Effect of High CO2 Concentration on FourPopulusby the Fast Fluorescence Rise OJIP
RuyuXie, Mu Peng, Tao Wang, Tie Li, FanjuanMeng*
College of Life Science, Northeast Forestry University, Harbin, China
*Corresponding author:Fanjuan Meng, College of Life Science, Northeast Forestry University, Harbin 150040, China. Tel: +8618845897145; Email: mfj19751@163.com
Received Date: 15 September, 2018;
Accepted Date: 26 September, 2018;
Published Date: 04 October, 2018
Citation: Xie R, Peng M,
Wang T, Li T, Meng F (2018) Effect of High CO2 Concentration on Four
Populus by the Fast Fluorescence Rise
OJIP. Curr Trends Forest Res: CTFR-124. DOI: 10.29011/ 2638-0013. 100024
1. Abstract
Increased atmospheric carbon dioxide (CO2) concentration affects plant physiological and ecosystem processes. The aim of this study was finding out the main reasons why PSII were affected by CO2 in four different kinds ofPopulus(PopulusL.) (PopulusX, Populusdeltoides ×cathayana, Poplus alba ‘Berdinensis’ L., Populuseuramerican‘N3016’×Populusussuriensis) and the differences of responses in these four kinds of Populus. The chlorophyll fluorescence technique was considered as an effective tool in the context of non-destructive leaf photosynthetic apparatus of the degree of thermal, and has been widely used in relevant studies of CO2 stress. The JIP-test is a method for analyze the fluorescence transient which transformed the measured value to a serials biological parameters, and also detect the energy strength generated by PSII. The results show that the PSII performance was negatively influenced by CO2stress. CO2stress resulted in down-regulation of Fm, φPo(=Fv/Fm), ψEo, φEoandPItotalin all four kinds of Populus. And a significant decrease in the P-step level of the fluorescence transients OJIP curves of four Populusspecies after 7 days of treatment with high CO2. So a fast decrease of the P-step level indicated there was main change to fluorescence transients. Generally speaking, these results indicated that the main reasons why PSII were affected by CO2 were degradation of antenna pigment and inhibition of the electron transport at the acceptor side of PSII.
2.
Keywords: Atmospheric Carbon Dioxide (CO2);
Photosynthetic Performance; PopulusL.;
OJIP
1.
Introduction
Environmental changes caused by increased emissions of
greenhouse gasses have influenced the stability of ecosystems worldwide[1]. The
increase of atmospheric carbon dioxide (CO2) is one of the most
important environmental changes in the world in the past and the future.
Especially, human activities also increased the concentration of CO2
in the atmosphere, which is expected to reach 700 μL/L by the middle of the
next century [2-5]. Current evidence showed the increase of CO2
concentration will influence on plant growth, development biological yield. In
general, high CO2 concentrations increase photosynthetic rates,
which promoted the growth
of
plants.
However,
there are most reports on the response of crop plant species to
elevatedatmospheric CO2, but few of them have given account of the
response of woody species to high CO2 levels. In this study, we
compared the effect of elevated CO2 on the growth and photosynthetic characteristics of four Populus
(PopulusL.) species.
Populus spp., as poplar
hybrids, belongs to a fastest-growing tree. For their rapid growth, their wood
can be used for construction, pulp, paper, and as a renewable, cost-effective
alternative to fossil fuels. Previous reports showed that poplars are sensitive to
environmental stress compared with other tree specise[6,7]. To date, the effects of high CO2 levels on Populusphysiology and growth have
been studied in numerous researches. For example, in
birch, elevated CO2 treatments had no major impacts
on wood anatomy or wood density [8]. Lee et al., (2014)
found that the cuttings of Populus alba × glandulosaunder the elevated
CO2treatment showed reduced tree height and
photosynthetic pigment contents such as chlorophyll and carotenoid. In
particular, the elevated treatment resulted in a marked reduction in the
chlorophyll a. However, some works also showed that increased CO2
delayed leaf fall, but this effect is species-specific. However, there are few
tests of whether differences in photosynthetic abilityexist between different Populusspecies in response to
elevated CO2. Generally, the photosynthetic ability was reported to a reliable
indirect indicator of tree performances under different environmental stress [9,10].
As a rapid and
non-destructive technique, this technology is very useful to investigate the
photosynthetic function, and has been used to study the effects of drought,
high temperature, salt stress on plant species. Additionally, this technology has also provided
valuable information on the functional and structural attributes of components
involved in photosynthetic electron transport and especially to study
photosystem II (PSII) behavior[11- 21]. In
general, a sequence of phases (labelled as O, K, J, I, P) can be obtained in
the fluorescence rise during the first second of illumination from the initial
(Fo) to the maximal (Fm) fluorescence value. This mathematical
model was named as JIP-test, which can provide quantum yields, biophysical
parameters and probabilities characterizing structure and function of PSII [22,23].
PSⅡ is very sensitive to environmental stresses [9,10].
However, a complex study comparing influences of high CO2 levels on
PSII behaviors of woody species is still lack. Therefore, a detailed comparison
of high CO2-induced changes in PSII photochemistry in different Populus spp. species was carried out by using the fast Chl
fluorescence records.
In our study, we have
examined photosynthetic responses of fourPopulus spp. species to high CO2 levels using
fast Chlorophyll (Chl) a fluorescence transient
(O-J-I-P) technology. In this study, we analyzed
the transient fluorescence using JIP-test
in four Populusspecies (PopulusX, Populusdeltoides
×cathayana, Poplus alba ′Berdinensis
′ L,Populuseuramericana′N3016′ ×Populusussuriensis) under atmospheric CO2 (1500 ± 50 μmol/mol).
Our objectives were to determine that whether differentPopulusspeciesvary in their PSⅡ traits under elevated atmospheric CO2.
2.
Materials
and Methods
2.1.
Plant Material and Stress Treatment
Experiments
were performed at College of Life Science, Northeast Forestry University, which
is located in Harbin, Heilongjiang Province. Four Populus
species including PopulusX,Populusdeltoides
× cathayana,Populus alba ′Berdinensis′ Land Populuseuramericana′N3016′
× Populusussuriensiswere used in the
experiments.
The cuttings were planted in plastic pots (60 cm in
length, 25 cm in breadth and 15 cm in depth) filled with 1.5 kg of
soil and sand (2: 1). The experiments were carried out in the close
gas-exchange system consisting of chambers of 300 L volume (71cm in
length, 73cm in breadth and 175 cm in height). There are 10 cuttings in each
pot. Potted plants were grown in the
conditions: day/night air temperature, 28/22°C; photoperiod,
12h; relative humidity, 65-85%. One Chamber
was kept at a CO2 concentration (average ± SD)
of 370 ± 15 μmol/mol (control),
while another chamber was treated with an elevated CO2 concentration
of 1500 ± 50 μmol/mol
(hereafter denoted as treatment). In order to study the effect of CO2
for every variety of poplar, we choose the seventh day after treatment to
JIP-test in this study.We repeated the experiment three times with 10 plants in
total, 10 for controls and 10 for elevated treatment.
2.2. Chlorophyll a Fluorescence Transient Measurement and the JIP-Test
JIP - test is a method to analyze the transient
fluorescence, also known as fluorescence fast dynamic research method.
Measuring the curve of rising fluorspar light (FLR) (rapid fluorescence
kinetics) needed very strict about equipment, and the light source for high
strength of saturated excitation light (strong degrees in 3000 ~ 10000 μmol
photons/(m-2 s)), starting fast, and can quickly capture the
fluorescence signal.
JIP - test is an important method of analysis of
fluorescence kinetics curve, the purpose of this method is to turn the
parameters of the measured values into a biological significance that can
direct energy intensity produced by PSII. In general, there are four important
inflection point on the fluorescence fast dynamic curve, namely the O - J - I -
P turning point, respectively is: 1) O point shows that
the system (PSI) release amount of the fluorescent light, which can be
understood as the light of the PSI and efficiency, the fluorescence intensity
is at 0.02 ms (F0). 2)
Fluorescence intensity at 2ms, called Fj,
J inflection point reflect the reaction in the accumulation of the electron
acceptor QA- to QB-, the oxidation
of the Q. 3) Fluorescence intensity at 30ms calledFi.4)Maximum fluorescence intensity is Fm.
Leaves were dark adapted for 30 min to ensure
that all PSII RCs were in the dark adapted state with open RCs. Then
chlorophyll-a fluorescence transients were recorded and digitized with the
portable Handy PEA (Hansatech Instruments, Ltd., King’s Lynn Norfolk, UK) with
a 12-bit resolution from 10 s to 1 s and a time resolution of 10 s for the first 200 data points (Strasser et al., 1995). All measured
and derived parameters (Table 1) are based on Strasser et al. [24,25] and
Tsimilli-Michael[26].
Poplar leaves can completely cover the fluorescent clip
test hole, it can measure directly. The excitation light was red light whose
intensity was 3000 µmol/m2s saturated light intensity with peak
wavelength of 650 nm. Fluorescent signal recording time of 10s, each group of
plant test repeat 5 times.
2.3.
Date Analysis
Each
experiment was conducted at least five times independently. All data presented
were mean values of each treatment. Standard Errors (SE) for the values
obtained were calculated. All the above data analyses were processed using
SPSS17.0 Software.
3.
Results
3.1.
Changes in Photosystem II (PS
II) Under CO2 Stress
In Figure 1, four typical O-J-I-P chlorophyll
fluorescence transient in leaves of untreated and treated seedlings of four Populus species are shown. To analyze
changes in the shape of the transients among all Populus genotypes, All O-J-I-P transients were normalized at the O-
and P-step. In four genotypes the response of treated seedlings was not
similar.
In PopulusX,
at the 7th day, relative fluorescence intensity was decreased (Figure 1A). Thus
high CO2 conditions after long time inhibited the fluorescence
intensity, especially from I- to P- step of Populus
X. In Populusdeltoides×cathayana, at 7th day, relative
fluorescence intensity was increased. While, relative fluorescence intensity
was increased from J- to I- step (Figure 1B), which showed different changes
from these genotypes in relative fluorescence intensity. In Populus alba ‘Berdinensis’ L, relative
fluorescence intensity was similar between control and treatment from J- to I-
step (Figure 1C). InPopuluseuramericana′N3016′ ×Populusussuriensis, an increase in
relative fluorescence intensity was observed from I- to P- step (Figure 1D).
3.2.
Changes of Fluorescence Parameters
Under CO2Stress
In Table 2, no significant high CO2-induced
changes were observed in the minimum fluorescence (Fo), fluorescence at the
J-step (Fj) and fluorescence at the I-step (Fi).
In contrast, drastic decreases inF maximum fluorescence (Fm)values of fourPopulusspecies
were recorded after 7 days of CO2 treatment (Table 2). In parallel,
all Populus
species showed significant decrease in maximum quantum yield of PSII primary
photochemistry (φPo), the efficiency with which the energy of a trapped
exciton is converted into
electron transport beyond QA- (ψEo), the quantum yield
of electron transport beyond QA(φEo)
and total performance index per absorption basis (PItotal) after high CO2 treatment.
Especially, PItotal value
sharply decreased after treatment. On the other hand, the values of relative
variable fluorescence at the J-step (Vj)
and relative variable fluorescence at the I-step (Vi) of treated-plants were higher than those of
controls. There is higher value in ABS/RC (measure of the average total
absorbance per active PSII RC) of treated plants compared to those of control
plants. However, an exception for the Populusdeltoides
× cathayanaafter treatment had no difference between CO2-treated
and control plants (Table 2).
4.
Discussion
In this study, the shapes of chlorophyll a fluorescence transient (O-J-I-P) were markedly different in the four high CO2-treated
leaves, however the values of Fv/Fm showed similar decreasing tendency (Table 2). Thus,
there is the heterogeneous behavior of PSII in Populusleaves as similar Fv/Fm. Generally, the
level of photochemical reaction can be evaluated according to the chlorophyll
fluorescence intensity. And Fv/Fm was used to describe the trapping efficiency of the
absorbed light, which can reduce primary quinone electron acceptor of PSII (QA) [27]. Therefore, the different fluorescence transients
of leaves under high CO2 levels indicated that the photochemical
reactions were different in differ Populusspecies, although there were similar
decreasing Fv/Fm(reflecting
trapping efficiencies of the absorbed light). In contrast, previous studies
showed the Fv/Fmratio reflects the
photochemical efficiency of PSII [28]. Various environmental stress can lead to
inhibition of photosynthetic efficiency, accordingly, affecting state of the
photosynthetic apparatus.
For
O-J-I-P, point O represents the fluorescence of PS Ⅱ action
center when all of the electron acceptor (QA, AB, PQ,
etc.) are fully open in the maximum oxidation state. The fluorescence intensity
of point O is connected with the content of the antenna pigment and the
activity of action center. Point J reflects the rate of reduction of QA,
which is connected with reaction centre pigments, light-harvesting pigment and
the state of QA and QB. If the electrons transfer from QA
to QB is restricted, the value of point J will rise [29]. Here,
higher J value in the leaves. In addition, point I reflects the heterogeneity
of PQ, the electron acceptor state in point I mainly is related to QA-
and QB2-. Furthermore, the structure and function of PSⅡ
complexes and the size of the PQ library is attributed to appearing time of
point P. In this study, high CO2
level caused a significant decrease in the P-step level of the fluorescence
transients OJIP curves of four Populus
species after 7 days of treatment with high CO2. So a fast decrease
of the P-step level indicated there was main change to fluorescence transients. Generally, the “P” level was
connected with the process of the electron transportation from QBto
PQ, and it can mark concentrations of both QA− QB2− and
PQH[30, 31].
No significant changes in Fo, Fj and Fiof different Populusspecies were observed when subjected to high CO2 stress.
However, high CO2stress result Fm
in decrease. Fm
reflects maximum fluorescence intensity at the P-step[32]. Therefore, this
result suggested that the Fmmay
be a good marker of PSII vitality under CO2 stress.
The
PSII switches from the process of converting light energy into biochemical
energy storage to the energy conversion process that transforms absorbed light
energy into heat dissipation[33].One of parameters used to analyze the response
of the plant’s PSII is PItotal.
PItotalis sensitive to
changes in either antenna properties, trapping efficiency
or electron transport beyond QA[34]. In this study, we found that
PSII performance was represented using this index (PItotal). In general, the observed PItotalis influenced by changes in antenna, RC, electron
transport and end-acceptor reduction dependent parameters. Thus, PItotalintegrates the
response of RC/ABS, TRo/ABS(=Fv/Fm), ETo/TRo(= [1 −Vj]) and REo/ETo(=[1 − Vi]/[1 −Vj]).
In summary, inhibition of PSII under CO2stress
involved in changes of Fm
and PItotal.
In other words, these two
parameters can be used in indicate the changes of PSII. These results indicated that the main reasons why PSII
were affected by CO2were degradation of antenna pigment and
inhibition of the electron transport at the acceptor side of PSII.
This study was supported by the Fundamental Research Funds
for the Central Universities (No. 2572015DA03 and No. 2572016EAJ4).
6.
Conflict
of Interest
The authors declare that there are no conflicts of interest.
Figures 1(A-D):The
relative fluorescence transients in fully dark-adapted PopulusX leaves (A), Populusdeltoides×cathayanaleaves (B), Populus alba ′Berdinensis′ L leaves (C) and Populuseuramericana′N3016′×
Populusussuriensisleaves (D)
under CO2stress and the control condition at 7 days.
Measured
parameters from the chlorophyll-α fluorescence transient |
|
Ft |
Fluorescence intensity at time measured after onset of
actinic illumination |
Fo= F20μs |
Minimum reliable fluorescence intensity at 20μs |
Fl |
Fluorescence intensity at the L-step (100 μs) |
Fk |
Fluorescence at the K-step (300 μs) |
Fj |
Fluorescence at the J-step (2 ms) |
Fi |
Fluorescence at the I-step (30 ms) |
Fp= Fm |
Maximum fluorescence intensity at the P-step |
Derived
parameters |
|
Selected OJIP-test parameters |
|
Vj= (F2ms− Fo)/ (Fm−
Fo) |
Relative variable fluorescence at the J-step |
Vi= (F30ms−
Fo)/(Fm− Fo) |
Relative variable fluorescence at the I-step |
Mo= 4 × (F300 s− Fo)/ (Fm−Fo) |
Approximated initial slope per ms of the fluorescence
transient |
ABS/RC = [Mo/Vj] × [1/(Fv/Fm)] |
Measure of the average total absorbance per active PSII
RC |
Quantum yields |
|
φPo= TRo/ABS
= (Fm− Fo)/Fm= Fv/Fm |
Maximum quantum yield of primary photochemistry, equal
to the efficiency by which an absorbed photon trapped by the PSII RC will
result in reduction of QA to QA− |
ψEo= ETo/TRo=
(1 − Vj) |
The efficiency by which a trapped exciton, having
triggered the reduction of QA to QA−can move
an electron further than QA− into the intersystem
electron transport chain |
δRo= REo/ETo=
(1 − Vi)/(1 − Vj) |
The efficiency with which an electron can move from the
reduced intersystem electron acceptors to the PSI end acceptors |
Performance index |
|
PIabs=
[RC/ABS] × [φPo/(1 −φPo)] × [ψEo/(1 −ψEo)] |
Performance index on absorption basis, incorporating
the steps from antenna, reaction center and electron transport parameters |
PItotal=
[RC/ABS] × [φPo/ (1 −φPo)] × [ψEo/ (1 −ψEo)] × [δRo/ (1 −δRo)] |
Total performance index per absorption basis,
integrates into the sum of changes in quantum yields and absorption |
Table1: Formulae and explanation the technical data of the OJIP
curves and the selected JIP-test parameters used in this study.
Species |
PopulusX |
Populusdeltoides ×
cathayana |
Poplus alba ‘Berdinensis’ L. |
Populuseuramericana“N3016”× Populusussuriensis |
||||
Measured parameters |
Control |
Treatment |
Control |
Treatment |
Control |
Treatment |
Control |
Treatment |
Fo |
2798±171 .57 |
2345±166.19 |
2576.75±116.56 |
2643.6±96.32 |
2284.4±75.49 |
2065±98.63 |
2282.75±66.48 |
2298.25±280.5 |
Fj |
7314.33±640.30 |
6703.5±323.45 |
7325±508.27 |
7493±686.81 |
6314.8±362.77 |
6051.33±323.15 |
6492.50±104.95 |
6325.25±111.60 |
Fi |
12332.67±258.46 |
11909.5±310.17 |
12008.5±194.37 |
12669.4±75.86 |
11297.4±233.28 |
10267±282.20 |
11315.25±252.66 |
10889.25±219.88 |
Fm |
16725.67±1263.26 |
13462±782.00 |
16936±580.53 |
15267.8±878.34 |
14546.2±1058.17 |
12577.33±578.35 |
14989.5±463.67 |
13330.5±578.09 |
Derived parameters |
||||||||
Vj |
0.324±0.009 |
0.395±0.090 |
0.328±0.028 |
0.385±0.005 |
0.327±0.022 |
0.379±0.016 |
0.332±0.012 |
0.366±0.015 |
Vi |
0.684±0.014 |
0.865±0.069 |
0.652±0.002 |
0.796±0.004 |
0.739±0.014 |
0.781±0.020 |
0.712±0.026 |
0.780±0.018 |
ABS/RC |
0.756±0.009 |
0.896±0.037 |
0.782±0.008 |
0.767±0.013 |
0.860±0.017 |
1.009±0.024 |
0.829±0.008 |
0.851±0.008 |
φPo=TRo/ABS=FV/FM |
0.833±0.002 |
0.825±0.001 |
0.848±0.002 |
0.826±0.009 |
0.842±0.004 |
0.836±0.005 |
0.848±0.003 |
0.827±0.01 |
ΨEo=ETo/TRo |
0.676±0.009 |
0.605±0.042 |
0.672±0.027 |
0.615±0.024 |
0.673±0.021 |
0.621±0.016 |
0.668±0.012 |
0.634±0.015 |
φEo |
0.563±0.006 |
0.500±0.008 |
0.570±0.013 |
0.508±0.019 |
0.567±0.018 |
0.519±0.016 |
0.566±0.017 |
0.525±0.018 |
PIABS |
8.141±0.137 |
7.053±0.163 |
11.639±0.64 |
6.126±0.937 |
8.597±0.129 |
8.488±0.094 |
9.033±0.519 |
7.315±0.183 |
PItotal |
2.134±0.0009 |
0.575±0.028 |
2.724±0.013 |
0.835±0.004 |
2.016±0.012 |
1.326±0.017 |
2.207±0.007 |
1.143±0.008 |
Values of the mean ±
standard error for the un-manipulated control are given. The parameters are,
minimum fluorescence at 20 s, Fo;
fluorescence intensity at 2 ms, Fj;
fluorescence intensity at 30 ms,Fi;
maximum fluorescence, Fm;
relative variable fluorescence at the J-step, Vj; relative variable fluorescence at the I-step, Vi; measure of the average
total absorbance per active PSII RC, ABS/RC; maximum quantum yield of primary
photochemistry, φPo(=TRo/ABS); probability that a trapped exciton moves an
electron into the electron transport chain beyond QA-, ETo/TRo; total
performance index per absorption basis, PItotal
(see also Table 1). Results are presented as mean of five individual
measurements. |
Table 2: The
fluorescence parameters on four Populusspecies under CO2 stress.
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