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Plant Physiol. (1999) 119: 277-288
A Steep Dependence of Inward-Rectifying Potassium Channels on
Cytosolic Free Calcium Concentration Increase Evoked by
Hyperpolarization in Guard Cells1
Alexander Grabov and
Michael R. Blatt*
Laboratory of Plant Physiology and Biophysics, University of
London, Wye College, Wye, Kent TN25 5AH, United Kingdom
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ABSTRACT |
Inactivation of inward-rectifying
K+ channels (IK,in) by a rise in
cytosolic free [Ca2+] ([Ca2+]i)
is a key event leading to solute loss from guard cells and stomatal
closure. However, [Ca2+]i action on
IK,in has never been quantified, nor are its
origins well understood. We used membrane voltage to manipulate
[Ca2+]i (A. Grabov and M.R. Blatt [1998]
Proc Natl Acad Sci USA 95: 4778-4783) while recording
IK,in under a voltage clamp and
[Ca2+]i by Fura-2 fluorescence
ratiophotometry. IK,in inactivation correlated positively with [Ca2+]i and
indicated a Ki of 329 ± 31 nM with cooperative binding of four Ca2+ ions
per channel. IK,in was promoted by the
Ca2+ channel antagonists Gd3+ and calcicludine,
both of which suppressed the [Ca2+]i rise,
but the [Ca2+]i rise was unaffected by the
K+ channel blocker Cs+. We also found that
ryanodine, an antagonist of intracellular Ca2+ channels
that mediate Ca2+-induced Ca2+ release, blocked
the [Ca2+]i rise, and Mn2+
quenching of Fura-2 fluorescence showed that membrane hyperpolarization triggered divalent release from intracellular stores. These and additional results point to a high signal gain in
[Ca2+]i control of
IK,in and to roles for discrete
Ca2+ flux pathways in feedback control of the
K+ channels by membrane voltage.
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INTRODUCTION |
Ca2+ underlies many fundamental regulatory processes
in plants, including adaptive responses to abiotic environmental stress (Knight et al., 1996 ; Russell et al., 1996 ; McAinsh et al., 1997 ) and
programmed cell death evoked by pathogen attack (Low and Merida, 1996 ;
Hammondkosack and Jones, 1997 ). Coordination of changes in
[Ca2+]i and its
integration with downstream response elements are central in coupling
stimulus input to cellular response in these processes.
In stomatal guard cells, the best characterized higher-plant cell
model, major downstream targets of
[Ca2+]i and their roles
in stomatal function have been identified. Increasing
[Ca2+]i is known to
inactivate IK,in and to activate
Cl channels, events that bias plasma membrane
transport for net efflux of osmotically active solute and a loss of
turgor, which drives stomatal closure (Blatt and Grabov, 1997 ).
Furthermore, changes in
[Ca2+]i are associated
with ABA, CO2, and the growth hormone auxin (Blatt and Grabov, 1997 ; McAinsh et al., 1997 ). These
[Ca2+]i signals have been
observed to oscillate (McAinsh et al., 1995 ; Webb et al., 1996 ),
characteristics that may constitute "Ca2+
signatures" to encode specific downstream responses (Berridge, 1996 ).
Yet, despite the evidence for
[Ca2+]i signaling in
guard cells, surprisingly little detail is known about the link between
[Ca2+]i changes and ion
channel activity at the plasma membrane or about the mechanisms
mediating such [Ca2+]i
changes. To our knowledge, in no instance have the characteristics of
ion channel regulation by Ca2+ been quantified
directly in any higher-plant cell.
We recently described the coupling of membrane voltage to
[Ca2+]i, demonstrating
that hyperpolarization, whether under a voltage clamp or in the
presence of low [K+]o,
evoked [Ca2+]i increases
in guard cells, and that the voltage threshold for [Ca2+]i rise was
profoundly altered by ABA (Grabov and Blatt, 1998 ). Our observations
indicated a link to Ca2+ influx across the plasma
membrane and raised questions about the efficacy of
[Ca2+]i in inactivating
IK,in and about the contributions of
intracellular Ca2+ release to the
[Ca2+]i signal. We have
used membrane voltage to experimentally manipulate [Ca2+]i and report that
IK,in is strongly dependent on
[Ca2+]i, consistent with
a cooperative binding of four Ca2+ ions to effect
inactivation. Additional experiments indicate that voltage-evoked
[Ca2+]i increases depend
both on Ca2+ influx and on release of
Ca2+ from intracellular stores. These results
underscore the role of
[Ca2+]i as a high-gain
"switch" in the control of IK,in, and
implicate [Ca2+]i in
feedback control linking membrane voltage to the activity of the
K+ channels.
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MATERIALS AND METHODS |
Plant Material
Broad bean (Vicia faba L. cv Bunyan, Bunyard
Exhibition) plants were grown and epidermal strips prepared as
described previously (Blatt and Armstrong, 1993 ). All operations were
carried out on a Zeiss Axiovert microscope fitted with Nomarski
differential interference contrast optics with strips bathed in rapidly
flowing solutions (10 mL/min [approximately 20 chamber volumes/min])
at 20°C to 22°C. The standard medium was prepared with 5 mM Mes titrated to its pKa
(= 6.1) with Ca(OH)2 (final
[Ca2+] approximately 1 mM). KCl and other compounds were included as required. Buffers and salts were from Sigma. All agonists/antagonists were from Calbiochem. In some experiments, Mes buffer was titrated with
KOH, and CaCl2 or MnCl2
were added separately as required.
Electrophysiology and Photometry
Electrical recordings and iontophoretic injections were achieved
with three-barreled microelectrodes coated with paraffin to reduce
electrode capacitance and, unless noted, microelectrode barrels were
filled with 200 mM potassium acetate to minimize salt
leakage and salt-loading artifacts associated with the
Cl anion (Blatt and Armstrong, 1993 ).
Connection to the amplifier headstage was via a 1 M
KCl/Ag-AgCl half-cell, and a matching half-cell and 1 M
KCl-agar bridge served as the reference (bath) electrode. Membrane
currents were measured by voltage clamp under microprocessor control
(µLAB/µLAN, WyeScience, Wye, UK) using three-pulse protocols
(sampling frequency, 2 kHz) and bipolar staircase duty cycles (Blatt
and Armstrong, 1993 ). Voltage and current were also sampled at low
frequency (64 Hz) concurrently with measurements of
[Ca2+]i.
[Ca2+]i was determined by
ratio fluorescence with a microphotometer (Cairn, Faversham, UK) using
the dye Fura-2 (Molecular Probes, Eugene, OR) excited at 340, 360, and
390 nm (10-nm half-bandwidth filter, Schott, Yonkers, NY). Fluorescence
was recorded through a slit diaphragm after filtering with a 480-nm
long-pass filter (Schott) and excluded microelectrode fluorescence. Dye
loading was by iontophoresis (Blatt and Armstrong, 1993 ) and was judged successful by visual checks for cytoplasmic dye distribution and by
stabilization of the fluorescence ratio signal. Measurements were
calibrated (Grabov and Blatt, 1997 ), and experiments were generally
carried out within the first 20 to 30 min after Fura-2 loading to avoid
difficulties associated with bleaching and decay of the fluorescence
signals.
Numerical Analysis
Data analysis was carried out by nonlinear, least-squares fitting
(Marquardt, 1963 ) and, where appropriate, results are reported as the
means ± SE of (n) observations.
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RESULTS |
K+ Channel Inactivation Is a Consequence of
[Ca2+]i Elevation
Although current through IK,in was
previously reported not to inactivate with time, past studies were
generally limited by voltage-clamp steps to periods of 2 to 4 s
(Blatt and Grabov, 1997 ; Thiel and Wolf, 1997 ) or, over longer times,
were carried out with
[Ca2+]i buffers present
at the cytosolic face of the membrane after exchange with patch-pipette
solutions (Schroeder, 1988 ). By contrast, concurrent measurements of
[Ca2+]i and
K+ channel current in vivo showed a pronounced
inactivation of IK,in evident only after
the first 2 to 4 s of 20-s voltage steps to 200 mV and suggested
a close link to moderate increases in
[Ca2+]i (Grabov and
Blatt, 1998 ).
To relate IK,in inactivation to the voltage
threshold initiating a
[Ca2+]i rise, guard cells
loaded with Fura-2 were driven through slow, 2-min voltage ramps from
+20 to 200 mV. f340,
f360, and f390 light, as well as the
f340/f390 ratio
as a measure of [Ca2+]i,
were recorded concurrently with a membrane current under voltage clamp.
Figure 1 shows the voltage, current, and
fluorescence ratios recorded from one guard cell, with the time course
of the [Ca2+]i rise in
Figure 1B calculated from
f340/f390 and
the individual fluorescence signals shown in Figure 1D. The
[Ca2+]i signal increased
appreciably, but only once the voltage was driven more negative than at
about 120 mV (Grabov and Blatt, 1998 ). Note that no change was seen
in the f360 trace with the voltage clamp in
contrast to f340 and
f390, indicating that the changes in
fluorescence were a consequence of changes in
[Ca2+]i rather than an
effect of voltage on dye leakage or redistribution. Under similar
voltage-clamp conditions (n = 55 cells), membrane hyperpolarization to 200 mV was accompanied by increases in
[Ca2+]i from a mean
resting value of 202 ± 23 nM to values
often in excess of 1 µM (Fig.
2C; mean ± SE, 703 ± 98 nM), and
depolarizations were followed by recovery of
[Ca2+]i to the initial
resting values.

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| Figure 1.
Voltage ramps demonstrate a voltage threshold for
increases in [Ca2+]i and consequent
inactivation of current carried by IK,in.
Concurrent records of voltage (A), [Ca2+]i
(B), and clamp current (C) are shown, along with the raw Fura-2
fluorescence recorded on f340,
f360, and f390
(D). Data are from one guard cell bathed in 5 mM
Ca2+-Mes, pH 6.1, with 10 mM KCl. Slowly
ramping membrane voltage from +20 to 200 mV under voltage clamp was
accompanied by an appreciable rise in [Ca2+]i
at voltages negative of about 120 mV. The outward (positive) current
at the start of the voltage ramp is associated with
IK,out (Blatt and Grabov, 1997 ). Activation
of inward (negative) current at voltages negative of 120 mV, carried
predominantly by IK,in (Blatt and Grabov,
1997 ), was followed by a near-complete decay in current amplitude
during the final 10 s of the ramp and coincident with the
[Ca2+]i rise near and above 400 nM. Gradual decay in fluorescence recorded on excitation at
all three wavelengths (D) is characteristic of progressive
photobleaching of Fura-2 under these conditions. Note the absence any
influence of the voltage ramp on the fluorescence trajectory recorded
at the isobestic wavelength f360.
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| Figure 2.
Inactivation of current through
IK,in is correlated with
[Ca2+]i elevation. Voltage steps of 20 s
duration from 50 to 200 mV leading to limited (A) and profound (B)
increases in [Ca2+]i (bottom trace, note
different scales) in two broad bean guard cells. The clamp current (top
trace, note different scales) shows the characteristic time course for
IK,in activation (A) in the absence of an
extensive rise in [Ca2+]i, and activation
followed by a decay in current amplitude (B) with the more pronounced
rise in [Ca2+]i. C, Summary of relative
IK,in inactivation as a function of the
change in [Ca2+]i
( [Ca2+]i) evoked by 20-s voltage steps
from 50 to 200 mV recorded in 52 independent experiments (solid
points). Histograms show the means ± SE of
measurements binned in successive pools of 10 or 11 experiments.
Inactivation of IK,in was calculated from
the ratio (Imax Ifinal)/Imax,
with Imax determined at maximum
IK,in amplitude and
Ifinal taken as the final current amplitude
without correction for instantaneous current.
[Ca2+]i values were determined from the
mean [Ca2+]i recorded over periods of 1 s immediately before and at the end of the voltage steps. Note that the
analysis does not account for measurements in which
[Ca2+]i was initially high, nor does it
account for measurements in which clamp steps yielded little inward
current. The distribution is therefore probably skewed to the right
along the x axis, but nonetheless shows that
current inactivation was associated with the rise in
[Ca2+]i. D, [Ca2+]i
elevation ( [Ca2+]i) after 20-s steps to
200 mV is dependent on the resting [Ca2+]i
level. Data from C plotted as a function of
[Ca2+]i before voltage steps to 200 mV.
Histograms show the means ± SE of measurements binned
in successive pools with [Ca2+]i 80 nM, 80 nM < [Ca2+]I 300 nM, and [Ca2+]I > 300 nM at rest. Note the logarithmic abscissa. The decline in
the mean [Ca2+]i from high starting
[Ca2+]i values is not consistent with
saturation of the Fura-2 signal.
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The voltage-clamp record in Figure 1 shows that the rise in
[Ca2+]i was accompanied
by a decline in the amplitude of inward membrane current. The initial
clamp step to +20 mV in Figure 1C showed a large, outward (positive)
current corresponding to the activation of
IK,out at this voltage. As the voltage was
driven to values between approximately 50 and 130 mV (at which,
with 10 mM K+ outside,
IK,out is inactive) the current declined to
close to 0. At voltages negative of about 140 mV a large, inward
current was observed, consistent with the activation of the
Ca2+-sensitive IK,in
(Lemtiri-Chlieh and MacRobbie, 1994 ; Grabov and Blatt, 1997 ). However,
this inward current decayed in magnitude in this and in the other
recordings as the voltage approached 200 mV, coincident with the rise
in [Ca2+]i.
To quantify the effect of prolonged membrane hyperpolarization on
IK,in, measurements were compiled from 52 independent experiments in which the membrane voltage was driven
stepwise to 200 mV for 20 s or longer. Again, the
characteristics of IK,in were related to
[Ca2+]i through
concurrent recordings of Fura-2 fluorescence. Examples of clamp-current
and [Ca2+]i recordings
from two guard cells are shown in Figure 2, A and B. The voltage step
for the cell in Figure 2A led to a small increase only in
[Ca2+]i (bottom
trace). In this case, and in cells showing a similar [Ca2+]i response, the
inward current exhibited prolonged activation, with an apparent
half-time near 100 ms, typical of IK,in.
This current remained stable or increased slowly thereafter during the
20-s period (Fig. 2A, top trace). In contrast, experiments in which
hyperpolarization led to an appreciable increase in
[Ca2+]i (Fig. 2B, bottom
trace) also showed a pronounced biphasic rise with a subsequent decline
in the clamp-current amplitude after the first 2 to 4 s at 200
mV (Fig. 2B, top trace). A summary of all 52 experiments shows the
positive correlation between the maximum change in
[Ca2+]i during clamp
steps and the relative inactivation of the current measured at the end
of the 20-s clamp step compared with that recorded 2 s after its
start (Fig. 2C). We also noted a dependence of voltage-evoked
[Ca2+]i increases on the
resting [Ca2+]i level
before stimulation (Fig. 2D). The analysis shows that the greatest rise
in [Ca2+]i was evoked
from resting values around a median of 140 nM,
whereas cells with resting
[Ca2+]i near and below 80 nM and above 300 nM
generally showed less sensitivity to the voltage stimulus.
The causal relationship of IK,in
inactivation to the
[Ca2+]i increases was
confirmed in single guard cells using a standard two-pulse protocol
with eight cycles of a 0.5-s conditioning step to 100 mV and 2-s
steps to test voltages from +20 to 200 mV, by introducing additional
0.5-s voltage steps between cycles to manipulate
[Ca2+]i. Figure
3 shows the results of two consecutive
voltage-clamp protocols with the additional steps either to 250
mV (a) or to 30 mV (b). The current records are overlaid in Figure 3A
in each case and show, in successive test pulses, the time-dependent
outward current of IK,out evoked on
positive voltage steps and IK,in on steps
negative of 120 mV. Intervening steps to 250 mV yielded a
cumulative rise in
[Ca2+]i (Fig. 3B, bottom
trace) and gave rise to the final time-dependent inward current (a,
numbered 1-8, corresponding to the numbered steps in Fig. 3B, top
trace) that declined in magnitude with each cycle coincident
with the rise in [Ca2+]i.
However, intervening steps to 30 mV, which did not evoke a rise in
[Ca2+]i, had little
effect on [Ca2+]i or on
the K+ current.

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| Figure 3.
Inactivation of current through
IK,in is evoked by
[Ca2+]i elevation. Data are from one guard
cell bathed in 5 mM Ca2+-Mes, pH 6.1, with 10 mM KCl. A, Clamp current recorded using standard two-pulse
protocols of eight cycles with the addition of a third, 0.5-s
intervening step at the end of each cycle to 250 mV (a) or to 30 mV
(b). Clamp cycles: 0.5-s conditioning step, 100 mV; 2-s test steps
(8) from +20 to 200 mV. B, Voltage (V, top trace) and
[Ca2+]i (bottom trace) records with
intervening voltage steps numbered according to the cycle (1-8,
cross-referenced to currents in A). The mean
[Ca2+]i during the final three cycles in each
protocol is indicated by the solid lines overlaid on the
[Ca2+]i record. C, Steady-state
current-voltage characteristic determined from the currents recorded at
the end of the test voltage steps in protocols a and b. The curves have
not been corrected for the background ("instantaneous") current.
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A cursory view of the last three cycles shows that
IK,in evoked by the test voltage steps was
greatly reduced in protocol a compared with the same steps in protocol
b, coincident with the mean
[Ca2+]i elevation (solid
bars over [Ca2+]i trace)
near 320 nM compared with 170 nM, respectively. In this case, analysis of the
steady-state current showed a 73% reduction of
IK,in after accounting for background
(instantaneous) currents (Fig. 3C). Current at 0 mV, which is
associated with IK,out, was recorded before
a significant rise in
[Ca2+]i and is known to
be insensitive to [Ca2+]i
(Hosoi et al., 1988 ; Lemtiri-Chlieh and MacRobbie, 1994 ; Grabov and
Blatt, 1997 ).
K+ Channel Activity Shows a Steep Dependence on
[Ca2+]i
To quantify the
[Ca2+]i sensitivity of
IK,in, a similar strategy of repeated
hyperpolarizations was used to manipulate
[Ca2+]i, and both current
and Fura-2 fluorescence were measured concurrently. In this case, 20-s
steps from a holding voltage of 50 to 200 mV were used to raise
[Ca2+]i and the intervals
between steps decreased from 90 to 20 s to give an elevated
background of [Ca2+]i at
the start of each subsequent step. IK,in
was characterized after subtracting the background (instantaneous)
current from measurements during the first 2 s of each step.
Figure 4A shows the results of
measurements from one guard cell obtained at four different
[Ca2+]i values (in
µM on right). The steady-state
IK,in from these data are included in
Figure 4B (solid symbols) along with the means ± SE of IK,in from
another 52 guard cells binned over
[Ca2+]i intervals of 80 nM. The results demonstrate a steep dependence of
IK,in on
[Ca2+]i that was most
pronounced over the range from 200 to 500 nM [Ca2+]i. When subjected
to nonlinear, least-squares fitting (Marquardt, 1963 ), the data could
not be accommodated satisfactorily with a simple titration function of
a single Ca2+-binding site. Therefore, fittings
were carried out using a formulation of the Hill equation (Hill, 1910 ):
where IK and
IK,max are the current and maximum current
at 200 mV, respectively; Kd is the
dissociation constant; and n is the cooperativity (Hill)
coefficient and corresponds to the apparent number of
Ca2+ ions binding per channel. Best fittings were
obtained with a Ki of 329 ± 31 nM. Analyses carried out on a cell-by-cell basis (not shown) gave a similar Ki of 346 ± 22 nM. In every case, the analyses also
yielded values for n close to 4 (mean ± SE, 4.1 ± 0.5 on a cell-by-cell basis), consistent
with the cooperative action of at least four Ca2+
ions to inactivate IK,in. Thus, the data
indicate a profound sensitivity of the channels to relatively small
changes in [Ca2+]i above
normal resting values, a point we will return to below.

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| Figure 4.
Inactivation of IK,in
shows a steep dependence on [Ca2+]i above
resting [Ca2+]i levels. A, Data are from one
guard cell bathed in 5 mM Ca2+-Mes, pH 6.1, with 10 mM KCl. IK,in recorded
during the first 2 s of 20-s steps to 200 mV with
[Ca2+]i elevated by successively decreasing
the interstep interval from 90 to 20 s. Data fitted to
single-exponential activation curves and points are shown at 100-ms
intervals for clarity. [Ca2+]i is on the
right (in µM). B, Summary of steady-state
IK,in from A (solid symbols) along with
means ± SE of data from 52 guard cells (open symbols)
binned in pools of eight to nine experiments with increasing
[Ca2+]i. [Ca2+]i
values were determined from the mean [Ca2+]i
recorded over the final 1 s of voltage steps after prior
stimulation to raise [Ca2+]i (see A) or from
equivalent measurements from resting [Ca2+]i
conditions. The solid line is the result of nonlinear least-squares
fitting of the means to the Hill equation (Eq. 1). Fitted parameters:
Ki, 329 ± 31 nM;
n (cooperativity coefficient), 4.1 ± 0.5. Statistically equivalent results were obtained when the data were
fitted without binning (not shown).
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Ca2+ Influx and the [Ca2+]i
Rise Are Independent of IK,in
Previous experiments showed that the amplitude of voltage-evoked
[Ca2+]i increases were
linearly related to the external Ca2+
concentration and were associated with Fura-2 quench when
Mn2+ was substituted for external
Ca2+ (Grabov and Blatt, 1998 ). These results and
the dependence of [Ca2+]i
on negative membrane voltages suggested a specific
Ca2+ influx triggered by the voltage across the
plasma membrane. However, because IK,in
also activates at these voltages, albeit over a much shorter time, it
could be argued that the Ca2+ influx occurred
through the K+ channels.
Ca2+ entry through the K+
channels in guard cells has been proposed, based on
tail-current-reversal analyses (Fairley-Grenot and Assmann, 1992 ).
To distinguish between these two possibilities, we recorded
[Ca2+]i and the channel
current under voltage clamp during challenge with
Ca2+ and K+ channel
antagonists. Figure 5A shows that adding
0.1 mM Gd3+, a
Ca2+ channel blocker (Klusener et al., 1995 ;
Sedbrook et al., 1996 ), outside virtually eliminated the
[Ca2+]i transients evoked
by subsequent voltage steps to 200 mV (bottom trace), while promoting
the current associated with IK,in (top trace). Similar results were obtained from an additional
four independent experiments with the Ca2+
channel blocker. Because Gd3+ may permeate the
plant plasma membrane (Klusener et al., 1995 ), albeit slowly, we also
explored the effects of higher-Mr peptide toxins that show specificity for plasma membrane
Ca2+ channels in animals.

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| Figure 5.
Voltage-evoked [Ca2+]i
rise is sensitive to extracellular Ca2+ channel blockers.
A, [Ca2+]i increases (trace below) and clamp
current (trace above) during 20-s steps from 50 to 200 mV ( ,
above) before and after adding 0.1 mM GdCl3 to
the bath. Period of GdCl3 exposure is indicated by the open
bar. Data are from one guard cell in 5 mM
Ca2+-Mes, pH 6.1, with 10 mM KCl. Inset, Clamp
current during steps to 200 mV ( , above) replotted on expanded
time scale shows characteristic activation of the
IK,in current (Grabov and Blatt, 1997 ) when
the [Ca2+]i rise is suppressed in the
presence of Gd3+ (fine line) and its time-dependent
inactivation when [Ca2+]i rises in the
absence of Gd3+ (solid line). B,
[Ca2+]i increases evoked during 20-s steps
from 50 to 200 mV ( , above) before and after adding 0.5 µM calcicludine to the bath. Data are from one guard cell
in 5 mM Ca2+-Mes, pH 6.1, with 10 mM KCl. Period of exposure to the Ca2+ channel
blocker is indicated by an open bar. Time scale (below), 2 min.
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Exposures to 0.5 µM calcicludine suppressed the
[Ca2+]i rise and relieved
IK,in inactivation at 200 mV (Fig. 5B).
Calcicludine is a 6.9-kD peptide toxin derived from Dendroaspis
augusticeps venom and preferentially blocks L-type
Ca2+ channels in animal tissues (Schweitz et al.,
1994 ). The toxin is a highly charged, soluble protein and is therefore
unlikely to pass across the plasma membrane. In contrast (not shown),
the voltage-evoked
[Ca2+]i rise was
unaffected by a peptide toxin, 1 µM
-conotoxin (GVIIIa), and a specific N-type
Ca2+ channel antagonist (Mori et al., 1991 ;
Leveque et al., 1994 ). Substitution of external
K+ with Cs+, which blocks
the current through IK,in (Thiel and Wolf,
1997 ), had no measurable effect on the voltage-evoked
[Ca2+]i rise in each of
the six experiments (not shown), and the
[Ca2+]i rise was
insensitive to changes in external K+ between 0.1 and 10 mM (Grabov and Blatt, 1998 ). These latter results, and the insensitivity of IK,in to
Gd3+ and calcicludine compared with the
[Ca2+]i transients,
implicate a unique class of Ca2+-permeable
channels at the plasma membrane that activate on hyperpolarization to
facilitate Ca2+ entry. The data also argue
against a predominance of the Ca2+ flux through
the K+ channels (Fairley-Grenot and Assmann,
1992 ), a point we comment on in ``Discussion''.
Evoked [Ca2+]i Increases Are Coupled to
Cytosolic Ca2+ Release
Although the data above point to entry across the plasma membrane
as the initial source of Ca2+ for the
voltage-evoked [Ca2+]i
transients, intracellular Ca2+ stores have also
been indicated in evoked
[Ca2+]i signals in guard
cells (Blatt and Grabov, 1997 ; McAinsh et al., 1997 ; Grabov and Blatt,
1998 ). Analogous patterns of Ca2+ entry and
subsequent release from intracellular stores are well known in animal
cells and result from positive feedback of Ca2+
that activates intracellular Ca2+ release
channels. Such CICR rapidly amplifies
[Ca2+]i signals and
facilitates [Ca2+]i
spikes and oscillations (Clapham, 1995 ; Berridge, 1996 ).
To assess the contribution of intracellular Ca2+
release to the voltage-evoked
[Ca2+]i transients, we
used a strategy of Fura-2 fluorescence quenching with
Mn2+, which passes through many
Ca2+-permeable channels (Fasolato et al., 1993 ;
Pineros and Tester, 1995 ; Schofield and Mason, 1996 ; Striggow and
Ehrlich, 1996 ). Its binding causes a loss of Fura-2 fluorescence that
can be separated from the effects of
[Ca2+]i by recording the
Fura-2 fluorescence emission at f360, the isobestic wavelength. Thus, if the
[Ca2+]i rise depended on
divalent release from intracellular stores, we reasoned that
hyperpolarization should be followed by a stimulation of Fura-2
quenching once guard cells were loaded with Mn2+.
For these experiments guard cells were exposed to 2 mM
Mn2+ for 8 h to load intracellular
Ca2+ stores with Mn2+
(Fasolato et al., 1993 ). Before the start of recordings, the guard
cells were washed in Ca2+-Mes buffer with 10 mM KCl to remove external Mn2+. After
impalements, membrane voltage was clamped to 50 mV and the cells were
loaded with Fura-2 in the usual manner. Thereafter, Fura-2 fluorescence
was recorded after excitation at 360 nm and the cells were challenged
with membrane voltage steps to 200 mV. Results from one guard cell
are shown in Figure 6A. Voltage steps to
200 mV resulted in a rise, and then a more rapid fall in
f360 when Ca2+ was
present outside. However, when Ca2+ was removed
from the bath to prevent Ca2+ entry, triggering
intracellular release, only a stepwise increase in
f360 was seen and then only during the
period that the voltage was clamped to 200 mV. In fact, comparing
f360 quench immediately after the voltage
steps showed that a 5.5-fold greater rate of dye quenching followed the
stimulus in the presence of external Ca2+ (Fig.
6A, inset). Equivalent results were obtained in each of six separate
experiments, including four experiments with and without external
Ca2+. On one occasion
f360 was seen to decay even before the end
of the voltage step in the presence of external
Ca2+. In every case, the quenching during the
first 30 s following voltage steps was accelerated in the presence
of external Ca2+ by comparison with measurements
in the absence of external Ca2+ (mean
acceleration ± SE:
+Ca2+, 6.2 ± 0.5-fold;
Ca2+, 0.9 ± 0.1-fold).

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| Figure 6.
Evoked [Ca2+]i rise is
facilitated by Ca2+ release from intracellular stores. A,
Fura-2 fluorescence quenching recorded on
f360. Data are from one guard cell recorded
after intracellular loading with Mn2+ in 20 mM
K+-Mes, pH 6.1, and 2 mM MnCl2.
Voltage steps of 20 s to 200 mV ( , above) applied with the
cell bathed in 20 mM K+-Mes, pH 6.1, plus 2 mM CaCl2, then in the same buffer without
CaCl2 (open bar), and finally with 2 mM
MnCl2 (striped bar). Inset, f360
during the first 20 s after voltage steps without ( ) and with
( ) Ca2+ outside after normalizing to the fluorescence
signal at the start of each voltage step. Note the rapid decay in
f360 after voltage stimulus in the presence
of external Ca2+. B to D,
[Ca2+]i rise was suppressed by 10 µM ryanodine (B) and augmented by 100 µM
heparin (C) and 1 mM neomycin sulfate (D). Data are from
three guard cells in 5 mM Ca2+-Mes, pH 6.1, with 10 mM KCl. Membrane voltages were clamped to 50 mV
in each case. Voltage steps to 200 mV (B) and 180 mV (C
and D) are indicated above ( ). Times
of treatments with ryanodine, heparin, and neomycin sulfate are
indicated by the open bars in each case. Note the prolonged secondary
rise in [Ca2+]i in the presence of heparin
and neomycin sulfate.
|
|
We interpret this behavior and the increase in fluorescence during the
voltage steps to reflect the characteristics of the two divalent flux
events. In the presence of external Ca2+, the
voltage stimulus evokes a Ca2+ influx and, with
the Mn2+ electrochemical gradient directed out of
the cell in the absence of external Mn2+,
simultaneously a Mn2+ efflux across the plasma
membrane, which leads to an increase in Fura-2 fluorescence. The entry
of Ca2+ then triggers Mn2+
release from intracellular stores and a consequent quenching of the
fluorescence. That quenching is potentiated beyond the period of the
voltage step implies that Mn2+ release continues
after the voltage step and is wholly consistent with the continued rise
in [Ca2+]i and prolonged
high [Ca2+]i recorded
even after voltage steps (compare Figs. 2 and 3; also see Grabov and
Blatt, 1998 ). By contrast, in the absence of external Ca2+ no intracellular release is evoked and only
the initial increase in fluorescence associated with
Mn2+ efflux during the voltage step is observed.
We also tested the effects of neomycin sulfate and heparin (Fig. 6, C
and D), antagonists of inositol-1,4,5-trisphosphate-mediated Ca2+ release, and ryanodine (Fig. 6B), which
blocks cADPR (ryanodine-receptor)-activated Ca2+
release channels (Ehrlich et al., 1994 ; Clapham, 1995 ). Of these antagonists, we found that only ryanodine antagonized the
[Ca2+]i response evoked
by the voltage steps (Fig. 6B). In the presence of 10 µM
ryanodine [Ca2+]i
transients recorded on negative voltage steps were reduced to 46% ± 8% (n = 5) of the control before treatments.
Ryanodine also affected the rate of the
[Ca2+]i rise in parallel
with the reduction in
[Ca2+]i peak amplitude
(Fig. 6B). By contrast, evoked
[Ca2+]i transients were
1.3- to 2.5-fold greater than those recorded before treatments in the
presence of 1 mM neomycin sulfate and 100 µM heparin (Mr
3000; Fig. 6, C and D), concentrations consistent with previous studies
of guard cells and pollen (Armstrong and Blatt, 1995 ; Franklin-Tong et
al., 1996). Furthermore, in the presence of these compounds the
[Ca2+]i transients in
every case failed to recover fully and were followed by prolonged
secondary increases in
[Ca2+]i. Because neomycin
sulfate and heparin can interact with ryanodine-sensitive Ca2+ channels (Ehrlich et al., 1994 ; Wang et al.,
1996 ), these results implicate a homologous pathway for
[Ca2+]i release in
facilitating these
[Ca2+]i transients.
 |
DISCUSSION |
Our demonstration of K+ channel control by
[Ca2+]i establishes the
[Ca2+]i signal as a
pivotal intermediate in feedback coupling between membrane voltage and
the K+ channels. Previous studies (Grabov and
Blatt, 1998 ) showed that prolonged membrane hyperpolarization within
the normal physiological voltage range led to a rise in
[Ca2+]i that was coupled
to Ca2+ influx across the plasma membrane. The
results summarized above show that, in vivo, this elevation of
[Ca2+]i leads to an
inactivation of IK,in (Figs. 1-3).
Remarkably, the action of
[Ca2+]i on the
K+ channels was realized at free concentrations
only just above normal resting values (apparent
Ki, 329 ± 31 nM). Furthermore, the
[Ca2+]i sensitivity of
the current indicated a concerted action of at least four
Ca2+ ions, leading to K+
channel inactivation (Fig. 4). Such exquisite sensitivity to [Ca2+]i has the effect of
a very high gain and, hence, a narrow dynamic range for control of
IK,in. In other words, relatively small
changes in [Ca2+]i are
able to act as a regulatory "on/off switch," transferring the
K+ channels between active and inactive states.
To our knowledge such cooperativity has not previously been documented
in vivo in plant cells. Previous studies broadly defined only the
limits of [Ca2+]i action
on IK,in in guard cells between 100 nM and 1 µM
[Ca2+]i (Schroeder and
Hagiwara, 1989 ; Lemtiri-Chlieh and MacRobbie, 1994 ; Grabov and Blatt,
1997 ). Nonetheless, a similar degree of [Ca2+]i sensitivity may
be characteristic of the KCO1 K+ channel recently
cloned from Arabidopsis (Czempinski et al., 1997 ). It is interesting,
too, that a 4-fold cooperativity is known in
Ca2+-signaling processes in animals (Clapham,
1995 ; Berridge, 1996 ; Cheng et al., 1996 ; Dolphin, 1996 ), including
cGMP cyclase activation in vertebrate rods (Stryer and Koch, 1988 ).
This situation, however, contrasts with pHi
control of IK,in that is graded over a
broad range of [H+]i and
appears to depend on the binding of only one H+
ion per channel (Grabov and Blatt, 1997 ).
In light of earlier studies of
[Ca2+]i action on
IK,in, it is worth noting the difficulties
of quantifying the effects of
[Ca2+]i in vivo and of
Ca2+ buffering, especially in patch-electrode
experiments. In general, whole-cell patch recording results in a rapid
exchange of the cytosol with the solution in the patch electrode and
leads to the loss of cytosolic regulatory factors and
Ca2+ buffering (Pusch and Neher, 1988 ) that may
be replaced in part by Ca2+ buffers included in
the patch pipette. Kelly et al. (1995) reported that
[Ca2+]i elevation
suppresses IK,in when buffered with
1,2-bis(o-aminophenoxy)ethane-N,N,N ,N -tetraacetic acid (BAPTA) but not with EGTA. They ascribed the difference to buffer
efficacy, the slower kinetics of Ca2+-EGTA
binding, and H+ competition with
Ca2+ for binding to EGTA. However, because their
measurements were carried out under steady-state
[Ca2+]i and with
pHi held constant, the discrepancy in
Ca2+ buffer actions remains difficult to explain.
In contrast, our use of intracellular microelectrodes has the advantage
that measurements are made without inclusion of
Ca2+ buffers and with a minimum of disturbance to
the cell and cytosol, because diffusional exchange with intracellular
microelectrodes is restricted by the bulk access resistance of the
microelectrode tip and shank (Purves, 1981 ).
In fact, the consequences of voltage-evoked
[Ca2+]i changes for the
current through the K+ channels are likely to be
appreciable, as the microelectrode recordings indicate. Guard cells
commonly show two states of membrane voltage that may often be
separated by 100 mV or more (Thiel et al., 1992 ; Gradmann et al.,
1993 ), and spontaneous membrane hyperpolarization can increase
[Ca2+]i from
approximately 100 to 200 nM to steady-state values near 500 nM (Grabov and Blatt, 1998 ). Under these conditions, the
positive effect of membrane hyperpolarization in activating
IK,in will be largely overshadowed with
inactivation of the current as the steady-state
[Ca2+]i becomes elevated.
In numerical terms, hyperpolarization from 140 mV to voltages near
and negative of 200 mV may still limit steady-state
IK,in to values of approximately 10 µA
cm 2 in the face of the
[Ca2+]i rise, despite the
increase in electrochemical driving force and the effect of voltage
otherwise on the open-channel probability (Figs. 3 and 4; see also
Grabov and Blatt, 1997 ).
How is this rise in
[Ca2+]i achieved?
Although the increase in
[Ca2+]i is triggered by
Ca2+ influx across the plasma membrane and at
voltages essentially parallel to those effective in activating
IK,in (Grabov and Blatt, 1998 ), present
evidence argues against Ca2+ entry through the
K+ channels themselves (Fairley-Grenot and
Assmann, 1992 ). We found that the Ca2+ channel
antagonist Gd3+ blocked the voltage-evoked rise
in [Ca2+]i, and yet the
same experiments showed that the antagonist actually promoted current
through the K+ channels (Fig. 5). The specificity
of Gd3+ for Ca2+ channels
is known to be relatively poor (Alexandre and Lassalles, 1991 ; Zou et
al., 1991 ). However, the
[Ca2+]i rise was also
sensitive to calcicludine (Fig. 5), a peptide toxin that shows high
specificity for L-type Ca2+ channels (Schweitz et
al., 1994 ). In contrast, voltage-evoked [Ca2+]i increases were
unaffected by another venom toxin, -conotoxin, that blocks N-type
Ca2+ channels (Leveque et al., 1994 ). In
complementary experiments we observed that the
[Ca2+]i rise was
independent of extracellular K+ (Grabov and
Blatt, 1998 ) and was unaffected by block of the
K+ current with Cs+. Were a
significant flux of Ca2+ to pass through the
K+ channels, both competition with
K+ and Cs+ block might have
been expected to reduce the
[Ca2+]i rise. So, the
simplest interpretation is that Ca2+ entry across
the plasma membrane occurs through hyperpolarization-activated Ca2+ channels. In fact, a sensitivity to membrane
hyperpolarization may be a common feature of many
Ca2+ channels in the plant plasma membrane,
although it remains to be seen whether hyperpolarization-activated
Ca2+ channels of higher plants are found
predominantly in specialized cells, such as guard cells.
Hyperpolarization-activated Ca2+ channels have
also been reported in tomato plasma membrane (Gelli and Blumwald,
1997 ), and there are indications of similar Ca2+
channels in Mimosa pudica (Stoeckel and Takeda, 1995 ).
Elevation of [Ca2+]i by
membrane hyperpolarization also appears to depend on
Ca2+ release from intracellular stores. We
observed an accelerated quenching of Fura-2 fluorescence by
intracellular (sequestered) Mn2+ following
voltage steps when guard cells were preloaded with the divalent
cation, and the results of studies with
Ca2+ release antagonists lead to a similar
conclusion (Fig. 6). Block of the voltage-evoked
[Ca2+]i rise by
ryanodine, and its stimulation by heparin and neomycin sulfate,
suggests a parallel to ryanodine-receptor Ca2+
channels that mediate Ca2+ release in
neuromuscular tissues (Ehrlich et al., 1994 ; Clapham, 1995 ). The fact
that ryanodine block was incomplete may reflect the relatively short
exposures that could be achieved within the time frame of these
experiments, or it may indicate a significant contribution of external
Ca2+ influx to the rise in
[Ca2+]i. However, we
cannot rule out additional contributions to
[Ca2+]i release via
inositol-1,4,5-trisphosphate-sensitive or other unrelated pathways
(Cheek et al., 1994 ; Jouaville et al., 1995 ). We also noted a
dependence of voltage-evoked
[Ca2+]i increases on the
resting [Ca2+]i level
before stimulation (Fig. 2D). A similar sensitivity to [Ca2+]i is common to many
Ca2+-release events in animals that show a
bell-shaped curve characteristic of potentiation by
[Ca2+]i (Callamaras and
Parker, 1994 ; Bezprozvanny and Ehrlich, 1995 ; Cheng et al., 1996 ; Thorn
et al., 1996 ).
These parallels to Ca2+ release events in animals
do raise questions about the nature of the guard cell
Ca2+-release pathway and the location of the
Ca2+ stores. It is possible, for example, that
[Ca2+]i changes are
mediated by spatially distinct Ca2+ stores with
different characteristics for Ca2+ release
(Bootman and Berridge, 1996 ; Plieth et al., 1998 ). Thus, conceivably,
short-term dynamic control of IK,in might
be more closely coupled to
[Ca2+]i and
Ca2+ release events close to the plasma membrane,
in contrast to the current characteristics determined under
quasi-steady-state
[Ca2+]i, as described
above. In this context, we note that ryanodine affects
Ca2+ release from plant microsomes but acts to
stimulate Ca2+ release even at micromolar
concentrations (Allen et al., 1995 ; Muir and Sanders, 1996 ), in
contrast to our observations (Fig. 6B). Furthermore, despite the
presumed role for vacuolar Ca2+ in plant cell
(and guard cell) signaling (Ward and Schroeder, 1994 ; Allen and
Sanders, 1995 , 1996 ; Johannes and Sanders, 1995 ), one recent study
indicated that evoked Ca2+ release in the alga
Chara does not depend on vacuolar
Ca2+ stores (Plieth et al., 1998 ). Therefore, it
is conceivable that the
[Ca2+]i signal in the
guard cells draws on more than one Ca2+-release
pathway, each with differing pharmacological characteristics and,
possibly, separate Ca2+ stores. Such issues
aside, these and our previous observations (Grabov and Blatt, 1998 )
implicate the coordination of Ca2+ influx and
Ca2+ release from intracellular stores that
parallels CICR events in animal cells (Clapham, 1995 ; Berridge, 1996 ).
Again, the data also underscore at least one important difference from
the animal models. The
[Ca2+]i rise in the guard
cells was evoked at negative voltages, whereas voltage-evoked CICR
in neuromuscular tissues is normally triggered by membrane
depolarization that activates Ca2+ influx through
pharmacologically distinct, L-type Ca2+ channels
(Schweitz et al., 1994 ; Chavis et al., 1996 ).
What are the physiological roles for coupling
IK,in to membrane voltage through
[Ca2+]i and for the high
gain inherent in IK,in inactivation by
[Ca2+]i? One clue may lie
in voltage oscillations that have been observed in guard cells (Thiel
et al., 1992 ; Gradmann et al., 1993 ). These oscillations occur
spontaneously, they are potentiated by ABA and auxin that effect
stomatal movements (Thiel et al., 1992 ; Blatt and Thiel, 1994 ), and
they may be aperiodic or exhibit periodicities of 10 to 20 s
(Gradmann et al., 1993 ) to many minutes (Thiel et al., 1992 ; Blatt and
Thiel, 1994 ). These events arise through fluctuations in the activities
of the K+ and anion channels (Blatt and Thiel,
1994 ) similar to those of the action potentials in Characean algae
(Beilby, 1986 ). The effect is to drive the membrane between the
hyperpolarized state, characterized by K+ uptake
via IK,in and balanced by
H+ efflux through the
H+-ATPase, and the depolarized state, in which
efflux of K+ and anions dominate. Significantly,
[Ca2+]i elevation leads
to inhibition of the H+-ATPase (Kinoshita et al.,
1995 ) and IK,in (Figs. 3 and 4), as well as
activation of anion channels (Hedrich et al., 1990 ; Schroeder and
Keller, 1992 ). Inhibition of the H+-ATPase shows
an apparent Kd of approximately 300 nM, similar to what we found for
IK,in (Fig. 4). We (Grabov and Blatt, 1998 ) previously demonstrated the coupling of
[Ca2+]i to membrane
voltage and suggest now that its function may be to provide the
necessary feedback to entrain K+ and anion
channels as a response "cassette" for osmotic balance, switching
the membrane between states for net uptake and net loss of these
solutes (Gradmann et al., 1993 ).
Coupling to membrane voltage may also serve to "condition"
[Ca2+]i signals that are
triggered in response to hormones and other stimuli (Grabov and Blatt,
1998 ). Downstream of the initial stimulus, effective control of the ion
channels and solute flux requires that second-messenger
"signatures" correctly reflect the needs for change in solute flux
dictated by the prior transport status of the cell. Thus, a second
function for voltage coupling may lie in adapting the
[Ca2+]i signal output on
stimulation to the prevailing requirements for solute flux. In the
simplest sense, if the purpose of a rise in
[Ca2+]i, for example, in
response to ABA (Blatt and Grabov, 1997 ; Thiel and Wolf, 1997 ), is to
trigger membrane depolarization when the voltage is situated well
negative of the K+ equilibrium voltage
EK, the same
[Ca2+]i rise will be
superfluous should the membrane already be situated at a voltage
positive of EK and, hence, biased for
solute loss. In fact, ABA does not evoke significant
[Ca2+]i increases when
the membrane voltage is clamped near 50 mV but only when the voltage
is situated near or negative of 100 mV (Grabov and Blatt, 1998 ).
These ideas lend a further dimension to concepts of frequency encoding
(Campbell et al., 1996 ; Knight et al., 1996 ) and to our understanding
of [Ca2+]i oscillations
in plants (McAinsh et al., 1995 ; Webb et al., 1996 ), and they raise
issues relating to the spatiokinetic mechanics that couple membrane
voltage, Ca2+ influx, and
Ca2+ release at the subcellular level.
In conclusion, we find that inactivation of
IK,in by
[Ca2+]i appears to depend
on the cooperative action of four Ca2+ ions,
conferring on the K+ channels a very steep
dependence on [Ca2+]i in
the free-concentration range just above normal resting values. Such
[Ca2+]i increases in
broad bean guard cells can be evoked on membrane hyperpolarization
within the normal physiological voltage range and thus couple
IK,in activity to membrane voltage in a
negative-feedback control loop. We also find that voltage-evoked
[Ca2+]i increases depend
on intracellular Ca2+ release and on
Ca2+ influx, the latter occurring via a pathway
that is pharmacologically distinct from
IK,in. These observations implicate a
process of CICR with characteristics that differ markedly from the
conventional neuromuscular models and suggest a function in coordinate
control of K+, H+, and
anion transport for osmotic balance.
 |
FOOTNOTES |
1
This work was supported by grants from the
Gatsby Charitable Foundation, the Royal Society, Human Frontiers
Science Program (no. RG95/303 M), and the European Community Biotech
(no. CT96-0062). A.G. was supported by the British Biotechnology and
Biological Sciences Research Council (grant no. 32/C098-1).
*
Corresponding author; e-mail mblatt{at}wye.ac.uk; fax
44-1233-813-140.
Received June 11, 1998;
accepted September 24, 1998.
 |
ABBREVIATIONS |
Abbreviations:
[Ca2+]i, cytosolic
free [Ca2+].
CICR, Ca2+-induced
Ca2+ release.
f340, f360, f390,
fluorescence excited by 340, 360, and 390 nm light, respectivelyIK,.
in, IK,out,
inward- and outward-rectifying K+ channels, respectively.
 |
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