First published online April 25, 2002; 10.1104/pp.011007
Plant Physiol, June 2002, Vol. 129, pp. 786-796
Reorientation of Seedlings in the Earth's Gravitational Field
Induces Cytosolic Calcium Transients1
Christoph
Plieth* and
Anthony J.
Trewavas
Zentrum für Biochemie und Molekularbiologie,
Christian-Albrechts-Universität, Am Botanischen Garten 1-9 (Room
517), D-24118 Kiel, Germany (C.P.); and Institute of Cell and
Molecular Biology, The King's Buildings (Botany), The University of
Edinburgh, Mayfield Road, Edinburgh EH9 3JH, United Kingdom
(A.J.T.)
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ABSTRACT |
The gravitational field controls plant growth, morphology,
and development. However, the underlying transduction mechanisms are
not well understood. Much indirect evidence has implicated the
cytoplasmic free calcium concentration
([Ca2+]c) as an important factor, but direct
evidence for changes in [Ca2+]c is currently
lacking. We now have made measurements of
[Ca2+]c in groups of young seedlings of
Arabidopsis expressing aequorin in the cytoplasm and reconstituted in
vivo with cp-coelenterazine, a synthetic high-affinity luminophore.
Distinct [Ca2+]c signaling occurs in response
to gravistimulation with kinetics very different from
[Ca2+]c transients evoked by other mechanical
stimuli (e.g. movement and wind). [Ca2+]c
changes produced in response to gravistimulation are transient but with
a duration of many minutes and dependent on stimulus strength (i.e. the
angle of displacement). The auxin transport blockers 2,3,5-tri-iodo
benzoic acid and N-(1-naphthyl) phthalamic acid
interfere with gravi-induced [Ca2+]c
responses and addition of methyl indole-3-acetic acid to whole seedlings induces long-lived [Ca2+]c
transients, suggesting that changes in auxin transport may interact
with [Ca2+]c. Permanent nonaxial rotation of
seedlings on a two-dimensional clinostat, however, produced a sustained
elevation of the [Ca2+]c level. This probably
reflects permanent displacement of gravity-sensing cellular components
and/or disturbance of cytoskeletal tension. It is concluded that
[Ca2+]c is part of the gravity transduction
mechanism in young Arabidopsis seedlings.
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INTRODUCTION |
Many studies have demonstrated that
the cytoplasmic free Ca2+ concentration
([Ca2+]c) is affected by
environmental stimuli such as touch, wind, cold, drought, light, and
oxidative stress. These stimuli induce transient elevations of
[Ca2+]c that modify the
activity of many Ca2+-dependent proteins. When
integrated together with other molecular processes of signal
transduction, [Ca2+]c
transients may help mediate biochemical and physiological responses of
the plant (for review, see Plieth, 2001 ). The variety of stimuli that
modify [Ca2+]c is
extensive and discussions of possible mechanisms to explain how
[Ca2+]c might
specifically mediate each stimulus are frequent (e.g. Trewavas and
Malhó, 1997 ; Malhó, 1999 ; Sanders et al., 1999 ).
[Ca2+]c has also been
suggested many times to be an important factor for producing an
appropriate graviresponse (Sinclair and Trewavas, 1997 ; Weisenseel and
Meyer, 1997 ; Chen et al., 1999 ; Chatterjee et al., 2000 ). Interactions
between the effects of auxin on growth and external
Ca2+ have also been reported a number of times
(Lee et al., 1983a , 1983b ) and other data suggest a correlated
transport of Ca2+ across the wall during
gravitropic bending (Roux and Serlin, 1987 ). Evidence relating to the
involvement of [Ca2+]c in
gravitropism is extensive but mainly indirect, often relying on
inhibitors (Belavskaya, 1996 ), calcium-binding proteins (Stinemetz et
al., 1987 ), or other cellular messengers known to be related to
[Ca2+]c signaling such as
IP3 (Perera et al., 1999 ).
[Ca2+]c changes in
response to gravistimulation in maize (Zea mays) coleoptiles have been reported (Gehring et al., 1990 ), but the data
have neither yet been kinetically analyzed nor reproduced. One
extremely thorough imaging investigation failed to observe any change
of [Ca2+]c in root tissue
(Legue et al., 1997 ).
The simplest method to measure
[Ca2+]c in whole
seedlings is to use aequorin transformation (Knight et al., 1991 ). We
have tried several times to detect
[Ca2+]c transients after
gravitational stimulation using this method but failed to observe
substantive [Ca2+]c
changes in single transformed seedlings (M.R. Knight and A.J. Trewavas,
unpublished data). To resolve this important issue, we have now
redesigned equipment to accommodate larger numbers of transformed
seedlings and reconstituted in vivo with cp-coelenterazine (CTZ), which
gives a much more sensitive Ca2+ indicator. With
these improvements, we can now routinely detect changes in
[Ca2+]c involved in graviresponse.
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RESULTS |
Gravitational Signals Induce Changes in
[Ca2+]c That Are Different to Other
Mechanical Stimuli
Transgenic Arabidopsis seedlings expressing aequorin in the
cytoplasm were grown on vertical agar in a petri dish and reconstituted with cp-CTZ. Seedlings were fixed to a wheel (Fig.
1) in front of a PMT, inside a
chemiluminometer, and rotated to various angles relative to the gravity
vector. Initially, a plate of seedlings was turned through 135° in
the chemiluminometer and returned within 5 s to the vertical
position. A short luminescence transient
was observed (Figs. 2A and 3B; ±135°),
followed by a slight shoulder. However, when the seedlings were left at
+135°, the initial spike (lasting about 25 s) and the second
shoulder transient (peaking at 90 s and lasting about 15 min) were
much more evident (Figs. 2A and 3A). Extrapolation of the shoulder back
along the time axis suggests it may be initiated at time zero (i.e.
time of movement). The initial spike and the shoulder, therefore, may
have different origins. Further rotation to restimulate the seedlings
produced a reduced response (Figs. 2A and 4).

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Figure 1.
Scheme of the rotatable wheel (two-dimensional
clinostat) for mounting Arabidopsis seedling vertically in front of a
photo multiplier tube (PMT).
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Figure 2.
[Ca2+]c changes
in Arabidopsis seedlings expressing the calcium indicator aequorin in
the cytoplasm in response to different mechanical stimuli. A,
Gravistimulation by turning seedlings growing on a vertical agar plate
upside down in front of a luminometer. At t = 25 min
and t = 50 min, seedlings were turned 135° upside down and
immediately back to vertical position (±135°). At t = 75 min,
seedlings were turned through 135° and left for 25 min in this
position. At 100 min, seedlings were turned back to normal
position. At t = 125 min, seedlings were turned to 135° position
and at 150 min, turned back. B, Mechanical stimulation by blowing
ambient air over seedlings growing on a vertical agar plate. Pulses of
air (50 mL s 1 for 1 s) were applied at
t = 25, 50, 75, 100, and 125 min.
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Figure 3.
Effect of different stimuli on the
[Ca2+]c response. A,
Gravistimulation: at t = 3 min, the plate with seedlings was
turned through 135°. B, Control: At t = 3 min, the plate was
turned 135° and immediately (within the same sample interval) back to
vertical position. C, Control: at t = 3 min, the plate was turned
360°. D, Control: stimulation by wind; at t = 3 min, 50 mL of
ambient air was blown in 1 s through the plate. SDs
are given at t = 1.0, 3.1, 4.5, 7.0, and 10 min with
n = 5 for all curves. E and F, Enlargements of A and D,
respectively, to show main initial
[Ca2+]c spike after
stimulation and reveal the difference in time scale.
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Figure 4.
Attenuation of the gravity-induced slow
[Ca2+]c phase, i.e.
desensitization, as measured by decreasing amplitudes with repeated
gravistimulation. Curves in A through D are averages of five.
SDs are given at t = 1.0, 3.1, 4.5, 7.0, and 10 min.
E, Light yields produced by stimulation (i.e. integrated areas under
the curves shown in A through D minus background).
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Gravistimuli have sometimes been regarded as kind of inside-out
mechanical stimuli (Trewavas and Knight, 1994 ). Figure 2B shows the
effect of brief mechanical stimulations on seedling luminescence by
blowing air over seedlings. Whereas the initial spike might be similar
to that shown in Figure 2A, the dip after the spike indicates a marked
difference in the [Ca2+]c
characteristics (Fig. 3, A versus D and E versus F).
Is the initial spike increased by leaving the seedlings at 135° or is
it simply induced by rotation itself? Figure 3B shows that turning the
seedlings to 135° and back again within 5 s leads to a reduced
luminescence compared with seedlings turned to 135° and left in that
position (Fig. 3A). A single rotation around 360° (Fig. 3C) also
leads to a smaller spike, thereby lacking any subsequent shoulder.
Figure 3, E and F, which expand the time scale, indicate that the
kinetics of this initial gravi-induced spike are different to those of
wind. The gravispike lasts some 25 s, whereas wind or touch is
limited largely to a 5-s response as reported before (Knight et al.,
1991 ). Figure 3, A and D, confirm the pronounced difference between the
gravity-induced changes in
[Ca2+]c and those of wind
in the second part of the response.
The [Ca2+]c transients in
response to gravistimulation of plants grown on Suc-free medium did not
differ from those in plants grown on full medium including 1%
(w/v) Suc (data not shown). Also, there was no significant
difference in gravity-induced
[Ca2+]c kinetics between
dark-grown and control seedlings (data not shown).
Signal Adaptation
A number of signals lead to adaptation in
[Ca2+]c responsiveness
such that successive stimulation either fails to elicit a second [Ca2+]c peak within a
defined time period of several minutes or even hours or that successive
stimuli elicit much smaller peaks (e.g. Knight et al., 1992 ; Plieth et
al., 1999b ). Figures 2A and 4 indicate that adaptation to gravistimuli
may also be present. Figure 4A shows the
response of seedlings rotated to 135° and left for 15 min, and Figure
4B shows that subsequent return to the vertical induces an additional
luminescence signal. Surprisingly, the turn back to the vertical
induces a luminescence response similar in character to that of the
initial response, although the amplitude of the shoulder is lower. This
suggests that the turn-back luminescence is also a gravitropic
response. Upon a second turn to 135° (Fig. 4C) and a subsequent
second turn back to the vertical (Fig. 4D), similar kinetics of
luminescence change are observed again except that the shoulder is
again smaller. The initial spike remains almost unchanged, indicating a
lack of adaptation of this response with the experimental design used
here. Figure 4E reports total luminescence produced by these
experiments, suggesting that the major reduction is in the second turn
to 135°.
Size of [Ca2+]c Response Is Related to
the Angle of Displacement
The optimum angle for gravitropic stimulation has been shown to be
between 120° and 135°, and slower responses are obtained at 45°,
90°, and 180° (Larsen, 1969 ). It is thought that 135° provides
the optimal situation for statocyte amyloplasts to slide down the cell
wall, providing maximal gravitropic stimulation. Batches of seedlings
were subjected to successively increasing angles of stimulation to
detect any relationship between the apparent strength of the stimulus
and the luminescence response (Fig. 5A). The bar underneath the trace in Figure 5A indicates the sequence of
changes in the angle of stimulation. Independent experiments (Fig. 5,
B-E) show that the maximum of luminescence was obtained at 135°. The
total transient length is clearly shorter at 45° and 90° as well,
being only about 6 min at 45°.

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Figure 5.
Effect of different angles of displacement on the
[Ca2+]c response in
Arabidopsis. A, The plate with seedlings was tilted as indicated by the
bar. Trace is average of four. SDs are given at 3, 7, 28, 32, 53, 57, 78, 82, 103, 107, 128, 132, 153, 157, 178, and 182 min. B
through E, Independent averaged experiments: The plate was tilted at
t = 5 min by the angle indicated in the figures and turned back to
vertical at t = 30 min. All traces are averages of five.
SDs are given at t = 4, 7, 29, 32, and 42 min. F,
Light yields produced by stimulation with different angles of
displacement (i.e. integrated areas from t = 5-30 min under the
curves shown in B-E minus background).
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Possible Relationship of Graviresponse in
[Ca2+]c with Auxin
N-(1-Naphthyl) phthalamic Acid (NPA) and 2,3,5-tri-iodo
benzoic acid (TIBA) are inhibitors that have been used for many
years to influence the polar transport of auxin and inhibit gravitropic responses (Katekar and Geissler, 1980 ). Reorientation of growth induced
by asymmetric gravity stimulation is in part the result of modified
auxin movement and normally commences with a lag period of about 15 to
20 min. On this basis, we reasoned that NPA and TIBA should have no
effects on the gravistimulated changes in luminescence that have
finished by this time.
Seedlings were pretreated with NPA and TIBA and the luminescence
response to a 135° displacement measured (Fig.
6). Both inhibitors had a substantive
effect on both components of the luminescence response, the spike and
the shoulder.

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Figure 6.
Effect of auxin transport inhibitors on the
[Ca2+]c response after
gravistimulation (A-C: At t = 3 min, the plate with seedlings was
turned through 135°). A, Control: as Figure 3A. B, Pretreatment of
seedlings with 100 µM NPA. C, Pretreatment of seedlings
with 100 µM TIBA. Curve in A is average of five. Curves
in B and C are averages of four. SDs are given at t = 1.0, 3.1, 4.5, 7.0, and 10 min. D, Light yields produced by stimulation
(i.e. integrated areas under the curves shown in A-C minus
background).
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If there is a direct requirement for continued polar transport for the
gravi-[Ca2+]c response,
can auxin actually increase
[Ca2+]c in these
seedlings? We have tried for some years to obtain [Ca2+]c changes in
response to auxin application and found the responses small and very
variable (M.K. Watahiki and A.J. Trewavas, unpublished data). However,
the sporadic positive results suggested that the rate of penetration of
auxin into the tissue may limit the rate at which the ultimate
[Ca2+]c responses occur.
As a consequence, a perfusion system has now been used (Plieth et al.,
1999a ) to avoid unstirred layers and methyl-indole-3-acetic acid
(IAA) to increase penetration of the effector through cuticle and cell
membranes. With these improvements, a
[Ca2+]c response
could easily be detected (Fig. 7).
There is a lag of several minutes before luminescence starts to
increase and the single
[Ca2+]c transient induced
is unlike that shown for the gravitropic response. However, an external
treatment with auxin is unlike interruption of a continually moving
stream of auxin by inhibitors, so this may not be surprising. We also
performed control experiments with the auxin analogs
sodium-butyrate and butyrate-methyl-ester, both classified as
class 3 auxins
(http://www-z.embl-heidelberg.de:8080/ExternalInfo/wade/pub/data/auxin_data/classes.html) with no physiological hormone activity. Butyrate, as a weak acid, is
able to acidify the cytoplasm (Plieth et al., 1997 ) with the result that [Ca2+]c
increases in parallel (Plieth, 2001 ). The data (Fig. 7B) show that the
low-pH-induced [Ca2+]c
changes are small and demonstrate that there is a significant effect of
active IAA on
[Ca2+]c.

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Figure 7.
[Ca2+]c in
response to auxin and auxin-analogs in 5-d-old Arabidopsis seedlings
expressing aequorin in the cytoplasm and reconstituted in vivo with
cp-CTZ. Seedlings were placed in a perfusion cuvette. The effector was
given at t = 30 min and washed out at t = 90 min as indicated
by the black bar. A, Upper trace, 1.0 mM IAA-methylester;
lower trace, 0.1 mM IAA-methylester. B, Upper trace, 1.0 mM Na-butyrate; lower trace, 1.0 mM
butyrate-methylester. All experiments were performed in KCl,
MgCl2, and CaCl2 0.1 mM each with 1.0 mM MES/NaOH at pH = 5.7. All traces are averages of five. SDs are given at t = 20, 40, 60, 80, 94, and 120 min.
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Effect of Clinostat Rotation on
[Ca2+]c
The clinostat has been used for over 100 years to try to simulate
weightlessness on the earth's surface. However, the use of the
clinostat has generally fallen out of favor because of undesired side
effects and an appreciation that plant growth may be different in true
weightlessness compared with a clinostat treatment (Sievers and
Hejnowicz, 1992 ; Hoson et al., 1997 ).
We reasoned that if a single rotation initiates a single initial spike
of [Ca2+]c, then
continuous rotation of seedlings grown on a vertical plate might
initiate a series of spikes, perhaps with a maximum each time
seedlings reached 135° and the shoulder to the
[Ca2+]c signal shown in
Figures 2 through 6 is eliminated. Also, if a clinostat abolishes
gravisensing altogether with seedlings grown on a horizontal plate
(i.e. "true clinostating" = "axial rotation"), then the typical
response should appear when the motor is switched off, giving the
gravitational force opportunity to take effect on the plants. Thus,
this might provide a useful tool to investigate the cellular origin of
both spike and shoulder further.
The wheel (Fig. 1) was connected to a motor and used as two-dimensional
clinostat rotating at low speed. We applied a rotation speed of 3 rpm
and switched the motor on and off every 30 min. Figure
8 shows the effect of permanent rotation
on luminescence. Surprisingly, there was no significant luminescence
yield when seedlings had been grown on a horizontal plate leading to
axial rotation ("screwdriver rotation") when mounted on the wheel
(Fig. 8, A and B, lower traces). However, luminescence signal with
permanent rotation of seedlings grown on vertical plate
("hands-of-a-clock rotation") was a sustained increase rather than
a transient (Fig. 8, A and B, upper traces). This information suggests
that the clinostat results in permanent stimulation of the seedlings
when rotating nonaxially. The large initial spikes seen in Figures 2
through 6 are still present when the motor is switched on, but are
lacking when switched off. The dip in the luminescence when the motor
is switched off (lower traces in Fig. 8, A and B) indicates that axial
rotation ("true clinostating") is sensed and that some Ca2+ pumping is going on.

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Figure 8.
Clinostat experiments with 4-d-old Arabidopsis
seedlings expressing aequorin in the cytoplasm. The plate was mounted
on a rotatable sample holder with horizontal axis (i.e. two-dimensional
clinostat). A motor placed outside the measuring chamber was connected
with the sample holder by a timing belt (see Fig. 1). Rotation speed of
the agar plate with seedlings was adjusted to 3 rpm. Motor was switched
on and off every 30 min as indicated by the bar. Upper traces,
[Ca2+]c responses to
rotation of seedlings grown on vertical agarplate (i.e.
"hands-of-a-clock" rotation). Lower traces,
[Ca2+]c responses
to rotation of seedlings grown on horizontal agarplate (i.e. axial
"screwdriver" rotation). Curves are averages of six.
SDs are given at t = 10, 20, 32, 40, 50, 62, 70, and
80 min. B is magnification of A.
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DISCUSSION |
The information reported here indicates that a gravitropic
stimulus does induce changes in
[Ca2+]c. There are
several possible reasons why
[Ca2+]c changes induced
by reorientation of plants have not been detected so far: Legue et al.
(1997) used the fluorescent calcium indicator dye indo-1, which very
likely dampens small calcium transients (Bormann et al., 2001 ) because
of slow dissociation (or "off") rates. Indo-1 has a high
Ca2+ affinity (half saturation at 250 nM; Grynkiewicz et al., 1985 ) compared with cp-aequorin
(half saturation at 400 nM; Fig.
9A), which might influence cellular
[Ca2+] transients substantially. Here, we used
aequorin, which emits light only when Ca2+ is
bound. It is not the balance of Ca2+-bound and
unbound indicator that reports [Ca2+] as is the
case with fluorescent dyes. As a consequence, aequorin is consumed
while reporting [Ca2+] (no dissociation
reaction). Therefore, aequorin luminescence has an extremely high
signal to background ratio that allows detection of even tiny
[Ca2+]c changes and/or
[Ca2+]c transients in a
few responding cells embedded in non-responding tissue. Finally, with
this method, the integrated signal of several hundreds of seedlings is
obtained at once, whereas Legue et al. (1997) focused on small parts of
a root from a single plant with each experiment. Thus, we obtained a
global [Ca2+]c signal at
the price of less spatial information (i.e. no information about origin
and/or location of the
[Ca2+]c transient in the
seedling). So, either the aequorin technique is sensitive to a pool of
calcium that was obscured or not measured in the previous study, or it
is measuring changes in calcium in a different part of the seedling
than was measured by Legue et al. (1997) . To find the origin
and/or location of
[Ca2+]c transients
produced by gravistimulation, one can express aequorin in certain
tissues or cells (e.g. columella cells, pericycle cells, and bundle
sheath cells; Kiegle et al., 2000 ; Plieth, 2001 ; J. Love, personal
communication), to make the indicator report just from these
tissues.

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Figure 9.
Differences between native aequorin and
cp-aequorin. A, Relationship between [Ca2+] and
luminescence (data taken from Shimomura et al., 1993 , and fitted with
sigmoidal Bolzmann fit). B, In vivo reconstitution of aequorin in the
cytoplasm of Arabidopsis roots with native CTZ (dark line) and cp-CTZ
(light line). Addition of CTZ at t = 0.5 h. Absolute
luminescence (×10,000) is given in B, which is luminescence of each
integration interval divided by total luminescence produced by the
specimen. Relative luminescence (×10,000) is given in all other
figures, which is luminescence of each integration interval divided by
luminescence still remaining in the specimen. The characteristics of
the fitted curves in A are: , native aequorin, 50% midpoint of 5.9 pCa, background of 6.8 log quanta s 1;
and , cp-aequorin, 50% midpoint of 6.4 pCa, background of
7.8 log quanta s 1.
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Two characteristics noted in the data here are an initial
[Ca2+]c spike followed by
a much longer shoulder of luminescence that peaks about 90 s after
gravitropic stimulation has been induced. However, rapid single spikes
are characteristic of mechanical stimuli such as touch or wind but as a
luminescence spike they rarely last more than 5 s (Knight et al.,
1991 , 1992 ). However, the luminescence spikes observed here are 20 to
25 s (Figs. 2 and 3). Nevertheless, gravitropic stimulation can be
interpreted as a kind of inside-out mechanical stimulation (Trewavas
and Knight, 1994 ; Sinclair et al., 1996 ). So, the gravity-induced
[Ca2+]c spikes might be
part of a group typical for mechanical stimuli-like touch (Knight et
al., 1991 ), wind (Knight et al., 1992 ), and raindrops (M. Viry-Moussaïd and A.J. Trewavas, unpublished data). As
Figure 8 shows, even permanent rotation gives rise to only one initial spike. The size of the spike is also influenced by NPA and TIBA (Fig. 6), but does not appear to experience significant adaptation (Fig. 4). If the specificity of these two inhibitors NPA and TIBA can
be believed (Katekar and Geissler, 1980 ), then the
[Ca2+]c signal
underpinning the spike may be related to auxin movement. Does this
indicate that changes in auxin flux are more rapid than previously thought?
There are two parameters used in gravitropic experiments that might
relate to those gravi-induced
[Ca2+]c. The presentation
time, that is the shortest time to elicit a graviresponse, can be as
small as 12 s (Volkmann and Sievers, 1979 ; Hejnowicz et al.,
1998 ); 20 s has been measured for Arabidopsis (Kiss et al., 1989 ).
The perception time, in contrast, is the minimum period necessary for
perception of a stimulus even though a response cannot be detected. It
can be deduced using intermittent stimulation on a clinostat;
periods as short as 0.5 s have been reported (Volkmann and
Sievers, 1979 ). The initial gravi-induced [Ca2+]c spike might then
be related to these early steps in gravitropic sensing. Figure 3
indicates that the size of the spike is smaller with a complete
rotation of seedlings within a 5-s period, compared with the maximum
amplitude of spike obtained when seedlings are left at 135°. A longer
gravistimulation period than 5 s is necessary for a full
[Ca2+]c spike and could
be related to the presentation time. Because starchless mutants exhibit
a much longer presentation and perception time (Kiss et al., 1989 ),
incorporation of aequorin into several of these mutants should help
clarify the nature of this relationship.
The second "shoulder" response noted here is a much more gradual
and prolonged [Ca2+]c
transient lasting about 15 min and peaking within 90 s (Figs. 2
and 3). Asymmetric growth generally starts within 15 min and again
there might be significance in the time at which the shoulder transient
finishes and asymmetric growth commences. However, a similar transient
is induced when the seedlings are turned back to the vertical position,
although the response is generally smaller. These data and those on
subsequent restimulating again to 135° (Fig. 4) suggest some
permanent modification in the cellular signaling system, reducing the
size of this response. From this, we conclude that it is likely that
these two facets of
[Ca2+]c response, spike
and shoulder, may have either different cellular or subcellular origins
because the spike shows no apparent adaptation. The shoulder
[Ca2+]c component does
seem to be dependent on the angle of gravitropic stimulus, showing a
maximum amplitude at 135° and a shorter total transient time at
45°. One attractive possibility that we are currently investigating
is that this second
[Ca2+]c shoulder could
represent movement of amyloplasts displacing endoplasmic
reticulum, from which
[Ca2+]c is then released.
The time required for amyloplast sedimentation of 6 to 12 min (Audus,
1969 ; Yoder et al., 2001 ) is in good agreement with the total transient
time of the [Ca2+]c
shoulder reported here.
It can be argued that reorientation of seedlings gives rise to changes
in sustained mechanical stresses in the tissues because of their
weight. This could also initiate changes in cytoplasmic calcium.
Although we cannot dismiss this possibility, neither do we have
evidence to support it. The fact that the angle at which the increase
of [Ca2+]c is maximum is
135° (Fig. 5) suggests that the gravitropic response is the main
cause for the [Ca2+]c
increase. Mechanical stress is more likely to yield a maximum [Ca2+]c transient at
90° and sustained mechanical stress usually gives rise to a sustained
[Ca2+]c increase (Fig. 8;
C. Plieth and M.R. Knight, unpublished data). Therefore, the more
attractive working hypothesis is that the shoulder
[Ca2+]c component is more
likely related to movement of amyloplasts.
The data in Figures 6 and 7 suggest that there might be a significant
relationship between auxin and
[Ca2+]c. Applied auxin
can influence [Ca2+]c
directly (Fig. 7) and NPA and TIBA both inhibited
[Ca2+]c transients
substantially (Fig. 6), but there is no selective inhibition of either
the initial spike or the longer shoulder transient. Taken at their face
value, might modification of polar auxin transport occur much earlier
after gravistimulation than commonly supposed? Older models of
modification of auxin transport suggest a fairly direct relationship
between auxin movement and amyloplast sedimentation. However,
whereas both inhibitors are known to impair auxin transport, other side
effects could account for the inhibition observed here (Ross, 1998 ).
Geldner et al. (2001) recently demonstrated that localization of the
auxin efflux carrier candidate PIN1 is maintained by rapid trafficking
between plasma membrane and endosomal compartments. This cycling (i.e. internalization and polar redistribution) is interrupted in the presence of TIBA, showing that auxin transport inhibitors generally interfere with membrane-trafficking processes. Hence, it is
conceivable that treatment with either inhibitor eventually damages
sensitive cells so they are no longer able to respond to gravity.
Moreover, TIBA supposedly acts as a weak auxin (Katekar and Geissler,
1980 ), but treatment often reduces the total auxin present in the
tissue (Goldsmith, 1969 ). Finally, TIBA reacts with sulfhydryl groups so side effects are likely, complicating interpretation. The recent isolation of mutants in which auxin transport is impaired (Lomax, 1997 ;
Müller et al., 1998 ) offers a way forward if aequorin can be
incorporated into such mutants.
However, the time when auxin redistribution is believed to commence has
been estimated a number of times and it is thought that there is a lag
of about 10 min in some tissues and even longer in others (Parker and
Briggs, 1990 ). If these times are correct (and they are usually results
obtained on shoots rather than roots), then the second long
[Ca2+]c transient
described here must be completed before auxin redistribution commences.
In that case, our data can only conclude at the best that continued
auxin movement may play a role for gravi-induced changes in
[Ca2+]c. However, in some
tissues, a change in sensitivity to auxin has also been detected
(Rorabaugh and Salisbury, 1989 ) and with clear adaptation of the
[Ca2+]c, suggesting some
more permanent change has happened after the first gravitropic rotation
(Fig. 4), a relationship between these two events may be more probable.
Redistribution of Ca2+ in the wall after
gravitropic stimulation has been reported in which a higher wall
Ca2+ is found in the slower growing half of the
tissue (Björkman and Cleland, 1991 ; Lee et al., 1983a , 1983b ;
Slocum and Roux, 1983 ). Some relationship between wall
Ca2+ redistribution and changes in
[Ca2+]c is certainly
possible and perhaps could be expected. Björkman and
Cleland (1991) report that Ca2+ redistribution
takes 10 min to start in maize roots but examination of their data
suggests 5 min might be the real time of initiation. Furthermore, they
show that the wall gradient may be essential for gravitropic curvature
because it can be inhibited by EGTA derivatives or by fusicoccin.
Because wall [Ca2+] is definitely regulated by
the cell through [Ca2+]c
(Trewavas and Malhó, 1997 ), a change in
[Ca2+]c could alter
wall [Ca2+] in turn.
However, there is a discrepancy in time. The shoulder
[Ca2+]c changes described
here peak between 1 and 2 min; compare this with the 5- to 10-min
period for wall Ca2+ change in maize.
However, Arabidopsis roots are much thinner than maize roots and wall
[Ca2+] events may reach their target much
quicker. A relationship between [Ca2+]c and wall
[Ca2+] remains a viable possibility and
Arabidopsis seedlings expressing aequorin in the wall are currently
being used to probe this possibility.
 |
MATERIALS AND METHODS |
Plant Material
Transgenic Arabidopsis
(http://plantpath.wisc.edu/~afb/protocol.html) of biotype background
Columbia-0 expressing cytosolic apoaequorin under the control of the
cauliflower mosaic virus promoter 35S were used for
[Ca2+]c measurements (Knight et al., 1997 ).
Five hundred to 1,000 vapor-sterilized seeds
(http://www.cropsci.uiuc.edu/faculty/bent/additions/vapster.html) were sown on sterile 1.2% (w/v) agar (no. A1296,
Sigma-Aldrich, St. Louis) in 5-cm-diameter petri dishes (Bibby
Sterilin Ltd., Stone, Staffs, UK). Agar was supplemented with
0.5× Murashige and Skoog medium (no. M0222, Duchefa, Haarlem,
The Netherlands), 1% (w/v) Suc (no. 10274, BDH, Poole, UK) and
adjusted with NaOH to a pH of 5.8. The plates were sealed with porous
tape (12.5-mm surgical tape, Micropore, St. Paul), incubated at
4°C in the dark for 2 to 4 d for vernalization, and subsequently
cultivated in the growth room at 21°C with 16-h photoperiod. To give
a stand-alone support for vertical cultivation, plates were clipped
with 5-cm fold-back clips. Whole plates with seedlings grown on the
agar surface were used for experiments 2 to 6 d after germination
where not stated otherwise.
Reconstitution of Aequorin
Reconstitution of aequorin with CTZ was performed in vivo
essentially as described previously (Knight et al., 1997 ). However, cp-CTZ (no. C-14260, Molecular Probes, Eugene, OR) was used
instead of native CTZ (Prolume Ltd., Pittsburgh;
http://www.nanolight.com/nanofuel.htm). In brief, seedlings grown
vertically on agar surface were covered with 2.5 mL of solution for 4 to 6 h. Therefore, cp-CTZ was dissolved first in methanol to give
a 1 mM stock solution and then added to water to give a 10 µM solution for reconstitution. Calibration curves for
luminescence against Ca2+ are shown in Figure 9A.
[Ca2+]c Measurements
For [Ca2+]c measurements, whole plates
were mounted vertically on a purpose-built rotatable stage (Fig. 1) in
a light-tight sample housing in front of a PMT (model 9829A,
Electron Tubes Ltd., Middlesex, UK). The stage could be rotated
by a rubber timing belt, either by hand or by a motor.
To avoid mechanical stimulation by external vibration and by the
built-in cooler fan, the Peltier PMT housing (FACT50, Electron Tubes
Ltd.) was replaced by a lab-made dry ice cooling housing. The
use of solid CO2 also improved noise reduction by cooling the PMT down to 60°C. The luminometer chamber was constantly aerated with ambient air (19.5°C ± 1.0°C) to avoid anoxic
stress and cooling of the specimen. Aequorin luminescence counts were integrated every 5 or 12 s. For reasons discussed below, relative luminescence is given in all curves instead of
[Ca2+]c.
Treatment with Inhibitors
TIBA (no. T5910, Sigma-Aldrich) and NPA (no. N0067, TCI,
http://www.tciamerica.com) were dissolved in dimethyl sulfoxide
to give a 100 mM stock solution and then added together
with cp-CTZ (see above) to water to give 100 µM final
concentration in reconstitution medium. Medium (2.5 mL) was used to
overlay young seedlings in a petri dish for 4 h.
Treatment with Auxin
For auxin treatment, 4-d-old seedlings grown on vertical agar
were used, reconstituted for 4 to 6 h with cp-CTZ (no. C-14260, Molecular Probes), and placed in a perfusion cuvette as described by
Plieth et al. (1999a) . The cuvette was constantly perfused with
aerated, buffered standard medium containing 0.1 mM each KCl, CaCl2, and MgCl2, and 1.0 mM
MES/NaOH at pH of 5.7. Treatment of auxin was achieved by switching
auxin containing standard medium into the perfusion stream. The
latter was prepared from 1 M stock of IAA-methyl
ester (no. I9770, Sigma-Aldrich) dissolved in dimethyl sulfoxide.
Calcium Sensitivity of Native Aequorin versus
cp-Aequorin
We used the synthetic luminophor cp-CTZ (Shimomura et al., 1993 ;
no. C-14260, Molecular Probes;
http://www.probes.com/servlets/datatable?id=32122&item=2944) to
reconstitute aequorin in vivo in Arabidopsis. The binding constant of
cp-aequorin is pKCa 6.4 compared with
pKCa 5.9 of native aequorin as calculated by
sigmoidal fit (Fig. 8A). This means that cp-aequorin has a 3.16 times
higher Ca2+-binding affinity. Hence, cp-aequorin produces
about 10 times more steady-state luminescence with usual resting level
of [Ca2+]c (i.e. about 50-150
nM) and is able to report tiny changes in [Ca2+]c with higher accuracy (Baum et al.,
1999 ). The higher steady-state luminescence in unstimulated plants
enabled us to detect calcium signals lower than the normal steady-state
level as is the case with wind-stimulated seedlings (Figs. 2B and 3D).
These "undervalues" were impossible to detect in earlier studies
because of the lower signal to noise ratio produced by native aequorin.
Calculation of the Relative Luminescent Yield
We found cp-aequorin in the seedlings to be more unstable
compared with native aequorin (Fig. 9B), possibly as a result of its
higher sensitivity to the resting level of
[Ca2+]c. Although we can calibrate
cp-aequorin "in vitro" (Fig. 9A), attempts to do this "in vivo"
presented major difficulties.
The normal tissue calibration for aequorin assesses the amount of
aequorin at the end of the experiment and sums the total luminescence
emitted during the experimental period so that luminescence values can
be converted to [Ca2+]c. The calculation is
based on the relative luminescence yield which is the ratio of
luminescence counts obtained per second from the PMT divided by the
counts still remaining in the system at each time point (Knight et al.,
1997 ; Baum et al., 1999 ).
This calibration and calculation of changes in
[Ca2+]c assumes that every cell responds
equally. This is not even the case for cold shock (Wood et al., 2001 )
and is less likely for gravitropic phenomena in the root. Therefore, we
depicted results in units of relative luminescence (i.e. relative
luminescence yield × 10,000). Because it is evident that only a
few specialized cells respond to gravistimulation (Blancaflor et al.,
1998 ; Tasaka et al., 1999 ), the [Ca2+]c
amplitude in these cells may well be 50 nM or even larger. With the perfusion experiments (Fig. 7), however, we attempted calibration with the assumption that all cells responded equally and
simultaneously to the effector to have at least a rough estimate.
 |
ACKNOWLEDGMENTS |
We are grateful to Michael Brix (Physics Department Workshop,
Kiel University, Germany) for manufacturing the luminometer sample
housing and to George Steadman and Alex Harower (Institute of Cell and
Molecular Biology Workshop, University of Edinburgh) for
manufacturing the rotatable sample holder and the dry ice-cooling housing for the PMT. We also thank anonymous referees for
helpful suggestions.
 |
FOOTNOTES |
Received November 6, 2001; returned for revision December 17, 2001; accepted January 30, 2002.
1
This work was supported by the European
Community (grant no. BIO4-CT97-5080 to C.P.).
*
Corresponding author; e-mail cplieth{at}zbm.uni-kiel.de; fax
49-431-880-4368.
Article, publication date, and citation information can be found at
www.plantphysiol.org/cgi/doi/10.1104/pp.011007.
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© 2002 American Society of Plant Physiologists
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