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Plant Physiol, January 2001, Vol. 125, pp. 292-305
A Patch-Clamp Study on the Physiology of Aluminum Toxicity and
Aluminum Tolerance in Maize. Identification and Characterization of
Al3+-Induced Anion Channels1
Miguel A.
Piñeros and
Leon V.
Kochian*
United States Plant, Soil, and Nutrition Laboratory, United States
Department of Agriculture, Agricultural Research Service, Cornell
University, Ithaca, New York 14853
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ABSTRACT |
The presence of Al3+ in the rhizosphere induces citrate
efflux from the root apex of the Al-tolerant maize (Zea
mays) hybrid South American 3, consequently chelating and
reducing the activity of toxic Al3+ at the root surface.
Because citrate is released from root apical cells as the deprotonated
anion, we used the patch-clamp technique in protoplasts isolated from
the terminal 5 mm of the root to study the plasma membrane ion
transporters that could be involved in Al-tolerance and Al-toxicity
responses. Acidification of the extracellular environment stimulated
inward K+ currents while inhibiting outward K+
currents. Addition of extracellular Al3+ inhibited the
remaining K+ outward currents, blocked the K+
inward current, and caused the activation of an inward Cl
current (anion efflux). Studies with excised membrane patches revealed
the existence of Al-dependent anion channels, which were highly
selective for anions over cations. Our success in activating this
channel with extracellular Al3+ in membrane patches excised
prior to any Al3+ exposure indicates that the machinery
required for Al3+ activation of this channel, and
consequently the whole root Al3+ response, is localized to
the root-cell plasma membrane. This Al3+-activated anion
channel may also be permeable to organic acids, thus mediating the
Al-tolerance response (i.e. Al-induced organic acid exudation) observed
in intact maize root apices.
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INTRODUCTION |
Al limits the agricultural
productivity on approximately 30% of the world's total land area, as
the rhizotoxic species Al3+ solubilizes into acid
soil solutions, accumulating to levels that inhibit root growth and
function. However, plants have evolved tolerance mechanisms enabling
them to grow in soil environments where the roots are exposed to
potentially high levels of Al (for review, see Kochian, 1995 ).
Identification of Al-induced organic acid release by the root apex of
Al-tolerant genotypes provided the first compelling evidence for the
existence of such a tolerance mechanism, where the exuded organic acids
chelate and reduce the activities of toxic Al3+
in the rhizosphere (Delhaize et al., 1993a , 1993b ). Al-induced exudation of several different organic acids has been described from
roots of a variety of Al-tolerant plant species: malate being released
in wheat (Triticum aestivum; Ryan et al., 1995b ; Pellet et
al., 1996 ), citrate in maize (Zea mays) and Cassia
tora (Pellet et al., 1995 ; Ma et al., 1997b ), and oxalate in
buckwheat and taro (Ma et al., 1997a ; Ma and Miyasaka, 1998 ; Zheng et
al., 1998 ). Given the neutral pH of the cytoplasm, organic acids in the
cytoplasm are largely deprotonated and exist as anions. Since the
equilibrium potential for organic acid anions (as well as inorganic
anions) is much more positive than that of the resting membrane
potential in root cells, activation (i.e. opening) of plasma membrane
anion channels will result in a large anion efflux down the outward electrochemical gradient. Thus, it is likely that anion channels (permeable to organic acids) will constitute the transport mechanism via which Al-induced organic acid exudation occurs. In support of this,
Ryan et al. (1997) reported an anion channel in protoplasts isolated
from root tips of Al-tolerant wheat, which was specifically activated
by extracellular Al3+. In addition to this
ligand-gated channel, several plasma membrane anion-permeable channels
have also been identified in other higher plant tissues. Voltage gated
anion channels have been reported in protoplasts derived from different
tissues such as root cortical (Skerrett and Tyerman, 1994 ; Tyerman et
al., 1997 ) and xylem parenchyma cells (Wegner and Raschke, 1994 ;
Köhler and Raschke, 2000 ), hypocotyl epidermal cells (Thomine et
al., 1995 ), guard cells (Schroeder and Hagiwara, 1989 ; Schroeder and
Keller, 1992 ), and suspension cells (Zimmermann et al., 1994 ; Amtmann
et al., 1997 ). Mechanically gated-anion permeable channels (e.g.
stretch activated) have also been reported in the plasma membrane of
guard cells (Cosgrove and Hedrich, 1991 ).
Anion channels are involved in a wide range of physiological responses
such as regulation of stomatal conductance, stabilization of membrane
potential, nutrient transport, and turgor adjustment (Tyerman, 1992 ;
Schroeder, 1995 ). Although these anion channels share many
similarities, there are also significant differences in their
biophysical properties. For example although most anion channels
catalyze anion efflux as they open upon membrane depolarization, anion
channels activating at hyperpolarized membrane potentials or mediating
anion influx have also been reported (Terry et al., 1991 ; Skerrett and
Tyerman, 1994 ). Also, a wide range of intracellular and extracellular
factors can modulate the activity of many of these channels. The ionic
environment surrounding the channel (e.g. intracellular and
extracellular Ca2+ activities, as well as the
extracellular concentration of other ions) has been shown to influence
the permeation of anions through some of these channels (Schroeder and
Hagiwara, 1989 ; Hedrich et al., 1990 ; Skerrett and Tyerman, 1994 ;
Schulz-Lessdorf et al., 1996 ; Tyerman et al., 1997 ; Köhler and
Raschke, 2000 ). Endogenous signals (e.g. auxins), as well as changes in
the channel's phosphorylation state may also be involved in the
modulation of channel activity (Hedrich et al., 1990 ; Zimmermann et
al., 1994 ; Schmidt et al., 1995 ; Schulz-Lessdorf et al., 1996 ; Thomine
et al., 1997 ).
These biophysical and regulatory differences point to the existence of
several types of anion channels with diverse physiological roles in
vivo. We have made use of the patch-clamp technique (Hamill et al.,
1981 ) to gain insight into the influence of extracellular Al3+ on some of the plasma membrane ion
transporters of root apical cells of the Al-tolerant maize hybrid South
American 3, as the root apex is considered to be critical in both
Al-toxicity and Al-tolerance responses in crop plants (Ryan et al.,
1993 ; Kochian, 1995 ).
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RESULTS |
Whole-Cell Conductances for Protoplasts from the Maize Root
Apex
The protoplasts isolated from the root apex (first 5 mm of the
root) of the Al-tolerant maize hybrid South American 3 were mainly a
mixture of meristematic, cortical, and stelar protoplasts that were
morphologically distinguishable. Visual examinations of the partially
digested tissue showed that neither root cap nor epidermal cells were
digested. According to the morphology described for maize root
protoplasts (Roberts and Tester, 1995 ), most cells selected for the
present study were likely to be cortex protoplasts with a diameter of
35 to 50 µm, containing large vacuoles and relatively little
cytoplasm. In contrast with the success we had in obtaining
high-resistance seals in protoplasts from the mature root region,
protoplasts isolated from the root tip proved to be more delicate,
allowing occasional (1 of every 8 attempts) formation of high
resistance seals (3 G in average). A total of 89 cells was examined
under experimental conditions where the cell's cytoplasmic solution
(i.e. the solution inside the patch pipette) and bath solution
contained physiologically relevant K+ activities
at different pH values. Under these conditions three main types of
currents co-existed in the plasma membrane of root tip protoplasts
(Fig. 1, A and B). At depolarizing
potentials the whole-cell conductance of most cells (74%) was
dominated by an instantaneous K+ outward current.
This current developed rapidly, reaching a steady magnitude within 100 ms with activation constants decreasing from 25 to 5 ms (in sealing
solution) as the holding potential became more positive (from 30-100
mV). Similar instantaneous K+ outward currents
have been reported for mature maize root cells (Roberts and Tester,
1995 ), as well as for root parenchyma (Wegner and De Boer, 1997 ),
cotyledonary tissue (Terry et al., 1992 ), and mesophyll (M.A.
Piñeros, L.V. Kochian, unpublished data) cells from other plant
species. A small fraction of the cells (23%) displayed a
time-dependent K+ inward rectifier at
hyperpolarizing holding potentials, whereas in a smaller fraction
(15%), a time-dependent K+ outward rectifier was
observed. The close relationship between the reversal potential
(Erev) and the electrochemical equilibrium for K+ (EK+)
in the different bathing solutions indicated that
K+ was the main ion carrying these currents
(Table I). The time-dependent K+ currents showed
whole-cell activation kinetics and K+ selectivity
similar to those characterized in protoplasts derived from mature root
tissues from maize (Roberts and Tester, 1995 ) and other species
(Schachtman et al., 1991 ; Findlay et al., 1994 ; Gassmann and Schroeder
1994 ; White and Lemtiri-Chlieh, 1995 ).

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Figure 1.
Example of the whole-cell K+
currents and their respective current-voltage (I/V) relationships,
measured across the plasma membrane of maize protoplasts isolated from
the first 5 mm of the root. The patch pipette contained
K+-based filling solution (see "Materials and
Methods" for the detailed explanation on voltage protocols). For
clarity, only currents in response to 20 mV steps are shown. A,
Instantaneous outward and time-dependent inward
K+ currents recorded from a cell with a diameter
of 35 µm and bathed in a solution containing 10 mM
K+ (pH 6). Right, I/V relationships from the
currents shown on the left in bath solutions containing 10 ( ) as
well as 1 ( ) and 30 mM ( ) K+
(pH 6). Similar results for K+ selectivity were
obtained in nine other cells. B, Time-dependent outward
K+ currents and their respective I/V relationship
(right) recorded in a cell with a diameter of 28 µm bathed in a
solution containing 1 mM K+ (pH 6).
C, Effect of extracellular pH on the instantaneous outward and
time-dependent inward K+ currents from a 36-µm
diameter cell bathed in a solution containing 10 mM
K+ at either pH 6 or 4. The I/V relationships for
the currents obtained at pH 4 ( ) and pH 6 ( ) are shown on the
right. The effect of pH on the currents was reversible upon
restoring the original pH in the bath medium. Similar observations were
recorded in four other cells.
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Table I.
Equilibrium potentials for ions in the pipette and
bath solutions used in most of the patch-clamp recordings of maize
hybrid South American 3 root tip protoplasts
The pipette solution contained either KCl (K-based) or TEA-Cl
(TEA-based). Equilibrium potentials were determined from the ionic
activities calculated using the GEOCHEM-PC speciation program. Values
are given in mV. The equilibrium potential for Mg2+ (not
shown) was set at very negative potentials (>> ) in all
cases.
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The fact that these currents co-existed (Fig. 1A) or occurred alone
(Fig. 1B) in different cells, plus the fact that in some cells there
was a lack of inward currents at membrane potentials negative of
EK+, suggests that
the three different K+ currents are mediated by
three different populations of channels. These three types of currents
were suppressed when the intracellular and/or extracellular media
contained tetraethylammonium (TEA; data not shown).
pH and Al3+ Effects on K+ Whole-Cell and
Single-Channel Conductances
Given the physical chemistry of Al (i.e.
Al3+ is the predominant and toxic Al species at
low pH values), we proceeded to dissect and characterize plasma
membrane transport under Al3+-toxic conditions.
We first evaluated the effect of imposing an extracellular acidic
environment on ion transport. Extracellular acidification had two major
effects on the predominant K+ currents (Fig. 1C).
First, it stimulated the inward time-dependent K+
current. The current recorded at pH 4 was between 2 and 4 times larger
than that recorded at pH 6 with the stimulation being larger as the
holding potential became more negative. In contrast, extracellular acidification caused a dramatic inhibition of the instantaneous outward
currents. The currents recorded at pH 4 were between 5 and 12 times
smaller than that recorded in pH 6 with the degree of inhibition being
larger at less positive holding potentials. The magnitude of the
current inhibition was larger as the pH of the extracellular medium was
progressively reduced from pH 7 to 4 in 1-pH-unit changes (data not
shown). The remaining outward current recorded at pH 4 was further
inhibited by perfusing the bath with a solution containing TEA, a
K+ channel blocker. The pH effects on the inward
and outward currents were observed in cells in which both types of
currents co-existed (as shown in the figure), and in cells in which
only one of the currents dominated the whole-cell conductance. In
contrast, the time-dependent K+ outward rectifier
seen in a small fraction of the cells was relatively insensitive to
changes in extracellular pH (data not shown).
These results established which currents were likely to dominate the
whole-cell conductance in an acidic extracellular environment. Consequently, we proceeded to evaluate the additional effect of extracellular Al3+ at low pH on root cell ion
transport processes. The activity of Al3+ added
to the bath solutions was similar to that previously found to
simultaneously trigger a large organic acid (citrate) release in the
maize genotype used in the present work and elicit the maximal
difference in Al tolerance (measured as inhibition of root growth)
between this and Al-sensitive maize genotypes (Pellet et al., 1995 ).
Addition of 50 µM Al (Al3+
activity = 12 µM) significantly inhibited
(80%-90% inhibition) the remaining instantaneous outward
K+ conductance (i.e. already inhibited by
the low extracellular pH) (Fig. 2).
Extracellular Al3+ also inhibited the
time-dependent K+ inward rectifier (Fig.
3). The inhibition was both
concentration and voltage-dependent with the magnitude of the
inhibition being larger as the holding potentials became more
negative. The sensitivity of the inward rectifier to
Al3+ was less than that observed for the
instantaneous outward current with the current being inhibited only
between 22% to 32% by 50 µM Al. Elevating extracellular
Al to concentrations as high as 400 µM only inhibited
this current by 46% (at a holding potential of 120 mV). In an effort
to further characterize these inhibitory effects, we also examined the
effect of extracellular Al3+ on single
K+ channel properties. In the absence of
Al3+, we could regularly (10 of 18 excised
patches) detect the single activity of one type of
K+ outward channel. This channel had a unitary
conductance of 15 ± 2 pS (in 10 mM
K+) in both pH-6 and -4 solutions. Addition of
extracellular Al3+ blocked the single-channel
K+ currents (Fig.
4). The blockade appeared to be fast with
the time transitions of the blocking and unblocking reactions being too
fast to be resolved at the cutoff frequency of the filtering used and
thus appearing as a time-averaged reduction in the single-channel current amplitude. The single-channel blockade by extracellular Al3+ was also concentration and voltage dependent
with the current inhibition being greater at more negative holding
potentials. This observation suggests a direct effect of the voltage on
the association/dissociation rates of Al3+
binding to a site within the channel. However, in contrast to the high
affinity blockade of the outward current in whole cells, 50 µM Al caused only a 7% reduction of the unitary
conductance at the single-channel level (with no significant change in
the reversal potential). Increasing Al3+
concentrations to as high as 330 µM resulted in further
inhibition of the single-channel unitary conductance, but only to
approximately a 28% reduction of the unitary conductance recorded in
the control.

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Figure 2.
Blockade of the instantaneous outward
K+ current by extracellular
Al3+. The pipette contained
K+-based solution. A, Currents recorded from a
32-µm-diameter cell bathed in 10 mM
K+ (pH 4; left) and subsequently perfused with
the same bath solution containing 50 µM
Al3+ (right). B, I/V relationship of the currents
shown in A recorded in bath solutions (pH 4) lacking ( ) and
containing ( ) Al3+; the I/V relationship
obtained in 10 mM K+ (pH 6) is shown
for reference ( ). Similar observations were recorded in a total of
six cells under identical ionic regimens.
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Figure 3.
Blockade of the whole-cell time-dependent inward
K+ currents by extracellular
Al3+. A, Currents were recorded in a
36-µm-diameter cell and bathed in 10 mM
K+ (pH 4), which was then perfused with the same
solution containing different levels of Al3+ as
described at the top of each set of traces. The pipette contained
K+-based solution. B, The I/V relationship (left)
for the currents shown in A recorded in solutions lacking ( ) or
containing 50 µM ( ) or 400 µM ( )
Al3+. Current inhibition (right) as a function of
extracellular Al3+. The percentage of current
inhibition was calculated from the ratio of the current magnitude in
the presence and absence of Al3+ at potentials of
118 ( ), 108 ( ), 98 ( ), and 88 ( ) mV. Data points
are from one representative experiment. Similar observations were
recorded in a total of four cells.
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Figure 4.
Effect of extracellular Al3+
on the amplitude of K+ single-channel currents.
A, Single-channel recordings from an outside-out patch with a
K+-based filling solution and bathed in 10 mM K+ (pH 4) solution ± Al3+. The traces shown were recorded at the
holding potential indicated in the left margin in the absence and
presence of 330 µM Al3+. The
horizontal dashed line represents the closed state. B, Single-channel
current inhibition as a function of extracellular
Al3+. Left, The percentage of current inhibition
was defined as the ratio of the recorded currents in the presence and
absence of varying Al3+ concentrations at test
potentials of +82 ( ), +62 ( ), and +22 ( ) mV. Right,
Single-channel unitary conductance inhibition as a function of
extracellular Al3+. The unitary conductance
values were calculated as described in "Materials and Methods"
(r2 values ranged between 0.988 and 0.998).
There were no significant differences in
Erev among treatments. Similar observations
were recorded in a total of four different patches.
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Al3+ Induces Whole-Cell and Single-Channel Anion
Currents in Protoplasts Isolated from the Root Apex
The above results indicated that K+
conductances could still be detected in whole-cell and isolated patches
at low extracellular pH and even in the presence of large extracellular
Al3+ activities. Thus, we proceeded to replace
the K+ in the intracellular and/or bath solutions
with TEA to suppress the background K+ currents
and facilitate dissection of other less predominant currents. A total
of 39 cells were examined under these experimental ionic conditions. We
occasionally (n = 5) recorded one type of single anion
channel activity in excised outside-out patches (Fig. 5). The kinetics of the channel were
distinct, displaying long opening and closing times, in the range of
seconds. The channel activity did not "rundown" over time, even
1 h after excising the patch. This channel had a small inward and
outward unitary conductance (approximately 2-4 pS) in 11 mM extracellular Cl and
consequently has been designated as SCAC (small conductance anion
channel). The unitary conductance of the outward current carried by
SCAC increased to 9.2 ± 0.5 pS when the
Cl activity was increased to 115 mM Cl . The I/V
relationship constructed from steady-state recordings as well as those
derived from slow voltage ramps established that the currents reversed
near and followed changes in equilibrium for Cl
(ECl ; Table I). This
indicated that among all ions present in the intracellular and bath
solutions, the current across the channel was carried by
Cl (Fig. 5, B and C). This channel was able to
mediate both anion efflux (inward currents) as well as anion influx
(outward current). Reconstruction of macroscopic inward currents from
this channel showed that at depolarizing membrane potentials (more
negative than ECl ) the
channel was able to sustain anion efflux, undergoing only a very slight
inactivation over time (Fig. 5D).

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Figure 5.
Single-channel recordings of SCAC from outside-out
patches in the absence of Al3+. The pipette
solution was TEA-based. All traces were taken from one representative
experiment. Recordings containing a single anion channel activity
similar to the one described above were obtained from five different
excised patches. The time and current scales for the individual and for
the summed recordings are given on the bottom right side of each set of
traces. See "Materials and Methods" for voltage protocols,
calculations, and data transformations. A, Example of single anion
channel activity at two different extracellular
Cl concentrations as indicated on the top of
each set of traces. Membrane potentials were stepped from 0 mV to the
voltage indicated in the left margin. Given the small conductance of
the channel, currents were filtered at 200 Hz. Note the different
current scales for each ionic condition. The horizontal dashed lines
represent the closed state. B, I/V relationship for single -channel recordings when the bath solution contained 11 ( ) or 151 ( ) mM extracellular
Cl . The right and left arrows indicate the
theoretical reversal potential for Cl when the
bath contained 11 or 115 mM Cl ,
respectively. In 11 mM Cl the
unitary conductances and Erev were 1.6 ± 0.1 pS and +33.9 mV (r2 = 0.943) for the
inward current and 4.2 ± 0.2 pS and +66 mV
(r2 = 0.971) for the outward current,
respectively. In 115 mM
Cl the unitary conductance of the outward
current was 9.2 ± 0.5 pS and the Erev
was +7.6 mV (r2 = 0.992). C, I/V
relationship derived from slow voltage ramps from an outside-out patch
with 11 mM Cl in the bath
solution The arrow indicates the theoretical reversal potential for
Cl . The unitary conductance of the inward
current was 2.5 pS. D, Reconstruction of macroscopic current (second
trace) from the single-channel activity (first trace) elicited by the
voltage protocol shown on top of the trace.
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Whole-cell recordings established that replacement of intracellular
and/or extracellular K+ by TEA greatly reduced
the whole-cell conductances. The lack of large inward anion currents in
isolated patches in the presence of TEA correlated with the detection
of small inward currents in whole-cell measurements where cells were
exposed to similar ionic conditions. With TEA-based solutions in the
pipette and 1 mM TEA (pH 4) in the bath, small currents
(presumably mediated by SCAC) dominated the whole-cell conductance and
reversed at 56 ± 3 mV (n = 12 cells), close to
ECl (Fig. 6). Under these ionic conditions,
addition of extracellular Al3+ caused an
immediate shift in Erev to more a positive
membrane potential (97 ± 4 mV; n = 10 cells),
with the magnitude of the shift averaging 41 ± 2 mV (Fig. 6).
This shift suggests Al3+-activation of an inward
current, which was verified by the observation that in 40% of the
cells examined, the shift in Erev was accompanied by the activation of a small (compared with the large
K+ conductances described above) inward current
(Fig. 6A). This whole-cell current was activated within minutes
following perfusion of the bath solutions with extracellular
Al3+. At negative holding potentials, this
Al3+-induced current activated instantaneously
and then partially deactivated with time. The remaining activated
current (measured at steady state) was 30% to 50% of the current
magnitude measured within 100 ms of imposition of the test potential.

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Figure 6.
Al3+-induced inward anion
current. The pipette solution for the two cells shown in these examples
was TEA-based and the recordings were obtained in 1 mM
TEA-Cl (pH 4) in the absence and presence of 50 µM
extracellular Al3+ (12 µM
activity), following a voltage protocol as described in "Materials
and Methods." The arrows indicate the theoretical reversal potential
for Cl . A, Whole-cell recordings obtained from
a 32-µm-diameter cell. The I/V relationship from these traces was
constructed by measuring the magnitude of the outward currents at the
end of the voltage pulse, whereas the current magnitude of the
instantaneous inward currents were measured 100 ms after imposition of
the test pulse. Similar whole-cell recordings were obtained in total of
12 cells. B, Single-channel events induced by Al3+ in recordings made in the
whole-cell configuration. The diameter of the cell was 41 µm.
Recordings were made before and immediately after the addition of
Al3+ to the extracellular medium. The
Erev, calculated from the I/V
relationship shown (reconstructed by measuring the current amplitude of
the individual single-channel events at each resting potential), was
+96 mV (r2 = 0.998). Similar activation of
single-channel events was obtained in a total of four cells.
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The Al3+-activated current reversed at holding
potentials near the theoretical reversal potential for
Cl , suggesting this inward current was being
selectively carried by Cl . The activation of
this current by extracellular Al3+ was
occasionally (25% of the total cells where activation was observed)
detected as an activation of individual single-channel events in the
whole-cell configuration (Fig. 6B). Take together, these observations
indicated a low density of this particular Al3+-activated channel. Single-channel events in
whole-cell configuration allowed a more accurate estimate of
Erev (+96 mV), confirming the close
relationship between the reversal potential of the current and the
theoretical reversal for Cl (see I/V
relationship in Fig. 6B). In addition, the unitary conductance of this
channel was significantly larger than that recorded for SCAC, and this
channel was active only in the presence of Al3+.
We have designated this Al3+-activated channel as
LCAC (large conductance anion channel). Under the electrical
conventions used in the present work, these Al3+-activated inward currents correspond to
Cl efflux. Similar
Al3+-activated currents were recorded in cells
where the pipette contained K+ based solutions,
providing that the K+ background currents prior
to Al3+ exposure were small enough to allow us to
resolve the small inward currents activated after
Al3+ exposure (data not shown).
Further characterization of the permeability and selectivity of LCAC
was performed in outside-out patches isolated from protoplasts that had
been exposed to Al3+ prior to patch excision.
LCAC was readily (7 of 16 patches) recorded in bath solutions
containing Al3+ (Fig.
7A). In contrast to SCAC, this second
type of channel was only recorded in patches exposed to
Al3+ and had different kinetics and unitary
conductance. LCAC exhibited a characteristic "noisy" open state,
and its unitary conductance was significantly larger than that of SCAC.
The unitary conductance of LCAC ranged from 18 to 27 pS, increasing as
the extracellular Cl concentration in the bath
increased (Fig. 7, B and C). The unitary conductance values were in the
range of those commonly reported for other plant anion channels
(approximately 10-40 pS; although unitary conductances as large as 150 pS have also been reported [Terry et al., 1991 ; Amtmann et al.,
1997 ]). Similar kinetics and unitary conductance values for this
Al3+ activated channel in excised patches were
observed when the pipette solution contained K+
and the bath solution contained KCl and extracellular
Al3+ (Fig. 7D). The I/V relationships derived
from slow voltage ramps indicated the single-channel current reversed
at holding potentials close to the electrochemical
ECl . Increasing the
Cl concentration in the bath solution caused a
negative shift in the Erev of the
single-channel current, closely following the change in
ECl (Fig. 7, B and C). These
observations indicated that for the ions present in the pipette
solution (in both K+ and TEA-based filling
solutions), the inward current was being selectively carried by
Cl . Thus, the data from isolated patches in
Figure 7 provided further support for the anion selectivity of the
Al3+-induced inward current that was previously
inferred from macroscopic and single-channel currents observed in
whole-cell preparations.

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Figure 7.
Ion selectivity of the LCAC activated by the
presence of Al3+. A, Examples of single-channel
recordings from outside-out patches. The pipette solution was TEA-based
and the bath solution contained 50 µM
AlCl3 in 10 mM TEA-Cl (pH 4.0).
Membrane potentials were stepped from 0 mV to the voltage indicated in
the top left margin of each trace. The horizontal dashed lines
represent the closed state. B to D, Current-voltage (I/V) relationships
derived from slow voltage ramps (see "Materials and Methods"). The
arrows indicate the Cl theoretical reversal
potential for each ionic condition. The pipette solution was TEA-based
and the bath solution contained 50 µM
AlCl3 in 1 mM TEA-Cl (pH 4.0) (B) or
10 mM TEA-Cl (pH 4.0) (C). The unitary conductances under
these conditions were 18 and 27 pS, respectively. Similar results were
obtained with other cells when the pipette solution was
K+-based and the bath solution contained 50 µM Al3+ in 10 mM KCl
(D). In this case, the unitary conductance was 25 pS. Similar channel
activity and selectivity was recorded in a total of seven different
patches in the different ionic environments containing extracellular
Al3+.
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Single-Channel Characterization of the Mechanism of
Al3+ Activation
Figure 8A shows a representative
example of a patch excised in the presence of extracellular
Al3+, where the activity of the two types of
anion channels described previously (LCAC and SCAC) were recorded. It
is worth highlighting that LCAC was only observed in excised patches
that were exposed to extracellular Al3+, whereas
SCAC (i.e. the SCAC described in Fig. 5) was observed in excised
patches in the presence and absence of extracellular Al3+. This observation suggests that the activity
of LCAC was dependent on the presence of extracellular
Al3+. Figure 8B shows a recording illustrating
the requirement of extracellular Al3+ to maintain
the activity LCAC. Single-channel activity was detected in a patch
excised from a cell that was exposed to extracellular Al3+. Under these conditions, the channel
remained active as evidenced by the frequent opening and closing events
over a time scale of minutes. Upon removal of
Al3+ from the bath, the channel inactivated and
remained in its closed state. This process was reversible (i.e. channel
re-activation) by re-introducing Al3+ to the bath
solution (data not shown). The specificity of the response was also
confirmed by the fact that exposure to equivalent extracellular
La3+ concentrations in the absence of
extracellular Al3+ did not restore channel
activity (data not shown).

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Figure 8.
Extracellular Al3+ is
required for maintaining activity of LCAC. A, Examples of
single-channel recordings from an outside-out patch containing the two
types (i.e. LCAC and SCAC) of anion channels. Membrane potentials were
stepped from 0 mV to the voltage indicated in the top left margin of
each trace. Downward deflections indicate channel opening. The solid
arrows indicate single-channel events for SCAC, the anion channel
observed with and without Al3+. The dashed arrows
indicate single-channel events for LCAC, the anion channel observed
only in solutions containing Al3+. The pipette
solution was TEA-based and the bath solution contained 50 µM Al3+ in 1 mM TEA-Cl
(pH 4.0). For clarity, the section of each trace indicated by the thick
horizontal line above it has been enlarged and presented in the bottom
two traces of Figure 8A. B, Continuous 8-min single-channel trace (each
trace containing 2 min of recording) from an outside-out excised patch
containing two channels of LCAC, recorded at a holding potential of
39 mV. The pipette solution was K+-based and
initially the bath solution contained 1 mM TEA-Cl (pH 4.0)
and 50 µM Al3+. The arrow on the
second trace indicates the time (2 min, 34 s) when the
recording chamber was perfused with an identical bath solution
lacking Al3+. Labels on the left of each trace
represent the closed (C) and open (O) states of the channel. The
current amplitude scale is shown at the right bottom of the Figure.
Similar results were obtained in another excised patch.
|
|
Having established the dependence on Al3+ for
activation of LCAC, the following experiments were conducted to isolate
and delimit the mechanism and pathways involved in the processes of
channel activation by Al3+. For such purposes we
attempted to trigger channel activation in excised patches (Fig.
9). We selected "electrically
quiet"(i.e. lacked any channel activity) outside-out patches excised
from protoplasts that had not previously been exposed to extracellular Al3+. Lack of channel activity was confirmed by
voltage protocols in which no channel activity was evoked in any of the
60 repetitions performed, as illustrated by the thin (i.e. quiet)
closed state (Fig. 9B). When the "quiet" patches were exposed to
extracellular Al3+, a channel mediating an inward
current (downward deflection) was activated (Fig. 9C). Channel activity
in the presence of Al3+ was sustained, as
indicated by a thick continuous open state, which was the product of
superimposing traces containing a large number of opening and closing
events over the 60 repetitions of the voltage protocol. Reconstruction
of macroscopic currents (Fig. 9D) for this particular channel shows
that at depolarizing membrane potentials the channel is able to
maintain sustained anion efflux, as it does not undergo inactivation,
at least over the time periods tested under this voltage protocol (1.4 s). Upon removal of Al3+ from the bath solution,
the channel once again inactivated (data not shown), in agreement with
previous observations (i.e. Fig. 8B). These results indicated that the
mechanism required for triggering channel activation is solely
localized to the plasma membrane (i.e. a membrane bound response). That
is, either the channel protein is directly activated when it binds
Al3+ or the Al receptor and signal transduction
pathways are localized to the plasma membrane in close proximity to the
Al3+-activated channel (LCAC).

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Figure 9.
Extracellular Al3+ activates
single channels in outside-out patches excised in the absence of
Al3+. The pipette contained
K+-based filling solution. Bath solutions
contained 1 mM TEA-Cl (pH 4.0) plus or minus 50 µM Al3+. Arrows and labels on the
right represent the closed (C) and open (O) states of the channel. The
time and current scales for B and C are shown at the bottom of C. The
current scale D is at the bottom; the time scale is the same as in B
and C. A, Two voltage protocols were used to test for single-channel
activity in solutions lacking and containing
Al3+. The voltage was stepped from a holding
potential of 2 mV to 62 (left column) or 122 mV (right column) and
held at this test potential for 1.4 s before returning to the
holding potential. B, Resulting trace of one single sweep (1 SW: one
sweep) from the voltage protocol described in A. The protocol described
in A was repeated consecutively 60 times with a 5-s resting phase
between repetitions. The panel labeled 60 SW shows the 60 repetitions
of individual sweeps superimposed. C, Same voltage protocol as in A
after 50 µM Al3+ was added to the
bath solution. As in B, 1 SW shows a trace for one of the 60 sweeps,
and 60 SW shows the traces of all 60 sweeps superimposed. D,
Reconstruction of macroscopic currents from the 60 single-channel
sweeps shown in C (see "Materials and Methods" for a detailed
description of reconstruction protocols). Similar results were obtained
in a total of three different excised patches.
|
|
 |
DISCUSSION |
In this study, the patch-clamp approach was used to further our
understanding of some of the ion transporters that are likely to be
involved in Al-tolerance mechanisms that take place in root tip cells
of Al-tolerant maize. Figure 10
summarizes the main observations recorded for some of these
transporters upon extracellular acidification and/or exposure to
extracellular Al3+.

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Figure 10.
Summary of the alterations induced in plasma
membrane ion transporters for root tip cells of Al-tolerant maize upon
extracellular acidification or exposure to extracellular
Al3+. The channel nomenclature is as follows:
LCAC corresponds to the Al3+-activated LCAC; SCAC
to the Al-independent SCAC; Kin to the
K+ inward rectifier; Kout1
to the time-dependent K+ outward rectifier; and
Kout2 to the K+
instantaneous outward rectifier channel, respectively. Channel
activation is indicated by an arrow of increased thickness, whereas
channel inhibition or blockade is indicated by crosses superimposed on
the arrows representing ion flux through a channel.
|
|
LCAC. An Al3+-Activated Anion Channel
In this study the functioning of an
Al3+-activated anion channel (designated as LCAC)
was described. This channel has some similarities to an
Al3+-activated channel reported from protoplasts
isolated from the root apex of Al-tolerant wheat (Ryan et al., 1997 ).
Our work extends and refines the understanding of Al-activation of this
anion channel by providing evidence for Al-dependent channel regulation
at the single-channel level. The Al dependence and Al activation of the channel in isolated patches represents a major breakthrough in our
understanding, as it indicates that the mechanism for channel activation is solely localized to the plasma membrane (i.e. a membrane-bound response). That is, either the channel protein is
directly activated when it binds Al3+, or the Al
receptor and signal transduction pathway are limited to the plasma
membrane and are co-localized with the channel. The lack of
inactivation of LCAC at the single-channel level (i.e. in excised
patches) suggests that the loss of cytoplasmic integrity (e.g. washout
of cytoplasmic factors by the pipette solution) does not disrupt the
mechanism(s) necessary to maintain this channel in the active state.
Although our findings reported here establish that this channel can
catalyze a Cl -selective efflux, permeability
and selectivity sequences derived from other studies have established
that plant cell anion channels are permeable to a variety of inorganic
and organic anions (Hedrich et al., 1990 ; Terry et al., 1991 ; Iwasaki
et al., 1992 ; Pantoja et al., 1992 ; Tyerman, 1992 ; Schmidt and
Schroeder, 1994 ; Schroeder, 1995 ; Dietrich and Hedrich, 1998 ; Frachisse
et al., 1999 ). In addition, the unitary conductance of LCAC in maize is
also dependent on extracellular anion activities, an intrinsic channel
property that has been proposed to enable the cell to sustain anion
efflux, despite the reduction of the electrochemical gradient across
the membrane as the extracellular anion concentration increases
(Hedrich and Marten, 1993 ). Given these generalized selectivity and
permeation properties, and taking into consideration the biophysical
properties exhibited by LCAC, it is likely that LCAC mediates the
Al-induced organic acid release observed in whole root studies (Pellet
et al., 1995 ).
SCAC
This second type of anion channel, which was readily observed in
excised patches bathed in solutions designed to minimize K+ conductances (i.e. pipette and bath solutions
containing TEA and lacking extracellular Al3+),
mediates both a selective influx and efflux of anions. Single-channel kinetics, as well as reconstructed macroscopic currents from
single-channel recordings, indicated this channel was able to maintain
a sustained anion efflux at potentials negative of
ECl and exhibited a very slow
inactivation with time. These kinetics resemble those described for the
slowly activating anion conductance in root parenchyma cells (Wegner
and Raschke, 1994 ; Köhler and Raschke, 2000 ) and the S-type
channel in guard cells (Schroeder and Keller, 1992 ). Also, we found
that SCAC also mediated a large outward current at very positive
potentials (at low extracellular Cl
concentrations), or at moderate positive membrane potentials under high
extracellular Cl concentrations, resembling the
anion outward rectifier in other plant cells (Terry et al., 1991 ;
Skerrett and Tyerman, 1994 ; Köhler and Raschke, 2000 ). The
existence SCAC and other additional types of plasma membrane anion
channels may account for the low levels of
Al3+-independent organic acid release described
previously in whole root studies.
Whole-Cell Anion Currents
Both maize (M.A. Piñeros and L.V. Kochian,
unpublished data) and wheat (Ryan et al., 1995a ) show very rapid
(appearing to occur almost instantaneously after Al exposure)
Al-induced root organic acid exudation, which is localized to the root
apex. However, whereas malate is the only organic acid released in
wheat, citrate is the primary organic released from maize roots. The
differences between the Al3+-induced anion
currents in maize and wheat root apical protoplasts (e.g. the current
density and current kinetics) are likely to reflect differences
observed at the whole root level (Delhaize et al., 1993a , 1993b ; Ryan
et al., 1995a ; Pellet et al., 1995 , 1996 ). In maize, this current
exhibits characteristics previously described for the quick activated
anion conductance and the S-type anion channels described in root
parenchyma and in guard cells (Schroeder and Hagiwara, 1989 ; Hedrich et
al., 1990 ; Schroeder and Keller, 1992 ; Köhler and Raschke, 2000 ).
It is worth noting that the whole-cell anion currents recorded in maize
in the presence of Al3+ are the sum of the
activity of LCAC as well as SCAC channels. However, reconstructed
macroscopic currents from SCAC and LCAC recordings indicate that these
channels were able to mediate a sustained anion flux (i.e. showed no
inactivation), in contrast to the partial inactivation of the
Al3+-induced inward currents observed in
whole-cell preparations. Although the exact mechanisms and factors
determining the partial inactivation recorded in the whole-cell
configuration remain unknown, these differences suggest
some likely scenarios. A complex cascade of events regulating this
channel might be involved, such that in addition to the requirement of
extracellular Al3+ for channel activation, other
intracellular and extracellular factors may modulate the activity of
this channel in the whole-cell mode. The activity of other voltage
gated plant anion channels have been shown to be modulated by a wide
range of signals such as changes in intracellular and/or extracellular
Ca2+ and anion activities as well as protein
phosphorylation or allosteric regulation by nucleotides
(Schroeder and Hagiwara, 1989 ; Hedrich et al., 1990 ; Skerrett and
Tyerman, 1994 ; Zimmermann et al., 1994 ; Schmidt et al., 1995 ; Thomine
et al., 1995 , 1997 ; Schulz-Lessdorf et al., 1996 ; Tyerman et al., 1997 ;
Frachisse et al., 1999 ). Although similar processes could
underlie the difference between the macroscopic currents and the
single-channel recordings reported here, contributions by other type(s)
of anion channel(s) activated by Al3+ cannot be
ruled out.
pH and Al3+ Effects on K+ Channels
Under physiological conditions (K+ in the
bath and pipette), instantaneous K+ outward
currents dominated the whole-cell conductance in root tip cells in
maize, although occasionally a time-dependent K+
inward rectifier and/or a time-dependent K+
outward rectifier were also recorded. As work on Al tolerance requires
that the studies be conducted at acidic extracellular pH, it was
interesting to note that extracellular acidification stimulated the
time-dependent K+ inward rectifier. It was
presumed that the mechanisms underlying the stimulation of this current
in maize root cells are similar to that recently reported for inward
K+ channels in root cells (Amtmann et al., 1999 ).
In contrast, although the whole-cell instantaneous
K+ outward current in maize root tip cells was
gradually inhibited as the pH of the extracellular medium was
decreased, the unitary conductance of single channels mediating the
K+ outward currents remained unchanged at
different extracellular pH values. It was presumed that pH regulation
of this current is due to a changes in the local electrical field
sensed by the gating structures of the channel, similar to that
proposed for the time-dependent K+ outward
current from guard cells (Ilan et al., 1994 ).
The addition of Al3+ had different effects on the
inward and outward K+ currents. Although high
affinity blockade (one-half maximal inhibitions occurring at
Al3+ activities of approximately 10 µM) by extracellular Al3+ has been
previously reported for K+ inward currents
(Gassmann and Schroeder, 1994 ; Ryan et al., 1997 ) and
Ca2+ inward currents (Piñeros and Tester,
1995 , 1997 ) from wheat root cells, the K+ inward
current observed in the present study showed little or no inhibition at
similar extracellular Al3+ activities (12 µM Al3+ activity; total Al
concentration of 50 µM). This current was moderately
inhibited in a voltage-dependent manner as the extracellular Al
concentration increased to 400 µM (128 µM
Al3+ activity). In contrast, exposure to 12 µM Al3+ activity almost completely
inhibited the instantaneous K+ outward current.
Although the single-channel recordings for the K+
outward current indicated that the binding of
Al3+ within the channel pore disrupts the
movement of the main permeant ion (K+) along the
conduction pathway, discrepancies in Al3+
sensitivity between the whole-cell and single-channel recordings indicate an additional effect of Al3+ on the
activation and inactivation processes governing the whole-cell currents
in maize.
Although the present study suggests that the
Al3+-activated anion channel is the underlying
mechanism for the Al-triggered organic acid release in intact roots,
the basis of the difference in this physiological response between
Al-tolerant and -sensitive maize varieties remains unknown. If indeed
this Al3+-activated channel is the basis for Al
tolerance, we currently can only speculate about the possible scenarios
accounting for the differences observed in the whole root studies. For
example, the Al3+-activated channel may exist
only in cells from the root apex of the tolerant varieties, or
alternatively it may be present in both varieties but at different
densities. Comparative studies between cells from the mature and the
root tip regions isolated from both Al-tolerant and Al-sensitive
varieties are planned for the future and will help establish the role
of this particular transporter in conferring Al tolerance in maize.
 |
MATERIALS AND METHODS |
Plant Material and Protoplast Isolation
Seeds of maize (Zea mays hybrid South
American 3) were surface sterilized in 0.5% (v/v) NaOCl
for 15 min and then germinated in the dark for 2 d on filter paper
saturated with deionized water. Germinated seeds were transferred to
polyethylene cups with mesh bottoms, covered with black polyethylene
beads, and then placed into the precut holes of the cover of a black
polyethylene container that held 2.4 L of aerated 0.2 mM
CaCl2 solution. Seeds were grown for an additional 3 d
(14-h-light/10-h-dark cycle at 22°C) before being used for
protoplast isolation. Protoplasts were isolated from root tips using
conventional enzymatic digestion and Suc gradient protocols. The first
5 mm of the primary root were finely chopped in 10 mL of a solution
consisting of 500 mM sorbitol, 1 mM
CaCl2, 5 mM MES
[2-(N-morpholino)ethanesulfonic acid]-KOH, pH 6.0, 0.5% (w/v) polyvinyl pyrrolidine (10,000 Mr), 0.5% (w/v) bovine serum albumin, 0.8%
(w/v) cellulysin (Calbiochem-Novabiochem, La Jolla, CA), and 0.08%
(w/v) pectolyase (Sigma, St. Louis). Following the incubation time (4 h
at 30°C in a rotatory shaker), released protoplasts were purified
using Suc step gradients as described by Schachtman et al.
(1991) .
Recording Solutions
All solutions were filtered (0.22-µm pore, Millipore, Bedford,
MA) before use. Two types of intracellular solutions were used to fill
the patch pipettes. These solutions contained 2 mM
MgCl2, 10 mM HEPES
(N-2-hydroxyethylpiperazine-N'-2-ethanesulphonic
acid)-Tris, pH 7.2, 4 mM Na2ATP, 2 mM EGTA, and 100 mM either KCl
(K+-based filling solution) or tetraethylammonium chloride
(TEA-based filling solution). The free Ca2+ concentration
in these solutions, as estimated by GEOCHEM, was 50 nM.
Pipette filling solutions were adjusted to 720 mosmol
kg 1 using sorbitol. The extracellular sealing solution
contained 10 mM KCl, 10 mM CaCl2,
and 10 mM MES-TRIS, pH 6.0. Bath solutions used for
recordings contained 0.5 mM CaCl2 and either
KCl or TEA-Cl at the concentration indicated for each particular
experiment. The pH of these solutions was adjusted to 6 with 10 mM MES-TRIS or to 4 with 10 mM HCl. All bath
recording solutions were adjusted to 700 mosmol
kg 1 using sorbitol. Al3+ was added from a
stock solution of 10 mM AlCl3 made up in 10 mM HCl.
Electrophysiology
Patch-Clamp Technique
Whole-cell and single-channel currents from protoplasts were
recorded at room temperature (22°C) with an Axopatch 200A amplifier (Axon Instruments, Foster City, CA), using conventional patch-clamp techniques (Hamill et al., 1981 ). A single junction reference electrode
(model MI-401F; Microelectrodes, Londonderry, NH) was connected to the
reference input of the head stage. Electrodes were pulled from
borosilicate glass capillaries (1.5-mm diameter without filament,
catalog no. PG 52150-4, World Precision Instruments, Sarasota, FL)
using a two-stage model P-87 Flaming-Brown horizontal electrode puller
(Sutter Instrument, Novato, CA). Electrodes were coated with Sylgard
(Dow Corning) and were fire polished using a CPM-2 microforge
(Scientific Instruments, Westbury, NY). Electrodes for
whole-cell recordings had a resistance of 5 to 8 M (in sealing solution and with KCl pipette filling solution). Electrodes used for
excised patch recordings had a resistance of 8 to 12 M . The small
chamber volume (less than 0.5 mL) allowed for rapid solution exchange.
After giga-ohm seals were formed, gentle suction was applied to the
interior of the pipette to obtain the whole-cell configuration. The
cell cytoplasm and pipette solutions were allowed to exchange for 10 min prior to data recording. Cell integrity was monitored using a video
camera (AVC-D7, Sony, Tokyo) attached to the microscope. Current
recordings were performed in the absence of microscope illumination.
Whole-cell series resistance and capacitance were partially compensated
for by the amplifier. Liquid junction potentials were corrected as
described by Neher (1992) . The access resistance was usually less than
10 M . Whole-cell and single-channel data were generally low-pass
filtered at 1 kHz using the low-pass Bessel filter of the
amplifier and digitized at 10 kHz, unless otherwise specified in
the figure legends. Unfiltered single-channel data simultaneously were
recorded and stored on videotape using a digital data recorder (VR-10B,
Instrutech, Elmont, NY). Ionic activities were calculated using
CHEOCHEM-PC (Parker et al., 1995 ). The Nernst potentials for ions
in the pipette and bath solutions are summarized in Table
I.
Whole-Cell Voltage Protocols
Voltage protocols, current recordings, data storage, as well as
data analysis were done with the software package PClamp 7 (Axon
Instruments) and a Pentium II personal computer. In experiments where
the pipette contained K+ based solutions (see above) the
voltage was clamped at a potential equal to the calculated
EK+ value (Table I), and a
sequence of step voltage pulses was applied with voltages ranging from
158 to +162 mV (in 10- or 20-mV increments). In experiments where the
pipette contained TEA+-based solution, the holding
potential was set to 0 mV and voltage pulses stepped between 102 to
+198 mV (in 20-mV increments). In either case, there was a 3-s resting
phase at the holding potential between each voltage pulse. Current
magnitudes were calculated after subtraction of the linear "leak"
current as described by Roberts and Tester (1995) . The current-voltage
(I/V) relationships were constructed by measuring the current amplitude
at the end of the test pulses (i.e. steady state).
Single-Channel Voltage Protocols
Single-channel current amplitudes for constructing I/V
relationships were determined from Gaussian fittings of
current-frequency distributions, using the Simplex and
Levenberg-Marquardt least-squares methods. Unitary conductances and
observed reversal potential (Erev) were
calculated from the linear regression of the linear portion of the I/V
relationship (r2 values are given in
parenthesis). In experiments where the pipette contained
TEA+-based solution, I/V relationships were also derived
from slow voltage ramps with outside-out patches. Slow voltage ramps
(1.0-1.4 s each) were applied between 122 and +118 mV from a holding
potential of 0 mV. Between each voltage ramp there was a 10-s resting
phase at the holding potential. The I/V relationships were
reconstructed by subtracting averaged ramps where no channel activity
was observed from individual ramps where channel events were detected.
The I/V relationships shown in each case contain at least 8 to 12 individual superimposed ramps showing the open and close states of the
channel. The unitary conductance of the single channel from I/V
relationships derived from ramp protocols was estimated from the slope
of the linear portion of the open state of the channel. Reconstruction
of macroscopic currents from single-channel recordings was done as
follows: single-channel activity was elicited by stepping the membrane
potential from 0 mV to a given test potential. This protocol was
repeated 50 times, allowing a 5-s resting phase between repetitions.
Capacitative currents were removed by subtracting a sweep were no
channel activity was detected from each individual sweep-exhibiting
channel activity. The reconstructed macroscopic current subsequently
was obtained by summing the resulting 50 to 60 recordings.
 |
FOOTNOTES |
Received May 19, 2000; modified July 18, 2000; accepted August 21, 2000.
1
This work was supported by the U.S. Department
of Agriculture National Research Initiative (grant no. 96-35100-3213
to L.V.K.).
*
Corresponding author; e-mail lvk1{at}cornell.edu; fax
607-255-2459.
 |
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