
7A). Thereafter, excess toxin
was removed by perfusion for 2 min in 10 mM
[Ca2+]e, which led to an
increase in average EPSC amplitude to 1.7 nA. After perfusion with 1.8 mM [Ca2+]e, EPSCs
decreased to 0.86 nA, a reduction to <60% of the average amplitude
recorded in 10 mM [Ca2+]e.
Perfusing again with 10 mM
[Ca2+]e resulted in an increase of the
average amplitude to 2.5 nA. Lowering the external calcium to 0.3 mM caused a remarkable decrease in the amplitude to <0.2
nA, which corresponds to <20% of the average amplitude recorded in 10 mM [Ca2+]e. The pooled
data for the toxin experiments are shown in Table 1; the average
amplitude in 10 mM [Ca2+]e
was 1.55 ± 0.36 nA.
Fig. 6.
Schematic comparison of actions of the synprint
peptide and an irreversible Ca2+ channel blocker.
The top panel illustrates the proposed action of the
synprint peptide, starting from the situation in the uninjected neuromuscular junction where both shown vesicles are linked to a
certain Ca2+ channel (left). The
solid lines represent the Ca2+
domains in 1.8 mM
[Ca2+]e; the horizontal,
dotted line indicates an assumed calcium threshold. After
opening of the Ca2+ channels, both vesicles would be
released. After action of the synprint peptide (right),
a vesicle was uncoupled from a Ca2+ channel. In 1.8 mM [Ca2+]e, only
one vesicle would be released, resulting in a reduction of EPSC
amplitude. Rising [Ca2+]e from 1.8 to
10.0 mM (dashed lines), however, would
release both vesicles. In the bottom panel, the action
of an irreversible Ca2+ channel blocker, e.g.,
-conotoxin GVIA, is illustrated. In the situation on the
left, the toxin has blocked one of the
Ca2+ channels. EPSC amplitude would be reduced in
1.8 mM [Ca2+]e
(solid lines), because the linked vesicle at the blocked
channel would not be released. Rising
[Ca2+]e from 1.8 to 10.0 mM (dashed lines) would again release both vesicles because of the increased Ca2+ domain of the
open Ca2+ channel.
[View Larger Version of this Image (22K GIF file)]
Fig. 7.
Ca2+ dependence of EPSC
amplitudes after blockade of a fraction of Ca2+
channels by
-conotoxin GVIA. A, EPSCs resulting from
stimulation of the nerve cell at 0.5 Hz.
-conotoxin GVIA (200 nM) was applied (indicated by the bar),
leading to a decrease in EPSC amplitude. After washout of the toxin, a
stable fraction of Ca2+ channels remained blocked.
The top trace shows the different external calcium
concentration [Ca2+]e (in
mM); the bottom trace shows the series
resistance on the muscle cell (Rs) during the
experiment. B, Examples of averaged EPSCs at the
indicated external calcium concentrations. Note that the shape of EPSCs
remained unaltered by the blockade of Ca2+ channels.
C, Comparison of the dependence of relative transmitter release on [Ca2+]e for control
synapses and synapses that had been treated with
-conotoxin GVIA.
For both types of synapses, averaged data of different cells are
displayed (for details, see Table 1). Pooled control data (open
circles) are best described if one assumes that 95% of all
releasable vesicles are linked to a Ca2+ channel
(solid curve). The Ca2+ dependence of
synapses treated with
-conotoxin GVIA (open squares) is predicted by the model, if it is assumed that 60% of the
Ca2+ channels have been blocked (dashed
curve). Error bars represent SEM.
[View Larger Version of this Image (29K GIF file)]
Comparison of the relative amplitudes in the toxin experiment with
those of the control cells reveals that the dependence on external
calcium is very different (Fig. 7C). On the other hand, the
toxin curve is very similar to the one obtained in peptide-loaded neurons, showing a higher dependence of synaptic transmission on
external calcium. It also correlates well with the assumption that
transmitter release in the case of blocked channels could be partially
restored by increasing [Ca2+]e from
1.8 to 10.0 mM. It is difficult, however, to calculate the
percentage of blocked channels from the relative decrease in release,
because the relation between calcium concentration and release is not
linear. To use our model to estimate the portion of blocked channels,
we introduced pnb as the probability of a channel not being blocked. Although the value for local calcium ([Ca2+]l) would not be
influenced, that of surrounding calcium
([Ca2+]s) would then be given
by:
The amount of release for each class of vesicles would then be
calculated with the following equations:
For the toxin simulation we used the same assumptions as for
the control cells (95% of the vesicles are docked, and the ratio between local calcium and surrounding calcium is 3:1). According to the
simulation, block of 60% of the channels would account for an expected
inhibition of 80% in relative transmitter release (Fig.
7C).
Thus, the experimental data as well as our model calculations suggest
that uncoupling a vesicle from the calcium channel through the action
of the synprint peptide or alternatively blocking a fraction of the
channels irreversibly will lead to a similar change in the calcium
dependence of synaptic transmission.
DISCUSSION
We have demonstrated that injection of peptides containing the
soluble NSF attachment protein receptor (SNARE) protein-binding region
of N-type Ca2+-channels changes the
Ca2+-dependence of transmitter release in cultured
frog neuromuscular junctions. This effect is most pronounced under
physiological conditions, i.e., in external solution containing 1.8 mM calcium. Our findings support the in vitro
binding data (Sheng et al., 1994
), which revealed an interaction of the
N-type but not the L-type calcium channel with syntaxin and SNAP-25
through that synprint site. They are also consistent with the data on
rat superior cervical ganglion neurons (Mochida et al., 1996
), in which
a maximum of 42% inhibition of synaptic transmission was observed
after diffusion of synprint peptide.
Our results further show that the effect of the synprint peptide is
attributable to neither reduced relative Ca2+ influx
into the terminal nor saturation of the postsynaptic response. It has
been reported that coexpression of syntaxin with L-, Q- and N-type
calcium channels in Xenopus oocytes resulted in a decrease of calcium influx through these channels because of stabilization of
the inactivated state (Bezprozvanny et al., 1995
; Wiser et al., 1996
),
but this effect was not observed in isolated chick ciliary ganglion
nerve terminals (Stanley and Mirotznik, 1997
). If syntaxin inhibits
Ca2+ channel function in our preparation, disruption
of the native syntaxin/channel-interaction by the synprint peptide
would therefore lead to an increase in Ca2+ influx
and consequently to an underestimation of the physiological effect. Our
fura-2 measurements indicate that the ratio of relative Ca2+ influx into injected and control terminals at
1.8 and 10.0 mM external calcium is virtually identical
(see Results). Because we do not measure the absolute
Ca2+ influx at a given calcium concentration, an
equal increase in influx into injected terminals in both 1.8 and 10.0 mM [Ca2+]e still remains
possible.
The model calculations in Figure 5 suggest that the observed 25%
reduction in relative release in 1.8 mM external calcium corresponds to an uncoupling of ~70% of the formerly linked vesicles by the synprint peptide. The fast, Ca2+-dependent
synaptic transmission at this neuromuscular junction is entirely
blocked by application of the N-type-specific
-conotoxin GVIA
(Yazejian et al., 1997
), but the toxin blocks Ca2+
influx and increases the number of vesicles linked to blocked channels,
so it reduces Ca2+ at both coupled and uncoupled
vesicles. One possible explanation for the vesicle fraction remaining
linked to a calcium channel would be the incomplete action of the
synprint peptide. We consider this possibility not very likely, because
varying the amount of injected peptide over a wide range did not
markedly change the effect, suggesting that the peptide was already
present in excess. Rather, the vesicle fraction remaining linked to a
calcium channel might be attributable to the high density of calcium
channels in the active zones of the frog neuromuscular junction (Heuser and Reese, 1981
; Robitaille et al., 1990
). The effect of moving vesicles away from local channels would then reach a maximum of reduction in transmitter release, after which the
Ca2+ influx through surrounding channels is high
enough to exceed the threshold of release.
Our model calculations also provide an explanation for the already high
relative transmission of control cells in 1.8 mM external calcium concentration. If indeed almost all vesicles are linked to a
local channel in this preparation, only minimal Ca2+
influx is needed to release them. The short distance between the
channel as the Ca2+ source and the
Ca2+ sensor of release would give endogenous calcium
buffers little time to remove the high calcium at the inner mouth of
the channel and consequently increase the probability of transmitter
release. This assumption is supported by biochemical data that
identified the Ca2+ binding protein synaptotagmin as
an integral member of the SNARE-complex (for review, see Südhof,
1995
).
In conclusion, our data further underscore the physiological importance
of the interaction between presynaptic Ca2+ channels
and members of the docking and fusion machinery. Interruption of this
physical link does not prevent synaptic transmission, but makes it less
probable by shifting its Ca2+ dependence to higher
values.
FOOTNOTES
Received May 9, 1997; revised June 17, 1997; accepted June 20, 1997.
This work was supported in part by Grants of the Deutsche
Forschungsgemeinschaft (J.R.), a predoctoral fellowship from Boehringer Ingelheim Fonds (C.H.), a postdoctoral Feodor Lynen-Minerva fellowship (U.A.), research Grant NS 22625 from National Institutes of Health (W.A.C.), a postdoctoral fellowship of the National Institute of Mental
Health (Z.-H.S.), and a predoctoral fellowship from National Institutes
of Health Training Grant T32 GM07108 (C.T.Y.). We thank Dr. Alan
Grinnell and members of his laboratory for their kind hospitality and
advice.
J.R., C.H., and U.A. contributed equally to this work.
Correspondence should be addressed to Dr. E. Neher at the above
address.
Dr. Sheng's present address: Synaptic Function Unit, National
Institutes of Health, Bethesda, MD 20892.
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