Research Article | Open Access
Guangjian Yan, Hailan Jiang, Jinghui Luo, Xihan Mu, Fan Li, Jianbo Qi, Ronghai Hu, Donghui Xie, Guoqing Zhou, "Quantitative Evaluation of Leaf Inclination Angle Distribution on Leaf Area Index Retrieval of Coniferous Canopies", Journal of Remote Sensing, vol. 2021, Article ID 2708904, 15 pages, 2021. https://doi.org/10.34133/2021/2708904
Quantitative Evaluation of Leaf Inclination Angle Distribution on Leaf Area Index Retrieval of Coniferous Canopies
Both leaf inclination angle distribution (LAD) and leaf area index (LAI) dominate optical remote sensing signals. The G-function, which is a function of LAD and remote sensing geometry, is often set to 0.5 in the LAI retrieval of coniferous canopies even though this assumption is only valid for spherical LAD. Large uncertainties are thus introduced. However, because numerous tiny leaves grow on conifers, it is nearly impossible to quantitatively evaluate such uncertainties in LAI retrieval. In this study, we proposed a method to characterize the possible change of G-function of coniferous canopies as well as its effect on LAI retrieval. Specifically, a Multi-Directional Imager (MDI) was developed to capture stereo images of the branches, and the needles were reconstructed. The accuracy of the inclination angles calculated from the reconstructed needles was high. Moreover, we analyzed whether a spherical distribution is a valid assumption for coniferous canopies by calculating the possible range of the G-function from the measured LADs of branches of Larch and Spruce and the true G-functions of other species from some existing inventory data and three-dimensional (3D) tree models. Results show that the constant G assumption introduces large errors in LAI retrieval, which could be as large as 53% in the zenithal viewing direction used by spaceborne LiDAR. As a result, accurate LAD estimation is recommended. In the absence of such data, our results show that a viewing zenith angle between 45 and 65 degrees is a good choice, at which the errors of LAI retrieval caused by the spherical assumption will be less than 10% for coniferous canopies.
Leaf area index (LAI) is an important parameter of vegetation canopy structure and is critical in the quantitative calculation of global mass and energy exchange between the biosphere and the atmosphere [1, 2]. Beer’s law  is widely used to retrieve LAI from gap fraction. An important factor that highly affects the retrieval accuracy of LAI based on Beer’s law is the leaf projection coefficient (G-function). The G-function is the effective projection proportion of leaves along the observing directions  and is dependent on the leaf inclination angle distribution (LAD) (assuming a uniform azimuth angle). Previous studies showed that LAD could be highly variable depending on a number of factors such as tree species, light exposure, growing season, and canopy height [5–9]. However, due to the inconvenience of in situ measurements, the spherical distribution assumption () of LAD is often used in LAI retrieval [10–13]. Some ground-based measurements utilize the gap fraction data close to a view zenith angle of 57.5°, where the values of the G-function with various LADs are close to 0.5 [14–17]. However, assuming G to be 0.5 may introduce large errors to the retrieval of LAI in other view directions.
The LAD measurement methods can be classified into two categories: direct and indirect. Direct methods measure leaf inclination angles by direct contact. A protractor with a lead hammer, an inclinometer, or a digitizer is used to measure the inclination angles of a certain number of leaves [18, 19]. These methods are time-consuming, labor-intensive, and fraught with potential errors [20, 21]. Indirect methods can be divided into several types: (i) a digital photography measurement was proposed by Ryu et al. (2010) . It uses a horizontal digital camera to view canopies and then manually measure the inclination angles of leaves which are approximately perpendicular to the viewing direction of the camera. This method was used in many studies and was then applied to Unmanned Aerial Vehicles (UAV) platforms [9, 23–25]. However, a large amount of human-computer interactions are required, and it is difficult to measure the leaf inclination angles on tall forest canopies. (ii) Another method was proposed to derive leaf inclination angles based on the relationship between light transmittance and LADs by using Beer’s law under the assumption of randomly distributed leaves [26, 27]. However, this method only provides the statistical average of leaf inclination angles rather than detailed LAD. In addition, the accuracy is affected by the nonrandom distribution of leaves and light conditions. (iii) With the development of Light Detection And Ranging (LiDAR) techniques, the use of Terrestrial Laser Scanning (TLS) has become more prevalent [21, 28–32]. However, it is difficult to extract individual needles from the LiDAR point clouds. As a result, current TLS-based methods mainly focus on the broad-leaved trees. (iv) Stereo imaging, which can be used to reconstruct vegetation canopies with photos taken from two or more positions based on the principle of geometric perspective, is a suitable approach to extract LAD. Wang et al. (2009)  reconstructed a three-dimensional (3D) corn model with photos and measured its LAD. Müller-Linow et al. (2015)  derived 3D surface models of plants from stereo images taken by two cameras aligned in a fixed geometry and computed geometric properties from them. Mobile phone photography is more portable and efficient compared with using the professional cameras. Qi et al. (2019)  proposed a new method to reconstruct 3D models of leaves using multiangle mobile photos that can be used to calculate accurate LADs.
The above methods are suitable mainly for broadleaf canopies. Convenient and efficient methods for measuring LADs for coniferous canopies have been less studied. Inspired by the method proposed by Müller-Linow et al. (2015) , we developed a portable and inexpensive measurement equipment called Multi-Directional Imager (MDI) that can capture stereo images of canopies, from which the leaf inclination angles can be computed. 3D line segment models were generated from stereo images taken from multiple directions, based on line segment detector and line-based 3D reconstruction method. Line segments can be used as image features to reconstruct the 3D scene . Some methods have been proposed using the pure line-based Structure-from-Motion (SfM) approach, which is challenging for pose estimation [37–39]. Camera pose information was used to overcome this problem by some subsequent Multiview Stereo (MVS) approaches (e.g., SURE ). However, MVS methods are typically accompanied by high computational costs. In this paper, we extracted 3D models with a low computational costs algorithm called Line3D++, developed by Hofer et al. (2015) .
In addition to the LAD, another factor that greatly affects the Beer’s law-based LAI retrieval is the clumping effect, which is caused by the nonrandomly spatial distribution of leaves in the canopy [1, 42]. Few studies both correct the clumping effect and calculate the true G-function in LAI retrieval . The clumping effect usually occurs at different spatial scales , including the large gaps-induced between-crown clumping, crown-shape clumping, and within-crown clumping due to the nonrandomness of foliage in the crown; these are difficult to be quantified. Thus, the clumping effect is not in the scope of this paper. Directly applying Beer’s law under the assumption of a randomly spatial distribution of leaves, we can obtain the effect of LAI. Given that measuring the angles of all the needles of a tree is challenging, we explored how to obtain the possible LADs and range of G-function of our field-measured species. To expand the calculation of LAD and G-function on more trees with various species, we further used existing inventory data and 3D tree models. Our objective was to explore the possible effect of LAD on effective LAI retrieval for coniferous canopies, which we achieved by the following: (1)Developing a method for retrieving LAD for coniferous branches using MDI(2)Obtaining the possible range of the G-function for the canopies of the studied Spruce and Larch species(3)Calculating LADs and G-functions of other species based on existing inventory data and 3D tree models(4)Analyzing the possible theoretical impact of LAD on Beer’s law-based LAI retrieval
Normally, the leaf area of a single needle is far smaller than that of a broad-leaved tree. It is difficult to distinguish needles in field measurement, even with the use of high-resolution digital cameras. Hence, we selected typical branch samples and measured the LADs of their needles in the laboratory. Numerous measurements were carried out to calculate the possible LADs and the range of G-function.
2.1. Field Measurement Using Multi-Directional Imager
2.1.1. Multi-Directional Imager
MDI (Figure 1) was developed based on our Multispectral Canopy Imager (MCI) . The improvement included upgrading three high-resolution digital cameras and adding a synchronous exposure device, which is useful to overcome the possible movements of the samples. MDI is a low-cost and portable instrument and can be used to obtain canopy images from multiple perspectives simultaneously without the help of any direction marker.
MDI consists of the following components: (i) three digital cameras (Canon 750D) with a suite of zoom lenses (EF-S 18-135 mm f/3.5-5.6 IS STM) per set. The CMOS size of each camera is , and the maximum resolution is per camera; (ii) a platform and supporting metal arms. The platform, which can be rotated from 0° to 360° in the azimuth direction and 0° to 90° in the zenith direction, is designed for controlling the camera’s orientation arbitrarily; (iii) a set of exposure controllers, which is used to control the simultaneous exposure of the three cameras; (iv) a tripod, which is used to support the platform and the cameras equipped on it.
Before the experiment, calibration is needed to obtain the interior orientation parameters of the cameras for the accurate measurement of the leaf inclination angles. The calibration of the MDI measuring system mainly consists of two parts: the calibration of the platform and that of the cameras. The platform was manufactured by a professional company and had been calibrated before use. The camera calibrations were carried out in the laboratory by using a checkerboard. Table 1, which can be used as a reference for selecting the camera focal length in the experiments, summarizes the theoretical maximum pixel size in an image when the actual observation distance is 10 m for two different camera resolutions ( and , respectively).
2.1.2. Study Sites and Samples
Field measurement campaigns of LADs were carried out from July 21 to July 26, 2016, in Chengde Saihanba National Forest Park (42.3°N, 117.2°E), including the local sampling of several conifer branches (Table 2): four Larch samples and three Spruce samples (see Section 4.2 for more details). There are some differences in measurement between Larch and Spruce samples: (i) for Larch sample I and II, the samples were fixed but the direction of the MDI observation changed; (ii) for Larch sample III and IV, the branches were rotated in different orientations but the MDI was fixed; (iii) for Spruce samples, both the samples and the direction of the MDI observation were fixed. This was done to test whether the direction of the MDI observation and the rotation of the branches have some influence on LAD and G-function (Details in section 4.3). In Table 2, the underlined sample ID denotes different observing directions of MDI around a specific sample; the corresponding number of photos taken by MDI are listed. In the experiment, the branch samples were scissored at different crown heights from a few representative trees. The branch samples were measured in the laboratory in one day after cutting to prevent the atrophy of the needles. The lengths of branches were measured, and the number of needle clusters and the number of needles in each cluster were counted. A white cloth was used as the background when taking photos in the laboratory to reduce the impact of background on object detection in photography.
2.2. 3D Tree Models and Inventory Data
What we did in section 2.1 is to obtain the possible LADs and range of G-function of Larch and Spruce through rotation of the branches. To investigate more species, we further used other kinds of data: (i) 3D tree models: 71 coniferous tree models of 13 species from OnyxTREE CONIFER library (http://www.onyxtree.com/conifer.html) with known true LADs (see Table 3); (ii) inventory data: 23 trees of Järvselja Scots Pine (https://rami-benchmark.jrc.ec.europa.eu/HTML/RAMI-IV/EXPERIMENTS4/ACTUAL_CANOPIES/JARVSELJA_SUMMER_PINESTAND/JARVSELJA_SUMMER_PINESTAND.php) and Ofenpass Mountain Pine (https://rami-benchmark.jrc.ec.europa.eu/HTML/RAMI-IV/EXPERIMENTS4/ACTUAL_CANOPIES/OFENPASS_WINTER_PINESTAND/OFENPASS_WINTER_PINESTAND.php) from RAMI IV. The measured LADs of these trees, one species measured in summer and the other in winter, are provided. More details about the inventory data can be found on the RAMI IV website. The number of trees, the average, and the range of tree heights for each species are summarized in Table 3. Front views of some of the studied 3D tree models from OnyxTREE are shown in Figure 2 as examples.
3.1. Estimation of Leaf Inclination Angle Distribution
3.1.1. Detection and Reconstruction of Needles
The exact leaf inclination angles can be calculated from 3D leaf models. LSD  and Line3D++  were used to generate 3D line segment models from stereo images of coniferous branches. To be specific, LSD was used to extract 2D lines from each image, and Line3D++ was used to develop 3D line models.
LSD is an efficient line segment detector that can be used to acquire accurate subpixel results . It follows the method proposed by Burns et al. (1986)  and uses a contrarian validation approach proposed by Desolneux et al. (2000)  to control false detections. LSD algorithms can be roughly divided into three steps. First, the image is segmented into a series of small continuous regions with the same gradient angle. Then, the most approximate line segment is determined in each successive small region. Finally, a validation criterion is used to control the number of false detections.
Line3D++ is a novel algorithm using line segments as fundamental features to abstract 3D scenes, which consists of several steps. First, a large number of potential line correspondences are established using epipolar geometry constraints. The epipolar geometry can be computed through known camera poses, which can be obtained by running any Structure-from-Motion (SfM) pipelines. Then, the most suitable correspondence is selected for each line segment. Hofer et al. (2017)  used a scoring formulation composed of angular similarity and positional similarity to distinguish between correct and incorrect matches. The final 3D line model is obtained by fusing 2D line correspondences through an arbitrary graph-clustering algorithm.
Figure 3 shows an example of line segment detection and reconstruction using LSD and Line3D++ algorithms. Apart from some highly occluded regions, most of the needles are detected from the original images. The result (Figure 3(c)) shows that the majority of needles are reconstructed effectively.
3.1.2. Calculation of Leaf Inclination Angle Distribution
The data processing flow chart of the LAD retrieval is shown in Figure 3. First, MDI was used to obtain the multiangle stereo images of the branch samples (Figure 3(a)). Then, dense matching and linear feature extraction techniques were used to get the orientation of each needle automatically from the coaxial stereo image pairs obtained by MDI. Finally, the view zenith angle of MDI was used to calculate the final LAD (Figure 3(d)) based on the extracted inclination angles of the needles.
Through the above steps, we can obtain the distribution of the needles in the camera coordinate system. It has to be converted to the world coordinate system to obtain the real inclination angles of the needles. From the schematic diagram of the MDI coordinate system shown in Figure 1, represents a real-world local coordinate system. is the direction of the metal arms, and is the zenith direction. represents the camera space coordinate system of the intermediate camera. The angles of the platform in the vertical direction ( in Figure 1(b)) can be read directly from the graduated collar on the rotatable platform.
represents the real vertical direction, which is transformed from the world space to the camera space. The inclination of the needle in world space is defined as where indicates the normal vector of a needle in camera space, .
The final LAD is obtained by weighting the relative areas with different leaf inclination angles.
3.1.3. Validation of the Retrieved Leaf Inclination Angles
To validate the accuracy of our method, the inclination angles of needles on a coniferous tree branch were measured manually with a protractor and were assumed to be ground-truth. It is unrealistic to measure the inclination angle of each needle directly because the needles on a branch are dense and are sheltered from each other; hence, most of the needles were cut off from the branch, and only 16 remaining needles were measured manually (Figure 4(a)). Meanwhile, 3D needle models were reconstructed from the stereo images obtained from MDI, and the inclination angles were calculated automatically. Then, the coefficient of determination () and the root mean square error (RMSE) were calculated. The results are shown in Section 4.1.
3.2. G-Function Calculation
The definition of the G-function proposed by Stenberg (2006)  was used in this study: where is the view zenith angle, is the needle inclination angle, and is the azimuth divergence angle between the needle and the observation directions.
The measured leaf inclination angles are binned to the leaf inclination angle intervals ranging from 0 to with a step of 5°. Thus, the relationship between the discrete leaf inclination angle and the G-function is where is the total number of leaf inclination angle intervals and , is the center needle inclination angle of each interval, is the leaf area fraction of the needle inclination angle interval centered at , and is the value of the G-function when the needle inclination angle equals to .
3.3. Calculating the Possible Range of G-Function of the Canopy
For the field measured species including Larch and Spruce, it is impossible to measure every needle on a tree due to the huge number of needles and highly complex canopy background. Thus, what we can obtain is just the LAD of a certain branch, not that of a tree. However, we believe that the possible range of LAD and G-function of a tree can be obtained by rotating the branches to different orientations, assuming that a tree is made up of branches in different directions. Thus, the reconstructed 3D needle leaf models were rotated in many different orientations in the 3D space to represent possible orientations of needles and branches in the real canopy, and then, the corresponding changes in LAD and G-function were studied. To obtain the 3D needle leaf models with different orientations, we used CloudCompare (http://cloudcompare.org) to rotate each reconstructed 3D needle leaf models in fifteen different orientations. The LAD and G-function were subsequently computed using the rotated 3D needle leaf models. At last, all of the possible G-functions of the Larch and Spruce samples were calculated, which can be treated as possible situations in real canopies of these two species. The real G-functions of the canopies should be in the range of these simulated G-functions due to the fact that more branches in different orientations in reality tend to smooth the change of the G-function.
For other species from inventory data and 3D tree models, the range of G-function of the canopy is calculated directly from all the trees we collected. This is due to the fact that the LAD is a statistic of leaf inclination angles and is not related to spatial distribution of trees in the canopy.
3.4. Calculation of the Impact of Leaf Inclination Angle Distribution on LAI Retrieval
The traditional Beer’s law of light transmission through a turbid medium is widely used in indirect LAI measurements [3, 52], assuming that the medium of the vegetation is homogeneous: where denotes the gap fraction in the viewing zenith angle ; is the G-function, assuming of spherical distribution, . LAI is the effective LAI assuming a random distribution of leaves without considering the clumping effect.
We assumed the true G-function value in view zenith angle as , and the relative error of LAI caused by the assumption of spherical distribution is
From this equation, we infer that if we use the spherical distribution assumption, a 10% error in the G-function results in a 10% error in Beer’s law-based LAI retrieval.
4. Results and Discussion
4.1. The Accuracy of Leaf Inclination Angles Retrieved from Stereo Photos
The leaf inclination angles of needles were measured manually as the ground-truth to validate the accuracy of our proposed method. Needles on a branch (Figure 4(a)) were manually measured, and the inclination angles were calculated automatically after they were detected. The enlarged details of the automatically extracted needles and the reconstructed point clouds are shown in Figure 4(b). As what is shown in Table 4, 14 of a total of 16 needles were extracted (except needles 11 and 15).
The comparison of manual measurements and algorithm extraction is shown in Figure 5. The algorithm performs well, with an of 0.98 and a RMSE of 1.63°. It shows that the proposed method can be used for accurate and rapid measurement of needle leaf inclination angle.
4.2. Leaf Inclination Angle Distribution and G-Function
Both the LADs and G-functions were estimated from different conifer samples: 4 Larch samples and 3 Spruce samples. Specifically, Larch sample I and II and the Spruce samples were fixed on the cantilever brackets at the time of data acquisition, and the position of MDI was moved. Sample III and IV on the cantilever brackets were manually rotated in different orientations. Photos around the samples were taken in different directions using MDI (Figure 6(a)), and at least 8 photos (details are listed in Table 2) with good quality were selected for line segment detection and 3D needle line segment reconstruction. The final LADs were calculated from the reconstructed needles (Figure 6(b)). Different trends were found in the results. For sample I and II, there were small differences in both the LADs and the mean leaf inclination angles (MLAs) measured in different directions, indicating that the observing direction of MDI has little impact on LAD. For sample III, the difference of MLAs between a31 and a32 was small, which was probably due to the relatively close orientations of them. However, there were relatively large differences in both the LADs and the MLAs before and after rotation for sample IV, and the maximum difference of MLA was about 10°.
Spruce samples were fixed on the cantilever brackets when data were acquired. Photos for different samples and the extracted LADs were shown in Figures 7(a1–a3) and 7(b1–b3), respectively. Results showed that the LADs might be different even with different samples of the same tree species, and the corresponding MLAs might have a large difference.
Figure 8 illustrates the G-function computed from abovementioned measurement data in this section. The G-function values calculated using the data obtained in different directions of the same conifer sample were close to each other, and the overall trend was consistent except for sample IV (black lines in Figure 8(a)). However, the G-function values of the three Spruce samples (Figure 8(b)) differ greatly.
4.3. Possible Range of the G-Function by Rotating the Reconstructed Needles
The main purpose of this section is to study the changes in LADs and G-functions with different needle orientations in the 3D space. We assume that the possible range of the G-function of the trees can be obtained by arbitrary rotations of the branches.
Larch sample IV-a43 was used as an example to illustrate the experimental processes and results. First, each reconstructed 3D needle leaf model was rotated in 15 different orientations in the 3D space using CloudCompare (Figure 9). We saved the rotated 3D needle leaf models and computed LADs (Figure 10) and G-functions (Figure 11).
The other remaining samples were also processed according to the above steps. Several G-functions to represent the Larch and Spruce samples in the 3D space were acquired (Figure 12). Figure 12 contains the G-function calculated from both the original reconstructed 3D needle leaf models and those after rotation.
Figures 10–12 show that large differences exist in the corresponding LADs and G-functions when the 3D needle leaf models are rotated in different orientations in the 3D space, which also exists in MLA. The range of G-functions is largest when the view zenith angle is 0°, which is 0.13 for Larch samples and is up to 0.21 for Spruce samples. However, the maximum range of G-function is only 0.05 and 0.09 for Larch and Spruce samples, respectively, when the view zenith angles are between 40° and 70°, which is commonly used in field measurement campaigns. It can be inferred that changes in the values of the G-function are not significant in this range across the whole forest, because a real canopy has a greater number of randomly orientated branches and needles.
In addition, the overall variation range of the G-functions of Larch samples is smaller than that of Spruce samples. The reason may lie in the different growth structure of the two different conifer species.
4.4. G-Functions of Inventory Data and 3D Tree Models
The G-functions of trees from RAMI IV inventory data and 3D tree models with known LADs were also calculated. The range of G-function is the largest when the view zenith angle is 0°, which is 0.09 for the inventory data (Figure 13(a)) and is up to 0.31 for the studied 3D tree models (Figure 13(b)). However, the maximum range of the G-function is only 0.02 and 0.09 when the view zenith angles are in 40°~70° and is much smaller when the view zenith angles are in 45°~65°. In addition, the overall variation range of the G-function of the inventory data is smaller than that of the 3D tree models, which is because both the number of trees and tree species of the 3D tree models are significantly larger than those of the inventory data, i.e., the 3D tree models reflect more conditions of realistic coniferous trees.
4.5. The Effects of Leaf Inclination Angle Distribution on LAI Retrieval
Due to the inconvenience of in situ measurements of LAD of coniferous trees, the spherical distribution assumption is usually used in LAI retrieval. Previous studies showed that a spherical distribution is not a valid assumption for most broadleaf tree species . However, relevant research in coniferous species is still lacking. In this section, whether the spherical distribution () is a valid assumption for coniferous canopies and the possible impact on LAI retrieval will be discussed. Specifically, we are interested in three kinds of view zenith angles: (i) 40°~70°, which is commonly used in field measurement campaigns; (ii) 0°, considering that the view zenith angle for spaceborne LiDAR instruments including Geoscience Laser Altimeter System (GLAS) and the Global Ecosystem Dynamics Investigation (GEDI) are all close to 0° (up to 1° for Geoscience Laser Altimeter System (GLAS) , and up to 6° for Global Ecosystem Dynamics Investigation (GEDI) ); (iii) 0°~15°, considering that the view zenith angle for airborne LiDAR is usually less than 15° and is widely used in LAI retrieval .
The relative errors of LAI retrieval under a constant G-function assumption of 0.5 were compared with those retrieved using the true G-function value for coniferous canopies (Figure 14). Results show that the relative errors of retrieved LAI depend on the view zenith angles and increase gradually with the deviation from 57.5°. When the view zenith angles are in 40°~70°, the relative errors of LAI are less than 15%. When the view zenith angle is at 0°, LAI could be underestimated by as much as 53%; when the view zenith angles range of 0°~15°, the relative errors of LAI are in the range of -53%~9%. However, the relative errors are less than 10% when the view zenith angles are in the range of 45°~65°.
Based on the above analysis, we recommend calculating LAD accurately in LAI retrieval, especially at nadir viewing. If the exact LAD measurement data is absent, we recommend using the remotely sensed data captured in the zenithal angle between 45° and 65°. In such cases, the possible LAI retrieval errors caused by fixing the G-function value as 0.5 is less than 10%.
4.6. Limitations and Suggestions for Future Research
It is difficult to obtain a general knowledge of the effect of the LAD on LAI retrieval for coniferous canopies just based on the field measurement. This is due to the fact that the field measurement is limited to a few branches of two species, since it is challenging to measure all the branches of a tree. Thus, the LAD of a tree is hard to be obtained. Two strategies were used in this study to overcome these problems: (i) rotating branches to obtain the possible range of the G-function and (ii) collecting as much data as possible to find a general impact of leaf inclination angles on LAI retrieval. Inevitably, there are some limitations of this work which should be further studied: (1)More branches can be measured in the future, considering that the selected branch samples may have some influence on the LAD and G-function estimation(2)More tree models can be collected to make the finding more general(3)More data of the same species can be collected in different seasons since the angles of leaves also change with the season. Even though both LAD data measured in summer and winter are included in the inventory data of RAMI IV, and the 71 tree models from a conifer database already contain diverse branches and leaves, which we believe can indirectly take the impact of season into consideration, a careful study on this issue is still an interesting topic(4)Both the LAD and clumping effect can be analyzed on the influence of true LAI retrieval. This study only focused on the impact of LAD on effective LAI. Previous studies showed that the clumping effect might cause a 30%~70% underestimation of true LAI [42, 57, 58]. Computer simulation, which can be used to generate diverse forest scenes with known gap fraction, LAD, and true LAI, might be a pathway to study the coupling effects of the clumping and the LAD to make sense of the total LAI retrieval error
Leaf inclination angle distribution (LAD) is an important factor affecting Beer’s law-based LAI retrieval. Despite the high variability of LAD in reality, a spherical distribution assumption is often used for coniferous canopies due to the difficulties in measuring it. However, the error caused by this assumption has been seldom studied. We estimated the possible range of the G-function of two species by rotating the reconstructed needles of the branches measured by our developed equipment—MDI, which was an alternative to the manual measurement of the leaf inclination angle. To study more species, both 3D tree models and existing inventory data with known LADs were used. Results show that the range of the G-function is highly variable at different view zenith angles, indicating the necessity to measure LAD accurately to improve LAI retrieval. We found that the relative error of LAI with spherical distribution assumptions could be as large as -53% in the zenithal view direction, which is nonnegligible for LAI retrieval from airborne and spaceborne LiDAR. Besides, our results show that 45°~65° is a good range of the view zenith angle to reduce the impact of LAD on LAI retrieval (relative error less than 10%) for coniferous canopies under the assumption of spherical distribution when the field-measured data is absent.
The data is freely available upon request.
General. Thank you for anonymous reviewers who gave constructive suggestions.
Conflicts of Interest
The authors declare no competing interests.
G.Y. proposed the method and wrote the paper with J.L., H.J., and X.M. conceptualized the method and revised the paper. F.L., J.Q., and R.H. contributed to the field measurement, and D.X. and G.Z. revised the paper.
This work was supported by the key program of the National Natural Science Foundation of China (NSFC) (Grant No. 42090013); Guangxi Innovative Development Grand Grant under the grant number: Guike AA18118038; and the China Scholarship Council, Grant No. 201906040055.
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