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The Journal of Neuroscience, January 15, 1999, 19(2):589-598
A Persistent Activity-Dependent Facilitation in Chromaffin Cells
Is Caused by Ca2+ Activation of Protein Kinase C
Corey
Smith
Department of Membrane Biophysics, Max-Planck-Institute for
Biophysical Chemistry, Am Fassberg 11, D-37077 Göttingen, Germany
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ABSTRACT |
Activity-dependent facilitation was studied in bovine adrenal
chromaffin cells. Stimulation with a train of depolarizations caused
subsequent triggered exocytotic activity to be significantly enhanced.
After the facilitating stimulus train, the readily releasable vesicle
pool (RRP) size was estimated from capacitance jumps in response to
paired depolarizations and found to be elevated for a period of at
least 10 min. The time dependency of onset and degree of facilitation
could be well fitted assuming protein kinase C (PKC)-dependent and
independent Ca2+-mediated processes. Both processes
increase the recruitment of vesicles from the reserve pool to the RRP,
resulting in an greater number of releasable vesicles. The data suggest
that cell activity can act as a trigger to increase cytosolic
Ca2+ to a level sufficient to cause an increase in
the number of readily releasable secretory vesicles, with the more
persistent component of the evoked facilitation being mediated through
activity-dependent activation of PKC.
Key words:
facilitation; exocytosis; vesicle pools; plasticity; membrane capacitance; chromaffin
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INTRODUCTION |
Many excitatory cells undergo
activity-dependent changes in their secretory response. Neuroendocrine
cells, like many neurons, display secretory depression after intense
stimulation (Thomas et al., 1993 ; Moser and Neher, 1997 ), augmentation
after elevation of cytosolic calcium (Bittner and Holz, 1992 ; Thomas et
al., 1993 ; von Rüden and Neher, 1993 ), long-lasting potentiation
after pharmacological activation of protein kinases (Knight and Baker,
1983 ; Vitale et al., 1995 ; Gillis et al., 1996 ), and a block of
potentiation after treatment with kinase inhibitors (Gillis et al.,
1996 ; Renström et al., 1997 ; Kumar et al., 1998 ).
As first shown for the neuromuscular junction (Elmqvist and Quastel,
1965 ; Betz, 1970 ), secretory behavior of neuroendocrine cells
can be simulated by sequential models that assume trafficking of
exocytotic vesicles between a large reserve pool and a smaller readily
releasable pool (RRP; Heinemann et al., 1993 ; Thomas and Waring,
1997 ; Neher, 1998 ). The amount of evoked transmitter release is
determined by the number of vesicles inhabiting the RRP and the
probability of each vesicle to undergo exocytosis in response to a
stimulus. In bovine adrenal chromaffin cells, the RRP size has been
shown to be increased by elevated
[Ca2+]i in a protein kinase C
(PKC)-independent manner and through the activation of PKC. PKC causes
facilitation by increasing the delivery rate of vesicles from the
reserve pool to the RRP (Smith et al., 1998 ). The goal of this study
was to test whether the Ca2+-mediated activation of
PKC was likely to play a physiological role in the modulation of
stimulus-evoked secretion. It was asked whether heightened cell
activity was indeed capable of raising [Ca2+]i to levels sufficient in
magnitude and duration to activate PKC and result in a facilitation of
the exocytotic process. To answer these questions, the RRP size was
estimated using paired depolarizations (Gillis et al., 1996 ) before and
at different times after conditioning trains of short depolarizations.
Exocytosis was monitored by means of patch-clamp measurements of cell
membrane capacitance (Cm, an index of
vesicle-membrane fusion). Average [Ca2+]i was recorded using the calcium
indicator fura-2. A computer simulation of the experimental protocol,
based on a two-step model of secretion (Heinemann et al., 1993 ,
1994 ) was used to determine the extent to which the increased RRP was
responsible for the observed secretory augmentation, to examine the
duration of the facilitation, and to track the activity of the
PKC-enhanced recruitment of vesicles from a reserve population to the RRP.
Reported here are the results of a study in which secretory efficiency
was measured during multiple trains of depolarizations. The data show
that trains of stimuli in chromaffin cells evoke two forms of
Ca2+-dependent facilitation previously described
(Smith et al., 1998 ) and that the more persistent form of facilitation
is sensitive to selective PKC blockers. Furthermore, facilitation is
not likely caused by a shift in the Ca2+ sensitivity
of the secretory process, rather to the increase in the total number of
vesicles that inhabit a releasable state.
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MATERIALS AND METHODS |
Chromaffin cell culture. Adult bovine adrenal glands
were acquired fresh from local slaughter houses, perfused with cooled sterile Locke's Ringer's solution, and transported to the laboratory. The glands were trimmed well of fat, and the cortex was cut around the
circumference of the long axis of the gland. Glands were again perfused
with Locke's Ringer's solution and placed in a 37°C shaking water
bath for 5 min. Glands were then perfused with collagenase (type I; 1.0 mg/ml; Worthington, Freehold, NJ) that had been solublized in a DMEM
growth medium (Life Technologies, Gaithersburg, MD). The DMEM
growth medium was supplemented with penicillin (20 U/ml), streptomycin
(20 µg/ml), and GMS-X (a defined serum substitute containing insulin,
transferrin, and selenium; Life Technologies). The collagenase
perfusion was performed twice, with each perfusion followed by a 15 min
incubation in a 37°C shaking water bath. After the collagenase
treatment, the cortex of the glands was manually separated from the
medulla, and the medulla was minced into small cubes with a scalpel.
The minced medulla was further manually dissociated with the blunt end
of a sterile Pasteur pipette and filtered through nylon mesh (~150
µm pore size). The filtrate was resuspended in 45 ml of Locke's
Ringer's solution and spun at 1000 × g for 2 min. The
pellet was then resuspended in Locke's Ringer's solution to a final
volume of 14.7 ml combined with 15.3 ml Percoll (Pharmacia, Uppsala,
Sweden) and 1.7 ml 10× Locke's Ringer's solution. The Percoll
suspension was spun at ~20,000 × g for 20 min at
room temperature. Enriched chromaffin cells were recovered from the
Percoll gradient and repelleted in 40 ml Locke's Ringer's solution by
a 1000 × g spin for 2 min. The cells were resuspended
in the DMEM growth medium (see above) and at an approximate
concentration of 4.4 * 103
cells/mm2, plated onto coverslips and maintained at
37°C in 10% CO2. Experiments were performed 1-4 d after
cell preparation.
Solutions. During recordings, cells were constantly
superfused at a rate of ~1 mm/min with a Ringer's solution of the
following composition (in mM): 150 NaCl, 10 HEPES-H, 10 Glucose, 2.5 CaCl2, 2.8 KCl, and 2 MgCl2, or as otherwise noted. The osmolarity was adjusted to 310 mOsm with mannitol, and pH was 7.2. The standard perforated-patch solution contained (in mM): 135 Cs
glutamate, 10 HEPES-H, 9.5 NaCl, 0.5 TEA-Cl, and 0.53 amphotericin B,
pH 7.2, and osmolarity 300 mOsm. Amphotericin B was prepared as
described by Smith and Neher (1997) . Pipettes were tip-dipped in
amphotericin-free solution for 2-10 sec, and back-filled with freshly
mixed amphotericin-containing solution. The liquid junction potential
between the extracellular Ringer's solution and the intracellular
solution was measured to be ~13 mV, and all potentials were adjusted
accordingly. All chemicals were obtained from Sigma (St. Louis, MO),
with the exception of CsOH (Aldrich, Milwaukee, WI) and amphotericin B
(Calbiochem, La Jolla, CA), or as otherwise noted.
Electrophysiological measurements. Pipettes of ~2-3 M
resistance were pulled from borosilicate glass, partially coated with a
silicone compound (G.E. Silicones, Bergen Op Zoom, The Netherlands), and lightly fire-polished. For acquisition, an EPC-9 amplifier and
Pulse software running on an Apple Macintosh were used. Cell capacitance (Cm) was estimated by the
Lindau-Neher technique (for review, see Gillis, 1995 ) implemented as
the "Sine + DC" feature of the Pulse lock-in module. A 700 Hz, 35 mV peak amplitude sinewave was applied to a holding potential of 83
mV, and the reversal potential of the lock-in module was set to 0 mV.
For depolarization, the sinewave was interrupted only after a complete
sine cycle and reinitiated at the start of a sine cycle. Data were
acquired through a combination of the high time resolution Pulse
software and the lower time resolution XChart plug-in module to the
Pulse software. Briefly, membrane current was sampled at 10 kHz shortly (100 msec) before, during, and for 3.5 sec after the depolarizations and cell capacitance, cell conductance, and pipette access resistance were calculated at 700 Hz. Data acquired between high time resolution Pulse protocols were typically sampled at 12 Hz with the lower time
resolution XChart plug-in. The higher time resolution Pulse data were
then digitally filtered and merged into the lower time resolution
XChart data off-line in IgorPro (Wavemetrics, Lake Oswego, OR) for
display purposes.
Capacitance increases caused by depolarizations were determined from
the high time resolution Cm traces as the difference between mean Cm measured in a 50 msec window starting 50 msec after the depolarization minus the mean prestimulus
Cm, also measured over a 50 msec window. The first
50 msec of the postdepolarization capacitance was neglected to avoid
influences of nonsecretory capacitance transients (Horrigan and
Bookman, 1994 ). With the stimulus protocol used here, it was assumed
that endocytosis was unlikely to be a contaminating factor in the
estimation of exocytosis. Triggered endocytosis in response to
Ca2+ influx of <90 pC, termed "compensatory
endocytosis" (Smith and Neher, 1997 ), has been shown to take place
with time constants of 6 sec or slower, or even to be totally absent
after single secretion events totaling less than ~50 fF (Engisch and
Nowycky, 1998 ). Endocytosis on such a slow time scale would be unlikely to effect Cm measurements made 50 msec after a
depolarization. Experiments were performed at 20-25°C. Data are
presented as mean ± SE.
Cytosolic Ca2+ measurements. Cellular
Ca2+ concentrations were measured in the
perforated-patch configuration by preincubating the cells in growth
medium containing a 1 µM concentration of the
membrane-permeant acetyl methyl ester form of fura-2 (fura-2 AM;
Molecular Probes, Eugene, OR; Grynkiewicz et al., 1985 ) for 5 min at
37°C. Cells were illuminated at either 360 or 390 nm light with a
monochrometer (TILL Photonics, Planegg, Germany) attached to the
fluorescence port of a Zeiss IM35 microscope (Zeiss, Jena, Germany).
Excitation light was reflected through the objective (50× water
immersion, NA = 1.0; Leitz, Wetzlar, Germany) by a 495 nm cutoff
extended range dichroic mirror (TILL Photonics). Emitted light then was
passed through an HQ535/50 nm bandpass filter (AHF, Tübingen,
Germany) before sampling with a photo multiplier tube (model
R928; Hamamatsu, Tokyo, Japan). The signal was passed into an
analog-to-digital converter channel of the EPC-9 and processed with the
fura extension of the Pulse Software. After the experimental protocol,
the perforated patch was ruptured causing the intracellular fura-2 to
dialyze out of the cell, allowing for the measurement of the
autofluorescence of the cell. The autofluorescence values at 360 and
390 nm wavelength excitation were subtracted from values measured
during the experiment, and the [Ca2+] was
estimated after Grynkiewicz et al. (1985) . No absolute estimate for the
cytosolic fura concentration was made, but the emitted fluorescence in
these experiments was roughly 0.2-0.5 times as bright as values
measured with 100 µM K+-fura in the
internal solution of whole-cell experiments. Also, after breaking into
the whole-cell configuration to allow fura to dialyze out, it was found
that the cell fluorescence dropped only by ~50% (fura fluorescence
was only as bright as autofluorescence). Taken together, these two
points imply that the fura-AM loading protocol used in these
experiments resulted in very low cytosolic fura concentrations, perhaps
only a few tens of micromolar. These concentrations of fura would be
very unlikely to significantly alter the cytosolic
Ca2+-buffering and the time course of poststimulus
Ca2+ clearance.
Computer simulation of measured RRP recovery. A computer
simulation of the measured RRP characteristics was based on the
"two-step model of secretion control" (Heinemann et al.,
1993 ) with code written within IgorPro. A brief summary of the
model and its current implementation is supplied here. The two-step
scheme for secretion describes the transition of vesicle between three
separate states. Pool A is considered to be a large reserve pool of
vesicles that mature, in a Ca2+-dependent manner,
into the release-ready vesicles of pool B. Vesicles in the B pool
either revert and rejoin pool A, or undergo evoked
Ca2+-dependent secretion, described as the
transition to pool C.
|
(1)
|
For the simulations, pool A was assumed to be equivalent to a
number of vesicles totaling in capacitance to 5 pF (Heinemann et al.,
1993 ). The forward rate constant k1
between pools A and B is dependent on
[Ca2+]i and is described by the
Michaelis-Menten relationship in Equation 2:
|
(2)
|
where a1 is the maximum possible value of
k1, and b1 has the
meaning of a KD of a regulating site. In the
simulations, the stimulus-evoked
[Ca2+]i transient was approximated as
monoexponential decay with a time constant of 5.5 sec (Smith et al.,
1998 ), except after the last pulse of a train, where the
[Ca2+]i decay was described by the
time constants Ca 4 and Ca 5 (see Table
1 and Fig. 4, legend, for description).
The backward rate constant k 1 represents the
spontaneous loss of vesicles from pool B to pool A. The rate of vesicle
exocytosis, transition from pool B to C, is represented in the two-step
model by the rate constant k2 and is defined by
Equation 3:
|
(3)
|
where a3 is calculated from the data of
Heinemann et al. (1994) , according to the secretion study of Klingauf
and Neher (1997) to be equal to 0.035 µM 3
* sec 1 (see Smith et al., 1998 for a more
detailed description of a3 calculation).
The [Ca2+]i-dependent steady state
size of pool B is described by Equation 4:
|
(4)
|
where A is the size of pool A in farads.
To estimate the poststimulus recovery of pool B, the differential
equations derived from the model were solved using the Runge-Kutta integration method. The kinetic input parameters that matched closely
the measured experimental data were determined by fitting both RRP
recovery after depletion, as well as steady state size (Smith et al.,
1998 ). The control kinetic input parameter set is summarized in Table
1. For further description of the limitations and assumptions of the
model, see Heinemann et al. (1993 ; 1994 ) and Smith et al.
(1998) .
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RESULTS |
Repetitive stimulation results in an increase in
exocytotic efficiency
The efficacy with which trains of depolarizations evoked granule
exocytosis was measured in single chromaffin cells in the perforated-patch configuration of the voltage-clamp technique (Zhou and
Misler, 1995 ; Engisch and Nowycky, 1996 ; Engisch et al., 1997 ;
Renström et al., 1997 ). For short experimental protocols, no
quantifiable or significant difference in the kinetics of exocytosis can be detected between whole-cell and perforated-patch recordings (von
Rüden and Neher, 1993 ; Smith et al., 1998 ). However, for the
prolonged times required for the protocols in this study, experiments
were performed in the perforated-patch configuration to avoid washout
of vital cytosolic factors that support exocytosis (Zhou and Neher,
1993 ; Burgoyne, 1995 ; Engisch and Nowycky, 1996 ; Smith and Neher, 1997 ;
Smith et al., 1998 ). Vesicle exocytosis was measured by monitoring the
electrical capacitance of the cell, an index of cell surface
area (Neher and Marty, 1982 ; Lindau and Neher, 1988 ). Total evoked
exocytosis was measured as the difference in cell capacitance before
and after the depolarizing stimuli, whereas stimulus intensity was
quantified as the integrated evoked Ca2+ influx
caused by the depolarization (Engisch and Nowycky, 1996 ; Seward and
Nowycky, 1996 ; Engisch et al., 1997 ; Renström et al., 1997 ).
Shifts in exocytotic efficiency would be reported as a steeper or
shallower slope of the integrated evoked capacitance increases to the
integrated Ca2+ influx, either caused by a change in
the affinity of a Ca2+ or caused by a change in the
number of readily releasable vesicles.
In neuroendocrine cells, studies designed to measure exocytotic
efficiencies under conditions that approach the physiological behavior
of cells have used depolarization trains as stimuli (Zhou and Misler,
1995 ; Engisch and Nowycky, 1996 ; Seward and Nowycky, 1996 ; Engisch et
al., 1997 ; Renström et al., 1997 ). For this same reason, and so
that results could be interpreted in the context of the existing
literature, cells were also stimulated with depolarizing trains in this
study. When stimulated with a train of depolarizations, chromaffin
cells exhibit a heightened secretory efficiency during subsequent
depolarization trains. Shown in Figure 1A is a
cell challenged with two stimulation trains with the second train of stimuli delivered ~3 min after the end of the first train. Evoked exocytosis was measured as the difference between cell capacitance before and shortly after depolarization. Evoked endocytosis, as seen
between individual stimuli, took place on time scales too slow to play
any significant role in the accurate estimation of triggered exocytosis
(see Materials and Methods for a description of exocytosis estimation
protocol). Total measured evoked capacitance increase is plotted
against integrated Ca2+ influx in Figure
1Aii. An increase in the slope of the
secretion-stimulus relationship occurred after approximately the
eighth depolarization of the train. Integrated evoked Cm
increases were divided by total integrated Ca2+
influx for the calculation of "exocytotic efficiency". This in effect gives the average efficiency within an entire train. The efficiency in many trains begins lower, but increases within the train,
as seen in Figure 1Aii. This is likely caused
by the buildup of [Ca2+]i during the
train and therefore an increase in the rate of vesicle delivery to the
RRP, and would therefore be limited to times of elevated
[Ca2+]i. Efforts were not focused on
quantification of the internal efficiency shifts within trains in this
study, rather were limited to increases of efficiency between trains.
Therefore, efficiencies are reported as mean values for all responses
from a train. In Figure 1Aii, the mean exocytotic
efficiency was 2.3 fF/pC, a result similar to the "standard
curve" described by Engisch et al. (1997) . The second train, after
the first by ~3 min, resulted in an average exocytotic efficiency of
3.1 fF/pC. The same protocol as described for Figure
1A was repeated with a 500 nM
concentration of the membrane-permeant PKC inhibitor
bisindolylmaleimide I (BIS; Calbiochem) in the bath (Fig.
1B). Although the Ca2+ influx from
the second stimulus train was smaller than that of the first, both
trains resulted in ~2.3 fF/pC exocytosis.
To confirm that the BIS-sensitive facilitation was indeed caused by
Ca2+-mediated activation of PKC, another potent
inhibitor, Gö 6983 (100 nM, Calbiochem), was used,
resulting again in a block of facilitation expected in the second
train. Treatment of the cells with 100 nM PMA, a
potent phorbol ester activator of PKC, resulted in an increase in
secretory efficiency in both stimulus trains, obscuring the
activity-dependent facilitation seen in control cells. Simultaneous
treatment with 100 nM PMA and 500 nM BIS
resulted in a block of the activity-evoked facilitation seen in control cells (results summarized in Fig. 1C). Taken
together, these pharmacological perturbations point to
Ca2+ activation of PKC as responsible for the
activity-dependent facilitation observed in the control condition.

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Figure 1.
Exocytotic efficiency is increased by cell
activity. Ai shows the capacitance record of a cell
stimulated by two trains of depolarizations. Cells were held at a
potential of 83 mV in the perforated-patch voltage-clamp technique.
Each train consisted of 20 depolarizations to 7 mV, 50 msec long,
separated by 5 sec intervals. In this experiment, the second train
followed the first train by 189 sec. Aii, Evoked
capacitance increases and Ca2+ influx were measured
for each stimulus. The integrated capacitance response is plotted
against the integrated Ca2+ influx for each train.
The first train resulted in a total Cm increase of 792 fF
caused by a Ca2+ influx of 343 pC, whereas the
second train resulted in a total Cm increase of 966 fF in
response to a Ca2+ influx of 304 pC. The same
protocol as described in A was repeated with the
specific membrane-permeant protein kinase C inhibitor BIS in the bath
at a concentration of 500 nM. Bi, The cell
capacitance recorded from the cell during the experiment is plotted.
Bii, As in Aii, the integrated
capacitance response is plotted against the integrated
Ca2+ influx for each train. The first train resulted
in a total Cm increase of 419 fF because of a
Ca2+ influx of 181 pC, whereas the second train
resulted in a total Cm increase of 347 fF in response to a
Ca2+ influx of 154 pC. C, The same
protocol and analysis as described in A and
B was repeated on a cell treated with 100 nM
Gö 6983, 100 nM PMA, and a cocktail of 500 nM BIS and 100 nM PMA. The data for all tested
conditions is summarized and displayed as measured femtofarads per
picocoulombs from the first and second trains. The
asterisks denote values that are significantly different
(p < 0.05; paired Student's
t test) from the control value of that group.
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With intertrain delays shorter than the 180 sec demonstrated in Figure
1, the second train showed a facilitated exocytotic efficiency in both
the control and the BIS-treated cells, although the control cells
always showed a greater increase than the BIS-treated cells (Fig.
2). The facilitation observed in the
BIS-treated cells with shorter intertrain delays most likely represents
a residual Ca2+-evoked, but PKC-independent
secretory facilitation (von Rüden and Neher, 1993 ; Thomas and
Waring, 1997 ; Smith et al., 1998 ).

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Figure 2.
The increase in exocytotic efficiency is greater
in cells with intact PKC activity. Exocytotic efficiencies for control
(dark bars) and BIS-treated cells (light
bars) was determined for first and second trains as total
evoked increase in cell capacitance divided by total evoked
Ca2+ influx. The time between the end of the first
train and the onset of the second train was varied between ~30 and
180 sec. The number of cells measured for each condition are reported
above the data sets. Asterisks represent data sets (with
and without BIS) that are significantly different as determined by a
paired Student's t test (p < 0.05).
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An increase in the RRP size is responsible for the
activity-dependent facilitation
Two possible mechanisms for the activity-evoked facilitation were
considered. In the first scenario, heightened cell activity could act
as a positive feedback mechanism for increasing the affinity of the
Ca2+-sensitive trigger in the fusion process. In
other words, activity would increase the likelihood that a given
vesicle would undergo exocytosis in response to a stimulus. The result
would be a greater exocytotic efficiency. The second scenario would be
to maintain the probability of a single vesicle to undergo exocytosis
but to supply more such vesicles, again effectively increasing the exocytotic efficiency of the cell. To distinguish between these two
possibilities, a protocol was devised by which the total number of
readily releasable vesicles was measured before and at varying times
after a train of depolarizations (Fig.
3). The RRP was measured through the use
of a "dual-pulse paradigm" (Gillis et al., 1996 ; Moser and Neher,
1997 ; Smith et al., 1998 ). From the sum and the ratio of the
capacitance increases ( Cm) to two identical
Ca2+-current injections given in rapid succession,
an upper limit of the RRP, Bmax, is derived:
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(5)
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where S represents the sum of the capacitance responses to the
first ( Cm1) and the second
( Cm2) depolarizations, and R is
defined as the ratio of
Cm2: Cm1. A value
<1 for R represents secretory depression, presumably caused by
depletion of the RRP. In experimental analyses, all cells with an R
value of >0.6 were discarded because accurate estimate of the RRP size
is only possible when adequate vesicle depletion occurs (see Gillis et
al., 1996 for a detailed description of the dual-pulse protocol and its limitations). This strict depression requirement eliminated 46% of the
responses measured under the dual-pulse protocol from analysis.

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Figure 3.
The activity-dependent facilitation is caused by a
larger RRP of vesicles. A, Plotted is the membrane
capacitance recorded from a cell stimulated by a pulse protocol
designed to measure the activity-dependent changes in the number of
vesicles in the readily releasable pool. The initial size of the RRP
was determined through the use of a dual-pulse protocol
(arrow). The RRP was then allowed to completely recover
before the cell was stimulated by a single train of depolarizations as
described in the legend to Figure 1. Again, after complete recovery to
its steady state, the size of the RRP was measured by a dual-pulse
stimulation protocol (arrow). The values R for the first
and second dual-pulse stimuli in this cell were 0.28 and 0.57. B, As in Figures 1 and 2, the integrated evoked cell
capacitance increase is plotted against total evoked
Ca2+ influx, showing a shift in secretory efficiency
during the train. The total evoked increase in Cm was 1136 fF in response to 269 pC total Ca2+ influx, an
exceptionally high increase of exocytotic efficiency during the train.
This cell was chosen for presentation because both dual-pulse stimuli
resulted in an adequate amount of exocytotic depression for an accurate
estimate of the RRP. C, In response to the train of
depolarizations, the size of the RRP grew from a pretrain value of 146 fF to the increased value of 393 fF.
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Figure 3 shows an example of an experiment in which the readily
releasable pool size was probed before and 60 sec after a train of
depolarizations (arrows). The RRP was a control value of 146 fF before the stimulus train but was found to have increased to 393 fF
after the train. Note that the dual-pulse stimuli were followed by
endocytosis returning Cm to prepulse baseline, whereas endocytosis was not as vigorous after depolarizations during the train
(Fig. 1Ai,Bi). This observation is consistent
with published studies that show endocytosis as dependent on
Ca2+ influx, being slower and smaller in magnitude
after stimuli that evoke less Ca2+ influx (Smith and
Neher, 1997 ) and may not occur at all after stimuli that result in <50
fF increase in Cm (Engisch and Nowycky, 1998 ). Although the
cell presented in Figure 3 represents a
high degree of facilitation within the train, the train-evoked increase in RRP size was repeated in 38 different cells with variable time intervals between the train and RRP measurement (see Fig.
6A). Therefore, it seems at least likely that a
significant portion of the activity-dependent facilitation observed in
the multiple-train excitation protocols is caused by an increase in the
number of immediately releasable secretory vesicles. To identify the
proportion of the facilitation that can be attributed to the increased
RRP size, a computer simulation of the process was designed to imitate the experimental protocol shown in Figure 3. However, to accurately calibrate the simulation for a quantitative comparison to the measured
data, a better understanding of the characteristics of Ca2+ clearance after a train of stimuli was first
necessary, because many of the parameters in the kinetic secretion
model are Ca2+-dependent.

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Figure 4.
Ca2+ clearance is slowed after
the train stimulation protocol. A, Voltage protocol
(top trace) and representative evoked currents
(bottom traces) from the first and last depolarization
of a train are shown. B, Average evoked
Ca2+ currents measured during each depolarization of
a train stimuli from 38 individual cells is plotted against the pulse
number (small dots). Only data from the first trains are
included to avoid effects of Ca2+-dependent
inhibition of calcium influx observed in the second trains of paired
train stimulation protocols. For clarity, the current magnitudes from
each pulse were averaged and overlay the individual points
(large dots). The decay in current amplitude was fitted
as a double exponential decay, resulting in time constants of 8.5 and
117.0 sec (Table 1, Ca 2 and Ca 3)
with magnitude of 137 and 253 pA, respectively. C,
[Ca+2]i measured in fura-AM
ester-loaded chromaffin cells after train depolarizations shows a
slowed clearance of Ca2+. A Ca2+
record from a representative cell is displayed, and the post-train
[Ca2+]i decay is fitted with a double
exponential decay, with time constants of 22 and 77 sec (Table 1,
Ca 4 and Ca 5), each of 250 nM in magnitude.
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Ca2+ clearance after trains of depolarizations
is slow
A slow clearance of residual Ca2+ after tetanic
stimuli has been strongly linked to a form of increased exocytotic
activity in crayfish neuromuscular junction termed long-term
facilitation (LTF; Tang and Zucker, 1997 ). A similar slow
Ca2+ clearance can also be recognized in
repetitively stimulated bovine chromaffin cells (Engisch et al., 1996 ,
their Fig. 12). Any such slowed Ca2+ clearance would
have dramatic effects on the Ca2+-dependent
refilling of the RRP in chromaffin cells (von Rüden and Neher,
1993 ; Smith et al., 1998 ), resulting in a residual increase in RRP size
after trains. Two major aspects to the cytosolic Ca2+ environment were considered for the calibration
of the kinetic model, Ca2+ influx during the train
and Ca2+ clearance after the train.
Ca2+-modulated inhibition of Ca2+
influx through voltage-gated calcium channels is well described in
bovine chromaffin cells and would diminish the predicted rate of basal
Ca2+ buildup in the cytosol of the cell or even
cause the steady-state [Ca2+]i to
slowly drop during a train of stimuli. As demonstrated in Figure 4,
this was indeed the case. Data shown in Figure 4, A and
B, demonstrate that during the train of 20 stimuli, the
average magnitude of the Ca2+ currents decreased by
48% in a dual-exponential manner. The second attribute of the
Ca2+ kinetic considered was the posttrain decay
toward basal Ca2+. After less intense stimulation,
[Ca2+]i recovers to baseline in a
monoexponential manner with a time constant of ~5-7 sec (Neher and
Augustine, 1992 ; Smith et al., 1998 ). In response to the more prolonged
Ca2+ influx evoked during the train stimulus,
[Ca2+]i decayed much slower, perhaps
because of a saturation of the faster Ca2+ clearance
mechanisms seen after briefer stimuli (Xu et al., 1997 ) or because of a
re-release of Ca2+ sequestered in cytosolic
organelles (Tang and Zucker, 1997 ). The representative cell in Figure 4
showed a posttrain [Ca2+]i decay
described by a double exponential with time constant of 22 and 77 sec.
The decaying magnitude of Ca2+ influx during the
train and slow clearance after the train were then used to create a
representative Ca2+ profile to serve as a template
for the Ca2+-dependent processes of the secretion
simulation (Fig. 5A). The Ca2+-dependent readily releasable pool behavior
predicted from the simulation is also presented (Fig. 5A,
dashed line). The simulated exocytosis efficiency of
2.16 fF/pC falls within the range measured for control cells (Fig. 2).
Assuming that the elevated Ca2+ caused by the train
of depolarizations, at some point, activates PKC, the steady-state RRP
size should increase because of a heightened rate of vesicle
recruitment. For the purposes of the simulation shown in Figure 4, the
Ca2+-dependent effects of PKC action were delayed
120 sec (arrow), an assumption to be justified below. The
size of the simulated RRP before and 60 sec after the train is plotted
in Figure 4C. The predicted increased RRP size observed
after the train is qualitatively similar to that experimentally
measured in cells (Fig. 3). Assuming that sustained increased cell
activity does indeed raise [Ca2+]i to
levels sufficient to activate protein kinase C, then the facilitation
observed seems to be at least mostly caused by an activity-dependent
increase in the number of releasable vesicles.

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|
Figure 5.
The computer secretion model reflects the
activity-dependent increase in RRP size. A, The rundown
in Ca2+ influx and post-train stimulus
Ca2+ clearance characteristics measured from cells
was incorporated into the two-step model for secretion control as
modified by Smith et al. (1998) . The Ca2+ profile
before, during, and after a train of depolarizations was composed, and
the resulting predicted RRP size was simulated. Activation of PKC
through a sustained elevation in Ca2+ was simulated
as occurring 125 sec into the protocol (arrow) or 120 sec after the initial increase in
[Ca2+]i from the first 50 msec
depolarization. B, The simulated plot of integrated,
evoked capacitance increases versus integrated Ca2+
influx, corresponding to Figures 1, B and
D, and 4B, is displayed with an
efficiency of 2.16 fF/pC. C, Shown are the steady-state
RRP sizes predicted by the model both before and 60 sec after the end
of the depolarization train, with magnitudes of 112 and 333 fF,
respectively.
|
|
The activity-dependent increase in RRP size is delayed
To quantify the proportion of facilitation that could be
attributed to the increased RRP size, measured and predicted
train-evoked increases in RRP size were compared (Fig.
6A). By definition, the
measured and simulated RRP size before the facilitation train were the
same, because it is under these conditions that the simulation is
calibrated. Thirty seconds after a 20 pulse train, the
measured RRP was found to increase by ~100%, even in the
BIS-treated cell, presumably because of residual effects of
the slowly cleared cytosolic Ca2+.
However, a further 30 sec later, a large difference in the RRP size was
measured between the control and BIS-treated cells, with the control
cells exhibiting a sudden and striking increase in the number of
vesicles composing the readily releasable pool. The sudden increase in
RRP size in control cells, with no such observation in the BIS-treated
cells, indicates a delayed onset of the PKC-determined heightened
recruitment of vesicles from the reserve pool A to the readily
releasable pool B.

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|
Figure 6.
The major component of evoked facilitation is
caused by delayed PKC activation. A, The size of the
readily releasable pool was measured in cells both before and at
different times after a train of 20 depolarizations. The protocol was
performed on both control and BIS-treated cells. The resulting RRP
sizes are displayed for all time intervals and for pharmacological
conditions (values accompanying each data point represent the number of
cells). Also displayed are the corresponding results of the computer
simulation of the experimental protocol, with the assumption that the
facilitative effects of PKC action are not measured before a time delay
of 120 sec, an assumption justified below. B, The
results of an analysis designed to track the increase in RRP size
caused by the effects of PKC activation is presented. The computer
simulation (Fig. 5) was run in a repetitive analysis with
Ca2+ activation of PKC assumed to occur immediately
in the first repetition of the model and then delayed by 1 sec for each
successive repetition (i.e., 45 sec delay on repetition number 46) for
a total of 200 repetitions. The goodness-of-fit between the result of
each simulation repetition was calculated as the 2
between the simulation and the data measured from cells
(Bi represents trains of 20 depolarizations, and
Bii represents trains of 10 depolarizations). The
minimum 2 value was 0.23 and 0.42 (Bi and
Bii, respectively), occurring at a delay time of 178 and
172 sec (Bi and Bii, respectively) or
~120 sec after the initial rise in
[Ca2+]i from the first pulse.
C, The activity-dependent facilitation observed persists
undiminished for at least 10 min. Shown are the actual and simulated
RRP magnitudes measured 600 sec after the end of a stimulus train. The
left bars represent five experiments in which the cells
were depolarized to 7 mV within the train, whereas the
bars on the right represent control cells
that were held constant at their clamped potential of 83 mV. The
differences between the two conditions were judged as significant
(paired Student's t test).
|
|
The large and abrupt BIS-sensitive increase in the RRP observed after
stimulus trains implied a delayed but temporally synchronized onset of
Ca2+-activated PKC action. To understand the time
course of the activity-dependent facilitation better, a comparison of
the experimentally measured data to a secretion simulation was made.
The repetitive simulation described a delayed PKC activation, and
subsequent increase in the maximal achievable rate constant (Eq. 2,
a1; Fig. 5, arrow) that
controls the recruitment of vesicles from the reserve pool A to the RRP
B from 0.007 sec 1 to 0.014 sec 1 (see Smith et al., for a further
discussion of the Ca2+-dependent increase in the
kinetic constant a1). The first
repetition contained an increase in a1 at
t = 0 sec, the second repetition incorporated the
elevated value for a1 at t = 1 sec, and each successive repetition delayed the increase in the
constant a1 by 1 additional second. The
simulation was run 200 times. The predicted RRP size was compared with
the measured data for each point (Fig. 6A), and the
"goodness-of-fit" of the simulation result to the measured data was
calculated as the 2 between the two data sets. The
resulting 2 values for each of the 200 repetitions is
plotted against the assumed PKC activity delay in Figure
6Bi. Clearly, the time point at ~180 sec (120 sec
after the first pulse and subsequent increase in
[Ca2+]i) fits the measured data
best, implying that an increase in cytosolic Ca2+
activates PKC but that the effects of the activation are not observed
for ~2 min.
The abrupt nature of the facilitation seen in Figure
6A seemed suspiciously sharp, as if the train
activated PKC but also had an inhibitory influence on the facilitation
mechanism. Then after the train was over, the inhibition would be
released and cause the observed abrupt increase in the readily
releasable pool size. To determine whether this was actually the case,
the same protocol used to produce the data in Figure
6A was repeated, except that the trains were half the
length, only 10 pulses delivered at 0.2 Hz. The RRP size was measured
60 sec before and 30, 60, and 180 sec seconds after the shorter train.
The same 2 analysis as in Figure 6B
was then repeated on these data, with the expectation that if the
BIS-sensitive facilitation was somehow masked during cell activity,
only to appear after a period of rest, that the minimum
2 value for the 10 pulse trains should occur earlier.
This was not the finding, the minimum 2 value for the 10 pulse trains was still only achieved 180 sec into the experimental
protocol, 120 sec after the initial increase in
[Ca2+]i (n = 9; Fig.
6Bii). It is interesting to note that the
2 of the 10 pulse trains failed to rise as strongly with
longer PKC activation delays as that for the 20 pulse trains. This may indicate that the 10 pulse trains were not strong enough to fully activate the Ca2+-dependent PKC.
How long does the activity-triggered BIS-sensitive facilitation last?
The RRP was measured 10 min after a 20 pulse protocol and found to be
still as large as that predicted for maximal PKC action (Fig.
6C). Therefore, it seems that once
[Ca2+]i is elevated to a sufficient
level for long enough, Ca2+-activation of the
delivery of vesicle from the reserve to the readily releasable pool
remains elevated even after [Ca2+]i
returns to baseline levels that would otherwise not activate the
persistent facilitation. This may be caused by several mechanisms. Assuming that the BIS-sensitive, Ca2+-mediated
facilitation does represent the activation of
Ca2+-sensitive PKC, it would be expected that PKC
would translocate to the plasma membrane (TerBush et al., 1988 ).
It is not yet clear how long the activated form of PKC remains at the
membrane. Alternately, the BIS- and Gö 6983-sensitive
facilitation may represent the phosphorylation of a target peptide that
experiences low basal phosphatase activity and therefore does not
return to a control phosphorylation state within 10 min.
 |
DISCUSSION |
The study of exocytotic plasticity enjoys a long history in the
field of synaptic as well as the neuroendocrine physiology. In cells in
which the probability of exocytosis for a single vesicle is low,
tetanic stimulation causes a build-up of residual
Ca2+ and results in an increase in evoked secretion.
Further stimuli begin to deplete vesicles, measured as secretory
depression. In many excitable cells, a period of post-tetanic
potentiation follows the stimulus train. Long-lasting modulation of
synaptic strength in cells of the brain is thought to underlie the
formation of memory and learning, both motor and cognitive (for review,
see Malenka, 1994 ; Byrne and Kandel, 1996 ). Exocytotic plasticity in
the neuroendocrine chromaffin cells exhibits many types of modulation
similar to those in neurons. The modulation of secretion in chromaffin
cells likely plays a role in an animal's stress response, because they
contribute to the "fight or flight" response of the sympathetic
nervous system.
Evidence implies that activity-dependent secretory modulation may occur
through mechanisms other than RRP modulation, relying rather on
alteration of the fusogenic stimulus or the Ca2+
sensitivity of the secretion process. The central synapse "calyx of
Held" exhibits synaptic depression that is at least in part caused by
activity-dependent rundown in presynaptic Ca2+
influx (Forsythe et al., 1998 ). Also decreasing stimulus intensity, the
autocrine action of presynaptically released ATP has been shown to
lower evoked Ca2+ influx, thereby limiting
transmitter exocytosis in crayfish neuromuscular junction (Lindgren and
Smith, 1987 ) and chromaffin cells (Currie and Fox, 1996 ). In the giant
synapse of the squid, decreased synaptic transmission occurs via
adaptation of the secretory apparatus to elevated
Ca2+ during periods of heightened activity (Hsu et
al., 1996 ). Post-tetanic potentiation at the neuromuscular junction of
crayfish, lasting minutes, is caused by the sequestration and slow
re-release of Ca2+ from mitochondrial stores (Tang
and Zucker, 1997 ). Other studies supply evidence that variable
levels of cell activity mobilize entirely mechanistically, kinetically,
or even morphologically different populations of vesicles (Vogel et
al., 1996 ; Engisch et al., 1997 ; Takahashi et al., 1997 ; Kumar et al.,
1998 ; Ma et al., 1998 ; Xu et al., 1998 ). Although activity-induced
decreases in evoked Ca2+ influx were also observed
in this study, stimulus normalization or the delivery of a saturating
stimulus effectively allows for the quantification of the remaining
exocytotic modulatory mechanisms.
Here it is reported that heightened cell activity is sufficient to
trigger at least two forms of activity-induced facilitation in bovine
adrenal chromaffin cells. The data show that a transient form is likely
caused by the Ca2+-regulated increased recruitment
of vesicles from the reserve to the readily releasable vesicle pool, as
previously described in cells with chemically manipulated cytosolic
[Ca2+]. This form of facilitation in seen within
trains and seems likely to be very similar to the evoked facilitation
seen with shorter and milder trains (Zhou and Misler, 1995 ; Engisch and
Nowycky, 1996 ; Engisch et al., 1997 ). It may also be analogous to the
activity-dependent facilitation described in neuronal systems such as
the neuromuscular junction (for review, see Zucker, 1989 , 1996 ; Fisher
et al., 1997 ). The second form of stimulus-evoked facilitation seems
consistent in magnitude and pharmacology to a facilitation previously
shown under either treatment with phorbol ester or with prolonged
elevations in buffered cytosolic Ca2+ and is
sensitive to specific inhibitors of Ca2+-sensitive
PKC (Gillis et al., 1996 ; Kumar et al., 1998 ; Smith et al., 1998 ). The
BIS- and Gö 6983-sensitive form of facilitation has not been
previously associated with heightened cell activity in the chromaffin
system, perhaps because of a threshold Ca2+
requirement that had not been reached in previous studies. Indeed, it
seems that even strong stimuli such as the dual-pulse protocol used
here are not sufficient to evoke the Ca2+-mediated
activation of PKC. It is further shown that both forms of increased
exocytosis are caused by an increase in the number of vesicles that
make up the RRP and are likely not caused by a change in the affinity
of the Ca2+-sensitive fusion step.
The ability for cells to regulate the number of releasable vesicles
through the activity of kinases is not unique to chromaffin cells or
even neuroendocrine cells. The observation that -cells of the
pancreas greatly increase their insulin secretion when treated with
agents such as forskolin, which activates protein kinase A (PKA)
through the cAMP pathways, is well known (Ämmälä et
al., 1993 , 1994 ). Inhibition of PKA blocks this facilitation (Renström et al., 1997 ). PKA, as well as PKC, also seems to play a role in facilitation measured and even a form of learning observed in
the mollusk Aplysia (for review, see Byrne and Kandel,
1996 ). Phosphorylation of the synaptic vesicle-associated peptide
Synapsin I by calcium-calmodulin-dependent protein kinase II is
believed to make more vesicles available for release in central
synapses such as neurons of the hippocampus (Greengard et al., 1993 ; Li et al., 1995 ) by releasing them from the cytoskeletal framework. A
tetanus-induced facilitation lasting hours, termed LTF, has been
demonstrated to be caused by a serotonin-evoked increase in the number
of releasable vesicles (Wang and Zucker, 1998 ). Although no molecular
pathway for LTF has yet been identified, serotonin has indeed been
shown to be an effective activator of PKC activity in medullary
respiratory neurons (Richter et al., 1997 ).
Facilitation evoked through stimulus trains observed by several groups
in chromaffin cells (Zhou and Misler, 1995 ; Seward and Nowycky, 1996 ;
Engisch et al., 1997 ) are accompanied by what initially seem to be
differing interpretations. For example, a previous study (Engisch et
al., 1997 ) concluded that different intensity trains cause secretory
efficiency to deviate from a standard stimulus-exocytosis
relationship, implying a shift in stimulus efficacy. The study
concluded that the modulation was not caused by the decrease or
increase in an RRP but rather to modulation through an unidentified
second messenger pathway. After consideration, however, these results
are not incompatible with the simpler two-step model shown in
chromaffin cells (Heinemann et al., 1993 ; Smith et al., 1998 ),
other neuroendocrine cells (Renström et al., 1997 ; Thomas and
Waring, 1997 ), and from neuronal preparations (Elmqvist and Quastel,
1965 ; Betz, 1970 ; Stevens and Tujimoto, 1995 ). An examination of
the shifts in Ca2+ efficacy reported by Engisch et
al. (1997) show that under light stimulation, a given
Ca2+ influx elicits more secretion than their
control efficiency (standard curve) and that under heavier stimulation
the secretion efficiency falls below the standard curve. If one assumes
that after an initial decrease in RRP size, evident as an exocytotic
burst (Neher and Zucker, 1993 ; Heinemann et al., 1994 ; Seward and
Nowycky, 1996 ), that the rate-limiting step to ensuing exocytosis is
the recruitment of vesicles from the reserve pool to the RRP,
Ca2+ would then essentially begin to approach
saturating concentrations for the release process, having a limited
number of vesicles on which to act. The result would be that greater
Ca2+ influx would on average be a less effective
secretagogue, lowering secretory efficiency. If the control stimulus
intensity of Engisch and Nowycky (1996) and Engisch et al. (1997) were
such that the RRP were always in a semidepleted state, as indicated by
the measured Ca2+ cooperativity of 1.5, [see
Heinemann et al. (1994) and Chow et al. (1994) for discussions of
Ca2+ cooperativity as a function of stimulus
intensity], one would expect exactly the reported facilitation and
depression reported.
Finally, on what level does stimulus frequency really cause secretion
and RPP modulation in chromaffin cells? Stimulus-secretion coupling in
chromaffin cells does not appear to be as tight as in neurons (Chow et
al., 1996 ; Klingauf and Neher, 1997 ). One could draw the conclusion
that single action potentials in chromaffin cells are designed to
elicit exocytosis, as occurs in neurons. However, it also seems
possible that, not single action potentials, rather their frequency may
play a larger role in triggering chromaffin cell secretion. But why
would a secretory cell chose to lose the stimulus-response fidelity
observed in many neurons? The answer may be twofold. (1) They don't
need it. The secreted products from chromaffin cells are mainly
released into the bloodstream for remote action, not requiring the very
high time fidelity observed in neurons. (2) It may not be such a great
sacrifice. As outlined in an elegant review by Zador and Dobrunz
(1997) , recent studies have implicated a form of synaptic modulation
that does not depend on frequency of single action potentials, rather
on the change in their frequency. In this model the changes in firing
frequency result in slight changes in the number of vesicles composing
the RRP, perhaps by changing the basal
[Ca2+]i and therefore the vesicle
delivery rate to the RRP. This results in an increase or decrease in
stimulus-secretion efficacy. A similar model may apply to chromaffin
cells in which not single action potentials, but rather changes in
firing frequency, modulate secretion efficiency as already considered
by Zhou and Misler (1995) .
 |
FOOTNOTES |
Received Aug. 24, 1998; revised Oct. 28, 1998; accepted Oct. 29, 1998.
This work was supported by a grant from the Human Science Frontiers
Program (RG-4/95B). I thank Dr. E. Neher for valuable discussion of
this manuscript and for both material and intellectual support
throughout the project. I also thank F. Friedlein, I. Herfort, and M. Pilot for expert technical assistance.
Correspondence should be addressed to C. Smith, Medical College of
Georgia, Department of Physiology and Endocrinology, School of
Medicine, Augusta, GA 30912-3000.
 |
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