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The Journal of Neuroscience, October 1, 2000, 20(19):7208-7219
Mitochondrial Membrane Potential and Glutamate Excitotoxicity in
Cultured Cerebellar Granule Cells
Manus W.
Ward,
A. Cristina
Rego,
Bruno G.
Frenguelli, and
David G.
Nicholls
Neurosciences Institute, Department of Pharmacology and
Neuroscience, University of Dundee, Dundee DD1 9SY, Scotland, United
Kingdom
 |
ABSTRACT |
The relationship between changes in mitochondrial membrane
potential (
m) and the failure of cytoplasmic
Ca2+ homeostasis, delayed
Ca2+deregulation (DCD), is investigated for cultured
rat cerebellar granule cells exposed to glutamate. To interpret the
single-cell fluorescence response of cells loaded with
tetramethylrhodamine methyl ester (TMRM+) or
rhodamine-123, we devised and validated a mathematical
simulation with well characterized effectors of 
m and
plasma membrane potential (
P). Glutamate
usually caused an immediate decrease in 
m of <10 mV,
attributable to Ca2+ accumulation rather than
enhanced ATP demand, and these cells continued to generate ATP by
oxidative phosphorylation until DCD. Cells for which the mitochondria
showed a larger initial depolarization deregulated more rapidly. The
mitochondria in a subpopulation of glutamate-exposed cells that failed
to extrude Ca2+ that was released from the matrix
after protonophore addition were bioenergetically competent. The onset
of DCD during continuous glutamate exposure in the presence or absence
of oligomycin was associated with a slowly developing mitochondrial
depolarization, but cause and effect could not be established
readily. In contrast, the slowly developing mitochondrial
depolarization after transient NMDA receptor activation occurs before
cytoplasmic free Ca2+
([Ca2+]c) has risen to the set
point at which mitochondria retain Ca2+. In the
presence of oligomycin no increase in
[Ca2+]c occurs during this
depolarization. We conclude that transient Ca2+
loading of mitochondria as a consequence of NMDA receptor activation initiates oxidative damage to both plasma membrane
Ca2+ extrusion pathways and the inhibition of
mitochondrial respiration. Depending on experimental conditions, one of
these factors becomes rate-limiting and precipitates DCD.
Key words:
glutamate excitotoxicity; mitochondrial membrane
potential; delayed calcium deregulation; glutamate receptors; TMRM; rhodamine-123
 |
INTRODUCTION |
Pathological activation of NMDA
receptors, with consequent disturbance in
Na+ and Ca2+
gradients across the plasma membrane, is a primary cause of delayed neuronal death after brain anoxia or ischemia (Rothman and Olney, 1986
;
Choi and Rothman, 1990
; Yoshimura et al., 1998
). Prolonged NMDA
receptor activation in cultures of primary neurons from spine (Tymianski et al., 1993a
), cerebellum (Kiedrowski et al., 1994
; Kiedrowski and Costa, 1995
; Budd and Nicholls, 1996a
; Castilho et al.,
1998
), forebrain (Hoyt et al., 1992
; Rajdev and Reynolds, 1994
),
striatum (Greene et al., 1998
), or hippocampus (Dubinsky and Rothman,
1991
; Randall and Thayer, 1992
; Dubinsky, 1993
; Keelan et al., 1999
;
Vergun et al., 1999
) can result in a failure of the cell to maintain
low, stable cytoplasmic free calcium
([Ca2+]c). This
delayed Ca2+ deregulation (DCD) precedes
and reliably predicts the subsequent necrotic death of the cell
(Tymianski et al., 1993b
) and has been used extensively to model
aspects of in vivo neuronal necrosis.
The potential across the inner mitochondrial membrane
(
m) is the central parameter that controls
mitochondrial respiration, ATP synthesis, and
Ca2+ accumulation (for review, see
Nicholls and Ferguson, 1992
; Nicholls and Budd, 2000
) as well as the
generation of reactive oxygen species (Boveris et al., 1972
; Van Belzen
et al., 1997
). Because each of these factors can influence the survival
of the cell directly or indirectly, the monitoring of

m in glutamate-exposed neurons provides
important information on the mechanism by which mitochondria influence
the survival of glutamate-exposed neurons. The matrices of the in
situ mitochondria load with Ca2+
during glutamate exposure (White and Reynolds, 1995
; Budd and Nicholls,
1996a
; Wang and Thayer, 1996
; White and Reynolds, 1997
), and there is a
general consensus that exposure of the neurons to glutamate results in
a qualitative mitochondrial depolarization (Ankarcrona et al., 1995
;
Budd and Nicholls, 1996a
; Isaev et al., 1996
; Khodorov et al., 1996
;
Schinder et al., 1996
; White and Reynolds, 1996
; Kiedrowski, 1998
;
Prehn, 1998
; Scanlon and Reynolds, 1998
; Stout et al., 1998
; Almeida et
al., 1999
; Keelan et al., 1999
; Vergun et al., 1999
). However, the
cause, extent, and bioenergetic consequences of such depolarization
remain unclear and need further clarification. Conversely, previous
depolarization of mitochondria under conditions that prevent ATP
depletion protects cultured neurons against DCD (Budd and Nicholls,
1996a
; Castilho et al., 1998
; Stout et al., 1998
).
Fluorescent membrane-permeant cations are used widely to monitor

m in these circumstances (for review, see
Nicholls and Ward, 2000
), but interpretation of the complex signals
obtained at single-cell resolution is far from trivial and has led to
confusing and contradictory conclusions. To help resolve these issues,
we have compared experimental traces with those obtained from a simple simulation of the whole-cell fluorescence in response to imposed changes in 
m and plasma membrane potential
(
p). Results are consistent with both
mitochondrial depolarization and failed
Ca2+ extrusion from the cell, the factor
precipitating DCD depending on which first becomes rate-limiting
under the experimental conditions.
 |
MATERIALS AND METHODS |
Materials. Fura-2 acetoxymethyl ester (fura-2 AM),
rhodamine-123, and tetramethylrhodamine methyl ester
(TMRM+) were obtained from Molecular
Probes (Leiden, The Netherlands). Fetal calf serum and MEM were
from Life Technologies (Paisley, Strathclyde, UK). Oligomycin,
rotenone, and all other reagents were from Sigma (Poole, Dorset, UK).
Preparation of cerebellar granule cells. Granule cells were
prepared as previously described (Courtney et al., 1990
) from 6-7 d
postnatal Wistar rats. Cells were plated on
poly-D-lysine-coated glass coverslips (13 mm circular for
nonperfusion experiments and 22 mm square for confocal microscopy) at a
density of 280,000 cells per coverslip. Cells were cultured in MEM
containing Earle's salts (Life Technologies) plus 10% (v/v) fetal
calf serum, 25 mM KCl, 30 mM glucose, 2 mM glutamine, 100 µg/ml streptomycin, and 100 U/ml
penicillin. After 24 hr 10 µM cytosine arabinoside was
added to inhibit non-neuronal cell proliferation. Cells were maintained
at 37°C in a humidified atmosphere of 5%
CO2/95% air and were used after 6-7 d in
vitro (DIV).
Incubation conditions. Unless otherwise stated, incubations
were performed at 37°C in medium containing (in mM) 120 NaCl, 3.1 KCl, 0.4 KH2PO4, 5 NaHCO3, 1.2 Na2SO4, 1.3 CaCl2, and 20 TES [N-tris(hydroxymethyl)methyl-2-aminoethane
sulfonic acid] pH-adjusted to 7.4 at 37°C with NaOH. Unless
otherwise stated, incubation media are
Mg2+-free.
Epifluorescent imaging. Single-cell imaging was performed in
a MiraCal Imaging facility (Life Science Resources, Cambridge, UK) with
a Nikon DIAPHOT-TMD inverted epifluorescence microscope equipped with a
40× oil immersion objective and Sutter filter wheel. The imager was
equipped with a Lambert intensifier 1187 (Life Science Resources)
providing a 30× enhancement of the fluorescent signal, thus limiting
photo toxicity. For imaging TMRM+, we
equilibrated the cells with 50 nM
TMRM+ (unless otherwise stated) for 30 min
at 37°C before the experiment. In most experiments the dye, which was
also present during the experiment, was excited via an Omega 485DF22
filter with peak transmission at 485 nm. The absorbance of
TMRM+ is only 10% of maximum at this
wavelength, but this has the advantage of limiting photodynamic damage
to the cells at the concentrations of
TMRM+ that are required to observe matrix
quenching. Additionally, the use of this filter allows a
dichroic/barrier filter transmitting at >520 nm to be used for both
single dye and combined TMRM+ plus fura-2
imaging. However, experiments performed with 340/380/535 nm excitation
and a Chroma fura-2/rhodamine dichroic gave essentially the same
results (data not shown).
For dual loading the cells were loaded with 50 nM
TMRM+ and 3 µM fura-2 AM for
25 min at 37°C in incubation medium containing additionally 30 µg/ml bovine serum albumin, 15 mM glucose, and 1.2 mM MgCl2. After washing, the cells
were incubated in the presence of 50 nM
TMRM+ and were excited at 340/380/485 nm
with emission >20 nm. Background subtraction and autofluorescence were
corrected for, and controls were performed with cells loaded singly
with either TMRM+ or fura-2, which
established the absence of any significant crosstalk between the dyes
at the wavelengths that were used. Fura-2 fluorescence is reported in
terms of 340/380 nm excitation ratios to avoid potential errors because
of any changes in the quenching of the >520 nm emission by cytoplasmic
TMRM+.
For rhodamine-123 fluorescence a commonly used empirical loading
protocol was applied (Khodorov et al., 1996
; Hagen et al., 1997
;
Buckler and Vaughan-Jones, 1998
; Schuchmann et al., 1998
; Vergun et
al., 1999
). Cells were equilibrated with the probe (1 µg/ml, i.e.,
2.6 µM) for 15 min at 22°C before the experiment; the
probe was not added to the experimental medium. Then the cells were
washed before the experiment (excitation 485 nm; emission >520 nm). It
was found that an alternative loading paradigm [10 µg of
rhodamine-123/ml (26 µM) for 15 min] sensitized the
cells to photo-induced damage (data not shown).
TMRM+ fluorescence within the matrix
of isolated mitochondria. TMRM+ (100 nM or 2 µM) was added to a medium containing
(in mM) 100 NaCl, 25 TES (Na+
salt), and 2 NaH2PO4 plus
16 µM albumin, pH 7.0, 37°C, in a thermostatted cuvette
inserted in a Perkin-Elmer LS50B fluorometer. Fluorescence was recorded
(excitation 543 nm, emission 580 nm) during the sequential additions of
rat liver mitochondria (0.25 mg of protein/ml incubation), prepared as
previously described (Nicholls, 1978
), and 2 mM succinate. Fluorescent quenching after uptake of the probe was determined. The
cuvette contents were centrifuged immediately for 30 sec in an
Eppendorf microcentrifuge to pellet the mitochondria. The fluorescence of the supernatant was measured to determine the contribution of
extramitochondrial TMRM+ to the total
signal, and the mitochondrial pellet was resuspended in water to
determine the fluorescence of the mitochondrial
TMRM+ after release from the matrix. The
assumption that the matrix fluorescence became invariant above the
stacking concentration was tested by incubating isolated mitochondria
in the presence of two widely differing concentrations of
TMRM+, each sufficient to exceed the
stacking concentration in the matrix, as confirmed by the decrease in
cuvette fluorescence when the mitochondria were energized (Fig.
1). The contribution of the quenched
matrix TMRM+ to the total cuvette
fluorescence was quantified by redetermining the fluorescence of the
incubation after removing the mitochondria by centrifugation as
described above. Figure 1 shows that the fluorescence of the
matrix-located probe was similar for mitochondria equilibrated with
both 100 nM and 2 µM
TMRM+, although the actual concentration
of TMRM+ in the matrix, confirmed by lysis
of the mitochondria to release TMRM+,
differed 12-fold.

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Figure 1.
The fluorescence of TMRM+ in
the mitochondrial matrix is concentration-independent above the quench
threshold. A suspension of rat liver mitochondria was equilibrated with
the indicated concentrations of TMRM+ in the absence
of substrate, and the fluorescence was monitored. The addition of
succinate as a substrate caused a decrease in fluorescence as the
indicator was accumulated into the matrix. The contribution of the
extramitochondrial probe to the total fluorescence
(C) was determined after the removal of
mitochondria by centrifugation. The difference
(A) attributable to the fluorescence of matrix
TMRM+ was similar at both concentrations although
the total matrix TMRM+ (B),
determined by resuspending the mitochondria in water, differed by
12-fold.
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|
Simulating single-cell fluorescence of neurons loaded with
membrane-potential probes. The simulation (see Appendix) is based on the following premises. (1) Cationic lipophilic probes are nonselectively permeant across both plasma and mitochondrial membranes. (2) Probe distribution tends to a Nernst equilibrium across both membranes. (3) The rate at which the probe equilibrates across the
small, highly invaginated inner mitochondrial membrane is much faster
than across the plasma membrane because of the differing surface-volume relationships of the mitochondrial matrix and the cell
soma. (4) The quantum yield of the probe is similar in both cytoplasm
and matrix until a threshold concentration is reached in the latter,
above which nonfluorescent H-aggregates form (Bunting, 1992
) (Fig.
1).
The initial 
p was taken to be
60 mV
(Becherer et al., 1997
). The initial value of 150 mV for

m is in agreement with values determined by
the distribution of the lipophilic cation
TPP+ in synaptosomes after correction for
the plasma membrane potential (Scott and Nicholls, 1980
). The
mitochondrial matrix within isolated nerve terminals accounts for 3%
of terminal volume (Scott and Nicholls, 1980
), whereas the lower value
of 1% taken here for the soma reflects the relatively thin annulus of
cytoplasm surrounding the nucleus.
The model is used to reproduce the behavior of two commonly used
fluorescent probes, rhodamine-123 and
TMRM+. The tetramethylrhodamine ester
equilibrates more rapidly across membranes than the slowly permeant
rhodamine-123 (Bunting, 1992
), and empirical fits with experimental
traces were obtained with a value for the permeability constant
k for equilibration across the somatic plasma membrane in
the presence of glutamate of 0.02/sec for
TMRM+ and 0.001/sec for rhodamine-123. It
should be emphasized that these values are for the somata of cultured
cerebellar granule cells and would be lower for larger cells or
conversely increased for thin neurites. In the absence of glutamate,
probe equilibration was limited by constraints of charge neutralization
across the plasma membrane (see Fig. 10), and lower values of
k were determined empirically.
The simulated "loading conditions" for the two probes followed the
empirically determined optimal conditions that were used in this study.
Because TMRM+ is rapidly lost from cells
in the absence of external probe, the granule cells were equilibrated
with probe, usually 50 nM, and this concentration was also
present continuously in the "incubation" to allow continuous
reequilibration across the plasma membrane. The less permeant
rhodamine-123 is normally loaded by a brief exposure (insufficient for
Nernstian equilibration across the plasma membrane) to a relatively
high concentration of probe, typically 2-20 µM (Vergun
et al., 1999
). After this the cells are washed, and the subsequent
experiments usually are performed in the absence of external probe.
Where indicated, the simulation reflects this. In view of the lower
permeability of this probe, loss across the plasma membrane is
sufficiently slow to permit most (but not all; see Fig. 2) short-term
experiments to be performed without excessive loss of probe from the cells.
Statistics. Each set of single-cell responses shown is
representative of at least 60 individual cell somata that were
monitored in at least three independent experiments from different cell preparations. Significance was assessed by unpaired variance Student's t test.
 |
RESULTS |
Validation of the simulation
Figure 2 displays a gallery of
fluorescence traces obtained by the addition of elevated KCl and
FCCP/oligomycin to granule cells exposed to 2.6 µM
rhodamine-123 for 15 min at 22°C before the experiment (Fig.
2A) or equilibrated with either 50 nM
(Fig. 2B,C,E) or 10 nM
TMRM+ (Fig. 2D). Also
shown are curves generated by the cell simulation for step changes in

p and 
m
that would be induced by these agents. The simulated curves were
fit to the experimental traces by varying the plasma membrane
permeability coefficient, k, appropriate for
TMRM+ and rhodamine-123 (see
Appendix Eq. 9) until a satisfactory fit was obtained. Values of
0.003/sec (TMRM+) and 0.0003/sec
(rhodamine-123) were adopted for these traces. A further empirically
determined constant is the threshold concentration at which
aggregation and quenching of the probe occur in the matrix. This was
established by determining the loading concentration for
TMRM+ at which protonophore-induced
dequenching disappeared. Thus equilibration with 50 nM TMRM+ allows
dequenching to be observed (Fig. 2C), but this vanishes when
the loading concentration is reduced to 10 nM
(Fig. 2D). With the initial conditions of a

p of
60 mV and a

m of 150 mV, this corresponds to a quench
threshold
(c+[stacking])
(see Appendix Eq. 4) of ~50 µM within the matrix, and this value was adopted for subsequent simulations.

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Figure 2.
Fluorescence of individual granule cell somata
loaded with rhodamine-123 or TMRM+ in response to
selective plasma and mitochondrial membrane depolarization; curve
fitting with the cell simulation. The incubation medium contained 1.2 mM MgCl2. Ai-Ei, Granule cells
were loaded with rhodamine-123 or TMRM+, as detailed
in Materials and Methods. Where indicated, 50 mM KCl
(K) or 5 µg/ml oligomycin plus 1 µM FCCP (F) was added, and
the fluorescence was monitored. Each trace is from a single
representative soma. Aii-Eii, Values for
 m (thin line) and
 p (thick line) used for the cell
simulation. Aiii-Eiii, Cell simulation; total
fluorescence (thin line) and mitochondrial component of
fluorescence (thick line) are shown. The following
parameters were used: matrix volume = 1% of cytoplasm; quench
threshold = 50 µM; rate constant for plasma membrane
equilibration = 0.0003/sec (rhodamine-123) or 0.003/sec
(TMRM+).
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Several features are revealed by these calibrating traces. When the
cells are equilibrated with sufficient probe to exceed the matrix
quench threshold, acute mitochondrial depolarization produces a spike
followed by a decay in signal (Fig. 2A,B); when loading is subthreshold (Fig. 2D), only the decay
phase is seen. This may reconcile some of the confusion in the
literature as to the signal expected from a mitochondrial depolarization.
Because the total fluorescence of a single cell is the sum of that
originating from the cytoplasm and matrix whereas the matrix fluorescence is invariant above the quench threshold, the changes in
fluorescence mainly reflect changes in cytoplasmic probe concentration. The short-term insensitivity of rhodamine-123 to changes in

p (Fig. 2A) can be
ascribed to the low permeability coefficient, although as will be seen
later (see Fig. 8) there are important conditions for which this is not
valid. In contrast, TMRM+ redistribution
across the plasma membrane must be considered under all conditions,
particularly with small somata such as those of granule cells.
Equilibration of TMRM+ across the plasma
membrane after KCl depolarization is slower than after protonophore
(Fig. 2B), consistent with the increased buffering in
the presence of the mitochondrial pool (see Appendix). Finally, the
decreased cell fluorescence after the decay of the FCCP/oligomycin
"spike" (e.g., Fig. 2B) is attributable to the loss of the unquenched component of the mitochondrial
TMRM+ fluorescence.
The cell simulation was devised to interpret the single-cell
fluorescence responses during the complex, slow changes in

m associated with glutamate exposure and
the delayed Ca2+ deregulation that occurs
as a consequence of glutamate excitotoxicity (Tymianski et al., 1993b
;
Budd and Nicholls, 1996a
). Figure 3 investigates the effects of inhibitors of the respiratory chain and ATP
synthase. Because the membrane potential of in situ
mitochondria in the presence of respiratory chain inhibitors is
supported by ATP synthase reversal and hydrolysis of glycolytic ATP,
respiratory chain inhibitors cause only a slight depolarization in
cells with active glycolysis (Scott and Nicholls, 1980
). However, the
further addition of oligomycin to inhibit the ATP synthase will
initiate a decay of 
m, the kinetics of
which will be limited by the inherent proton permeability properties of
the inner mitochondrial membrane. Studies with isolated mitochondria
indicate the presence of a non-ohmic inner membrane proton conductance,
large at high potential and changing at lower potential to a decreased
"ohmic" conductance (Nicholls, 1974
; Nobes et al., 1990
).

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Figure 3.
Fluorescence of individual granule cell somata
equilibrated with 50 nM TMRM+ in
response to mitochondrial inhibition; curve fitting with the cell
simulation. Ai-Ci, Granule cells were equilibrated with
50 nM TMRM+. Where indicated, 3 µM antimycin A (A), 5 µg/ml
oligomycin (O), 2 µM rotenone
(R), or 50 mM KCl
(K) was added. The incubation medium contained
1.2 mM MgCl2. Each trace is from a single
representative soma. Aii-Cii, Values for
 m (thin line) and  p
(thick line) were obtained by curve fitting for the cell
simulation. Aiii-Ciii, Cell simulation; total
fluorescence (thin line) and mitochondrial component of
fluorescence (thick line) are shown. The following
parameters were used: matrix volume = 1% of cytoplasm; quench
threshold = 50 µM; rate constant for plasma membrane
equilibration = 0.003/sec (TMRM+).
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If this information is put into the cell simulation, the traces that
are generated closely resemble the time course of the fluorescence
response of granule cells exposed to these combinations of inhibitors.
Thus Figure 3A suggests that antimycin A inhibition of
mitochondrial complex III, which will inhibit respiration totally, causes only a 5-10 mV mitochondrial depolarization, consistent with
the near-equilibrium bidirectional operation of the ATP synthase. The
further addition of oligomycin to initiate decay of the proton gradient
clearly reveals the biphasic decay consistent with the non-ohmic
inherent proton conductance of the mitochondrion.
If the order of additions is reversed, the initial addition of
oligomycin causes a slight mitochondrial hyperpolarization as use of
the proton circuit for ATP generation is inhibited. This produces a
decreased whole-cell signal (Fig. 3B). The addition of
antimycin A now initiates the non-ohmic decay of potential. It should
be noted in Figure 3Ci that the decay of fluorescence after
the final KCl addition is faster than that simulated by even an
instantaneous plasma membrane depolarization (Fig. 3Ciii). In the particular circumstances in which the efflux across the plasma
membrane of TMRM+, which is electrogenic,
can be charge-compensated by the entry of
Ca2+ through voltage-activated
Ca2+ channels, transiently activated by
the depolarization, the reequilibration of
TMRM+ is accelerated. It appears,
therefore, that single-cell fluorescence can provide information on the
kinetics of change in potential, as well as the approximate magnitude
of any change.
The direction in which 
m changes on the
addition of oligomycin reveals whether the mitochondria within the cell
are net generators or users of ATP (Fig. 3A,B), providing an
independent in situ means to investigate the bioenergetic
competence of the mitochondria, for example during glutamate exposure.
We previously have exploited the combination of rotenone plus
oligomycin to depolarize mitochondria within cerebellar granule cells
(Budd and Nicholls, 1996a
,b
; Castilho et al., 1998
, 1999
). However,
rotenone is only ~90% effective as an inhibitor of electron transfer
through complex (Rottenberg and Wu, 1998
), and it is evident from
Figure 4A that a
residual 
m still can be detected in the
presence of rotenone plus oligomycin, because the subsequent addition
of FCCP causes a spike and decay of the
TMRM+ signal consistent with a further
collapse of potential. However, the residual proton current in the
presence of rotenone plus oligomycin cannot maintain a detectable

m in the face of an increased load, for
example Ca2+ uptake after KCl
depolarization of the plasma membrane (Fig. 4B),
because 
m immediately collapses, as shown
by the TMRM+ response synchronous with the
spike in the fura-2 response indicating Ca2+ entry across the plasma membrane. As
in Figure 3C, a rapid reequilibration of
TMRM+ across the plasma membrane is seen
as the probe efflux can be charge-balanced by
Ca2+ entry.

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Figure 4.
Residual mitochondrial polarization in the
presence of rotenone plus oligomycin. Granule cells (6-7 DIV) were
loaded with fura-2 AM and 50 nM TMRM+.
The medium contained 1.2 mM Mg2+. Where
indicated, 2 µM rotenone (R), 5 µg/ml oligomycin (O) and 2.5 µM
FCCP (F), or 50 mM KCl was added.
Note that FCCP and KCl are each able to depolarize the mitochondria
further (shown by the dequenching spike) in the presence of rotenone
plus oligomycin. Smooth trace, TMRM+
fluorescence; filled circles trace, fura-2 fluorescence
ratio.
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Acute changes in mitochondrial membrane potential in
glutamate-exposed cerebellar granule cells
The consensus that glutamate addition depolarizes mitochondria
within neurons (see introductory remarks) has been essentially qualitative so that the extent, mechanism, and bioenergetic
consequences of the depolarization generally have not been addressed.
Two phases of depolarization have been distinguished, an acute response
on receptor activation and a second phase associated with DCD (Vergun et al., 1999
). In cultured hippocampal neurons these phases generally follow closely on each other (Vergun et al., 1999
), thereby preventing a clear separation of the two phases.
An experimental protocol was devised to monitor sequentially any acute
mitochondrial depolarization on glutamate addition, the redistribution
of TMRM+ across the plasma membrane in
response to nondesensitizing NMDA receptor activation, the ability of
the mitochondria to generate ATP during the glutamate exposure (by
monitoring oligomycin-induced hyperpolarization), and the residual
mitochondrial depolarization on the addition of protonophore.
Figure 5A shows representative
traces for the subset of cells loaded with
TMRM+ or rhodamine-123 that fail to
undergo glutamate-induced delayed Ca2+
deregulation within the time scale of the experiment (~32% of the 7 DIV cells). It is apparent that equilibration of the probes across the
plasma membrane is considerably more rapid in the presence of glutamate
than in the presence of high KCl. Thus, comparing Figures
2A and 5Ai shows that the final decay of
the rhodamine-123 signal after FCCP is much more rapid in the
glutamate-exposed cells than in the KCl-exposed cells. Similarly, the
redistribution of TMRM+ because of plasma
membrane depolarization is more rapid with glutamate (Fig.
5Bi) than with KCl (see Fig. 2B). This
difference can be explained plausibly as a glutamate-induced increase
in the rate constant for equilibration across the plasma membrane. Increasing k for TMRM+ from
0.003 to 0.02 and for rhodamine-123 from 0.0003 to 0.001 allowed these
signals, and subsequent glutamate traces, to be fit kinetically to the
simulation with good precision (Fig. 5Bii,Cii). As discussed
in the context of Ca2+ channel activation,
it is likely that this increased rate of reequilibration is a
consequence of the need for charge compensation during the net
transport of the cationic probes across the plasma membrane (see also
Fig. 10) and that this is facilitated by
Na+ or Ca2+
influx via the NMDA receptor.

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Figure 5.
In situ membrane potential of
granule cell mitochondria exposed to glutamate plus glycine: retained
capacity to generate ATP. Shown is single soma fluorescence of granule
cells loaded with rhodamine-123 (Ai) or 50 nM TMRM+ (Bi) exposed to
100 µM glutamate plus 10 µM glycine
(G). Where indicated, 2 µg/ml oligomycin
(O) and 1 µM FCCP
(F) were added. Aii,
Bii, Simulated traces were fit to the following
potential changes:  p, depolarization from 60
to 20 mV on the addition of glutamate;  m,
depolarization from 150 to 145 mV on the addition of glutamate and
hyperpolarization to 155 mV on the addition of oligomycin (indicating
retained capacity to generate ATP) and collapse of potential with
FCCP.
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We have reported previously (Castilho et al., 1999
) that granule cells
that maintain a stable
[Ca2+]c plateau in
the presence of glutamate may fail to extrude the Ca2+ that is released from the
mitochondrial matrix into the cytoplasm by oligomycin plus FCCP, and we
have ascribed this to damaged plasma membrane
Ca2+ efflux pathways. To establish whether
this is associated with any sign of mitochondrial dysfunction, we
monitored TMRM+ fluorescence in parallel
with fura-2 (Fig. 6). The 20% of the 7 DIV cells that restore a low
[Ca2+]c after
FCCP/oligomycin (Fig. 6A) maintain a stable
fluorescence and show oligomycin-induced mitochondrial
hyperpolarization, indicative of functional oxidative phosphorylation.
The rapid recovery of a low
[Ca2+]c after FCCP
indicates that plasma membrane Ca2+
extrusion is still unimpaired in these cells.

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Figure 6.
Delayed Ca2+ deregulation
induced in a subpopulation of cells by release of matrix
Ca2+ into the cytoplasm occurs in the absence of
previous mitochondrial dysfunction. The 7 DIV granule cells were loaded
with fura-2 and equilibrated with 50 nM
TMRM+. The cells were exposed to 100 µM glutamate/10 µM glycine
(G); 2 µg/ml oligomycin
(O) and 1 µM FCCP
(F) were added where indicated. The traces
represent the fura-2 (filled circles trace) and
TMRM+ (smooth trace) responses from a
single representative soma. A, Cell that regains
cytoplasmic Ca2+ homeostasis after FCCP. The
FCCP-induced fura-2 spike occurs during release of matrix
Ca2+ and its subsequent removal from the cytoplasm.
Note the oligomycin-induced fluorescent quenching diagnostic of
mitochondrial ATP synthesis before the inhibitor addition.
B, Cell that fails to restore a low
[Ca2+]c after FCCP. Note that the
mitochondria in this cell also generated ATP before the oligomycin
addition.
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|
The subpopulation of cells that failed to restore a low
[Ca2+]c after
FCCP/oligomycin (Fig. 6B) accounts for 32% of the
total population of the 7 DIV cells. As previously reported (Castilho et al., 1999
), these cells tend to display a slowly rising
[Ca2+]c during the
plateau. The bioenergetic integrity of their mitochondria is
unimpaired, because oligomycin-induced hyperpolarization and the FCCP
spike are still apparent. This suggests that these cells have
increasing difficulty extruding Ca2+ and
that this occurs before any detectable mitochondrial dysfunction. However, it is also likely that the mitochondria in cells that deregulate on protonophore addition also have accumulated more Ca2+ (compare the magnitude of the
Ca2+ elevations in Fig.
6A,B).
Relation between initial mitochondrial depolarization and survival
time before DCD
A minor population (14%) of the 7 DIV granule cells shows an
extensive dequenching immediately on glutamate addition, accompanied by
a rapid onset of DCD. This is the dominant response in published studies of hippocampal neurons cultured >11 DIV that are exposed to
glutamate (Vergun et al., 1999
). Figure
7A shows an extreme example of
a cerebellar granule neuron for which the mitochondria depolarize
extensively with the addition of glutamate, followed by immediate
Ca2+ deregulation. The relationship
between the initial dequenching of TMRM+
and the survival time before the onset of DCD was determined for 107 cells (Fig. 7B) that were incubated in varying external Ca2+ concentrations or in the presence of
oligomycin. It is apparent that an inverse relationship exists between
the extent of the initial dequenching and the time it takes cells to
lose their Ca2+ homeostasis and
deregulate.

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Figure 7.
Acute glutamate-induced mitochondrial
depolarization: estimation of extent and consequences for DCD. The 7 DIV granule cells were loaded with fura-2, equilibrated with 50 nM TMRM+, and incubated in the presence
of varying external Ca2+. A, Example
of a cell showing massive initial depolarization and early DCD.
Smooth trace, TMRM+ fluorescence;
filled circles trace, fura-2 fluorescence ratio.
B, Scatter plot relating the percentage of increase in
TMRM+ fluorescence immediately after the addition of
100 µM glutamate/10 µM glycine to the time
delay before DCD. The predicted mitochondrial depolarization was
calculated as a function of fluorescence increase by running the
simulation. Open circles, 1.3 mM
Ca2+; filled circles, 1.3 mM Ca2+ plus 2 µg/ml oligomycin;
open triangles, 2 mM
Ca2+; open squares, 2.6 mM Ca2+. C, Mean increase
in fluorescence as a function of external Ca2+ for
the cells shown in B.
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|
The cell simulation can be used to predict the extent of the initial
depolarization corresponding to a given degree of dequenching. The
alternative scale in Figure 7B suggests that an initial
mitochondrial depolarization in excess of 10 mV is associated with a
greatly decreased survival time. The acute mitochondrial depolarization is dependent on the extracellular concentration of
Ca2+, persists in the initial presence of
oligomycin, and is reduced in Ca2+-free
medium (Fig. 7C). Thus the mitochondrial depolarization appears to be a direct consequence of calcium uptake rather than an
associated enhancement in mitochondrial ATP demand, for example in
response to increased Na+ pump activity.
Mitochondrial membrane potential during the plateau
preceding DCD
Net
45Ca2+
accumulation by granule cells after glutamate exposure is maximal
immediately on agonist addition and then declines (Castilho et al.,
1998
). However, the partial mitochondrial depolarization induced by
this uptake appears more permanent, as judged by the rhodamine-123
response (see Fig. 5A; see also Vergun et al., 1999
). Ca2+-induced mitochondrial depolarization
can be either dynamic, reflecting the use of the proton gradient during
rapid net accumulation of the cation, or persistent, reflecting a
limitation in the availability of cytoplasmic phosphate to accompany
Ca2+ into the matrix (Nicholls, 1978
). In
the latter case
pH across the inner mitochondrial membrane will
increase at the expense of 
m, and this will
be retained even after net Ca2+
accumulation ceases. The present results suggest, therefore, that
phosphate limitation rather than continuous net
Ca2+ accumulation could be responsible for
the initial depolarization.
Although the simulation is consistent with an initial mitochondrial
depolarization of only 5-10 mV in cells that do not undergo DCD (Fig.
7), it is perhaps more relevant in the present context simply to
determine whether the protonmotive force (
p) of the partially
depolarized mitochondria is still sufficient for the generation of ATP.
To this end, the ability to detect an oligomycin-induced mitochondrial
hyperpolarization during the plateau phase was investigated. Sufficient
time was allowed for the TMRM+ to
reequilibrate across the plasma membrane in response to the NMDA
receptor activation before oligomycin was added. In the majority of the
7 DIV neurons, oligomycin induced a significant step decrease in
whole-cell fluorescence, indicating that the mitochondrial population
in these individual cells was generating ATP before the addition of the
inhibitor. Thus in these cells the calcium-induced decrease in
mitochondrial membrane potential does not lower
p below the
threshold required for net ATP synthesis during the plateau phase
before DCD. It should be noted that the oligomycin-induced hyperpolarization can be detected more readily with the slowly permeant
rhodamine-123 (see Fig. 5A).
Kinetics of mitochondrial depolarization during delayed
calcium deregulation
Delayed calcium deregulation is a stochastic event (Dubinsky et
al., 1995
) that is accompanied by a profound mitochondrial depolarization (Isaev et al., 1996
; Khodorov et al., 1996
; Schinder et
al., 1996
; White and Reynolds, 1996
; Vergun et al., 1999
). The majority
of the 7 DIV granule cells undergoes DCD after 30-60 min of continuous
exposure to glutamate and glycine (Budd and Nicholls, 1996a
).
Simultaneous monitoring of the fura-2 and
TMRM+ signals allows the onset of DCD to
be correlated with mitochondrial depolarization in individual cells.
Granule cells loaded with fura-2 in
Mg2+-free, low KCl medium exhibit
responses to glutamate/glycine that vary from an almost immediate
failure of cytoplasmic Ca2+ homeostasis to
the maintenance of a low
[Ca2+]c throughout
the duration of the experiment (Budd and Nicholls, 1996a
).
The TMRM+ fluorescence decreases during
DCD sometimes are preceded by a shallow hump (Fig.
8A). The model can
simulate this response as either a further plasma membrane
depolarization or as a slowly developing mitochondrial depolarization.
To distinguish between these possibilities, we used rhodamine-123 in
parallel experiments (Fig. 8C). The rate of mitochondrial
depolarization during DCD differs from cell to cell; however, the
simulation can reproduce the experimental traces if the mitochondrial
population within individual cell somata undergoes exponentially
developing collapses of 
m (Fig.
8D). Figure 8, E and F, shows
the families of simulated traces obtained for
TMRM+ and rhodamine-123, respectively, in
response to the depolarization protocols shown in Figure
8C.

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Figure 8.
Temporal relationship between mitochondrial
depolarization and DCD for granule cells exposed to glutamate/glycine.
Cells were loaded with fura-2 and either 50 nM
TMRM+ (A, B) or 2.6 µM
rhodamine-123 (C). Where indicated, 100 µM glutamate plus 10 µM glycine was added
to the incubation. D, Simulated depolarization time
courses used to fit the experimental
TMRM+ or rhodamine traces. The simulated plasma
membrane potential changes from 60 to 20 mV on glutamate addition,
whereas  m undergoes an initial 5 mV depolarization on
glutamate addition, followed by an exponentially developing collapse in
 m. Four increasing rates of mitochondrial
depolarization are shown in the simulation. E, F,
Simulated responses to glutamate of a cell loaded with
TMRM+ (E) or rhodamine-123
(F) during the depolarization protocols shown in
D. Smooth traces,
TMRM+ or rhodamine-123 fluorescence; filled
circle traces, fura-2 fluorescence ratio.
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|
The time course of mitochondrial depolarization during DCD is clearly
distinctive from that induced by protonophore plus oligomycin (see Fig.
6), which results in an "instantaneous" collapse in 
m, or by antimycin A plus oligomycin (see
Fig. 3) in which a biphasic decay can be modeled. Depolarization is
sufficiently slow to prevent a temporary accumulation of
TMRM+ in the cytoplasm and hence a
significant increase in whole-cell fluorescence (Fig.
8A), and it is necessary to use the slowly permeant
rhodamine-123 to show this transient increase in whole-cell signal
(Fig. 8C). DCD and mitochondrial depolarization appear to be
initiated at approximately the same time, although an extensive loss of
Ca2+ homeostasis can be seen before
mitochondrial depolarization has become extensive.
Mitochondrial depolarization will result in ATP synthase reversal and
the depletion of cytoplasmic ATP, particularly if the proton
conductance of the inner membrane is increased, for example by
protonophore. In the presence of glutamate, protonophore or respiratory
chain inhibition results in a failure of cytoplasmic Ca2+ homeostasis in these cells (Budd and
Nicholls, 1996a
; Castilho et al., 1998
) that can be ascribed to ATP
synthase reversal because it may be prevented or reversed by
oligomycin. The close association of DCD with the collapse of

m therefore could be a bioenergetic consequence of such ATP depletion. To control for this possibility, we
repeated the experiment in Figure 8A in the presence
of oligomycin (Fig. 8B). A similar relationship
between DCD and mitochondrial depolarization was observed in the
presence of the inhibitor, eliminating ATP synthase reversal as a
direct cause of the failed cytoplasmic
Ca2+ homeostasis.
Mitochondrial membrane potential and DCD after transient glutamate
receptor activation
Although transient NMDA receptor activation can be followed by a
restoration of basal
[Ca2+]c,
subsequent DCD can still occur (Tymianski et al., 1993b
). In Figure
9 the fura-2 and
TMRM+ signals are monitored in granule
cells that were exposed to glutamate followed by the addition, after 10 min, of MK 801 plus NBQX to inhibit NMDA and AMPA receptors. As has
been reported by Thayer and Miller (1990)
, the recovery of the fura-2
signal to basal when Ca2+ loading is
terminated is biphasic under conditions of mitochondrial Ca2+ accumulation. The shoulder after the
first rapid recovery phase has been ascribed (Thayer and Miller, 1990
)
to the buffering effect on the cytoplasm of the efflux of
Ca2+ from the mitochondrial matrix as
[Ca2+]c falls
below the set point (Nicholls, 1978
) at which the mitochondrial uptake
and efflux pathways are in kinetic balance. Depletion of nonmitochondrial Ca2+ stores has little or
no effect on the shape or duration of the shoulder (data not
shown).

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Figure 9.
Delayed Ca2+ deregulation and
mitochondrial depolarization in cells after transient exposure to
glutamate/glycine. The 7 DIV cells were loaded with fura-2 and
TMRM+ as in Figure 6 and exposed to 100 µM glutamate plus 10 µM glycine
(G). Where indicated, 10 µM each of
MK 801 and NBQX was added (MK/NBQX). Note that
this is well before the fura-2 signal indicates that
[Ca2+]c has risen to the set point at
which mitochondria become net accumulators of Ca2+
(horizontal dashed line). Smooth trace,
TMRM+ fluorescence; filled circles
trace, fura-2 fluorescence ratio; vertical dotted
line, time point at which mitochondrial depolarization
starts.
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|
The recovery of the TMRM+ signal appears
to be delayed until this mitochondrial unloading is complete. The
slowness of the recovery may reflect the problems of charge balance
experienced in the absence of glutamate as discussed above, because
plasma membrane repolarization presumably will be instantaneous after receptor inhibition. Support for this is found in the experiment in
Figure 10B, in which
a 1 µM concentration of the membrane-permeant anion tetraphenylboron is included in the incubation as a
charge-compensating counter ion. Averaged over 30 cells, the time for
the equilibration of TMRM+ after glutamate
was reduced from 465 ± 17 to 192 ± 7 sec in the presence of
TPB
and that for recovery after receptor
inhibition from 990 ± 30 to 290 ± 18 sec.

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Figure 10.
Tetraphenylboron accelerates plasma membrane
equilibration of TMRM+. The 7 DIV cells were loaded
with fura-2 and TMRM+ as in Figure 6 and exposed to
100 µM glutamate plus 10 µM glycine
(G). Where indicated, 10 µM each of
MK 801 and NBQX (MK/NBQX) was added.
Tetraphenylboron (1 µM;
TPB ) was additionally present in
B.
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|
The spontaneous loss of signal that is initiated in Figure
9A at ~60 min reflects a slowly developing mitochondrial
depolarization. Importantly, the depolarization is almost complete
before [Ca2+]c, as
given by the fura-2 ratio, rises beyond the critical set point at which
the mitochondria become net accumulators of
Ca2+ (horizontal dashed
line). Thus under these conditions mitochondrial depolarization can precede cytoplasmic
Ca2+ deregulation. To establish whether
this DCD is a consequence of cytoplasmic ATP depletion after ATP
synthase reversal, we repeated the experiment in the presence of
oligomycin that was added after recovery of the fura-2 signal (Fig.
11A). The
experimental trace can be fit to a slow delayed mitochondrial
depolarization (Fig. 11B,C), but it is remarkable
that cytoplasmic Ca2+ homeostasis is
retained completely for the duration of the experiment. In particular,
[Ca2+]c remains at
a stable baseline value far below the mitochondrial set point indicated
by the shoulder after MK 801/NBQX addition. It is evident that no ATP
depletion or plasma membrane depolarization occurs during the duration
of this experiment, because this would result in an increase in
[Ca2+]c by failed
Ca2+ extrusion or voltage-activated
Ca2+ channel activation, respectively.

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Figure 11.
Oligomycin prevents DCD, but not mitochondrial
depolarization, in cells after transient exposure to glutamate/glycine.
The 7 DIV cells were loaded with fura-2 and TMRM+ as
in Figure 6 and exposed to 100 µM glutamate plus 10 µM glycine (G). Where indicated, 10 µM each of MK 801 and NBQX
(MK/NBQX) and 5 µg/ml oligomycin
(O) were added. The vertical dotted
line represents the time point at which mitochondrial
depolarization can be detected. The horizontal dashed
line shows the set point at which mitochondria become net
accumulators of Ca2+. Smooth trace,
TMRM+ fluorescence; filled circles
trace, fura-2 fluorescence ratio. B, Time
course of  p and  m input into the
simulation; note that the plasma membrane rate constant is taken to be
k = 0.02/sec while NMDA receptors are active and
0.003/sec when the receptors are inhibited. C, Cell
simulation. The vertical dashed line represents the time
point at which mitochondrial depolarization starts.
|
|
 |
DISCUSSION |
Monitoring 
m in intact neurons
The role of mitochondrial depolarization and/or dysfunction in
glutamate excitotoxicity (Ankarcrona et al., 1995
, 1996
; Isaev et al.,
1996
; Khodorov et al., 1996
; Schinder et al., 1996
; White and Reynolds,
1996
; Kiedrowski, 1998
; Prehn, 1998
; Keelan et al., 1999
; Marks and
Zhang, 1999
; Vergun et al., 1999
) may need reevaluation in the light of
the present study. The technical complexity in the use of membrane
potential probes at single-cell resolution has given rise to
considerable confusion (for review, see Nicholls and Ward, 2000
). The
cell simulation may help to resolve some of these ambiguities. Although
not precisely predicting the experimental trace, it allows for plasma
membrane reequilibration, while differing patterns of mitochondrial
depolarization can be distinguished, from the sharp spike and rapid
recovery after the collapse of 
m by
protonophore (see, for example, Fig. 5) to the biphasic decay kinetics
seen with antimycin A plus oligomycin (see Fig. 3), the exponentially
developing depolarization during DCD (see Fig. 8), and the extremely
slow, more linear, depolarization observed after NMDA receptor
inactivation in the presence of oligomycin (see Fig. 11). In addition,
approximate estimates can be obtained of the extents of the initial
depolarization (see Fig. 7), oligomycin can be used to test for
continued ATP synthesis (see Fig. 5), and finally the distinctive shape
of rhodamine-123 and TMRM+ traces can be
explained (see Fig. 5).
The relationship between mitochondrial depolarization and DCD
In the continued presence of glutamate, DCD and the final collapse
in 
m cannot be separated readily in time
(see Fig. 8), which makes it difficult to establish whether
mitochondrial depolarization causes DCD, DCD causes mitochondrial
depolarization, or whether the two are independent effects. Certainly a
mitochondrion cannot retain a high 
m in an
ambient free Ca2+ concentration that is
maintained continuously above the set point, because, in the presence
of sufficient phosphate, the matrix would load inexorably with
Ca2+ until the mitochondria become damaged
or the permeability transition is induced. A primary mitochondrial
depolarization, on the other hand, could initiate DCD either by
cytoplasmic ATP depletion or by dumping a massive matrix
Ca2+ load into the cytoplasm.
Oxidative stress is a key component in acute glutamate excitotoxicity
(for review, see Beal et al., 1997
), and because the mitochondrial
generation of superoxide is dependent on the maintenance of a high

m (Boveris et al., 1972
; Skulachev, 1996
;
Braidot et al., 1999
), reactive oxygen species generation by the
calcium-loaded polarized mitochondria may be the key factor that
depletes the antioxidant defenses of the cell, resulting in the
ultimate failure of cytoplasmic calcium homeostasis.
Analysis of the extent of the initial mitochondrial depolarization on
glutamate addition reveals that the larger the initial depolarization,
the sooner the onset of DCD (see Fig. 7). This is similar to the
correlation observed by Vergun et al. (1999)
between the acute
rhodamine-123 fluorescence increase with glutamate and the failure of
hippocampal neurons to restore cytoplasmic Ca2+ homeostasis after glutamate removal.
Because the TMRM+ spike is still seen in
the presence of oligomycin, a depolarization associated with increased
ATP demand can be ruled out, indicating that any depolarization is
attributable to mitochondrial Ca2+ uptake.
Indeed, a somewhat surprising feature of these cells is that survival
in the continuous presence of glutamate is the same in control cells
and cells preincubated with oligomycin (Budd and Nicholls, 1996a
;
Castilho et al., 1998
). This suggests that the ATP demand of the
glutamate-exposed cells is not greatly in excess of that of control cells.
Modes of mitochondrial depolarization
The following modes of mitochondrial depolarization in response to
potentially excitotoxic NMDA receptor activation can be resolved in
this and related studies.
(1) An acute depolarization on the addition of glutamate reflects
accumulation by the mitochondria of Ca2+
entering via the NMDA receptor. In most of the 7 DIV granule cells this
depolarization only amounts to 5-10 mV (see Fig. 7). Mitochondria
continue to generate ATP in the presence of glutamate for at least 30 min (see Figs. 5, 6), as judged by the oligomycin-induced hyperpolarization. This is consistent with the ability of granule cells
supported by lactate or pyruvate in glucose-free media (cells dependent
entirely on oxidative phosphorylation) to maintain a stable
[Ca2+]c in the
presence of glutamate for as long as glucose maintained the cells
(Castilho et al., 1998
)
(2) As the initial depolarization increases above 20%, the survival
time of the cells before DCD is shortened greatly (see Fig.
7A), suggesting that Ca2+ entry
via the NMDA receptors overwhelms the capacity of the mitochondrion plus plasma membrane to maintain cytoplasmic
Ca2+ homeostasis in these neurons (see
Fig. 7A).
(3) Immediate Ca2+ deregulation, ICD
(Castilho and Nicholls, 1999
), can be induced after glutamate by
restricting respiratory chain capacity by rotenone (Budd and Nicholls,
1996a
; Castilho et al., 1998
) or antimycin A (Nicholls and Budd, 1998
).
Mitochondrial depolarization is limited by ATP synthase reversal (see
Fig. 3) but at the cost of acute cytoplasmic ATP depletion by ATP
synthase reversal (Budd and Nicholls, 1996a
). ICD does not appear to be attributable to oxidative damage because it can be reversed by the
inhibition of the NMDA receptor and ATP synthase (Castilho et al.,
1998
). The rapid loss of Ca2+ homeostasis
observed in >11 DIV hippocampal neurons may relate to nitric
oxide-mediated restriction of respiratory chain activity (Keelan et
al., 1999
).
(4) If mitochondria are depolarized without depleting cytoplasmic ATP
by the combination of respiratory chain inhibitor plus oligomycin
before the addition of glutamate, survival of the granule cells is
enhanced greatly (Budd and Nicholls, 1996a
). Cell-permeant antioxidants
such as Mn-TBAP enhance granule cell survival, suggesting that the
Ca2+-loaded polarized mitochondria are
generating potentially toxic reactive oxygen species.
(5) If granule cells are exposed continuously to glutamate, the onset
of DCD is associated with a slowly developing profound mitochondrial
depolarization (see Fig. 8), which the simulation indicates may take
between 10 and 15 min from inception to completion (see Fig.
8C). As with hippocampal neurons (Vergun et al., 1999
) it is
not easy to resolve cause and effect when NMDA receptors are activated
continuously. If the critical targets of oxidative damage are the
plasma membrane Ca2+ extrusion pathways,
this would increase
[Ca2+]c, leading
to an inexorable mitochondrial Ca2+
overload and ultimate depolarization. Alternatively, mitochondrial Ca2+ overload and depolarization could be
the primary event initiating DCD, attributable possibly to induction of
the permeability transition and the dumping of an irrecoverable
Ca2+ load into the cytoplasm. However,
brain mitochondria are highly resistant to the permeability transition
(Murphy and Fiskum, 1999
), and interpretation of the ability of
cyclosporin derivatives to delay DCD in brain is controversial (Li et
al., 1997
; Nakai et al., 1997
; Friberg et al., 1998
, 1999
).
(6) Transient exposure to glutamate is the classical paradigm in which
to monitor in vitro neuronal necrosis (Choi et al., 1987
;
Tymianski et al., 1993b
). When it is used in the present context, a
clear dissociation between mitochondrial depolarization and DCD is
evident. In the absence of oligomycin (see Fig. 9) mitochondrial
depolarization is initiated well before
[Ca2+]c rises
above the set point. That the subsequent DCD is a consequence of ATP
synthase reversal and cytoplasmic ATP depletion is seen by comparison
to Figure 11, in which the presence of oligomycin totally prevents DCD
during the slow collapse of 
m.
Because the cells will have only a slow basal
Ca2+ influx after NMDA receptor inhibition
by MK 801, the demands on the plasma membrane
Ca2+ extrusion pathways are decreased
relative to experiments in which the NMDA receptor is continuously
active, first because Ca2+ influx is
reduced to basal and second because the
Na+/Ca2+
exchanger should be competent to extrude
Ca2+ from the cell. Thus the experiment
does not preclude oxidative damage to the plasma membrane
Ca2+-ATPase occurring during the glutamate exposure.
Because the mitochondria are Ca2+-depleted
at the stage in which they depolarize, it is unclear whether the
permeability transition is responsible. It is notable that
mitochondria that are isolated from glutamate-exposed granule cells
(Atlante et al., 1996
) show no increase in State 4 respiration, which
monitors the proton leakiness of the inner membrane (Nicholls and
Ferguson, 1992
), but they do show a greatly decreased State 3 respiration (NADH supply or respiratory chain capacity). A similar
respiratory inhibition is observed in glutamate-exposed retinal neurons
(Rego et al., 2000
). This is also consistent with the high sensitivity
of enzymes such as aconitase to oxidative damage (Melov et al.,
1999
).
Conclusion
Mitochondrial Ca2+ loading is the
critical step in acute glutamate excitotoxicity (Budd and Nicholls,
1996a
; Castilho et al., 1998
; Stout et al., 1998
). Even brief exposure
to glutamate initiates DCD, and it is apparent that mitochondrial
dysfunction is initiated in this period. The damage inflicted by
transient Ca2+ loading may include
cytochrome c release (Atlante et al., 1999
), altering the
redox poise of complex III and enhancing the generation of superoxide
(Gonzalez Flecha and Boveris, 1995
). The critical parameter that
becomes rate-limiting to initiate DCD depends on the experimental
design. Under the conditions of continued
Ca2+ entry, plasma membrane
Ca2+ extrusion may be the first to fail,
whereas after inhibition of the receptor, mitochondrial dysfunction may
precipitate DCD.
 |
FOOTNOTES |
Received May 28, 2000; revised June 21, 2000; accepted July 19, 2000.
This research was supported by grants from the Wellcome Trust
(054633/Z/98) and the Biomed program of the European Union
(FMRX-CT98-0236). M.W.W. is supported by a Medical Research Council studentship.
Correspondence should be addressed to Dr. David Nicholls, Buck Center
for Research in Aging, Novato, CA 94945 (courier mail) or P.O. Box 638, Novato, CA 94948-0638 (mail). E-mail: dnicholls{at}buckcenter.org.
 |
APPENDIX |
Modeling single-cell fluorescence of a cationi