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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume 5 Issue 3, March-April 2021 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470
@ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1171
Calculation of Dynamic System of Solar Photo Electric Batteries
Halimov G. G1, Maxamov X. Т1, Qurbonov B. E2
1Candidate of Technical Sciences, Docent of Department of Labor Training,
2Teacher of Department of Labor Training,
1,2Karshi State University, Karshi, Uzbekistan
ABSTRACT
The study presents the results of the calculation of the dynamic (auto-
rotation) system of solar photovoltaic batteries, which shows that the power
consumed by the auto-turning devicedependsonthesize, massandfrequency
of rotation of the device.
KEYWORDS: Electricity, renewable energy sources, atmospheric mass, total
current, photoelectric battery, two-axis tracker, photoelectricstation, mechanical
power, angular velocity, kinetic energy
How to cite this paper: Halimov G. G |
Maxamov X. T | Qurbonov B. E
"Calculation of Dynamic System of Solar
Photo Electric
Batteries" Published
in International
Journal of Trend in
Scientific Research
and Development
(ijtsrd), ISSN: 2456-
6470, Volume-5 |
Issue-3, April 2021, pp.1171-1174, URL:
www.ijtsrd.com/papers/ijtsrd41110.pdf
Copyright © 2021 by author (s) and
International Journal ofTrendinScientific
Research and Development Journal. This
is an Open Access article distributed
under the terms of
the Creative
CommonsAttribution
License (CC BY 4.0)
(http://creativecommons.org/licenses/by/4.0)
1. INTRODUCTION
It is known that the consumption of energy resources is a
decisive factor in the sustainable development of any
country. Because a certain amount of energy is consumed to
produce each type of product, that is, the unit cost of each
unit of product is directly related to energy consumption [1-
4].
Due to global economic development, by 2030 the demand
for electricity will increase by5%comparedtothe beginning
of the century, and the demand for this will be 23.27 billion
tons of conventional fuel [2,3].
39.1% of the world's electricity is generatedby burningcoal,
17.5% by burning natural gas, 16.9% by nuclear energy,
17.1% by hydropower and 7.9% by burning oil products [2-
7].
As a result of the use of natural fuel and energy resources,
the world annually emits 200 million tons of electricity.tons
of solid particles, 200 mln. tons of sulfur dioxide, 700 mln.
tons of carbon monoxide and 150 mln. tons of nitrogen
oxides are extracted. As a result, various climate changes
occur in nature and lead to severe air pollution [5].
The analysis of the above shows that the current global
population growth and the growing demand for energy, the
rapid development of science and technology, will lead to
socio-economic, environmental and energy problems. This,
in turn, will pave the way for more rapid development of
renewable energy in the world, especially in our country.
2. Method
Determination of the strengthofthesupportingstructuresof
the device and their resistance to wind speed and other
influences through calculations for engineers and
technicians designing and operatingdynamic(auto-turning)
systems (trackers) of solar photovoltaic cells (FEB), and for
maximum absorption of sunlight. it is importanttoknowthe
orientation, evaluate the efficiency of the application of the
tracker, analyze the power consumption and show its
dependence on the device parameters.
Methods of calculation, simplification, evaluation of
efficiency, comparison and analysis were used in the study.
3. Results of the research
It is the basis of renewable energy sources. Solar energy is
calculated. The source of solar radiation (QN) is the Sun,
which has a mass of about 2·1030 kg, a radius of 695300 km,
a temperature of about 60000С in the photosphere, and 40
million 0С in its core. In a year, the Sun radiates 1,3·1024
calories of energy into space.
99% of the solar radiation energy corresponds to a
wavelength in the range of 0.1 ÷ 3 μm. The solar spectrum
consists of three areas: ultraviolet (λ<0.38 μm), the visible
part of the spectrum (0.38 μm < λ <0.78 μm), and infrared
radiation (0.78 μm < λ <3 μm).
The effect of atmospheric parameters on the intensity of
solar radiation reaching the Earth's surfaceisdeterminedby
the atmospheric mass (AM):
IJTSRD41110
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1172
α
Sin
p
p
AM
1
0
⋅
= (1)
where p is the atmospheric pressure and p0 is the normal
atmospheric pressure (101,3kPа),
α is the angle of elevation of the Sun with respect to the
horizon.
The flux density E of solar radiation on the Earth's surface is
determined by the following formula:
∫
∫
∫
∞
∞
−
∞ −
=
=
=
0
1
0
0
0
0
0 λ
λ
λ α
λ
α
τ
λ
τ
λ
λ
λ
d
P
E
d
e
E
d
e
E
E Sin
Sin
h
m
(2)
where - λ
τ is the absorption coefficient in the atmosphere
depending on the wavelength, - QN is the distance traveled
in the atmosphere, h is the altitude of the atmosphere,
h
h e
E
E
P λ
τ
λ
λ −
=
=
0
is the transparency coefficient
describing atmospheric absorption.
Solar radiation falls on an arbitrarily oriented receiving
device on the surface in the form of three different solar
energy flows (Figure 1). At each moment of time (t) on the
surface, the total current QN to the receiving field RS (t) isas
follows [3].
RΣ(t) = Rпр(t) + Rд(t) + Rот(t) (3)
where, the directional solar energy flux is Rpr (t); diffuse or
scattered by clouds, aerosols, dust particles in the
atmosphere - Rd (t); The return of a portion of QN from the
surface in the reflected state is Rot (t).
Solar radiation is converted into electricity when it hits
photoelectric batteries installed in an automotive turning
device on the ground.
Below, we consider the dependence of the power consumed
by a solar photovoltaic cell (FEB) autotransformer(dynamic
system) device on the device size, mass, and rotational
frequency, as well as the efficiency of the device and the
relevance of using this technology.
Figure 1. The main constituents of QN on the surface
1- Sun, 2- Earth's surface, 3- Receiving field, 4- Cloud,
aerosol, dust.
Solar photovoltaic systems serve as an important part of the
supporting structure for photovoltaic batteries (solar
panels) [8-12]. It provides the necessary rigidity for the
entire system and the correct slope angle for the solarpanel.
The combination of the base structure withthesolarpanel is
required to be resistant to various wind speeds and other
environmental influences.
FEBs are installed on base systems. The basesystemhastwo
main views, namely static and dynamic. A characteristic
feature of a static system is that the angle of inclination of
the Sun-oriented modules cannot be changed. Logically, the
solar modules should be maximally illuminated during
daylight hours and oriented to the south.
The dynamic system is called a tracker in English. Its
working process is very simple, the device is designed to
monitor the Sun to the maximum, to increase the FIC. There
are two types, the first is single-axle and the second is
double-axle. A view of a photovoltaic station with a two-axis
tracker is shown in Figure 2.
Figure 2. A solar photovoltaic station with a two-axis
tracker.
A single-axis tracker changes its position relativetoonlyone
axis. Typically, such a tracker looks like a static structure,
and when viewed carefully, this structure is equipped with
an actuator, which changes the angle of inclination of the
device. The actuator, in turn, consistsofa motor-reducerand
a stock. The stock attaches to the table and moves it up or
down. A single-axis tracker changes its angle relative to the
sun several times a year. This is managed through software
that makes 2 to 20 changes per year.
A two-axis tracker is a complex engineering structure that
can be oriented in two different planes. The difference
between a two-axle tracker and a single-axistrackeristhatit
rotates the table at an unlimited 1800 angles, maximizing
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1173
sunlight during the day from sunrise to sunset. It also has a
safe mode in the horizontal position and is also resistant to
strong winds. They automatically control the system for
maximum sunlight reception. The efficiencyofsucha system
is 30-40% higher than that of a static system. It is 15%
higher than a single-base system.
The photovoltaic batteries (FEB) [13-15] auto-rotation
system (hereinafter referred to as the solar tracker) serves
to increase the power generation using them. According to
the company that makes tracker models, the increase in
power generation is up to 45% higher per day than the
electricity produced without the use of solar trackers. The
Solar Tracker also allows you to stabilize the value of
electricity generated during a bright day [16-17].
The main disadvantages of solar trackers are:
1) consumption of electricity for special needsofthetracker;
2) the need for system maintenance.
In the catalogs of the company that manufactures tracker
models, the value of electricity consumed by private devices
alone is shown to be negligibly small, without specifying
certain values of power consumption by transmission
devices (stepper motors). The lack of this data makes it
necessary to evaluate the effectiveness of using a solar
tracker.
To do this, it will be necessary to conduct an analysis of the
power consumption for the specific needs of the device,
especially the transmission. Knowing that the rotationofthe
device depends on the mechanical force, it is also possibleto
determine the effect of the size (mass), mass and rotational
frequency of the device on the required force. Let us
consider a simplified model of a tracker to determine the
mechanical force required for the rotation of a FEB with
mass m, size h, l, f, and rotation frequency n around its axis.
To simplify the calculations, we cannot take into accountthe
effect of friction forces. A simplified drawing ofthetracker is
shown in Figure 3.
Figure 3. Simplified drawing of the tracker.
We use the following formula to determine the mechanical
strength of an object:
t
E
N kin
∆
= , (4)
where N is the mechanical power, Wt; Ekin is the kinetic
energy of the body after the end of the process, J; Δt is the
process time, seconds.
We calculate the kinetic energy of an object using the
following formula:
π
ϕ
ω
2
2
2
∆
= c
kin
j
E , (5)
where
12
)
( 2
2
h
l
m
jc
+
= is the moment of inertia of the body
about the axis passing through the center of mass of the
body according to Steiner's theorem, kg • m2; angular
velocity, rad • s, change in angle of rotation, rad.
In that case, the formula for determining the kinetic energy
will look like this:
π
ϕ
ω
2
24
)
( 2
2
2
∆
+
=
l
h
m
Ekin
(6)
Substituting (6) into (4) we obtain the mechanical force of
the body:
t
l
h
m
N
∆
⋅
∆
+
=
π
ϕ
ω
2
24
)
( 2
2
2
, (7)
From the following expression for determining the angular
velocity, we obtain the following by determiningthevalueof
ϕ
∆
t
∆
∆
=
ϕ
ω , (8)
t
∆
=
∆ ω
ϕ . (9)
Substituting (9) into (7), we obtain the formula for
determining the force required for an object to rotate once
around an axis passing through its center of mass:
π
ω
2
24
)
( 3
2
2
⋅
+
=
l
h
m
N (10)
According to formula (10), the results of the calculation of
the force required for the body to rotate once around the
axis passing through the center of mass are given in Table 1.
Table 1 Power calculation results.
Pном, Wt м.kg h, m l, m n, circle/min N, Wt
250 18 1,64 0,992 1 0,0005
250 18 1,64 0,992 10 0,503
500 36 1,64 1,984 1 0,0018
500 36 1,64 1,984 10 0,815
3000 108 3,28 5,952 1 0,038
3000 108 3,28 5,952 10 37,95
4. Conclusion
The results of the force calculation show that when the
rotational speed of an object (FEB) is small, a small force is
expended so that the body rotates once around an axis
passing through the center of mass. As the mass (m) and
dimensions (h, l) of the FEB increase, so does the force
required for its rotation. The results of thisstudyareofgreat
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1174
importance for engineers and technicians who design and
build dynamic (auto-turn) systems of solar photovoltaic
batteries. In subsequent studies, it will be necessary to take
into account the effect of frictional forces on mechanical
supports and bearings, as well as FIC in different branches of
the tracker.
References
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Теория и экспримент / пер с англ. Под ред. М. М.
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[9] Юлдошев И. А. Кристалли кремнийфотоэлектрик
батареялари асосида бириктирилган энергетик
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авторефарати. Тошкент 2016. 82 бет.
[10] Мамадалимов А. Т., Турсунов М. Н.
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Calculation of Dynamic System of Solar Photo Electric Batteries

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume 5 Issue 3, March-April 2021 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470 @ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1171 Calculation of Dynamic System of Solar Photo Electric Batteries Halimov G. G1, Maxamov X. Т1, Qurbonov B. E2 1Candidate of Technical Sciences, Docent of Department of Labor Training, 2Teacher of Department of Labor Training, 1,2Karshi State University, Karshi, Uzbekistan ABSTRACT The study presents the results of the calculation of the dynamic (auto- rotation) system of solar photovoltaic batteries, which shows that the power consumed by the auto-turning devicedependsonthesize, massandfrequency of rotation of the device. KEYWORDS: Electricity, renewable energy sources, atmospheric mass, total current, photoelectric battery, two-axis tracker, photoelectricstation, mechanical power, angular velocity, kinetic energy How to cite this paper: Halimov G. G | Maxamov X. T | Qurbonov B. E "Calculation of Dynamic System of Solar Photo Electric Batteries" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-5 | Issue-3, April 2021, pp.1171-1174, URL: www.ijtsrd.com/papers/ijtsrd41110.pdf Copyright © 2021 by author (s) and International Journal ofTrendinScientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative CommonsAttribution License (CC BY 4.0) (http://creativecommons.org/licenses/by/4.0) 1. INTRODUCTION It is known that the consumption of energy resources is a decisive factor in the sustainable development of any country. Because a certain amount of energy is consumed to produce each type of product, that is, the unit cost of each unit of product is directly related to energy consumption [1- 4]. Due to global economic development, by 2030 the demand for electricity will increase by5%comparedtothe beginning of the century, and the demand for this will be 23.27 billion tons of conventional fuel [2,3]. 39.1% of the world's electricity is generatedby burningcoal, 17.5% by burning natural gas, 16.9% by nuclear energy, 17.1% by hydropower and 7.9% by burning oil products [2- 7]. As a result of the use of natural fuel and energy resources, the world annually emits 200 million tons of electricity.tons of solid particles, 200 mln. tons of sulfur dioxide, 700 mln. tons of carbon monoxide and 150 mln. tons of nitrogen oxides are extracted. As a result, various climate changes occur in nature and lead to severe air pollution [5]. The analysis of the above shows that the current global population growth and the growing demand for energy, the rapid development of science and technology, will lead to socio-economic, environmental and energy problems. This, in turn, will pave the way for more rapid development of renewable energy in the world, especially in our country. 2. Method Determination of the strengthofthesupportingstructuresof the device and their resistance to wind speed and other influences through calculations for engineers and technicians designing and operatingdynamic(auto-turning) systems (trackers) of solar photovoltaic cells (FEB), and for maximum absorption of sunlight. it is importanttoknowthe orientation, evaluate the efficiency of the application of the tracker, analyze the power consumption and show its dependence on the device parameters. Methods of calculation, simplification, evaluation of efficiency, comparison and analysis were used in the study. 3. Results of the research It is the basis of renewable energy sources. Solar energy is calculated. The source of solar radiation (QN) is the Sun, which has a mass of about 2·1030 kg, a radius of 695300 km, a temperature of about 60000С in the photosphere, and 40 million 0С in its core. In a year, the Sun radiates 1,3·1024 calories of energy into space. 99% of the solar radiation energy corresponds to a wavelength in the range of 0.1 ÷ 3 μm. The solar spectrum consists of three areas: ultraviolet (λ<0.38 μm), the visible part of the spectrum (0.38 μm < λ <0.78 μm), and infrared radiation (0.78 μm < λ <3 μm). The effect of atmospheric parameters on the intensity of solar radiation reaching the Earth's surfaceisdeterminedby the atmospheric mass (AM): IJTSRD41110
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1172 α Sin p p AM 1 0 ⋅ = (1) where p is the atmospheric pressure and p0 is the normal atmospheric pressure (101,3kPа), α is the angle of elevation of the Sun with respect to the horizon. The flux density E of solar radiation on the Earth's surface is determined by the following formula: ∫ ∫ ∫ ∞ ∞ − ∞ − = = = 0 1 0 0 0 0 0 λ λ λ α λ α τ λ τ λ λ λ d P E d e E d e E E Sin Sin h m (2) where - λ τ is the absorption coefficient in the atmosphere depending on the wavelength, - QN is the distance traveled in the atmosphere, h is the altitude of the atmosphere, h h e E E P λ τ λ λ − = = 0 is the transparency coefficient describing atmospheric absorption. Solar radiation falls on an arbitrarily oriented receiving device on the surface in the form of three different solar energy flows (Figure 1). At each moment of time (t) on the surface, the total current QN to the receiving field RS (t) isas follows [3]. RΣ(t) = Rпр(t) + Rд(t) + Rот(t) (3) where, the directional solar energy flux is Rpr (t); diffuse or scattered by clouds, aerosols, dust particles in the atmosphere - Rd (t); The return of a portion of QN from the surface in the reflected state is Rot (t). Solar radiation is converted into electricity when it hits photoelectric batteries installed in an automotive turning device on the ground. Below, we consider the dependence of the power consumed by a solar photovoltaic cell (FEB) autotransformer(dynamic system) device on the device size, mass, and rotational frequency, as well as the efficiency of the device and the relevance of using this technology. Figure 1. The main constituents of QN on the surface 1- Sun, 2- Earth's surface, 3- Receiving field, 4- Cloud, aerosol, dust. Solar photovoltaic systems serve as an important part of the supporting structure for photovoltaic batteries (solar panels) [8-12]. It provides the necessary rigidity for the entire system and the correct slope angle for the solarpanel. The combination of the base structure withthesolarpanel is required to be resistant to various wind speeds and other environmental influences. FEBs are installed on base systems. The basesystemhastwo main views, namely static and dynamic. A characteristic feature of a static system is that the angle of inclination of the Sun-oriented modules cannot be changed. Logically, the solar modules should be maximally illuminated during daylight hours and oriented to the south. The dynamic system is called a tracker in English. Its working process is very simple, the device is designed to monitor the Sun to the maximum, to increase the FIC. There are two types, the first is single-axle and the second is double-axle. A view of a photovoltaic station with a two-axis tracker is shown in Figure 2. Figure 2. A solar photovoltaic station with a two-axis tracker. A single-axis tracker changes its position relativetoonlyone axis. Typically, such a tracker looks like a static structure, and when viewed carefully, this structure is equipped with an actuator, which changes the angle of inclination of the device. The actuator, in turn, consistsofa motor-reducerand a stock. The stock attaches to the table and moves it up or down. A single-axis tracker changes its angle relative to the sun several times a year. This is managed through software that makes 2 to 20 changes per year. A two-axis tracker is a complex engineering structure that can be oriented in two different planes. The difference between a two-axle tracker and a single-axistrackeristhatit rotates the table at an unlimited 1800 angles, maximizing
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1173 sunlight during the day from sunrise to sunset. It also has a safe mode in the horizontal position and is also resistant to strong winds. They automatically control the system for maximum sunlight reception. The efficiencyofsucha system is 30-40% higher than that of a static system. It is 15% higher than a single-base system. The photovoltaic batteries (FEB) [13-15] auto-rotation system (hereinafter referred to as the solar tracker) serves to increase the power generation using them. According to the company that makes tracker models, the increase in power generation is up to 45% higher per day than the electricity produced without the use of solar trackers. The Solar Tracker also allows you to stabilize the value of electricity generated during a bright day [16-17]. The main disadvantages of solar trackers are: 1) consumption of electricity for special needsofthetracker; 2) the need for system maintenance. In the catalogs of the company that manufactures tracker models, the value of electricity consumed by private devices alone is shown to be negligibly small, without specifying certain values of power consumption by transmission devices (stepper motors). The lack of this data makes it necessary to evaluate the effectiveness of using a solar tracker. To do this, it will be necessary to conduct an analysis of the power consumption for the specific needs of the device, especially the transmission. Knowing that the rotationofthe device depends on the mechanical force, it is also possibleto determine the effect of the size (mass), mass and rotational frequency of the device on the required force. Let us consider a simplified model of a tracker to determine the mechanical force required for the rotation of a FEB with mass m, size h, l, f, and rotation frequency n around its axis. To simplify the calculations, we cannot take into accountthe effect of friction forces. A simplified drawing ofthetracker is shown in Figure 3. Figure 3. Simplified drawing of the tracker. We use the following formula to determine the mechanical strength of an object: t E N kin ∆ = , (4) where N is the mechanical power, Wt; Ekin is the kinetic energy of the body after the end of the process, J; Δt is the process time, seconds. We calculate the kinetic energy of an object using the following formula: π ϕ ω 2 2 2 ∆ = c kin j E , (5) where 12 ) ( 2 2 h l m jc + = is the moment of inertia of the body about the axis passing through the center of mass of the body according to Steiner's theorem, kg • m2; angular velocity, rad • s, change in angle of rotation, rad. In that case, the formula for determining the kinetic energy will look like this: π ϕ ω 2 24 ) ( 2 2 2 ∆ + = l h m Ekin (6) Substituting (6) into (4) we obtain the mechanical force of the body: t l h m N ∆ ⋅ ∆ + = π ϕ ω 2 24 ) ( 2 2 2 , (7) From the following expression for determining the angular velocity, we obtain the following by determiningthevalueof ϕ ∆ t ∆ ∆ = ϕ ω , (8) t ∆ = ∆ ω ϕ . (9) Substituting (9) into (7), we obtain the formula for determining the force required for an object to rotate once around an axis passing through its center of mass: π ω 2 24 ) ( 3 2 2 ⋅ + = l h m N (10) According to formula (10), the results of the calculation of the force required for the body to rotate once around the axis passing through the center of mass are given in Table 1. Table 1 Power calculation results. Pном, Wt м.kg h, m l, m n, circle/min N, Wt 250 18 1,64 0,992 1 0,0005 250 18 1,64 0,992 10 0,503 500 36 1,64 1,984 1 0,0018 500 36 1,64 1,984 10 0,815 3000 108 3,28 5,952 1 0,038 3000 108 3,28 5,952 10 37,95 4. Conclusion The results of the force calculation show that when the rotational speed of an object (FEB) is small, a small force is expended so that the body rotates once around an axis passing through the center of mass. As the mass (m) and dimensions (h, l) of the FEB increase, so does the force required for its rotation. The results of thisstudyareofgreat
  • 4. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD41110 | Volume – 5 | Issue – 3 | March-April 2021 Page 1174 importance for engineers and technicians who design and build dynamic (auto-turn) systems of solar photovoltaic batteries. In subsequent studies, it will be necessary to take into account the effect of frictional forces on mechanical supports and bearings, as well as FIC in different branches of the tracker. References [1] Зохидов Р. А. Возобновляемыеисточникиэнергии –новый поворот в энергетике. Гелиотехника - 2002. -№2. С. 101-111. [2] Хайриддинов Б. Э., Холмирзаев Н. С., Халимов Ғ. Ғ., Рисбаев А. С., Эргашев Ш. Ҳ. Муқобил энергия манбаларидан фойдаланиш асослари. – Тошкент: “Адабиёт учқунлари”, 2017. -422 бет. [3] Юлдашев И. А., Турсунов М. Н., Шоғўчқоров С. Қ., Жамолов Т. Р. Қуёш энергетикаси. Ўқув қўлланма Тошкент. ТошДТУ. 2020. 166 бет. [4] Зайнутдинова Х. К. Использование солнечной энергии в Узбекистане: Вопросы рынков и маркетинга // Ташкент: Фан, 2015, -336 с. [5] Яблоков Л. Д., Логинов И. Г. Паровые и газовые турбоустановки: Учебное пособие для техникумов. – М. Энергомиздат, 1988. – 352 с. [6] Ҳалимов Ғ. Ғ., Вардияшвили А. А., Эшматов М. М. Қуёш энергиясини электр энергиясига айлантирувчи фотовольтаикқурилма.Materialsof international conference “The modern problems of renewable energy sources and sustainable environment” Тashkent, September 25-27th, 2019. 65-68 бетлар. [7] Халимов Ғ. Ғ., Хайриддинов Б. Э., Вардияшвили. А. А., Холмирзаев Н. С. Европа иттифоқининг “ERASMUS” дастури асосида бажариладиган “RENES” лойиҳаси. ҚарДУ хабарлари. 2017-422 бет. [8] Фаренбрух А., Бьюб Р. Солнечные элементы: Теория и экспримент / пер с англ. Под ред. М. М. Колтуна - М, : Ээнергоатомиздат, 1987. -280 с. [9] Юлдошев И. А. Кристалли кремнийфотоэлектрик батареялари асосида бириктирилган энергетик қурилмалар. Докторлик диссертацияси авторефарати. Тошкент 2016. 82 бет. [10] Мамадалимов А. Т., Турсунов М. Н. Яримўтказгичли қуёш элементлари физикаси ва технологияси. Ўқув қўлланма. Тошкент, ТошДТУ 2002. 94 бет. [11] Чопра К., Дас С. Тонкопленочные солнечные элементы. Перевод с английского с сокращениями. – Москва: Мир, 1986. — 435 с. с иллюстрациями. [12] Н. Герасименко, Ю. Пархоменко. Кремний – материал наноэлектроники. Москва: Техносфера, 2007. — 351 с. с иллюстрациями. [13] Германович В., Турилин А. Альтернативные источники энергии и энергосбережение практические конструкции по использованию энергии ветра, солнца, земли, воды, биомассы. Санкт-Петербург: Наука и Техника, 2014. – 320 с. [14] В. И. Виссарионов, Г. В. Дерюгина, В. А. Кузнецова, Н. К. Малинин. Солнечная энергетика. Методы расчетов. Москва: «Солнечная энергетика» МЭИ, 2008. – 317 с. [15] Стэн Гибилиско. Альтернативная энергетика без тайн. Перевод с английского. – Москва: Эксмо- Пресс, 2010. – 368 с. с иллюстрациями. [16] Пабло Росси,МатиасСейсас.Солнечныебатареии трекеры. Техническое исследование в области энергетики. Sciencia Scripts. 2020. -152 с. [17] Гросс К. А., КрауиньшП. Я., Крауиньш Д. П., Кухта М. С., Соколов А. П. Энергоэффективность подвижных и неподвижных конструкций солнечных панелей. Известия Томского политехнического университета. Инжиниринг георесурсов. 2018. Т. 329. №3. с. 113-122.