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Frontiers in Energy

ISSN 2095-1701

ISSN 2095-1698(Online)

CN 11-6017/TK

Postal Subscription Code 80-972

2018 Impact Factor: 1.701

Front. Energy    2018, Vol. 12 Issue (2) : 239-248    https://doi.org/10.1007/s11708-018-0533-7
RESEARCH ARTICLE
Effect of non-uniform illumination on performance of solar thermoelectric generators
Ershuai YIN1, Qiang LI1(), Yimin XUAN2
1. MIIT Key Laboratory of Thermal Control of Electronic Equipment, School of Energy and Power Engineering, Nanjing University of Science and Technology, Nanjing 210094, China
2. IMIIT Key Laboratory of Thermal Control of Electronic Equipment, School of Energy and Power Engineering, Nanjing University of Science and Technology, Nanjing 210094, China; School of Energy and Power, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China
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Abstract

Solar thermoelectric generators (STEGs) are heat engines which can generate electricity from concentrated sunlight. The non-uniform illumination caused by the optical concentrator may affect the performance of solar thermoelectric generators. In this paper, a three-dimensional finite element model of solar thermoelectric generators is established. The two-dimensional Gaussian distribution is employed to modify the illumination profiles incident on the thermoelectric generator. Six non-uniformities of solar illumination are investigated while keeping the total energy constant. The influences of non-uniform illumination on the temperature distribution, the voltage distribution, and the maximum output power are respectively discussed. Three thermoelectric generators with 32, 18 and 8 pairs of thermocouples are compared to investigate their capability under non-uniform solar radiation. The result shows that the non-uniformity of the solar illumination has a great effect on the temperature distribution and the voltage distribution. Central thermoelectric legs can achieve a larger temperature difference and generate a larger voltage than peripheral ones. The non-uniform solar illumination will weaken the capability of the TE generator, and the maximum output power decrease by 1.4% among the range of non-uniformity studied in this paper. Reducing the number of the thermoelectric legs for non-uniform solar illumination can greatly increase the performance of the thermoelectric generator.

Keywords solar thermoelectric generators      non-uniform solar illumination      performance evaluation      solar energy     
Corresponding Author(s): Qiang LI   
Issue Date: 04 June 2018
 Cite this article:   
Ershuai YIN,Qiang LI,Yimin XUAN. Effect of non-uniform illumination on performance of solar thermoelectric generators[J]. Front. Energy, 2018, 12(2): 239-248.
 URL:  
https://academic.hep.com.cn/fie/EN/10.1007/s11708-018-0533-7
https://academic.hep.com.cn/fie/EN/Y2018/V12/I2/239
Fig.1  Schematic diagram of STEGs
Fig.2  Structure diagram of the TE generator with 32 pairs of thermocouples
Fig.3  Properties of Bi2Te3 semiconductor materials
Fig.4  Heat fluxes of six uniformities at a solar radiation density of 10000 W/m2
Parameters Value
Length of TE legs/mm 1
Width of TE legs/mm 1
Height of TE legs/mm 1.5
Number of TE legs 64,36,16
Length of cu electrode/mm 3
Width of cu electrode/mm 1
Height of cu electrode/mm 0.3
Thermal conductivity of copper/(W?(m?K)-1) 400
Density of copper/(kg?m-3) 8960
Specific heat capacity of copper/(J?(kg?K)-1) 385
Electrical conductivity of copper/(S?m-1) 5.998 × 107
Length of ceramic plate/mm 16,12,8
Width of ceramic plate/mm 16,12,8
Height of ceramic plate/mm 0.8
Thermal conductivity of ceramic plate/(W?(m?K)-1) 18
Density of ceramic plate/(kg?m-3) 3960
Specific heat capacity of ceramic plate/(J?(kg?K)-1) 850
Transmittance of the glass 0.94
Emissivity of selective absorber 0.05
Absorptance of the solar selective absorber 0.95
Temperature of environment/K 293.15
Convection heat transfer coefficient at the lower surface of TE/(W?m-2?K-1) 10000
Tab.1  Parameters for the simulation
Fig.5  Temperature distribution of TE generator under six non-uniform solar illuminations at G0 = 50 kW/m2, re = 1.84 W, and h = 10000 W/(m2?K)
Fig.6  Influence of solar illumination non-uniformity on temperature of thermoelectric legs at G0 = 50 kW/m2, re = 1.84 W, and h = 10000 W/(m2?K)
Fig.7  Voltage distribution of TE generator at a uniform radiation of G0 = 50 kW/m2, re = 1.84 W, and h = 10000 W/(m2?K)
Fig.8  Generated voltage of each thermoelectric semiconductor leg at re = 1.84 W and h = 10000 W/(m2?K)
Fig.9  Influence of solar illumination non-uniformity at G0 = 50 kW/m2 and h = 10000 W/(m2?K)
Fig.10  Influence of number of thermoelectric legs on total performance of STEG
CP Specific heat capacity/(J?(kg?K)-1)
T Temperature/K
t Time/s
q Heat flux vector/(W?m-2)
q ˙ Heat generation rate/(W?m-3)
Hamiltonian
s Seebeck coefficient/(V?K)
k Thermal conductivity/(W?(m?K)-1)
J Electric current density vector/(A?m-2)
E Electric field intensity vector/(V?m-1)
D Electric fluxdensity vector/(A?m-2)
Z Figure of merit of TE generator
G Solar radiation density/(W?m-2)
D2 Variance of Gaussian distribution
G0 Density of uniform radiation/(W?m-2)
As Area of selective absorber/m2
Q Heat flux density/(W?m-2)
P Output power of TE generator/W
V Voltage/V
r Resistance/W
r Density/(kg?m-3)
s Electrical conductivity/(S?m-1)
j Electric scalar potential/V
p Eircumference ratio
w Normalization factor
t Transmittance of the glass
a Absorptance of the solar selective absorber
e Emissivity of selective absorber
e External resistance
oc Open circuit voltage
max Maximum output power of TE generator
TE Thermoelectric generator
  
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