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Analysis of the Influence of Grating Plate on the Internal Illumination Uniformity of Zigzag Photovoltaic Greenhouse

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22 December 2023

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26 December 2023

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Abstract
As one of the main projects of facility agriculture promotion, the photovoltaic greenhouse has the problems of photovoltaic power generation competing for light with crop production, strong indoor chiaroscuro, and uneven light distribution. The internal light uniformity is tested by a zigzag greenhouse model to compare the light transmission effects of different light-transmitting materials applied to photovoltaic greenhouses. 20 line\inch 3mm and 30 line\inch 3mm, 40 line\inch 2mm, 25 line\inch 4mm grating plates, 2mm, and 3mm thick ordinary glass were used as light transmitting components, and the light intensity and light uniformity in the greenhouse were the measurement indicators. The results show that the use of grating plates as covering material can improve the light intensity at the intersection of light and dark, but the overall light transmittance is not as good as glass, because it is plastic which is easy to age with low light transmittance. It can also improve the use of land under the shade of photovoltaic modules to provide a better growth environment for crops. Test results show that the use of a 2mm thick 40-line grating plate can maximize the light intensity of the greenhouse, and the peak value can reach 69336 Lx. In sunny weather, the light intensity from point G to point I in the greenhouse is greater than 20,000 Lx, and the light environment in other areas is between 5,000 Lx and 20,000 Lx, which is suitable for planting shade-loving crops.
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Subject: Biology and Life Sciences  -   Agricultural Science and Agronomy

1. Introduction

At present, the energy structure at home and abroad is mainly based on fossil fuels. However, fossil fuels are non-renewable energy. With the increasing demand for energy and the continuous exploitation and consumption of fossil energy, it is urgent to develop renewable energies, such as wind power, hydropower, solar energy, etc. Among them, solar energy is the most popular energy, and photovoltaic power generation is one of the main forms of solar energy utilization. Photovoltaic power generation includes rooftop photovoltaic, water photovoltaic, and traditional photovoltaic ground power stations. A photovoltaic greenhouse is an application form of photovoltaic power generation, which is mainly used in agricultural production, especially in areas with limited land resources or lack of power supply. Photovoltaic greenhouse converts solar energy into electricity, which can be directly supplied to lighting, heating, ventilation, and other equipment and automation systems in the greenhouse, and can also be connected to power grids [1]. Photovoltaic greenhouse technology is closely related to sustainable development. The use of clean energy can reduce the dependence on traditional power grids, use less fossil energy, improve the utilization rate of solar energy, and contribute to environmental protection and sustainable economic development. In addition, when used properly, photovoltaic greenhouse can also provide a good growing environment, such as suitable temperature, light, and ventilation conditions, to promote the growth of crops and increase yields. However, the shading of photovoltaic modules will inevitably reduce the light intensity in the greenhouse, change the light distribution characteristics in the greenhouse, and affect the growth of plants. At present, the scattering film is mainly used as the light-transmitting component, which can expand the illumination area and improve the light distribution characteristics in the greenhouse, but the effect is not satisfactory. There are still some challenges in photovoltaic greenhouse technology, such as the cost, efficiency, and reliability of photovoltaic panels, as well as technical issues in terms of light uniformity, ventilation, and temperature control inside the greenhouse, and solving these challenges requires continuous technological innovations and improvements.
In order to solve the problem of uneven light distribution in photovoltaic greenhouses caused by the shading of photovoltaic cell modules from the perspective of light-transmitting modules on the greenhouse roof, the grating plates with high scattering and high transmittance used as light-transmitting modules to improve the light distribution in zigzag photovoltaic greenhouses can effectively improve the light intensity in the greenhouse [2]. Liu Chengyu, et al. [3] pointed out that a large number of experimental studies have been carried out on photovoltaic greenhouses. The experimental results of these studies have summarized the problems and opinions regarding the research and development of photovoltaic greenhouses, as well as the relatively low utilization rate of light energy and the high maintenance price of photovoltaic equipment, and it is particularly important to ensure that the light uniformity in the photovoltaic greenhouse is suitable for plant growth and ensure the thermal insulation function of the greenhouse while not affecting the operation of photovoltaic power generation in the greenhouse [4].
In this study, grating panels with different thicknesses and number of lines were used as photovoltaic greenhouse light-transmitting modules, and ordinary glass was used as the control to test the light intensity and uniformity in the greenhouse. The use of grating panels as greenhouse roof covering material was evaluated.
As shown in Figure 1, the grating plate is a plastic material with one side extruded into a cylindrical line and one side as a complete plane, and the cylindrical line spacing is equal to that called "grating". The light transmittance of the grating plate used in this experiment is 93.77%, and the spectroscopic light waves of the grating will be diffracted at each slit, and the light waves diffracted through all slits will interfere to form interference fringes and be localized to infinity. When sunlight is incident on the grating plate, the area that can be irradiated by the light passing through the grating plate is greater than the area of the grating plate itself [5]. As a polymer light scattering material, the grating plate converts the parallel direct light into an isotropic surface light source and expands the illumination area, thus solving the problem of illumination uniformity to a certain extent.

2. Materials

2.1. Zigzag photovoltaic greenhouse

The test greenhouse is a zigzag photovoltaic greenhouse [WS-GFJ-X.X(HD)] developed from the patented shed greenhouse of Professor Liu Jian of Hainan University: A Combined Photovoltaic Greenhouse Roof Structure (ZL201621352420.7) [6]. The span of the photovoltaic greenhouse is 5.5-7.5m, the bay is 4m, the shoulder height is 2.2-2.5m, and the top height is 3.4-3.7m, as shown in Figure 2 and Figure 3.
Combined with the climatic characteristics of the Hainan hot area and the needs of the solar and thermal environment of vegetable planting, the standard sawtooth photovoltaic vegetable greenhouse reasonably optimizes the layout of the roof structure and uses photovoltaic modules as roof covering materials to replace some traditional transparent covering materials such as films. Because of its reasonable structure, the ground planting utilization rate becomes higher, and the light and heat environment are more suitable, which can achieve the goal of not reducing the output of vegetable production compared with open field planting, and can ensure the uninterrupted production of photovoltaic vegetable greenhouses [7].
The research on indoor lighting problems of zigzag photovoltaic greenhouses mainly focuses on the location of the greenhouse (latitude and longitude, altitude, etc.), orientation, structure, light characteristics of covering materials and enclosure materials (light transmittance, reflectivity, etc.), surrounding features, weather and other factors that have a great impact on the lighting in the greenhouse. The problem of shading and lighting in greenhouses also needs to solve the problem of reasonable distribution of sunlight in crops and photovoltaic power generation, and to maximize the benefits of agriculture and photovoltaic industry.

2.2. Zigzag photovoltaic greenhouse model

The model greenhouse is constructed according to the scale of 1:11 with a span of 500 mm, a column height of 160 mm, and a bay of 600 mm. 20mm×20mm aluminum profiles were used as the model greenhouse skeleton material. The azimuth of the greenhouse is set to due south, and the roof of the south slope is facing the sun [8]. Figure 4, Figure 5 and Figure 6 shows the structural diagram and the physical drawing of the greenhouse model, the column and the roof beam of the model are connected by a rotating corner chain, the column and the beam part are connected by a vertical corner piece, the roof beam and the roof beam are connected by a vertical turning angle piece, and are covered with 40 mesh insect nets around it.

3. Experimental design and field management

3.1. Selection of test measurement sites

As shown in Figure 7, six lines were set in the east-west direction of the greenhouse, which were respectively recorded as N1 to N6 at the distance from the 5.5.cm, 14.50cm, 23.50cm, 32.50cm, 41.50cm, and 50.50cm of the gable on the east side. There were nine points on each line, which were evenly distributed in the east-west direction and north-south direction from the inside of the greenhouse. The distances were 3.0cm, 8.0cm, 13.0cm, 18.0cm, 23.0cm, 28.0cm, 33.0cm, 38.0cm, and 43.0cm, which were recorded as point A to point I.

3.2. Experimental time

The outdoor experiment was conducted at the Agricultural Science Base of Danzhou Campus of Hainan University (19°11’N, 108°56’E) from 10:00 to 16:00 on June 1, 2023 (sunny) and from 10:00 to 16:00 on June 2 (sunny).
U0=Emin/Eav

3.3. Experimental process

First of all, according to the formula mentioned in the Environmental Engineering of Facility Agriculture edited by Zou Zhirong and Shao Xiaohou [9]: the number of inclination angles of the south roof β>90°-40°-α=50°-α (α is the solar altitude angle at a certain time), the latitude of Danzhou at this time is 19°, and the solar regression movement from June 1 to 2 is moving from south to north, the days are getting longer, and the sunshine time in the northern hemisphere is all lengthened, we assume that the solar altitude angle is 38°, and 12° is selected as the inclination angle of the south roof; secondly, according to the test schedule in Table 1, the relationship between the light transmitting components of different specifications and the light transmission of the point zone was tested one by one. Finally, Origin64 software was used for data analysis and comparison [10].

4. Results

4.1. Light distribution characteristics of the corresponding area of the light-transmitting material in the greenhouse

4.1.1. Characteristics of light distribution in the north-south direction of the greenhouse

As shown in Figure 8 below, the largest theoretical solar altitude angle is at 90 degrees when not considering the difference in the Tropic of Capricorn, and Figure 8 shows the north-south light distribution characteristics of the corresponding area of each material during this time, which is at 12:00. Combined with the analysis method of Li H et al. [11], the relevant lighting characteristics were analyzed by the one-day variation law and the significance Duncan analysis was performed on this basis.
On the whole, the light intensity from point A to point E is significantly lower than that from point F to point I, and the highest light intensity is at point G or H. In the southern area, the scattered light entering from the south increases the illumination intensity of point A, which is obviously higher than that of points B and C. In the middle area, the growth trend from point D to point E is lower than that from point E to point F, and the illuminance of glass at point F is greater than that of grating plate. The light intensity from point G to point H in the back-end area is generally greater than that of the grating plate, while point I is the opposite [12].

4.1.2. North-south light distribution in the greenhouse

The distribution of light intensity in the north-south direction in different time periods in the greenhouse is shown in Figure 9, Figure 10, Figure 11, Figure 12 and Figure 13, and in general, the influence of cloud cover is excluded Choab N et al. [13] Bulik, T, Piacentini et al. [14] The distribution trend of light intensity in the north-south direction of each light transmitting material in each time period is as follows: the light intensity from point B to point G or H gradually increases and reaches the peak value. According to the analysis methods of Igoe, D, Turner et al. [15], and Ayet A et al. [16], it is inferred that point A is affected by the scattered light from the ground to the south, and the light intensity is greater than that of point B. The light intensity of glass as a light-transmitting component of a greenhouse is generally greater than that of grating panels [17].

4.2. Data processing and analysis

As shown in Figure 14, Figure 15, Figure 16, Figure 17, Figure 18 and Figure 19, the variation of the illuminance of each material over time is distributed over time and appears in a "W" shape assuming that cloud interference is excluded [18,19]. The illumination intensity of each dot zone of each material will reach a small peak at 12:30 because the solar altitude angle is the highest and the light intensity is strongest at noon, and the illumination of each dot zone at 11:30 and 13:30 is lower than the value of 12:30. The illumination of each point at 10:30 and 14:30 is greater than that at 11:30 and 13:30, because the light measured at the N1 or N6 lines at the measurement points in the greenhouse is directly through the insect net and is not refracted through the light transmitting element and obscured by the greenhouse skeleton [20]. In fact, the light intensity of the outdoors changes at any time [21], the cloud layer is always moving, and the measurement process takes time, which makes the measurement results not exactly the same as the conjecture. Meanwhile, considering the evaporation of water vapor is the highest when the solar altitude angle at noon, the blocking of water vapor will also affect the measurement results [22,26,27,28].

4.3. Light uniformity in the greenhouse

4.3.1. Light uniformity and variation coefficient

Table 2, Table 3, Table 4, Table 5, Table 6 and Table 7 shows the light uniformity and variation coefficient in the model greenhouse at different time periods [23] when the grating plate and glass are used as light-transmitting components. The data varied a lot due to the different measurement times of each point and the rapid change of the atmospheric cloud layer [24]. The results of data processing are as follows:
In Table 2, the illumination uniformity of the 20-line 3mm thick grating plate as the light transmitting module from point A to point I and from 10:30 to 14:30 increased with time, the variation coefficient increased with time, and the variance decreased with the increase of time.
In Table 3, the illumination uniformity of the 25-line 4mm thick grating plate as the light transmitting module from point A to point I and from 10:30 to 14:30 decreased with the increase of time, the variation coefficient increased with the increase of time, the variance increased with the increase of time, the average point G, point H and point I decreased with the increase of time, and the other points increased with the increase of time.
In Table 4, the illumination uniformity of the 30-line 3mm thick grating plate as the light transmitting module from point A to point I and from 10:30 to 14:30 decreased with the increase of time, the variation coefficient increased with time, the variance increased with the increase of time, and the variance increased with the increase of time.
In Table 5, the illumination uniformity of the 40-line 2mm thick grating plate as the light transmitting module from point A to point I and from 10:30 to 14:30 increased with time, the variation coefficient decreased with the increase of time, and the variance decreased with the increase of time.
In Table 6, the illumination uniformity of 2mm thick glass as the light transmitting module from point A to point I and from 10:30 to 14:30 increased with the increase of time, the variation coefficient decreased slightly with the increase of time, the rest of the points increased with time, the variance except for point A increased slightly with time, the variance decreased slightly with the increase of time, the variance except for point A increased slightly with time, and decreased with the increase of time, the average point A, point F, point G, point H increased with the increase of time, and point B, point C, point D, point E, and point I decreased with the increase of time.
In Table 7, the illumination uniformity of the 3mm thick glass translucent module from point A to point I and from 10:30 to 14:30 decreased with the increase of time, the variation coefficient increased with the increase of time, the variance increased with the increase of time, the average points A, B, C, D, E, and F increased with the increase of time, and the average points G, H and I decreased with the increase of time.

5. Discussion

1. The use of grating plate as the light transmitting module can improve the light uniformity of the light and dark zone junction area in the low light area caused by the shading of photovoltaic modules in the zigzag photovoltaic greenhouse. However, the light transmittance of the grating plate is lower than that of the translucent glass, and the light entering through the translucent roof will be reduced, causing a low utilization rate of sunlight and lower light intensity under the grating plate in the greenhouse compared with ordinary translucent glass. From the perspective of light distribution characteristics, the grating plate has a high scattering feature to refract the light to an area larger than its own size, which improves the light intensity of some dark band areas, and the increased intensity would decrease with distance. Therefore, grating plates are a good way to deal with the need to block a part of the light and increase the light intensity near the band area. At the same time, it provides ideas for improving the light environment in the greenhouse by using the optical path of light transmitting materials to light.
2. In addition to this experiment, the greenhouse model that can change the inclination angle of the roof can also be used to determine the lighting environment in the greenhouse under different roof coverage rates. Since the model greenhouse is based on the size of the actual greenhouse and is scaled down, the light intensity in the room is affected by the skeleton. At the same time, due to the volume of the measuring instrument, the existing model fails to measure the light intensity in the greenhouse from different heights.

6. Conclusions

In this study, on the basis of constructing a zigzag photovoltaic greenhouse model, the light intensity of the model greenhouse under different roof inclination angles and different simulated solar altitude angles was compared through pre-experiments using grating panels and ordinary glass as light-transmitting modules, and the optimal roof inclination angle range suitable for field experiments was obtained. On this basis, the illumination intensity of the model greenhouse was measured when the grating plate and ordinary glass were used as the light transmitting components in different time periods of the day, and the illuminance of each measurement point was obtained and compared [25]. The following main conclusions were obtained:
(1) In the outdoor experiment, the roof inclination angle of the model greenhouse is 12 degrees, and the roof coverage rate is 41.92%. From the experimental results, it is not difficult to see that the light in the greenhouse with the light transmitting component is ordinary glass, the dark band is concentrated in the front end (A, B, C points) area, the bright band is concentrated in the rear end (G, H, I points) area, and the middle (D, E, F points) area belongs to the light and dark junction zone. At noon, when the grating plate is used as the light transmitting component, the uniformity of the points (A to I) in the north-south direction is the same as in the east-west direction. The light intensity in the front area of the greenhouse is the same as that of the grating group and the glass group. The grating plate can be used as the light transmitting module to reduce the light intensity of the bright belt, improve the light intensity at the intersection of light and dark, and expand the planting area in the photovoltaic greenhouse.
(2) When the grating plate is used as the light transmitting module, the light intensity from point G to point I in the greenhouse is greater than 20000Lx, and the light environment in other areas is less than 20000lx and greater than 5000Lx, which is suitable for planting shade-loving crops, and the light intensity of the 40-line specification with a thickness of 2mm can be maximized to improve the light intensity of the greenhouse. At present, the cost of grating plate on the market is about 90-120 yuan per square meter, which is roughly the same as the cost of glass, and there is the possibility of actual production.
In summary, grating panels can be used as greenhouse covering materials to improve the light intensity at the intersection of light and dark bands in photovoltaic greenhouses.

Author Contributions

Conceptualization, J.L.; methodology, B.W.; software, Y.S.; validation, Y.S.; formal analysis, B.W.; investigation, Y.S.; resources, B.W.; data curation,B.W.; writing—original draft preparation, Y.S.; writing—review and editing, B.W.; visualization, Y.S.; project administration, J.L.; funding acquisition, J.L. All authors have read and agreed to the published version of the manuscript.

Funding

This research was supported by China Huaneng Group Co., Ltd. Headquarters Technology Project, grant number HNKJ22-HF77; Hainan Provincial Natural Science Foundation of China, grant number 322RC583.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

All data are presented in this article in the form of figures and tables.

Acknowledgments

We would like to thank the Innovation and utilization team of tropical melon crop genetic germplasm, Hainan University.

Conflicts of Interest

The authors declare no conflict of interest.

Nomenclature

U0 Illumination uniformity
Emin Minimum illumination value
Eav Average illuminance value

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Figure 1. Grating plate.
Figure 1. Grating plate.
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Figure 2. Schematic diagram of zigzag photovoltaic greenhouse structure (mm).
Figure 2. Schematic diagram of zigzag photovoltaic greenhouse structure (mm).
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Figure 3. A real picture of the zigzag photovoltaic greenhouse.
Figure 3. A real picture of the zigzag photovoltaic greenhouse.
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Figure 4. Schematic diagram of greenhouse model structure (mm).
Figure 4. Schematic diagram of greenhouse model structure (mm).
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Figure 5. North end of the field experiment model (insect net can be opened).
Figure 5. North end of the field experiment model (insect net can be opened).
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Figure 6. Side view of the field experiment model.
Figure 6. Side view of the field experiment model.
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Figure 7. Schematic diagram of the front and back sections of the light intensity measurement point (mm).
Figure 7. Schematic diagram of the front and back sections of the light intensity measurement point (mm).
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Figure 8. 12:00 a.m. The light distribution of each point in the north-south direction of the corresponding area in each plate greenhouse.
Figure 8. 12:00 a.m. The light distribution of each point in the north-south direction of the corresponding area in each plate greenhouse.
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Figure 9. 10:30 a.m. Average light intensity at each point.
Figure 9. 10:30 a.m. Average light intensity at each point.
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Figure 10. 11:30 a.m. Average light intensity at each point.
Figure 10. 11:30 a.m. Average light intensity at each point.
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Figure 11. 12:30 p.m. Average light intensity at each point.
Figure 11. 12:30 p.m. Average light intensity at each point.
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Figure 12. 13:30 p.m. Average light intensity at each point.
Figure 12. 13:30 p.m. Average light intensity at each point.
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Figure 13. 14:30 p.m. Average light intensity at each point.
Figure 13. 14:30 p.m. Average light intensity at each point.
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Figure 14. The average illumination intensity of each point of the 20line\inch 3mm thick grating plate at different times (Illuminance at different time points from point A to point I).
Figure 14. The average illumination intensity of each point of the 20line\inch 3mm thick grating plate at different times (Illuminance at different time points from point A to point I).
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Figure 15. The average illumination intensity of each point of the 25line\inch 4mm thick grating plate at different times (Illuminance at different time points from point A to point I).
Figure 15. The average illumination intensity of each point of the 25line\inch 4mm thick grating plate at different times (Illuminance at different time points from point A to point I).
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Figure 16. The average illumination intensity of each point of the 30line\inch 3mm thick grating plate at different times (Illuminance at different time points from point A to point I).
Figure 16. The average illumination intensity of each point of the 30line\inch 3mm thick grating plate at different times (Illuminance at different time points from point A to point I).
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Figure 17. The average illumination intensity of each point of the 40line\inch 2mm thick grating plate at different times (Illuminance at different time points from point A to point I).
Figure 17. The average illumination intensity of each point of the 40line\inch 2mm thick grating plate at different times (Illuminance at different time points from point A to point I).
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Figure 18. The average light intensity of each dot band of 2 mm thick glass at different time (Illuminance at different time points from point A to point I).
Figure 18. The average light intensity of each dot band of 2 mm thick glass at different time (Illuminance at different time points from point A to point I).
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Figure 19. The average light intensity of each dot band of 3 mm thick glass at different time (Illuminance at different time points from point A to point I).
Figure 19. The average light intensity of each dot band of 3 mm thick glass at different time (Illuminance at different time points from point A to point I).
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Table 1. Experimental arrangement.
Table 1. Experimental arrangement.
Roof inclination
angle\°
Point Translucent components Data Acquisition
(Time)
12 A Translucent glass: 10:30
B 2mm glass 11:30
C 3mm glass 12:00
D Grating plate: 12:30
E 20 line\inch 3mm 13:30
F 30line\inch3mm 14:30
G 25 line\inch 4mm
H 40 line\inch2mm
I
Table 2. Light uniformity and variation coefficient of 20line\inch 3mm grating transmittance component.
Table 2. Light uniformity and variation coefficient of 20line\inch 3mm grating transmittance component.
Time 20line\inch 3mm A B C D E F G H I
10:30 Average(Lux) 13204 19023 16967 17407 18648 30788 42619 51477 47391
Variance 6540 22226 19731 19084 14952 13310 7521 5145 8753
Cv 0.495 1.168 1.163 1.096 0.802 0.432 0.176 0.100 0.185
Illumination(%) 68.27 29.86 31.12 33.93 47.29 69.89 88.47 93.12 87.35
11:30 Average(Lux) 9048 8280 8264 9791 21463 37555 49452 43701 29714
Variance 829 2293 2334 1469 7380 19831 28091 25080 11564
Cv 0.092 0.279 0.282 0.150 0.344 0.528 0.568 0.530 0.389
Illumination(%) 94.48 81.46 81.24 86.97 61.38 39.35 34.41 38.78 55.07
12:30 Average(Lux) 9028 8038 8154 9658 18696 36957 53929 52073 32435
Variance 691 2395 2417 1724 4369 17637 30407 29221 14127
Cv 0.077 0.298 0.296 0.178 0.234 0.477 0.564 0.542 0.436
Illumination(%) 94.50 79.81 81.84 89.51 75.73 45.28 35.27 37.43 50.33
13:30 Average(Lux) 9658 6819 6363 7419 11937 25959 45146 46941 35807
Variance 371 661 623 557 2081 847 1631 620 403
Cv 0.038 0.097 0.098 0.075 0.174 0.033 0.036 0.012 0.011
Illumination(%) 97.25 90.36 94.24 95.22 80.80 96.31 96.94 98.56 98.71
14:30 Average(Lux) 10925 7501 6888 7732 12879 26428 45861 52064 37354
Variance 236 672 680 587 2602 2088 598 2253 44
Cv 0.022 0.090 0.099 0.076 0.202 0.079 0.013 0.043 0.001
Illumination(%) 98.40 91.94 93.22 94.86 79.45 91.40 99.02 95.20 99.92
Table 3. Light uniformity and variation coefficient of 25line\inch 4mm grating transmittance component.
Table 3. Light uniformity and variation coefficient of 25line\inch 4mm grating transmittance component.
Time 25line\inch 4mm A B C D E F G H I
10:30 Average(Lux) 7396 5065 4822 5164 6655 22408 54588 62107 50615
Variance 355 339 292 612 845 2064 3541 2908 3423
Cv 0.048 0.067 0.060 0.119 0.127 0.092 0.065 0.047 0.068
Illumination(%) 95.54 92.42 93.06 87.17 85.35 94.28 94.56 95.85 93.81
11:30 Average(Lux) 8112 6979 7042 8397 18387 63385 69224 70738 27373
Variance 347 800 918 745 1173 4378 1649 2320 3084
Cv 0.043 0.115 0.130 0.089 0.064 0.069 0.024 0.033 0.113
Illumination(%) 96.59 90.7 89.51 92.99 95.94 92.03 97.35 96.22 87.24
12:30 Average(Lux) 9381 7627 8062 9429 12317 48343 73348 74430 41962
Variance 540 468 615 412 755 7606 8581 7972 12486
Cv 0.058 0.061 0.076 0.044 0.061 0.157 0.117 0.107 0.298
Illumination(%) 94.52 95.11 94.92 95.22 94.04 83.84 87.28 88.4 65.64
13:30 Average(Lux) 10104 9750 9164 11042 12616 25106 42049 45063 33875
Variance 1211 4999 4936 6048 2943 6374 19338 22079 13807
Cv 0.120 0.513 0.539 0.548 0.233 0.254 0.460 0.490 0.408
Illumination(%) 91.56 69.21 64.09 64.40 81.90 70.71 47.25 44.30 53.65
14:30 Average(Lux) 12001 20822 13874 12921 12601 30164 50966 53427 44685
Variance 2623 23121 11788 8119 3735 9618 5415 6994 3589
Cv 0.219 1.110 0.850 0.628 0.296 0.319 0.106 0.131 0.080
Illumination(%) 82.33 34.12 49.32 59.76 78.10 79.42 87.79 85.88 92.01
Table 4. Light uniformity and variation coefficient of 30line\inch 3mm grating transmittance component.
Table 4. Light uniformity and variation coefficient of 30line\inch 3mm grating transmittance component.
Time 30line\inch 3mm A B C D E F G H I
10:30 Average(Lux) 8011 5681 5429 6154 8516 21483 40911 53604 43729
Variance 623 314 221 369 762 2041 1320 810 943
Cv 0.078 0.055 0.041 0.060 0.089 0.095 0.032 0.015 0.022
Illumination(%) 91.18 93.62 95.44 94.21 93.37 94.32 97.12 98.94 97.83
11:30 Average(Lux) 8284 7163 7400 8724 18439 45389 59922 59721 28496
Variance 32 910 1243 910 4871 1065 3915 2257 7023
Cv 0.004 0.127 0.168 0.104 0.264 0.023 0.065 0.038 0.246
Illumination(%) 99.76 92.24 88.06 93.97 74.35 97.44 92.46 95.64 74.01
12:30 Average(Lux) 8766 7496 7453 8850 13514 42574 60516 60966 34265
Variance 257 1370 1240 1178 743 4757 8019 8106 5524
Cv 0.029 0.183 0.166 0.133 0.055 0.112 0.133 0.133 0.161
Illumination(%) 97.58 87.98 90.22 91.38 94.96 87.65 85.8 86.97 81.71
13:30 Average(Lux) 10004 9421 9822 10729 12250 25349 41733 40815 31104
Variance 1007 4856 5564 5299 2827 6305 18830 18184 10752
Cv 0.101 0.516 0.566 0.494 0.231 0.249 0.451 0.446 0.346
Illumination(%) 93.45 66.27 63.77 66.86 84.47 73.61 47.95 48.83 60.1
14:30 Average(Lux) 11645 19694 13903 20654 12680 25656 41968 51813 41898
Variance 1454 21146 11520 21417 3433 3852 2897 4085 1971
Cv 0.125 1.074 0.829 1.037 0.271 0.150 0.059 0.079 0.047
Illumination(%) 92.41 35.91 48.63 37.28 80.91 84.56 95.57 91.14 96.06
Table 5. Light uniformity and variation coefficient of 40line\inch 2mm grating transmittance component.
Table 5. Light uniformity and variation coefficient of 40line\inch 2mm grating transmittance component.
Time 40line\inch 2mm A B C D E F G H I
10:30 Average(Lux) 9405 11212 12172 9641 12899 20918 38975 47467 37986
Variance 845 8610 11568 6609 9737 2795 16851 24483 19033
Cv 0.091 0.768 0.950 0.686 0.755 0.134 0.432 0.516 0.501
Illumination(%) 90.85 50.88 41.87 56.51 50.87 85.18 50.30 40.44 42.14
11:30 Average(Lux) 9427 8627 8439 10027 19644 43479 51796 69087 28332
Variance 1190 2989 2872 2065 5843 25311 30460 3758 6618
Cv 0.126 0.346 0.340 0.206 0.297 0.582 0.588 0.054 0.234
Illumination(%) 91.34 78.53 78.16 86.61 66.10 32.85 32.10 94.25 73.18
12:30 Average(Lux) 9503 7830 7856 9000 13836 42032 54445 62260 45913
Variance 348 1001 1058 655 1104 4201 17210 12000 19112
Cv 0.037 0.128 0.135 0.073 0.080 0.100 0.316 0.193 0.416
Illumination(%) 97.71 90.29 89.38 92.20 92.94 90.50 69.21 82.21 55.49
13:30 Average(Lux) 9021 6865 6417 7534 11112 32497 52424 53927 37280
Variance 428 800 912 655 634 2331 1324 1066 1625
Cv 0.047 0.117 0.142 0.087 0.057 0.072 0.025 0.020 0.044
Illumination(%) 96.76 93.04 87.64 91.52 94.55 93.54 97.31 97.84 96.26
14:30 Average(Lux) 12096 8644 7912 8880 11863 27015 51228 53309 43105
Variance 832 899 653 684 623 1454 3546 4118 3685
Cv 0.069 0.104 0.083 0.077 0.053 0.054 0.069 0.077 0.085
Illumination(%) 92.34 90.60 93.81 95.33 94.91 95.22 94.57 95.50 91.58
Table 6. Light uniformity and variation coefficient of 2mm thick glass transmittance component.
Table 6. Light uniformity and variation coefficient of 2mm thick glass transmittance component.
Time 2mm glass A B C D E F G H I
10:30 Average(Lux) 9902 9074 8832 9122 10991 14192 52549 54144 52454
Variance 628 5010 5686 5235 4189 2291 29768 32019 31339
Cv 0.063 0.522 0.644 0.574 0.381 0.161 0.566 0.591 0.597
Illumination(%) 93.99 65.98 59.89 62.86 75.45 90.64 34.62 31.72 31.01
11:30 Average(Lux) 9456 8788 9121 10278 13611 53302 59227 73413 36486
Variance 1367 2964 3416 2708 346 33545 29411 5037 23825
Cv 0.145 0.337 0.375 0.263 0.025 0.629 0.497 0.069 0.653
Illumination(%) 91.16 78.5 76.51 84.28 97.50 28.08 42.81 93.06 48.73
12:30 Average(Lux) 9793 7747 7734 8933 12144 65639 75127 75470 41387
Variance 434 400 791 405 441 2096 6677 13279 21467
Cv 0.044 0.052 0.102 0.045 0.036 0.032 0.089 0.176 0.519
Illumination(%) 94.97 96.91 92.75 97.03 95.86 96.79 90.76 83.68 40.41
13:30 Average(Lux) 9494 7467 7027 7905 11045 41105 67277 70382 57833
Variance 300 663 586 210 326 21427 8882 7255 10947
Cv 0.032 0.089 0.083 0.027 0.030 0.521 0.132 0.103 0.189
Illumination(%) 96.94 93.44 94.97 96.99 96.60 42.86 85.33 88.23 78.97
14:30 Average(Lux) 11773 8288 7283 8085 10378 14806 53669 55271 50436
Variance 667 651 561 562 707 915 4657 3782 2368
Cv 0.057 0.079 0.077 0.070 0.068 0.062 0.087 0.068 0.047
Illumination(%) 94.77 91.89 91.11 92.19 93.22 95.10 91.45 92.38 96.20
Table 7. Light uniformity and variation coefficient of 3mm thick glass transmittance component.
Table 7. Light uniformity and variation coefficient of 3mm thick glass transmittance component.
Time 3mm glass A B C D E F G H I
10:30 Average(Lux) 8165 5556 5200 5998 8404 12613 69234 71640 65709
Variance 439 380 397 463 110 643 4043 2468 510
Cv 0.054 0.068 0.076 0.077 0.013 0.051 0.058 0.034 0.008
Illumination(%) 93.93 96.01 94.71 93.46 99.10 95.32 93.36 96.47 99.40
11:30 Average(Lux) 7820 6548 6691 8200 12278 69336 70410 71778 21230
Variance 473 527 222 491 1446 4832 299 3039 4317
Cv 0.060 0.0800 0.033 0.060 0.118 0.070 0.004 0.042 0.203
Illumination(%) 94.76 90.96 96.24 93.52 93.10 93.04 99.52 96.29 83.32
12:30 Average(Lux) 10639 9223 9104 10371 12292 47526 52557 56379 48093
Variance 1032 2777 2676 2827 727 28626 33213 34108 26582
Cv 0.097 0.301 0.294 0.273 0.059 0.602 0.609 0.605 0.553
Illumination(%) 94.15 81.45 82.24 83.67 93.61 33.56 33.61 33.59 36.9
13:30 Average(Lux) 10511 8768 81.2 9220 11238 20650 50111 51299 48239
Variance 1093 3339 3201 3593 1783 6321 27683 28179 27861
Cv 0.104 0.381 0.393 0.390 0.159 0.306 0.552 0.549 0.566
Illumination(%) 91.42 76.30 76.20 76.97 89.80 77.44 36.36 37.09 35.00
14:30 Average(Lux) 17584 22986 19327 22834 23440 27171 50479 42862 55392
Variance 9495 24502 18756 22999 19510 19982 6235 20472 1599
Cv 0.540 1.066 0.970 1.007 0.832 0.735 0.124 0.478 0.092
Illumination(%) 68.53 38.23 42.01 39.32 48.24 55.98 87.98 44.88 96.68
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