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IOSR Journal of Computer Engineering (IOSR-JCE)
e-ISSN: 2278-0661,p-ISSN: 2278-8727, Volume 18, Issue 1, Ver. I (Jan – Feb. 2016), PP 16-23
www.iosrjournals.org
DOI: 10.9790/0661-18111623 www.iosrjournals.org 16 | Page
Effect of Angle Orientation of Flat Mirror Concentrator on Solar
Panel System Output
Assist.prof Dr.Ali H.AL-Hamadany*
Assist.prof. Dr.Faten Sh. Zain Al-Abideen** Jinnan H. Ali
*University of Technology/Renewable Energy Research Center
**Almustansiriyah University /Education College/Physics Department
*** Baghdad Governorate
Abstract: In this research two flat glass mirrors is used as concentrator of solar panel system. The mirrors
increase's the concentration of sun light ray on the solar module. Anew model of solar panel system is designed
by mean of software Zemax in order to find best possible inclination angle of the concentrator that improves the
performance of the solar panel. So the efficiency is 59.5% for designed system with inclination angle 60° of the
concentrator. Then a practical design for the solar panel system with concentrators is established. The outdoor
measurements for the practical design indicated that the output power and efficiency is increasing by increasing
the inclination angle of the concentrator and reaches its maximum value at 60o
at different times of the date 5-2-
2014. Also the results showed that the maximum value of efficiency is 0.85 at 11 o'clock at 60o
. While the
maximum value of the output power is 72.8w at 12 o'clock of the same day.
Keywords: solar panel, concentrators, flat mirror concentrator. .
I. Introduction
The need for energy from renewable sources has become a pressing issue in recent years. Renewable
energy is the essential development for the secure future. Among various natural resources, solar energy is a
radiant energy that produced by the sun. The solar energy that is incident on the earth surface can be converted
directly to electricity by photovoltaic (PV) or into thermal energy by solar collectors.
A PV module consists of individual solar cells electrically connected together to increase their power
output. They are packaged so that they are protected from the environment and so that the user is protected from
electrical shock. However, several aspects of PV module design which may reduce either the power output of
the module or its lifetime need to be identified. A final structural component of the module is the edging or
framing of the module. A conventional PV module frame is typically made of aluminum. The frame structure
should be free of projections which could result in the lodgment of water, dust or other matter [1].
The using of solar energy in Iraq faces real problems which indicated as accumulation of dust on solar
panels and the high ambient temperatures. The accumulation comes from the increasing of activity of dust storm
after the year of 2000 due to the global climate change, enlarging the desertification and the shortage in water
resources. The input optical power, that reaches to the solar cells, decrease with period time and reached to
about 50% for one month under the effect of natural deposition of dust [1].
Over the last few decades, there has been an increasing effort from governments, industry and
academic institutions to find useful way to improve the solar cell or photovoltaic cell efficiency. One of these
ways is concentrator photovoltaic systems, which use a limited number of small, specialized, efficient solar cells
and concentrating optics to increase the intensity of sunlight striking the cells such as [2-6].
II. Solar Module Characteristic
A solar Module is a set of solar cells connected in series. Solar panels are referred to by the industry as
solar cell modules or PV modules. Module or panel is flat arrangement of series connected silicon solar cells.
There are generally 30 to 36 solar cells per module. The modules can be wired as series or parallel arrays to
produce higher voltage and currents as illustrated in Figure (1).
Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 17 | Page
Figure (1): The image of solar array [7].
The equivalent circuit of a solar Moduleis the sum of the solar cells equivalent circuits connected in
series. These circuits are shown in Figure (2). With sunlight on the Module and no external load, all the current
from the source is through the series diodes, but the output voltage of the Module is the sum of the voltages
across the diodes [8].
Figure (2): (A) Solar cell equivalent circuit and (B) solar module equivalent circuit [9].
The open circuit voltage (VOC) is the maximum voltage available from a solar cell, and this occurs at
zero current. The open circuit voltage corresponds to the amount of forward bias on the solar cell due to the bias
of the solar cell junction with the light – generated current. The VOC is shown on the IV curve in Figure (2)
[9,10] .
Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 18 | Page
Figure (3): Solar Module Characteristic Curve under Standard Test Conditions (STC) [9].
The VOC can be calculated from the relation [8]:
𝑉𝑜𝑐 =
𝑘𝑇
𝑞
𝑙𝑛
𝐼 𝐿
𝐼 𝑜
+ 1 …………………………………………………. (1)
Where kT/q, is the equivalent thermal voltage, IL is photocurrent (light generated current ) and Io is
reverse saturation current [11].
With sunlight on the Module and a short- circuit load, the entire current source is through the short. This is
the solar Module short-circuit current from the current source is through the short which is denoted (Isc) [8]. Isc
occurs on a point of the curve where the voltage is zero as shown in Figure (2). At this point, the power output
of the solar cell is zero. The series resistance (Rsi) of the solar cell contributes highly on power loss as the
current reaches its maximum limits. Ideally the Isc is equal to the light generated current (IL) which is countered
by all wavelengths less than ( ), numerically expressed as follows [12]:
…………………………………………… (2)
Where( λg) is the maximum wavelength causing generation of carriers, is the external quantum
efficiency which represents the ratio of Photo- generated current to the number of incident photons and
is the incident photon flux. The ISC is due to the generation and collection of light – generated carriers. For an
ideal solar cell at most moderate resistive loss mechanisms , the ISC maximum when the VOC is zero and the light
generated current are identical .Therefore, the (Isc) is the largest current which may be drawn from the solar
cell. It depends on a number of factors like the area of the solar cell, the number of photons, the spectrum of the
incident light, the optical properties (absorption and reflection) of the solar cell, the collection probability of the
solar cell, which depends chiefly on the surface passivation and the minority carrier lifetime in the base [10].
The point (Pm) on the knee of the curve, marks the value of current and voltage at which the module
delivers the greatest power for a given level of sunlight. Under standard test conditions (Irradiance 1000 W/m²,
air mass (AM=1.5 at θ= 60°), angle of incidence (AOI=0°) and temperature (25°C), the maximum current (Im)
and maximum voltage (Vm) at maximum output power (Pm) defined the rated power of the module. The other
characteristics of solar module are conversion efficiency (η) and Fill factor (FF). The conversion efficiency is
defined as the ratio of output electrical power to incident optical power.
The efficiencies equation can be written as [13].
……………………………………………… (3)
Pm =VOC ISC FF ………………………………………………………... (4)
Pin = I× A …………………………………………………………….. (5)
Where Pin is the incident power of the sun and can be calculated from multiplying the (I) solar irradiance in
(W/m²) by the area of the solar cell or module (A) in square meter unit.
Since the (Isc) is proportional to the irradiation, it is important to measure the incident irradiation during the
measurements. The irradiation can be measured using a pyranometer or solar meter device. The surface of the
solar meter is mounted normal to the sun [14].
g

g
dIL


0
)()(
)(
)(
%100%100 
in
mm
in
m
P
VI
P
P

Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 19 | Page
And FF is the ratio of the maximum output power to the product ISC.VOC [13]
………………………………………………………………. (6)
If all the solar cells in a module have identical electrical characteristics, and they all experience the same
insolation and temperature, then all the cells will be operating at exactly the same current and voltage. In this
case, the IV curve of the PV module has the same shape as that of the individual cells, except that the voltage
and current are increased [1]. The overall IV curve of a set of identical connected solar cells is shown Figure (4)
[1].
Figure (4): I-V curve for N cells in series × M cells in parallel [1].
The equation for the circuit is [1]:
𝐼 𝑇 = 𝑀 · 𝐼𝐿 − 𝐼𝑜 𝑒𝑥𝑝
𝑞
𝑉 𝑇
𝑁
𝑛𝑘𝑇
− 1 ………………………………………….(7)
where:
N is the number of cells in series.
M is the number of cells in parallel.
IT is the total current from the circuit.
VT is the total voltage from the circuit.
Io is the saturation current from a single solar cell.
IL is the short-circuit current from a single solar cell.
n is the ideality factor of a single solar cell.
q, k, and T are constants
The total current is simply the current of an individual cell multiplied by the number of cells in parallel.
Such that:
ISC total = ISC × M ……………………………………………….………… (8)
IMP total = IMP × M ……………………………………………………….... (9)
VOC total = VOC × N ………………………………………………………... (10)
VMP total = VMP × N …………………………………………………….…. (11)
III. Solar Panel Model Design Using Software Zemax
A theoretical model has been designed by using software Zemax to determine the best angle of
inclination of the flat mirror concentrator (FMC) which is fixed on the solar panel module and then its
inclination angle is changed from 10o
to 90o
by steps of 10o
in order to get optimum angle that gives higher
efficiency. The input parameters in Zemax window includes:
1-The object distances (for the sun i.e infinity distance).
2- The radius of curvature of the concentrator mirror (∞ i.e plane).
3-The coated material of the concentrator (Ag), (refraction index of the reflection coating).
4-The inclination angle between the concentrator mirror and the solar panel.
5- The dimension of solar concentrator and solar panel (length 146 cm – width 68cm).
6- The wavelength of the incident light (UV wavelength 0-380) nm, (visible wavelength380-780) nm.
7- Entrance pupil diameter of the system 150cm.
8- Filed of view of the total system 0.25
9- The angle of the incident light with the system 45°.
Table (1) shows the change in the inclination angles of the concentrator with the solar panel using the
Zemax and the values of η at each angle.
OCSC
mm
VI
VI
FF 
Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 20 | Page
Table (1): The efficiency of the each angle by Zemax software
Efficiency η %tilt y(θ)z-positionx-position
28%10-60610mir 1
-10-60-610mir2
28%20-120600mir 1
-20-120-600mir2
28%30-180590mir 1
-30-180-590mir2
29.40%40-220550mir 1
-40-220-550mir2
44.30%50-240500mir 1
-50-240-500mir2
59.50%60-280480mir 1
-60-280-480mir2
52%70-320440mir 1
-70-320-440mir2
38%80-350370mir 1
-80-350-370mir2
28%90-360320mir 1
-90-360-320mir2
Table (1) shows that the maximum efficiency is 59.90% at angle 60o
.
The output result after optimaization include:
1-The irradiance distribution on the solar panel.
2-The collection efficiency by the solar panel.
IV. Practical design
The designed system (Figure 5) consist of two concentrator (flat mirrors that made of glass) with length
146 cm and width 68 cm for each one of the mirrors enclosed by aluminum frame and connected with a solar
panel tilted at 45° from the horizon in the direction of the sun to concentrate light on the solar panel in order to
make the sun light covering a largest area of it. The length of the solar panel is 147cm, width 68cm and consists
of 36 solar cell peak power 110W ,peak voltage 17.5V, peak current 6.29Amp, VOC = 22 V and the ISC =6.85
Amp ,weight 12.5 kg, maximum system voltage 1000V ,temperature T=25ºC, Solar radiation 1000W/m².
(a) (b)
Figure (5): (a) The static solar panel with inclination angle 45 ° with horizon
(b) The concentrator inclined with angle 60°.
Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 21 | Page
The inclination angle of the concentrator on the solar panel has changed with different values from
30°to 80° with step by 5° during every 55 minutes once for several times a day.
V. Results
The Figure (6-a -b) show the designed system with inclination angle 60° at which the efficiency is
(59.5%) that constructed from software Zemax. The two plates (red and green), represents the concentrator and
the black one represent the solar panel. The blue lines represent the incident light. The intensity of solar
radiation on the solar panel system is shown in figure (7). While figure (8) show the spectrum of the
illumination intensity of the solar panel system at inclination angle 60°
.
(b) (a)
Figure (6-a-b): Designed solar panel system using software Zemax
with a FM concentrator.
Figure (7): The intensity of solar radiation on the solar panel system.
Figure (8): The spectrum of the illumination intensity of the solar panel system at 60°
The out dower measurements of ISC , VOC , P , T , FF and η for the solar panel system at different times
of the date 5-2-2015 are illustrated in tables (2), (3), (4) and (5).
Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 22 | Page
The results showed the optimum angle that gives the best efficiency for the designed system is 60o
and
this is in a good agreement with the result that is constructed from software Zemax.
Table (2): The characteristics for the static solar panel at different inclination angles of the concentrator at 9 am
on 5-2-2014.
Solar radiation Intensity
( W/cm²)%ƞFF
T
(h.m)
P
(W)
ISC
(amp)
VOC
(V)
Angle
(degree)
1500.421.6922.91.120.980
1500.541.29.229.21.420.975
1500.571.19.531.31.520.970
1500.611.19.833.21.620.865
1500.6819.1137.21.820.760
1500.651.09.1335.11.720.755
1500.611.19.1633.11.620.750
1500.531.29.1928.81.420.645
1500.461.49.2224.91.220.840
1500.381.79.2420.8120.835
1500.381.79.2720.8120.830
Table (3): The characteristics for the static solar panel at different inclination angles of the concentrator at 10 am
on 5-2-2014.
Solar radiation Intensity
( W/cm²)%ƞFF
T
(h.m)
P
(W)
ISC
(amp)
VOC
(V)
Angle
(degree)
1500.312.51017.20.8320.880
1500.382.110.220.8120.875
1500.421.910.423.11.12170
1500.581.410.631.51.52165
1500.82110.944.3221.160
1500.771.010.114222155
1500.771.010.1441.8220.950
1500.731.110.1739.51.920.845
1500.651.210.1935.11.720.740
1500.531.510.2229.11.420.835
1500.382.110.2520.8120.830
Table (4): The characteristics for the static solar panel at different inclination angles of the concentrator at 11
am on 5-2-2014 .
Table (5): The characteristics for the static solar panel at different inclination angles of the concentrator at 12 on
5-2-2014.
Solar radiation Intensity
( W/cm²)%ƞFF
T
(h.m)
P
(W)
ISC (amp)VOC (V)
Angle
(degree)
2500.571.41251.52.520.680
2500.621.312.255.82.720.775
2500.691.112.562.7320.970
2500.761.012.768.63.320.865
2500.80112.1172.83.520.860
2500.801.012.1372.43.520.755
2500.751.012.1668.33.720.750
2500.731.012.1966.53.220.845
2500.731.012.2166.23.220.740
2500.691.112.2462.1320.735
2500.681.112.2761.8320.630
Solar radiation Intensity
( W/cm²)%ƞFF
T
(h.m)
P
(W)
ISC
(amp)
VOC
(V)
Angle
(degree)
2000.481.71135.11.720.780
2000.541.511.439.51.920.875
2000.601.411.643.42.120.770
2000.681.211.849.42.420.665
2000.85111.1161.8320.660
2000.821.011.1359.70.920.655
2000.831.011.15602.920.750
2000.801.011.1757.92.820.745
2000.801.011.1957.62.820.640
2000.771.111.2155.62.720.635
2000.771.1112355.62.720.630
Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output
DOI: 10.9790/0661-18111623 www.iosrjournals.org 23 | Page
VI. Conclusion
The results showed that the output power of the designed system and its efficiency is increasing by
increasing the inclination angle of the concentrator. It reaches its maximum value at 60o
at different times of the
date 5-2-2014. Also the results showed that the maximum value of efficiency is 0.85 at 11 o'clock with
inclination angle 60o
of the concentrating mirror with solar panel. While the maximum value of the output
power is 72.8w at 12 o'clock of the same day.
References:
[1]. Ahmed F. Atwan, Naseer K. Kasim, Ala'a H. Shnieshil, "PV Solar Panel Performance under the Effect of Dust in Baghdad",
RONCHI, Italy, N.3, PP.379-388, 2012.
[2]. Karvelas .E, Papadopoulos A., Dousis D., Markopoulos Y. P., Mathioulakis E., Panaras G., Vamvakas V. and Davazoglou D., ''
Mirrors Based on Total Reflection for Concentration PV Panels'', 4th International Conference on Solar Concentrators for the
Generation of Electricity or Hydrogen, pp 165-168, Attiki, Greece, 2002.
[3]. Maria B., ''Optical Efficiency of Low – Concentrating Solar Energy Systems With Parabolic Reflectors'', 2004.
[4]. David N. W., ''Improved boost mirror for low concentration photovoltaic solar power systems'', Silver Spring, Maryland, e-mail:
davidnelsonwells@yahoo.com, 2009.
[5]. Alaa M. A., "Solar Energy the Suitable Energy Alternative for Iraq Beyond Oil", International Conference on Petroleum and
Sustainable Development IPCBEE , IACSIT Press, Singapore, vol. 26 , 2011.
[6]. Abdilmoutalib H. A. Al- Shareefy, "Study The Performance of Fresnel – Based Photovoltaic Concentrator'', MSc Thesis, Al-
Mustansiriyah University, Education College, Physics Dep., [2012].
[7]. Science and technology ministry, 2008.
[8]. Horowitz, Paul and Hill, "The Art of Electronics'', 2nd
Edition", University of Cambridge, Winfield, P. 932-933, 1989.
[9]. Chesney Mc. P. J., "Solar Electric Power for Instruments at Remote Sites", University of Washington Geophysics Program, Science
for a Changing World (USGS), Open File Report 00-128, 2000.
[10]. Sinton R.A., Cuevas A., "Contactless determination of current – voltage characteristics and minority – carrier lifetimes in
semiconductors from quasi – steady – state photoconductance data ", journal of Applied physics Letters, vol. 69, p.p. 2510-2512,
1996.
[11]. Edward S. Y., "Microelectronic Devices", McGraw-Hill, 1988.
[12]. Hovel H. J., "Semiconductor and Semimetals, Solar Cells", Vol.11, Academic Press, 1975.
[13]. Ashok S. and Pand K. P., "Photovoltaic Measurements ", Solar Cells, Vol. 14, 1985.
[14]. Nilsson, J., "Optical Design and characterization of Solar Concentrators for photovoltaics", Division of Energy and Building Design
Department of architecture and built Environment Lund University, p.p. 43-53, 2005.

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  • 1. IOSR Journal of Computer Engineering (IOSR-JCE) e-ISSN: 2278-0661,p-ISSN: 2278-8727, Volume 18, Issue 1, Ver. I (Jan – Feb. 2016), PP 16-23 www.iosrjournals.org DOI: 10.9790/0661-18111623 www.iosrjournals.org 16 | Page Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output Assist.prof Dr.Ali H.AL-Hamadany* Assist.prof. Dr.Faten Sh. Zain Al-Abideen** Jinnan H. Ali *University of Technology/Renewable Energy Research Center **Almustansiriyah University /Education College/Physics Department *** Baghdad Governorate Abstract: In this research two flat glass mirrors is used as concentrator of solar panel system. The mirrors increase's the concentration of sun light ray on the solar module. Anew model of solar panel system is designed by mean of software Zemax in order to find best possible inclination angle of the concentrator that improves the performance of the solar panel. So the efficiency is 59.5% for designed system with inclination angle 60° of the concentrator. Then a practical design for the solar panel system with concentrators is established. The outdoor measurements for the practical design indicated that the output power and efficiency is increasing by increasing the inclination angle of the concentrator and reaches its maximum value at 60o at different times of the date 5-2- 2014. Also the results showed that the maximum value of efficiency is 0.85 at 11 o'clock at 60o . While the maximum value of the output power is 72.8w at 12 o'clock of the same day. Keywords: solar panel, concentrators, flat mirror concentrator. . I. Introduction The need for energy from renewable sources has become a pressing issue in recent years. Renewable energy is the essential development for the secure future. Among various natural resources, solar energy is a radiant energy that produced by the sun. The solar energy that is incident on the earth surface can be converted directly to electricity by photovoltaic (PV) or into thermal energy by solar collectors. A PV module consists of individual solar cells electrically connected together to increase their power output. They are packaged so that they are protected from the environment and so that the user is protected from electrical shock. However, several aspects of PV module design which may reduce either the power output of the module or its lifetime need to be identified. A final structural component of the module is the edging or framing of the module. A conventional PV module frame is typically made of aluminum. The frame structure should be free of projections which could result in the lodgment of water, dust or other matter [1]. The using of solar energy in Iraq faces real problems which indicated as accumulation of dust on solar panels and the high ambient temperatures. The accumulation comes from the increasing of activity of dust storm after the year of 2000 due to the global climate change, enlarging the desertification and the shortage in water resources. The input optical power, that reaches to the solar cells, decrease with period time and reached to about 50% for one month under the effect of natural deposition of dust [1]. Over the last few decades, there has been an increasing effort from governments, industry and academic institutions to find useful way to improve the solar cell or photovoltaic cell efficiency. One of these ways is concentrator photovoltaic systems, which use a limited number of small, specialized, efficient solar cells and concentrating optics to increase the intensity of sunlight striking the cells such as [2-6]. II. Solar Module Characteristic A solar Module is a set of solar cells connected in series. Solar panels are referred to by the industry as solar cell modules or PV modules. Module or panel is flat arrangement of series connected silicon solar cells. There are generally 30 to 36 solar cells per module. The modules can be wired as series or parallel arrays to produce higher voltage and currents as illustrated in Figure (1).
  • 2. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 17 | Page Figure (1): The image of solar array [7]. The equivalent circuit of a solar Moduleis the sum of the solar cells equivalent circuits connected in series. These circuits are shown in Figure (2). With sunlight on the Module and no external load, all the current from the source is through the series diodes, but the output voltage of the Module is the sum of the voltages across the diodes [8]. Figure (2): (A) Solar cell equivalent circuit and (B) solar module equivalent circuit [9]. The open circuit voltage (VOC) is the maximum voltage available from a solar cell, and this occurs at zero current. The open circuit voltage corresponds to the amount of forward bias on the solar cell due to the bias of the solar cell junction with the light – generated current. The VOC is shown on the IV curve in Figure (2) [9,10] .
  • 3. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 18 | Page Figure (3): Solar Module Characteristic Curve under Standard Test Conditions (STC) [9]. The VOC can be calculated from the relation [8]: 𝑉𝑜𝑐 = 𝑘𝑇 𝑞 𝑙𝑛 𝐼 𝐿 𝐼 𝑜 + 1 …………………………………………………. (1) Where kT/q, is the equivalent thermal voltage, IL is photocurrent (light generated current ) and Io is reverse saturation current [11]. With sunlight on the Module and a short- circuit load, the entire current source is through the short. This is the solar Module short-circuit current from the current source is through the short which is denoted (Isc) [8]. Isc occurs on a point of the curve where the voltage is zero as shown in Figure (2). At this point, the power output of the solar cell is zero. The series resistance (Rsi) of the solar cell contributes highly on power loss as the current reaches its maximum limits. Ideally the Isc is equal to the light generated current (IL) which is countered by all wavelengths less than ( ), numerically expressed as follows [12]: …………………………………………… (2) Where( λg) is the maximum wavelength causing generation of carriers, is the external quantum efficiency which represents the ratio of Photo- generated current to the number of incident photons and is the incident photon flux. The ISC is due to the generation and collection of light – generated carriers. For an ideal solar cell at most moderate resistive loss mechanisms , the ISC maximum when the VOC is zero and the light generated current are identical .Therefore, the (Isc) is the largest current which may be drawn from the solar cell. It depends on a number of factors like the area of the solar cell, the number of photons, the spectrum of the incident light, the optical properties (absorption and reflection) of the solar cell, the collection probability of the solar cell, which depends chiefly on the surface passivation and the minority carrier lifetime in the base [10]. The point (Pm) on the knee of the curve, marks the value of current and voltage at which the module delivers the greatest power for a given level of sunlight. Under standard test conditions (Irradiance 1000 W/m², air mass (AM=1.5 at θ= 60°), angle of incidence (AOI=0°) and temperature (25°C), the maximum current (Im) and maximum voltage (Vm) at maximum output power (Pm) defined the rated power of the module. The other characteristics of solar module are conversion efficiency (η) and Fill factor (FF). The conversion efficiency is defined as the ratio of output electrical power to incident optical power. The efficiencies equation can be written as [13]. ……………………………………………… (3) Pm =VOC ISC FF ………………………………………………………... (4) Pin = I× A …………………………………………………………….. (5) Where Pin is the incident power of the sun and can be calculated from multiplying the (I) solar irradiance in (W/m²) by the area of the solar cell or module (A) in square meter unit. Since the (Isc) is proportional to the irradiation, it is important to measure the incident irradiation during the measurements. The irradiation can be measured using a pyranometer or solar meter device. The surface of the solar meter is mounted normal to the sun [14]. g  g dIL   0 )()( )( )( %100%100  in mm in m P VI P P 
  • 4. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 19 | Page And FF is the ratio of the maximum output power to the product ISC.VOC [13] ………………………………………………………………. (6) If all the solar cells in a module have identical electrical characteristics, and they all experience the same insolation and temperature, then all the cells will be operating at exactly the same current and voltage. In this case, the IV curve of the PV module has the same shape as that of the individual cells, except that the voltage and current are increased [1]. The overall IV curve of a set of identical connected solar cells is shown Figure (4) [1]. Figure (4): I-V curve for N cells in series × M cells in parallel [1]. The equation for the circuit is [1]: 𝐼 𝑇 = 𝑀 · 𝐼𝐿 − 𝐼𝑜 𝑒𝑥𝑝 𝑞 𝑉 𝑇 𝑁 𝑛𝑘𝑇 − 1 ………………………………………….(7) where: N is the number of cells in series. M is the number of cells in parallel. IT is the total current from the circuit. VT is the total voltage from the circuit. Io is the saturation current from a single solar cell. IL is the short-circuit current from a single solar cell. n is the ideality factor of a single solar cell. q, k, and T are constants The total current is simply the current of an individual cell multiplied by the number of cells in parallel. Such that: ISC total = ISC × M ……………………………………………….………… (8) IMP total = IMP × M ……………………………………………………….... (9) VOC total = VOC × N ………………………………………………………... (10) VMP total = VMP × N …………………………………………………….…. (11) III. Solar Panel Model Design Using Software Zemax A theoretical model has been designed by using software Zemax to determine the best angle of inclination of the flat mirror concentrator (FMC) which is fixed on the solar panel module and then its inclination angle is changed from 10o to 90o by steps of 10o in order to get optimum angle that gives higher efficiency. The input parameters in Zemax window includes: 1-The object distances (for the sun i.e infinity distance). 2- The radius of curvature of the concentrator mirror (∞ i.e plane). 3-The coated material of the concentrator (Ag), (refraction index of the reflection coating). 4-The inclination angle between the concentrator mirror and the solar panel. 5- The dimension of solar concentrator and solar panel (length 146 cm – width 68cm). 6- The wavelength of the incident light (UV wavelength 0-380) nm, (visible wavelength380-780) nm. 7- Entrance pupil diameter of the system 150cm. 8- Filed of view of the total system 0.25 9- The angle of the incident light with the system 45°. Table (1) shows the change in the inclination angles of the concentrator with the solar panel using the Zemax and the values of η at each angle. OCSC mm VI VI FF 
  • 5. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 20 | Page Table (1): The efficiency of the each angle by Zemax software Efficiency η %tilt y(θ)z-positionx-position 28%10-60610mir 1 -10-60-610mir2 28%20-120600mir 1 -20-120-600mir2 28%30-180590mir 1 -30-180-590mir2 29.40%40-220550mir 1 -40-220-550mir2 44.30%50-240500mir 1 -50-240-500mir2 59.50%60-280480mir 1 -60-280-480mir2 52%70-320440mir 1 -70-320-440mir2 38%80-350370mir 1 -80-350-370mir2 28%90-360320mir 1 -90-360-320mir2 Table (1) shows that the maximum efficiency is 59.90% at angle 60o . The output result after optimaization include: 1-The irradiance distribution on the solar panel. 2-The collection efficiency by the solar panel. IV. Practical design The designed system (Figure 5) consist of two concentrator (flat mirrors that made of glass) with length 146 cm and width 68 cm for each one of the mirrors enclosed by aluminum frame and connected with a solar panel tilted at 45° from the horizon in the direction of the sun to concentrate light on the solar panel in order to make the sun light covering a largest area of it. The length of the solar panel is 147cm, width 68cm and consists of 36 solar cell peak power 110W ,peak voltage 17.5V, peak current 6.29Amp, VOC = 22 V and the ISC =6.85 Amp ,weight 12.5 kg, maximum system voltage 1000V ,temperature T=25ºC, Solar radiation 1000W/m². (a) (b) Figure (5): (a) The static solar panel with inclination angle 45 ° with horizon (b) The concentrator inclined with angle 60°.
  • 6. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 21 | Page The inclination angle of the concentrator on the solar panel has changed with different values from 30°to 80° with step by 5° during every 55 minutes once for several times a day. V. Results The Figure (6-a -b) show the designed system with inclination angle 60° at which the efficiency is (59.5%) that constructed from software Zemax. The two plates (red and green), represents the concentrator and the black one represent the solar panel. The blue lines represent the incident light. The intensity of solar radiation on the solar panel system is shown in figure (7). While figure (8) show the spectrum of the illumination intensity of the solar panel system at inclination angle 60° . (b) (a) Figure (6-a-b): Designed solar panel system using software Zemax with a FM concentrator. Figure (7): The intensity of solar radiation on the solar panel system. Figure (8): The spectrum of the illumination intensity of the solar panel system at 60° The out dower measurements of ISC , VOC , P , T , FF and η for the solar panel system at different times of the date 5-2-2015 are illustrated in tables (2), (3), (4) and (5).
  • 7. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 22 | Page The results showed the optimum angle that gives the best efficiency for the designed system is 60o and this is in a good agreement with the result that is constructed from software Zemax. Table (2): The characteristics for the static solar panel at different inclination angles of the concentrator at 9 am on 5-2-2014. Solar radiation Intensity ( W/cm²)%ƞFF T (h.m) P (W) ISC (amp) VOC (V) Angle (degree) 1500.421.6922.91.120.980 1500.541.29.229.21.420.975 1500.571.19.531.31.520.970 1500.611.19.833.21.620.865 1500.6819.1137.21.820.760 1500.651.09.1335.11.720.755 1500.611.19.1633.11.620.750 1500.531.29.1928.81.420.645 1500.461.49.2224.91.220.840 1500.381.79.2420.8120.835 1500.381.79.2720.8120.830 Table (3): The characteristics for the static solar panel at different inclination angles of the concentrator at 10 am on 5-2-2014. Solar radiation Intensity ( W/cm²)%ƞFF T (h.m) P (W) ISC (amp) VOC (V) Angle (degree) 1500.312.51017.20.8320.880 1500.382.110.220.8120.875 1500.421.910.423.11.12170 1500.581.410.631.51.52165 1500.82110.944.3221.160 1500.771.010.114222155 1500.771.010.1441.8220.950 1500.731.110.1739.51.920.845 1500.651.210.1935.11.720.740 1500.531.510.2229.11.420.835 1500.382.110.2520.8120.830 Table (4): The characteristics for the static solar panel at different inclination angles of the concentrator at 11 am on 5-2-2014 . Table (5): The characteristics for the static solar panel at different inclination angles of the concentrator at 12 on 5-2-2014. Solar radiation Intensity ( W/cm²)%ƞFF T (h.m) P (W) ISC (amp)VOC (V) Angle (degree) 2500.571.41251.52.520.680 2500.621.312.255.82.720.775 2500.691.112.562.7320.970 2500.761.012.768.63.320.865 2500.80112.1172.83.520.860 2500.801.012.1372.43.520.755 2500.751.012.1668.33.720.750 2500.731.012.1966.53.220.845 2500.731.012.2166.23.220.740 2500.691.112.2462.1320.735 2500.681.112.2761.8320.630 Solar radiation Intensity ( W/cm²)%ƞFF T (h.m) P (W) ISC (amp) VOC (V) Angle (degree) 2000.481.71135.11.720.780 2000.541.511.439.51.920.875 2000.601.411.643.42.120.770 2000.681.211.849.42.420.665 2000.85111.1161.8320.660 2000.821.011.1359.70.920.655 2000.831.011.15602.920.750 2000.801.011.1757.92.820.745 2000.801.011.1957.62.820.640 2000.771.111.2155.62.720.635 2000.771.1112355.62.720.630
  • 8. Effect of Angle Orientation of Flat Mirror Concentrator on Solar Panel System Output DOI: 10.9790/0661-18111623 www.iosrjournals.org 23 | Page VI. Conclusion The results showed that the output power of the designed system and its efficiency is increasing by increasing the inclination angle of the concentrator. It reaches its maximum value at 60o at different times of the date 5-2-2014. Also the results showed that the maximum value of efficiency is 0.85 at 11 o'clock with inclination angle 60o of the concentrating mirror with solar panel. While the maximum value of the output power is 72.8w at 12 o'clock of the same day. References: [1]. Ahmed F. Atwan, Naseer K. Kasim, Ala'a H. Shnieshil, "PV Solar Panel Performance under the Effect of Dust in Baghdad", RONCHI, Italy, N.3, PP.379-388, 2012. [2]. Karvelas .E, Papadopoulos A., Dousis D., Markopoulos Y. P., Mathioulakis E., Panaras G., Vamvakas V. and Davazoglou D., '' Mirrors Based on Total Reflection for Concentration PV Panels'', 4th International Conference on Solar Concentrators for the Generation of Electricity or Hydrogen, pp 165-168, Attiki, Greece, 2002. [3]. Maria B., ''Optical Efficiency of Low – Concentrating Solar Energy Systems With Parabolic Reflectors'', 2004. [4]. David N. W., ''Improved boost mirror for low concentration photovoltaic solar power systems'', Silver Spring, Maryland, e-mail: davidnelsonwells@yahoo.com, 2009. [5]. Alaa M. A., "Solar Energy the Suitable Energy Alternative for Iraq Beyond Oil", International Conference on Petroleum and Sustainable Development IPCBEE , IACSIT Press, Singapore, vol. 26 , 2011. [6]. Abdilmoutalib H. A. Al- Shareefy, "Study The Performance of Fresnel – Based Photovoltaic Concentrator'', MSc Thesis, Al- Mustansiriyah University, Education College, Physics Dep., [2012]. [7]. Science and technology ministry, 2008. [8]. Horowitz, Paul and Hill, "The Art of Electronics'', 2nd Edition", University of Cambridge, Winfield, P. 932-933, 1989. [9]. Chesney Mc. P. J., "Solar Electric Power for Instruments at Remote Sites", University of Washington Geophysics Program, Science for a Changing World (USGS), Open File Report 00-128, 2000. [10]. Sinton R.A., Cuevas A., "Contactless determination of current – voltage characteristics and minority – carrier lifetimes in semiconductors from quasi – steady – state photoconductance data ", journal of Applied physics Letters, vol. 69, p.p. 2510-2512, 1996. [11]. Edward S. Y., "Microelectronic Devices", McGraw-Hill, 1988. [12]. Hovel H. J., "Semiconductor and Semimetals, Solar Cells", Vol.11, Academic Press, 1975. [13]. Ashok S. and Pand K. P., "Photovoltaic Measurements ", Solar Cells, Vol. 14, 1985. [14]. Nilsson, J., "Optical Design and characterization of Solar Concentrators for photovoltaics", Division of Energy and Building Design Department of architecture and built Environment Lund University, p.p. 43-53, 2005.