Research Article  Open Access
Qingjun Liu, Fei Cao, Yanhua Liu, Tianyu Zhu, Deyou Liu, "Design and Simulation of a Solar Chimney PV/T Power Plant in Northwest China", International Journal of Photoenergy, vol. 2018, Article ID 1478695, 12 pages, 2018. https://doi.org/10.1155/2018/1478695
Design and Simulation of a Solar Chimney PV/T Power Plant in Northwest China
Abstract
A solar chimney PV/T power plant (SCPVTPP) is proposed. Mathematical models are established for the PV/T solar collector, the chimney, and the power conversion unit, respectively. Performances of the designed SCPVTPP are then simulated. The SCPVTPPs with different PV module areas are finally discussed. It is found that the PV cells hold the highest temperature in the solar collector. Temperature rise of the PV module has significant influences to its power generation. Without cooling, the PV power capacity has an average decrease of 28.71%. The contradictory influences of temperature rise and airflow cooling lead to an 11.81% decrease of the average power capacity. By adding the power generated by PVT, the total PVrelated power contribution increases by 4.72%. With the increase of the solar collector ratio, the temperature rise and the wind velocity both first decrease then increase, the SCPP power productivity decreases linearly, and the PV power productivity increases linearly, whereas the PVT power productivity first increases linearly then increases superlinearly. There is a reversed solar collector ratio, exceeding which the PV generates most power. In this study, solar thermal power takes the major role when the solar PV area ratio is smaller than 0.055.
1. Introduction
The solar chimney power plant (SCPP) consists of three essential parts: a solar collector, a chimney, and a power conversion unit. The schematic of a SCPP is shown in Figure 1(a). Sunlight transfers through the transparent collector cover and heats the ground below. The ground temperature increases and heats the air above it through heat convection. The air temperature increases, leading to the decrease of air density. The density difference then is generated between the ambient air and the air in the solar collector. With the chimney, the air flows towards to the center of the solar collector under buoyancy effect. The air flows through the chimney and runs out of the SCPP at the top of the chimney.
(a)
(b)
Theoretical, experimental, and case studies of the SCPPs all around the world have concluded that the SCPP is with low power efficiency [1–3], huge solar collector area [4–6], and high chimney [6–9]. Some case studies of SCPPs are summarized in Table 1. Our previous studies have concluded that the reason of SCPP’s low efficiency is a compound result of the air characteristics, the solar radiation, and the chimney height [10, 11]. Air is the only practical working fluid of the SCPP because of the huge air mass flow rate inside the SCPP [11]. For a given location, the solar radiation is fixed. Therefore, it is concluded that the SCPP power capacity can be increased through enlarging the solar collector area or the chimney height [4, 8]. However, there must be a limit for both these solutions from the technoeconomical and safety points of view. A solution that can increase the power capacity but would not increase the chimney height and collector area, or even decrease both of them, is of high significance from the engineering points of view. We then noticed that the huge solar collector, which is empty for the airflow, can be used to place the solar PV modules. On one side, the solar collector area can be used, not influencing the airflow. On the other side, the PV module can be cooled by the airflow in the solar collector by forced heat convection. Correspondingly, a new solar chimney PV/T power plant (SCPVTPP) is proposed in Figure 1(b) to fulfill this target. In the system, some solar PV modules are set on the ground of the solar collector. Due to the considerations of safety and construction cost, there are no PV modules in the vertical chimney. The solar radiation transfers through the transparent glass cover and then reaches the PV modules. The insulating layer and the wire connection are set between the PV modules and the ground. Solar radiation transfers through the glass cover and reaches the PV modules. Electricity is generated directly from the PV modules. Meanwhile, some solar radiation is converted into the thermal energy and heats the PV models. The hightemperature PV modules then heat the air above it through heat convection. The other area of the solar collector without the PV modules absorbs the solar radiation directly, which leads to the temperature increase of the ground. The ground then heats the air above it through heat convection. The hightemperature air above the ground and the PV modules then flows into the chimney through buoyancy effect. The solar PV/T technology or device was proposed for the purpose of cooling the PV module to increase its power efficiency [12] and recovering the waste heat to increase the system’s total efficiency [13]. It has been widely utilized in the solar water heating (SWH) [14], heating ventilation air conditioning (HVAC) [15], solarpowered buildings [16], and so on. However, the largescale PV/T system has not been investigated. Considering this, the main tasks in this study include (1) to build a mathematical model for the SCPVTPP, (2) to analyze the performance of the SCPVTPP, and (3) to study the SCPVTPP with different PV areas.
 
^{1}The authors of [24] did not supply the detailed solar radiation and power capacity in their literature. We calculated the results according to the results supplied in their paper and the solar duration supplied by the China Meteorological Information Center (CMIC). ^{2}The solar radiation and power capacity are calculated according to the data supplied by the authors. 
2. Mathematical Model
A mathematical model is built for the SCPVTPP. The mathematical model can be divided into three parts, namely, the PVT solar collector model, the chimney model, and the power conversion unit (PCU) model. Practically, the SCPVTPP has a large solar collection area, high chimney height, high PV surface temperature, and high airflow velocity, compared with the collector height, the collector cover thickness, and the temperature rise in the solar collector are much smaller. Correspondingly, the next assumptions can be made: (a) temperature rises linearly along the airflow direction in the solar collector; (b) ignore the velocity and temperature gradient on the vertical direction in the solar collector; (c) ignore the velocity and temperature gradient on the cross section of the chimney; (d) ignore the temperature difference between the collector upper and back surface; (e) airflow is under adiabatic condition in the chimney; and (f) PV lower surface and ground up surface are connected together.
2.1. PVT Solar Collector Model
Energy balance of a representative elemental volume in the solar collector and PV is established (Figure 2). In the model, there are three energy balance equations presented in (1), (2), and (3), respectively.
(a)
(b)
Continuity equation:
Momentum equation:
Energy equation:
Considering the energy balance of a representative elemental volume, as shown in Figure 2(a), the energy source is where the first and the second terms on the right side of (4) are the heat exchange between the collector cover and airflow and between the PV and the airflow, which can be expressed as where is the radiation heat exchange between the PV and the collector cover, is the convection and radiation heat exchange between the collector cover and the ambient, is the heat contribution from the PV, is the solar radiation absorbed by the collector cover, and is the solar radiation absorbed by the PV module or the ground. The PV modules are laid on the ground directly as shown in Figure 2(b). There are six layers in the PV modules, namely, the glass, the antireflective coating (ARC), the EVA (ethylenevinyl acetate), the PV cell, and the Tedlar Polymer Layer (TPL).
Taking a depth of of the ith layer inside the PV layer into consideration, we obtain where is the heat contribution from upper surface to the lower surface and for the layers excluding the PV cell. And at the depth of , we obtain
And taking a depth of inside the ground into consideration, we obtain
is the energy output of the PV and can be calculated according to [17]: where is the transmittance of the PV cover, is the efficiency of PV under standard conditions, is the temperature coefficient, and is the standard testing temperature of PV.
2.2. Chimney
Continuity equation:
Momentum equation:
Energy equation:
For a vertical adiabatic chimney, the pressure difference created in the chimney is
And the pressure difference between the inlet and outlet of the solar collector is calculated as where denotes the height. Comparing with the chimney height, the solar collector height is much smaller. Thus, .
According to Boussinesq assumption and (13) and (14), the momentum equation of the chimney can be simplified as
2.3. PCU
As the connection section of the PCU is irregular, a randomized coordinate along the power generator surface is built for this area (Figure 3). And we can obtain the following:
Continuity equation:
Momentum equation:
Energy equation:
As and , we can obtain that where is the chimney height, is the collector radius, and is the length of the PCU channel.
Consequently, the momentum equation can be simplified as
The generated pressure is consumed by four parts, that is, the friction losses in the collector and the chimney , the kinetic energy losses at the turbine inlet , the kinetic energy losses at the chimney outlet , and the rest is the effective pressure which is used by the turbine to generate electricity . where is the friction loss coefficient, is the hydraulic diameter, is the length of the channel, and is the turbine inlet loss coefficient.
The power generated by the turbine is
2.4. Simulation Methodology
Equations to calculate the coefficients, namely, the heat transfer coefficients, the loss coefficients, the friction loss, and turbine efficiency, follow the previous studies [1, 4, 18]. The equations are converted into the codes to solve the equations. Flowchart of the simulation in this study is shown in Figure 4. As shown in Figure 4, the initial values of the parameters, that is, the collector cover temperature, PV temperature, airflow temperature, and ground temperature, are firstly assumed. An iterative calculation is then made to use the new values to replace the old values. When the differences between any corresponding new and old values are less than the maximal acceptable difference (namely, smaller than 10^{−6}), the iteration process is finally stopped.
3. Result and Discussion
3.1. Configuration Sizes of the SCPVTPP
The configuration sizes of the SCPVTPP are shown in Table 2. The SCPVTPP is designed according to 5 and MW SCPP to [19]. And the SCPVTPP is assumed to be operated in Lanzhou. Lanzhou (103.50°E, 36.03°N) is located in the geographical center of Northwest China. And it has typical Northwestern Chinese climate, that is, strong solar radiation, rare rainfall that diminishes from east to west, dry and cold winter, hot summer, and broad daily temperature width. Its annual global solar radiation is more than 5020 MJ/m^{2} and sunshine duration is over 2600 h per year. Its annual mean temperature is 9.8°C. The properties of six layers in the PV module are shown in Table 3.


3.2. Temperature Increase and Wind Velocity of the SCPVTPP
As the SCPP is dominated by the buoyancy effect, temperature rise in the solar collector is of high significance. Moreover, two contradictory phenomena occur concerning the temperature rise in the PV/T solar collector. On one side, the PV modules are sensitive to the temperature rise. The PV power generation would decrease with the rise of temperature. On the other hand, the updraft wind would enhance with the temperature rising and the generated wind would reduce the temperature of the PV modules. Considering this, the meteorological data, temperatures, and wind velocity inside the SCPVTPP are calculated and the results are shown in Figure 5.
(a)
(b)
Solar radiation and ambient temperature of Lanzhou is shown in Figure 5(a). It is found from the figure that the solar radiation first increases from January to June, with the peak of 689.73 W/m^{2}. Then the solar radiation decreases till December. The tendency of the ambient temperature is similar with the solar radiation, whereas the highest ambient temperature appears at July. Temperatures of the glass cover, airflow, PV module, and ground and the temperature increase inside the collector at different months in the year are shown in Figure 5(b). It is found from the figure that the temperatures of the glass cover, airflow, PV module, and ground have the same tendency with the ambient temperature, with the peak values at July. Moreover, the PV cell holds the highest temperature among the four temperature groups throughout the year, followed by the ground temperature, the glass cover temperature, and the airflow temperature. Temperature differences between each two groups of temperatures increase from January to July and then decrease till December.
3.3. Power Generation
There are three parts contributing to the power generation in the SCPVTPP, namely, the PV power capacity, the SCPP power capacity, and the PVT power capacity, which, respectively, refers to the power generation directly from the PV modules, the power contribution by the airflow from the solar collector without PV modules, and the power contribution by the airflow heated by the PV modules. Power generations from the PV, the PVT, and the SCPP are shown in Figure 6. It is found from the figure that PV generates much higher power than PVT and SCPP. SCPP generates more power productivity than PVT. The power generates from the solar thermal effect, namely, the power generation from PVT and SCPP is much smaller than that from the PV. This is reasonable as the energy conversion efficiency of SCPP is at 1% level [1–3], whereas the energy conversion efficiency of PV is near 16% [17]. Power productivities from the PV, PVT, and SCPP have similar tendencies with the solar radiation, except the start and the end of the year for the PV power productivity. It is found in Figure 5(a) that the solar radiation increases from January to February. However, power productivities decrease from January to February in Figure 6. The reason is that the power productivity is a compound result of the solar radiation and the ambient temperature. It is believed that less power is generated as the PV cell temperature rises according to (9). And the tendency of the ambient temperature rise is much larger than the increase of solar radiation from January to February (Figure 5(a)). The two effects lead to the decrease of power productivity of PV from January to February in Figure 6. This also explains the tendency of PV power productivity from November to December in Figure 6.
As mentioned above, the temperature takes contradictory effect on the PV power generation. The temperature influences on the PV power generation is thus analysed. By taking the PV power generation under ambient temperature as a reference, the PV model power, the PVT power contribution, and the total PVrelated power contribution (PV + PVT) in the present study and the PV power generation without airflow cooling are then compared in Table 4. In can be found from Table 4 that the temperature rise of the PV module has significant influences to its power generation. Without cooling, the PV power capacity has an average decrease of 28.71%. The contradictory influences of temperature rise and airflow cooling lead to an 11.81% decrease of the average power capacity, reflecting the temperature rise which takes the major role in the SCPVTPP. The PVT power contribution is much smaller than the others. But adding the power generated by the PVT effect, the total PVrelated power contribution would increase by 4.72%. And there are some conditions, that is, in January, February, November, and December, the total PVrelated power contribution is larger than the reference P_{PV_Ta}. The reason is that the PV models’ temperatures are low in these months, due to also low ambient temperatures. And the system takes full advantage of PV modules and generated updraft winds in these months.

3.4. SCPVTPP with Different PV Areas
The performances of the SCPVTPP is discussed in Figures 5(b) and 6 for the case that PV area takes 30% of the whole solar collector. However, there are some cases that the PV area can take more or less percentage to the whole solar collector. The SCPVTPP performances and power productivities under different solar collector area ratios are then calculated with the same methodology as the case of 30%. The results are shown in Figures 7(a) and 7(b). It is found in Figure 7(a) that with the increase of the solar collector ratio, the temperature rise and the wind velocity both first decrease then increase. However, the valleys of the temperature rise and the wind velocity appear at different solar collector ratios. The lowest temperature rise is located at the solar collector ratio of 0.4, whereas the lowest wind velocity is located at the solar collector ratio of 0.6. Moreover, tendencies of the temperature rise and the wind velocity differ from each other. The temperature rise first decreases gradually and then increases gradually. But the wind velocity first decreases slowly and then increases quickly. It is found from Figure 7(b) that with the increase of the solar collector ratio, the SCPP power productivity decreases linearly and the PV power productivity increases linearly, whereas the PVT power productivity first increases linearly then increases superlinearly. The total power productivity increases with the solar collector ratio rises. There is a reversed solar collector ratio, exceeding the PV which generates most of the power. With detailed calculation, it is found that the solar collector ratio is 0.055, which means that solar thermal power takes the major role of power generation when the solar PV area ratio is smaller than 0.055.
(a)
(b)
4. Conclusions
The SCPP has a large solar collector area, which can be used to lay the PV modules. A SCPVTPP is proposed and studied in this study. A mathematical model is established for the proposed system. The SCPVTPP performances and the power productivities under different solar collector ratios are then discussed. It can be concluded from this study that (1)The PV cells hold the highest temperature in the solar collector throughout the year, followed by the ground temperature, the glass cover temperature, and the airflow temperature. The temperature rise of the PV module has significant influences to its power generation. Without cooling, the PV power capacity has an average decrease of 28.71%. The contradictory influences of temperature rise and airflow cooling lead to an 11.81% decrease of the average power capacity. By adding the power generated by PVT, the total PVrelated power contribution increases by 4.72%.(2)With the increase of the solar collector ratio, the temperature rise and the wind velocity both first decrease then increase. The lowest temperature rise is located at the solar collector ratio of 0.4, whereas the lowest wind velocity is located at the solar collector ratio of 0.6.(3)With the increase of the solar collector ratio, the SCPP power productivity decreases linearly and the PV power productivity increases linearly, whereas the PVT power productivity first increases linearly then increases superlinearly.(4)There is a reversed solar collector ratio, exceeding the PV which generates most of the power. In this study, solar thermal power takes the major role when the solar PV area ratio is smaller than 0.055.
Nomenclature
A:  Area (m^{2}) 
c_{p}:  Specific heat (J·m^{−2}·K^{−1}) 
E_{PV}:  PV power (W) 
f:  Friction loss coefficient (−) 
:  Acceleration of gravity (m·s^{−2}) 
h:  Heat transfer coefficient (W·m^{−2}·K^{−1}) 
H:  Height (m); solar radiation (W·m^{−2}) 
K:  Extinction coefficient (m^{−1}) 
L:  Length (m); channel length (m) 
P:  Pressure (Pa); electrical power generation (W) 
Q:  Energy flux (J·hr^{−1}) 
r:  Direction (−) 
R:  Radius (m) 
S_{1}:  Solar radiation absorb by glass (W/m^{2}) 
S_{2}:  Solar radiation absorb by PV (W/m^{2}) 
T:  Temperature (K) 
U:  Compound heat coefficient (W·m^{−2}·K^{−1}) 
v:  Air velocity (m·s^{−1}) 
∆P_{tot}:  Total pressure difference (Pa). 
Δ:  Difference (−) 
ρ:  Air density (kg·m^{−3}); reflectance (−) 
θ:  Angle (°); direction (−) 
γ:  Turbine inlet loss coefficient (−) 
μ:  Dynamic viscosity (kg·m^{−1}·s^{−1}) 
η_{t}:  Turbine efficiency. 
a:  Ambient 
c:  Collector cover 
col:  Collector 
chi:  Chimney 
f:  Airflow 
gro:  Ground 
in:  Turbine inlet 
o:  Outlet of the solar collector 
out:  Outlet of the chimney 
PV:  Photovoltaic. 
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
This research was supported by the National Natural Science Foundation of China (Grant no. 51506043), the Natural Science Foundation of Jiangsu Province (Grant no. BK20141153), the “Dayu Scholar” Foundation of Hohai University, and the China Scholarship Council (Grant no. 201706715058).
References
 F. Cao, L. Zhao, and L. Guo, “Simulation of a sloped solar chimney power plant in Lanzhou,” Energy Conversion and Management, vol. 52, no. 6, pp. 2360–2366, 2011. View at: Publisher Site  Google Scholar
 T. Z. Ming, Y. Zheng, C. Liu, W. Liu, and Y. Pan, “Simple analysis on thermal performance of solar chimney power generation systems,” Journal of the Energy Institute, vol. 83, no. 1, pp. 6–11, 2010. View at: Publisher Site  Google Scholar
 X. Zhou, F. Wang, and R. M. Ochieng, “A review of solar chimney power technology,” Renewable and Sustainable Energy Reviews, vol. 14, no. 8, pp. 2315–2338, 2010. View at: Publisher Site  Google Scholar
 S. Larbi, A. Bouhdjar, and T. Chergui, “Performance analysis of a solar chimney power plant in the southwestern region of Algeria,” Renewable and Sustainable Energy Reviews, vol. 14, no. 1, pp. 470–477, 2010. View at: Publisher Site  Google Scholar
 R. Sangi, “Performance evaluation of solar chimney power plants in Iran,” Renewable and Sustainable Energy Reviews, vol. 16, no. 1, pp. 704–710, 2012. View at: Publisher Site  Google Scholar
 C. D. Papageorgiou and P. P. Katopodis, “A modular solar collector for desert floating solar chimney technology,” in Energy, Environment, Ecosystems, Development and Landscape Architecture, pp. 126–132, WSEAS Press, Athens, Greece, 2009. View at: Google Scholar
 X. Zhou, J. Yang, B. Xiao, G. Hou, and Y. Wu, “Numerical investigation of a compressible flow through a solar chimney,” Heat Transfer Engineering, vol. 30, no. 8, pp. 670–676, 2009. View at: Publisher Site  Google Scholar
 X. Zhou, M. A. D. S. Bernardes, and R. M. Ochieng, “Influence of atmospheric cross flow on solar updraft tower inflow,” Energy, vol. 42, no. 1, pp. 393–400, 2012. View at: Publisher Site  Google Scholar
 S. Nizetic, N. Ninic, and B. Klarin, “Analysis and feasibility of implementing solar chimney power plants in the Mediterranean region,” Energy, vol. 33, no. 11, pp. 1680–1690, 2008. View at: Publisher Site  Google Scholar
 F. Cao, H. Li, L. Zhao, T. Bao, and L. Guo, “Design and simulation of the solar chimney power plants with TRNSYS,” Solar Energy, vol. 98, pp. 23–33, 2013. View at: Publisher Site  Google Scholar
 F. Cao, L. Zhao, H. Li, and L. Guo, “Performance analysis of conventional and sloped solar chimney power plants in China,” Applied Thermal Engineering, vol. 50, no. 1, pp. 582–592, 2013. View at: Publisher Site  Google Scholar
 J. A. Duffie and W. A. Beckman, Solar Engineering of Thermal Processes, John Wiley & Sons, New York, NY, USA, 2006.
 E. C. J. Kern and M. C. Russell, “Combined photovoltaic and thermal hybrid collector systems,” in IEEE Photovoltaic Specialists Conference, vol. 1, pp. 1153–1157, Washington, DC, USA, 1978. View at: Google Scholar
 L. W. Florschuetz, “Extension of the HottelWhillier model to the analysis of combined photovoltaic/thermal flat plate collectors,” Solar Energy, vol. 22, no. 4, pp. 361–366, 1979. View at: Publisher Site  Google Scholar
 A. A. Hegazy, “Comparative study of the performances of four photovoltaic/thermal solar air collectors,” Energy Conversion and Management, vol. 41, no. 8, pp. 861–881, 2000. View at: Publisher Site  Google Scholar
 H. Yang, J. Burnett, and J. Ji, “Simple approach to cooling load component calculation through PV walls,” Energy and Buildings, vol. 31, no. 3, pp. 285–290, 2000. View at: Publisher Site  Google Scholar
 G. Chao, Numerical and Experimental Study of TriFunctional Photovoltaic/Thermal Collector [Ph.D. Thesis], University of Science and Technology of China, China, 2015.
 X. Zhou and Y. Xu, “Solar updraft tower power generation,” Solar Energy, vol. 128, pp. 95–125, 2016. View at: Publisher Site  Google Scholar
 J. Schlaich, R. Bergermann, W. Schiel, and G. Weinrebe, “Design of commercial solar updraft tower systems—utilization of solar induced convective flows for power generation,” Journal of Solar Energy Engineering, vol. 127, no. 1, pp. 117–124, 2005. View at: Publisher Site  Google Scholar
 W. Haaf, “Solar chimneys. Part II: preliminary test results from the Manzanares pilot plant,” International Journal of Solar Energy, vol. 2, no. 2, pp. 141–161, 1984. View at: Publisher Site  Google Scholar
 J. Schlaich, The Solar Chimney: Electricity from the Sun, Axel Menges, Stuttgart, Germany, 1995.
 Y. J. Dai, H. B. Huang, and R. Z. Wang, “Case study of solar chimney power plants in Northwestern regions of China,” Renewable Energy, vol. 28, no. 8, pp. 1295–1304, 2003. View at: Publisher Site  Google Scholar
 M. O. Hamdan, “Analysis of a solar chimney power plant in the Arabian gulf region,” Renewable Energy, vol. 36, no. 10, pp. 2593–2598, 2011. View at: Publisher Site  Google Scholar
 X. Zhou, F. Wang, J. Fan, and R. M. Ochieng, “Performance of solar chimney power plant in QinghaiTibet plateau,” Renewable and Sustainable Energy Reviews, vol. 14, no. 8, pp. 2249–2255, 2010. View at: Publisher Site  Google Scholar
 A. Asnaghi and S. M. Ladjevardi, “Solar chimney power plant performance in Iran,” Renewable and Sustainable Energy Reviews, vol. 16, no. 5, pp. 3383–3390, 2012. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2018 Qingjun Liu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.