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Volume 270,
Number 33,
Issue of August 18, pp. 19659-19667, 1995
©1995 by The American Society for Biochemistry and Molecular Biology, Inc.
Metabolic
Modulation of Transport Coupling Ratio in Yeast Plasma Membrane
H -ATPase (*)
(Received for publication, March 29, 1995; and in revised form, June 16, 1995)
Kees
Venema (§),
,
Michael G.
Palmgren (¶)
From the Department of Plant Biology, Royal Veterinary and
Agricultural University, Thorvaldsensvej 40, DK-1871 Frederiksberg C,
Copenhagen, Denmark
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
DISCUSSION
FOOTNOTES
ACKNOWLEDGEMENTS
REFERENCES
ABSTRACT
The plasma membrane proton pump (H -ATPase) of
yeast energizes solute uptake by secondary transporters and regulates
cytoplasmic pH. The addition of glucose to yeast cells stimulates
proton efflux mediated by the H -ATPase. A >50-fold
increase in proton extrusion from yeast cells is observed in
vivo, whereas the ATPase activity of purified plasma membranes is
increased maximally 8-fold after glucose treatment (Serrano, R.(1983) FEBS Lett. 156, 11-14). The low capacity of yeast cells
for proton extrusion in the absence of glucose can be explained by the
finding that, in H -ATPase isolated from
glucose-starved cells, ATP hydrolysis is essentially uncoupled from
proton pumping. The number of protons transported per ATP hydrolyzed is
significantly increased after glucose activation. We suggest that
intrinsic uncoupling is an important mechanism for regulation of pump
activity.
INTRODUCTION
The H -ATPase in fungal plasma membranes
functions physiologically to hydrolyze ATP and to pump H out of the cell; the resulting electrochemical H gradient provides energy for an array of secondary transport
systems (Serrano, 1988). Structurally, the fungal plasma membrane
ATPase is a member of the P class of ATPases (Pedersen and Carafoli,
1987), which includes the Na /K -ATPase
of animal cell membranes, the
H /K -ATPase of gastric mucosa, the
Ca -ATPase of sarcoplasmic reticulum, and the plasma
membrane Ca ATPases. Like these enzymes, it contains a
major M 100,000 subunit, which is partly
embedded within the membrane bilayer. During the reaction cycle, the
major subunit is phosphorylated at a conserved aspartate residue, and
also the ATPase activity is highly sensitive to vanadate, which
resembles the transition state of phosphate (Cantley et al.,
1978). For all ion-translocating ATPases, an important property is
the stoichiometric relationship between ions pumped and ATP molecules
split. The number of ions transported per ATP hydrolyzed is the prime
determinant of the capacity of these pumps to form a gradient
(Läuger, 1991). Two approaches have been used to
determine such stoichiometries (Briskin and Hanson, 1992; Sanders,
1990). On the one hand, there are kinetic approaches, in which the
addition of ATP leads to detectable transport into the lumen of
vesicles or organelles. In the case of the
Na /K - and
Ca -ATPases, net ion fluxes can be measured using
radioisotopes, but in the case of the H -ATPases, such
measurements are not possible. Instead, by employing weakly buffered
membrane suspensions, the pH change in the external solution measured
with a pH electrode or the change in intravesicular acidification
measured with pH probes has been taken as a measure for net
H fluxes. On the other hand, there is a thermodynamic
or electrophysiological approach, in which the free energy for ATP
hydrolysis is compared with the free energy available in the
steady-state ion gradient produced in vivo or in
vitro. As a result of these studies, most investigators favor a
stoichiometry of 1 H extruded per 1 ATP split for
P-type H -ATPases (Sanders, 1990), although it has been
suggested that in Neurospora this ratio is modified to 2
H /1 ATP split, by chronic energy restriction (Warncke
and Slayman, 1980). The results presented in this paper show that
the net efflux of H per ATP split by the yeast plasma
membrane H -ATPase is a flexible rather than a fixed
parameter. Apparently, this ratio can attain at least two values
determined by the regulatory state of the pump. Our experimental
findings can be explained by assuming that, in one of the regulatory
states, H pumping is essentially uncoupled from ATP
hydrolysis.
MATERIALS AND METHODS
Yeast Growth and Incubation
ConditionsSaccharomyces cerevisiae strain BWG1-7A (MATaade1-100 his4-519 leu2-3, 112
ura3-52) (Guarante et al., 1982) was grown to the
stationary phase overnight at 30 °C in medium containing 2%
glucose, 1% yeast extract (Difco), and 2% Peptone (Difco). Cells were
collected by centrifugation for 10 min at 3000 rpm (Sorvall SS-34
rotor) and washed twice with water. Yeast cells (30-150 mg (fresh
weight)/ml) were incubated for 10 min at room temperature with mild
agitation in water (glucose-starved cells) or in water supplemented
with 2% glucose (glucose-activated cells).
Homogenization and Membrane PreparationYeast
plasma membranes were purified from glucose-metabolizing and
glucose-starved cells by differential and sucrose gradient
centrifugation (Villalba et al., 1992). All steps were
performed at 4 °C. Cells (1 volume) were homogenized by vortexing
with glass beads (2 volumes; 0.5-mm diameter) in medium containing 20%
(v/v) glycerol, 10 mM Tris-HCl, pH 7.5, 1 mM EDTA,
and 1 mM dithiothreitol (buffer GTED 20) supplied with 1
mM phenylmethylsulfonyl fluoride and 0.1 mg/ml chymostatin.
Cell debris and glass beads were removed by centrifugation for 10 min
at 3000 rpm (Sorvall SS-34 rotor). The supernatant was diluted two
times with buffer GTED 20 and centrifuged for 60 min at 40,000 rpm
(Beckman Ti-70 rotor). The pellet was resuspended in 1 ml of buffer
GTED 20, layered on top of a 12-ml 43/53% (w/w) sucrose step gradient,
and centrifuged for 16 h at 30,000 rpm (Kontron TST 41.14 rotor).
Plasma membranes were collected from the 43/53% interface and diluted
four times with ice-cold water. After centrifugation at 50,000 rpm
(Beckman Ti-70 rotor) for 45 min, the pellet was resuspended in buffer
GTED 20 supplemented with 1 mM phenylmethylsulfonyl fluoride
and 0.1 mg/ml chymostatin. The plasma membrane fraction was frozen in
liquid nitrogen and stored at -80 °C.
Reconstitution of Plasma Membrane
H -ATPaseAll the following steps were
performed at room temperature. Mixed soybean phospholipids (30 mg/ml; L- -phosphatidylcholine, type II-S, Sigma) were dispersed
by vortexing under argon for 5 min in 10 mM Mes( )-KOH, pH 6.5, 50 mM K SO , and 20% (v/v) glycerol. Plasma
membranes (106 µg of protein) were mixed with lipids at a
lipid/protein mass ratio of 22 in a final volume of 208 µl. The
protein/lipid mixture was solubilized by the addition of 12 µl of 1 M octyl glucoside (Sigma), giving an effective mass ratio of
3. The mass ratio is given by the following equation: R = ([detergent] -
(critical micelle concentration of
detergent))/[phospholipids]. Unsolubilized material was
removed by spinning the protein/lipid/detergent mixture at 100,000
g for 10 min in a Beckman Airfuge and discarding the
pellet. Disposable syringes (2 ml), fitted with siliconized glass wool
at the bottom, were filled with Sephadex G-50 (fine, Pharmacia Biotech
Inc.) equilibrated in 10 mM Mes-KOH, pH 6.5, 50 mM K SO , and 20% (v/v) glycerol and
centrifuged for 5 min at 180 g. Solubilized
protein/lipid/detergent mixture (220 µl) was applied to the top of
the column and centrifuged again for 7.5 min at 180 g.
The volume of the eluate recovered was within 80-100% of the
volume applied.The volume of the vesicles was estimated from the
fluorescence of trapped pyranine within reconstituted membrane
vesicles. The reconstitution was performed as described above but
including 25 mM pyranine in the buffer used for reconstitution
and Sephadex G-50 equilibration to ascertain the presence of 25 mM pyranine inside eluted vesicles. In a second gel filtration step,
dye trapped in vesicles was separated from external dye. Using an
approximation for the surface area of 1 phospholipid molecule of 75
Å (Rossignol et al., 1982) and assuming pure
phospholipid vesicles, the mean vesicle radius was estimated.
ATPase AssayATPase activity was assayed according
to a modified protocol of Baginsky et al.(1967) with 1-3
µg of membrane protein at room temperature. The assay medium (100
µl) contained 20 mM Mes, 20 mM Mops, 50 mM KNO (to inhibit vacuolar ATPase), 5 mM NaN (to inhibit mitochondrial ATPase), 3.5 mM
Na MoO (to inhibit acid phosphatase), 1 mM Mg free in solution, and the indicated
concentrations of MgATP . The pH was adjusted to the
desired pH with N-methyl-D-glucamine. After 20 min,
the reaction was stopped by the addition of 500 µl of ice-cold stop
solution (10 ml of 102 mM ascorbic acid, 0.3 N HCl,
0.065% sodium dodecyl sulfate mixed with 1 ml of 57 mM NH -heptamolybdate to obtain a bright yellow solution).
The tubes were incubated for 10 min on ice to allow formation of the
P -molybdate complex. Excess molybdate was complexed by the
addition of 450 µl of a solution containing 154 mM NaAsO , 68 mM trisodium citrate, and 350
mM acetic acid. After 60 min at room temperature, a stable
color had developed, and absorbance at 860 nm was determined. Concentrations of free Mg and MgATP were calculated using and (Morrison,
1979; Wach et al.,
1990):
where K = 14.3 µM (dissociation constant, MgATP ), K = 1.44 mM (dissociation
constant, MgHATP ), and K = 0.107 µM (dissociation constant,
HATP ).
Measurement of pH with Acridine
OrangeH transport was assayed by measuring
acridine orange absorbance changes at 495 nm (Palmgren, 1990). Changes
in the absorbance of acridine orange observed during the formation of
pH gradients are due to accumulation of free dye inside the vesicles
and subsequent dimerization leading to a spectral shift of this
metachromatic dye (Palmgren, 1991). Reconstituted membrane vesicles
(50-100 µl; 0.5 mg of protein/ml) were diluted in 1 ml of 20
mM Mes-KOH, pH 6.0, 40 mM
K SO , 25 mM KNO , 30
µM acridine orange (Sigma), 5 mM NaN ,
3.5 mM Na MoO , and (when indicated) 0.5
µM valinomycin. The reaction was started by the addition
of 40 µl of 134 mM MgSO and 124 mM ATP, pH 6.0, to obtain a final concentration of 4 mM MgATP and 1 mM free Mg . The developed
pH gradient was dissipated by the addition of 0.5 µM nigericin.
Coupled Assay of ATPase Activity and Proton
TransportATP hydrolysis and H transport were
measured simultaneously with a Shimadzu UV-160A spectrophotometer by
coupling ATP hydrolysis to NADH oxidation (measured at 340 nm)
(Palmgren, 1990). The cycling time between measurements at 340 and 495
nm, respectively, was 12 s. Assay conditions were as described above
for H transport measurements employing acridine orange
but including 0.3 mM NADH, 2.4 mM phosphoenolpyruvate
(neutralized with KOH), 33 µg/ml pyruvate kinase (Boehringer
Mannheim 109 045; solution in glycerol), and 33 µg/ml lactate
dehydrogenase (Boehringer Mannheim 127 221; solution in glycerol).
Measurement of pH with PyraninePyranine
fluorescence was measured with a Perkin-Elmer LS 50B spectrofluorometer
at excitation/emission wavelengths of 460/511 nm. Plasma membrane
vesicles were reconstituted as indicated, but with 25 mM
pyranine (trisodium salt, pH 7.0; Molecular Probes, Inc.) included in
the reconstitution buffer. External probe was separated from vesicles
during the gel filtration step. The reaction cuvette was thermostatted
at 24 °C. The assay medium (3 ml) contained 20 mM Bis-Tris
propane-Mes, pH 7.0, 87.5 mM K SO , 50
nM valinomycin, and 10% glycerol. Membrane vesicles (10
µl; 5 µg of protein) were added to the reaction medium and
incubated until a stable fluorescence signal was observed. The ATPase
was energized by the addition of 120 µl of 126 mM MgS0 and 104 mM ATP, pH 7.0, giving rise to a
final concentration of 4 mM MgATP and 1 mM free
Mg .At the end of the experiment, internal and
external pH values were equilibrated by the addition of 80 nM nigericin, and the fluorescence signal was calibrated with pH in
the same cuvette by the addition of aliquots of 0.5 N HCl. A
calibration equation was made by fitting the fluorescence versus pH data with a second-order polynome, from which the
intravesicular pH during the experiment was calculated. In this way,
calibration of pyranine fluorescence with intravesicular pH was
achieved.
Passive Proton Fluxes and Determination of Passive Proton
PermeabilityThe net proton flux across the membrane was
calculated by derivation of the kinetics of pH gradient dissipation
taking into account the buffer strength (B) of pyranine (pK 7.2) and Mes (pK 6.1) according to the following
equation: J = B
(V/A) dpH/dt = B
(r/3) dpH/dt, where J is the net proton flux and V, A, and r are the volume, area, and radius
of the vesicle, respectively (Venema et al., 1993). In the
absence of a surface potential or diffusion potential, which was
ascertained in our experiments by high ionic strength and high
concentrations of K at both sides of the membrane in
the presence of valinomycin, the net proton permeability is given by
Fick's law according to the following equation: P = J
H , where P is the net proton permeability coefficient and H is the proton gradient between inside and outside of the vesicle
(Rossignol et al., 1982).
Measurement of  with Oxonol VIOxonol
VI fluorescence was measured at 614/646-nm excitation/emission
wavelengths (Venema et al., 1993). Development of an inside
positive membrane potential leads to uptake of the anionic dye into the
intravesicular space and to enhanced partitioning into the lipid
membrane, giving rise to an augmentation of fluorescence (Apell and
Bersch, 1987). The reaction medium contained 20 mM Mes
adjusted to pH 6.0 with KOH, 50 mM
K SO , 10% glycerol, and 50 nM oxonol
VI. Reconstituted vesicles (30 µl; 15 µg of membrane protein)
were added to the reaction cuvette. The H -ATPase
reaction was initiated by the addition of 120 µl of 134 mM MgS0 and 124 mM ATP, pH 6.0, giving rise to a
final concentration of 4 mM MgATP and 1 mM free
Mg .
Protein EstimationProtein concentration was
determined by the method of Bradford(1976) with the Bio-Rad protein
assay reagent and bovine serum albumin as the standard.
Gel Electrophoresis and ElectrotransferPlasma
membrane proteins were separated by SDS-polyacrylamide gel
electrophoresis on 10% acrylamide using the system of Laemmli(1970).
Western blotting with a polyclonal antibody against the C terminus of
the yeast plasma membrane H -ATPase (Monk et
al., 1991) and a second antibody conjugated to alkaline
phosphatase (Promega) was as described previously (Blake et
al., 1984).
Proton Extrusion ExperimentsCells were grown to
stationary phase overnight in growth medium containing 1% yeast
extract, 2% Peptone, and 2% glucose as carbon source. Cells were
pelleted and resuspended at a concentration of 1 10 cells/ml in 20 mM KCl, and 20 µM antimycin
when indicated. After incubation for 30 min, 2% glucose was added.
Acidification of the external medium was monitored for 10 min with a pH
electrode.
RESULTS
Effect of Glucose on H Extrusion
in VivoYeast cells suspended at high concentrations in
unbuffered medium supplemented with 20 mM KCl did not extrude
a significant number of H ions ( 0.01 pH unit/min
at 10 cells/ml) (Fig. 1). The initial pH of the
suspension of cells was close to 4. The addition of glucose (100
mM) to the yeast cells caused an extensive acidification of
the external medium after a lag phase of <1 min (initial rate of 0.7
pH unit/min at 10 cells/ml) (Fig. 1), in accordance
with Serrano(1983). The cells were able to reduce external pH to
3, at which point pH stabilized. The subsequent addition of
glucose had no effect on pH. The glucose effect was not affected by the
inclusion in the medium of antimycin (an inhibitor of electron
transport) and therefore was not the result of endogenous respiration
producing CO . Glucose-induced H secretion
was the same whether a fresh overnight culture of cells had been
starved for 1 h in H O or grown in the presence of
alternative carbon sources (e.g. glycerol). Therefore, the
glucose effect in vivo cannot be explained in terms of
glycolysis providing extra ATP to be utilized by the pump.
Figure 1:
Effect of glucose on in vivo H extrusion from yeast cells. Yeast cells, grown
in glucose medium to stationary phase, were washed in water and
resuspended in a solution of 20 mM KCl to a final
concentration of 10 cells/ml. H extrusion
was measured by monitoring the pH of the medium with a pH electrode. At
the arrow, 2% glucose was added. The initial rate of
H extrusion was 0.01-0.02 pH unit/min before the
addition of glucose and 0.5-0.7 pH unit/min after the addition of
glucose.
Effect of Glucose on Plasma Membrane ATPase
ActivityWhen yeast cells were incubated with glucose, a rapid
activation of the plasma membrane H -ATPase measured in
purified plasma membranes was observed (Fig. 2), in accordance
with Serrano(1983). The activation was rapidly reversed after glucose
removal, and it was therefore essential to homogenize the
glucose-metabolizing cells without washing. The ATPase activity of the
plasma membrane H -ATPase in isolated plasma membranes
from yeast grown in glucose was 3-5 times higher (3
µmol/min/mg of protein at pH 6.0) than in plasma membranes isolated
from yeast that had been deprived of glucose 10 min prior to
homogenization (Fig. 2).
Figure 2:
ATP
hydrolytic activity as a function of pH of plasma membranes isolated
from glucose-starved and glucose-activated cells. Plasma membranes were
isolated from glucose-starved and glucose-activated cells as described
under ``Materials and Methods.'' ATP hydrolytic activity was
measured by measuring the release of inorganic phosphate as described
under ``Materials and Methods'' with a MgATP concentration of
4 mM and 1 mM free Mg . The pH was
adjusted with N-methyl-D-glucamine. Triangles, glucose-starved; circles,
glucose-activated.
The glucose-activated ATPase had a
pH optimum around 6, whereas the nonactivated enzyme had a pH optimum
around 5.5 (Fig. 2). At all pH values studied, however, the
increase in specific activity was never more than 8 times ( Fig. 2and Fig. 4-6) compared with the >50-fold
increase in H efflux from whole cells after the
addition of glucose in vivo.
Figure 4:
Dependence
of the rate of ATP hydrolysis on the concentration of MgATP of native
and reconstituted plasma membrane ATPases from glucose-activated and
glucose-starved yeast cells. Plasma membranes were isolated from
glucose-starved and glucose-activated cells as described under
``Materials and Methods.'' ATP hydrolytic activity was
measured by measuring the release of inorganic phosphate as described
under ``Materials and Methods'' with MgATP concentrations
ranging from 0.25 to 7.5 mM and 1 mM free
Mg . The data represent the means of four independent
repetitions with the same membrane preparation. Open symbols,
native ATPase; closed symbols, reconstituted ATPase; triangles, glucose-starved ATPase; circles,
glucose-activated ATPase. The data were fitted to the following
equation: v/[E] = (a[S] + b[S] )/(1
+ c[S] + d[S] ) (Koland and Hammes, 1986) with the
following values for the constants a, b, c,
and d. Glucose-activated native membranes: a =
7.5 µmol/min/mg/mM, b = 2.1
µmol/min/mg/mM , c =
5.95/mM, and d = 0.47/mM and r = 0.998; glucose-activated
reconstituted membranes: a = 6.5
µmol/min/mg/mM, b = 4.2
µmol/min/mg/mM , c =
7.6/mM, and d = 1.2/mM and r = 0.998; glucose-starved native
membranes: a = 0.29 µmol/min/mg/mM, b = 0.22 µmol/min/mg/mM , c = 0.215/mM, and d =
0.188/mM and r =
0.997; glucose-starved reconstituted membranes: a =
0.043 µmol/min/mg/mM, b = 0.486
µmol/min/mg/mM , c =
0.35/mM, and d = 0.39/mM and r = 0.998. In the inset,
a logarithmic transformation of the data shows the fit to the Hill
equation. Values of 0.64 and 2.2 mM for H and K ` were calculated from the slope of the
line and the intercept with the yaxis, respectively,
for the glucose-activated ATPase and values of 1.64 and 2.9 mM for H and K ` for the glucose-starved
ATPase.
The promoter of the yeast
plasma membrane H -ATPase gene (PMA1) contains
recognition sequences for a promoter-binding factor positively
regulated by glucose (Capieaux et al., 1989). The
glucose-mediated increase in H -ATPase activity,
however, was rapid and completed within the 10 min of incubation. This
relatively rapid activation suggests that de novo synthesis of
H -ATPase does not contribute to the observed increase
in activity. This was supported by the protein staining and
immunostaining shown in Fig. 3(A-B). The plasma
membranes contained a prominent band of M 105,000 corresponding to the H -ATPase. The
intensity of this H -ATPase band was not increased in
samples from glucose-activated cells when compared with controls.
Figure 3:
SDS-polyacrylamide gel electrophoresis of
native and reconstituted plasma membrane vesicles from
glucose-activated (GA) and glucose-starved (GS) yeast
cells. A, plasma membranes (PM; 12.5 µg of
protein) were subjected to SDS-polyacrylamide gel electrophoresis as
described under ``Materials and Methods.'' The resulting gels
were stained with Coomassie Blue. B, Western blot analysis is
shown of plasma membranes (2.5 µg of protein). A polyclonal
antibody against the C terminus of the yeast plasma membrane
H -ATPase was used. C, plasma membranes (200
µl; 100 µg of protein) in the presence of asolectin and
detergent were subjected to centrifugation for 100,000 g in a Beckman Airfuge for 10 min. The pellet was resuspended in the
same volume. Equal volumes (25 µl) of total membranes (PM
+ det), supernatant (sup), and resuspended pellet (pellet) were subjected to SDS-polyacrylamide gel
electrophoresis. D, the supernatant from C was passed
through a Sephadex G-50 column as described under ``Materials and
Methods.'' An aliquot (25 µl) of the eluate (200 µl) was
diluted 8-fold and subjected to centrifugation for 100,000 g in a Beckman Airfuge for 30 min (pellet ). As a control, another aliquot
was diluted 8-fold, after which octyl glucoside was added at the same
concentration as during reconstitution to solubilize the vesicles
before subjecting it to centrifugation for 100,000 g for 30 min (pellet ). Undiluted
eluate (eluate; 25 µl) and the resulting pellets (pellet and pellet ; resuspended in 25 µl) were
subjected to SDS-polyacrylamide gel electrophoresis. Molecular mass
standards (in kilodaltons) are shown at the left
.
Reconstitution of Plasma Membrane
H -ATPaseIsolated yeast plasma
membranes do not form vesicles that are sufficiently tight to allow
measurements of H pumping. Our next goal was therefore
to reconstitute the H -ATPase into liposomes so that
its transport properties could be studied. The starting point for this
work was the discovery by Perlin et al.(1984) that when
isolated plasma membrane vesicles from Neurospora are
solubilized with deoxycholate in the presence of asolectin, vesicles
are re-formed when detergent is removed by column chromatography. In
reconstituted vesicles produced this way, Neurospora H -ATPase constitutes 35% of the protein. In
preliminary experiments, we observed that deoxycholate was not so
effective for reconstitution of the yeast H -ATPase
(data not shown). Octyl glucoside, on the contrary, was found to be
superior to deoxycholate and was used in subsequent experiments. Sodium dodecyl sulfate-polyacrylamide gel electrophoresis profiles
of plasma membranes and reconstituted vesicles are compared in Fig. 3. Densitometric scanning showed the 105-kDa
H -ATPase band to account for 20% of the total
Coomassie Blue-staining material in the plasma membranes. Octyl
glucoside solubilized 40-60% of the total protein and
80-90% of the H -ATPase (Fig. 3C). After treatment with octyl glucoside, the
relative amount of the M 105,000
H -ATPase band increased 2-fold to 40% of the
solubilized Coomassie Blue-staining material. The SDS-polyacrylamide
gel electrophoresis profile remained the same after detergent had been
removed by passage of solubilized material through the gel filtration
column. After spinning the reconstituted vesicles at 100,000 g in a Beckman Airfuge for 30 min, >50% of the protein was
pelleted (Fig. 3D, pellet ), suggesting that at least 50% of
the H -ATPase was effectively reconstituted.
Solubilized H -ATPase was not pelleted under these
conditions (Fig. 3D, pellet ). As judged from the intensity of
the 105-kDa band, the same amount of H -ATPase was
present in samples from glucose-activated and glucose-starved cells
during all stages of the reconstitution procedure (Fig. 3). The volume of vesicles was estimated from the fluorescence of
trapped pyranine in reconstituted membrane vesicles (Table 1).
When this value was compared with the molar amount of lipid present in
the samples, it was possible to estimate the mean vesicle size (Table 1). Reconstituted asolectin vesicles had a mean radius of
70 nm. The volumes of reconstituted plasma membrane vesicles were
smaller (mean radius of 40 nm) and were the same no matter whether
the vesicles were derived from glucose-starved or glucose-activated
cells.
ATP Hydrolysis by Native and Reconstituted
H -ATPasesThe dependence of ATP
hydrolysis on MgATP concentration was not affected by the
reconstitution procedure (Fig. 4). The ATP hydrolysis rate of
H -ATPase isolated from glucose-starved cells showed a
sigmoidal relationship on MgATP concentration (Fig. 4) that can
be fitted by the following equation: v/[E] = (a[S] + b[S] )/(1
+ c[S] + d[S] ) as described before (Koland and
Hammes, 1986). Two interpretations of these results are as follows. 1)
The enzyme possesses multiple catalytic sites that interact in a
positive cooperative way, and 2) the enzyme can exist in multiple
conformational states that catalyze MgATP hydrolysis by parallel
pathways (Koland and Hammes, 1986). After activation by glucose, we
found that the plot was no longer sigmoidal, but not purely hyperbolic
either. However, the data can still be fitted by the same equation as
above (Fig. 4). The shape of the curve obtained for
glucose-activated ATPase suggests negative cooperativity or the
presence of a mixture of enzymes catalyzing the same reaction. It is
thus theoretically possible that only part of the ATPase molecules are
activated upon addition of glucose, giving rise to a mixture of
glucose-activated and glucose-starved ATPases in this preparation. Our
data do not permit us to distinguish between the various possibilities.
Complex kinetics of the glucose-activated ATPase requiring an equation
composed by the sum of two Michaelian terms to fit the experimental
data has been described before (Berberián et
al., 1993). The data can also be fitted adequately by the Hill
equation: v = V
S /(K ` + S )
(see inset in Fig. 4), classically used to indicate
cooperative effects and which can also fit data obeying the equation
used by Koland and Hammes (Dixon and Webb, 1979). The difference in
shape between the curves for glucose-starved and glucose-activated
ATPases is described by changing the value of H from >1 (positive
cooperativity) to <1 (negative cooperativity), while the value of K ` remains approximately the same.
H Pumping by Reconstituted
H -ATPaseReconstitution of the plasma
membrane H -ATPase as outlined above allowed direct
demonstration of H pumping activity. The
MgATP-dependent intravesicular acidification of the plasma membrane
asolectin vesicles was followed by the quenching of acridine orange
absorbance (Palmgren, 1990). Upon addition of MgATP, a decay in
absorbance was observed, which leveled off within 2 min (Fig. 5A). The quenching of acridine orange absorbance
was stimulated severalfold by the K ionophore
valinomycin (0.5 µM) (Fig. 5A), which
dissipates the membrane potential, and was abolished by nigericin (0.1
µg/ml) (Fig. 5A), which catalyzes the
electroneutral exchange of H for potassium (Pressman,
1976).
Figure 5:
Effect of glucose on H transport and ATP hydrolysis by plasma membrane
H -ATPase in reconstituted vesicles. H transport activity and ATPase activity of plasma membrane
H -ATPase in reconstituted vesicles derived from
glucose-starved and glucose-activated cells were measured
simultaneously in the same cuvette as indicated under ``Materials
and Methods'' at pH 6.5. Note that only half the amount of protein
was used in those assays employing vesicles derived from
glucose-activated cells as compared with glucose-starved cells. A, H transport activity expressed as the
initial rate of acridine orange absorbance quenching at 495 nm; B, ATP hydrolytic activity as calculated from the coupled NADH
oxidation measured at 340 nm. Triangles, membranes from
glucose-starved cells (100 µg of membrane protein/ml); circles, membranes from glucose-activated cells (50 µg of
membrane protein/ml); open symbols, activity in the absence of
valinomycin; closed symbols, activity in the presence of 0.5
µM valinomycin. At the closed arrow, the reaction
was started by the addition of MgATP (4 mM MgATP + 1 mM Mg , final pH 6.5). At the open arrow, the pH gradient was collapsed by the addition of
0.5 µM nigericin. Numbers indicate activities in
terms of A /min/ml (H pumping) and nmol of ADP/min/ml (ATPase
activity).
ATP hydrolysis by the reconstituted plasma membrane
H -ATPase was measured in an assay in which ADP release
was coupled to oxidation of NADH. Since the absorbance spectra of
acridine orange and NADH are not overlapping, it was possible to
measure H pumping (Fig. 6, upperpanel) and ATP hydrolysis (lowerpanel)
simultaneously. Neither valinomycin (Fig. 6, lower
panel), which facilitates the formation of a pH gradient, nor
nigericin (data not shown), which dissipates the pH gradient, affected
ATPase activity significantly. The apparent insensitivity of ATP
hydrolysis to valinomycin observed here and by others (Dufour et
al., 1982; Serrano, 1984) suggests that the reversal potential for
ATP hydrolysis has not been reached in these systems. Thus, the maximal
rates of H pumping in the system are determined by the
passive H permeability of the vesicles, and the
quenching of acridine orange absorbance levels off when H influx matches H efflux.
Figure 6:
ATP dependence of H
transport activity and ATP hydrolytic activity of reconstituted
H -ATPase derived from glucose-starved (GS)
and glucose-activated (GA) cells. H transport
and ATP hydrolysis were measured simultaneously as described under
``Materials and Methods'' with 50 µg of membrane
protein/assay, MgATP concentrations ranging from 0
to 6 mM, and 1 mM free Mg , pH 6.0,
and in the presence of 0.5 µM valinomycin. Note that
H pumping by the glucose-activated ATPase was
increased significantly more than ATP hydrolysis. Closed
symbols, proton pumping; open symbols, ATPase activity.
The experimental data were fitted to the following equation: v/[E] = (a[S] + b[S] )/(1
+ c[S] + d[S] ) (Koland and Hammes, 1986). For the
glucose-activated ATPase, the values were as follows: a = 15 A /min/mg/mM and b = 5.6
A /min/mg/mM (H pumping) or a = 5.3
µmol/min/mg/mM and b = 2.0
µmol/min/mg/mM (ATP hydrolysis) and for both
H pumping and ATP hydrolysis, c =
2.7/mM and d = 0.44/mM .
For the glucose-starved ATPase, the values were as follows: a = 0.12 A /min/mg/mM and b = 0.40
A /min/mg/mM (H pumping) or a = 0.39
µmol/min/mg/mM and b = 1.31
µmol/min/mg/mM (ATP hydrolysis) and for both
H pumping and ATP hydrolysis, c =
0.79/mM and d =
1.12/mM .
H pumping and the hydrolysis of ATP were catalyzed by the same
enzyme as based on the following observations. (a)
H pumping and ATPase activity exhibited similar
dependence on MgATP concentration (Fig. 6), and (b)
comparable pH-activity profiles were observed for both H pump activity and ATPase activity in the activated as well as the
nonactivated state (data not shown).
Effect of Glucose on H Pumping by
ATPaseThe glucose-activated ATPase had an increased
potential for H pumping that exceeded the increase in
specific ATPase activity by about an order of magnitude ( Fig. 5and 6). Calculated on an equal protein basis, the rate of
H transport exhibited by the glucose-activated ATPase
was 20-50 times higher than that of the nonactivated ATPase.
Thus, the relative change in H transport observed
between glucose-activated and nonactivated ATPases matches the relative
changes in H efflux in vivo when yeast cells
are challenged with glucose.Internal pH in liposomes containing
H -ATPase from glucose-starved and glucose-activated
cells was estimated using the fluorescent pH probe pyranine (Fig. 7). Glucose-activated H -ATPase was able
to acidify the interior of the vesicles from pH 7.0 to 6.9, whereas
glucose-starved H -ATPase could not produce any
detectable acidification of the intravesicular volume.
Figure 7:
Internal pH in liposomes containing
reconstituted plasma membrane H -ATPase from
glucose-activated (GA) and glucose-starved (GS)
cells. Internal pH was calculated from the fluorescence of the pH probe
pyranine trapped inside reconstituted vesicles as described under
``Materials and Methods.'' The reaction was started by the
addition of 4 mM MgATP and 1 mM free
Mg , pH 7.0. At the end of the experiment, the pH
gradient was abolished by the addition of 80 nM
nigericin.
We next
employed the  probe oxonol VI to study the electrogenic
properties of the two regulatory states of the
H -ATPase. It appeared that the glucose-activated
enzyme readily established a membrane potential both in the absence and
presence of K (Fig. 8). In marked contrast, the
glucose-starved enzyme did not produce a clear fluorescence signal (Fig. 8). As expected, the stability of the membrane potential
was influenced by the presence of K in the
intravesicular medium. However, K did not alter the
maximal amplitude of the signal produced by glucose-starved and
glucose-activated H -ATPases.
Figure 8:
Changes in  in liposomes
containing plasma membrane H -ATPase from
glucose-activated (GA) and glucose-starved (GS)
cells.  was measured by oxonol VI fluorescence quenching as
described under ``Materials and Methods.'' Upon development
of an inside positive membrane potential by the
H -ATPase, the probe will fix to the internal leaflet
of the membrane, giving rise to an augmentation of fluorescence. A, membranes were reconstituted as described under
``Materials and Methods'' with 50 mM K SO . ox, oxonol. B,
membranes were reconstituted in the absence of K .
MgSO (1 mM) was included instead of
K SO to screen the negative charges of the
phospholipids. The membrane potential was abolished by the addition of
valinomycin (50 nM; A) or gramicidin (200
nM; B).
Passive Ion Permeability of Reconstituted
VesiclesIn principle, H accumulation in
membrane vesicles could be stimulated (a) indirectly by
preventing the formation of a membrane potential that could otherwise
inhibit H influx (e.g. by affecting the
permeability of a secondary system), (b) by reducing the
passive efflux of H from the vesicles, or (c)
by direct stimulation of H transport systems. Electrical balance between the exterior and interior of the membrane
vesicles was obtained during the assay since the potassium ionophore
valinomycin was present. In the absence of valinomycin, the passive
permeability of the membrane to K was determined
according to Venema et al.(1993). Glucose treatment did not
change the estimated K permeability (data not shown). The permeability coefficient for H was determined
by analyzing the dissipation of an imposed pH gradient (Fig. 9).
Intravesicular pH was determined by the pH probe pyranine. After
imposing a pH gradient of 1.1 pH units (pH outside = 7.6; inside
= 6.5), intravesicular pH was monitored as a function of time (Fig. 9, left panels). The kinetics of H fluxes could be fitted by a single exponential function (Fig. 9, right panels). First-order kinetics is
indicative of emptying a single compartment through a homogeneous
barrier. If multilamellar structures had been present, more complex
kinetics would have been expected. The permeability coefficients for
proteoliposomes derived from glucose-activated cells, glucose-starved
cells, and liposomes derived from asolectin were 1.74 ± 0.44
10 , 2.20 ± 0.35
10 , and 1.20 ± 0.27 10 m s , respectively, confirming that
glucose treatment did not alter the passive permeability of the
proteoliposomes to H . Taken together, these results
suggest that glucose stimulates the active H influx.
Figure 9:
Passive H permeabilities
of reconstituted plasma membrane vesicles prepared from glucose-starved (GS) and glucose-activated (GA) cells. Plasma
membrane vesicles were reconstituted as described under
``Materials and Methods'' in the presence of 2 mM pyranine. Reconstituted vesicles (10 µl; 5 µg of protein)
were added to 3 ml of 10 mM Mes adjusted to pH 6.5 with KOH,
50 mM K SO , 50 nM valinomycin,
and 20% glycerol. The pH of the medium was next raised to pH 7.6 by the
addition of 30 µl of 1 MN-methyl-D-glucamine, and the time course of
augmentation of pyranine fluorescence at a 460-nm excitation wavelength
was followed. The fluorescence signal was calibrated with pH as
described under ``Materials and Methods'' (left
panels). The proton flux (right panels) and permeability
coefficients were calculated as described under ``Material and
Methods.'' The kinetics of the proton fluxes were fitted by a
logarithmic function (right panels, smooth lines). The
estimated permeability coefficients were 1.74 ± 0.44
10 m s for reconstituted
glucose-activated membranes, 2.20 ± 0.35 10 m s for reconstituted glucose-starved
membranes, and 1.20 ± 0.27 10 m
s for reconstituted
liposomes.
DISCUSSION
It was shown by Serrano(1983) that ATP hydrolytic activity of
the plasma membrane H -ATPase is positively regulated
by glucose. We have found that glucose-activated yeast plasma membrane
H -ATPase has an increased potential for H pumping that is about an order of magnitude higher than the
increase in specific ATPase activity ( Fig. 5and Fig. 6).
The glucose-starved H -ATPase was hardly able to
establish a membrane potential across the vesicle membrane (Fig. 8), suggesting that in this regulatory state, the
H -ATPase is not functioning as an electrogenic pump.
The fact that H accumulation is stimulated to a higher
degree by glucose than is ATP hydrolysis suggests that H pumping can be regulated independently of ATP hydrolysis. Glucose
may alter the H /ATP stoichiometry of the plasma
membrane H -ATPase or promote coupling of ATP
hydrolysis to H translocation. It is possible that
the absence of a functioning state of the H -ATPase
could be due to its relative sensitivity to denaturation by detergent,
in the regulatory state induced by glucose starvation. This, however,
seems unlikely since the enzyme under the experimental conditions
readily hydrolyzes ATP, and the dependence of ATP hydrolysis on MgATP
concentration was not altered by the reconstitution procedure (Fig. 3). Another possibility is that the successful
reconstitution of enzyme units into sealed vesicles is affected by the
same structural change, e.g. regulatory phosphorylation, which
could affect enzyme lability or structure. However, we have
demonstrated that a large fraction of the detergent-solubilized protein
is incorporated into structures that sediment, and we have shown that
there is no visible difference in the amount of protein incorporated
when starved and glucose-activated membranes are the source or in the
amount of ATPase activity recovered. In addition, the volume of
vesicles harboring glucose-starved and glucose-activated
H -ATPases was the same, indicating that the same
amount of sealed vesicle structures is present in both preparations.
Therefore, although it remains formally possible that stability of
function to the reconstitution procedure may be influenced by the
glucose-induced modification, the evidence presented strongly supports
a model in which glucose activation modifies the coupling efficiency of
the H -ATPase. An alternative artifact is that the
acridine orange signal is not linearly related to changes in the rate
of H pumping. This is less likely since acridine
orange absorbance changes were closely related to changes in ATPase
activity when ATP concentration (Fig. 6) and pH (data not shown)
were altered. In addition, by employing two fluorescent probes
(pyranine and oxonol VI) that report intravesicular pH (Fig. 7)
and  (Fig. 8), respectively, the discrepancy between
activation of H pumping and ATP hydrolysis was
confirmed. The maximal gradient in our system is probably determined
by the high H leakiness of the liposomes both in the
presence and absence of protein (Fig. 9). The maximal pH
gradient produced by the glucose-activated ATPase amounted to 0.1 pH
unit (measured at pH 7.0 in the extravesicular medium) when using
pyranine as a probe to report intravesicular pH (Fig. 7), and 1
pH unit (pH 6.0 in the extravesicular medium; pH 5.0 inside the
vesicles) (data not shown) when measured by employing acridine orange
and using the pH jump method introduced by Dufour et
al.(1982). This discrepancy is probably caused by the different
mechanism by which these probes report pH gradients. Pyranine, trapped
inside the lumen of vesicles, reports the mean internal pH of all
vesicles. Acridine orange, on the contrary, only accumulates inside
vesicles that harbor functional H -ATPase. Thus, it
seems likely that a population of vesicles does not contain any
H -ATPase at all. Using pure Neurospora H -ATPase protein, a different reconstitution
procedure, and 100 times more asolectin relative to protein than in the
present study, Goormaghtigh et al. (1986) found that <0.5%
of liposomes contained H -ATPase. Most authors have
suggested a coupling ratio of 1 H transported per ATP
hydrolyzed for plasma membrane H -ATPase from yeast
(Serrano, 1984), Neurospora (Warncke and Slayman, 1980;
Perlin et al., 1986), algae (Blatt et al., 1990), and
higher plants (Brauer et al., 1989; Briskin and
ReynoldsNiesman, 1991). The limits for the H /ATP
stoichiometry of the pump are set by the free energy supplied by the
chemical reaction per turnover (Läuger, 1991). If
the pump is tightly coupled and if leakage pathways are negligible, the
system reaches equilibrium when the electrochemical gradient
counterbalances the chemical driving force ( G). If the
pump translocates n ions/cycle, this equilibrium condition is
given by the following equation: G = n(RT 2.3 pH + zFV) (where z is the valency of the ion, F is the Faraday
constant, and V is the membrane potential). Assuming that the
free energy for ATP hydrolysis under physiological conditions is
40 kJ/mol, the maximal pH gradients that can be created (for V = 0) would be 6.8, 3.4, and 0.68 for n = 1,
2, and 10, respectively. In vivo, glucose-metabolizing cells
can sustain pH gradients of at least 4 pH units (Serrano, 1984). The
size of the electrical gradient produced by the plasma membrane
H -ATPase (membrane potentials of up to 300 mV are
generated by the Neurospora H -ATPase
(Gradmann et al., 1978)) makes it a potent electrogenic
transport protein. With a ratio of 5-10 H pumped
per ATP consumed, the maximal capacity for formation of electrochemical
gradients would be far below these values. It is therefore reasonable
to suggest a 1 H /ATP stoichiometry for the ATPase
under conditions where it generates maximal pH gradients and membrane
potentials. The initial rates of H translocation
observed by us suggest that the glucose-activated
H -ATPase translocates more H per ATP
consumed than the enzyme isolated from glucose-deprived cells (Fig. 5). Assuming that the activated H -ATPase
operates with a stoichiometry of 1 H /ATP, our results
immediately suggest that the stoichiometry of the nonactivated yeast
ATPase is <1 H /ATP (e.g. 0.1), i.e. net transport of H is essentially uncoupled from
the splitting of ATP. In future studies, the actual
H /ATP stoichiometry of the purified yeast plasma
membrane H -ATPase before and after glucose activation
needs to be determined, e.g. by optimizing the reconstitution
procedure, by a thermodynamic approach using the patch-clamp method
(Davies et al., 1994), or after reconstitution of the ATPase
into planar lipid bilayer membranes (Ziegler et al., 1993). Intrinsic uncoupling (defined here as ATP hydrolysis without net
translocation of the full potential complement of H )
has previously been suggested to play a role in the regulation of a
variety of ion pumps such as bacteriorhodopsin (Westerhoff and
Dancsházy, 1984; Caplan, 1988), vacuolar
H -ATPase (Davies et al., 1994; Kibak et
al., 1993; Tu et al., 1987; Yoshinori and Nelson, 1988),
cytochrome oxidase (Blair et al., 1986),
F F -ATPase (Krenn et al., 1993; Muller,
1993; Pietrobon et al., 1986; van Walraven et al.,
1990), and sarcoplasmic reticulum Ca -ATPase (Caplan,
1988; Inesi and de Meis, 1989; Meltzer and Berman, 1984; Navarro and
Essig, 1984; Soler et al., 1990). Intrinsic uncoupling has
been suggested to play a role in providing a ``safety valve''
for the formation of gradients (Caplan, 1988) or in matching the pump
to the load for optimization purposes (Stucki, 1980). The
mechanistic implications of H -ATPase uncoupling remain
to be explored. Intrinsic uncoupling of H -ATPase may
arise in at least two ways (Läuger, 1991). First,
kinetic studies on members of the P class of ATPases suggest that
hydrolysis of the aspartylphosphoryl (E-P) intermediate is
closely associated with the simultaneous translocation of the
transported ion(s). The phosphorylated state, however, may
spontaneously dephosphorylate without ion translocation (slippage).
However, since the nonactivated ATPase is not deficient in H transport and is able to build up a H gradient (Fig. 5A), slippage would have to be partial. Second,
glucose activation may result in a decreased H permeability intrinsic to the yeast plasma membrane
H -ATPase. Intrinsic H transport in
the reverse direction by a process that is not linked to ATP synthesis
may take place without conformational change of the protein (tunneling)
or may occur by a carrier-like operation mode of the pump involving
conformational changes. At least tunneling may be specific for active
ATPases (Fröhlich, 1988), which could explain why
the apparent passive permeability of vesicles, measured in absence of
ATP, is not affected by glucose regulation of the
H -ATPase (Fig. 9). It is thus possible that the
intrinsic pathway is rendered more permeable under conditions of pump
turnover, allowing a higher leakage of H . Removal
of the last 11 amino acids from the yeast H -ATPase
(Glu stop) produces an enzyme in glucose-starved
cells with kinetic parameters similar to those of the glucose-activated
wild-type H -ATPase (Portillo et al., 1989).
The truncated H -ATPase is not activated further in
glucose-metabolizing cells. The same phenotype is exhibited by a
mutation (Ala Val) affecting a residue in the
nucleotide-binding site that is located in the large central
cytoplasmic domain (Cid and Serrano, 1988). Therefore, the C terminus
seems to interact with this site. Glucose-activated
H -ATPase is phosphorylated at a residue not
phosphorylated in glucose-starved cells (Chang and Slayman, 1991). A
double mutation at the C terminus destroying putative phosphorylation
sites (Ser Ala,Thr Ala) locks
the enzyme in the inhibited state. This double mutation results in
almost no activation of the H -ATPase by glucose and no
growth of yeast in glucose medium (Portillo et al., 1991),
suggesting that kinase-mediated phosphorylation of amino acids at the C
terminus is part of the glucose response. A Tyr
Gly mutant at the top of transmembrane segment M5 of the
Ca -ATPase of sarcoplasmic reticulum is uncoupled in
the sense that it catalyzes a high rate of
Ca -activated ATP hydrolysis without net accumulation
of Ca in membrane vesicles (Andersen, 1995). It has
been suggested that the side chain of Tyr might play a
critical role in the gating mechanism normally preventing the occluded
calcium ions from dissociating to the cytoplasmic site upon
dephosphorylation (Andersen, 1995). In analogy, one could speculate
that the C terminus of the yeast H -ATPase stabilizes a
conformation of the enzyme that is unable to effectively occlude
H . Jencks(1980) has defined certain rules for the
reaction cycle that need to be obeyed for coupling in ion pumps. The
main concept that emerges is that ATP hydrolysis does not occur without
ion transport, and no reverse flux of ions occurs without ATP
synthesis. Thus, existing models for ion pumps, which are generally
based on mechanisms having integral stoichiometry, cannot account for
our experimental findings of variable coupling. Since uncoupling would
theoretically result in futile cycling of ATP and is typically induced
only under in vitro conditions, variable stoichiometry has
remained a controversial concept. In this paper, we have demonstrated a
change in coupling ratio of an ion pump induced by a metabolite under in vivo conditions. This points to a physiological role for
uncoupling as a mechanism for regulation of pump activity. The tightly
coupled high activity state induced by glucose may be essential for the
formation of the very steep H gradients required for
efficient solute uptake. Regulated uncoupling may be advantageous when
taking into consideration that, with a stoichiometry of 1
H /ATP, yeast H -ATPase is
physiologically irreversible (Serrano, 1984). Uncoupling intrinsic to
the pump would allow for regulation of the magnitude of the
steady-state electrochemical gradient. Still, the partially uncoupled
low activity state of the ATPase may be sufficient to maintain
H gradients required for normal growth. It seems
clear, however, that extensive kinetic controls must operate to avoid
undesired H leakage or futile consumption of ATP.
FOOTNOTES
- *
- This work was supported by the Danish Natural
Science Research Council, the NOVO Nordisk Fonden, and the European
Communities' BIOTECH Programme as part of the Project of
Technological Priority 1993-1996. The costs of publication of
this article were defrayed in part by the payment of page charges. This
article must therefore by hereby marked
``advertisement'' in accordance with 18 U.S.C.
Section 1734 solely to indicate this fact.
- §
- A European Molecular Biology Organization short
term fellow.
- ¶
- To whom correspondence should be
addressed. Tel.: 45-3528-3338; Fax: 45-3528-3333.
- (
) - The abbreviations used are: Mes,
4-morpholineethanesulfonic acid; Mops,
3-(N-morpholino)propanesulfonic acid.
ACKNOWLEDGEMENTS
We are grateful to Frank C. Lanfermeijer and Morten
Kielland-Brandt for valuable discussions and critical reading of the
manuscript.
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