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Plant Physiol, November 2001, Vol. 127, pp. 1204-1211
Growth in Elevated CO2 Can Both Increase and Decrease
Photochemistry and Photoinhibition of Photosynthesis in a Predictable
Manner. Dactylis glomerata Grown in Two Levels of Nitrogen
Nutrition1
Graham J.
Hymus,2
Neil R.
Baker, and
Stephen P.
Long3 *
Department of Biological Sciences, John Tabor Laboratories,
University of Essex, Wivenhoe Park, Colchester CO4 3SQ, United
Kingdom
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ABSTRACT |
Biochemically based models of C3 photosynthesis can be
used to predict that when photosynthesis is limited by the amount of Rubisco, increasing atmospheric CO2 partial pressure
(pCO2) will increase light-saturated linear
electron flow through photosystem II
(Jt). This is because the stimulation
of electron flow to the photosynthetic carbon reduction cycle
(Jc) will be greater than the
competitive suppression of electron flow to the photorespiratory carbon
oxidation cycle (Jo). Where elevated
pCO2 increases
Jt, then the ratio of absorbed energy
dissipated photochemically to that dissipated non-photochemically will
rise. These predictions were tested on Dactylis
glomerata grown in fully controlled environments, at either
ambient (35 Pa) or elevated (65 Pa) pCO2,
and at two levels of nitrogen nutrition. As was predicted, for
D. glomerata grown in high nitrogen,
Jt was significantly higher in plants
grown and measured at elevated pCO2 than for
plants grown and measured at ambient pCO2.
This was due to a significant increase in
Jc exceeding any suppression of
Jo. This increase in photochemistry at elevated pCO2 protected against
photoinhibition at high light. For plants grown at low nitrogen,
Jt was significantly lower in plants
grown and measured at elevated pCO2 than for
plants grown and measured at ambient pCO2.
Elevated pCO2 again suppressed Jo; however growth in elevated
pCO2 resulted in an acclimatory decrease in
leaf Rubisco content that removed any stimulation of
Jc. Consistent with decreased
photochemistry, for leaves grown at low nitrogen, the recovery from a
3-h photoinhibitory treatment was slower at elevated
pCO2.
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INTRODUCTION |
The majority of experimental
evidence points to a stimulation of light-saturated photosynthesis
(Asat) for C3
plants, grown in the atmospheric partial pressure of
CO2 (pCO2)
predicted for the end of this century (for review, see Drake et al.,
1997 ). In the field, increased photosynthesis in elevated
pCO2 has been shown to both increase
and decrease photochemical requirements for light-saturated electron
flow through photosystem (PS) II (Jt;
Scarascia-Mugnozza et al., 1996 ; Hymus et al., 1999 ). What basis
might there be for a variable response in electron transport when
assimilation is consistently increased?
Elevated pCO2 will stimulate the
photosynthetic carbon reduction cycle and the electron flow that
drives it (Jc). However, elevated
pCO2 will also competitively suppress
the photorespiratory carbon oxidation (PCO) cycle and the electron flow
that drives it (Jo). Whether or not there
is an increase in the demand of carbon metabolism for
Jt will depend on the net effect of these changes in Jc and
Jo. The mechanistic understanding of
C3 photosynthesis proposed by Farquhar et
al. (1980) predicts that, when pCO2 is increased, if Asat is limited by the
amount of Rubisco the stimulation of Jc
will be greater than the suppression of
Jo, and an increase in
Jt will result. This predicted increase in
Jt may not be observed where growth in
elevated pCO2 results in acclimation
of either: (a) the amount of Rubisco in the leaf, or (b) sinks for
Jt other than the photosynthetic carbon
reduction and PCO cycles. Decreased leaf Rubisco content in elevated
pCO2 will decrease both
Jc and Jo. In
addition, Jo will be competitively
suppressed by increasing pCO2. Many
studies have shown no effect of growth in elevated pCO2 on sinks for
Jt, other than carbon metabolism (Epron et
al., 1994 ; Habash et al., 1995 ; Bartak et al., 1996 ; Hymus et al., 1999 ). However, there is some evidence that growth in elevated pCO2 decreases antioxidant activity
(Polle et al., 1997 ), suggesting a possible change in potential
electron flux to a Mehler reaction.
Where elevated pCO2
changes photochemical quenching of absorbed photosynthetically active
photon flux density (PPFD), changes in non-photochemical quenching of
absorbed PPFD will result. Non-photochemical quenching
constitutes a dynamic form of photoinhibition (Baker and Ort, 1992 ;
Long et al., 1994 ; Osmond, 1994 ). At high light, if elevated
pCO2 increases photochemistry, a
decrease in non-photochemical quenching and protection against
photoinhibiton would be expected.
In this study, Dactylis glomerata was grown under controlled
environment conditions, at two levels of nitrogen nutrition. A previous
study of D. glomerata showed decreased leaf Rubisco content
with growth in elevated pCO2, but only
when nitrogen supply was limiting (Davey, 1998 ). Given this potential
to change leaf Rubisco content of plants growing in elevated
pCO2 in controlled environments, the
following two hypotheses were tested: (a) In the absence of
acclimation, elevated pCO2 will result
in a net increase in Jt because the
stimulation of Jc will be greater than the
inhibition of Jo, decreasing
photoinhibition; and (b) an acclimatory decrease in leaf Rubisco
content in elevated pCO2 will offset the stimulation of Jc,
Jo will be suppressed,
Jt will decrease, and photoinhibition will
increase in elevated pCO2.
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RESULTS |
Light-Saturated Photosynthesis
Growth in elevated pCO2
did not affect Vc,max or
Jmax in the high-nitrogen treatment (Fig.
1a; Table I), where
Vc,max is the maximal Rubisco catalyzed
carboxylation rate and Jmax the maximal
whole-chain electron transport rate. In
the low-nitrogen treatment,
Vc,max was significantly decreased, by
42%, in elevated pCO2, the reduction
in Jmax was not significant (Fig.
2a; Table I). In high nitrogen,
Asat was Rubisco limited under ambient pCO2. As a consequence,
Asat, Jc, and
Jt were significantly increased, by 86%,
73%, and 55%, respectively, for plants grown and measured at elevated
pCO2, relative to those grown and
measured at ambient pCO2 (Fig. 1a;
Table I). In the low-nitrogen treatment, acclimation to elevated
pCO2 resulted in no stimulation of
Asat and a significant decrease in both
Jc and Jt of
11% and 20%, respectively, when the comparisons at respective growth
pCO2 were made (Fig. 2a; Table I). In
high nitrogen, the suppression of photorespiration by elevated
pCO2 reduced
Jo by an apparent 16%. In low nitrogen, Jo was decreased by 57% due to
suppression of photorespiration by elevated
pCO2 and decreased Rubisco (Table I).
Neither decrease in Jo was statistically
significant.

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Figure 1.
Light-saturated photosynthesis: high
nitrogen. a, The responses of light-saturated CO2
uptake (Asat) against intercellular
CO2 concentration
(Ci) for leaves of D. glomerata
grown in high nitrogen and at either elevated (black symbols and black
lines) or current ambient (white symbols and dotted lines)
pCO2. Values of
Vc,max and
Jmax, calculated using the equations and
constants in von Caemmerer (2000) and Bernacchi et al. (2001) , were
used to fit a nonlinear regression to observed values above
(Jmax) and below (Vc,
max) the inflection of the curves. Also shown are the
supply functions for each curve (dashed line) that indicate the
operating point of photosynthesis at the growth
pCO2 for each treatment. Data points
shown are the means (±1 SE) for five replicate
leaves. Measurements were made in 21 kPa O2 and
at a PPFD of 1,300 µmol m 2
s 1. b, Jt,
Jc, and Jo
for ambient (white bar) and elevated (black bar)
pCO2 treatments were calculated for
measurements at the respective growth
pCO2 for each group of leaves using
the equations of Valentini et al. (1995) . Values shown are the means
(±1 SE) for five replicate leaves.
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Table I.
Light-saturated photosynthetic characteristics
Asat, the quantum efficiency of PSII
( PSII), photochemical quenching coefficient
(qP), and
F'v/F'm
measured simultaneously at the growth pCO2 for
ambient (35 Pa) and elevated (65 Pa) treatments.
Vc,max and Jmax were
calculated using the equations and constants in von Caemmerer (2000)
and Bernacchi et al. (2001) . Jt,
Jc, and Jo were
estimated using the model of Valentini et al. (1995) . All values are
the means (±1 SE) for five replicate plants. A significant
interaction between growth pCO2 and nitrogen was
found for each parameter measured, except Jo. As
a consequence, differences between individual means were tested using a
post hoc Tukey's test. Different superscript letters
identify means that are significantly different within that row
(P < 0.05). Asat,
Vc,max, Jmax,
Jt, Jc, and
Jo are expressed in µmol m 2
s 1. Units for PSII,
qP, and
F'v/F'm
are dimensionless.
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Figure 2.
Light-saturated photosynthesis: low nitrogen. a,
Plot of light-saturated A against
Ci for leaves of D. glomerata
grown in low nitrogen. As described previously for Figure 1. b,
Measurements of Jt,
Jc, and Jo
made at the respective growth pCO2 for
D. glomerata grown in low nitrogen. As described previously
for Figure 1.
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In the high-nitrogen treatment, elevated
pCO2 significantly increased
PSII when measurements made at the two
growth pCO2 were compared, as a
result of increases in both
Fv'/Fm' and
photochemical quenching coefficient (qP;
Fig. 1b; Table I), where
Fv'/Fm' is the
probability of an absorbed photon reaching an open PSII reaction center. In low nitrogen,
Fv'/Fm' was
significantly lower in elevated pCO2;
the decreases in PSII and
qP were not statistically significant (Fig. 2b; Table I).
Ratio of Electron Transport to CO2 Fixation
For all nitrogen and
pCO2 treatments,
PSII and
CO2 were highly correlated
(r2 = 0.74-0.82; P < 0.05) and linearly related with an intercept that was not significantly
different from zero (Table II), where CO2 and PSII are
the quantum efficiencies of CO2 uptake and of linear
electron transport through PSII, respectively. It is important that
growth pCO2 had no statistically
significant effect on the
PSII/ CO2
relationship for plants grown in either high or low nitrogen (Table
II). These relationships indicated that growth in elevated
pCO2 had not resulted in additional
sinks for Jt, such as to a Mehler
reaction.
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Table II.
Ratio of electron transport to CO2
fixation
The gradient (k) of the relationship
PSII/ CO2
was unaffected by elevated pCO2 in low nitrogen
(F1.64 = 2.1; P > 0.05) and high
nitrogen (F1.62 = 2.79; P > 0.05).
The intercept (b) was not significantly different from zero
for each plot. Low nitrogen ambient, t1.29 = 0.02, P = 0.98; low nitrogen elevated,
t1.31 = 0.95, P = 0.34;
high nitrogen ambient, t1.34 = 1.14,
P = 0.26; high nitrogen elevated,
t1.28 = 0.34, P = 0.73.
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Photoinhibition and Recovery
Fv/Fm
measured prior to the beginning of the photoperiod was unaffected
by growth pCO2 for both nitrogen
treatments (F1,16 = 0.1; P > 0.1). For all treatments,
Fv/Fm declined
during the 3-h high-light treatment at a PPFD of 2,000 µmol
m 2 s 1 (Figs.
3a and 4a).
After 3 h,
Fv/Fm was
significantly higher by 7% in elevated
pCO2 for the high-nitrogen plants
(t18 = 2.3; P < 0.05; Fig. 4a). In low nitrogen,
Fv/Fm measured after
3 h was unaffected by pCO2 (Fig.
4a).

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Figure 3.
Photoinhibition and recovery: high nitrogen. a,
Photo-inhibitory reduction in
Fv/Fm. b,
Changes in Fo during a 3-h exposure to a
PPFD of 2,000 µmol m 2
s 1. c, Recovery of
Fv/Fm
measured after 10 min dark adaption (black lines), and
Fv'/Fm'
measured under growth PPFD (dashed lines), for D. glomerata
grown in high nitrogen. Plants were grown, photoinhibited, then allowed
to recover in their growth pCO2 either ambient
(white symbols) or elevated (black symbols). Each symbol represents the
mean (±1 SE) for 10 replicate plants.
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Figure 4.
Photoinhibition and recovery: low nitrogen. a,
Photo-inhibitory reduction in
Fv/Fm. b,
Changes in Fo during a 3-h exposure to a
PPFD of 2,000 µmol m 2
s 1. c, Recovery of
Fv/Fm
measured after 10 min of dark adaption (black line), and
Fv'/Fm'
measured under growth PPFD (dashed line), for D. glomerata
grown in low nitrogen. As described previously for Figure 3.
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In high nitrogen with elevated pCO2,
60% of the reduction in
Fv/Fm had recovered
after 10 min of dark adaptation and after 1 h,
Fv/Fm had returned
to dark-adapted levels. Although the ambient pCO2 treatment similarly recovered
after 1 h,
Fv/Fm and
Fv'/Fm' after
10 min were lower than in elevated
pCO2. This difference in
Fv/Fm was
statistically significant (t18 = 3.5;
P < 0.05; Fig. 3c).
For plants grown in low nitrogen, the recovery of
Fv/Fm took between 3 and 4 h (Fig. 4c). Values of Fo
measured before and at the end of the 3-h treatment were not
significantly different in either the ambient
(t18 = 1.5; P > 0.1) or
elevated (t18 = 0.01; P > 0.1) pCO2 treatments (Fig. 4b).
Although there was no effect of pCO2
on the recovery of
Fv'/Fm' in
the low-nitrogen treatment, the initial recovery of
Fv/Fm was
significantly reduced by elevated pCO2
during the first (t18 = 3.9;
P < 0.05) and second (t18 = 3.0; P < 0.05) hours of the recovery. Given that
Fv'/Fm' was
unaffected by pCO2, the slower
recovery of Fv/Fm
should reflect an affect of pCO2 on
the dark-adapted relaxation of non-photochemical quenching.
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DISCUSSION |
This controlled-environment study confirmed the hypothesis that
elevated pCO2 decreases
photoinhibition in high nitrogen, but increases photoinhibition in low
nitrogen, at a level assumed to restrict growth. This is explained by a
greater demand for electrons in photosynthetic carbon metabolism
in the absence of limitations, and a decreased demand by both
photosynthetic and photorespiratory carbon metabolism, relative to
ambient pCO2, when resources other
than carbon restrict production.
For D. glomerata, light-saturated photosynthesis at ambient
pCO2 was limited by the amount of
Rubisco, regardless of nitrogen treatment (Fig. 1a). At high nitrogen,
elevated pCO2 had no effect on
Vc,max. Therefore, in keeping with the
theory of Farquhar et al. (1980) , elevated
pCO2 stimulated
Jc to a greater extent than it suppressed
Jo, increasing
Jt (Fig. 1b; Table I). As a consequence, when exposed to a high PPFD, the proportion of absorbed photons dissipated photochemically was increased in the elevated
pCO2 treatment, reducing
photoinhibition (Fig. 3).
For D. glomerata grown under low nitrogen supply,
acclimation of the photosynthetic apparatus significantly reduced
Vc,max (Fig. 2). The magnitude of the
acclimation was sufficient to totally remove the short-term stimulation
of Jc by elevated
pCO2 (Fig. 2). Because
photorespiration was suppressed, a similar
Asat at elevated
pCO2 to that in ambient
pCO2, was achieved with about 20%
lower Jt (Table I). If
triose-phosphate utilization (TPU) had been
limiting photosynthesis, we would have expected a similar decrease in Jt. Under conditions of TPU
limitation, Asat and
Jc will be insensitive to increasing
pCO2 and
Jo will be suppressed, and decreased
Jt and increased non-photochemical
quenching can result (Sharkey et al., 1988 ; Pammenter et al., 1993 ). In
this study, Asat of leaves grown in low
nitrogen and elevated pCO2 increased
with an increase in Ci to 150 Pa. As a
consequence, decreased Vc,max, not TPU
limitation of photosynthesis, was responsible for decreased
Jt. The nitrogen dependence of the
pCO2-dependent decrease in
carboxylation capacity observed here is consistent with other studies
of the interactive effects of growth at elevated pCO2 and nitrogen supply (Tissue et
al., 1993 ; Thomas et al., 1994 ; Curtis, 1996 ; Rogers et al.,
1996 ). Rogers et al. (1998) showed, with a related herbage grass,
Lolium perenne, that when nitrogen supply was limited there
was a loss of carboxylation capacity and Rubisco at elevated
pCO2, but not when nitrogen supply was
adequate. Partial defoliation removed this acclimatory response. This
showed that low nitrogen affected acclimation by limiting sink size
relative to source because when source size was decreased acclimation
was removed. For D. glomerata, in low nitrogen, the deceased
demand for photochemical energy was reflected in a significant depression in
Fv'/Fm' in
elevated pCO2 and therefore increased the probability of absorbed photons being dissipated as radiation-less decay from the antenna of PS II (Table I, Fig. 2). The gradient of the
straight line describing the dependence of
PSII on
CO2 was not significantly different in
elevated pCO2 for either nitrogen treatment. This suggested that growth in elevated
pCO2 did not produce significant sinks
for photochemical energy other than the photosynthetic carbon reduction
or PCO cycles, in agreement with published findings (Epron et al.,
1994 ; Habash et al., 1995 ; Bartak et al., 1996 ; Hymus et al., 1999 ).
However, there was no evidence of any significant sink beyond
photosynthetic and photorespiratory carbon metabolism at the current
ambient pCO2 in D. glomerata. In other species, notably those that bare leaves
throughout long periods of environmental stress restricting carbon
metabolism, alternative sinks for electron flow, primarily to oxygen,
are suggested to be very significant (Lovelock and Winter, 1996 ;
Cheeseman et al., 1997 ). Responses of species with these stress
tolerance strategies might be very different.
After the 3-h photoinhibitory treatment, the recovery of
Fv/Fm in low
nitrogen was slower for the elevated
pCO2 treatment. Because
Fo was unaffected (Fig. 3), the decreased
Fv/Fm was almost certainly associated with zeaxanthin-dependent quenching (Demmig-Adams and Adams, 1992 ; Owens, 1994 ; Horton et al., 1996 ). Under stress conditions, this recovery can require many hours (Demmig-Adams and
Adams, 1992 ; Fryer et al., 1995 ). The results suggest that in addition
to increasing the potential for photoinhibition, elevated pCO2 may also decrease capacity for
recovery. Hymus et al. (1999) showed that loblolly pine (Pinus
taeda) photoinhibited during winter low temperature stress
recovered more slowly when growing at elevated
pCO2. Together, these results indicate
that elevated pCO2, may decrease the
capacity of the plant to recover from stress-induced photoinhibition.
This may be part of a wider pattern of decreased stress tolerance in
leaves growing at elevated pCO2 (Lutze
et al., 1998 ; Terry et al., 2001 ).
In a study on wheat (Triticum aestivum) grown for 6 weeks under optimal conditions, without an acclimatory loss of Rubisco, both A and total non-cyclic electron flow through PSII were
enhanced by elevated pCO2 at high
light (Habash et al., 1995 ). A similar study on ryegrass (Lolium
perenne) showed that A and
PSII were increased by instantaneous
elevation of pCO2 for plants grown at
current pCO2, but longer term
acclimation completely reduced the stimulation of both A and
PSII (Bartak et al., 1996 ). For natural
vegetation growing in the field, studies show seasonal decreases in
photochemistry, and increased photoinhibition in elevated
pCO2 (Scarascia-Mugnozza et al., 1996 ;
Hymus et al., 1999 ).
Here, we have extended these findings by providing quantitative
evidence that elevated pCO2
can either increase or decrease photochemistry and photoinhibition,
depending on whether down-regulation of photosynthetic capacity has
occurred. Plants were grown at 400 µmol m 2
s 1, but exposed to higher light for the
photoinhibitory treatment. This is not unrealistic of many areas of the
globe where a series of cloudy days may be followed by clear sky days
with higher photon flux or where grazing exposes lower canopy leaves to
high light. This finding has important ecological implications.
Although under optimal conditions, elevated
pCO2 increases photochemical energy use and decreases the probability of photoinhibition, the reverse is
true of limiting nitrogen conditions. Most of the natural terrestrial biosphere and much subsistence agriculture is nitrogen limited. It has
been widely appreciated that the response of photosynthesis to rising
pCO2 may be diminished by acclimation
in these conditions. Here, we show that not only is capacity for carbon
assimilation decreased, but the probability of photoinhibition, due to
increased non-photochemical quenching, is increased. Such
non-photochemical quenching would serve to protect the reaction centers
from photo-inactivation and damage when the rate of excitation of PSII
is in excess of the rate of photochemistry. The cost of this protection
is that when a leaf is in low light after photoinhibition the
efficiency of photosynthesis remains low for minutes to hours,
resulting in a significant loss of potential carbon fixation (Long et
al., 1994 ). Elevated pCO2 will
increase this loss, both by increasing the potential for
photoinhibition and by slowing the rate of recovery.
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MATERIALS AND METHODS |
Growth Conditions
Dactylis glomerata (IGER, Aberystwyth, UK) was
grown from seed for 56 to 57 d in a washed silver sand media
(William Sinclair Horticulture, Lincoln, UK), in 0.62-L pots. Four
seeds were sown in each pot. These were then divided between two
controlled environments (PG660, Sanyo, Loughborough, UK); one was
maintained at 35 Pa pCO2 (ambient), the
other at 65 Pa pCO2 (elevated). An infrared gas analyzer integrated with a feedback control system (WMA-2, PP
Systems, Hitchin, UK), which controlled the injection of scrubbed, pure
CO2 gas (Linde Gas Ltd, Stoke on Trent, UK), maintained the pCO2 within the controlled environment
cabinets. Plants were grown in a day/night temperature regime of
16°C/12°C and a relative humidity of 80%, giving a daytime
water vapor pressure deficit of 0.5 kPa. The photoperiod was 14 h
long at a PPFD of 400 µmol m 2 s 1 at pot
height, providing a total photon flux of 20 mol m 2
d 1 over the photoperiod and similar to that which
D. glomerata would receive in the field during summer in
Western Europe.
From planting to 1 week after emergence, the sand media was fully
saturated with deionized water. At this point, the plants were divided
into two nutrient regimes in each cabinet. They were supplied with
either high (12 mM) or low (4 mM) nitrogen by a Long Ashton (nitrate type) solution (Hewitt, 1966 ). Throughout the
growth period, the sand media was flushed twice weekly with deionized
water to prevent accumulation of salts.
To minimize undetected inter-cabinet environmental differences,
pCO2 treatments and their plants were
swapped between cabinets each week. To minimize the effects of
intra-cabinet environmental gradients, the plants were randomly
repositioned within the cabinets each week. Between 56 and 57 d
into growth, five plants of the eight grown for each treatment were
randomly selected for simultaneous measurements of leaf gas exchange
and chlorophyll a fluorescence. Measurements were made
on the youngest leaf with an emerged ligule on the main stem.
Leaf Gas Exchange
Leaf net CO2 uptake (A) and water vapor
efflux were measured in an open gas exchange system. A combined
CO2 and water vapor analyzer (LI-6262, LI-COR, Lincoln,
NE), calibrated against a water vapor generator (WD600, ADC Ltd.,
Hoddesdon UK) and a standard CO2 concentration of 50 Pa
(Linde Gas Ltd) was used. Inlet CO2 concentration was
controlled by a gas dilutor (GD-600, ADC Ltd.), and inlet humidity was
controlled by passing the dry airflow through a temperature-controlled
ferrous-sulfate crystal column (WG-600, ADC Ltd.). The
temperature-controlled leaf section chamber used (LSC, ADC
Ltd.) allowed for rapid mixing of gases, and a small response time to
changes in pCO2 and PPFD.
Chamber cooling was by circulating coolant through each half of the
chamber. All measurements were made at a leaf temperature of 16.0°C
(±0.3°C) and a water vapor pressure deficit of 1.2 (±0.04) kPa.
The light-saturated response of A to
Ci was made at a PPFD of 1,300 µmol
m 2 s 1. Photosynthetic induction was
performed at the growth pCO2. Calculations of A and Ci followed
von Caemmerer and Farquhar (1981) . Vc,max and
Jmax were estimated for each
individual leaf by fitting maximum likelihood regressions to the
initial slope and plateau of the A/Ci
response curves, respectively, using the calculations of von Caemmerer
(2000) and Bernacchi et al. (2001) .
Leaf Chlorophyll a Fluorescence
A modulated chlorophyll fluorimeter and leaf clip (PAM 2000, H
Walz, Effeltrich, Germany) were used to measure minimum
(Fo'), maximum
(Fm'), and steady-state
(Fs) levels of fluorescence simultaneously with the gas exchange measurements. These values were used to calculate
the efficiency of excitation energy capture by open PSII reaction
centers
(Fv'/Fm'), the
qP, and
PSII (Genty et al., 1989 ).
The response of A and
PSII to PPFD was determined over a
range of light levels from 0 to 1,420 µmol m 2
s 1 under non-photorespiratory conditions (1 kPa
O2; Linde Gas Ltd). Leaf absorptance ( ) was measured
with a Taylor integrating sphere attached to a quantum sensor (SKP 215, Skye Instruments Ltd, Llandrindod Wells, UK) following the
method of Rackham and Wilson (1968) . From these measurements,
CO2 was then calculated
as:
where Q is PPFD. When measured in
1% (v/v) O2, the relationship of
PSII to
CO2 is linear (Genty et al., 1989 ).
The model and assumptions of Valentini et al. (1995) use the
PSII/ CO2
relationship in 1% (v/v) O2, to calculate
light-saturated linear electron flow through PSII (Jt) and partition it between electron
flow to the photosynthetic carbon reduction
(Jc) and PCO
(Jo) cycles. In this model, the linear
relationship between PSII and CO2 is assumed to describe the
apparent quantum efficiency of photosynthetic linear electron flow
( e ) using the equation:
where 4 is the number of electrons needed per
CO2 molecule fixed, k is the gradient, and
b is the y intercept. The model assumes
that this relationship holds in both photorespiratory and
non-photorespiratory conditions, enabling
Jt to be calculated
as:
By assuming only the photosynthetic carbon reduction and PCO
cycles are sinks for linear electron flow, the model calculates the
partitioning of Jt between
Jc and
Jo as:
where 4 is the number of electrons required to fix one
molecule of CO2 and Rl is the
rate of CO2 production by photorespiration. Jc and
Jo are then solved
as:
Photoinhibitory Treatment
Between 54 and 58 d into growth, leaves of D.
glomerata grown in the nitrogen and
pCO2 treatments described previously were selected for a photoinhibitory, high-light treatment. The criteria used
for leaf selection were as for the previous measurements. Leaves were
exposed to a PPFD of 2,000 µmol m 2 s 1 for
3 h, within a custom-built controlled environment in which the
pCO2 was maintained at growth
levels, air temperature was maintained at 16°C to 18°C, and
relative humidity was maintained at 75% to 82%,
approximating growth conditions. Eight plants, two from each
treatment, were randomly selected and photoinhibited on each of 5 consecutive d. In total, 10 plants from each treatment were photoinhibited.
Measurements of Fo and
Fm were made in the dark prior to the
beginning of the photoperiod to determine the maximum quantum yield of
PSII (Fv/Fm),
then every 45 min during the photoinhibitory treatment, using a
modulated chlorophyll fluorometer (PAM 2000). The
photoinhibitory treatment was begun 1 h into the photoperiod. After 3 h, the plants were returned to their respective growth environments to recover. The recovery of
Fv/Fm measured
after 10 min of dark adaptation, and
Fv'/Fm'
measured under growth light levels, was followed. Measurements were
made immediately following the photoinhibitory treatment and then at
hourly intervals until the recovery was complete, using the equipment
and protocols for measurement described previously.
Statistical Analysis
The effects of growth pCO2 and
nitrogen supply on Asat,
Vc,max,
Jmax,
PSII,
qP,
Fv'/Fm',
Jt,
Jc, Jo, and were tested using ANOVA.
Where a significant interaction between pCO2
and nitrogen was found, post hoc pair-wise comparisons using Tukey's
test were performed to identify differences between individual means.
The effect of pCO2 treatment on the recovery
of Fv/Fm was
tested using a two-tailed Student's t test. All ANOVA
and Student's t tests were performed using statistical software (Systat 7.0, Systat Inc, Evanston, IL). The effect of pCO2 treatment on the relationship between
PSII and CO2 was examined by regression
analysis of variance (Zar, 1999 ). Fluorescence yields were arcsine
transformed to generate a normal distribution for statistical analysis
(Zar, 1999 ). An effect was described as significant where
P < 0.05.
 |
ACKNOWLEDGMENTS |
We thank Mr. Paul Beckwith and Mrs. Sue Corbett for their
skilled technical support.
 |
FOOTNOTES |
Received March 12, 2001; returned for revision May 8, 2001; accepted July 17, 2001.
1
This work was supported by the Natural
Environment Research Council of the United Kingdom (research
studentship to G.J.H.).
2
Present address: Smithsonian CO2 Site, Mail
Code DYN-2, Kennedy Space Center, FL 32899.
3
Present address: Departments of Crop Science and Plant
Biology, University of Illinois, Edward R. Madigan Laboratory
190, 2206 West Gregory Drive, Urbana, IL 61801.
*
Corresponding author; e-mail stevel{at}life.uiuc.edu; fax
217-244-7563.
Article, publication date, and citation information can be found at
www.plantphysiol.org/cgi/doi/10.1104/pp.010248.
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