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Advances in Materials Science and Engineering

Volume 2014 (2014), Article ID 192707, 7 pages

http://dx.doi.org/10.1155/2014/192707
Research Article

Membrane Material-Based Rigid Solar Array Design and Thermal Simulation for Stratospheric Airships

School of Aeronautic Science and Technology, Beihang University, Beijing 100191, China

Received 3 April 2014; Revised 29 June 2014; Accepted 1 July 2014; Published 19 August 2014

Academic Editor: Ying Li

Copyright © 2014 Kangwen Sun 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.

Abstract

In order to improve effective utilization of rigid solar array used in stratospheric airships here, the flexible connection design and light laminated design were introduced to rigid solar array. Based on the analysis of the design scheme, firstly, the equivalent coefficient of thermal conductivity was calculated by the theoretical formula. Subsequently, the temperature variation characteristics of the solar cell module were accurately modeled and simulated by using Computational Fluid Dynamics (CFD) software. Compared to the results of test samples, the solar cell module described here guaranteed effective output as well as good heat insulating ability, effectively improving the feasibility of the stratospheric airship design. In addition, the simulation model can effectively simulate the temperature variation characteristics of the solar cell, which, therefore, provides technical support for the engineering application.

1. Introduction

The advantages of stratospheric airships include long endurance, wide-area coverage, strong-survival ability, and low cost of manufacture and maintenance. As a high-altitude platform, stratospheric airships have wide military and civilian applications, especially in communication relay, remote sensing, high-resolution earth observation, environmental monitoring, and so on, which has become a hot research field around the world [13].

In 2003, NASA carried out a feasibility research on the stratospheric airship and the efficient solar array, advanced energy storage and management system, novel high-altitude propeller and electric propulsion system, and lightweight high-strength envelop materials were defined as the four key technologies of the stratospheric airship [4].

At present, the analysis on energy system has been relatively perfected, especially on the electrical characteristics of the solar array [58], but the analysis on the thermal characteristics of the solar array was relatively few [9, 10], and the effective control methods of the thermal characteristics of it were fewer reported than above. However, in the conventional design scheme, solar array mounts on the surface of the stratospheric airship; then, the temperature difference between solar cell surface and envelop surface, where no solar array overcasts, could go up to 60°C in the daytime, which is discussed by Xia et al. [9], because the conversion efficiency of thin film flexible solar array was very low . Therefore, the conversion efficiency of the solar cell must be enhanced, and the imperative heat insulation measures between solar cells and the airship envelop must be taken.

As for the problems mentioned above, this paper will focus on rigid solar cell, whose conversion efficiency can reach up to 20% and even higher, and effective utilization in the stratospheric airship with rigid-flexible design method. Furthermore, as support structure to rigid solar cell, the honeycomb sandwich structure can also obtain effective insulation. In this paper, the temperature variation characteristics of solar cell module were accurately simulated and analyzed by Computational Fluid Dynamics (CFD) software followed by the verification of the rationality of the design, as well as the validity of the simulation model.

2. Flexible Processing of Rigid Solar Cell

American researchers have studied the application of rigid solar cell in the stratospheric aerostats, and the implementation scheme adopted hanging method to mount solar array on the buoyancy body in the form of modules [11, 12]. Due to the solar array irresponsibility in the drive mechanism and the big scale existing in the whole structure in the height direction, this leads to the failure of the application of design plans.

To deal with the big global scale and small local curvature of stratospheric airship, this paper proposed a “fish scale” shape design for the flexible application of rigid solar cell. One or more pieces of efficient solar cell were lightweight-hard packaged to form modules (module size was designed according to airship curvature), and then they were mounted on the soft net laminated with soft fabric woven, and finally the series parallel cables between rigid solar cell and the final main transmission cables were laid in the pipeline above the soft net (as shown in Figure 1). The above design scheme can ensure high-efficiency output of solar array as much as possible; meanwhile, it realizes the effective application of rigid cell array in the stratospheric airship. In addition, the reasonable application of monolayer board honeycomb sandwich structure can achieve rigid support and effective heat insulation for the rigid solar cell. The solar array design based on the above idea is shown in Figure 2.

192707.fig.001
Figure 1: “Fish scale” design scheme for rigid solar cell module (single piece as shown).
192707.fig.002
Figure 2: “Fish scale” design scheme for rigid solar array on stratospheric airship.

3. Analysis of Equivalent Thermal Conductivity

The stratospheric solar cell module discussed in this paper uses a multilayer film and Nomex honeycomb sandwich structure to meet the requirement of lightweight design. And its composition and basic characteristics of each layer are shown in Table 1. The areal density of this module can achieve the lighter density at which is lower than that of solar cell module at 2.25 kg/m2 (tensile membrane semirigid structure, given by Guoxin [13]).

tab1
Table 1: Materials physical parameters of lightweight and high-efficiency solar cell module.

According to Table 1, in order to determine the temperature characteristics of the upper and lower surface of the above solar cell module, parameter analysis is shown as follows.

The upper of solar cell module consists of 5-layer materials that are tightly compressed together, and the overall thermal resistance can be expressed as denotes the total thickness of the upper: denotes the equivalent thermal conductivity of the upper: After calculation, ; .

According to Figure 3 and Table 1, the lower part of the solar cell module is made up of two monolayer carbon fiberboards which are tightly laminated on 10 mm honeycomb sandwich formed by both top and bottom of Nomex honeycomb. Heat conducts from the surface to the upper monolayer carbon fiberboard through 5-layer materials, and then through honeycomb it conducts to the bottom of the monolayer carbon fiberboard. Finally, the monolayer carbon fiberboard transfers heat into the environment through thermal radiation and heat convection. In order to build a calculation model of equivalent thermal conductivity coefficient, it is necessary to inspect honeycomb cell unit.

192707.fig.003
Figure 3: Test chamber and test specimen.

The specification of the honeycomb core used in solar cell module is described as follows: side length , height , and thickness of monolayer wall . Within the cavity formed by this core, air convection heat transfer within honeycomb can be ignored because of relative seal of the space. Based on the above analysis, the heat transfer model of honeycomb sandwich structure includes solid heat conduction inside the cell wall of sandwich layer, air heat conduction inside honeycomb, and radiation heat transfer between the top-bottom panel and honeycomb cell wall. With reference to the above three kinds of heat transfer mechanism, the effective thermal conductivity of honeycomb sandwich structure can be expressed as follows: where is the thermal conductivity coefficient of honeycomb matrix material, is the thermal conductivity coefficient of air within the sandwich structure, is the radiation thermal conductivity coefficient between the top-bottom board and honeycomb cell wall, is the cross-sectional area of the material, and is the cross-sectional area of cell unit.

The air thermal conductivity coefficient within honeycomb sandwich structure is formulated as follows: where Ta is the characteristic temperature of air thermal conductivity coefficient, while and are the top and bottom temperature, respectively:

The calculation formula of equivalent radiation thermal conductivity is shown as follows (given by Swann Robert and Pittman Claud [14]): is the ratio of honeycomb height to its cell size; is the radiation rate of internal honeycomb structure; and is the Stefan-Boltzmann blackbody radiation constant.

and are unknown, and they need to be determined by the iterative calculation. The experimental measurement value (according to the test data,  K,  K are defined in this paper) is substituted into the formula, and the surface temperature of solar cell module is iteratively calculated after the thermal conductivity coefficient of the air and the equivalent thermal conductivity coefficient of the honeycomb are calculated.

The thermal resistance of the lower solar cell module is expressed as , and its expression is described as follows: denotes the total thickness of the lower part and its expression is shown as follows: denotes the equivalent thermal conductivity coefficient of the lower part and its expression is shown as follows: Consequently,  m; .

4. Experimental Measurements

The dimension of environmental test chamber was and the solar simulator was installed in the middle so as to simulate the radiation from the sun, whereas the dimension of the test specimen was (which can be seen from Figure 3). Then, the specimen beneath the solar simulator was put in the environmental test chamber and the distance between the specimen and the top of the chamber was , whereas the distance between the specimen and the bottom of the chamber was . And the remaining length is the height of the bracket (i.e., ).

The test ambient pressure was 5000 pa (20 km altitude), and the ambient temperature of test site was 12°C. At the same time, according to the calculation model of solar radiation, which is discussed by Lacis and Hansen [15], the solar vertical radiation reference intensity in stratosphere can be set at 1260 W/m2. When the chamber reached a steady state, the temperature of chamber wall and the temperature of internal chamber air were 15°C (assume for December 22 in this paper) [16], due to the radiation heating effect of the solar simulator. Test image was shown in Figure 4.

192707.fig.004
Figure 4: Test specimen temperature test.

The locations of temperature measuring point are shown in Figure 5. There are three temperature measuring points on the upper surface of the solar cell module, where the temperature measuring point (TMP) 4 is on the back of the TMP 1, the TMP 5 is on the back of the TMP 2, and the TMP 6 is on the back of the TMP 3.

192707.fig.005
Figure 5: Schematic diagram of test specimen surface TMPs arrangement.

At room temperature, the infrared thermometer was used to measure the temperature on the surface of the specimen and 9 groups of data were obtained and listed in Table 2; at the same time, the average temperature of specimen surface and the data of the temperature difference are shown in Table 3.

tab2
Table 2: Temperature test data of test specimens.
tab3
Table 3: Test specimens’ surface average temperature and temperature difference.

For Tables 2 and 3, there are two points that need to be made as follows.(1)The temperature difference for the same side point was mainly due to the inhomogeneity of the solar simulator light intensity in a certain scale.(2)The standard deviation of the test points in the same side is about 1.6, less than the final temperature difference value of 1.65%, whose effect on the analysis results is very small. Then, it is belongs to the range of acceptable.

5. Simulation Calculations

5.1. Modeling and Setting Up of Boundary Conditions

According to the test equipment dimension, a three-dimensional model for temperature calculation of solar cell module was built, and test specimen was set up in the middle of environmental test chamber and below the solar simulator.

The inwall thickness of test chamber was 4 mm, and the surface emissivity and absorptivity were 0.98 after roughness of copper because the copper could guarantee the temperature of environmental chamber being uniform. Therefore, the inwall emissivity and absorptivity of ambient chamber model were set as 0.98, and the temperature of the chamber wall was set as 15°C, which could guarantee the internal ambient temperature of simulation module being stable at 15°C. The radiation intensity of solar simulator was 1260 W/m2.

The radiation characteristics of the specimen upper surface are directly related to the radiation properties of surface encapsulating film and transparency adhesive film, and the light transmittance of the surface encapsulating film and the transparency adhesive film are 0.92 and 0.91, respectively. Thus, the absorption rate of the sunlight on the upper surface of the specimen is set as 0.8372, and the emissivity of the surface encapsulating film is 0.92, so the emissivity of specimen upper surface is set as 0.92. The absorption rate of the specimen lower surface is set as 0.94, and the emissivity is set as 0.98.

When calculating the temperature field and flow field, the approach of local grid refinement is applied in the calculation because the smallest thickness is the upper part of the solar cell module (0.77 mm). The solid grid minimum size of the specimen is set as 0.5 mm to ensure that the upper part of the solar cell module can fully participate in heat transfer calculation. 385900 grids are generated from the calculation, and the temperature field and the velocity field of test chamber; the temperature field of the specimen surface can be obtained accurately after calculation in 100 min.

5.2. Results of Simulation Calculation

The distribution of the temperature field and velocity field outside the test chamber are shown in Figures 6 and 7, and obviously the wall temperature of the test chamber is higher than the ambient temperature. Therefore, the air outside the test chamber rises up along the wall of the test chamber, and the air temperature close to the surface goes up higher and higher due to frictional heating. Meanwhile, the difference between this air temperature and ambient temperature is getting bigger and bigger. Therefore, the rising velocity of air close to the wall is getting bigger and bigger.

192707.fig.006
Figure 6: Cross-section temperature and velocity field of the test specimen.
192707.fig.007
Figure 7: Longitudinal section temperature and velocity field of the test specimen.

In the test chamber, the temperature of the specimen went up due to solar radiation effect, which simultaneously heated the surrounding air. The heated air flowed up under the drive of buoyancy, and it went along the wall of the test chamber by the drive of hot air after it reached the top. The hot air was cooled and flowed down along the wall of the test chamber because the temperature of hot air was higher than that of the wall of the test chamber. Therefore, the air within the test chamber was heated by the specimen, forming two circles by the buoyancy.

Figure 8 was the distribution of the specimen surface temperature, and the labels in figure were corresponding to the temperature data in the measuring point.

192707.fig.008
Figure 8: The temperature distribution of test specimen upper surface and lower surface.

Comparing the simulation results and test results (as shown in Table 4), there is little relative error between them, which indicated that the simulation model built here is effective for the thermal characteristics analysis of lightweight and high-efficiency solar cell module. Data comparison shows that the relative error on the absolute value of the upper and lower surface temperatures that were obtained by measurement and calculation is less than 2%, and the relative error of the temperature difference is less than 12%, which can completely satisfy the requirement of the early stage design precision; thus it can be applied to the analysis of the related design reference.

tab4
Table 4: Data of experiment and simulation comparison table.

6. Conclusions

Taken together, in consideration of the low conversion efficiency of thin film solar cell used in the stratospheric airship and the lack of the thermal control measures between the capsule body and the cell, rigid solar cell modules are flexibly connected and secured to the stratospheric airship with the method of rigid-flexible integration design which can ensure that solar arrays incorporate into the airship surface properly. Meanwhile, the honeycomb sandwich structure used in space solar array is applied to this scheme. Based on the characteristics of the stratospheric environment, membrane-packaged materials are used to largely reduce the surface density of solar arrays. On the basis of component analysis of the design scheme, theoretical formula is employed to calculate the equivalent thermal conductivity coefficient of this structure. Subsequently, the CFD software is applied to accurately model and analyze the temperature variation characteristics of the solar cell module. The comparative analysis of the experimental data and simulation results shows that the application solutions for the solar cell module proposed in this paper can insulate heat effectively between the solar array and the airship envelop; meanwhile it can reduce the covering area for the solar array mounted on the airship as much as possible. In addition, the simulation model built in this paper can effectively simulate the temperature variation characteristics of the solar cell, which provides further technical supports for the engineering application.

Conflict of Interests

The authors declare that they do not have any commercial or associative interest that represents a conflict of interests in connection with the work submitted.

Acknowledgments

This work was supported by the National Natural Science Foundation of China under Grant no. 51307004 and Shanghai Aerospace Science and Technology Innovation Fund no. SAST201268.

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