Yusufoglu, Institute of Semiconductor Electronics
Modeling and simulation of annual
energy yields of bifacial modules at
different climate zones
U. Yusufoglu, T. Lee, T. Pletzer, H. Kurz
Institute of Semiconductor Electronics, RWTH Aachen University, Germany
A. Halm, L. J. Koduvelikulathu, C. Comparotto, R. Kopecek
International Solar Energy Research Center (ISC), Konstanz, Germany
bifiPV Workshop 2014, 27.05.2014
Yusufoglu, Institute of Semiconductor Electronics
Albedo
moduleelevationVertical
Outline
Annual energy yield simulation based on individual characteristics of solar cells
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones2
Optimization of tilt angle
Location
South facing
S i m u l a t i o n r e s u l t s
Gain with respect to standard module
Annual E
nergy Yield
Measured I-Vof solar cells
Cell/Module Temperature
M o d e l i n g s t e p s
Two-Diode-Model
Irradiance reaching both cell surfaces
Direct Diffuse Albedo (effect of shadow for rear)
AOI losses & spectral mismatch
Yusufoglu, Institute of Semiconductor Electronics
Measurement of I-V characteristics
27.05.2014
Modeling and simulation of annual energy yields of bifacial modules at different climate zones3
Six-inch mono-Si n-type bifacial solar cells [1] Separately available I-V characterics of front and rear Bifaciality of cells on average 80 %
Front
Rear
Rear
FrontBlack chuck
Front illumination Rear illumination
Black chuck
[1] Mihailetchi et al., bifiPV2012
Black chuckBlack chuck
Simulations with 60-cell modules using their two-diode model representation
Yusufoglu, Institute of Semiconductor Electronics
Irradiance at both planes
GHI, DNI, DHI data acquired from GeoModel Solarwith a time resolution of 15 minutes
Three irradiance types separately determined for front/rear
Direct irradiance– Angle of incidence using azimuth and elevation– For rear planes of south facing modules mainly insignificant
Diffuse irradiance– Perez model [1]
Encapsulation losses resolved over angle of incidence via raytracing [2]
Spectral mismatch with King‘s model [3]
[1] Perez et al., Solar Energy 1990; 44(5); 271-289[2] Tracey, PVLighthouse, http://www.pvlighthouse.com.au/simulation/hosted/tracey/tracey.aspx[3] King et al., SAND2004-3535
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones4
Yusufoglu, Institute of Semiconductor Electronics
Albedo
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones5
)cos1(5.0, TiltAngleGHIE frontAlbedo
odulemRodulemRrearAlbedoPOM VFDHIVFGHIE 21,,
R1
R2
METHOD 1
Calculation of view factor from center of shadow to module surface
Low computational load Homogeneous irradiance at rear plane
METHOD 2
Twice numerical double integration over shadow and each cell surface
Large computational load Inhomogeneous irradiance at rear plane
2
2221
21coscos
AAdA dA
SVF
2 1212
21
121
coscos1A A
AA dAdASA
VF
Yusufoglu, Institute of Semiconductor Electronics
Cell temperature
Time resolved ambient temperature data available
Cell temperature calculation with NOCT formula
𝑇𝑐𝑒𝑙𝑙 = 𝑇𝑎𝑚𝑏𝑖𝑒𝑛𝑡 +𝐼𝑟𝑟𝑎𝑑𝑖𝑎𝑛𝑐𝑒 [𝑊/𝑚2]
800 𝑊/𝑚2(𝑇𝑁𝑂𝐶𝑇 − 20 °𝐶)
Standard modules TNOCT = 45 °C
Bifacial modules TNOCT = 47 °C
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones6
Yusufoglu, Institute of Semiconductor Electronics
Locations studied
Two locations with highly different climates
Oslo, Norway: predominantly diffuse lighthigher percentage of low-light
Cairo, Egypt: predominantly direct lightlong time intervals with high insolation
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones7
0 200 400 600 800 10000
200
400
600
800
1000
Freq
uenc
y [h
ours
/yea
r]
Global horizontal irradiance [W/m2]
Oslo
Cairo
Constraints in simulations: Single module operation
smaller shadows than in field no additional reflection from next row
No soiling/snow
Constant albedo throughout the year
Yusufoglu, Institute of Semiconductor Electronics
South facing modules: Tilt angle optimization
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones8
1397
1402
1208
1213
1088
1093
44 46 48 50 52 54 56 58 60 621045
1050
Ann
ual e
nerg
y yi
eld
[kW
h/kW
p]
2323
2331
1988
19961777
1785
22 24 26 28 30 32 34 36 38 401746
1756
α= 0.5
α= 0.2
Oslo Cairo
STD STD
STDSTD
BIF
BIF
BIF
BIF
Tilt angle [°]
α = 0.2 Larger optimal tilt angles for bifacial modules
α = 0.5 Similar optimal tilt angles for both module types
Larger tilt angles for higher reflective ground
[1] Yusufoglu et al., Energy Procedia, in press
Yusufoglu, Institute of Semiconductor Electronics
South facing modules: Tilt angle optimization
Larger tilt angles for
– Higher reflective ground
– Lower installations
Changes smaller for Oslo
1.5% yield loss @Cairo α=0.5 h=2m when using θopt = 32° instead of 42°
[1] Yusufoglu et al., Energy Procedia, in press
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones9
Module
elevation
Oslo Cairo
α = 0.2 α = 0.5 α = 0.2 α = 0.5
2 m 54 56 31 32
0.5 m 54 57 32 34
0 m 55 58 35 42
Yusufoglu, Institute of Semiconductor Electronics
Vertically installed modules
Vertically installed modules yield nearly same whether front facing East or West
Provided a high albedo vertical installations can yield more than standard modules
No change in yield with varying module elevation
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones10
0
300
600
900
1200
1500
Ann
ual e
nerg
y yi
eld
[kh/
kWp]
STD
sou
thB
IF s
outh
BIF
fron
t E
ast
BIF
fron
t W
est
STD
sou
thB
IF s
outh
BIF
fron
t E
ast
BIF
fron
t W
est
OSLO
α = 0.20
400
800
1200
1600
2000
2400CAIRO
α = 0.2
STD
sou
thB
IF s
outh
BIF
fron
t E
ast
BIF
fron
t W
est
STD
sou
thB
IF s
outh
BIF
fron
t E
ast
BIF
fron
t W
est
α = 0.5 α = 0.5
Yusufoglu, Institute of Semiconductor Electronics
Module elevation & albedo on yield
Annual gain increases with increasing height– Effect of module elevation small in Oslo less prone to nonoptimal installation
Linear relationship between albedo coefficient and annual yield– Larger slope for higher installed modules
[1] Yusufoglu et al., Energy Procedia, in press
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones11
0,20 0,35 0,501900
2000
2100
2200
2300
2400
Ann
ual e
nerg
y yi
eld
[kW
h/kW
p]
Albedo coefficient
Distance of lowermodule edge from ground
2 m 0.5 m 0 m
@ Cairo
190020002100220023002400
0,0 0,5 1,0 1,5 2,01210
12141304
13081398
1404
Cairo
Albedo coefficient 0.5 0.35 0.2
Oslo
Ann
ual e
nerg
y yi
eld
[kW
h/kW
p]
Lower module edge from ground [m]
Yusufoglu, Institute of Semiconductor Electronics
Comparison with standard modules
Increased yields with bifacial modules than standard ones with
– Higher reflective ground
– Higher installations
Yield gain with higher installations insignificant for Oslo
[1] Yusufoglu et al., Energy Procedia, in press
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones12
Module
elevation
Oslo Cairo
α = 0.2 α = 0.5 α = 0.2 α = 0.5
2 m 15.5 % 28.3 % 13.8 % 30.6 %
0.5 m 15.5 % 28.3 % 12.9 % 28.8 %
0 m 15.4 % 28.1 % 10.6 % 24.3 %
Bifaciality gain in yield with respect to standard modules
Yusufoglu, Institute of Semiconductor Electronics
Inhomogenity at rear module plane
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones13
Module elevation: 2 mα = 0.5
Module elevation: 0.1 mα = 0.5
Irradiance at the module rear side [W/m2] on an examplary summer day in Cairo
Yusufoglu, Institute of Semiconductor Electronics
Inhomogenity at rear module plane
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones14
Reduction of nonuniformity with higher module elevation
Module installation optimization more beneficial for direct light dominated regions
Module
elevation
Oslo Cairo
α = 0.2 α = 0.5 α = 0.2 α = 0.52 m 15.5 % 9.3 % 28.3 % 13.9 % 13.8 % 10.0 % 30.6 % 21.5 %0 m 15.4 % 9.3 % 28.1 % 13.3 % 10.6 % 8.3 % 24.3 % 16.5 %
Bifaciality gain in yield with respect to standard modules
Including the inhomogenity at the rear side
Yusufoglu, Institute of Semiconductor Electronics
Conclusion
Optimal tilt angles of south facing bifacial modules is f(Location, α, h)
Generally larger than those of standard modules
Larger tilt angles required for higher reflective ground & lower installations
Locations under predominant diffuse light less sensitive to non-optimal installations
Vertical installations are favorable provided a high reflective ground
Larger annual yields with higher elevated modules Increased influence of module elevation at direct light dominated regions Linearity between α and annual energy yield
Annual yield gain through bifaciality– 30 % (upper limit) vs. 10 - 20 % (realistic) for single module case
27.05.2014Modeling and simulation of annual energy yields of bifacial modules at different climate zones15
Yusufoglu, Institute of Semiconductor Electronics
Thank you for your attention!
This work is part of the project “Kompetenzzentrum für innovative Photovoltaik-Modultechnik NRW” and has been supported by the European Union – European Regional Development Fund and by the Ministry of
Economic Affairs and Energy of the State of North Rhine-Westphalia, Germany.
Thanks to the colleagues at ISC Konstanz for
the measurements.