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The Journal of Neuroscience, September 15, 2002, 22(18):7968-7981
Rac GTPase Plays an Essential Role in Exocytosis by Controlling
the Fusion Competence of Release Sites
Yann
Humeau1,
Michel R.
Popoff2,
Hiroshi
Kojima1,
Frédéric
Doussau1, and
Bernard
Poulain1
1 Neurotransmission et Sécrétion
Neuroendocrine, UPR2356 du Centre National de la Recherche
Scientifique, IFR-37 des Neurosciences, F-67084 Strasbourg Cedex,
France, and 2 Toxines Microbiennes, Institut
Pasteur, F-75724 Paris Cedex 15, France
 |
ABSTRACT |
The role of small GTPases of the Rho family in synaptic functions
has been addressed by analyzing the effects of lethal toxin (LT) from
Clostridium sordellii strain IP82 (LT82) on
neurotransmitter release at evoked identified synapses in the buccal
ganglion of Aplysia. LT82 is a large
monoglucosyltranferase that uses UDP-glucose as cofactor and
glucosylates Rac (a small GTPase related to Rho), and Ras, Ral, and Rap
(three GTPases of the Ras family). Intraneuronal application of LT (50 nM) rapidly inhibits evoked acetylcholine (ACh) release as
monitored electrophysiologically. Injection of the catalytic domain of
the toxin similarly blocked ACh release, but not when key amino acids
needed for glucosylation were mutated. Intraneuronal application of
competitive nucleotide sugars that differentially prevent glucosylation
of Rac- and Ras-related GTPases, and the use of a toxin variant
that affects a different spectrum of small GTPases, established that
glucosylation of Rac is responsible for the reduction in ACh release.
To determine the quantal release parameters affected by Rac
glucosylation, we developed a nonstationary analysis of the
fluctuations in postsynaptic response amplitudes that was performed
before and after the toxin had acted or during toxin action. The
results indicate that neither the quantal size nor the average
probability for release were affected by lethal toxin action. ACh
release blockage by LT82 was only caused by a reduction in the number
of functional release sites. This reveals that after docking of
synaptic vesicles, vesicular Rac stimulates a membrane effector (or
effectors) essential for the fusion competence of the exocytotic sites.
Key words:
Aplysia; synapse; exocytosis; quantal
parameters; synaptic vesicle fusion; Rho-GTPases; clostridial toxins; fluctuation analysis
 |
INTRODUCTION |
Rho proteins (Rho, Rac, Cdc42) are
widely expressed monomeric GTPases. They cycle between a soluble,
GDP-bound inactive state and a membrane-associated GTP-bound state that
stimulates downstream effectors. The effectors include protein kinase
N, Rho-kinase, the myosin-binding subunit of myosin phosphatase,
several phosphatidylinositol protein kinases (PI3-kinase, PI4-kinase,
PI5-kinase), and phospholipase C and phospholipase D (PLD). Despite the
ubiquitous distribution of cytosolic Rho-GTPases, their translocation
to specific membrane domains allows them to intervene in distinct
biological functions such as regulation of actin cytoskeletal dynamics,
cell cycle progression, gene transcription, and membrane transport
(Hall, 1998 ; Bishop and Hall, 2000 ; Ridley, 2001 ). Recently, Rho, Rac, and Cdc42 have been implicated in the regulation of neuronal
morphogenesis (axonal guidance, maintenance of dendritic spines and
branching) (Luo, 2000 ; Nakayama et al., 2000 ; Dickson, 2001 ; Liu and
Strittmatter, 2001 ; Redmond and Ghosh, 2001 ), control of
neurotransmitter-receptor density (Meyer et al., 2000 ), and induction
of neuronal apoptosis (Linseman et al., 2001 ; Mota et al., 2001 ). Our
previous findings that RhoA, RhoB, Rac1, and Cdc42 are present in nerve
terminals and that Rac1 is associated with synaptic vesicles (SVs)
(Doussau et al., 2000 ) have suggested that these GTPases may also play a role in neurotransmitter release.
The cellular function of endogenous Rho and Ras proteins can be acutely
manipulated by using bacterial protein toxins that modify and
inactivate them in a highly specific manner (Busch and Aktories, 2000 ;
Just and Boquet, 2000 ). Clostridium sordellii lethal toxin
(LT) glucosylates a conserved threonine in the effector domain of Rac
(which is related to Rho), and Ras, Rap, and Ral, (which are members of
the Ras family). LT variants have been reported to also affect Cdc42.
When glucosylated, the Rho-GTPases can associate with target membranes
but cannot activate their effectors, thereby silencing the downstream
pathways (Just et al., 1996 ; Popoff et al., 1996 ; Busch and Aktories,
2000 ; Just and Boquet, 2000 ).
We have found previously that intraneuronal injection of LT or toxins
that glycosylate or ADP-ribosylate Rho-related GTPases blocks
acetylcholine (ACh) release at Aplysia synapses (Doussau et
al., 2000 ). This indicates that members of the Rho family play a role
in neurotransmitter exocytosis and extends to neurons the idea that
Rho-related proteins control secretion mechanisms (Prepens et al.,
1996 ; Kowluru et al., 1997 ; Brown et al., 1998 ; Gasman et al., 1998 ,
1999 ; Djouder et al., 2000 ; Hong-Geller and Cerione, 2000 ; Guo et al.,
2001 ).
To identify the key GTPase(s) whose inactivation is responsible for the
LT-blocking action on ACh release, we have investigated the causal
relationship between the glycosylating activity of two LT variants that
each affect a distinct set of GTPases and inhibition of
neurotransmitter release at identified Aplysia synapses. We
found that ACh release blockage is caused by glucosylation of Rac
GTPase. To determine the release step(s) altered after LT application,
we analyzed the fluctuations in postsynaptic response amplitudes before
and during LT-induced blocking action. Our results show a decrease in
the number of active release sites, but quantal size and release
probability are unaltered. This reveals that the Rac-mediated pathway
is implicated in the activation of release sites.
 |
MATERIALS AND METHODS |
Preparation of toxins and determination of their
glucosylating activity
The toxins were purified from C. sordellii IP82
(LT82) and VPI9048 (LT9048) strains as described previously (Popoff,
1987 ). The DNA coding for the 546 N-terminal amino acids, which
contain the enzymatic site (Hofmann et al., 1998 ), was amplified
by PCR from C. sordellii IP82 strain. Primers were taken
from the LT gene sequence (Green et al., 1995 ), and xSalI
and XhoI sites were added at the 5' and 3' ends of the
coding sequence, respectively. The resulting PCR DNA fragment
was cloned into the corresponding sites of pET28b (Novagen). The
plasmid was transformed into the Escherichia coli BL21
strain, and production of the 6 His-tag fusion protein was induced with
isopropyl-1-thio- -D-galactopyranoside. Purification was performed with a cobalt column (Novagen) according to
the recommendations of the manufacturer. An inactive mutant of the LT82
N-terminal part (Ala-286-Asp, Ala-288-Asp) was prepared as described
previously (Busch et al., 1998 ), and the protein was produced and
purified as mentioned above.
Recombinant small GTPases were produced in E. coli, purified
with glutathione-Sepharose 4B (Amersham Biosciences), and prepared by
thrombin digestion according to the recommendations of the manufacturer. Rho, Rac1, and Cdc42 clones were a generous gift from Dr.
Alan Hall (London, UK). H-Ras, Rap1a, and RalC clones were kindly
donated by Dr. Robert Cool (Max Plank Institute, Dortmund, Germany).
In vitro glucosylation of small GTPases was performed in 50 mM triethanolamine, pH 7.5, containing 2 µl of
UDP-14C-glucose (DuPont NEN; 286.2 mCi/mmol; final concentration 7 µM), 2 mM MgCl2, 1 mM DTT, 0.3 mM GDP, 1 µg
of recombinant GTPase, and 5 µg/ml LT82, LT82 recombinant fragment,
or LT9048. The reaction was performed for 1 hr at 37°C and stopped by
adding 10 µl of sample buffer (three times) followed by boiling for 3 min. Then samples were electrophoresed on a 15% SDS-PAGE and
autoradiographed. When necessary, UDP-mannose, ADP-glucose, and
TDP-glucose (Sigma) were used to prevent glucosylation.
Detection and glucosylation of small GTPases in Aplysia
Aplysia californica (70-120 gm body weight; Marinus
Inc., Long Beach, CA) were anesthetized by injection of 50-75 ml of
solution containing 400 mM
MgCl2, and the nervous system was removed.
Freshly dissected nerve ganglia (buccal, cerebral, pleural, pedal, and abominal) were homogenized in Tris buffer containing 10 mM Tris, pH 7.5, 2 mM
MgCl2, 1 mM DTT, 10 µg/ml
leupeptin, 1 µM pepstatin, and 0.1 mM PMSF. Complete lysis was achieved by three
cycles of freeze thawing.
Detection of Aplysia GTPases. Total
proteins were extracted in Tris buffer containing 1% Triton X-100 for
20 min at room temperature. For Western blotting, samples containing 20 µg Aplysia proteins were subjected to SDS-PAGE on 15%
gels, transferred to nitrocellulose, and incubated with a 1:50 dilution
of antibodies against small GTPases in PBS-milk at room temperature for
16 hr. Polyclonal rabbit antibodies against Rho, Ras, Rap, and Ral were from Santa Cruz Biotechnology; anti-Rac1 was from Upstate
Biotechnology. Polyclonal rabbit antibodies directed against Cdc42 were
kindly provided by Dr. Philippe Chavrier (Institut Curie, Paris,
France). Immunoblots were processed with peroxidase conjugate and
chemiluminescence kit (ECL, Amersham) and analyzed by autoradiography.
Glucosylation of Aplysia GTPases. Lysates
were centrifuged (15,000 rpm for 15 min) to separate a pellet
containing membrane fractions [denoted as insoluble (I) fraction] and
a fraction containing cytosolic and crude vesicle fractions [denoted
as soluble (S) fraction]. The pellet was washed four times with
distilled water and extracted with the buffer described above, but
containing 1% Triton X-100, for 20 min at room temperature. Total
proteins were assayed using a manufactured protein assay (Bio-Rad Life Science, Marne la Coquette, France). Glucosylation was performed on
samples (100 µg protein) of the soluble and insoluble fractions as
described above.
Acetylcholine release and electrical recordings at
Aplysia synapses
Electrophysiological experiments were performed at identified,
chloride-dependent, inhibitory cholinergic synapses in dissected buccal
ganglia of Aplysia as described previously (Poulain et al.,
1986 , 1988 ; Schiavo et al., 1992 ; Doussau et al., 1998 , 2000 ; Humeau et
al., 2001a ,b ). Two presynaptic cholinergic interneurons termed B4 and
B5 (Gardner, 1971 ) and one postsynaptic neuron (either B3 or B6) were
impaled with two glass microelectrodes (3 M KCl, Ag/AgCl2, 2-10 M ). To initiate action potentials and evoke ACh release, the presynaptic neurons were depolarized by a square pulse of
50 msec duration and appropriate intensity. To avoid overlap of the
postsynaptic responses originating from the two B4 and B5 presynaptic
neurons, the stimulus protocols were alternated, and each presynaptic
neuron was stimulated every 40 sec (0.025 Hz).
Evoked ACh release was monitored by measuring the amplitude of the
evoked IPSCs using the conventional two-electrodes voltage-clamp technique (AxoClamp2B, Axon Instruments). The postsynaptic currents are
purely chloride dependent (Gardner and Stevens, 1980 ; Simonneau et al.,
1980 ; Kehoe and McIntosh, 1998 ). Moreover, to measure accurately
the amplitude of the postsynaptic response, the holding potential
Vh was maintained at 30 mV above the
reversal potential of postsynaptic responses,
Vrev.
Vrev was determined every 5 min. The
recordings were digitized at 40 kHz and filtered at a cutoff frequency
of 250 Hz using an eight-pole low-pass Bessel type filter (902LPS,
Frequency Device).
To express the amplitude of the IPSC as a value proportional to the
amount of released ACh but independent of the driving force for
Cl , the IPSC amplitude was converted as
an apparent membrane conductance (G) by taking into
account the reversal potential Vrev
(at these synapses, Vrev = ECl ) of the evoked response
according to the equation G = I/(Vh Vrev). However, although the
postsynaptic response amplitude has the dimension of a membrane
conductance, we refer to it in this paper as the IPSC amplitude,
I (nanosiemens).
Extracellular media
Dissected buccal ganglia were maintained at 22°C using a
Peltier-plate system and superfused continuously (10 ml/hr) with a
physiological medium containing (in mM): NaCl 460, KCl 10, CaCl2 43.8, MgCl2 76.2, MgSO4 28, Tris Buffer 10, pH 7.5. This high concentration in divalent cations was used to minimize spontaneous neuron firing activity as described (Humeau et al., 2001a ). This medium
corresponds to an extracellular
[Ca2+/Mg2+]
ratio of 0.42. To change
[Ca2+]e, the
extracellular
[Ca2+/Mg2+]
ratio was modified by changing the concentrations of
CaCl2 and MgCl2 but not
that of MgSO4 (to keep the sulfates unmodified), as described previously (Doussau et al., 1998 ; Humeau et al., 2001a ).
Intraneuronal injection procedure
Injection electrodes were pulled from glass tubing without a
capillary and contained a silver wire to allow the electrophysiological monitoring of the impalement. Samples to be injected were mixed with a
vital dye (fast green FCF, 10% v/v; Sigma) as detailed elsewhere (Poulain et al., 1986 ; Doussau et al., 1998 ; Humeau et al.,
2001a ). The samples were air pressure-injected using a picopump PV820
(World Precision Instruments) under visual and electrophysiological
monitoring. The injected volume was in the range of 1-2% of the cell
body volume. Therefore, assuming a homogenous distribution of the
injected material, the final intraneuronal concentration was ~1% of
that in the injection micropipette. After injection, the micropipette
was removed carefully, and only presynaptic neurons with no alterations
in action potentials and with membrane potentials between 60 and 45
mV were analyzed. The time of injection is denoted in most experiments
as time zero. In several sets of experiments, we verified that the
various buffers used for dissolving toxin samples had no effect on
neurotransmitter release.
Determination of IPSC amplitude and rise and decay times
IPSC amplitude (I) was determined as the peak
current of recorded IPSC. The time to rise from 20 to 80% of the
maximal IPSC amplitude was determined and denoted as "IPSC rise
time." IPSC rise times were determined from at least 10 IPSCs
recorded under the same experimental condition and averaged. The IPSC
decay time constant was determined by fitting the IPSC with
multi-exponential regression I(t) = Ipeak*[w1*exp( t/ 1) + w2*exp( t/ 2)],
in which 1 and 2 are
the time constants and w1 and
w2 are the respective weights of the
two components. In nearly all experiments analyzed,
w1 1 and
w2 0, indicating single
exponential decay for IPSCs.
Estimation of the quantal parameters: theoretical aspects
In brief, consider the synaptic inputs attributable to the
multiple contacts between a presynaptic neuron and its postsynaptic target and consider the three parameters: q, the amplitude
of elementary postsynaptic response, n, the mean number of
independent release sites, and p, the mean release
probability at these sites. First, we assume that at each release site
p is the product of the output probability
po (i.e., the probability for a
release-ready SV to fuse in response to presynaptic stimulus) and the
probability pA that the site is eligible
for release (i.e., that a primed SV is available for release)
(Brown et al., 1976 ; Zucker, 1989 ; Quastel, 1997 ; Scheuss and Neher,
2001 ). Second, we assume that release probability and quantal size are
uniform, that quanta sum up linearly, and that quantal release follows
a simple binomial distribution. Therefore, following these assumptions,
the average amplitude of IPSC is given by following equation:
|
(1)
|
and the fluctuations of the responses around the mean have a
variance:
|
(2)
|
Similar to the ion channel analysis developed by Sigworth
(1980) , the analysis of the Var = f(Imean) relationship when
the release probability is experimentally modified permits an
evaluation of the quantal parameters n and q
(Quastel, 1997 ; Silver et al., 1998 ; Reid and Clements, 1999 ;
Oleskevich et al., 2000 ; Clements and Silver, 2000 ; Meyer et al., 2001 ;
Scheuss et al., 2002 ). Although this does not allow separate
evaluations of pA and
po (Scheuss and Neher, 2001 ),
modifications of the product
po*pA
= p can be detected. The simple binomial model of
synaptic transmission predicts a parabolic relationship between Var and
f(Imean). Indeed, this relationship can be reexpressed as a function of
Imean:
|
(3)
|
which can be fitted by a simple parabola of equation:
|
(4)
|
This allows determination of two parameters: A, the
initial slope of the parabola, and B, the extent factor of
the parabola. Parameter A refers to q. However
quantal variability (denoted as CVq,
CV being the variation coefficient) also contributes to Var.
Therefore, A provides an overestimate of q
(Silver et al., 1998 ; Reid and Clements, 1999 ; Oleskevich et al., 2000 ,
Scheuss and Neher, 2001 ):
|
(5)
|
Parameter B refers to 1/n.
However, probability parameters
po and pA are
heterogeneous between the release sites at vertebrate synapses
(Rosenmund et al., 1993 ; Murthy et al., 1997 ), and this is also likely
to be the case at Aplysia synapses. Therefore, 1/B underestimates n according to equation:
|
(6)
|
in which, CVp is the average
variation of
po*pA and
CVq inter is the
fraction of quantal variance attributable to intersite variability
(Brown et al., 1976 ; Silver et al., 1998 ; Meyer et al., 2001 ; Scheuss
and Neher, 2001 ).
Determination of Imean and Var:
practical aspects
Stationary conditions. When under a given
experimental condition the amplitude of the IPSCs was stable with time
(i.e., during control recordings or when ACh release was stable after a
change in extracellular
[Ca2+/Mg2+]
or stimulation frequency), Imean and
Var were calculated directly from the IPSC amplitude values determined
in recording epochs of at least 25 IPSCs. Because background noise can
contribute to Var, its variance, Varnoise,
was calculated from the baseline fluctuations in IPSC recordings, and
subtracted from Var. Then the Var = f(Imean) plots were constructed.
Nonstationary conditions. When IPSC amplitude does not
stabilize, determination of Imean and
Var can be performed by nonstationary analysis, as reported previously
for analysis of channel fluctuations during the course of evoked
postsynaptic responses (Robinson et al., 1991 ; Traynelis et al., 1993 ).
In essence, the aim of the nonstationary analysis is to determine
Imean at each time of
I = f(t) plot. The result of
subtracting the set of Imean to
I = f(t) plot generates the set
of the fluctuations of I data around Imean, the variance of which is then
determined. The accurate determination of
Imean is critical for Var
determination. In the earlier studies of Robinson et al. (1991) and
Traynelis et al. (1993) , Imean was
approximated by the mean of fitting procedures or by averaging the
recorded postsynaptic responses. We could not use this latter approach
because each experiment had a unique time course, which could not be
adjusted by simple mathematical equations. As an alternative, we
estimated Imean at each time t of the I = f(t)
plots as follows: I = f(t) plots
were submitted to local linear fitting using a modified built-in
procedure of SigmaPlot5 software (SPSS Inc., Chicago, IL) based on
least squared estimation of parameters. The local linear fitting was
performed on a window of w data (Fig.
1A,B,
straight line into brackets) and repeated for the
whole data range by moving the window by a step of one IPSC data. The
mid-value of each local fit was considered as the estimate of
Imean at the corresponding time. The
set of Imean fits the
I = f(t) plot (Fig.
1B, solid line with small black dots). The result of subtracting the set of
Imean to I = f(t) plot (I Imean) shows fluctuations around the
zero level. I Imean
values are denoted by I in Figure 1C.
The variance, Var, of these fluctuations was then calculated in a
window of W data that was moving, with a step of one,
along the whole data range to be analyzed. Var was corrected for
background noise variance (Varnoise) (see above).
Then, the Var = f(Imean) plots were
constructed (Fig. 1D).

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Figure 1.
Determination of quantal parameters by
nonstationary analysis as tested on a simulated experiment.
A, IPSC amplitude = f(t) values ( ) were calculated
as the product binomial (n,
pt)*q in which
n = 600 sites and q = 2 nS. A
sigmoid decrease of release probability p = po*pA with
time, t, was simulated using equation
pt = 0.8/[1 + exp( (t 20)/ 3.5)0.5]. The solid
line denotes the set of the Imean
values determined at each t (for details see Materials
and Methods). B, Magnification of box
shown in A. The window width used for local linear
fitting (w) is indicated within
brackets (here w = 9). Linear fit is
indicated by solid straight line. The mid-values of the
local linear fits are the estimates of Imean
and are indicated by small dots on a solid
line. C, Fluctuations in IPSC amplitude are
approximated at each time t of the I = f(t) plot, by subtracting
Imean from corresponding I
value ( ). The Imean values determined by
nonstationary analysis deviate from the true
Imean. This difference was determined by
subtracting the determined Imean values from
the predicted Imean and is represented by a
solid thick line. The brackets denote the
window width W used for Var determination (here
W = 16). D, The corresponding
Var = f(Imean)
plot. Solid line denotes the adjustment of the data by
simple parabola (Eq. 4). The predicted parabola (dashed
line) was calculated using Equations 1 and 2 and the
above-mentioned quantal parameters. The difference between both
parabolas generates errors in the determinations of q
and n. The extent of this error can be minimized by
optimizing the window width (w) used for local
linear fitting of IPSC = f(t). Error in estimation of
q is shown in E
[ q(%)] as a function of w, for two
"experimental" conditions: when simulated IPSC amplitude decreases
rapidly (t1/2 = 25 min) or slowly
(t1/2 = 75 min). These situations are
denoted by and , respectively. For these two conditions, optimal
w values are indicated by arrows.
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For each experiment analyzed, the width of the windows used for linear
local fitting (w) and the variance calculation
(W) needed to be adapted to the kinetics of the IPSC
amplitude changes. Indeed, except in the case of a linear change in
IPSC amplitude, when the window (w) used for local linear
fitting is too wide, the local fit deviates from the actual
Imean, and this results in an
overestimation of Var (i.e., the problem of fitting a curve with a
straight line); in contrast, when w is too narrow, the local
fit adapts to local fluctuations but leads to an underestimation of
Var. The window width used for variance calculation, W,
depended also on the kinetics of IPSC amplitude changes. Here, when the window is too wide, Var is calculated from the fluctuations in amplitude of IPSCs corresponding to very different mean amplitude, and
the Var = f(Imean)
plot is significantly distorted. To determine the
W and w to be used, experiments in which
either product of po*pA,
n or q was changed were simulated. They were
submitted to the nonstationary analysis described above. The most
appropriate w and W were determined as those
minimizing the deviation of estimated quantal parameters from the
parameters used for simulation. For the faster changes in IPSC
amplitude (such as those caused by a rapid fall in extracellular
[Ca2+/Mg2+]),
a good compromise was to use w = 9 or 11 data and
W = 15-17 (Fig. 1E). For slower IPSC
changes, w and W were increased. Even in these
conditions, there was a remaining deviation of overall estimate of
Imean (as determined by local moving
linear fitting) with the true Imean
(as calculated by the equation that we used to simulate IPSC amplitude
change). This is illustrated by the thick dotted or
hatched line in Figure 1C. A consequence of this deviation was that the Var = f(Imean) plots were fitted
by parabolas (Fig. 1D, solid line) that
were not exactly superimposable onto the theoretical calculated
parabolas (Fig. 1D, dashed line). The uncertainty in the determination of parabola parameters A
and B in the faster experiments was ~10%, whereas in
slower experiments this error remained marginal.
Parabola adjustment and determination of quantal parameters
at Aplysia synapses
Var = f(Imean)
plots were fitted by Equation 4 constrained to pass the origin using a
built-in procedure of SigmaPlot5 software. The coefficient of
determination r2 is reported in the
Figures or corresponding text to indicate how good the fit is.
CVq was not determined in this study
because of the difficulty in distinguishing miniature events issuing
from B4 or B5 presynatic neurons from the inhibitory inputs caused by
the many other presynaptic neurons, and
CVp was not estimated. Therefore, to
provide insights on possible changes in q, we determined the
parabola fitting parameter A (see Eq. 5), and B
provides an estimate of 1/n (see Eq. 6). According to
Equation 1,
po*pA = Imean/(n*q), and
we calculated its approximation, P, according to the
equation:
|
(7)
|
P differs from actual values of average release
probability
po*pA by the
contribution of quantal variability and probability variability (Eq. 5, 6).
If not stated otherwise, results are presented as means ± SEM.
When appropriate, the significance was tested by the paired or unpaired
Student's t test.
 |
RESULTS |
Effect of the intraneuronal injection of lethal toxin from
C. sordellii on evoked ACh release
To restrict the action of the toxin to a single presynaptic
element, LT82, which in vitro glucosylates recombinant Ras,
Rac, Ral, and Rap but not Cdc42 and Rho, was pressure injected into either B4 or B5 cholinergic neurons to give a final intraneuronal concentration of ~50 nM. This induced a rapid
decrease in IPSC amplitude, indicating inhibition of ACh release (Fig.
2A-C). No inhibition of ACh release was detected with the noninjected control neurons (Fig. 2A,C). In all
experiments, the inhibitory action of LT manifested after an average
delay of 15.2 ± 3.9 (SD, n = 53) min after the
injection. This may represent the time needed for LT molecules
[molecular weight (MW) ~250 kDa] to diffuse up to the nerve
terminals that are distant by 300-500 µm from the presynaptic soma.
This delay is comparable with that (5-10 min) observed for tetanus and
botulinum neurotoxins (MW ~150 kDa) at the same synapses (Poulain et
al., 1988 ; Schiavo et al., 1992 ).

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Figure 2.
Inhibition of evoked ACh release by LT toxins that
inactivate small GTPases. A, A representative experiment
is illustrated. ACh release was evoked at identified synapses in the
buccal ganglion of Aplysia californica. See
inset for a schematic drawing of the neuronal
connections. The amplitude of the IPSCs (percentage of average IPSC in
control period) is plotted against time, before and after pressure
injection of lethal toxin from C. sordellii
(LT) into one of the two presynaptic cholinergic
neurons ( ). The final concentration of LT in the cell body was ~50
nM. The second presynaptic neuron ( ) was not injected.
B, Recordings of presynaptic action potentials and IPSC
at the time indicated before and after injection of LT. The mean IPSC
amplitude (C) and mean percentage changes in the
IPSC rise time and decay time (D, E) were
determined 180 min after the time of toxin injection for noninjected
(open bars) and LT82-injected (filled
bars) neurons and normalized with respect to the mean values
observed before the time of toxin injection. The number
of experiments is indicated. C-E, ** denotes
significant difference (p < 0.001) as
compared with the controls; other comparisons are nonsignificant
(p > 0.5).
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Typical recordings, illustrated in Figure 2B, exhibit
no detectable alteration in the action potentials recorded in the
injected neurons at a time when IPSC amplitude was strongly depressed. This suggests that the inhibitory action of LT on ACh release does not
result from an alteration in presynaptic membrane excitability. We also
found no change in either the IPSC rise or decay time after LT had
exerted its blocking action (Fig.
2D,E). This latter finding
indicated that release kinetics and synchronization of released quanta
remained unchanged after LT action.
Blocking of ACh release needs an LT intact catalytic site
The impressive blocking action of LT (Fig.
2A,C) was comparable, on a molar
basis, to that produced by intraneuronal application of tetanus or
botulinum neurotoxins (Poulain et al., 1988 ; Schiavo et al., 1992 ).
This raised the question of whether the blocking action of LT was
causally linked to its well characterized glucosylating enzymatic
activity. Glucosylation of small GTPases by LT involves an enzymatic
domain localized in the N-terminal region of the toxin (for review, see
Busch and Aktories, 2000 ). A recombinant polypeptide (amino acids
1-546, denoted as LT82 NH2) was produced in E. coli.
Similar to its parent holotoxin, this peptide retained the ability to
glycosylate mammalian recombinant Rac, Ras, Ral, and Rap, but neither
Rho nor Cdc42, in vitro (Fig.
3A, compare the top two
autoradiograms). Intraneuronal application of LT82 NH2 (50 nM, final intrasomatic concentration) also
blocked ACh release in a manner comparable to the holotoxin (Figs.
2C, 3B) (no significant difference:
p = 0.33). In contrast, when a double mutation
(aspartate to alanine exchange at positions 286 and 288) was introduced
to abolish Mn2+ coordination and
UDP-glucose binding (Busch et al., 1998 ), the recombinant peptide (Fig.
3, LT82 NH2 mutant) had no glucosyltransferase activity on
recombinant GTPases, in vitro (Fig. 3A,
bottom panel), and no blocking action on
neurotransmitter release when applied intraneuronally (50 nM, final intrasomatic) (Fig. 3B,
white bar).

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Figure 3.
Mutations in catalytic domain of LT82 abolish both
GTPase-glucosylating and ACh release-blocking activities.
A, Protein substrate specificity of glucosylation by
LT82 (top panel), recombinant LT82 fragment
(amino acids 1-546) containing an intact catalytic domain
(middle panel; LT82 NH2) or a D to A
exchange at positions 286 and 288 (bottom panel;
LT82 NH2 mutant). Recombinant GTPases (1 µg of each)
were incubated with LT or fragments (5 µg/ml) in the presence of
UDP-14C-glucose for 60 min at 37°C. Labeled proteins were
analyzed by SDS-PAGE and autoradiography. Position of molecular weight
markers is indicated. B, The effect of recombinant
fragments on ACh release. Same presentation of the data as in Figure
2C. ** denotes significant difference (p < 0.001).
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LT glucosylates small GTPases in Aplysia
Figure 4A shows a
Western blot analysis of the small GTPases present in
Aplysia nerve tissue. These immunoreactivities were detected
using specific antibodies raised against members of the Rho and Ras
families and correspond to proteins migrating with an apparent
molecular weight of 20-30 kDa (data not shown). They cannot be
strictly assigned as being Rho, Rac, Cdc42, Ras, Ral, or Rap. Indeed,
because of possible divergent evolution of Rho and Ras GTPases,
cross-reactivities of the mammalian antibodies with several GTPases
cannot be excluded.

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Figure 4.
LT induces glucosylation of GTPases in
Aplysia. A, Immunochemical detection of
small GTPases present in Aplysia nerve tissue. Total
protein homogenates (20 µg) were subjected to gel electrophoresis and
transferred to nitrocellulose sheets, and the GTPases were detected
using anti-Rho, anti-Rac1, anti-Cdc42, anti-Ras, anti-Ral, and anti-Rap
antibodies. B, Samples of Aplysia nerve
tissue fractions (S, soluble; I,
insoluble) containing 100 µg of neuronal proteins were incubated with
LT82 or LT9048 (5 µg/ml each) and UDP-14C-glucose alone
(denoted as ) or in the presence of 10 mM UDP-mannose
(denoted as +), submitted to SDS-PAGE, and autoradiographed. The
position of molecular weight markers is indicated.
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The intraneuronal targets affected by LT were examined by determining
incorporation of 14C-glucose into
Aplysia proteins. Because UDP-glucose, the LT cosubstrate, cannot cross the plasma membrane, these experiments were performed on
Aplysia neuronal tissue fractions. Fractions containing
either soluble (i.e., mostly cytosolic) or insoluble (i.e., membrane associated) protein material were treated with LT82 or LT9048 (5 µg/ml for 1 hr) in the presence of 7 µM
UDP-14C-glucose, and then proteins were
separated by SDS-PAGE. Figure 4B, (first,
second, fifth, and sixth lanes from
left) shows that 14C-glucose
incorporation was detectable only in proteins of 18-30 kDa MW and may
correspond to the glucosylation of the Aplysia monomeric
GTPases revealed by Western blotting (Fig. 4A).
Blocking activity of LT on ACh release is causally linked to
glucosylation of Rac
Substitution of glucose in the nucleotide-sugar by other sugar
moieties inhibits the glucosylation reaction (Hofmann et al., 1998 ;
Busch et al., 2000 ). Moreover, the nucleotide moiety is also important:
for example, UDP-mannose but not GDP-mannose competitively inhibits Ras
glucosylation, in vitro (Busch et al., 2000 ). We found that
incubation of 10 mM UDP-mannose completely
prevented LT-induced incorporation of
14C-UDP-glucose into protein extracts of
Aplysia (Fig. 4B, third, fourth, seventh, and eighth lanes from
left) or recombinant small GTPases (Fig.
5A, lane 2). In
good agreement with this observation, we observed that intraneuronal
coapplication of UDP-mannose and LT82 (1 mM and
50 nM final, respectively) did not block ACh
release (Fig. 5B, second bar from
left). This provided further support for a causal
link between glucosylation of GTPases and inhibition of exocytosis.
Moreover, when UDP-mannose (1 mM) was injected into neurons preinjected with LT82, UDP-mannose immediately froze the
blocking action of LT82 (a representative experiment of three in shown
in Fig. 5C), but no recovery of ACh release was observed (i.e., for at least 6 hr after injection of UDP-mannose).

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Figure 5.
Glucosylation of Rac and inhibition of ACh release
by LT. A, The substrate specificity of LT82 and LT9048
was determined as described in Figure 3A except that
in vitro glucosylation was performed in the absence or
presence of glucosylation competitors: 1 mM unlabeled
UDP-mannose (UDP-man.) or 10 mM unlabeled
TDP-glucose (TDP-gluc.). The position of molecular
weight markers is indicated. B, The ACh release
inhibition determined 90 min after injection of LT82 alone (50 nM, final intrasomatic) or together with UDP-mannose (1 mM final) or TDP-glucose (10 mM final), or
LT9048 (50 nM final). Data are expressed as a percentage of
the average IPSC amplitude determined before injection. The
horizontal dashed line means no inhibition. The
number of experiments in each conditions is indicated.
** denotes significant difference (p < 0.001) as compared with the other conditions. All other comparisons are
nonsignificant. C, Same kind of experiment as in Figure
2A, except that both presynaptic neurons were
injected with LT82 (50 nM, final, white
arrow), but one of them ( ) was later injected with
UDP-mannose (1 mM, final) at the time denoted by the
black arrow (similar results were obtained in 5 experiments).
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Interestingly, we found that the glucosylation reaction could be
assigned more selectively to Rac by using ADP- or TDP-glucose as
competitive inhibitors for UDP-glucose. Indeed, when the glucosylation reaction was performed, in vitro, in the presence of 10 mM ADP-glucose (data not shown) or TDP-glucose
(Fig. 5A), 14C-glucose
incorporation into Ras-related proteins (Ras, Rap, and, at a lesser
extent, Ral) was markedly reduced, whereas glucosylation of Rac was
mostly unaffected. Therefore, intraneuronal application of TDP-glucose
(10 mM, final) with LT82 (50 nM, final) was used to minimize intraneuronal
glucosylation of Ras, Rap, and Ral. In this experimental condition, we
observed that the release of ACh was blocked to a similar extent as
that produced by LT82 alone (Fig. 5B; compare
first and fourth bar from
left).
To determine whether the residual glucosylation of Ral participates in
the LT82-induced blockage of ACh release, we used LT9048, which has
hardly any effect on Ral but efficiently glucosylates Rac, Ras, and Rap
as LT82, but also Cdc42 (Fig. 5A, fourth lane from left). The blocking action of LT9048 (50 nM, final) was comparable to that induced by
injection of LT82 (Fig. 5B, fourth bar from left). This indicated that glucosylation of Ral by
LT82 does not contribute to the LT-induced blockage of ACh release. To
summarize, these combinations of treatments and toxins indicate that
the glucosylation of Rac is sufficient to explain the inhibitory action of LT on ACh release.
The second part of the study was aimed at determining the release
process altered by LT (i.e., implicating Rac-mediated pathway). Previously, we showed that ACh release can recover from near total inhibition to initial values in ~1 sec when sustained high-frequency stimulations (> 10 Hz) are applied to poisoned nerve terminals (Doussau et al., 2000 ). This time duration is shorter than the average
SV cycle in active synaptic buttons (~11 sec) and average residency
time of docked SVs at active zones (~2-5 sec) (Klingauf et al.,
1998 ; Murthy and Stevens, 1999 ). Therefore, the SVs participating in
ACh release recovery are likely to be recruited in a pool that is
already tethered or docked at the active zone but cannot undergo fusion. Therefore, LT action may disrupt a membrane step of the exocytotic process. To investigate this possibility, we analyzed the
possible modifications of the quantal release parameters by LT.
Determination of quantal size and number of active release
sites at the identified cholinergic synapses in the buccal ganglion of
Aplysia
To estimate the quantal size, q, and number of
functional release sites, n, we generated IPSC variance
versus mean plots (see Materials and Methods) by submitting buccal
ganglion synapses to protocols aimed at changing average release
probability, (i.e., the product
po*pA) and
thus ACh release. Average product
po*pA was
altered by two different manipulations. The first one involved a change
in the extracellular
[Ca2+/Mg2+]
ratio and was aimed at changing the effectiveness of an action potential in activating a release site (i.e., to alter mainly but not
exclusively po). The second manipulation
was based on changes in stimulation frequency inducing a variable
degree of depression (Silver et al., 1998 ) and was expected to affect
mainly but not exclusively pA. Indeed, the
probability for a site to be filled with a SV ready for release depends
on the balance between the release rate and the replenishing kinetics
of the release site and also from the priming mechanisms that allow a
docked SV to become fully releasable.
In the first series of seven experiments, the release probability was
changed by manipulating the extracellular
[Ca2+/Mg2+]
ratio. In the first part of the experiments, we analyzed (stationary analysis) the fluctuations in amplitude of IPSCs during stable epochs of ~30 min after the ganglia had been superfused with medium containing different
[Ca2+/Mg2+]
ratios (five distinct levels between 2.1 and 0.14) (Fig.
6A). In the second part
of these experiments, nonstationary analysis was performed on the
fluctuations in IPSC amplitude during the reduction in ACh release
caused by a fast transition between high (2.1) and low (0.14)
extracellular
[Ca2+/Mg2+]
ratios (Fig. 6B). As shown in Figure 6, C
and D, the A and B parameters of the
parabolas (Eq. 4) adjusting the Var = f(Imean) plots were the
same for both protocols (compare black-filled and open
bars). The duration of the second protocol (45-60 min) was short
enough to be performed twice on the same neuron, before and after
injection of LT (see below).

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Figure 6.
Stationary and nonstationary analysis of the
fluctuations in IPSC amplitude when release probability is modified.
The experiment illustrated in A and B is
representative of a series of seven performed under the same
experimental conditions. The Aplysia ganglion was
superfused with physiological medium containing modified extracellular
[Ca2+/Mg2+] (as indicated in
A1 and
B1) to change release probability.
A1, The I = f(t) plot reporting IPSC amplitude
(I) measured after stabilization or evoked
ACh release at the indicated extracellular
[Ca2+/Mg2+].
B1, The I = f(t) plot during transition
between high and low extracellular
[Ca2+/Mg2+].
A2, B2, The
result of subtracting Imean from the
corresponding I as determined by stationary
(A) or nonstationary analysis using a window for
local linear fitting w = 9, and variance window
width w = 16 (B). For
details, see Materials and Methods and Figure 1.
A3,
B3, The corresponding Var = f(Imean) plots. The
solid line denotes the approximation of the data by a
simple parabola using Equation 4. The regression coefficients
r2 are indicated to indicate how good
the fits are. A and B are taken from the
same experiment in which the corresponding values of A
that refer to q are 2.91 nS
(A3) and 2.83 nS
(B3) and 1/B that refer
to n are 426 sites (A3)
and 389 sites (B3). C,
D, Averaged parabola parameters A and
1/B. Black-filled bars, open
bars, and gray-filled bars refer to
A and 1/B determined by stationary and
nonstationary analysis when extracellular
[Ca2+/Mg2+] was changed as
described in A and B and when stimulation
rate was modified as described in E, respectively. These
two experimental conditions are denoted as
[Ca2+/Mg2+]
and Stim. rate. The number of experiments
is indicated, and ns denotes nonsignificant difference.
E, To change release probability, presynaptic neurons
were submitted to various stimulation frequencies. A representative
experiment of a series of six is illustrated. IPSC amplitudes from
epochs of 50 recordings at the indicated stimulation frequency were
reported against the total number of IPSCs analyzed.
E2, Using stationary analysis, the
fluctuation of IPSC around Imean was
determined. E3, The corresponding
Var = f(Imean)
plot. The solid line denotes the parabola adjusted to
the plot using Equation 4.
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In a second series of experiments, we attempted to modify product
po*pA by
changing the rate of stimulation. Increasing the stimulation rate
resulted in synaptic depression (Fig.
6E1), which is thought to reflect
synaptic vesicle depletion at release sites. After stabilization of ACh
release in each stimulation condition, the amplitude of fluctuation in
IPSC around Imean was determined using
stationary analysis. The Var = f(Imean) plots (Fig.
6E3) were satisfactorily fitted
(r2 > 0.90) by a simple
parabola (Eq. 4). This graphically confirmed our assumption (see above)
that when the rate of stimulation is increased, release probability
is diminished. Figure 6, C and D
(gray-filled bars), shows that the A and
B parameters determined by this protocol were not
significantly different from those determined by manipulating
extracellular
[Ca2+/Mg2+]
ratios to change product
po*pA (Fig.
6C,D, compare the gray-filled bars
with open and black-filled bars).
The average A values (Fig. 6C) as determined by
these three procedures indicate a quantal size, q, of
~2.5-2.8 nS at the studied synapse. This value overestimates true
q because quantal variability (CVq) contributes to IPSC fluctuations
(Eq. 5). Nevertheless, the A value is comparable to the
uncorrected q values determined previously (1.5-2 nS) at
the same Aplysia synapse using a different approach
(Simonneau et al., 1980 ; Poulain et al., 1986 ). The parameter B (expressed as 1/B in Fig. 6D
to refer to n) suggests that the number of independent
release sites at which quantal release can take place is between 400 and 500 at the studied Aplysia synapse. Because variability
in release probability (CVp) and intersite quantal variability (CVq inter) were not
determined, 1/B is likely to underestimate n (Eq. 6).
Quantal parameters determined by manipulating extracellular
[Ca2+/Mg2+] after LT action
To determine which of the quantal parameters were modified and
accounted for the decrease in IPSC amplitude that characterizes LT
action, the fast change in extracellular
[Ca2+/Mg2+]
protocol was applied before and after LT82 had significantly inhibited
ACh release. Figure 7A shows a
typical experiment from a series of five. To minimize the difficulty in
analyzing the combined blocking action of LT82 and the reduction in
synaptic efficacy caused by
[Ca2+/Mg2+]
change, the protocol was applied at a time when the LT-induced block
was at least 80% (on average by 84%) (Fig.
8A). During the high to
low
[Ca2+/Mg2+]
transition protocol (40-60 min), we determined that the blockage caused by LT82 was 11.7 ± 2% (SEM) as compared with the
91.8 ± 1% decrease in IPSC amplitude observed when
[Ca2+/Mg2+]
was lowered from 2.1 to 0.14. The corresponding nonstationary analysis
of fluctuations in IPSC amplitude and Var = f(Imean) plots is shown in
Figure 7, B and C. After LT had blocked ACh release, the Var = f(Imean) relationship still
appeared parabolic (Figs. 7D, 8B). The
initial slope of the parabola, A, remained unmodified (Figs.
7D,E, 8C), suggesting
that quantal size, q, was not changed. However, if the
studied synapse is saturating, it is conceivable that small changes in
the presynaptic component of q (SV content) may not have
been detected.

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Figure 7.
The effect of changing extracellular
[Ca2+/Mg2+] before and during
LT action. The experiment illustrated is representative of a series of
five performed under the same experimental conditions.
A, To determine the quantal parameters before and after
LT82 application, extracellular
[Ca2+/Mg2+] was modified
between 2.1 and 0.14 as indicated in the bottom panel.
Arrow denotes the time of LT injection. Solid
lines denote the set of Imean
determined by nonstationary analysis (with w = 9).
The horizontal, long-dashed line denotes
average I in the control period with
[Ca2+/Mg2+] = 0.42. Dashed line (after LT) denotes the
extrapolated I values (by sigmoid fitting) that would
have been obtained without changing extracellular
[Ca2+/Mg2+]. B,
C, Top panels, Magnification of the
I = f(t) plot
portions boxed in A; bottom
panels, the result of subtracting I values from
the Imean estimated using nonstationary
analysis. D, E, The corresponding
Var = f(Imean)
plots before ( ) and after ( ) LT action. The dashed
straight line indicates that the initial release probability
observed with [Ca2+/Mg2+] = 2.1 was similar before and after LT. In D, the
plots have been scaled to the Imean observed
before changing [Ca2+/Mg2+]
and to the corresponding averaged Var. The identical initial slope of
the parabolas indicates that quantal size, q, is not
modified by LT.
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Figure 8.
Determination of the parabola parameters
affected by LT action using the fast change in extracellular
[Ca2+/Mg2+] protocol. Five
experiments similar to that illustrated in Figure
6B were analyzed before (open bars
or open symbols) and 190 ± 20 min (mean ± SD) after LT injection (closed symbols or filled
bars). A, The mean IPSC amplitude.
B, Mean Var = f(Imean) plot was
obtained by averaging the Var values for
Imean over a 5% amplitude interval.
C, The average parameter A of the
adjusted parabolas, which refers to quantal size, q.
D, The relationships between IPSC amplitude and
extracellular [Ca2+/Mg2+].
The data were normalized to values observed at
[Ca2+/Mg2+] = 0.14 to highlight
possible differences. E, The average 1/B
ratio, which refers to n. F,
Relationships between P parameter (see Eq. 8), which
refers to
po*pA, and
extracellular [Ca2+/Mg2+]. In
A, B, and E, a significant difference
(p < 0.001) was found compared with controls;
C, D, and F show a nonsignificant
difference (p > 0.5).
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The relationship between ACh release and extracellular
Ca2+ was examined by plotting the
I = f([Ca2+/Mg2+]).
To highlight possible changes in this relationship, the IPSC amplitude
values were normalized to the amplitudes observed at the lowest
extracellular
[Ca2+/Mg2+]
used. However, no apparent modification could be found after LT
treatment compared with the control period (Fig. 8D).
In all experiments, we observed that the portion of the parabola
depicted in the Var = f(Imean) plots during
decreasing extracellular
[Ca2+/Mg2+]
started at the same initial average probability as that observed before
applying LT (Figs. 7E, 8B, straight
lines), thereby indicating that average product
po*pA was
unchanged. Moreover, the relationship between P (which
refers to product
po*pA, Eq. 7)
and extracellular [Ca2+/Mg2+]
did not significantly change before and after LT (Fig.
8F). This suggests that the coupling between
Ca2+ influx and exocytosis is unlikely to
be altered by LT action.
After LT, the only difference that we detected was the decrease in
parabola parameter B. Indeed, 1/B (Fig.
8E) was reduced to an extent similar to the
reduction in mean IPSC amplitude induced by LT (Fig.
8A). This suggests that the blocking action of LT action is caused by a diminution in n, the number of active
release sites.
Intracellular application of the
Ca2+-buffer EGTA has been shown to
interfere with LT action (Doussau et al., 2000 ). Moreover, in rat
basophilic leukemia (RBL) mast cells, LT application as well as
expression of dominant-negative Rac results in the disruption of
Ca2+ mobilization from internal stores
(Djouder et al., 2000 ; Hong-Geller and Cerione, 2000 ). Hence, we
cannot exclude the possibility that the change in extracellular
[Ca2+/Mg2+]
protocol used above for determining the quantal parameters did not
interfere with LT inhibitory action leading to false deduction that
only n was modified. To test this possibility, we next
analyzed the variance-mean plots generated by changing the stimulation frequency to alter average product
po*pA, as
described in Figure 6E.
Quantal parameters determined by changing stimulation
frequency after LT action
The "change in stimulation rate" protocol was applied
before and after LT82 had inhibited ACh release (Fig.
9A). In preliminary experiments, we noticed that a significant inhibitory effect of LT
developed during the long duration needed for this protocol (120-180
min to collect enough data for variance determination). To avoid this
problem, the effects of LT were stopped by intraneuronal injection of
UDP-mannose (1-10 mM, final) after that ACh
release was inhibited by ~80% (Figs. 9A,
10A). Because of the
technical difficulty in injecting the same neuron twice without trauma, only four experiments could be analyzed. The "stimulation rate protocol" was performed ~60 min after the UDP-mannose injection to
verify that LT action was indeed stopped. Fluctuations in IPSC amplitude were analyzed before (control) and after LT
injection by the stationary procedure (Fig.
9B,C).

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Figure 9.
The effects of changing stimulation rate
before and during LT action. A representative experiment of a series of
four is illustrated. A, Top panel, To
determine the quantal parameters before and after LT82 injection
(white arrow), ACh release was modified by increasing
the stimulation rate between 0.01 and 10 Hz to change release
probability. The inhibitory action of LT was arrested by injection
(black arrow) of UDP-mannose (10 mM, final).
Bottom panel indicates the different stimulation
intervals used during the experiment. B,
C, Top panels, The IPSC amplitudes are
observed at the indicated stimulation rate and correspond to the data
boxed in A. Bottom panels,
The result of subtracting I values from
Imean (stationary analysis).
D, The corresponding Var = f(Imean) plots before
( ) and after ( ) LT action. The dashed straight
line indicates that release probability observed at a
stimulation rate of 0.01 Hz is similar before and after LT.
E, The plots reported in D have been
scaled to the Imean observed at 0.01 Hz and
to the corresponding averaged Var. The identical initial slope of the
parabolas indicates that quantal size is not modified by
LT.
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Figure 10.
Determination of the parabola parameters before
and after LT action using the change in stimulation rate protocol. Same
presentation as in Figure 8, except that changes in the stimulation
rate were used to modify release probability. In
B, Imean and Var values were
averaged for similar stimulation rate conditions. Averages were made
from four successful experiments. In A, B, and
E, a significant difference (p < 0.001) was
found compared with controls; C, D, and
F show a nonsignificant difference (p > 0.5).
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The Var = f(Imean) plots were well
fitted (r2 > 0.90) by a simple
parabola (Figs. 9D,E,
10B). As expected, the parabola parameter A was not significantly modified by LT treatment, confirming
that quantal size is unchanged (Fig. 10C). Here also, the
Var = f(Imean) plots
depicted the same portion of parabola (Figs. 9D,
10B) before and after blockage of ACh release by LT.
Neither the shape of the Imean = f (stimulation interval) plots (Fig. 10D)
nor the relationships between P and the stimulation interval
were modified after LT injection, as compared with controls (Fig.
10F). We could not explore the responsiveness of the
synapse to very high frequency because at a stimulation rate over 10 Hz, LT-induced block is relieved (Doussau et al., 2000 ). These findings
confirm that our deduction made above that the product
po*pA is not
changed by LT action. Here also, the only parameter modified after LT
was B (Fig. 10E), indicating that
n is reduced by LT action.
Variance to mean relationship during LT-induced blockage of ACh
release confirms a reduction in the number of release sites
If LT82-induced blockage of ACh exocytosis is caused by a decrease
in n, this should also manifest as a linear relationship between Imean and Var in the Var = f(Imean) plots made by
nonstationary analysis of IPSC amplitude fluctuations during the ACh
release blockage produced by LT injection. Indeed, when IPSC amplitude changes as the result of a reduction of n, Var should
decrease linearly with Imean according
to equation:
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(8)
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A fall in IPSC amplitude caused by a change in the product
po*pA should
be described by Equation 3, which is a parabola (see Eq. 4), similarly
as this has been illustrated above when
po*pA was
experimentally modified by distinct procedures. After
progressive q changes, the Var = f(Imean) relationship
should be described by a quadratic function of positive curvature of
equation:
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(9)
|
Data were submitted to a nonlinear regression analysis using the
quadratic function Var = a*Imean + b*I2mean.
Indeed, this procedure avoids any a priori on the linearity
or nonlinearity of the Var = f(Imean) relationship. A
linear slope should manifest with b = 0 and
a > 0 (Var = a*Imean). If
a = 0 and b >0, Var = b*I2mean,
and the corresponding Var = f(Imean) plot would display
a positive curvature pinpointing a change in q size (Eq. 9).
If a > 0 and b < 0, Var = f(Imean) plot would exhibit a negative curvature indicating a change in product
po*pA (Eq. 3).
In Figure
11A3,
the parameters for nonlinear regression analysis of the Var = f(Imean) plot were
a = 0.68 and b = 10 4
(r2 = 0.88) (dashed
line). The mean adjustment parameter for the 11 LT82 and 5 LT9048
experiments analyzed (Fig. 11B,C)
were a = 0.83, b = 1.4 10 3,
r2 = 0.78, and
a = 1.12, b = 0.8
10 3,
r2 = 0.76, respectively. In all
cases, b approaches to 0, indicating that Var = f(Imean) is of the form
Var = a*Imean.
Accordingly, good adjustments of the Var = f(Imean) plots were also
obtained using linear regressions: Figure
11A3: a = 0.73, r2 = 0.83; Figure
11B: a = 0.97, r2 = 0.77; Figure
11C: a = 1.03, r2 = 0.75. Therefore, the
relationships between Var and Imean
when LT82 or LT9048 blocks ACh release are likely to be linear, and this graphically confirms that inactivation of Rac by LT causes inhibition of ACh release by reducing the number of release sites.

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Figure 11.
Graphical determination of n as
the quantal parameter modified by LT action. A, IPSC
fluctuations during the course of LT82-induced blockage of ACh release
were analyzed by nonstationary analysis using a window width for local
linear fitting w = 33, and variance window
W = 21. A1,
I = f(t) plot.
The set of Imean is represented by a
solid white line. A2,
The result of subtracting I values from
Imean. A3,
The corresponding Var = f(Imean) plot.
B, C, The Var = f(Imean) plots from
experiments in which either LT82 (n = 11) or LT9048
(n = 5) was injected. Individual plots are
indicated by different symbols and are scaled to the
Imean and Var values determined
before LT injection. For clarity, only 1 point of 10 is plotted.
A3-C, The adjustment
of the data by linear (solid straight line) or nonlinear
regression analysis (dashed curves) is presented. For
r2 values see Results. The
linear Var = f(Imean) relationships
indicate that Imean diminution is caused by
a decrease in n, the number of active release
sites.
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As an outcome of this study, one may anticipate that the graphical
procedure described above [see also Humeau et al. (2001b) ] may help
to identify the quantal parameter(s) modified when synaptic efficacy is
changed in response to a treatment |