Accurately predicting the crown photosynthesis of trees is necessary for better understanding the C circle in terrestrial ecosystem. However, modeling crown for individual tree is still challenging with the complex crown structure and changeable environmental conditions. This study was conducted to explore model in modeling the photosynthesis light response curve of the tree crown of young Larix principis-rupprechtii Mayr. Plantation. The rectangular hyperbolic model (RHM), non-rectangular hyperbolic model (NRHM), exponential model (EM) and modified rectangular hyperbolic model (MRHM) were used to model the photosynthetic light response curves. The fitting accuracy of these models was tested by comparing determinants coefficients (R2), mean square errors (MSE) and Akaike information criterion (AIC). The results showed that the mean value of R2 of MRHM (R2 = 0.9687) was the highest, whereas MSE value (MSE = 0.0748) and AIC value (AIC = -39.21) were the lowest. The order of fitting accuracy of the four models for Pn-PAR response curve was as follows: MRHM > EM > NRHM > RHM. In addition, the light saturation point (LSP) obtained by MRHM was slightly lower than the observed values, whereas the maximum net photosynthetic rates (Pmax) modeled by the four models were close to the measured values. Therefore, MRHM was superior to other three models in describing the photosynthetic response curve, the accurate values were that the quantum efficiency (α), maximum net photosynthetic rate (Pmax), light saturation point (LSP), light compensation point (LCP) and respiration rate (Rd) were 0.06, 6.06 μmol·m-2s-1, 802.68 μmol·m-2s-1, 10.76 μmol·m-2s-1 and 0.60 μmol·m-2s-1. Moreover, the photosynthetic response parameters values among different layers were also significant. Our findings have critical implications for parameter calibration of photosynthetic models and thus robust prediction of photosynthetic response in forests.
Accurately predicting the crown photosynthesis of trees is necessary for better understanding the C circle in terrestrial ecosystem. However, modeling crown for individual tree is still challenging with the complex crown structure and changeable environmental conditions. This study was conducted to explore model in modeling the photosynthesis light response curve of the tree crown of young Larix principis-rupprechtii Mayr. Plantation. The rectangular hyperbolic model (RHM), non-rectangular hyperbolic model (NRHM), exponential model (EM) and modified rectangular hyperbolic model (MRHM) were used to model the photosynthetic light response curves. The fitting accuracy of these models was tested by comparing determinants coefficients (R2), mean square errors (MSE) and Akaike information criterion (AIC). The results showed that the mean value of R2 of MRHM (R2 = 0.9687) was the highest, whereas MSE value (MSE = 0.0748) and AIC value (AIC = -39.21) were the lowest. The order of fitting accuracy of the four models for Pn-PAR response curve was as follows: MRHM > EM > NRHM > RHM. In addition, the light saturation point (LSP) obtained by MRHM was slightly lower than the observed values, whereas the maximum net photosynthetic rates (Pmax) modeled by the four models were close to the measured values. Therefore, MRHM was superior to other three models in describing the photosynthetic response curve, the accurate values were that the quantum efficiency (α), maximum net photosynthetic rate (Pmax), light saturation point (LSP), light compensation point (LCP) and respiration rate (Rd) were 0.06, 6.06 μmol·m-2s-1, 802.68 μmol·m-2s-1, 10.76 μmol·m-2s-1 and 0.60 μmol·m-2s-1. Moreover, the photosynthetic response parameters values among different layers were also significant. Our findings have critical implications for parameter calibration of photosynthetic models and thus robust prediction of photosynthetic response in forests.
As the largest carbon flux in global carbon (C) cycling, photosynthesis can
assimilate CO2 from the atmosphere and thus dedicating to climate change
mitigation. It plays a crucial role in the material cycle and energy flow of forest
ecosystems [1-3]. In addition to the stage of
leaf development and genetic constitution of plant, photosynthesis is also strongly
affected by surrounding environmental conditions (e.g., light, leaf, CO2
concentration, humidity and temperature etc.), during which intensity of light and
its availability particularly determine the amount of C assimilated by
photosynthesis [4-7]. For the trees, the canopy
is the most direct part for photosynthesis to response to incoming solar irradiance.
Therefore, better understanding the mechanism of crown leaf photosynthesis response
to light availability is thus critical for maintaining forest productivity and
management, in particular for dynamic simulation growth models and in
parameterization of crown photosynthesis.Light response curves (Pn-PAR curves) describe the
relationship between net photosynthetic rate (Pn) and
photosynthetically active radiation (PAR), and provide information
about the photosynthetic efficiency of plants (e.g. quantum yield, the maximum
photosynthetic capacity, light compensation point and leaf radiation use efficiency
of leaves) [8-10]. The simulation of
Pn-PAR curves are becoming increasingly
important to study the photosynthetic response process of plants to the environment,
and analyze the primary productivity of vegetation and forests [1, 11–13]. A series of photo-physiological core
parameters, such as maximum net photosynthetic rate
(Pmax), apparent quantum yield
(AQY), light-saturation point (LSP),
light-compensation point (LCP), and dark respiration rate
(Rd), can be used to assess the canopy
photosynthetic rate and capacity of plants in different growth stage. To date, in
order to investigate the response of net photosynthetic rate
(Pn) to light intensity of different plants, many
models, including the rectangular hyperbola model (RHM) [14, 15], the nonrectangular hyperbola model (NRHM)
[16, 17], the exponential model (EM)
[18, 19], and the modified
rectangular hyperbola model (MRHM) [20], have been widely applied in modeling the photosynthetic
light-response curve (Pn-PAR curve)
[1, 12]. However, RHM, NRHM, and EM are very
complex, some photo- and biochemical parameters (such as
Pmax and LSP) are subject to
environmental conditions and cannot be calculated directly using these models when
light intensity are above zero [21-24], and the
fitted values of photosynthetic parameters were significantly different from the
measured ones [20, 25]. In the contrary, owing to
the addition of two adjusting factors (β and γ) into this model, which made the
model highly advantageous in fitting the photo-inhibition and light saturation
stages [20, 26], the MRHM can directly
produce Pmax and LSP, and overcome the
limitation of above three models, the accuracy were higher and the results were
suitable for fitting Pn-PAR curve and
photosynthetic parameters under various environmental conditions [20, 24, 26, 27], it has been successfully applied in
simulating light-response curves of many plants, such as Keteleeria
calcarea [28],
Pinu stabulaeformis Carr. [29], Pinus koraiensis [30], Betula
utilis [31].Larix principis-rupprechtii Mayr (Larch)., one of
the main species of the total area of all plantations in Northern China, plays an
important role in wood production, biodiversity protection, and forest ecological
construction, due to its advantages of fast growth, strong adaptability, and high
economic value. To the best of our knowledge, little attention has been paid to the
application of a variety of dynamic crown photosynthetic light-response models in
Larch, and the fitting effect and differences of light
responses by these models remains unclear. Therefore, the determinant coefficients
(R2), mean square error (MSE), and
Akaike information criterion (AIC) were used to evaluated the
performance of four types of light-response models(such as RHM, NRHM, EM, and MRHM)
in 16-years-old Larch. Planation. The objectives of the study were
to select an optimal
P-PAR curve model
for fitting the Pn-PAR curves of
Larch, and to explore the relationships between the parameters
of the optimal Pn-PAR curve model and
leaf vertical positions. The results are helpful to further explore the spatial
heterogeneity of carbon sequestration capacity of Larch needles in
canopy, and provide a basis for accurately estimating photosynthetic physiological
characteristics and the productivity of its plantation.
Materials and methods
Ethics statement
Conflicts of interest
The authors declare no conflict of interest.
Ethical approval
The authors declare that this article does not contain any research with
humans or animal subjects.
Site description and sample tree selection
The experiments were conducted in the field at the the scientific research base
of the State Forestry and Grassland Bureau established by Hebei Agricultural
University, and the practice Base for postgraduate training of Forestry Master’s
Degree in Hebei Agricultural University. which is located in Saihanba Forest
Farm of Weichang County of Hebei Province in the northern China (Fig 1, Table 1). The farm was mainly composed with
Larixprincipis-rupprechtii,
Populusdavidiana, Betula platyphylla, and
Quercus mongolica. The total forest coverage is
approximately 82.6%, including 72.6% plantation.
Fig 1
Study location and field experiment of L.
principis-rupprechtii in Hebei Province,
China.
Table 1
Description of sample site used in the experiment.
Sample site
Latitude (N)
Longitude (E)
Elevation (m)
Climate
Annual mean temperature (°C)
Annual precipitation (mm)
Annual evaporation (mm)
Sunshine hours (hs)
Number of frost-free period (d)
Population size (hm2)
Saihanba Forest Farm
42°02′-42°36′
116°51′-117°39
1500–2067
cold temperate semi-arid and semi humid
continental monsoon
-1.5(from -42.8 to 30.9°C)
452.6
1230
2368
60
93333
Three sample plots (20 m width × 30 m length) were set up within 16-year-old
Larch plantations of the same habitat. The diameter at
breast height (DBH, cm) and tree height (H, m) were measured for all trees with
the D >5 cm in each plot, and the mean D (Dm) for three plots were calculated
independently. Then, three sample trees, whose D values respectively was similar
to Dm of the three plots, were selected to represent experimental materials.
According to the previous studies, for trees, the upper limit of the
P-PAR curves
was significantly different within different crown whorls in the vertical
direction [32-34]. Thus, we divided the
crowns of three sample trees respectively into three vertical layers with the
trisection of crown depth (the distance from the top of the tree to the base of
its live crown, CD), and each layer was divided into two parts in horizontal
direction (sunny and shaded) ( [35].
Sketch map of the crown divisions.
Upper, Middle and Lower represent three equal divisions of crown depth in
the vertical direction.
Measurements of the light-response process
The light responses of photosynthesis were measured using a portable
photosynthetic gas analysis system (LI-6400, LI-COR, Inc., Lincoln, Nebraska,
USA) coupled with a standard red-blue light-emitting diode (LED) radiation
source (85% red, emission peak at 655 nm + 15% blue, emission peak at 465 nm)
(Li-6400-02B, LI-COR, Inc., Lincoln, NE, USA), photosynthetic active radiations
(PAR) intensities were set at thirteen lever of 2000, 1500, 1200, 1000, 800,
600, 400, 200, 150, 100, 50, 25, and 0 μmol (photons)
m-2s-1). Before measuring, the instrument was
preheated and calibrated each time, these sample needles were kept for 10–20 min
at a CO2 concentration of 380 μmol (photons) m-2
s-1 and a PAR value of 1,400 μmol (photons)
m-2 s-1 in the leaf chamber, which reach a steady
state around the needles. Then, the sample needles were allowed to equilibrate
to 20°C conditions for a minimum time of 2 min and a maximum of 3 min before the
data were logged during the measurement of the
Pn-PAR curves. The measurements
(experiments) were conducted from 8:30 a.m. to 16:30 p.m. on a cloud-free
periods day, with an air temperature at 24–26°C and a relative humidity at
30–40%, the fixed exposure time for each level of PAR was set
at 2–3 min, these methods are described previously [32, 33]. The data for the
Pn-PAR curves were measured
once every half month during the growing season (approximately from 15th June to
10th August) in 2018 and 2019
Photosynthesis-light response curve-fitting model and its parameters
The rectangular hyperbola model, the nonrectangular hyperbola model, the
exponential model, and the modified rectangular hyperbola model were used to fit
the light-response curves and to estimate photosynthetic parameters. The
environmental conditions (CO2 concentration, temperature and
humidity) are given. The expressions and parameters of the four models were as
follows:The rectangular hyperbola model (RHM) [15, 36] was represented to the following form:Where: Pn represents the net photosynthetic rate
(μmol (photon) m-2·s-1), a represents the
initial quantum efficiency at low light intensities [22], Pmax
represents the maximum net photosynthetic rate (μmol (photon)
m-2·s-1), Rd represents
the respiration rate in the dark (μmol (photon) m-2·s-1),
and I represents the PAR. α,
Pmax, and Rd are the
main parameters to used describe the characteristics of the
Pn-PAR.
is the initial slope of the
Pn-PAR when
PAR is 0–200 μmol·m-2·s-1, which
indicates the plants’ light use efficiency [37-39].The Pmax and LSP cannot be
calculated directly using RHM, therefore, Pmax was
estimated and calculated by using the nonlinear least squares method under high
light intensity [36,
40, 41], LSP
could be expressed respectively as:
where: A (AQE) represents
apparent quantum efficiency; LSP represents the light
saturation point (μmol (photon) m-2·s-1);
Rd is as described above. A was
obtained by fitting the light response data which PAR is equal
to or less than 200 μmol (photon) m-2s-1)Where: LCP represents the light compensation point (μmol
(photon) m-2·s-1); LSP,
A, Pmax,
Rd are as described above.The nonrectangular hyperbola model (NRHM) [42] was represented to the following form:
where: Pn indicates the net
photosynthetic rate (μmol (photon) m-2·s-1);
θ (0 < θ < 1) indicates the
convexity (curvilinear angle) (dimensionless); and α,
I, Pmax, and
Rd are as described above.The LSP was calculated by. Formula 3.The LCP can be obtained by:Where: LCP represents the light compensation point (μmol
(photon) m-2·s-1); k, α, Pmax,
Rd are as described above.The expressions for the exponential model (EM) [18] was represented to the following form:Where: e indicates the base of natural logarithm,
α, I, Pmax,
Pn, and Rd are as
described above.The LSP was calculated by. Formula 3,The LCP was calculated by. Formula 8.The modified rectangular hyperbola model (MRHM) [20, 23, 26] was represented to the following form:
where: β and γ are adjusting
factors. β represents the photoinhibition item (dimensionless),
γ represents the light saturation item (dimensionless), and
γ = α/Pmax. α, I,
and Rd are as described above.The Pmax, LCP and
LSP were expressed on the modified rectangular hyperbola
model in Eqs 10,
11, and 12, respectively:
where LCP, LSP,
α, β, γ, and
R are as described above.
Model assessment and validation
The fitting quality of the different models were assessed by mean square errors
(MSE), determinants coefficients
(R2), and Akaike information criterion
(AIC), the best combination with the largest
R2 value and smallest MSE and
AIC value represented the higher fitting accuracy.Mean square error (MSE) was the average of squared forecast
errors, it is the specific value of the sum of squared errors to the number of
errors.Determinants coefficients (R2) represents the fitting
degree of net photosynthetic rate and light intensity.Akaike information criterion (AIC) is a fined technique based on
in-sample fit to estimate the likelihood of a model to predict/estimate the
future values.
where yi, ŷi and in the equations above represented the
measured value, the fitted value and the mean of the measured values,
respectively n is the number of observations. k is the number of estimated
parameters [43].
Statistical analyses
The measured light-response data are collated and analyzed and expressed as mean
± standard deviation (SD) of three replicates. Statistical analyses of the data
were performed using two-way analysis of variance (ANOVA) by GraphPad Prism 8.0
or the SPSS software (version 18.0) and Duncan tests. Parameter values which are
significantly different (p<0.05) are indicated by different letters.
Results
Pn in response to PAR
To describe the relationships between Pn and
PAR, photosynthetic light-response curves
(Pn-PARs) of
Larch was studied. The results showed that light response
curves (Pn—PAR) fitted by NRHM, EM
and MRHM from different layers were of similar tendency, while RHM were
difficult to implement because the curves increased gradually with no extreme.
Taking the middle layer as an example, the
Pn-PAR curves could be divided
into three stages, the net photosynthetic rate (Pn)
increased linearly (rapidly) with the augments of photosynthetic available
radiation (PAR) in the first stage, where PAR
< 200 μmol (photon) m-2 s-1, then increased nonlinearly
up to the maximum Pn, in the second stage, the
maximum Pn is 6.00 μmol (photons)
m-2s-1 when PAR is 600 μmol (photons)
m-2s-1, and decreased gradually with increasing
PAR in the third stage (Fig 3). At the same PAR,
needles under upper layer had a higher Pn than those
of the middle and lower leaves, and Pn values under
different leaf layer could be ranked as: Upper layer >Middle layer >lower
layer.
Fig 3
Comparison of the measured values and fitted values of net
photosynthetic light response curves in different layers on the RHM
(a1-a3), NRHM (b1-b3), MRHE (c1-c3) and EM (d1-d3) models.
PAR represents photosynthetic available radiation,
MSE represents mean square error,
R2 represents the coefficient of
determination and AIC represents Akaike information
criterion.
Comparison of the measured values and fitted values of net
photosynthetic light response curves in different layers on the RHM
(a1-a3), NRHM (b1-b3), MRHE (c1-c3) and EM (d1-d3) models.
PAR represents photosynthetic available radiation,
MSE represents mean square error,
R2 represents the coefficient of
determination and AIC represents Akaike information
criterion.
Fitting and comparison of photosynthesis-light response curves
The fitting results showed the fitting Pn values of
the four models were very close to the measured values actually when the
PAR was low (PAR <100 μmol (photons)
m-2s-1), the gap increased with an increasing
PAR, and the difference in Pn
was more remarkable. The Pn value simulated by NRHM,
MRHM, and EM was slightly greater than measured value when PAR
values are 200–2000 μmol (photons) m-2s-1, and the
simulated pattern of Pn-PAR curves
showed similar trend, the light-response curve was best described by three
models, especially when light intensity (PAR) is beyond
Pmax (Fig 3). However, the
Pn value simulated by the RHM increased with the
increasing PAR, the fitting error was too large to use directly
(Fig 3A1-3A3). In addition, the mean
value of R2 (range from 0.9748 to 0.9930) of the
MRHM model was the highest among the four models, and MSE value
(MSE range from 0.0646 to 0.0866 μmol (photons)
m-2 s-1) and AIC value (range from
-45.7887 to -34.8321 respective) of the MRHM were significantly smaller than
those of other three models in upper, middle and lower layer respectively (Table 2). In addition, MRHM
model was superior to other three models in south and north orientation.
Table 2
Fitting accuracy of different
Pn-PAR.
Position
Fitting accuracy
Pn-PAR
models
RHM
NRHM
MRHM
EM
Upper layer
MSE
0.2998
0.1903
0.0733
0.129
R2
0.967
0.982
0.993
0.9856
AIC
-14.57
-17.18
-34.8321
-21.1756
Middle layer
MSE
0.23
0.1518
0.0646
0.144
R2
0.9628
0.9816
0.9923
0.9746
AIC
-17.06
-20.79
-45.7887
-26.5774
Lower layer
MSE
0.4581
0.3
0.0866
0.2398
R2
0.8961
0.9473
0.9748
0.912
AIC
-15.73
-19.27
-37.0383
-22.5198
North
MSE
0.3706
0.1988
0.0748
0.1565
R2
0.9563
0.9807
0.9904
0.9735
AIC
-13.71
-17.52
-39.6365
-22.6997
South
MSE
0.288
0.2292
0.0748
0.1853
R2
0.9276
0.9598
0.983
0.9413
AIC
-16.32
-20.38
-40.393
-22.943
Fitting analysis of the photosynthetic parameters based on the models
The Fitting value of photosynthetic parameters were used to estimate the fitting
quality of the model, its accuracy and rationality are affected by the model and
layer [16, 19, 20, 27]. Therefore, it is very important to
study the fitting effect of different models, different layers and different
orientations on light response parameter of needle leaves. The results showed
Pmax calculated from the RHM, NRHM and EM were
closer to the measured value in the up layer, and was slightly greater than the
measured values in the middle and lower layer. The light saturation point
(LSP) obtained by above three models were much lower than
the measured values in the up, middle and lower layer respectively. The fitted
values of Pmax and LSP by MRHM were
close to the measured values in each layer respectively. In addition, the
LSP values were significant difference between MRHM and the
other three models, while the Pmax and
LCP values were no significant difference, the
a values of each model, which are the quantum efficiency at
low irradiance, ranged from 0 to 0.125 [44], Rd value
was closer among four models (Fig
4).
Fig 4
Comparison of light response parameters of different models at the
same layer.
(a) Parameters of (a) the initial quantum efficiency
(a). (b) maximum net photosynthetic rate
(Pmax). (c) light saturation point
(LSP). (d) light compensation point
(LCP). (e) dark respiration rate
(Rd) for needles at different models.
different letters indicate significant difference at p<0.05 level
with the least significant difference test, n.s. indicated no
significant difference at the level of P<0.05.
Comparison of light response parameters of different models at the
same layer.
(a) Parameters of (a) the initial quantum efficiency
(a). (b) maximum net photosynthetic rate
(Pmax). (c) light saturation point
(LSP). (d) light compensation point
(LCP). (e) dark respiration rate
(Rd) for needles at different models.
different letters indicate significant difference at p<0.05 level
with the least significant difference test, n.s. indicated no
significant difference at the level of P<0.05.In the different layers, some simulated values of
Pn-PAR response parameters
revealed somewhat different, there was no significant difference for LSP
LCP and Rd in upper and middle layers,
but was significant difference in lower layers, the values of α
and Pmax were significant for in each layer. In
addition, the layer is one of the main factors of affecting the light response
parameters (e.g. a, Pmax,
LCP) (Fig
4, S1
Table). Some simulated values of
Pn-PAR response parameters
calculated by MRHM was more accurate than those obtained from other three models
(Fig 5, S1 Table).
The photosynthetic parameters which were fitted by four models showed no
significant difference between north and south direction (Fig 6, S3
Table).
Fig 5
Comparison of light response parameters of different layers at the
same model.
(a) Parameters of the initial quantum efficiency (a).
(b) maximum net photosynthetic rate (Pmax).
(c) light saturation point (LSP). (d) light
compensation point(LCP). (e); dark respiration rate
(Rd) for needles at different canyon
(different letters indicate significant difference at p<0.05 level
with the least significant difference test).
Fig 6
Comparison of light response parameters of different models between
south and north direction.
(a) maximum net photosynthetic rate (Pmax);
(b) dark respiration rate (Rd); (c) light
saturation point (LSP). (d) light compensation point
(LCP). (e) the initial quantum efficiency (α).
(different letters indicate significant difference at p<0.05 level
with the least significant difference test).
Comparison of light response parameters of different layers at the
same model.
(a) Parameters of the initial quantum efficiency (a).
(b) maximum net photosynthetic rate (Pmax).
(c) light saturation point (LSP). (d) light
compensation point(LCP). (e); dark respiration rate
(Rd) for needles at different canyon
(different letters indicate significant difference at p<0.05 level
with the least significant difference test).
Comparison of light response parameters of different models between
south and north direction.
(a) maximum net photosynthetic rate (Pmax);
(b) dark respiration rate (Rd); (c) light
saturation point (LSP). (d) light compensation point
(LCP). (e) the initial quantum efficiency (α).
(different letters indicate significant difference at p<0.05 level
with the least significant difference test).
Discussion
The light response curve (Pn-PAR curve)
is an important tool for describing the response of the
Pn to PAR, identifying a series of
photosynthetic parameters and evaluating the photosynthetic efficiency of plants
[11, 45, 46]. Therefore, constructing of
Pn-PAR curve and choosing the
appropriate model are helpful to simulate canopy photosynthesis and predict plant
productivity [47, 48]. In the study, the net
photosynthetic rate increased initially and then decreased gradually with the
increase of PAR (Fig
3), which was consistent with the study of leaf
Pn-PAR curves of some plants in
different growth stages [49,
50]. The results
indicated light energy absorbed by plants exceeded the needs of plants, the
absorption of the excessive light energy would restricted photosynthetic mechanism
and series of enzymatic reaction rates in the chloroplasts and result in
photo-inhibition of Larch. The upper limit value of
Pn-PAR curve maintained the state
of upper layer >middle layer > lower layer during the whole growth period,
which was also proved in other Larch species [32], indicated that the metabolic capacity was
closely related to the light environment [34]. The differences of the
Pn-PAR curve among different
canopies might be associated with leaf characteristics, solar elevation angle,
higher chlorophyll a/b ratios, relative depth into crown (RDINC), etc [32, 51]. Additional, The photosynthetic parameters
which were fitted by four models showed no significant difference between north and
south direction, which was consistent with that of previous study [52].The fitting of light-response model is an important method to describe the response
mechanism of Pn to PAR and evaluate the
photosynthetic efficiency [45]. Among four models, the Pn value simulated
by the RHM consistently increased with the increasing PAR with no
stable or declined trend (Fig
3A1–3A3), indicated that RHM was more suitable for fitting consistently
increased type of Pn-PAR curves. This
result agreed with the previous study [53]. Compared to the other three models, the
determinants coefficients (R2) value of the MRHM was the
highest, and mean square errors (MSE) value and Akaike information
criterion (AIC) value were the lowest (Table 2), indicated that MRHM performed better
than other three models [23].
In addition, some fitted values of photosynthetic parameters (e.g
Pmax and LSP) were close to the
measured values (Fig 4, S1 Table), Ye
[20] has proved that the
unique structure of MRHM made it more flexible in simulating different trends of
Pn-PAR curves.Compared with data fitted (Fig 3)
and error analysis (Table 2)
on the Pn-PAR curves of the needles at
different leaf canopy, there was no significant difference for LSP,
LCP and Rd in upper and middle
layers, but was significant difference in lower layers. However, the values of
a and Pmax were significant in each
layer. The Pn in the upper canopy was significantly
higher than those in the middle and lower canopy, which was not consistent with that
of previous study [53]. The
different may be due to the comprehensive effects of genetic diversity, different
producing areas and environmental factors of trees [54]. It can be seen that layer was one of the
main factors of affecting the light response parameters (e.g. a,
Pmax, LCP) (Fig 4, S1 Table).Based on the above discussion, we considered that the light response process and
photosynthetic parameter (Pmax, LSP,
LCP, and Rd) fitting by the MRHM
models was more reliable (S2 Table). and MRHM could fit well the
Pn-PAR curves of
Larch (Fig
4, S2
Table). In addition, the
Pn-PAR of the middle leaf layer can
better reflect the changes in leaf layer photosynthetic parameters. However, the
results, obtained in the vigorous growth period of Larix principis
rupprechtii from June to August, are of spatial and temporal limitation
in Saihanba, the further studies are needed to better understand the mechanisms of
the photosynthetic physiological ecology of plants to the environment.
Conclusion
This study describe canopy photosynthesis for Larix principis
rupprechtii plantation, the
Pn-PAR curves and photosynthetic
response parameters were measured under different layer of three planted
L. principis-rupprechtii trees by different
models during the growing season. The results showed that the fitting effect of MRHM
model was superior to those of other three models and it could analyze the
light-response data more accurately, the selection of the middle layer of the plant
is the best when measuring the photosynthetic performance of the whole tree in
combining with the analysis of fitting precision (Fig 3), the accurate values were as follows: α,
Pmax, LSP, LCP and
Rd were 0.06, 6.08
μmol·m-2s-1, 931.08 μmol·m-2s-1, 11.45
μmol·m-2s-1 and 0.61 μmol·m-2s-1,
respectively. This study not only helps to further explore the spatial heterogeneity
of carbon sequestration capacity of Larix principis rupprechtii
leaves in canopy, but also provides a scientific and effective guidance for
accurately estimating the productivity of Larix principis
rupprechtii plantation.
Pn-PAR response parameters
of leaves in different layers of Larch.
Black letter ‘a’ indicates significant differences between models, red letter
‘a’ indicates significant differences among different layers.(DOC)Click here for additional data file.
Analysis of light response parameters at different layers.
(DOC)Click here for additional data file.
Analysis of light response parameters between south and north.
Authors: Harshini Pinto; Jeff R Powell; Robert E Sharwood; David T Tissue; Oula Ghannoum Journal: Plant Cell Environ Date: 2015-12-21 Impact factor: 7.228