A New Porometer Based upon the Electrical Current Produced by Guard Cells Author(s): D. J. F. BOWLING Source: Journal of Experimental Botany, Vol. 40, No. 221 (December 1989), pp. 1407-1411 Published by: Oxford University Press Stable URL: http://www.jstor.org/stable/23691992 Accessed: 26-05-2015 11:34 UTC
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Journal
of Experimental
Vol.
Botany,
40, No.
221,
December
pp. 1407-1411,
1989
upon the Electrical by Guard Cells
A New Porometer
Based
Current Produced D. J. F. BOWLING of Plant
Department
26 June
Received
and
Soit Science,
University
St. Machar
of Aberdeen,
Drive,
Aberdeen
AB9
UK
2UD,
1989
ABSTRACT when Stomatal guard cells extrude protons An instrument opening. degree of stomatal The performance of the new of porometer.
the stomata has
been
open.
This
developed has been
gives rise to an electrical to measure this leaf surface
current current
which
is proportional to the is, in effect, a new type available diffusion
which
with that of a commercially porometer compared for all the species conductance was observed between leaf surface current and stomatal relationship in particular, its small over the diffusion porometer, It is concluded that the instrument has several advantages investigated. in the field. suitable for use and simplicity of operation, it making especially and
porometer
Key
words:
a close
Leaves,
stomata,
electrical
currents,
size
porometry.
INTRODUCTION There
are two basic
of measuring stomatal and porometry. In the direct
methods
opening, direct observation method stomatal aperture is measured under the microscope using a micrometer eyepiece. This gives a value for the aperture in micrometres but is tedious and timeat a time need to be
as at least 30 stomata
consuming measured to
obtain a statistically significant result. size of the pore provides only limited the Furthermore, information about the diffusion capacity of the stomata. Porometers
have
been
developed
to
overcome
the
disad-
vantages of the direct method. They measure gas transfer through the open stomata and can be divided into two types, viscous flow and diffusion. The firstviscous flow porometer was introduced in 1911 by Darwin and Pertz. In this device air was pulled through the leaf by reduced pressure created by a water column. A modification of their instrument incorporating a double manometer system was described by Gregory and Pearse
(1964) and Van Bavel, Nakayama, and Ehrler (1965). This instrument measures the diffusion of water vapour out of the stomatal pores using a relative humidity sensor. The humidity sensor is housed in a leaf cup which can be
clamped onto the leaf. The sensor and the air in the cup is dried to a pre-determined humidity level by passing dry air through the leaf cup and after that the time required for transpiration to bring the humidity up to some pre determined indication
point is measured.
of
transpiration
rate
This time-interval is an and
leaf
resistance
to
water vapour transfer. The device is calibrated using a plate with perforations of known diffusion resistance and a flow of water vapour saturated air. Versions suitable for use in the field have been developed by Byrne, Rose, and Slatyer (1970) and Stiles, Monteith, and Bull (1970). The latter instrument is commercially available as the Delta-T Devices Automatic Porometer Mark 3. Another diffusion is the Li-cor 1600 porometer commercially available
in 1934. This was followed in 1951 by the Wheatstone bridge porometer of Heath and Russell in which flow
which works on a steady-state null balance principle, Water vapour diffusion porometers have proved to be the most useful instruments available up to the present
needle
time and have largely replaced the viscous flow type. They have the advantage that, because they measure total gas exchange, i.e. leaf conductance, the results relate directly to the phenomenon being studied. Furthermore, measure ments by diffusion porometers can be used to calculate stomatal aperture, provided certain anatomical character
from a split air-stream is balanced between the leaf and a valve by adjustment with a single manometer. These instruments were relatively complicated and un-
wieldy and so this led to the development of more simple, portable, viscous flow porometers for use in the field (Bierhuizen, Slatyer, and Rose, 1965; Weatherley, 1966). The diffusion porometer was introduced by Wallihan ©
Oxford
University
Press
1989
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1408
New Porometer
Bowling—A
istics are known (Jarvis, Rose, and Begg, 1967). The main of diffusion porometers is that they are disadvantage in their construction, containing components complicated such
as
means
RH
thermistors, that
are
they
leaf
and
to build,
expensive
care in their operation. between
timers
sensors,
Also
porometer
and
pumps.
bulky
and
a good
seal
This require
is required
cup.
The purpose of this paper is to introduce a new type of The
porometer.
new
instrument
is
based
on
a
principle
entirely different from those of the viscous flow and diffusion types already described and avoids many of their It is based on the discovery that a small disadvantages. electrical current is produced in the leaf epidermis which is proportional to the stomatal aperture (Bowling, Edwards, and Gow, 1986). The current appears to be due to a flow of protons
from
emanating
the
cells
guard
but
not
Fig. 2. Circuit of the current-voltage
used in the instrument.
converter
from
the other cells in the epidermis (Edwards, Smith, and Bowling 1988). Evidence suggests that it is due to the activity of a proton efflux pump which plays a fundamen tal role in the mechanism of the stomatal opening (Zeiger, of this current should, therefore, 1983). Measurement an
provide
indirect
MATERIALS In
place diffusion current used
measure
AND
of
the
in some
moistened
used
cup
in
viscous
flow
and
was used to collect the pad surface. It consisted of a filter of the type automatic Medical Electronics, (Gilson pipettes
Villiers-le-Bel, A diameter.
France) sintered
a
aperture.
METHODS
conventional
porometers from the leaf
of piece electrode
of stomatal
contact
held
in a
tubing made contact
with
of tubing was held
length electrode
Ag/AgCl fitted inside
the
first
the bottom
with
tap water and 0-5 cm2 of contact area. It could
so
that
of suitable in
another
the
tip of the of the filter. The filter, to the leaf provided
adpressed be fitted into a clip made from a modified hair grip for 'hands-ofT of fixing to the leaf. A diagram the contact in Fig. 1. As long as the contact pad is shown pad was saturated it did not matter whether distilled water or tap water For not
was
used
the same
as
the currents
reason
the degree to be critical.
appear The current
picked
being measured of pad pressure
up from the contact converter. A simple
were
so
using a current-voltage and an operational was required amplifier (CA3140) together with a resistor an output of 1 mV nA_1 (1 Mohm) provided was connected to a digital panel meter (RS (Fig. 2). The output
and the completed in Components, Corby, England 258-041) strument housed in a hand held case (RS The instru 507-983). ment was powered batteries 591 by two 9 V rechargeable (RS pad was con cable and the
—silicone tubing -rubber tubing
2mm connector pin Fig.
1. Diagram porometer.
to show the construction
of the contact
1. The new porometer
complete
with its contact
pad and earthing
circuit
connected to a completed by a similar length of cable rod. A photograph of the complete instrument is earthing in Plate shown 1. brass
The the size
with dimensions instrument, of a hand-held multimeter.
of 15 x 8 x 5 cm, was about only one operational
It had
an on-off switch. The meter was set to read zero when control, the electrodes were disconnected. With the contact pad on the leaf and the brass earthing rod inserted into the soil close to the roots
of the plant the maximum was 2 V (2 ju.A). reading possible the reading 1 ¡j.A. There was a small rarely exceeded in the instrument case where the electrodes and compartment In practice cables
could
be stored
Calibration T
Mark
when
not in use.
of the instrument
3 diffusion
was
carried
(Delta-T porometer of four species, two
out against
a Delta
Devices,
Cambridge, two dicotyledonous,
Leaves England). at 18-24 °C monocotyledonous, growing in pots in a greenhouse were sampled at different times of the day for a period at random of 5 d. Readings from the same
-filter
sintered Ag/AgCI
rod.
small.
on the leaf did
pad was measured circuit was all that
and weighed less than 300 g. The contact 089) nected to the instrument by a length of flexible
Plate
pad used in the
from both porometers were taken consecutively part of the leaf with that from the Delta-T instrument taken first. Current was plotted being (jj.A cm-2) stomatal conductance was also against (cm s~ '). The instrument calibrated in one stomatal of the species against aperture A {Commelina communis). then the epidermis stripped
of 30 stomata measured apertures number of similar measurements were at random
at different
times
was taken and reading of the leaf and the
porometer from that
in one
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part under
taken
day.
A microscope. from leaves chosen
the
Bowling-—A New Porometer
1409
RESULTS The relationship between current and stomatal conduc tance for three species, Commelina communis, Tradescan tia virginiana and Pelargonium zonale is shown in Fig. 3. There was good correlation between the data (r=0-86) and the line fitted by regression analysis had a slope of 0-64. This indicated that the current could be used as a measure of stomatal
conductance
and that the relation
ship was linear. Also, all three species investigated ap peared to behave in a similar manner. Measurements were also carried out on Vicia faba and the results shown in Fig. 4. It can be seen that a similar relationship was obtained but with a slightly higher correlation coefficient (0-95) and a higher slope (0-69). The measurements in
Figs 3 and 4 were taken throughout the day between dawn and dusk and so the relationship between current and conductance appeared to be independent of light levels. In steady-state conditions, therefore, there appeared to be a linear relationship between leaf current and stomatal conductance. It was necessary to find out if this relation conditions were ship remained when environmental changing rapidly. A potted plant of Commelina was taken from the greenhouse at midday and placed in a dark cupboard in the laboratory for 3 h. Current and conduc tance measurements were made for 10 min before the plant was taken out of the dark and placed on the bench in bright sunlight. Measurements were continued with
readings being taken 2 min before those for current on the same part of the leaf. Different leaves of conductance
0.6
0.4
0.2
Stomatal Fig. 4. Calibration
of the porometer
1.0
0.8
conductance
1
cm s
for Vicia faba.
similar age were used for each pair of readings. The results are shown in Fig. 5. The scatter of the points appeared to be due to sampling error. The behaviour of the stomata varied markedly from place to place over the leaf surface and it was not easy to sample exactly the same location each time. The stomata began to open almost immediately after the plant was transferred to the light as shown by the rise in stomatal conductance.
Leaf
current
rose
at
the
approximately
same
rate indicating that it was just as responsive to the changing conditions as the stomatal conductance. The relationship between current and stomatal conduc tance during stomatal closure was also investigated. Figure 6 shows the results from an experiment in which two Commelina plants were left in sunlight at 20 °C in the laboratory.
Current
measurements
were
made
on
one
plant
and conductance
followed on the other. In order to reduce error the same part of the leaf was tested at 1 min sampling or 2 min intervals. After a short time the plants were transferred to a dark cupboard. There was rapid stomatal closure as shown by the fall in leaf conductance and it can be seen that the current responded
to stomatal
closure
equally rapidly. Alternating periods of light and dark produced results similar to those shown in Figs 5 and 6. The relationship between leaf surface current and sto matal aperture was investigated in Commelina. Current measurements were made at random on the leaves of a 0.2
0.4
0.6
Stomatal
conductance
0.8 cm s
1.0 -1
Fig. 3. Calibration of the porometer conductance, against stomatal Closed for three species. measured circles, by diffusion porometer, Commelina; closed triangles, Tradescantia\ closed squares, Pelargonium.
plant standing in the laboratory in sunlight. The epidermis was removed and stomatal immediately apertures measured. Figure 7 shows that there was a linear relation ship between current and aperture, with each increase by a micrometre in aperture being accompanied by an incre ment in current of approximately 01 /aA cm-2.
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1410
New
Bowling—A
Porometer light
40
50 Time minutes
measured by a diffusion porometer (open circles) and current output measured Fig. 5. Stomatal conductance the lower surface of the leaves of a plant of Commelina communis transferred from darkness to light.
10
12
14
16
18
20
22
by the new porometer
(closed
circles) of
24
Time minutes Fig. 6. The trend in current output (closed circles) and conductance Current and (open circles) for the lower leaf surface of Commelina. conductance were measured on two separate plants which were trans ferred from light to dark.
DISCUSSION The results establish that the leaf epidermis current pro a
vides
reliable
measure between
relationships tance
and
current
of the
and
stomatal
Therefore,
would
diffusion
as
opening.
Current
measurement sion
is very
a
of
sensitive
to
be
valid
that
as
the
gaseous during over
advantage
diffusion in that gaseous changes
in
the
diffu
through
temperature
changes of relative humidity in the porometer cup, whereas current is likely to change only by the direct effect of leaf temperature on the metabolism of the guard cells. The
new
porometer
provides
a
way
of
measuring
stomatal activity depending on neither mass flow nor diffusion. It avoids the problem of changing internal tissue resistance
because
inherent
with
viscous
flow
porometers
aperture
pm
Fig. 7. The relationship between current output and storaatal for the lower surface of leaves of Commelina communis.
aperture
activity.
conductance
has
Stomatal
linear
conduc
indicate
as
stomatal
measurement
of gaseous
stomatal
aperture to
appear
measure
The
opening. and
attribute of stomatal
current is a fundamental it
stomatal current
and,
it follows guard cell activity directly, it measures
stomatal which The
conductance measure
per
the
instrument
se
unlike
had
diffusion
of the
conductance several
other
porometers
leaf.
advantages
over
the
diffusion and viscous flow types. First, it was completely portable because of its simple design. Second, the instru ment could be set up and a reading obtained within 30 s without the need for any preliminary adjustment. There was, surprisingly, very little outside interference with the current
readings
and
there
was
usually
very
little
drift,
with the reading often reaching a steady value well within 30 s. Third, the instrument did not require to be calibrated before
each
series
of measurements.
Fourth,
by incorpora
tion of a potentiometer into the circuit it was possible to
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1411
New Porometer
Bowling—A make the instrument read directly in units of stomatal conductance.
its small size and simplicity in use. These features make it very suitable for measurements in the field. It is envisaged
It was interesting to find that the slope of the calibra tion curve was approximately the same for all the four species examined. Some more limited data were also obtained for Phaseolus vulgaris, Zea mays and Helianthus
that its underlying principle could provide a valuable new method for following the behaviour of stomata both in the laboratory and in the field.
annuus which indicated
that, they too, behaved in the same way. This consistency in behaviour occurred, pre sumably, because stomata occupy a surprisingly con
ACKNOWLEDGEMENTS The author wishes to thank Dr M. C. Edwards
for his
stant proportion of the surface area of the leaf. Meidner and Mansfield (1968) presented data which indicate that
help and encouragement during the early stages of this work and Mr Harry Cobb for assembling the instrument.
the pores of moderately open stomata of a large number of species occupy approximately 1% of the surface of the leaf. The curves in Figs 3, 4 and 6 did not pass through the origin after extrapolation indicating a residual current
LITERATURE
when the stomata were closed. This appeared to be due to electrical activity at the interface between the earthing electrode and the soil. In preliminary work platinum, copper, stainless steel and iron earthing electrodes were tried but they gave larger residual currents than the brass electrode which was eventually adopted. However, it is possible that there is also a component of the residual current which originates at the leaf surface. Edwards et al. (1988) observed that proton efflux by the guard cells of Commelina preceded stomatal opening. It would be expected, therefore, that on transferring leaves of Commelina to the light, there should be a lag between the rise in current and the increase in diffusive conduc tance as the stomata open. This lag is not apparent in the results shown in Fig. 5. The reason for this could be statistical as Edwards et al. (1988) looked at individual stomata whilst porometers sense large numbers of sto mata
at each
reading. Also the lag could have been disguised by the scatter of the results due to sampling error. On the other hand, as the diffusion porometer measures leaf conductance rather than stomatal conduc tance, it was conceivable risen
coincidently
that leaf conductance
as the leaf
surface
current
might have
rose
when
the
light was switched on. The experiments described by Figs 5 and 6 where there were rapid changes in stomatal aperture show neither an initial surge of current during stomatal opening (Fig. 5) nor an initial trough on stoma
tal closure (Fig. 6). This indicated that the relationship between conductivity and current observed under steady state conditions (Figs 3 and 4) held also during rapid changes of stomatal aperture.
To summarize, the strong points of the instrument are
CITED R.
Bierhuizen,
F.,
for
porometer
R.
Slatyer,
46, Botany, Experimental D. J. F., Edwards, currents
C.
Rose,
field
1965.
W.,
A
Journal
operation.
of
182-91. M.
Bowling,
Electrical
and
O.,
and
laboratory
and
C.,
at the leaf surface
N. A.
Gow,
of Commelina
1986.
R.,
communis
and their relationship to stomatal activity. Ibid. 37, 876-82. Byrne,
G.
F.,
C.
Rose,
diffusion
aspirated
and
F.,
D.
Pertz,
the aperture
estimating
F.
1911.
M.,
of stomata.
Society, Series B, 84, 136-54.
Edwards,
M.
Guard
cells
C.,
Smith,
extrude
G.
R.
Slatyer, Agricultural
porometer.
39-44.
Darwin,
and
W.,
and
N.,
protons
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1970.
An
Meteorology,
7,
O.,
a new
On
D.
Bowling, to
method
of
of the Royal
Proceedings
J. F.,
1988.
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and pH study using fluorescence microscopy Journal of Experimental 39, 1541-7. Botany, F. G., and H. 1934. Pearse, L., Gregory,
opening—A micro-electrodes. The
resistance
and its application to the study of stomatal move porometer ment. Proceedings Series B, 114,477-93. of the Royal Society, O. V. S., and Russell, Heath, J., 1951. The Wheatstone bridge Journal of Experimental porometer. P. J., Rose, C. W., and Begg,
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tal and
theoretical
tances
to gas
comparison
flow
leaves. through amphistomatous Agricul 103-17. 4, Meteorology, T. A., 1968. and Meidner, Mansfield, H., Physiology of stomata. London. McGraw-Hill, tural
Stiles, W., resistance
Monteith, porometer
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C. H. Bavel, 1965. Measuring 40,
Physiology, E.
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of an
aperture.
L., Plant
electric Ibid.
39,
for use in the field. New
of stomatal 34, 441-75.
use
W.
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cells.
Annual