Plant Physiol. (1999) 121: 253-262
Sulfate Is Both a Substrate and an Activator of the
Voltage-Dependent Anion Channel of
Arabidopsis Hypocotyl
Cells1
Jean-Marie Frachisse*,
Sébastien Thomine2,
Jean Colcombet,
Jean Guern, and
Hélène Barbier-Brygoo
Institut des Sciences Végétales, Centre National de la
Recherche Scientifique, Unité Propre de Recherche 40, Avenue de
la Terrasse, 91198 Gif sur Yvette cedex, France
 |
ABSTRACT |
On the
basis of the anion content of in vitro-cultured Arabidopsis plantlets,
we explored the selectivity of the voltage-dependent anion channel of
the plasma membrane of hypocotyl cells. In the whole-cell
configuration, substitution of cytosolic Cl
by different
anions led to the following sequence of relative permeabilities:
NO3
(2.6)
SO42
(2.0) > Cl
(1.0) > HCO3
(0.8)
malate2
(0.03). Large whole-cell currents were measured
for NO3
and SO42
,
about five to six times higher than the equivalent Cl
currents. Since SO42
is usually considered to
be a weakly permeant or non-permeant ion, the components of the large
whole-cell current were explored in more detail. Aside from its
permeation through the channel with a unitary conductance, about
two-thirds that of Cl
, SO42
had
a regulatory effect on channel activity by preventing the run-down of
the anion current both in the whole-cell and the outside-out configuration, increasing markedly the whole-cell current. The fact
that the voltage-dependent plasma membrane anion channel of hypocotyl
cells can mediate large NO3
and
SO42
currents and is regulated by nucleotides
favors the idea that this anion channel can contribute to the cellular
homeostasis of important metabolized anions.
 |
INTRODUCTION |
Plant anion channels play central roles in signal transduction and
cell turgor regulation. They have been implicated in stomatal function,
where their activation is thought to be one of the limiting steps in
the loss of guard cell turgor leading to stomatal closure (for review,
see Ward et al., 1995
). Pharmacological arguments in favor of the
involvement of anion channels in elicitor signal transduction have been
obtained in cultured parsley and soybean cells (Ebel and Cosio, 1994
;
Jabs et al., 1997
). Recent studies in Arabidopsis hypocotyls have also
shown that anion channel activation might be a step in the transduction
of two signals modulating hypocotyl growth: blue light (Cho and
Spalding, 1996
) and auxin (Thomine et al., 1997b
). Although anion
channels are implicated in a wide range of physiological functions in
plant cells, their detailed characterization is still far from complete
in differentiated cells other than stomatal guard cells.
The determination of ions that permeate a channel is important, as it
may be indicative of its specific physiological role. In particular,
the ability of a given channel to transport a particular anion species
suggests that this channel could be involved not only in the general
processes of membrane depolarization and cell turgor decrease but also,
more specifically, in the regulation of the concentration of this
anion. For some anions such as
NO3
, which are substrates
for intracellular metabolic enzymes, this type of regulation might be
important to maintain a suitable intracellular concentration. In
parallel with patch-clamp studies of animal systems, the properties of
most plant anion channels have been explored with
Cl
as the permeating anion, in spite of the
fact that Cl
is rarely accumulated in plant
cells at high concentrations. Anions other than
Cl
could be more relevant substrates for plant
anion channels, but only in a few cases has the selectivity of anion
channels been extensively studied (Hedrich and Marten, 1993
; Elzenga
and VanVolkenburgh, 1994; Schmidt and Schroeder, 1994
; Skerrett and
Tyerman, 1994
).
Previous studies of anion channels residing at the plasma membrane in
the hypocotyl epidermal cells of Arabidopsis allowed us to characterize
a voltage-dependent anion channel (Thomine et al., 1995
). This channel
is tightly controlled by the transmembrane voltage, being deactivated
at resting membrane potentials and activated by depolarization. In a
detailed study, we recently showed that voltage regulation is under the
control of cytoplasmic nucleotides and does not require nucleotide
hydrolysis (Thomine et al., 1997a
). A pharmacological characterization
of the channel has revealed a poor sensitivity to most anion channel
blockers except niflumic acid (Thomine et al., 1997a
). We explored the selectivity of this channel toward physiological anions, which has not
been previously investigated to our knowledge. Analysis of the anion
content of in vitro-grown Arabidopsis plantlets showed that
NO3
,
SO42
, and
PO42
are the major accumulated anions. This gave
hints about which anions might be substrates for the voltage-dependent
anion channel. Indeed, whole-cell patch-clamp recording with various
internal anions revealed a high current amplitude for
NO3
and, unexpectedly,
for SO42
compared with
Cl
. Further experiments using
SO42
, which is usually
considered to be an non-permeant anion, provided arguments that this
anion not only permeates the channel but also regulates its activity.
 |
MATERIALS AND METHODS |
Plant Material and Protoplast Isolation
Arabidopsis (ecotype Columbia) seedlings were grown on a medium
containing 5 mM KNO3, 2.5 mM
K2HPO4/KH2PO4,
pH 6.0, 2 mM MgSO4, 1 mM
Ca(NO3)2, 1 mM
MES, 50 µM Fe-EDTA, Murashige and Skoog micro-elements (Murashige and Skoog, 1962
), 10 g/L Suc, and 7 g/L agar. Culture conditions were 21°C and a 16-h daylength at lighting levels of 120 µE m
2 s
1 with neon
tubes (a combination of Mazdafluor, Blanc Industrie, Lille,
France, and Mazdafluor, Prestiflux, Lille, France).
Seedlings aged 7 to 12 d were used for electrophysiological
investigations. Hypocotyls were excised from 30 to 40 seedlings, and
protoplasts were isolated according to the method of Elzenga (1991)
as
described in Thomine et al. (1995)
.
Electrophysiological Investigations
Patch-clamp experiments were performed as described by Hamill et
al. (1981)
using a patch-clamp amplifier (EPC 7, List Electronic, Darmstadt, Germany) with a low-pass filter (8-pole Bessel filter) for
whole-cell recordings, and an amplifier (model 200A, Axon Instruments,
Foster City, CA) for single-channel recordings. During measurements,
freshly isolated epidermal protoplasts from Arabidopsis hypocotyls were
maintained in bathing medium: 50 mM
CaCl2, 5 mM MgCl2, and 10 mM MES-Tris, pH 5.6. The pipettes were filled with 150 mM KCl (or other
K+ salts as indicated), 2 mM
MgCl2, and 10 mM Tris-HEPES, pH 7.2, supplemented with either 5 mM MgATP and LiGTP or 1 or 3 mM MgATP, as indicated in the figure legends. The free
Ca2+ concentration of 1 µM in the
pipette, calculated with Ligandy software (Steinhardt Software
Bank, Berkeley, CA), was obtained with 5 mM EGTA and 4.2 mM CaCl2. The osmolalities of both
solutions were adjusted to 450 mosmol with mannitol using a vapor
pressure osmometer (model 5500, Wescor, Logan, UT). Gigaohm resistance seals between pipettes (pipette resistance, 1-5 M
)
coated with Sylgard (General Electric) pulled from capillaries
(Kimax-51, Kimble Glass, Owens, IL) and protoplast membranes were
obtained with gentle suction leading to the whole-cell configuration.
The liquid junction potentials were measured according to the method of
Neher (1992)
, and all potentials given, including reversal potentials
(Erev), have been corrected by
subtracting the junction potentials for each ionic condition (150 mM Cl
, 2 mV; 150 mM
NO3
, 4 mV; 75 mM
SO42
, 11 mV; 75 mM malate, 19 mV; and 150 mM
HCO3
, 13 mV). Whole-cell
currents were measured in response to 10-s voltage ramps from
180 mV
to +80 mV. We checked that the estimation of the
Erev was independent of the voltage
protocol, and similar values were measured using voltage pulse
protocols or ramps starting from a positive voltage. We also ensured
that, even when we used a two-times faster ramp, the I-V relationship
stayed at steady state. To exclude recordings presenting a
voltage-independent current, a leak was determined as the linear
component between a hyperpolarized potential at which the
voltage-dependent current is completely deactivated, and 0 mV, the
value at which the leak current is null. The I-V relationships for
which the contribution of leak at the peak potential was larger than
30% of the peak current were rejected. Therefore, the permeability
ratio has not been corrected.
Outside-out patches were obtained by withdrawing the pipette from the
whole-cell configuration. The single-channel recordings were stored on
videotape, and digitized with a sample interval of 0.1 ms (five times
the filter frequency) using Fetchex (pClamp 6.0.2. Axon Instruments)
for analysis. The distribution of amplitudes was fitted by a Gaussian
model in pSTAT patch-clamp software (pClamp version 6.0.2., Axon
Instruments).
Application of voltage programs and handling of the data were performed
using a Digidata 1200 interface (Axon Instruments) and pClamp
software with Clampex and Clampfit. The filter frequency was set to 2 kHz, and capacitive transients were corrected during the patch-clamp
experiments. The series resistance was compensated to more than 85%
when the access resistance was higher than 5 M
. Unless
otherwise indicated, figures are shown for one representative protoplast, and statistics are given as means ± SE
(n indicates the number of protoplasts tested).
Permeability ratios for mixtures of Cl
and
other monovalent anions
(Pmonoval/PCl)
or for mixtures of Cl
and divalent anions
(Pdival/PCl)
were calculated from Erev measurements with Equations 1 and 2, respectively. Both equations were derived from
the Goldman-Hodgkin-Katz equation (Lewis, 1979
) and adapted to anions.
|
(1)
|
|
(2)
|
where E is the Erev,
R is the gas constant, T is the absolute
temperature, F is the Faraday's constant,
Cle and Cli are the extracellular and intracellular activities of
Cl
, respectively, and
Ai(monoval) and
Ai(dival) are the extracellular and
intracellular activities of the other intracellular monovalent or
divalent anions, respectively. Activity coefficients were estimated according to the method of Dean (1985)
.
Anion Content Analysis
Eleven-day-old plantlets grown in vitro on the same medium and in
the same conditions as for electrophysiological investigations were
harvested. Plants were gathered in pools of five and cut at the level
of the crown in order to remove the roots. Each sample (fresh weight
around 20 mg) was ground in liquid nitrogen, transferred into an
eppendorf tube, suspended in 500 µL of ultrapure water, and
centrifuged for 2 min at 4,000g. The supernatant was
collected and stored. The pellet was re-extracted three times using the same procedure. The four supernatants of each sample were pooled, filtered on 0.2-µm sterilized filters (DynaGard, Microgon, Laguna Hills, CA), and used for capillary microelectrophoresis ion
determination. The anion concentrations were expressed relative to the
plant volume (moles per liter of plant) assuming that the plantlet
density is 1 g mL
1.
Capillary electrophoresis was performed with an automated analyzer
(Quanta 4000, Waters) controlled by a computer fitted with Millenium
2010 software (Waters) running in a Windows environment. Analog data
(20-Hz sampling rate) were collected from the column absorbance
inverse-UV detector (254 nm). The silica capillary dimensions were 75 µm i.d. and 60 cm length. The electrolyte solution used for migration
was 4.6 mM chromate and 0.5 mM
OFM-Br
at pH 8.0. Separations were performed
using a 20-kV applied potential.
 |
RESULTS |
Anion Selectivity and Permeability of the Voltage-Dependent
Anion Channel
We previously identified a channel with a strong
voltage-dependence at the plasma membrane of protoplasts from epidermal
cells of Arabidopsis hypocotyls. Using Cl
as
the permeant anion, this channel was shown to carry essentially anion
currents (Thomine et al., 1995
). In the presence of 5 mM intracellular ATP (Thomine et al., 1997a
), a voltage ramp from
180 to
80 mV applied at the plasma membrane in the whole-cell configuration
allowed us to record an anion current with the characteristic voltage
dependence displayed in Figure 1A. For
potentials more negative than
130 mV, no current was recorded.
Depolarization of the membrane to potentials more positive than
130
mV activated an inward current corresponding to an outward anion flux.
For voltages more positive than the peak potential, the current
decreased with the diminution of the driving force for anions and
reversed as this driving force became in favor of anion influx. The
flattening of the curve in the vicinity of the
Erev indicated a marked rectification of the current in this voltage range.

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| Figure 1.
Current-voltage relationships of the
voltage-dependent anion channel for various intracellular anions.
Whole-cell currents were measured on hypocotyl epidermal protoplasts.
The currents result from a 10-s voltage ramp from 180 mV to +80 mV
applied at the plasma membrane. I-V curves were obtained in the
presence of 150 meq Cl (A), 150 meq
NO3 (B), 150 meq
SO42 (C), 150 meq
HCO3 (D), or 150 meq malate2
(E). For comparison, each I-V curve is presented with the
Cl current corresponding to 150 meq Cl .
Note the different current scalings for A and B, C and D, and E. The
bath solution contained 110 mM Cl and the
pipette solution contained 5 mM ATP, 5 mM GTP,
150 meq of the anion to be tested, and 12.4 mM
Cl . Representative I-V curves from data sets of five to
10 independent recordings for each anion are shown, and arrows indicate
the position of Erev on the voltage axis.
The inset in A shows an expanded picture of the
Erev region.
|
|
To get hints about the possible substrates for plant anion channels, we
analyzed the anion content of young plantlets used to prepare hypocotyl
protoplasts. The anion content analysis was performed on the aerial
part of Arabidopsis seedlings grown and harvested in the same
conditions as for patch-clamp experiments. In 11-d-old plantlets, the
aerial part consists of a hypocotyl that had already reached its
maximum length of about 2 mm, two cotyledons, two fully expanded
leaves, and two immature leaves. Ions were separated from aqueous plant
extracts by capillary ion electrophoresis (Fig.
2A) as described in ``Materials and Methods''. Comparison of electrophoregrams of plant extracts and
solutions containing reference anions at different concentrations, we
identified six peaks corresponding to Cl
,
SO42
,
NO3
, citrate, malate, and
PO42
(Fig. 2A). The quantification of these
peaks (Fig. 2B) revealed a high concentration of
NO3
(close to 70 mM), a concentration for both
SO42
and
PO42
(around 22 mM), and a low
concentration for Cl
(3 mM). For
the identified organic anions, malate and citrate, the concentrations
were 14.4 and 9.7 mM, respectively.

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| Figure 2.
Quantitative analysis of the anion content in the
aerial parts of 11-d-old Arabidopsis plantlets. A, Capillary ion
electrophoregram of a water-soluble extract showing the six identified
peaks. B, Mean values ± SE of the anion
concentrations (n = 9).
|
|
To determine whether the voltage-dependent channel can allow effluxes
of anions other than Cl
, the 150 meq of
Cl
contained in the patch pipette was
substituted with 150 meq of NO3
,
SO42
,
malate2
,
HCO3
, or Glu provided as
K+ salts. The substitution of the cytosolic
rather than extracellular anions was favored as closer to the in vivo
conditions in which the different anions concentrated inside the cell
tend to flow out at physiological membrane potentials, and because it
also integrates putative internal regulatory effects of the anions. As
previously reported (Thomine et al., 1995
), the anion current intensity
slowly increased, reached a maximum 3 to 10 min after getting the
whole-cell configuration, and started to decrease after a few minutes
of steady state. All of the curves presented in the figures and used
for the determination of Erev and
maximum peak current amplitudes were recorded at the time of maximum
activation.
Comparison of the I-V curves in Figure 1 shows a similar voltage
dependence for the different channel-mediated anion currents. Some
differences appear in the threshold activation potential according to
the anion tested; this potential was the most negative for
SO42
and the least
negative for Cl
. Figure 1 reveals large
differences in the current amplitude at the peak potential and in the
position of the Erev depending on the
anion species loaded into the cytosol. The current recorded in the
whole-cell configuration reflects the activity of the entire channel
population. Two types of information can be deduced from this current.
The first one is the current density for each ion tested. The
macroscopic whole-cell current (I) is the product of the
number of functional channels in the cell membrane (N), by
the open probability of a channel at the peak potential
(Po), and the single-channel current
(i) (I = iNPo). Although the measurement of
whole-cell current density combines information about regulatory and
permeation properties of an anion toward the channel, it is most likely
a physiologically relevant parameter. The second one concerns the
selectivity of the channel that can be deduced from the
Erev. This potential is indicative of
the relative affinity of anions for the channel pore, but does not
presume the ion permeation through the channel (Hille, 1992
).
We compared the whole-cell current at the peak potential for the
different intracellular anions (Table I;
Fig. 1). The highest current amplitudes were reached when 92% of the
intracellular Cl
was replaced by
NO3
(Fig. 1B) or
SO42
(Fig. 1C).
Interestingly, small but reproducible currents representing about 25%
of the Cl
current were observed when 92% of
the intracellular Cl
was replaced by
HCO3
(Fig. 1D). Very low
currents with high variability were observed in the presence of malate
(Fig. 1E). For these small
HCO3
and malate currents
there was the question of their contamination by inward
Cl
currents corresponding to the 12.4 mM Cl
left in the pipette solution.
Figure 3 shows the peak current amplitudes measured when varying the Cl
concentration in the pipette (for a total pipette anion content adjusted in each case to 162.4 mM with the non-permeant
anion Glu), with Cl
in the bath kept constant
at 110 mM. The intensity of the Cl
current decreased linearly when Cl
was replaced
by Glu, extrapolating to zero for zero Cl
in
the pipette. This confirmed that Glu could effectively be considered a
non-permeant anion. The small current measured with 12.4 mM
Cl
(+150 mM non-permeant Glu) was
1.0 ± 0.2 pA/pF (n = 10), thus representing the
contribution of the residual 12.4 mM
Cl
present in all of the pipette
solutions. When corrected for this value, the
HCO3
current appeared
6-fold lower than the Cl
current. For malate,
the high variability of the small corrected current precluded any
precise quantitative comparison.
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|
Table I.
Peak current amplitudes and permeability ratios for
different anions
Peak current amplitudes and reversal potentials were measured in the
whole-cell configuration, with 150 meq L 1 of the anion to
be tested, 12.4 mM Cl in the pipette, and 110 mM Cl in the bath. The relative permeability
ratios were calculated from Equations 1 and 2 as described in
``Materials and Methods''. Mean values of peak current and
permeability ratios are expressed as ±SE for the number of
seals indicated within parentheses.
|
|

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| Figure 3.
Amplitude of the peak current as a function of the
internal Cl concentration. Internal Cl was
varied from 12.4 to 162.4 mM while maintaining the total
anion concentration in the pipette to 162.4 mM by adding
the non-permeant anion Glu. External Cl was kept at 110 mM. Peak current amplitudes were measured from 10-s voltage
ramps as described in ``Materials and Methods''. Each current
amplitude is the mean ± SE of five to 13 measurements. The line represents the linear regression of the data
(r2 = 0.93).
|
|
The channel selectivity for each anion was investigated by measuring
the Erev. The relative permeability
ratios for different anions over Cl
were
calculated from the Erev with
Equations 1 or 2 (see ``Materials and Methods'') derived from the
Goldman-Hodgkin-Katz current equation. The
Erev of the whole-cell current in the
presence of 162.4 mM Cl
in the pipette and 110 mM
Cl
in the bath (20.4 ± 5.6 mV,
n = 10) was similar to the calculated equilibrium
potential for Cl
(20.1 mV), indicating that the
voltage-dependent inward current is highly selective for anions. When
using a Cl
-free bath solution (CaOH neutralized
with MES), no outward current could be detected (n = 5). This shows that in our experimental conditions the outward current
is essentially carried by Cl
, excluding any
large error in Erev measurement due to
an outward K+ current. This was confirmed by
showing that the exchange of K+ by
Cs+ in the pipette solution did not influence significantly
the Erev (40.7 ± 8.5 mV,
n = 10 with 150 mM
CsNO3, and 41.2 ± 4 mV, n = 10 with 150 mM KNO3). The
permeability ratios for a range of physiological anions are reported in
Table I. The largest values were obtained for
NO3
(PNO3
/PCl
=2.6 ± 0.3) and
SO42
(PSO42
/PCl
=2.0 ± 0.2). The relative permeability of
HCO3
compared with
Cl
was slightly lower than 1, and malate
appeared almost non-permeant. Different ionic conditions were tested to
ascertain the relative permeabilities of
NO3
and
SO42
over
Cl
. For example, a
PNO3
/PCl
of 2.9 ± 0.4 (n = 3) was calculated when
NO3
was added in the bath
(100 mM
NO3
and 10 mM Cl
); the pipette
solution contained 150 mM Glu and 12.4 mM Cl
. This value is not
significantly different from that obtained in the ionic conditions
described in Table I. In summary, these results lead to the following
selectivity sequence:
Considering the above results, the most surprising finding was
that SO42
appears to be a
good substrate of the voltage-dependent anion channel. As this anion is
usually considered as non-permeant, we performed additional experiments
to demonstrate that the current recorded in our experimental conditions
of high external Ca2+ (50 mM
CaCl2) was not a voltage-dependent inward
Ca2+ current like the one described in carrot
cells and Arabidopsis (Thuleau et al., 1994
; Thion et al., 1998
). Using
SO42
as the intracellular
anion, we applied a voltage ramp every 30 s to monitor the current
as a function of time. After getting stable I-V curves for 5 min, we
substituted the extracellular solution (50 mM
CaCl2 and 5 mM
MgCl2) with a Ca2+-free
solution containing the same amount of Cl
and a
large-spectrum Ca2+-channel blocker,
La3+ (95 mM TEA-Cl and 5 mM LaCl3). Following
Ca2+ removal, the properties of the current
remained unchanged (n = 3; Fig.
4); neither the amplitude nor its
Erev was modified. This result rules
out the hypothesis that the inward current under investigation bears
any significant contribution of Ca2+ ions and
confirms that it is only carried by
SO42
. Furthermore,
the nucleotide regulation, a characteristic feature of the
Cl
current mediated by this channel (Thomine et
al., 1997a
), was also observed with
SO42
as the intracellular
anion (data not shown).

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| Figure 4.
Characteristics of the current-voltage
relationship in the presence or absence of extracellular
Ca2+. A 10-s voltage ramp between 180 mV to +30 mV was
applied every 30 s. The pipette solution contained: 5 mM ATP, 5 mM GTP, 75 mM
SO42 , and 12.4 mM
Cl . The I-V curve was recorded in the standard bath (50 mM CaCl2 and 5 mM
MgCl2) 10 min after breaking to the whole-cell
configuration when a stable current amplitude was reached (50 mM Ca2+), and after 5 min of perfusion with the
Ca2+-free bath (no Ca2+) (95 mM
TEA-Cl, 5 mM LaCl3). Results are shown for one
representative experiment out of three. In all cases, the current
amplitude was unchanged and the Erev was not
significantly modified.
|
|
Regulatory Effects of SO42
on the Anion
Current
We reported previously (Thomine et al., 1995
) that the amplitude
of the Cl
current changed after the
establishment of the whole-cell configuration: the amplitude of the
current first slowly increased, reached a maximum after 3 to 10 min,
and then started to decrease. In all cases, the current completely
disappeared within 10 to 30 min. A similar evolution of the current
amplitude with time was observed for
NO3
,
HCO3
, and malate. Figure
5 compares the changes of the peak
current when either NO3
or SO42
was used as the
internal anion. The NO3
current ran down and disappeared completely after 12 min of
intracellular perfusion. In contrast, the
SO42
current decreased
very slowly, with the maximal peak current being decreased by about
27% after 30 min. Overall, when a
SO42
-containing solution
was perfused through the patch pipette in the whole-cell configuration,
the peak current was only decreased by 12% ± 6% after 15 min
(n = 8) and by 19% ± 4% after 25 min (n = 4), whereas at this latter time the
voltage-dependent current was completely lost with all other anions
tested. Thus, SO42
is not
only a substrate for the voltage-dependent anion channel, it also
prevents its run-down. This suggests that
SO42
ions play a
regulatory role on channel activity.

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| Figure 5.
Time course of the NO3
and SO42 currents in the whole-cell
configuration. A 10-s voltage ramp between 180 mV to +80 mV was
applied every 30 s. The NO3 current
( ) and the SO42 current ( ) amplitudes
at the peak (I peak) are displayed as a function of time after the
establishment of the whole-cell configuration. The pipette solution
included either 150 mM NO3 or 75 mM SO42 , 12.4 mM
Cl , and 3 mM ATP, while the bath included 110 mM Cl . Results are from one representative
experiment out of eight for each condition.
|
|
Single-Channel Analysis of the SO42
Current
To analyze further the permeation of
SO42
ions through the
voltage-dependent anion channel of the hypocotyl, we recorded the single-channel activity in the outside-out configuration. Again, in
contrast with what happens with Cl
, in the
presence of intracellular
SO42
, the anion channel
activity did not undergo any run-down. While this allowed us to record
channel activity for over 1 h on the same patch, we could never
isolate any patch containing less than about five to 10 active
channels. This impaired the analysis of channel activity, allowing the
single-channel amplitude to be resolved only for potentials more
hyperpolarized than
100 mV, at which no more than three to four
channel openings overlapped.
Figure 6A illustrates the single-channel
activity of the anion channel in the outside-out configuration with an
internal solution containing 75 mM
SO42
and 1 mM
ATP. An increase in open probability when the membrane is depolarized
was observed (compare
181 mV and
141 mV), which correlated with the
voltage dependence of the current in the whole-cell configuration.
Niflumic acid, the most potent blocker of the whole-cell anion current
(Thomine et al., 1997b
), inhibited the single-channel activity (Fig.
6B). The amplitude of single-channel currents was analyzed in the
voltage range between
200 mV and
150 mV (n = 3). A
linear regression of the I-V plot of single-channel amplitudes yielded
a single-channel conductance of 14.6 ± 0.5 picoSiemens (pS) (Fig.
6C). When measured in otherwise identical conditions, the conductance
was found to be higher with internal Cl
(22.6 ± 2.3 pS) than with internal
SO42
(14.6 ± 0.5 pS) (Fig. 6C). Thus, the 5- to 6-fold increase in SO42
whole-cell current
compared with Cl
current could not be accounted
for by an increase in single-channel conductance.

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| Figure 6.
SO42 permeation through
single voltage-dependent anion channels. A, Single-channel currents
were recorded in the outside-out configuration with membrane potential
clamped in the range 131 mV to 181 mV (c, closed; o, open). The
pipette solution included 75 mM
SO42 , 12.4 mM Cl ,
and 1 mM ATP, while the bath contained 110 mM
Cl . B, Inhibition of single-channel current by 300 µM niflumic acid. Single-channel currents were recorded
in the outside-out configuration with membrane potential clamped at
151 mV. The control trace was obtained 10 s before adding the
channel blocker, while the trace in the presence of niflumic acid was
obtained about 10 s after adding the blocker. The pipette solution
included 75 mM SO42 , 12.4 mM Cl , and 3 mM ATP, while the
bath was 110 mM Cl . C, Single-channel I-V
curve for SO42 current ( ) gave a
conductance of 14.9 ± 0.5 pS (n = 3). For
comparison, channel I-V curve for Cl current ( ) gave a
conductance of 22.6 ± 2.3 pS (n = 3). The
pipette solution included either 150 mM Cl or
75 mM SO42 , 12.4 mM
Cl , and 1 mM ATP, while the bath was 110 mM Cl . D, I-V relationship of an outside-out
excised patch that exhibits both the activity of single channels in the
range 200 to 100 mV and a typical current rectification in the
range 70 to +20 mV, where single channels are not resolved. The
pipette solution included 75 mM
SO42 , 12.4 mM Cl ,
and 1 mM ATP, while the bath was 110 mM
Cl .
|
|
A linear extrapolation of the experimental I-V curve obtained with
SO42
crosses the voltage
axis for a value of
78 mV. This value is not in agreement with the
Erev value of +16 mV measured in the whole-cell configuration. This difference likely results from current
rectification around the Erev
occurring at the single-channel level as it occurred at the whole-cell
level. Evidence for single-channel current rectification is given by
I-V curves from outside-out excised patches containing 20 to 50 channels: they exhibit both the activity of single channels in the
range
200 to
100 mV and a typical current rectification in the
range
70 to +20 mV, even though single channels cannot be resolved in
this range (Fig. 6D).
 |
DISCUSSION |
Anion Channel Permeability
We investigated the anion selectivity and permeability of the
voltage-dependent anion channel of Arabidopsis hypocotyl cells, and
analyzed in parallel the anion content of Arabidopsis plantlets by
capillary electrophoresis. Such analysis gives only a mean global
concentration for each ion species and does not provide information on
the localization within plant tissues and cell compartments, but helped
us to identify putative substrates for the plasma membrane anion
channels.
We found that Arabidopsis anion channels are highly permeable to
NO3
. A large
NO3
permeability was also
found for the two types of anion channels of fava bean guard cells
(rapid type: NO3
[4.2] > Cl
[1]
malate2
[0.1], Hedrich and Marten, 1993
; slow type:
NO3
[20.9] > Cl
[1]
malate2
[0.24], Schmidt and Schroeder, 1994
), anion channels from wheat root
(Skerrett and Tyerman, 1994
), cotyledonary cells of amaranth (NO3
[2.4] > Cl
[1], Terry et al.,1991
), pea epidermal
cells (NO3
[1.34] > Cl
[1]
malate2
[0.002], Elzenga and Van Volkenburgh, 1994), and suspension-cultured coffee cells (Dieudonné et al., 1997
). High
NO3
permeability thus
seems to be a general feature of plant plasma membrane anion channels.
The finding that SO42
,
which is usually considered to be a weakly permeant or non-permeant ion
in anion channels, was indeed permeant in the Arabidopsis voltage-dependent anion channel is a striking and novel result from
this study. Although the
SO42
uptake transporter
of the plasma membrane has been extensively studied (Rennenberg et al.,
1989
; Clarkson et al., 1992
), we report here the first example (to our
knowledge) of large channel-mediated SO42
currents.
Phosphate permeability has not been investigated because
Ca2+ phosphate precipitation is a technical
limitation that we have not yet been able to overcome. Malate is only
weakly permeant through the Arabidopsis hypocotyl anion channel, as
already shown for the rapid and slow anion channels in guard cells
(Hedrich and Marten, 1993
; Schmidt and Schroeder, 1994
). Glu, with the highest Mr of the anions tested, is
not significantly permeant and can thus be safely used as a reference
nonpermeating anion. Our data showing small but reproducible
HCO3
currents open an
interesting new area of investigations.
HCO3
permeability of
plant anion channels has, to our knowledge, never been reported, and
even information concerning the permeability of animal channels to
HCO3
is scarce. However,
HCO3
permeability can be
quite significant, as exemplified by the anion channel of human
secreting epithelia, for which a
HCO3
permeability ratio
PHCO3
to
PCl
in the range of 0.50 to 0.64 has
been reported (Tabcharani et al., 1989
) and by the cystic fibrosis
transmembrane conductance regulator for which a
PHCO3
to
PCl
ratio of 0.14 to 0.25 has been
recently measured (Linsdell et al., 1997
). Several technical
difficulties, among which the small amplitude of the currents and the
run-down of the channel, limit the study of the
HCO3
currents mediated by
the voltage-dependent anion channel of Arabidopsis hypocotyls.
Nevertheless, the potential roles of channel-mediated HCO3
fluxes in pH
regulation and/or carbon metabolism call for such a study to be
undertaken.
The high NO3
and
SO42
whole-cell currents
mediated by the voltage-dependent anion channel of Arabidopsis
hypocotyls, combined with the high concentrations of
NO3
and
SO42
in plantlet tissues,
suggest that these two ions are in vivo substrates of the channel and
that the channel could play a role in the homeostasis of their cellular
concentrations.
SO42
Regulation of the Anion Channel
In addition to its unusual permeation, the second property of
SO42
is its regulatory
effect on the channel. As measured on excised outside-out patches, the
anion channel conductance was higher in the presence of internal
Cl
compared with
SO42
. This can be
reconciled with the results of whole-cell
Erev measurements. These
Erev values indicate that
SO42
has a higher
affinity for the channel pore than Cl
. As
SO42
is more tightly
bound inside the channel, it tends to reside longer in the channel
pore, which results in a lower rate of permeation (as revealed by lower
single-channel conductance). However, the high whole-cell current
density cannot be accounted for by a higher permeation rate, since the
single-channel conductance is actually lower. This indicates that
SO42
modifies other
parameters that determine the whole-cell current density: the open
probability (Po) or the number of active channels (N).
From the single-channel amplitude of the
SO42
current at the peak
potential (Fig. 6C) and the mean whole-cell current density at the same
potential (Fig. 1C), we estimated at least 4,000 to 6,000 active
channels for a cell 40 µm in diameter. A number of active channels
about 10-fold lower was estimated to account for whole-cell
Cl
currents. These estimations suggest that the
large amplitude of the whole-cell
SO42
currents compared
with the Cl
currents results not only from the
more hyperpolarized activation potential (see Fig. 1) but also from a
regulatory effect of SO42
on the number of active channels. Another effect of
SO42
was to prevent the
run-down of the anion current both in the whole-cell and in the
outside-out configuration. Thus,
SO42
is able to maintain
the channel in an active state. This effect was initially observed when
this anion was used as the major substrate for the anion channel, i.e.
with 75 mM internal
SO42
. No dose response of
the regulatory effect of
SO42
has been
constructed, but when the
SO42
solution was diluted
in the Cl
solution to one-half (75 mM Cl and 37.5 mM
SO42
), one-fourth (112.5 mM Cl and 18.8 mM
SO42
), and one-sixteenth
(131.3 mM Cl and 9.4 mM
SO42
), the run-down
remained slower than in the presence of Cl
only
(data not shown). The fact that
SO42
was also able to
prevent run-down in excised patches suggests either a direct action on
the channel or a membrane-delimited activation pathway. The mechanism
underlying the regulatory effect of
SO42
is still unknown,
but it appears to be quite different from other types of run-down
prevented by effectors of tubulin (Thion et al., 1996
, 1998
),
indicating the involvement of the cytoskeleton, or by effectors of
protein kinase or phosphatase (Wang et al., 1991
), indicating a
regulation via phosphorylation. The stabilizing effect of
SO42
suggests an original
mechanism that could involve a regulatory site where most anions except
SO42
bind and induce
run-down or where only
SO42
can bind to prevent
run-down. Understanding this mechanism will require further
investigation.
A Metabolic Link between NO3
and
SO42
Permeation and the Regulation of
the Channel by Nucleotides?
Considering together the high
NO3
and
SO42
whole-cell currents
mediated by the channel and the channel regulation by nucleotides raises the hypothesis that this channel could function as a metabolic valve to avoid the cytoplasmic accumulation of
NO3
and
SO42
ions when they
cannot be extensively metabolized.
SO42
assimilation
requires an ATP-sulfurylase whose activity is directly controlled by
the ATP status (Schmidt and Jäger, 1992
), while NO3
reduction and
incorporation into amino acids is a highly energy-consuming process
(Botrel and Kaiser, 1997
). The voltage-dependent anion channel could be
involved in the regulation of the cytosolic concentration of
NO3
and
SO42
, depending on the
variation of the energy balance of the cell. When the energy level of
the cell is high, which is reflected by an increased cytosolic ATP
concentration, the efflux channel is inhibited (Thomine et al., 1997a
),
NO3
and
SO42
are trapped in the
cytoplasm, where they can be reduced and incorporated into amino acids.
Alternatively, when the energy level of the cell is decreased, the ATP
and ADP concentrations are reduced and the channel is not inhibited,
allowing the efflux of these anions out of the cytoplasm, where no
energy for their metabolism is available.
In conclusion, the voltage-dependent anion channel of Arabidopsis
hypocotyl cells shares a high permeability to
NO3
with the previously
described plant anion channels. It exhibits a first original property
of being permeable to
SO42
with a unitary
conductance about two-thirds that of Cl
. The
second original property concerns the strong regulatory effect of
SO42
, increasing the
number of active channels per cell and responsible for the large
whole-cell SO42
currents
measured. These properties associated with high concentrations of
NO3
and
SO42
in Arabidopsis
plantlets highlight the likely participation of the voltage-dependent
channel in in vivo NO3
and SO42
fluxes through
the plasma membrane contributing to the homeostasis of their cellular
concentrations and metabolism.
 |
FOOTNOTES |
1
This research was supported by the Centre
National de la Recherche Scientifique (grant no. UPR0040).
2
Present address: Department of Biology,
University of California at San Diego, 9500 Gilman Drive, La Jolla, CA
92093-0116.
*
Corresponding author; e-mail frachisse{at}isv.cnrs-gif.fr; fax
33-169823768.
Received January 4, 1999;
accepted June 8, 1999.
 |
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