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The Journal of Neuroscience, August 1, 1999, 19(15):6372-6384
Depolarization-Induced Mitochondrial Ca Accumulation in
Sympathetic Neurons: Spatial and Temporal Characteristics
Natalia B.
Pivovarova1,
Jarin
Hongpaisan1,
S. Brian
Andrews1, and
David D.
Friel2
1 Laboratory of Neurobiology, National Institute of
Neurological Diseases and Stroke, National Institutes of Health,
Bethesda, Maryland 20892-4062, and 2 Department of
Neuroscience, Case Western Reserve University, Cleveland, Ohio
44106-4975
 |
ABSTRACT |
Several lines of evidence suggest that neuronal mitochondria
accumulate calcium when the cytosolic free Ca2+
concentration ([Ca2+]i) is
elevated to levels approaching ~500 nM, but the spatial, temporal, and quantitative characteristics of net mitochondrial Ca
uptake during stimulus-evoked [Ca2+]i
elevations are not well understood. Here, we report direct measurements
of depolarization-induced changes in intramitochondrial total Ca concentration ([Ca]mito)
obtained by x-ray microanalysis of rapidly frozen neurons from frog
sympathetic ganglia. Unstimulated control cells exhibited undetectably
low [Ca]mito, but high K+
depolarization (50 mM, 45 sec), which elevates
[Ca2+]i to ~600 nM,
increased [Ca]mito to 13.0 ± 1.5 mmol/kg dry
weight; this increase was abolished by carbonyl cyanide
p-(trifluoromethoxy) phenylhydrazone (FCCP). The
elevation of [Ca]mito was a function of both
depolarization strength and duration. After repolarization, [Ca]mito recovered to prestimulation levels with a time
course that paralleled the decline in
[Ca2+]i. Depolarization-induced
increases in [Ca]mito were spatially heterogeneous. At
the level of single mitochondria, [Ca]mito elevations depended on proximity to the plasma membrane, consistent with predictions of a diffusion model that considers radial
[Ca2+]i gradients that exist early
during depolarization. Within individual mitochondria, Ca was
concentrated in small, discrete sites, possibly reflecting a
high-capacity intramitochondrial Ca storage mechanism. These findings
demonstrate that in situ Ca accumulation by
mitochondria, now directly identified as the structural correlate of
the "FCCP-sensitive store," is robust, reversible, graded with
stimulus strength and duration, and dependent on spatial location.
Key words:
mitochondria; calcium; calcium signaling; calcium
regulation; neurons; depolarization; electron probe x-ray
microanalysis
 |
INTRODUCTION |
Classical studies have demonstrated
that isolated mitochondria from various tissues accumulate Ca via a
Ca2+-sensitive uniporter whose activity is
half-maximal when the extramitochondrial free Ca2+
concentration is ~10-20 µM (for review, see Gunter and
Gunter, 1994
). With improved methods for measuring cytosolic free
Ca2+ concentration
([Ca2+]i) (Grynkiewicz et al.,
1985
), it became clear that many physiological stimuli elevate global
[Ca2+]i to submicromolar levels and
that higher levels are achieved only after excessive stimulation. These
two lines of evidence led to the conclusion that mitochondria serve as
low-affinity Ca2+ buffers during Ca overload but do
not participate in the physiological control of
[Ca2+]i (Somlyo, 1984
; Carafoli et
al., 1995
). This conclusion was supported by the observation that in
some cells intramitochondrial Ca concentration rises only after
excessive stimulation (Moravec et al., 1997
; Horikawa et al.,
1998
).
Despite these observations, a growing body of evidence suggests that
mitochondria in various cells do accumulate Ca even when [Ca2+]i rises within the physiological
range (Babcock and Hille, 1998
; Miller, 1998
). Much of this evidence is
based on measurements of
[Ca2+]i, which provide only
indirect indications of mitochondrial Ca2+ transport
(Thayer and Miller, 1990
; Friel and Tsien, 1994
; White and Reynolds,
1995
; Drummond and Fay, 1996
; Herrington et al., 1996
; Hoth et al.,
1997
; David et al., 1998
; Peng, 1998
), although similar conclusions
have been reached using Ca2+ indicators that provide
estimates of intramitochondrial free Ca2+
concentration (Miyata et al., 1991
; Rizzuto et al., 1992
; Hajnoczky et
al., 1995
; Babcock et al., 1997
; Hoth et al., 1997
). Nevertheless, reversible elevations of the total Ca concentration in structurally identified neuronal mitochondria after stimuli evoking submicromolar [Ca2+]i elevations have not been
reported so far.
Sympathetic neurons contain an intracellular pool that accumulates
Ca2+ during membrane depolarization as
[Ca2+]i approaches ~500
nM. Ca2+ accumulation by this pool slows
the rise in [Ca2+]i and speeds the
initial phase of recovery that follows repolarization. Subsequent
Ca2+ release greatly prolongs the
[Ca2+]i recovery (Friel and Tsien,
1994
). Because Ca2+ sequestration by this pool is
inhibited by proton ionophores such as carbonyl cyanide
p-(trifluoromethoxy) phenylhydrazone (FCCP) that collapse
the mitochondrial membrane potential, the pool appears to be
mitochondrial. In the present study, we used energy-dispersive x-ray
(EDX) microanalysis (Hall and Gupta, 1983
; Somlyo, 1985
; Roomans, 1988
)
to measure directly depolarization-induced changes in the total Ca
concentration ([Ca]mito) within structurally identified mitochondria of sympathetic neurons. The measurements demonstrate that mitochondria accumulate Ca when
[Ca2+]i rises to levels as low as
~300 nM and that [Ca]mito elevations are
graded with stimulus strength and duration, blocked by FCCP, and
reversed on repolarization, with a recovery that parallels the decline
of [Ca2+]i. Moreover, mitochondrial Ca
accumulation is fast enough that activation of
Ca2+-sensitive mitochondrial dehydrogenases would be
expected within seconds of depolarization. Finally, the rise in
[Ca]mito is strikingly heterogeneous, both among and
within individual mitochondria.
Some of these results have been published previously in abstract form
(Andrews et al., 1998
; Pivovarova et al., 1998
).
 |
MATERIALS AND METHODS |
Cell dissociation and culture. Sympathetic ganglia
were obtained using a modification of a procedure described previously (Friel and Tsien, 1992
). In brief, adult male bullfrogs (Rana catesbeiana) were killed by decapitation and pithing, after which the sympathetic chains were removed, desheathed, and incubated, first
for 40 min at 35°C in low Ca2+ Ringer's solution
containing 3 mg/ml collagenase (Worthington, Type I) and subsequently
for 10 min in Ringer's solution supplemented with 1.5 mg/ml trypsin
(EC 3.4.21.4; Sigma, St. Louis, MO). All procedures conform with
guidelines established by our institutional animal care and use
committees. The composition of low Ca2+ Ringer's
solution was (in mM): 128 NaCl, 2 KCl, 10 HEPES, 10 glucose, pH adjusted to 7.3 with NaOH. The ganglia were then washed in
this solution with gentle trituration and transferred to normal Ringer's solution that contained 2 mM added
CaCl2. This procedure yielded individual ganglia consisting
of clusters of Schwann cell-free neurons tethered by their proximal
axons, with neurons resembling grapes on a vine. To obtain dissociated
cells, the ganglia were further triturated, and cells were plated onto
poly-lysine-coated coverslips and placed in primary culture as
described in Friel and Tsien (1992)
.
Cytosolic calcium measurements. To measure cytosolic free
Ca2+ concentration, cells were incubated with 3 µM fura-2 AM in normal Ringer's solution for ~40 min
at room temperature with gentle agitation followed by a rinse with
normal Ringer's solution. Fura-2 AM was dispensed from a 1 mM stock solution in DMSO containing 25% (w/w) pluronic
F127 (BASF Corporation). Fura-2 AM-loaded ganglia were transferred with
a fire-polished Pasteur pipette to poly-D-lysine-coated coverslips that were affixed with Sylgard (Dow Corning) to the underside of 60 mm culture dishes so that the coverslips covered 20 mm
holes in the dish. After ganglia settled onto the substrate, dishes
were placed on the stage of an inverted microscope (Nikon Diaphot TMD)
and superfused continuously (~5 ml/min) with normal (Ca2+-containing) Ringer's solution. Recordings
began ~20 min after washing away fura-2 AM, permitting
de-esterification of the Ca2+ indicator.
Depolarization-evoked [Ca2+]i changes
in single neurons within ganglia were made using cells from the
periphery of the ganglia that were attached to the substrate. Solution
changes (~250 msec) were made using a multi-tube system of
microcapillaries (Drummond microcaps, 20 µl) mounted on a micromanipulator.
Cells were illuminated with light from a 150 W xenon lamp that was
alternately filtered by bandpass filters (350 ± 5 nm, 380 ± 5 nm) mounted on a filter wheel rotating at 40 Hz and then focused by a
40× objective (Nikon, Fluor, NA 1.3). Emitted light passed through a
dichroic mirror (400 nm) and longpass filter (510/20 nm) and was
detected by a photomultiplier tube. The filter wheel was controlled by
a Cairn spectrophotometer, and data acquisition was controlled
by a laboratory computer. [Ca2+]i was
calculated according to the method of Grynkiewicz et al. (1985)
as
described previously (Friel and Tsien, 1994
).
Rapid freezing, cryosectioning, and electron microscopy.
Dispersed ganglia were transferred from normal Ringer's solution to
various test solutions in 35 mm culture dishes with a P-20 Pipetman
whose tips were cut off with a razor blade to give an opening (~1-2
mm) that was much larger than the diameter of the ganglia, thus
avoiding mechanical injury during transfer. After a ganglion was
incubated in a given test solution, it was incubated for 15 sec in
another dish containing the same solution supplemented with 5% (w/w)
polyvinylpyrrolidone (PVP-10), which served to increase the mass
content of the extracellular milieu. This step was also performed on
untreated control ganglia. Ganglia were then transferred to a freezing
stage consisting of a one-quarter-inch-diameter, ~500-µm-thick pad
of agar/gelatin (2%/2%, equilibrated with appropriate Ringer's
solution) mounted on an aluminum disk designed to fit the specimen
chuck of a Leica ultracryomicrotome, as described in Buchanan et al.
(1993)
. Just before freezing, excess saline was wicked away from the
edge of the ganglion with filter paper. Rapid freezing was carried out
by impact against an LN2-cooled copper block using a
modified LifeCell CF-100 freezing machine (The Woodlands, TX).
Cryosectioning of frozen ganglia was performed essentially as described
in Buchanan et al. (1993)
. In brief, cryosections (80 nm nominal
thickness) were cut with a Diatome cryodiamond knife (Diatome, Fort
Washington, PA) mounted in a Leica Ultracut S/FCS ultracryomicrotome
(Leica, Deerfield, IL) equipped with an antistatic device (Hauf Static
Line, Diatome). Sections were obtained as smooth, continuous ribbons
from the superficial, well frozen surface (<20 µm deep) of each
ganglion at less than
160°C and mounted on carbon/Formvar-coated
grids (EMS, Fort Washington, PA). Grids containing frozen-hydrated
sections were cryotransferred into a LEO EM912 Omega electron
microscope (LEO Electron Microscopy, Thornwood, NY), where they were
freeze-dried at approximately
100°C and recooled to less than
160°C before imaging and elemental analysis. Structural images of
freeze-dried sections were obtained as low-dose, zero-loss images,
recorded digitally by means of a calibrated ProScan slow-scan CCD
camera (1024 × 1024 pixels, LEO) and AnalySIS software
(Soft-Imaging Software GmbH, Munster, Germany). Distances measured on
images of cryosections were corrected for unrelieved
unidirectional compression that occurs during cryosectioning (Shi et al., 1996
) by means of DigitalMicrograph software (Gatan, Pleasanton, CA). Only sections through or near the equatorial plane of
these essentially spherical neurons (Pick, 1963
) were selected for
distance measurements.
For conventional electron microscopy, cultured cells were fixed in a
2% paraformaldehyde, 2% glutaraldehyde cacodylate buffer, pH 7.4, for
1 hr, washed 3 times, post-fixed in 1% OsO4 for 1 hr, and
then rinsed with distilled water. Cells were stained with 1% uranyl
acetate in distilled water for 1 hr, followed by dehydration, embedding
(Spurr's), and sectioning using standard procedures. Sections were
viewed and photographed using a JEOL 1200EX transmission electron
microscope (JEOL, Inc., Peabody, MA).
X-ray microanalysis. EDX microanalysis was performed as
described in Buchanan et al. (1993)
and Pozzo-Miller et al. (1997)
. In
brief, compartment-specific x-ray emission was elicited by focusing an
electron probe of ~5 nA beam current on morphologically selected
subcellular regions of sectioned neurons. The size of the probe was
small enough (diameter ~100 nm) to fit well within a typical
mitochondrion in section, but not so small that it would resolve
differences between the matrix and individual cristae. Such
measurements provide information about the spatial average of total Ca
concentration over ~104 nm2
regions of the mitochondrial matrix.
Spectra from single analyses were recorded for 100 sec at less than
160°C using a Linksystem Pentafet EDX detector (Oxford Instruments,
Concord, MA) and were subsequently processed and quantified by
established procedures (Shuman et al., 1976
; Hall and Gupta, 1983
;
Buchanan et al., 1993
; Pozzo-Miller et al., 1997
) as implemented by the
program NIST/NIH DeskTop Spectrum Analyzer (DTSA) for the Macintosh
(C. E. Fiori, C. R. Swyt, and R. Mykelbust, available at
http://micro.nist.gov/DTSA/dtsa.html). The Simplex fitting routine and
the Hall peak/continuum method were used to quantify the
total elemental concentrations of Na, Mg, P, S, Cl, K, and
Ca. This procedure directly provides total (i.e., free plus bound)
elemental concentrations (Cdry) in units
of millimoles per kilogram dry weight. Conversion to concentrations in
millimoles per liter of water-accessible volume
(Caq) was performed according to the
following formula:
|
(1)
|
where fw is the fractional water weight
and
is the density of the cellular compartment under consideration.
The basis for this approach, as well as the underlying assumptions, is
discussed by Roomans (1988)
. Values of fw for
mitochondria (0.60) and cytosol (0.88) were estimated on the basis of
the continuum x-ray emission of EDX spectra and are consistent with
literature data (cf. Buchanan et al., 1993
; Andrews et al., 1994
),
taking
= 1.0 for both mitochondria and cytosol:
|
(2)
|
|
(3)
|
Statistics. Population measurements are expressed as
mean ± SEM (n), where n is the number of
individual measurements. Typically, measurements from 5-15
mitochondria or cytosolic regions were performed in each of 11-13
neurons taken from three to four ganglia per experimental condition.
The overall variability of elemental concentrations reflected
differences within regions of individual cells, differences between
cells and ganglia, and instrumental variability. Analysis of errors
showed that instrumental variability and cell-cell variability were
negligible compared with regional variability within individual cells.
Statistical significance was assessed using Student's t
test (two-tailed).
Computer simulations. Simulations were based on a
model of Ca transport in sympathetic neurons described in Friel and
Tsien (1994)
. Mitochondrial Ca transport was represented by a
[Ca2+]i-sensitive unidirectional
uptake pathway operating at constant membrane potential, which gives a
flux (per unit volume) that is proportional to
[Ca2+]i, with a proportionality
factor that increases sigmoidally with [Ca2+]i
(kmax = 165 × 103/sec, EC50 = 10 µM, nHill = 2).
Ca2+ release was described by a saturable efflux
pathway (Vmax = 300 nM/sec,
EC50 = 3 µM,
nHill=1), and a small linear leak (rate constant 0.2 × 10
9/sec). Plasma membrane
Ca2+ extrusion was represented by a linear pump and
leak (rate constants 0.3/sec and 5 × 10
6/sec) and Ca2+ entry was
described by an inactivating Ca2+ current
ICa(t) = Ifaste
t/
fast + Islowe
t/
slow + Iss, where
Ifast = 4 nA,
Islow = 0.5 nA, Iss=
20 pA,
fast = 80 msec,
slow = 500 msec. Diffusion was modeled as in Sala and Hernandez-Cruz (1990)
but with a single diffusible cytosolic Ca2+ buffer
(on and off rate constants 108 M/sec and
1000 sec, total concentration 1 mM, diffusion coefficient 0.5 × 10
6 cm2/sec).
Mitochondria were assumed to be uniformly distributed and to occupy a
fractional volume of 0.05, in keeping with morphometric analysis of our
electron micrographs, as well as those in the literature (Pick, 1963
).
A single nondiffusible intramitochondrial Ca buffer was included with
the same on and off rate constants as the cytosolic buffer but a
10-fold higher total concentration (10 mM). Simulated
responses to Ca2+ entry depend on the distribution
of mitochondria but are largely insensitive to the properties of the
intramitochondrial Ca buffer. Changes in buffer characteristics have
little effect, because during stimulation Ca2+
accumulation is dominated by (unidirectional) uptake. For simplicity, it was also assumed that mitochondria are stationary within the cell;
mobility and remodeling of these organelles would be expected to
partially dissipate spatial [Ca]mito gradients. The model
cell was assumed to be spherically symmetrical (radius 30 µm) and was represented as a series of 60 0.5-µm-thick shells. It was assumed that for a given distance from the plasma membrane, all
intramitochondrial species (free and bound Ca and buffer) are
distributed uniformly. Integration step size was 1 µsec.
Chemicals and drugs. Concentrated aliquots of FCCP
(10 mM) in 100% ethanol were stored at
80 C° and
diluted in normal Ringer's solution just before each experiment.
Fura-2 AM was obtained from Molecular Probes (Eugene, OR). Unless
indicated otherwise, all reagents were obtained from Sigma and EMS.
 |
RESULTS |
Pharmacological evidence implicating mitochondrial
Ca2+ transport during depolarization-evoked Ca
responses
Sympathetic neurons respond to membrane depolarization with a rise
in [Ca2+]i that is initiated by
Ca2+ entry through voltage-gated
Ca2+ channels but is strongly influenced by
Ca2+ uptake and release by intracellular stores.
Pharmacological evidence for mitochondrial Ca2+
transport during these responses is illustrated in Figure
1. Exposure to 30 mM
K+, which steadily depolarizes
Vm from a resting potential of approximately
70 mV to approximately
35 mV (Friel and Tsien, 1992
), elevates [Ca2+]i from a resting level of
~50-80 nM to ~200-300 nM (Fig.
1a, left); repolarization initiates a recovery
with a simple time course. In the presence of the proton ionophore
FCCP, the same stimulus elicits a
[Ca2+]i response (Fig. 1a,
right) that is very similar to the control response.

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Figure 1.
Comparison between
[Ca2+]i responses elicited by weak and
strong depolarization and their sensitivity to FCCP in fura-2 AM-loaded
sympathetic neurons. a,
[Ca2+]i responses from a sympathetic
neuron in primary culture elicited by weak depolarization (30 mM K+) before (left) and
after (right) treatment with 1 µM FCCP.
b, [Ca2+]i responses
elicited from the same cell by stronger depolarization (50 mM K+) before (left) and
after (right) treatment with 1 µM FCCP. In
this cell, the initial rate of recovery after repolarization was 71
nM/sec in the absence of FCCP, whereas the rate of decline
in the presence of FCCP measured over the same range of
[Ca2+]i was 18 nM/sec.
Collected results indicate that FCCP slows the rate of recovery to
~14% of the control value (from 121 ± 15 nM/sec
to 17 ± 3 nM/sec; n = 11)
measured over the same range of
[Ca2+]i. Cell b13j.
c, [Ca2+]i response
recorded from a cell (b16f) on the periphery of a ganglion like those
used in this study for EDX microanalysis. This ganglion was treated
enzymatically according to the same procedure used to prepare
dissociated cells, but cells were not dispersed by trituration.
|
|
In contrast, stronger depolarizations induced by exposure to 50 mM K+, which depolarizes
Vm to approximately
20 mV (Friel and Tsien, 1992
), elicit larger [Ca2+]i
elevations followed by complex recoveries that are strongly modified by
FCCP. In the absence of FCCP (Fig. 1b, left),
such depolarizations elevate [Ca2+]i
to ~500-800 nM, whereas repolarization initiates a
recovery consisting of an initial rapid decline followed by a slow
plateau phase that lasts for many seconds. Similar response kinetics
are observed when [Ca2+]i is elevated
by other means, including trains of stimulated action potentials (Friel
and Tsien, 1994
) and voltage-clamp depolarization (data not shown). In
the presence of FCCP, the same stimulus elevates [Ca2+]i to a much higher level, and
the subsequent recovery occurs without the fast and slow phases seen in
control responses (Fig. 1b, right). It is
unlikely that these effects of FCCP reflect reduced ATP availability
and suppression of ATP-dependent Ca2+ extrusion
because FCCP does not alter resting
[Ca2+]i, and overall recoveries
are speeded, not slowed, by the drug. Taken together, these
observations implicate Ca2+ uptake and release by an
FCCP-sensitive intracellular store, presumably mitochondrial, that
becomes increasingly influential as
[Ca2+]i rises above several hundred
nanomolar. According to this idea, net Ca2+
accumulation by the store blunts the rise in
[Ca2+]i during depolarization and
speeds the initial phase of recovery after repolarization, with net
Ca2+ release slowing the return of
[Ca2+]i to its resting level. Similar
observations have been reported for a variety of excitable cells
(Babcock and Hille, 1998
; Miller, 1998
).
The interpretation described above is indirect and relies on the
mitochondrial specificity of FCCP. To determine directly whether
membrane depolarization causes reversible mitochondrial Ca
accumulation, EDX microanalysis was used. This approach requires a cell
preparation that can be rapidly frozen and cryosectioned. To this end,
sympathetic ganglia were treated enzymatically as in the preparation of
dissociated cells but were not dispersed by trituration. This procedure
yielded clusters of neurons whose individual response properties
closely resembled those of cells in primary culture. For example,
Figure 1c illustrates a
[Ca2+]i response induced by 50 mM K+ from a fura-2 AM-loaded cell on
the periphery of such a ganglion (a location similar to that from which
cells were cryosectioned for microanalysis). This response was
essentially indistinguishable from those elicited from single cells in
culture, with quantitative differences being well within the range of
cell-to-cell variability. Similar responses were seen in five of
five cells. Therefore, ganglia prepared in this way were used for EDX
microanalysis in the following experiments.
Subcellular structure and elemental composition of
sympathetic neurons
The appearance and subcellular distribution of mitochondria in
cultured sympathetic neurons as seen using conventional fixation procedures is illustrated in Figure
2A, whereas Figure
2B shows a freeze-dried cryosection from a rapidly
frozen ganglion, prepared as described above without chemical fixation
or staining. In both preparations, mitochondria can be readily
identified by their characteristic electron density, shape, size
(~200 nm in cross section, of variable length), and distribution. The
extent to which mitochondria of sympathetic neurons exist as an
interconnected reticulum is unknown. If they do form a continuous
network, it is perhaps more accurate to refer to mitochondrial profiles
in section as "local regions of the mitochondrial network" rather than "individual mitochondria." The distinction is not material to
the results of this study, however, and so we shall use the term
"individual mitochondria" as a convenient formalism.

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Figure 2.
Subcellular structure of sympathetic neurons.
A, Transmission electron micrograph of conventionally
prepared thin section of chemically fixed, plastic embedded neuron
under resting conditions. Field illustrates typical peripheral region
of the neuronal soma. Cytoplasm contains numerous, polymorphic
mitochondria (arrows) and a rich network of small
cisterns of endoplasmic reticulum (arrowheads).
B, Digital transmission electron micrograph (1024 × 1024) of freeze-dried cryosection prepared from superficial neuron
of an unfixed, rapidly frozen sympathetic ganglion. Micrograph was
recorded at low dose in the zero-loss mode of an energy-filtering
cryoanalytical electron microscope at approximately 170° C by means
of a slow-scan CCD camera. Image of cryosection reveals the same
organelles and same subcellular organization as in the reference-fixed
preparation. Inset, White dot on
enlargement of one mitochondrion indicates the relative size of
100-nm-diameter electron probe used for EDX analysis. Scale bars, 1 µm.
|
|
In cryosections of rapidly frozen cells, all elements remain
distributed essentially as they were at the instant of freezing, making
them suitable for quantitatively analyzing the elemental composition of defined subcellular compartments. Figure
3a shows representative EDX spectra recorded from similar 100-nm-diameter regions of cytosol and mitochondria (thin and thick traces,
respectively) in freeze-dried cryosections of resting neurons
maintained in normal Ringer's solution before freezing. These spectra
exhibit large peaks corresponding to the characteristic
K
,
x-ray lines for the abundant elements P
and K, smaller peaks for the other major elements Na, Mg, S, and Cl,
and a slowly varying background, the continuum, that is proportional to
the dry mass of the target cell compartment. Quantitative analysis of
such spectra (see Materials and Methods) provides total dry weight
concentrations of all cellular elements between Z = 11 (Na) and Z = 20 (Ca), as summarized by the collected
results for selected elements in Table 1.
These data indicate that the neurons maintained an appropriate
nonequilibrium distribution of Na and K across the plasma membrane
(extracellular concentrations of K+ and
Na+ were 2 and 128 mM, respectively).
Calculation of the cytoplasmic [K+]/[Na+] ratio gives
950/31
30; conversion to millimoles per liter cell water (see
Materials and Methods) gives [K]cyto = 133 mM and [Na]cyto = 4.3 mM,
both values being typical for living cells.

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Figure 3.
Detection and quantitation of changes in
[Ca]mito by elemental analysis. a, EDX
spectra recorded from typical areas (<104
nm2, size indicated by white dot on
mitochondrion in Fig. 2b, inset) of
cytoplasm (fine line) and mitochondrial matrix
(heavy line) within cryosectioned neurons from a control
ganglion. Spectra are plots of the number of binned x-ray counts versus
energy (resolution 10 eV per channel). So-called characteristic peaks
identify individual elements, and the integrated counts for each peak
are proportional to the amount of that element. Elements corresponding
to the major characteristic K-shell x-ray peaks are identified; in the
case of K and Ca, two K-shell transitions arising from alternative
electronic transitions are resolved, indicated as
K and K
according to standard spectroscopic notation. Spectra in
a, representing the sum of eight individual spectra each
recorded for 100 sec at a beam current of ~4.0 nA, illustrate typical
distributions of major elements in living neurons. Note the
approximately twofold difference in the slowly varying continuum
radiation, e.g., between 1.50 and 1.75 keV, which reflects differences
in the mass density of these cellular compartments. b,
Mitochondrial EDX spectrum (sum of 10 individual spectra, each recorded
for 100 sec) over the energy range 3.0-4.2 keV (dashed box
in a) recorded under control conditions. Superimposed are
best-fit Gaussians for the K K plus
K peaks (dotted curve)
obtained as described in Materials and Methods. Vertical
lines indicate energies of the K and Ca lines.
c, Residual spectrum, obtained by subtracting the
calculated K K and
K counts from the experimental spectrum,
indicates the absence of resolvable Ca peaks. d,
Mitochondrial EDX spectrum (sum of 11 individual spectra, 100 sec each)
recorded from a ganglion after a 45 sec exposure to 50 mM
K+. Dotted and dashed
traces show best-fit Gaussians for characteristic K and Ca
peaks, respectively. e, Difference spectrum illustrating
contributions from the Ca K and
K peaks. The mean depolarization-induced
elevation in [Ca]mito over these 11 mitochondria was
~25 mmol/kg dry weight.
|
|
It is apparent from Figure 3a that a distinct x-ray peak for
Ca is not evident under resting conditions. This reflects an intracellular K concentration that is typically 100-fold greater than
the Ca concentration, combined with overlap between the potassium K
and calcium K
peaks (centered at 3.59 and 3.69 keV, respectively). Figure
3b shows the 3.0-4.2 keV region of the mitochondrial x-ray
spectrum along with the fitted potassium peaks
(K
and K
, dotted
trace). If the fitted curve is subtracted from the spectrum, the
resulting residual spectrum (Fig. 3c) is flat, indicating
that the peaks in this energy range can be completely accounted for by
K. The minimum concentration of total Ca that can be detected with this
technique is ~0.4 mmol/kg dry weight (Kitazawa et al., 1983
, Somlyo,
1985
; Andrews et al., 1994
; Moravec et al., 1997
), which places an
upper limit on [Ca]mito of resting sympathetic neurons in
our preparation of ~250 µmol/l water-accessible matrix volume.
Assuming that the ratio of total to free Ca concentration within
mitochondria is ~4000 (Babcock et al., 1997
), this would correspond
to a resting [Ca2+]mito of 250 µM/4000 ~ 63 nM, in rough
agreement with literature estimates of 100-200 nM
[summarized in Babcock et al. (1997)
].
Effects of 50 K+ depolarization on total
mitochondrial and cytosolic Ca concentrations
To evaluate the effects of depolarization on mitochondrial calcium
concentration, sympathetic ganglia were exposed to high K+ Ringer's solution (50 mM
K+, equimolar substitution of
Na+) and then rapidly frozen. A
depolarization-induced rise in [Ca]mito is apparent by
inspection of the relevant EDX spectra. Figure 3d shows the
3.0-4.2 keV region of a spectrum representing measurements from 11 mitochondria at the end of a 45 sec exposure to 50 mM K+. After stimulation, the peak in the 3.5-3.8 keV
range was broadened and shifted to the right; this occurs because of
overlap between the K K
peak and a
newly appearing Ca K
peak (dotted and dashed
traces, respectively, with peaks at 3.59 and 3.69 keV, respectively).
Subtraction of the fitted K peaks from the original spectrum in Figure
3d reveals a prominent peak centered at the Ca
K
line (Fig. 3e), indicating that
membrane depolarization leads to a resolvable increase in the total
mitochondrial Ca concentration. Collected results from sympathetic
ganglia after a 45 sec exposure to 50 mM
K+ Ringer's solution are shown in Figure
4 (also see Table 1). Total mitochondrial
Ca concentration was undetectably low in resting cells (
0.4 ± 0.2 mmol/kg dry weight; n = 107) but was elevated to
13.0 ± 1.5 mmol/kg dry weight by depolarization
(n = 77; significantly higher than control,
p < 0.01) (Fig. 4a). The
depolarization-induced rise in [Ca]mito was prevented by
treatment with 1 µM FCCP ([Ca]mito = 0.6 ± 0.7 mmol/kg dry weight; n = 28; not
significantly elevated compared with control).

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Figure 4.
Depolarization-induced calcium entry elevates
mitochondrial and cytosolic total calcium concentrations. Collected
results describing the effects of depolarization on total mitochondrial
(a) and cytosolic Ca concentrations (b).
Ganglia were exposed to 2 mM K+
Ringer's solution (Control) and then to 50 mM K+ for 45 sec, either in the absence
(50 K) or presence of 1 µM FCCP
(50 K+FCCP). FCCP was applied 2 min before
depolarization and remained until the instant of freezing.
Results show mean ± SEM over the indicated number of
individual measurements, in each case taken from three or more
different ganglia. Statistical significance of the difference relative
to control values is indicated by ** (p < 0.01) or * (p < 0.05).
|
|
Parallel measurements of cytosolic total Ca2+
concentration ([Ca]cyto) are shown in Figure
4b. Under resting conditions, [Ca]cyto was
3.3 ± 1.0 mmol/kg dry weight (n = 59), higher
than [Ca]mito, and increased during depolarization
to 7.3 ± 1.1 or 6.9 ± 1.5 mmol/kg dry weight
(n = 81) in the absence or presence, respectively, of
FCCP. These results demonstrate that during depolarizations that
elevate [Ca2+]i to ~500-800
nM and [Ca]cyto to levels of ~7 mmol/kg dry
weight, [Ca]mito rises in an FCCP-sensitive manner to
concentrations in excess of 10 mmol/kg dry weight. Given that resting
[Ca2+]i is ~65 nM in
these cells, it is also possible to estimate the ratio of total to free
cytosolic Ca as ~(0.14 × 3.3 × 10
3)/(65 × 10
9) = 7000 (±30%). Therefore, under resting conditions >99.9% of Ca
within the cytosol is bound. A similar calculation of the total to free
cytosolic Ca ratio after depolarization gives a value of ~1500. The
fact that [Ca2+]i and
[Ca]cyto increase in a nonlinear manner hints at
saturation of endogenous cytosolic Ca2+ buffers.
Nonlinear buffering may also explain, at least in part, the observation
that although FCCP-treated cells exhibit larger [Ca2+]i responses than untreated
controls (Fig. 1), they do not respond with a proportionate increase in
[Ca]cyto (Fig. 4b). Assuming a simple linear
buffering model, [Ca]cyto in the presence of FCCP should
have risen to ~11 mmol/kg, which would have been detectable, given
the precision of the present cytosolic EDX measurements. Failure to
detect a significant increase in [Ca]cyto under these conditions implies that with larger cytosolic Ca2+
loads, a larger fraction of entering Ca2+ remains
free. These points remain speculative, and a definitive demonstration
of this and related possibilities requires further investigation.
Time- and voltage-dependence of depolarization-evoked
[Ca]mito elevations
Longer depolarizations lead to larger elevations in
[Ca]mito. For example, a 2 min exposure to 50 mM K+, which raises
[Ca2+]i to ~500-800 nM
(Fig. 5a), elevates average
[Ca]mito to 32.7 ± 5.1 mmol/kg dry weight
(n = 114) (Fig. 5b, Table 1); this is more
than twice the level reached after a 45 sec depolarization (13.0 ± 1.5 mmol/kg dry weight). After repolarization,
[Ca]mito recovers within 2-5 min, reaching in 5 min a
level (0.8 ± 0.4 mmol/kg dry weight; n = 93) that
is indistinguishable from the prestimulation value. Therefore, the rise
in [Ca]mito evoked by depolarization is completely
reversible. [Ca]mito recovers with a time course that is
similar to the [Ca2+]i recovery after
depolarizations of the same strength and duration in single cells (Fig.
5a), providing good evidence that the
[Ca2+]i recovery is slowed, at least
in part, by Ca2+ release from loaded
mitochondria.

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Figure 5.
Comparison between the time courses of
[Ca2+]i,
[Ca]mito, and [Na]mito during and
after depolarization. a, Typical
[Ca2+]i response elicited by exposing
a single cultured cell to 50 mM K+ for 2 min. b, Collected results (mean ± SEM) showing how
[Ca]mito responds to 50 mM
K+ ( ) or 30 mM K+
( ). Ganglia were exposed to the indicated concentrations of
K+ for either 45 or 120 sec and then were rapidly
frozen. Using another population of ganglia, a 120 sec exposure to 50 mM K+ was followed by a 2, 5, or 15 min
recovery period during which ganglia were incubated in normal Ringer's
solution, followed by rapid freezing. For a given depolarization
strength, the rise in [Ca]mito increased with the
duration of depolarization, and for a given stimulus duration,
[Ca]mito increased with stimulus strength.
c, The rise in [Ca]mito was accompanied by
a reversible increase in [Na]mito, whose peak
magnitude was also graded with depolarization strength and
duration.
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|
The observed rate of mitochondrial Ca accumulation is consistent with
known properties of mitochondrial Ca2+ transport.
Our measurement of ~33 mmol/kg dry weight after a 2 min
depolarization converts to ~0.37 nmol/mg mitochondrial protein per
second (assuming that protein accounts for ~75% of
mitochondrial dry weight). This is compatible with published rates of
Ca2+ uptake by the uniporter, e.g., 0.2 nmol/mg
protein per second by liver mitochondria at
150 mV in the presence of
1 µM Ca2+ (Gunter and Pfeiffer, 1990
).
Maintained over several seconds, this rate of uptake would be
sufficient to activate Ca2+-sensitive dehydrogenases
in heart mitochondria (Gunter et al., 1994
). It is interesting to note
that, consistent with the remarkable Ca buffering capacity of isolated
mitochondria (Gunter and Gunter, 1994
), mitochondrial
Ca2+ accumulation continues at a nearly constant
rate even 120 sec after the onset of depolarization, when
[Ca2+]i is 554 ± 88 nM (n = 5). The observation that during
maintained depolarization mitochondrial Ca2+
accumulation continues despite a nearly steady elevation in
[Ca2+]i indicates that under these
conditions Ca2+ accumulation nearly balances net
Ca2+ entry across the plasma membrane, as proposed
by Friel and Tsien (1994)
.
Weak depolarizations also elevate [Ca]mito. For example,
a 45 sec exposure to 30 mM K+ produces a
small elevation in [Ca]mito to 3.0 ± 0.4 (n = 113), whereas longer exposures (120 sec) elevate
[Ca]mito to levels that are similar to those seen after a
45 sec exposure to 50 K+ (Fig. 5b). This
is interesting in view of the observation that FCCP has little or no
effect on small [Ca2+]i responses
induced by 30 K+ depolarization (Fig.
1a). We will return to this point in Discussion.
Neuronal mitochondria release Ca2+ principally via a
Na+/Ca2+ exchanger that couples
energetically uphill Ca2+ release with downhill
Na+ uptake driven by its strong electrochemical
gradient (Gunter and Gunter, 1994
). During the 2 min exposure to 50 mM K+, [Na]mito rose from
11 ± 2 to 34 ± 1 mmol/kg dry weight (Fig. 5c),
equivalent to a rise in [Na+]mito from
7 ± 1 to 23 ± 1 mmol/l matrix water (assuming that only an
insignificant fraction of Na+ ions are bound). This
elevation was reversed on repolarization, with [Na]mito
declining to its resting level roughly in parallel with
[Ca]mito. These parallel changes in
[Ca]mito and [Na]mito are consistent with
coupled movements of Na+ and
Ca2+, presumably reflecting operation of the
mitochondrial Na+/Ca2+ exchanger.
Spatial heterogeneity of depolarization-evoked elevations
in [Ca]mito
The [Ca]mito results presented so far reflect
averages of measurements taken from many mitochondria from different
cells and ganglia. These measurements were obtained using a
100-nm-diameter electron probe, with generally 10 or more mitochondria
sampled per cell. This sampling strategy provides an estimate of
[Ca]mito averaged over whole cells. However, frequency
histograms illustrating how [Ca]mito is distributed over
the entire population of analyzed mitochondria indicate that the
distribution is more complex than can be adequately conveyed by
population averages (Fig. 6). Under resting conditions, [Ca]mito was normally distributed
near zero with a small dispersion (Fig. 6a). After
depolarization, the distribution was skewed toward higher
[Ca]mito, reflecting the emergence of a
subpopulation of mitochondria with elevated [Ca]mito
(Fig. 6b). This subpopulation appeared as a pronounced
shoulder on the distribution, with a tail extending to values of
[Ca]mito well over 100 mmol/kg dry weight. At the same
time, some mitochondria continued to exhibit low [Ca]mito
levels much like those seen in unstimulated cells. After a 5 min
recovery period, the distribution of [Ca]mito closely resembled that seen before stimulation (Fig. 6c).

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Figure 6.
Frequency distributions of [Ca]mito
reveal intermitochondrial heterogeneity during depolarization.
a, [Ca]mito in resting neurons is low and
normally distributed with no detectable differences between cells or
between individual mitochondria within a given cell. Smooth
curve represents fitted Gaussian with mean and SD 0.6 and 3.6 mmol/kg dry weight, respectively. b, Collected results
from 114 mitochondria from 12 cells illustrating the distribution of
[Ca]mito after a 2 min, 50 K+
depolarization. All 12 cells tested responded in a qualitatively
similar manner. The skewed distribution of mitochondrial responses
persists into the recovery phase, as revealed by a continued nonuniform
distribution of [Ca]mito at 2 min after repolarization
(data not shown). c, At 5 min after repolarization, the
[Ca]mito distribution is indistinguishable from that
observed in control neurons. Mean and SD for fitted Gaussian are 0.14
and 3.1 mmol/kg dry weight.
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|
The skewed distribution of [Ca]mito observed during
depolarization could reflect (1) cell-to cell variability, (2)
intracellular differences in mitochondrial Ca2+
accumulation arising from nonuniformities in local
[Ca2+]i or mitochondrial energetics,
or (3) heterogeneity in the spatial distribution of Ca within
individual mitochondria resolved by the 100-nm-diameter electron beam.
It is possible that all three factors contribute to the observed
distribution of [Ca]mito. The similarity of
depolarization-induced mitochondrial responses found in all 12 cells
examined implicates [Ca]mito heterogeneity within individual cells. To examine this point in more detail,
[Ca]mito was measured in multiple mitochondria from
individual cells. If the dispersion of the collected results reflects
intracellular mitochondrial heterogeneity, then single-cell
distributions should resemble the collected results. Alternatively, if
cell-to-cell variability is dominant, single-cell distributions of
[Ca]mito should be narrow (as in Fig. 6a),
with mean [Ca]mito varying widely among cells. Figure
7a shows a tracing of an
equatorial section containing 45 analyzed mitochondria from a
representative neuron after a 45 sec, 50 mM
K+ depolarization. Figure 6b shows the
distribution of [Ca]mito over this population of
mitochondria. The similarity between this distribution and the results
in Figure 6b indicates that a significant contribution to
the variability of [Ca]mito in the collected results arises from differences between individual mitochondria in single cells
(or between different regions of the mitochondrial network).

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Figure 7.
Heterogeneity of [Ca]mito responses
in a single cell. a, Tracing indicating spatial
distribution and location of 45 mitochondria within a cryosection of a
single representative neuron that was frozen after a 45 sec exposure to
50 mM K+. Much of the plasma membrane
was present in this section, and the position of the nucleus was clear
because although it was torn away in this particular section (indicated
by Cut Edge), it was present in an adjacent fragment of
the same section. These characteristics, together with the diameter of
the neuronal profile (~25 µm), ensure that the section was taken
from near the equatorial plane of the cell. Numbers
identify specific mitochondria in c and
d. Thirty-three of these could be analyzed in two or
three different intramitochondrial locations. b,
Frequency distribution of [Ca]mito in this cell is
similar to that for the collected results representing mitochondria
from many cells under the same conditions (Fig. 6b).
c, Plot of [Ca]mito versus distance from
the plasma membrane ( ) showing dependence on proximity to the plasma
membrane. Distances were corrected for section compression as described
in Materials and Methods. Because these measurements were performed
only on equatorial sections, it is unlikely that a given mitochondrion
was close to regions of the plasma membrane that were out of the plane
of section. Filled squares show the mean ± SEM
calculated over five contiguous 2.5 µm subintervals.
d, Histograms of [Ca]mito measurements
from 10 of the 26 mitochondria that were analyzed at three separate
intramatrix locations; these 10 were selected because they span the
range of distances and are representative of the entire population. The
intramitochondrial regions selected were near the two extremities and
the center. Given that a typical mitochondrial profile was rarely
longer than 3 µm, the spacing between analyzed regions was usually 1 µm or less. Large differences in [Ca]mito are evident
within each of these mitochondria, indicating pronounced spatial
heterogeneity of [Ca]mito within individual organelles.
Similar results were obtained in each of four cells.
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|
One possible explanation for the intracellular heterogeneity of
[Ca]mito is provided by the analysis illustrated in
Figure 6c, which shows how [Ca]mito varies
with distance from the plasma membrane. A decline in
[Ca]mito with increasing distance from the plasma
membrane can be demonstrated by averaging [Ca]mito from
mitochondria in contiguous 2.5 µm subintervals and comparing the
means (Fig. 7c,
). For example, average
[Ca]mito in the shell closest to the plasma membrane
(43.5 ± 7.3 mmol/kg dry weight; n = 11 mitochondria) is significantly higher than the average over the shell
furthest from the plasma membrane (12.2 ± 2.9 mmol/kg dry weight;
n = 12 mitochondria; p < 0.0005). The
basis for this form of intermitochondrial heterogeneity is unclear, but
it could reflect mitochondrial proximity to cell surface Ca channels or differential regulation of mitochondrial energetics in a way that depends on distance from the plasma membrane.
Figure 7c indicates that there is still appreciable
variability between [Ca]mito measurements even when they
are taken from mitochondria that are similarly distant from the plasma
membrane, indicating that there are additional factors contributing to
the dispersion of [Ca]mito. To assess the uniformity of
the Ca distribution within individual mitochondria, the 33 largest
mitochondria from the section shown in Figure 7a were each
analyzed in two or three maximally spaced, nonoverlapping
100-nm-diameter regions within the same mitochondrion. Figure
7d shows the distribution of [Ca]mito within
10 selected but representative mitochondria in which three measurements
were made; corresponding spatial averages of [Ca]mito are
indicated in c. In virtually every mitochondrion, regions of
high [Ca]mito co-exist near regions of low
[Ca]mito. Heterogeneity of [Ca]mito within
mitochondria was evidently more pronounced in peripheral organelles,
where the spatially averaged [Ca]mito was also higher.
Such heterogeneity explains, at least in part, the scatter in Figure
7c. If intramitochondrial Ca is concentrated in small
regions that are distributed at moderate or low density, such regions
could be missed by a randomly placed 100 nm probe. This would occur
even in mitochondria with the highest spatially averaged
[Ca]mito. Thus, more detailed quantitative information about the way [Ca]mito declines with distance from
the plasma membrane will require higher spatial resolution and better
sampling than is practical with EDX analysis, perhaps using mapping techniques.
For those analysis sites with the highest [Ca]mito (>200
mmol/kg), there was a significant correlation between
[Ca]mito and [P]mito (r = 0.97, molar ratio ~1:1), but this correlation was weak at lower
[Ca]mito, possibly because of contributions from matrix phosphorus in regions between sites of high
[Ca]mito. Local regions of high [Ca]mito
were not observed in cells from ganglia that had not been depolarized
or that were depolarized (50 K+, 2 min) and then
allowed to recover for
5 min in normal Ringer's solution (11 cells),
indicating that the foci of high Ca, whatever their chemical form,
readily exchange Ca with the mitochondrial matrix.
 |
DISCUSSION |
Summary and comparison with previous studies
Mitochondria in sympathetic neurons accumulate Ca when global
[Ca2+]i is elevated to submicromolar
levels during membrane depolarization. Ca accumulation is reversible,
graded with depolarization strength and duration, and is inhibited by
FCCP, much like Ca accumulation by the FCCP-sensitive store previously
described in these cells (Friel and Tsien, 1994
). Our results agree
with previous studies implicating mitochondrial Ca accumulation during
physiological [Ca2+]i elevations in
various cell types. The findings contrast with x-ray microanalytical
[Ca]mito measurements in muscle, indicating that
[Ca]mito rises only during excessive stimulation (Somlyo, 1984
; Moravec et al., 1997
; Horikawa et al., 1998
; but see
Wendt-Gallitelli and Isenberg, 1991
), implying that mitochondria do not
participate in physiological Ca2+ regulation. The
reason for this discrepancy is unclear, but it likely reflects
differences between experimental preparations and the duration of
[Ca2+]i elevations.
Mitochondrial Ca2+ accumulation at low
[Ca2+]i
Isolated mitochondria accumulate Ca2+ via a
[Ca2+]i-sensitive uniporter with
EC50 ~10-20 µM (Gunter and Gunter, 1994
).
Yet the present study indicates that mitochondria accumulate
Ca2+ during depolarization even when spatially
averaged [Ca2+]i is <1
µM. Moreover, Ca2+ accumulation
continues after spatial [Ca2+]i
gradients should be largely dissipated (Fig. 5b) (see
below), arguing against a requirement for microdomains of high
[Ca2+]i. One likely explanation is
that although activity of the Ca2+ uniporter is far
from maximal when [Ca2+]i is <1
µM, it is not zero (Carafoli, 1979
; McCormack et al., 1989
). Assuming an EC50 of 10 µM and Hill
coefficient of 2 (Gunter and Gunter, 1994
), the uniporter would have an
activity when [Ca2+]i is 300 nM and 500 nM that is 9 and 25%, respectively,
of that observed at 1 µM, where Ca2+
uptake is appreciable; activity could transiently be even higher with
the rapid uptake mode described by Sparagna et al. (1995)
. Therefore,
if mitochondria behave in intact cells as they do in isolation,
Ca2+ uptake would be expected when
[Ca2+]i ~300 nM. This
provides a clear way to reconcile the low affinity and steep
[Ca2+]i-dependence of the uniporter
with the widely reported finding that mitochondria accumulate
Ca2+ at submicromolar
[Ca2+]i.
If mitochondria accumulate Ca during weak depolarization, why does FCCP
have so little effect on [Ca2+]i
responses elicited by such depolarizations, in contrast to the
pronounced effects seen with stronger depolarizations that elevate
[Ca2+]i to higher levels? One possible
explanation is provided by the finding that although inhibition of
Ca2+ accumulation either by the
endoplasmic reticulum (with thapsigargin) or by mitochondria (with
FCCP) has only a small effect on
[Ca2+]i responses elicited by weak
depolarization, simultaneous inhibition of Ca2+
uptake by both organelles strongly potentiates
[Ca2+]i responses (our
unpublished observations). This suggests that when
Ca2+ uptake by one organelle is inhibited, uptake by
the second is enhanced, possibly because reduced
Ca2+ buffering by the first organelle enhances
stimulus-evoked local [Ca2+]i
elevations near the second. Overall, this mechanism would reduce the
impact of inhibitors on [Ca2+]i
responses to depolarization. The pronounced effects of FCCP on
responses to strong depolarization may reflect a steeper
[Ca2+]i dependence of uptake by
mitochondria than for the endoplasmic reticulum (ER), such that at high
[Ca2+]i, compensatory ER
Ca2+ accumulation is overwhelmed. Thus, although
microdomains of high [Ca2+]i are not
required for mitochondrial Ca2+ accumulation during
depolarization, they may influence quantitatively the spatial and
temporal properties of accumulation (Rizzuto et al., 1998
).
Intermitochondrial heterogeneity
In resting cells, [Ca]mito is normally distributed
near zero with small dispersion. During maintained depolarization, the distribution becomes skewed, with some mitochondria exhibiting low
[Ca]mito and others having very high
[Ca]mito. Analysis of mitochondria from single cells
reveals a similar skewed [Ca]mito distribution,
indicating marked intracellular mitochondrial heterogeneity.
One possible explanation for such a distribution comes from the finding
that during depolarization [Ca]mito tends to be highest in mitochondria that are close to the plasma membrane (Fig. 7). This
may reflect more avid Ca2+ accumulation by
peripheral versus central mitochondria owing to differences in
energetic state. Alternatively, different mitochondria may be exposed
to distinctive [Ca2+]i environments.
Sympathetic neurons respond to depolarization under voltage clamp with
a rise in [Ca2+]i that is initially
highest near the plasma membrane (Hernandez-Cruz et al., 1990
; Hua et
al., 1993
). Therefore, peripheral mitochondria would be exposed to
higher [Ca2+]i, and accumulate
Ca2+ at a higher rate, than central organelles
during this phase of depolarization. A similar role of mitochondrial
proximity to a Ca2+ source has been proposed
previously (Rizzuto et al., 1994
; Hajnoczky et al., 1995
; Lawrie et
al., 1996
).
Because radial [Ca2+]i gradients are
largely dissipated within seconds of a step depolarization (Hua et al.,
1993
), it must be asked whether differences in the rate of
Ca2+ uptake by central and peripheral mitochondria
during the first few seconds of depolarization could account for
differences in [Ca]mito that persist for 45 sec.
Diffusion simulations incorporating [Ca2+]i-sensitive mitochondrial
Ca2+ uptake (Fig. 8)
show that [Ca]mito could retain a record of early differences between central and peripheral
[Ca2+]i even after
[Ca2+]i gradients are largely
dissipated, so long as mitochondrial Ca2+
accumulation continues. This condition is clearly satisfied at 45 sec
during maintained depolarization with 50 mM
K+, because [Ca]mito is rising at this
time (Fig. 5b). Even more pronounced spatial heterogeneity
of [Ca]mito would be expected if inactivation of
voltage-sensitive Ca2+ channels occurred more
rapidly than the radial spread of Ca2+ within the
cytosol. In this case, peripheral
[Ca2+]i could reach levels during the
initial phase of depolarization that are never attained deep within the
cell interior.

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Figure 8.
Simulated changes in
[Ca2+]i and [Ca]mito
during a 45 sec depolarization. Diffusion simulation illustrating
radial dependence of [Ca2+]i and
[Ca]mito at different times after membrane
depolarization. a, Step depolarization of the membrane
potential (Vm, top,
arbitrary ordinate scale) elicits an inactivating Ca current
(ICa, middle) that
causes spatially averaged [Ca2+]i
([Ca2+]i,ave,
bottom) to increase with both transient and maintained
components. b, During the first 500 msec of the
depolarization, [Ca2+]i
(top) is much higher near the plasma membrane than it is
in the cell interior, leading to a spatially nonuniform rise in
[Ca]mito (middle). After several seconds,
[Ca2+]i is nearly uniform spatially,
but [Ca]mito continues to rise, retaining a strong
dependence on position. The bottom panel shows the
calculated distribution of [Ca]mito after conversion to
dry weight concentrations and convolution with the fitted distribution
of measurements taken from unstimulated cells (normalized Gaussian with
zero mean and SD 3.5 mmol/kg dry weight). The general form of this plot is qualitatively similar to the
experimentally observed distributions, e.g., Figures 6b,
7b.
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|
Mitochondrial Ca2+ uptake is exquisitely sensitive
to [Ca2+]i; therefore,
stimulation is expected to elicit complex, interdependent changes in
cytosolic and mitochondrial free Ca2+
([Ca2+]m) concentrations.
Stimulated Ca2+ entry (e.g., during trains of action
potentials) would be expected to influence both
[Ca2+]i and [Ca]mito
over a spatial range that depends critically on stimulus frequency and
duration. Mitochondrial proximity to sites of Ca2+
entry may permit regulation of
[Ca2+]m-sensitive dehydrogenases so
that ATP production meets local energy demands (Robb-Gaspers et al.,
1998
). Reciprocally, changes in local
[Ca2+]i resulting from mitochondrial
Ca2+ uptake or release may modulate
Ca2+ entry (Budd and Nicholls, 1996
; Hoth et al.,
1997
). Finally, conjunctive elevations in
[Ca2+]i and mitochondria-dependent
oxidative activity, occurring preferentially at the neuronal periphery,
may be important in activity-dependent changes in gene expression (Bito
et al., 1996
).
Intramitochondrial Ca heterogeneity and its relationship to
Ca2+ buffering
It is clear that the vast majority of Ca within mitochondria is
bound, not free (Babcock et al., 1997
; Horikawa et al., 1998
), but the
mechanisms of intramitochondrial Ca2+ buffering are
poorly understood. These mechanisms are critically important because,
when exhausted, [Ca2+]m may rise to
levels that trigger opening of the mitochondrial permeability
transition pore, leading to cell death (Miller, 1998
). Mitochondria do
not express large quantities of Ca-binding proteins such as
calsequestrin or calreticulin, yet they have an enormous capacity for
storing Ca (Gunter and Pfeiffer, 1990
). Possible contributors to
intramitochondrial buffering include phospholipids (Gunter et al.,
1978
), Ca2+-binding proteins (Lucas-Heron et al.,
1995
; Evtodienko et al., 1998
), andinorganic complexes formed with
anions such as phosphate (Nicholls and Akerman, 1982
). It has long been
known that electron-dense Ca- and P-containing deposits can form within
the mitochondrial matrix in a variety of cells, including sympathetic
neurons (Fujimoto et al., 1980
), after exposure to high
Ca2+ (Lehninger, 1964
). Such inclusions are known to
occur as fixation artifacts, or alternatively, as hallmarks of cell
injury (Somlyo et al., 1979
; Somlyo, 1984
). On the other hand, there is
evidence that soluble Ca2+ complexes are involved in
cell protection (Nicholls, 1985
; Carafoli et al., 1995
).
Our results demonstrate that Ca-enriched regions (
100 nm diameter)
form transiently within individual mitochondria during depolarizations
that raise [Ca2+]i to levels well
within the physiological range. [Ca]mito within these
regions sometimes exceeded 100 mmol/kg dry weight, yet Ca must have
been readily mobilized because they were not observed in mitochondria 5 min after repolarization. Because our measurements were obtained from
neurons rapidly frozen without chemical fixation, they show that focal
sites of Ca accumulation are compatible with normally functioning
mitochondria in situ and suggest that the deposits reflect a
mechanism of mitochondrial Ca buffering. Preliminary Ca mapping
experiments (Andrews et al., 1999
) using spectrum imaging by electron
energy loss spectroscopy (for review, see Leapman et al., 1994
) reveal
mitochondria in peripheral regions of depolarized sympathetic neurons
(45 sec and 120 sec, 50 K+) in which Ca and P are
colocalized in small (<20 nm diameter), discrete inclusions, each
containing only a few thousand atoms of Ca, within an otherwise low-Ca
matrix. The chemical form of Ca in these sites is unknown, but the Ca/P
ratio of ~1:1 suggests the presence of calcium phosphate complexes.
It is possible that such complexes are chemically related to both the
coarse deposits implicated in cell injury and to the soluble
complexes important for cell protection; this in turn suggests a
continuum of calcium phosphate compounds, differing mainly in size,
solubility, and number. Under physiological conditions of stimulation,
the smaller complexes might serve as a fast, reversible,
Ca2+ buffering system, but under conditions of Ca
overload, they might grow in size until exhaustion of counter ions
(e.g., phosphate) causes an uncontrolled
[Ca2+]m elevation and its sequellae.
According to this view, large intramitochondrial Ca deposits observed
under conditions favoring Ca overload would be a correlate, not a
cause, of mitochondrial dysfunction and cell death.
 |
FOOTNOTES |
Received Feb. 2, 1999; revised April 20, 1999; accepted May 17, 1999.
This work was supported by a grant (No. 96011490) from the American
Heart Association and by the National Institutes of Health Intramural
Research Program. We thank Dr. R. D. Leapman (National Institutes
of Health) for helpful discussion and critical evaluation.
Correspondence should be addressed to Dr. David Friel, Department of
Neuroscience, Case Western Reserve University, 10900 Euclid Avenue,
Cleveland, OH 44106. E-mail: ddf2{at}po.cwru.edu