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The Journal of Neurophysiology Vol. 88 No. 2 August 2002, pp. 802-816
Copyright ©2002 by the American Physiological Society
Department of Physiology, University of Wisconsin School of Medicine, Madison, Wisconsin 53706
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ABSTRACT |
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Verbny, Yakov, Chuan-Li Zhang, and Shing Yan Chiu. Coupling of Calcium Homeostasis to Axonal Sodium in Axons of Mouse Optic Nerve. J. Neurophysiol. 88: 802-816, 2002. Axonal populations in neonatal and mature optic nerves were selectively stained with calcium dyes for analysis of calcium homeostasis and its possible coupling to axonal Na. Repetitive nerve stimulation causes a rise in axonal [Ca2+]i the posttetanus recovery of which is impeded by increasing the number of action potentials in the tetanus. This effect is augmented in 4-aminopyridine (4-AP; 1 mM), which dramatically increases the calcium and presumably sodium load during the tetanus. Increasing axonal [Na]i with the Na-ionophore monensin (4-50 µM) and ouabain (30 µM) retards posttetanus calcium decline, suggesting that efficient calcium clearance depends on a low level of axonal [Na]i. Posttetanus calcium clearance is not affected by K-mediated depolarization. To further examine coupling between axonal [Na]i and [Ca2+]i, the resting axonal [Ca2+]i was monitored as axonal [Na+]i was elevated with ouabain, veratridine, and monensin. In all cases, elevation of axonal [Na+]i evokes a calcium influx into axons. This influx is unrelated to activation of calcium channels but is consistent with calcium influx via reversal of the Na/Ca exchanger expected as a consequence of axonal [Na+]i elevation. In conclusion, this study demonstrates that calcium homeostasis in the axons of the optic nerve is strongly coupled to axonal [Na+]i in a manner consistent with the Na/Ca exchanger playing a major role in extruding calcium following nerve activity.
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INTRODUCTION |
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Traditionally,
translation of electricity to biochemistry is thought to take place at
the nerve terminal of a neuron where electricity (the action potential)
is translated into biochemistry via calcium mediated vesicular release
of neurotransmitters. Prior to the nerve terminal, the axon has been
regarded as a high-speed conduit whose major role is transmission of
electricity rather than translation of electricity to biochemistry.
This picture of axons is no longer tenable, as recent studies have
firmly established activity-dependent calcium influx into mammalian
axons, including unmyelinated axons from rat neocortical pyramidal
neurons (Schiller et al. 1995
), cerebellar Purkinje
cells (Callewaert et al. 1996
), cultured dorsal root
ganglion cells (Lüscher et al. 1996
), neonatal rat
optic nerve (Sun and Chiu 1999
), and rat vagus nerves
(Wächtler et al. 1998
). Activity-dependent calcium
signals have also been detected from myelinated axons in the rat optic
nerves (Lev-Ram and Grinvald 1987
). The physiological
role of axonal calcium influx remains unknown. In developing axons of
the rat cerebellar interneurons, Forti et al. (2000)
observed local calcium hot spots, which they speculated, might
represent functional clusters of voltage-dependent Ca2+ channels marking the future position of
presynaptic terminals. A local rise in calcium may trigger
actin/cytoskeletal assembly (Bentley and O'Connor
1994
; Lankford et al. 1996
). Edwards and Cline (1999)
hypothesize that local axonal calcium influx may regulate the addition of new branch points in growing retinal axons.
However, in mature axons such as the mammalian optic nerves where
varicosities or branches are absent, the functional role of calcium
influx along the entire length of axon remains unclear. Pathologically,
excessive elevation of axonal calcium is injurious to axons (for
review, see Stys et al. 1995a
,b
). One of the best-studied mammalian CNS white-matter
tracts where calcium has been implicated in axonal pathology is the
mammalian optic nerve (Stys et al. 1995
). This nerve can
be isolated without neuronal contaminations and is highly amenable to
experimental studies, including calcium imaging (Kriegler and
Chiu 1993
; Sun and Chiu 1999
), electrophysiology and ischemia (Stys et al. 1995
). These studies have led
to the identical of physiological and pathological calcium-influx
pathways. In particular, the reversal of the Na/Ca exchanger in
ischemic axons has been proposed to produce damaging calcium influx
into axons (Stys et al. 1995
).
In this report, we examined the mechanisms for calcium clearance in axons of optic nerves. Because of the technical difficulty of staining axons in these nerves with calcium dyes for direct visualization of axonal calcium signals, very little is known about the calcium clearance mechanisms in axons of mammalian optic nerves under physiological conditions, including such basic issues as how these axons clear a calcium load following repetitive nerve activity and how the clearance is regulated. In this paper, we removed a major technical difficulty in studying calcium signaling in the optic nerve axons by devising a method to selectively stain pure population of axons in these nerves with calcium indicators, thereby allowing the first direct visualization of axonal calcium signals in these nerves in physiological time scales. We then applied this technique to examine some very basic properties of calcium clearance in these axons. We found a strong coupling between axonal [Na]i and axonal [Ca2+]i and suggest that this coupling is best explained if the Na/Ca exchanger is a key player in calcium extrusion following physiological nerve activity.
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METHODS |
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Selective axonal staining and calcium imaging
Optic nerves, excised between the eye and the chiasm, were
freshly obtained from mice of two age groups, neonatal (P5-P10) and
adult (3-8 wk), and laid down on the bottom of an experimental perfusion chamber. The distal end of the nerve trunk was loosely drawn
into a stimulating pipette, and the proximal end drawn tightly into a
recording pipette (Fig.
1A). The
nerves were allowed to stabilize for 60 min before dye loading began.
For dye loading, the normal saline solution in the recording pipette
(the one with the cut end of the nerve tightly drawn in) was replaced a
high-K (140 mM), low-calcium (0 calcium plus 1 mM EGTA) solution
containing 4-5 µl of the cell impermeant form of various calcium
dyes (2-8 mM). The axons were stained by diffusion of the dye from the
cut end. A standard loading time of 3 h was allowed before
experiments began. At the end of the loading period, there was
typically a spatial gradient of dye along the axis of the nerve, with
the resting dye fluorescence highest at the loading end, and smallest at the other end (the stimulating end). We typically performed calcium
imaging in the middle of the nerve trunk, ~500-1,000 µm away from
the dye-loading pipette. The dyes were allowed to remain in the loading
pipette (also serve as the recording pipette) during the entire
experiment. During a typical 1- to 2-h experiment, the calcium
fluorescence baseline measured at the middle of the nerve was quite
stable in most studies (see Fig. 11). We believed that this stable
baseline was due partly to our use of the high-molecular-weight, dextran-conjugated Oregon Green
bis-(o-aminophenoxy)-N,N,N',N'-tetraacetic acid
(BAPTA)-1, which has restricted dye mobility and excellent retention in
the axons without leaking. While a slowly changing baseline
fluorescence was sometimes observed in some experiments, these slow
baseline changes can be easily distinguished from fast calcium
fluorescence changes induced by the various pharmacological (veratridine, ouabain, or monensin) used in this study. In most of the
figures, we reported the calcium responses as either
F/F0 or
F/F0, which normalizes
differences in background fluorescence due to differences in dye
loading.
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Confocal fluorescence imaging of axonal calcium
Calcium images were viewed with a ×40 (Olympus) objective lens
on a Noran Odyssey confocal system (Madison, WI). Throughout the course
of our study, we tried four membrane-impermeant calcium indicators:
Oregon Green 488 BAPTA-1 (MW = 1114) with or without conjugation
to the high-molecular-weight dextran [MW = 10,000; Kd = 170 nM,
Kd values from Handbook of
Fluorescence Probes (6th ed.), Molecular Probes], Oregon Green
488 BAPTA-2 (Kd = 580 nM), Magnesium
Green (Kd = 6,000 nM), and Oregon
Green 488 BAPTA-5N (Kd = 20,000 nM).
We finally chose the high-affinity, dextran-conjugated Oregon Green
BAPTA-1 due to its excellent dye retention and signal-to-noise ratio.
The disadvantage of this high-affinity dye is potential distortion of
calcium signal kinetics due to dye saturation. The low-affinity dyes
were used in this study mostly as a control to assess dye-saturation as
a potential source of error in the interpretation of our data. All dyes
were used at a concentration of 5-10 mM in the loading pipette. The
actual axonal dye concentration at the site of optical recording was
estimated to be ~0.013 of that at the loading pipette (see
RESULTS). Most of the experiments were performed with the
Noran Odyssey System where the dyes were excited with an argon laser at
488 nm and confocal fluorescence images monitored with a 500-nm
long-pass emission filter. The average fluorescence signal from the
whole field (15,000 µm2 area) was collected
on-line at near video rate (30 Hz) and stored for off-line analysis;
image acquisition and on-line calculations were controlled through the
Metamorph software (Universal Imaging). The disadvantage of the Noran
system is poor time resolution (the calcium signal was sampled every
30-40 ms). To achieve higher time resolution where needed, some
experiments were performed with a Praire Technology System (NED) that
collects nonconfocal calcium signals every 500 µs. In most figures,
intracellular calcium concentration was reported as
F/F0 or
F/F0 without calibration for absolute values. Experiments were either done at room temperature (22°C) or at 36°C. Temperature was controlled by a
DC-thermistor-based system.
Electrophysiology
Compound action potentials were evoked by a 125% supra-maximal stimulus applied via the suction electrode to the cut end and recorded from a second suction electrode at the other cut end. Compound action potential (CAP) data were analyzed using pClamp 6.0 software (Axon Instruments, Foster City, CA).
Solution and drugs
The optic nerves were normally bathed in a Ringer solution that contained (in mM) 129 NaCl, 3 KCl, 1.2 NaH2PO4, 2.4 CaCl2, 1.3 MgSO4, 3 HEPES, 20 NaHCO3, and 10 glucose. Calcium-free solutions were prepared by replacing Ca2+ with Mg2+ and by adding EGTA (1 mM); pH was adjusted to 7.4 with NaOH or HCl as necessary. All compounds were from Sigma.
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RESULTS |
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This paper consists of two sections. In the first section, we will describe a technique for selective staining of axons in the mouse optic nerves and provide arguments as well as experimental evidence that we have indeed succeeded in selectively staining axons. This section is an important technical prerequisite to the second section, which uses this staining technique to examine several basic properties of calcium clearance mechanism in the mouse optic nerve axons.
Technique for selective staining of axonal population
In the rat optic nerve, the mean diameter of the axons remains
~0.2 µm for the first postnatal week and increases rapidly to ~1
µm in adult (>P28 days after birth) when the axons are fully myelinated (Foster et al. 1982
). No morphometric data
exist for the mouse optic nerves, the nerves used in this paper, and
the developmental profile for the axon diameters is assumed to be similar to rats. An important prerequisite for a rigorous analysis of
axonal calcium homeostasis is selective staining of axons with calcium
indicators. In our previous studies, the cell-permeant form of the dye
was injected into the extracellular space in the nerve trunk, which was
taken up by both glial cells and axons (Kriegler and Chiu
1993
; Sun and Chiu 1999
). This staining method is useful for analysis of axonal signals only for short electrical stimulations that evoke only axonal calcium transients. For prolonged electrical stimulations, glial calcium responses are evoked
(Kriegler and Chiu 1993
) that contaminate the axonal
signal, rendering conclusive analysis of axonal calcium homeostasis
impossible. In this study, we selectively stained axons by allowing the
cell-impermeant form of the calcium dye to diffuse into axons via a
nerve cut end for 3 h before experiments began (Fig.
1A). Figure 1B compared optic nerve staining
obtained with Kriegler and Chiu (1993)
's method, which
stained both axons and glia (left), and that obtained with our current method (right). Our current staining method
resulted in no glial cell staining (Fig. 1B,
right), both in neonatal and in adult optic nerves. When we
first started this study, we used Oregon Green BAPTA-1 (MW = 1,114). One concern we had was that this low-molecular-weight dye may
cross gap junctions, allowing dyes that enter damage glial cells at the
cut end to spread through glial network to reach the site of optical
recording, which is typically 500-1,000 µm away from the site of dye
loading. However, we did not observe staining of glial cells at the
optical recording site, suggesting that this source of contamination of
the axonal signal did not occur. To further exclude dye transfer via
glial gap junctions, we switched (in later experiments) to calcium dyes conjugated to the high-molecular-weight dextran (MW = 10,000; Oregon Green BAPTA-1), which cannot penetrate gap junctions
(Eckert et al. 1999
). Because the site of optical
recording is 2.5-5 times longer than the length of the average
longitudinal processes of glial cells in mammalian optic nerves (~200
µm) (see Butt and Ransom 1993
), transfer of the
dextran-conjugated dye through glial processes to the recording site is unlikely.
To further confirm that we have in fact selectively stained axons, we
performed the experiment in Fig. 2. We
first loaded the calcium impermeant form of the calcium dye
(dextran-conjugated Oregon Green) through the cut ends of the nerve
with a tight suction pipette, the standard loading method in this
paper. After 3 h (A), we evoked a whole-field calcium
response with a single compound action potential (
). The nerve was
allowed to rest for 10 min, after which adenosine was applied to the
bath (Fig. 2A). The important observation is that no
adenosine response was seen. The rationale behind the use of adenosine
is that glial cells are known to express adenosine receptors, and
previous calcium imaging studies from our laboratory (Kriegler
and Chiu 1993
) have demonstrated adenosine-evoked calcium
responses in glial cells of mammalian optic nerves in situ. The fact
that no adenosine-evoked calcium response was seen following our
standard dye loading suggests that glial cells were not stained in our
current study, and that the action potential evoked response (
) is
purely axonal in origin. To show that glial cells are indeed viable and
can respond to adenosine, we stained glial cells in the same
nerve with a second dye loading (Fig. 2B) using the
method of Kriegler and Chiu (1993)
. This was done by
injecting into the middle of the nerve trunk, the calcium-permeant form
of Oregon Green, which was taken up by both glial cells and axons. Two
hours after this second dye loading, glial cells were stained and
clearly visible. Further, the background fluorescence was greatly
increased, due presumably to additional loading of the axonal
population following the second dye loading. To compare the calcium
responses following the second loading to that of the first one, we
normalized the calcium fluorescence signal to the prestimulation
baseline signal. Confirming our previous studies (Kriegler and
Chiu 1993
), this second dye loading, which stained glial cells,
produced a robust adenosine response (Fig. 2B). To further
exclude the possibility that our standard axonal loading paradigm
(i.e., the 1st dye loading), if allowed to stain for an additional
2 h after the first 3 h (the addition time needed for the 2nd
loading), would by itself lead to gradual glial staining, we did the
control experiment in Fig. 2, C and D. Here we
employed only the standard axonal loading method (putting the dye in
the loading pipette), and applied adenosine twice, one at 3 h
(C), and another at 5 h (D) after loading.
In neither case was an adenosine response seen (C and
D), suggesting our axonal loading method did not lead to
glial loading even after extended periods.
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Our loading method relies on diffusion of dyes from the cut ends along
the axoplasm of axons. Is it reasonable to expect that a
dextran-conjugated molecule with a large MW of 10,000 can produce significant diffusion in only 3 h to allow calcium imaging in our
studies. For example, McClellan et al. (1994)
found that
injection of dextran-conjugated Calcium Green in spinal cords resulted
in retrograde labeling of neurons 5-14 mm away but only after 4 days. How might it be possible that we observed detectable dye loading in
axons 3 h after dye loading? One explanation is that the mode of
dye entry may be different. In McClellan et al. (1994)
,
the dextran dye, which is impermeant, will have to be taken up by the
cells, presumably via pinocytosis. In our case, we cut the axons, which
allowed direct dye entry through the cut ends. Further, our loading
pipette is filled with a calcium-free, EGTA-buffered solution intended
to keep the cut ends of the axons from re-sealing. Hence, our in vitro
loading method may allow faster dye diffusion into axons than in vivo
loading. We further estimated the coefficient of diffusion for the
dextran dye in our experiments. At a distance of ~540 µm from the
loading site (the typical site of optical recording in experiments
involving dextran dyes), the resting fluorescence is ~0.013
(n = 3) of the fluorescence in the loading pipette
(which contains 2-8 mM of the dye) after a 3-h loading period. From
this we estimated a diffusion coefficient (Crank 1956
)
of ~6.8 µm2/s at room temperature. This is
considerably smaller than the coefficient of diffusion of 102 µm2/s measured for fura-2 (Gabso et al.
1997
), which is a much smaller molecule. Our estimate suggests
a very sluggish diffusion of dextran in our experiments. However, the
use of a high dye concentration in the loading pipette evidently
allowed sufficient dye diffusion to a recording site ~540 µm away
to allow optical recording to be performed after a 3-h loading period.
In most of the experiments, we measured the whole-field calcium response (area ~15,000 µm2) elicited from a large number of axons. One concern is whether the whole-field response misses local heterogeneity and whether it faithfully represents response at the single axon level. We therefore compared the whole-field response simultaneously with several spot responses selected randomly from the same nerve, with each spot having an area that is ~300 times less than the whole field. Figure 1C shows the shape of the whole field (smooth trace) and spot (nosier traces) responses are virtually identical, suggesting the calcium response is spatially homogeneous and that the whole-field response faithfully captures the essence of the response at the single fiber level. Given that whole-field response has excellent signal-to-noise ratio, this measurement was routinely adopted as the primary tool for analysis of axonal calcium homeostasis in this paper.
Prior to our study, Ren et al. (2000)
published a method
of selective loading of axons in the mammalian optic nerves with calcium indicators by incubating the nerve in a solution containing the
cell-impermeant form of the dye. Both that work and our work are in
agreement that axons are selectively stained. Collectively, we believe
that we have achieved staining of a pure population of axons in the
optic nerve for rigorous analysis of axonal calcium homeostasis in this
study. In the following section, we will apply this technique to
examine several basic properties of axonal calcium clearance in the
mouse optic nerves.
Basic properties of axonal calcium clearance mechanisms
4-AP INCREASES EVOKED CALCIUM TRANSIENTS. To facilitate analysis of calcium responses with acceptable signal-to-noise, in some experiments we applied 4-AP, a blocker of fast K channels, to increase the amplitude of the evoked calcium transients. Figure 3 shows the effects of 4-AP on the calcium transient and compound action potential evoked by a single stimulation for a P6 (top) and an adult (bottom) optic nerve. In both nerves, 4-AP increased the amplitude and duration of the compound action potential (B and E) and concomitantly increased the area of the evoked calcium transient (C and F). Interestingly, 4-AP has a much more dramatic enhancing effect on the evoked calcium load (area of the calcium transient) in the adult than in the neonatal nerve. For example, 1 mM 4-AP enhanced the calcium load per action potential ~80 times in adult (D) versus ~13 times (D) in the neonatal nerve. In experiments where 4-AP was used to increase the calcium transient, a concentration of 1 mM was used.
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GRADED CALCIUM DECAY FROM PROGRESSIVELY HIGHER CALCIUM LEVEL. We started our analysis of calcium homeostasis by examining the time course of axonal calcium restoration following repetitive nerve activity. Figure 5A shows superimposed axonal calcium transients evoked in a P27 optic nerve (without 4-AP) by a single action potential and a train of 20 action potentials (10 Hz). On termination of the stimulation, the axonal calcium decays toward baseline (A). Interestingly, the calcium decay is graded according to the calcium level at which the decay began, being slower following the 20 action potentials (which elevated axonal calcium to a higher level) than following the single action potential (B). The calcium decay is not a single exponential, either following the single or 20 action potentials.
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CALCIUM DECAY DEPENDS ON THE NUMBER OF ACTION
POTENTIALS.
In the preceding studies, both the calcium level at the start of
the calcium decay and the number of action potentials during the
tetanus were varied. It is possible that the number of action potentials itself (via axonal Na loading) is an important determinant of the posttetanus calcium decline. This issue was examined in Fig.
6. Figure 6A shows
superimposed calcium responses to 1, 20, and 100 action potentials (at
5 Hz) at 22°C for a P8 nerve. The 20-action potential train
elevates calcium to a higher level than the 1-action potential
before the calcium decay began. However, for the 100-action potential
train, the calcium response during the tetanus first reached a peak
then slowly declined, so that by the end of the tetanus (at which the
calcium decay began), the axonal calcium level is actually lower than
that at the end of the 20-action potential train. The decline of the
calcium response during the 100-action potential train may have various
causes. First, there may be calcium-induced calcium inactivation, so
that the increment of calcium influx per action potential is reduced during the tetanus. Second, there may be gradual axonal Na loading so
that the amplitude of the compound action potential is gradually reduced during the tetanus, which leads secondarily to a reduction in
the calcium influx per action potential. This gradual reduction of the
compound action potential amplitude during a prolonged tetanus is
frequently observed (also see Fig. 14), which is consistent with Na
loading and is unlikely due entirely to refractory period. When we
compared the posttetanus calcium decay following the 1-, 20- and
100-action potential train, we found a progressive slowing of the
posttetanus decay (Fig. 6B). This is in spite of the fact the calcium decay started at a lower level at the end of the 100-action potential than at the 20-action potential train. Figure 6C
shows posttetanus calcium decay from another experiment at 35°C where the calcium level at the start of the calcium decay actually reduced (from
F/F0 = 2.8 to 2.6 to 1.13) as the action potential number during the tetanus (5 Hz)
increased from 20 to 100 to 300 respectively. Figure 6D
demonstrates a similar phenomenon using two tetani of different
frequency. The first tetanus is brief (4 action potentials/5 Hz), which
brought the axonal calcium level to
F/F0 ~ 3 before the calcium decay. This is followed by a second tetanus that is
considerably longer but at a lower frequency (40 action potentials/1
Hz), which elevated calcium to a slightly lower level (
F/F0 < 3) before the
decay began. The second decay is slower than the first one (Fig.
6D).
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RESIDUAL COMPONENT IN CALCIUM CLEARANCE. Figure 6, A and C, shows that after a long tetanus, a residual, ultra-slow component in the calcium recovery appeared. We further examined this residual component, particularly with respect to its reversibility, over long time scales in Fig. 6E. To reliably measure the persistent component in the recovery, a 200-s baseline was obtained before applying tetanus stimulation. The control tetanus was brief (20 action potentials at 10 Hz) and produced no significant residual posttetanus component. As the tetanus was increased to 94 action potentials (at 1 Hz), a residual posttetanus component developed that lasted ~10 min before slowly returning to baseline. When the nerve was re-stimulated with the control brief tetanus 18 min later, the residual posttetanus component disappeared, showing reversibility in the development of the persistent component. This argues against irreversible axonal damage due to the long tetanus stimulation. In this plot, only the pretetanus baseline and the posttetanus calcium response were shown; the calcium response during the tetanus deleted for clarity of presentation. The residual component in the calcium recovery could be demonstrated in nerves with or without treatment with 4-AP.
PHARMACOLOGICAL INCREASES IN AXONAL Na
IMPEDES POSTTETANUS CALCIUM CLEARANCE.
The sensitivity of the posttetanus calcium decay on the number of
action potentials suggests that axonal Na loading during the tetanus
may impede posttetanus calcium clearance. To further test this idea, we
examined the effects of pharmacologically increasing axonal
[Na]i on the posttetanus calcium clearance. To
increase axonal [Na]i, we bath applied monensin
(4-50 µM, a Na-ionophore) (Senatorov et al. 2000
),
ouabain (20-30 µM, a Na/K-ATPase inhibitor), and veratridine (a
modifier of Na channel inactivation).
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POSTTETANUS CALCIUM CLEARANCE IS NOT AFFECTED BY K-DEPOLARIZATION.
A simple explanation for the impeding effect of monensin (or ouabain)
on the posttetanus clearance is that [Na]i
loading inhibits the Na/Ca exchanger that normally plays a role in
posttetanus calcium extrusion. However, an alternative explanation
might be that the membrane depolarization produced by monensin or
ouabain (Leppanen and Stys 1997
) directly inhibits the
Na/Ca exchanger, which is electrogenic. This depolarization may be
minimal in low dosage of monensin (4 µM) since the action potential
amplitude was not appreciably affected (Fig. 7A). However,
in higher doses of ionophore (or ouabain), there was a ~30-50%
reduction of action potential that accompanies the retardation of the
posttetanus calcium decay. We therefore tested if a K-mediated membrane
depolarization can retard the posttetanus calcium clearance. To achieve
a similar depolarization of the resting membrane as in the case of
ionophore (or ouabain), the extracellular K was increased by 15 mM to
produce a ~50% reduction in the action potential. Figure
9 shows that tetanizing the nerves
in a solution with K elevated by 15 mM did not result in a slowing of
the posttetanus calcium decline (B), suggesting that
membrane depolarization cannot explain the retardation of posttetanus
decay seen in Na loading experiments.
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Na-free solutions and bepridil
Because we postulate that the Na/Ca exchanger is involved in
calcium extrusion after a tetanus, we should be able to slow the
extrusion by tetanizing nerves in a Na-free solution. The extrusion
efficacy of this exchanger is coupled to the transmembrane Na
concentration, which is normally high outside and low inside. We
therefore tetanized nerves in solutions in which Na was replaced by
lithium (Li). Li is permeable to Na channels and should support action
potentials. We found that the compound action potentials (both in
neonatal and in adult nerves) were gradually abolished in the Li-saline
solutions. However, at 10-15 min after Li application (before a
complete block of the action potentials), we found a approximate
twofold slowing of the posttetanus calcium decay, consistent with the
exchanger playing a role in the calcium extrusion (Fig.
10, A and B).
Next, we applied bepridil (10 µM), which has been suggested to
inhibit Na/Ca exchangers in ischemic optic nerves (Stys et al.
1995a
,b
). The compound action potentials also gradually declined in bepridil. However, we found an ~1.5-fold slowing of the
posttetanus calcium decay after bepridil application (Fig. 10,
A and B). Thus both the bepridil and Li
experiments suggest that the Na/Ca exchanger is involved in the
posttetanus calcium clearance.
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Figure 10 (A and B) summarizes effects of the various drug treatments on the posttetanus calcium decay according to two age groups, neonate (P5-P8) and adult (P60). In both age groups, pharmacological manipulations used to elevate axonal [Na]i (metabolic blocker ouabain, Na ionophore monensin, Na channel inactivation inhibitor veratridine) or to inhibit the Na/Ca exchanger (bepridil, Li+ replacement of bath Na+) all result in a retardation of the posttetanus calcium clearance.
ELEVATION OF AXONAL Na CAUSES AN INCREASE IN RESTING
CALCIUM INFLUX INTO AXONS.
The preceding studies suggest a coupling between axonal
[Na]i and calcium clearance following nerve
activity. In this section, we examined if axonal
[Na]i is also coupled to the resting axonal calcium level. As noted in the preceding text with regard to ouabain and monensin, application of these agents, in addition to retarding the
posttetanus calcium decline, also caused a rise in the resting axonal
[Ca2+]i. What are the
mechanisms underlying this rise in the resting calcium level? There are
at least three possibilities. First, increasing axonal
[Na]i may cause a depolarization, presumably by
increasing the sodium conductance of the membrane. This membrane depolarization could cause calcium channel activation, leading to
calcium influx into axons. Second, increasing axonal
[Na]i triggers calcium release from internal
stores (Mulkey and Zucker 1992
). Third, increasing
axonal [Na]i causes influx of calcium through
the Na/Ca exchanger when it is driven by intracellular Na accumulation
to operate in the reversed mode. To raise axonal [Na]i, we used ouabain and monensin (as used in
preceding studies), as well as veratridine (which activates a resting
Na influx by shifting the inactivation of the Na channels so that they
are open at the resting potential).
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), the resting
axonal [Ca2+]i rose to
F/F0 = 4 while the compound
action potential declined to ~40% of the normal value (A,
). By making the reasonable assumption that the decline in the
compound action amplitude is due to depolarization of the resting
membrane potential, we deduced that veratridine caused a larger calcium
influx (F/F0 = 4) than in
the K solution (F/F0 = 1.1)
but with less membrane depolarization (40% action potential remaining
in veratridine vs. 10% action potential remaining in the K solution).
This shows that most of the veratridine-induced calcium influx is
unrelated to voltage-gated calcium channels. The same conclusions were
reached for ouabain- and monensin-induced calcium influx in similar
studies (the corresponding values are F/F0 = 5.8 and
F/F0 = 3.6 for 30 µM
ouabain and 50 µM monensin, respectively). We believe that the most
likely candidate for the calcium influx pathway is the Na/Ca exchanger,
which is driven to run in the reverse mode under elevated axonal
[Na]i conditions.
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EFFECT OF MITOCHONDRIAL BLOCKERS.
Besides various calcium extrusion mechanisms located on the plasma
membrane (such as Na/Ca exchanger, Ca-ATPase), cytosolic calcium
buffers such as mitochondria may influence the decay kinetics of the
evoked calcium response. For example, Colegrove et al. (2000)
have recently shown that mitochondria in sympathetic
neurons participate in buffering fairly modest elevation in cytoplasmic calcium induced by depolarizations. We therefore examined the role of
mitochondria in the optic nerves by applying the mitochondrial blocker
carbonyl cyanide p-(trifluoromethoxy) phenylhydrazone (FCCP,
1 µM) or carbonyl cyanide m-chlorophenylhydrazone (CCCP, 1 µM) (Colegrove et al. 2000
; Fierro et al.
1998
).
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EFFECTS OF POSTTETANUS CALCIUM ELEVATION ON EXCITABILITY. Our analysis of axonal calcium reveals a prolonged phase of calcium elevation following a long tetanus (Fig. 6). An interesting issue is whether this protracted posttetanus calcium elevation has any physiological consequences on nerve excitability. We therefore measured posttetanus recovery of compound action potentials with or without calcium in the bath (Fig. 14). Mg2+ was added to replace the omitted calcium to minimize effects on the nerve excitability due to screening of surface charges. To produce significant posttetanus calcium elevation, we used a 5-min tetanus at 5 Hz. The amplitude of the compound action potentials was reduced at the end of the tetanus, to 49 and 39% of the control values for Ca-free and normal solutions, respectively (Fig. 14). The posttetanus recovery of the compound action potential is calcium dependent. In the case where calcium is present, the recovery occurred in an initial fast phase (~1 min) followed by a slow one that took ~20 min. In calcium-free bath solutions (i.e., no activity-dependent axonal calcium elevation), the two recovery phases are still present. However, fully recovery to the pretetanus level is achieved faster (~10 min). This suggests that the posttetanus axonal calcium elevation demonstrated in our calcium analysis modulates posttetanus excitability.
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DOES INTRODUCTION OF CALCIUM DYES DISTORT AXONAL CALCIUM SIGNALING? One potential source of uncertainty in this study is that the calcium dyes introduced in the axons might distort calcium signaling. We addressed this issue by using different concentrations of calcium dye in the loading, and by using low-affinity calcium dyes.
Different dye loading concentrations. One potential uncertainty in this study is the use of a very high concentration of high-affinity calcium dyes in the loading pipettes (2-8 mM of dextran-conjugated Oregon Green). The intra-axonal dye concentration at the site of optical recording may be excessively high, which could distort the kinetics of the calcium transients. However, as estimated earlier, the intra-axonal dye concentration at a typical recording site of ~540 µm from the loading pipette after a 3-h loading might be only in the order of ~0.013 of that in the loading pipette (2-8 mM), which translates to 26-104 µM. This intra-axonal dye concentration is clearly in line with other studies of the kinetics of calcium transients using high-affinity dyes, such as fura-2, where a known concentration of ~200 µM is introduced into the cells via a whole cell pipette (Fierro et al. 1998
|
F/F0 values than
high-affinity dyes, resulting in poor signal-to-noise ratios. Because
these two low-affinity indicators have a
Kd for calcium that is 35-117 times
less than the high-affinity dye, we conclude that the key observations
in this study are not artifacts of dye saturation.
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DISCUSSION |
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In this paper, we reported a method for selective staining of
axonal populations in the mouse optic nerves with calcium dyes and
argued, based on the use of a dextran-conjugated dye that is known to
be impermeable to gap junctions, and on the lack of an
adenosine-induced calcium response (the hallmark of glia), that we have
indeed successfully achieved selective axonal staining. We then applied
this method to examine several basic properties of calcium clearance
mechanisms in these axons and obtained two key observations regarding
the clearance mechanisms. The first observation is tetanus-dependent
calcium decay. A tetanus that elevates axonal calcium to a higher level
leads to a slower calcium clearance. Further, even from a similar
calcium level, the posttetanus calcium clearance is slower if it is
preceded by a larger number of action potentials. The second
observation is that inducing axonal Na loading with pharmacological
agents retards posttetanus calcium clearance as well as induces a
resting calcium influx into axons. We believe that our observations can
be explained by evoking the Na/Ca exchanger as a key player in calcium
homeostasis in the axons of the mouse optic nerves; the coupling of
calcium homeostasis to axonal [Na]i simply
reflects the dependence of the operation of the exchanger on the Na
gradient across the axolemma. Our postulated role for the Na/Ca
exchanger makes excellent functional sense given the intense staining
of the exchanger in the axons of the mammalian optic nerves
(Steffensen et al. 1997
).
Determinants of the shape of the posttetanus calcium decline
A key observation in this paper is that the posttetanus calcium
decline is multi-exponential, and its shape is dependent on the calcium
level and the action potential numbers during the tetanus. Posttetanus
slowing of the calcium decline is observed with both high and low
affinity calcium indicators, suggesting that it is not related to dye
saturation artifacts. Bi-phasic calcium decline following a
stimulus-induced calcium load has been observed in various neuronal
preparations, including terminals of pyramidal cells of rat neocortex
(Koester and Sakmann 2000
), mouse cerebellar Purkinje
cells (Maeda et al. 1999
), and presynaptic terminals of
cerebellar granule cells (Regehr 1997
).
What determines the shape of the calcium decline after a calcium load?
In general, uptake by mitochrondria, binding to endogenous axonal
calcium buffers, extrusion through axolemmal Ca-ATPase and Na/Ca
exchanger will jointly determine the shape of the posttetanus calcium
decline. As discussed by Koester and Sakmann (2000)
,
several factors may produce multi-exponential calcium decay. One is the existence of multiple species of endogenous calcium buffers. For example, Maeda et al. (1999)
suggested that the
bi-phasic calcium decline in Purkinje neurons can be explained by the
presence of two endogenous buffers, one with high affinity and the
other with low affinity. In their model, raising the calcium level to
different levels by increasing the intensity of the tetanus will lead
to various degree of saturation of the endogenous buffers, producing a
calcium decline whose shape is tetanus-dependent. In the optic nerve
axons, we found that increasing the tetanus duration makes the
bi-phasic calcium decline more prominent, particularly after 4-AP
treatment, which dramatically increases the calcium influx per action
potential. The complex calcium clearance time course in the mouse optic
nerve axons could be explained by the saturation of several distinct
as-yet-unidentified endogenous calcium buffer species. In neuronal
systems, strong candidates for endogenous buffers include the
calcium-binding proteins calbindin-D and parvalbumin. The nature of
endogenous buffers in the axons of the mammalian optic nerves has not
been explored.
Another factor that can influence the shape of the calcium decline at the site of influx is diffusion along the axoplasm to regions of low calcium. Such diffusion can act as spatial buffering to restore calcium level at the site of entry. After an axon has been fully myelinated, the tiny nodal gap (~1 µm) is presumably the site of local calcium influx. The two long internodes flanking the node might act as a large "low-calcium" sink to spatially dissipate a high calcium increase at the node. The diffusion of calcium ions away from the node to the internode, coupled with calcium extrusion at the node, may produce a multi-exponential calcium decline. However, this spatial diffusion is unlikely to explain the multi-exponential calcium decay seen also in premyelinated axons (P5-P7) where the calcium influx is likely to be uniform over the entire length of the axon.
Besides endogenous buffers and axial diffusion of calcium, saturation
of calcium extrusion mechanisms might also produce tetanus-dependent calcium decay (Blaustein 1988
). Of the two extrusion
pathways, Ca-ATPase and Na/Ca exchanger, which one might produce
tetanus-dependent calcium decline? Regehr (1997)
examined this issue with computer modeling of calcium decline in the
granule cell terminals. He found that Ca-ATPase extrusion does not
produce tetanus-dependent calcium decline. That is, increasing the
calcium level in the tetanus by increasing the action potential numbers
will not affect the shape of the posttetanus calcium decline if
Ca-ATPase is the sole source for calcium extrusion. This is contrary to
our observation. On the other hand, Regehr (1997)
shows
that extrusion through the Na/Ca exchanger will produce a
tetanus-dependent calcium decline. According to Regher's model,
following a calcium load, the Na/Ca exchanger will operate in the
extrusion mode to extrude calcium, which will cause the initial fast
decline in calcium. However, this extrusion also simultaneously brings
in Na, which causes axonal [Na]i to rise above
the normal, pretetanus level. The Na/Ca exchanger will rapidly reach a
new equilibrium, with a slightly higher axonal
[Na]i level and a higher axonal
[Ca]i level than the pretetanus level. As the
calcium load is progressively increased (as happens after 4-AP
treatment), the posttetanus axonal [Ca]i will
recover to a higher level. This predicts a persistent posttetanus calcium elevation whose amplitude should be proportional to the calcium
level at the start of the decline as indeed observed in Fig. 6. With
the participation of the Ca-ATPase in the extrusion process, this
posttetanus, persistent calcium elevation should be slowly dissipated.
Thus the behavior of the posttetanus calcium decline observed in this
study fits qualitatively with Regehr's model (Regehr
1997
), and argues for a role for Na/Ca exchanger in calcium
extrusion following nerve activity. This conclusion is clearly in line
with recent immunohistochemical data showing heavy staining of the
Na/Ca exchangers in axons of the rat optic nerves (Steffensen et
al. 1997
).
Na accumulation retards posttetanus calcium clearance
Regher's model (Regehr 1997
) cannot account for
our observation that increasing the number of action potentials also
can impede posttetanus decline, even under conditions where there is no
increase in the calcium level from which the decline begins. We
hypothesize that Na accumulation during tetanus retards posttetanus
calcium clearance. This would explain why under certain conditions, the posttetanus decline is dependent on the number of action potentials during the train and not on the calcium level reached at the end of the
train. This hypothesis is supported by the observation that elevation
of axonal [Na]i with pharmacological agents
does indeed retard posttetanus calcium decay. What kind of calcium clearance mechanism might be sensitive to axonal
[Na]i? Extrusion via the Na/Ca exchanger would
exhibit such a property. Calcium extrusion is coupled to the Na
gradient, and elevation of internal Na is known to inhibit the
exchanger (for review, see Stys et al. 1995
).
Alternatively, elevation of axonal Na might weaken the buffering
capacity of endogenous buffers or inhibit calcium uptake into
organelles, thus retarding the fall of free calcium in the axon.
However, such an effect of Na has not been described. Finally, calcium
clearance might be directly inhibited by the calcium elevation that
accompanies pharmacological elevation of axonal Na. It is unclear what
kind of calcium clearance mechanism might be inhibi