Evaluation of Concentrated Solar Power Systems and the Impact of
Different Heat Transfer Fluids on Performance
MOHAMED R. GOMAA*, RIAD AHMAD, M. A. NAWAFLEH
Mechanical Engineering Department,
Faculty of Engineering, Al-Hussein Bin Talal University,
Maan, 71110 Maan,
JORDAN
*Corresponding Author
Abstract: - Concentrated solar power (CSP) is one of the main technologies used. Thus, the object of research is
the different concentrated solar power technologies. Moreover, this study aimed to compare the different
concentrated solar power technologies in terms of their efficiency, cost, concentration ratio, and receiver
temperature. Results showed that technologies were arranged according to high to low temperatures: the
parabolic dish reflector, central receiver collector, linear Fresnel reflector, and parabolic trough collector. As
well as, in this study, ranges of the heat transfer fluids are compared with each other by using exergy and
energy analysis. The heat transfer fluids that are examined are liquid sodium, molten salt (60 % NaNO3, 40 %
KNO3), supercritical carbon dioxide (sCO2), water/steam, and air. Results showed that the liquid sodium at an
elevated temperature range of (540–740 °C) is performed the best, with exergy efficiency of 61% of solar-to-
fluid, the best liquid sodium case is at (do=10.3 mm, nbanks = 1, Δprec= 7.72 bar, ηII = 45.47 %) has been found.
Finally, vas a positive and effective approach to solving the energy problems.
Key-Words: - Solar energy; Concentrated solar power; Heat transfer fluid, Concentration ratio, Receiver
efficiency.
Received: November 6, 2022. Revised: August 21, 2023. Accepted: October 1, 2023. Published: October 13, 2023.
1 Introduction
The world is currently moving towards using clean
energy to obtain energy due to the near depletion of
conventional energy sources and the issue of climate
change. In recent years, solar energy has become
one of the most widely used sources of renewable
energy; its use has increased by 35 percent over the
past decade. Among these technologies are CSP
technologies, [1], [2]. It is an active solar system,
meaning that it requires mechanical equipment, such
as fans and pumps, to convert solar energy into
electricity or heat, [3], [4]. A CSP system can
provide high and medium heat for a variety of
applications, including industrial processes,
electricity generation, solar heating, and cooling, as
well as water desalination, [5]. It is the primary
characteristic of CSP systems that they deal directly
with sunlight, as they use solar energy tracking
systems to maximize the amount of sunlight that can
be used to generate and supply power to the tracking
system. Construction and maintenance of this
system are expensive, despite its high efficiency and
productivity, [6]. Globally, solar energy capacity is
growing rapidly to meet the energy demand. The
installed capacity of CSPs indeed increased from
1266 MW in 2010 to 6479 MW in 2020, [7].
Furthermore, the heat transfer fluid (HTF) in
concentrated solar power is also an important
objective, given the large quantity of HTF required
for the operation of CSP plants. Hence, the HTF
must be kept as cost-effective as possible while
maximizing its performance.
The purpose of this study is to compare the
efficiency, cost, concentration ratio, and receiver
temperature of the various concentrated solar power
technologies.
2 Materials and Methods
2.1 System Components
There are typically multiple components to a
Concentrated Solar Power (CSP) system, including
a receiver, an electrical generator, solar
concentrators, and a steam turbine. Figure 1
illustrates the most important parts of this system,
[8].
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Fig. 1: Components of CSP plant, [8].
Mirrors or concentrators are used in solar fields to
direct normal irradiance to an absorber referred to as
the receiver, as well as a heat transfer system and
thermal energy storage system that enhances energy
efficiency and stores energy to allow the plant to be
used at night, however not all CSP plants have
storage capabilities, [9], [10], [11].
2.2 Working Principle of CSP
As part of the solar field, mirrors or concentrators
are used to direct normal sunlight to an absorber,
referred to as the receiver, as well as heat transfer
and thermal energy storage systems that enhance
energy efficiency and store energy for the use of the
plant at night (as shown in Figure 2), though not all
CSP plants can store energy, [12], [13], [14].
Fig. 2: Power generation in the parabolic trough,
[14].
In the first instance, direct solar rays fall onto
the reflecting mirrors, which act as concentrators for
solar rays. After the mirrors are constructed, the
solar rays are reflected toward the receiver, which
can either be a tower or a tube, depending on the
type of station. It is the receiver that receives the
solar radiation coming from the mirrors, and then
the receiver stores the energy of the radiation by
converting it into heat through the use of a working
fluid, which retains the heat in the form of steam for
later use, [13].
2.3 Thermal Energy Storage In CSP
The limited availability of renewable energies such
as wind and solar poses a problem for renewable
energies. Therefore, to resolve these problems,
energy storage is a critical solution, as thermal
energy storage is more cost-effective than electrical
energy storage, Figure 3 shows a parabolic trough
station integrated with a thermal energy storage unit,
[15].
Fig. 3: A parabolic trough station integrated with a
thermal energy storage unit, [15].
Energy industry professionals view the
combination of CSPs and energy storage as an
efficient and effective way of addressing the energy
crisis, [16]. CSPs are considered a vital source of
power generation, as they can provide deployable
electricity in addition to the capability to store
thermal energy. the largest widely used technique in
thermal energy storage (TES) in commercial CSPs
is Molten salt TES, but the industry is searching for
cheaper and more efficient TES systems; and phase
change materials (PCM) are marked as low-cost,
high-energy TES systems, [17]. Because PCMs
offer high-density energy storage, isothermal in
nature, and operation in a variety of temperature
conditions is available, [15]. The use of the PCM
has several advantages including, [17];
1-Improved exergy efficiency.
2- Faster charging and discharging rate.
3- Raised heat transfer rate at the time of charging
and discharging, specifically during phase
change.
Among the phase change processes involved in
PCM energy storage are evaporation,
crystallization, and melting. When the material's
temperature reaches a transition temperature, phase
transition occurs, and the material is transferred
from one state to another, such as from a liquid to a
gas, solid to a liquid, and solid to a gas. In the phase
transition process, solid-to-liquid PCMs are
commonly utilized due to their high density and
low volume change, [18].
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2.4 Types of CSP
A concentrating solar collector consists of a tracking
reflector that tracks the sun and concentrates
radiation onto a line or point receiver. A thermal
fluid circulates in the receiver and its temperature
can rise to about 400 °C (for linear focus) or up to
800 °C (for point focus), [19]. In terms of economic
and technical criteria, CSP technology can be
divided into four different types. They are referred
to as parabolic trough concentrators (PTCs), [4],
linear Fresnel reflectors (LFR), [11], [19], [20],
central receiver\solar towers (ST), and solar dishes,
[21]. Today, CSP technologies are making
tremendous progress around the globe, where the
total installed at the end of 2015 was 4.8 GW, and it
is predicted that by the end of 2030, it will reach
261 GW, [22].
2.4.1 Parabolic Trough Collector (PTC)
In electrical power plants, parabolic trough
collectors are one of the most advanced and mature
technologies that are employed to produce steam or
process heat by absorbing direct solar radiation
using mechanical or hydraulic tracking systems
associated with sensors, [4], [23]. PTC consists of
[24];
a) Collector: polished aluminum, steel, or glass.
b) Receiver: made up of a glass covering and metal
pipe.
c) Reflector: reflector sheet or glass mirrors.
d) Tracking system.
Figure 4 Clarify this component, [24]. Many types
of working fluid can be used as heat carriers inside
the receiver, like; pressurized water, thermal oil, and
Nanofluids which can increase the efficiency of the
process; when using it the temperature of the PTC
receiver tube can reach 350–400 °C, [25], [26], the
installation cost of it about 4500–5800 $/kW, [24].
In addition, the efficiency is about 13-14 %, while
the concentration ratio ranges between 15 and 70.
Fig. 4: Parabolic trough component, [14].
2.4.2 Linear Fresnel Reflector (LFR)
The linear Fresnel reflector (LFR) is a technology in
constant development and has proven to be a cost-
effective means of generating heat over the years.
However, LFR undergoes high optical losses,
resulting in lower thermal efficiency, which is
estimated between 11%-19 %. LFR consists of
separate linear primary mirrors placed near the
ground at a height of about 3-5m above the ground,
this construction is a prosperous future option due to
its low cost and few mechanical issues due to wind
loads compared to PTC. On the other hand, the
optical efficiency of LFRs is limited due to the
space between the main mirrors in addition to the
shadowing and blocking effects of the main mirrors,
[27]. A linear focusing technique requires a single-
axis tracking mechanism to accurately track the
position of the sun Figure 5 shows an LFR station.
In addition, it’s one of the most important
concentrating solar systems for producing usable
heat in the medium and high-temperature range (<
500°C). The concentration ratio ranges from 10 to
50 and the cost of it is very low. LFR receivers
typically have an evacuated tube collector coupled
to a secondary concentrator that is commonly a
compound parabolic concentrator (CPC).
Water/steam is frequently chosen to produce a high-
pressure Super heater saturated steam, which can be
used in Rankine cycle turbines or industrial
processes, Thermal oil Therminol VP-1, and others
are used for various thermal applications up to
400°C.
Fig. 5: LFR power plant, [28].
In addition to that, molten salts can be further
utilized in power generation and used for storage
goals. It is also emphasized that molten salt
application is found to be more thermally efficient
compared to hot oil operation and that molten salt
offers the possibility of operation at higher
temperatures up to 600°C, [28]. Its advantages are
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summed by: firstly, the support structure is simple
and has an acceptable price. Furthermore, the fixed
receiver reduces the risk of heat transfer fluid
(HTF) leakage; in addition, it allows for
comfortable extension of the automatic cleaning
appliance. Finally, its production and spare parts
are readily available on the market, [20].
2.4.3 Parabolic Dish Reflector
An effective solar dish is a point-focus device that
uses a parabolic concentrator to focus direct solar
radiation into a cavity. It can generate a large
amount of clean energy with higher efficiency and
quietness compared to conventional engines, but
the cost of maintenance and installation will be
higher. The system consists of a parabolic
concentrator coupled to a power conversion unit
that consists of a Stirling engine, an alternator, and
a spiral cavity receiver. A parabolic concentrator
collects incident solar irradiation and concentrates it
at a stable focal point on a receiver, Figure 6 shows
the system photograph.
The temperature of the receiver will be very
high because it receives a large supply of
concentrated solar energy, this heat, which is
absorbed by the receiver, will work on heating the
working fluids, which can be hydrogen gas or
helium gas. As the temperature of these gases will
reach 650 °C 750 °C. In addition, for a 25MW
plant, the cost of investment is about 2000 $/kW
and 8000 $/kW and the efficiency may reach 35%
when a concentration ratio equals 1300, and the
temperature of the receiver is 850 K, [28].
Fig. 6: Construction of parabolic dish collector
system, [29[.
Since it possesses high thermal energy and
efficiency, it is generally suitable to supply prime
movers such as Bryton cycles, Rankine cycles,
organic Rankine cycles, and micro gas turbines,
[30]. In addition, one of its properties is that it
doesn't require water for its cooling or operating
processes, making it more suitable for power plant
construction in water-shortage areas, [31]. The
Solar Dish Stirling System has several uses, the
most important of which is shown in Figure 7, [32].
Fig. 7: Solar dish Stirling application, [33].
2.4.4 Central Receiver Collector/Heliostat Field
Collector
Through a two-axis tracking mechanism, the
mirrored collectors, called heliostats, reflect the
incident solar radiation to the absorbing surface
which is located at the top of the tower so that the
sunlight is concentrated at the focal point. This heat
can then be absorbed into the HTF by convection
and radiation. This technique helps in raising the
temperature of HTF and increases the efficiency in
addition to reducing thermal losses, [34], [35].
It’s distinguished by its ability to produce a
hundred megawatts or a thousand gigawatts
universally in 2050 in inexpensive ways, [35].
Moreover, it does not need large spaces to create
the solar tower station. In addition, the temperature
of HTF can reach 1000°C or above, Figure 8
illustrates the Opillustratesa solar power plant with
a central receiver, [36]. Its efficiency ranges from
17% - 21%, and its concentration ratio = 1000, [37],
[38].
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Fig. 8: Working principle of the solar tower, [39].
3 Results and Discussion
3.1 Comparison between CSP Systems
In the next table and charts, the main differences
between the various CSP systems are summarized.
In addition to efficiency, cost, and concentration
ratio, CSPs differ in their receiver temperature as
well. In terms of efficiency, the parabolic dish
reflector occupies the highest rank, as it can reach
up to 35 %, followed by the central receiver
collector with an efficiency of about 21 %, then the
Linear Fresnel reflector and the parabolic trough
collector with an efficiency of about 19 % and 14 %
respectively. On the other hand, in the field of
price, the Linear Fresnel reflector is the most cost-
effective with a very low price, followed by the
parabolic trough collector, central receiver
collector, and parabolic dish reflector respectively.
The concentration ratio is categorized in ascending
order as follows; firstly, the Linear Fresnel reflector
with a ratio of 50, secondly, the Parabolic trough
collector with a ratio of 70, thirdly, the central
receiver collector with a ratio of 1000, the parabolic
dish reflector with the highest ratio of concentration
up to 1300. According to the receiver temperature
for each concentrator, the parabolic trough collector
receiver temperature can reach 400 °C. The Linear
Fresnel reflector with a Receiver temperature of
about 500 °C, as well as, the central receiver
collector receiver temperature can be estimated at
1000 °C. The highest receiver temperature among
each concentrator is for a parabolic dish reflector,
which can reach 1500 °C.
Fig. 9: Efficiencies difference for CSPs
Figure 9 refers to the difference between the
efficiencies of each technique of CSPs. Indeed, the
parabolic dish reflector has the highest efficiency
among the others, and it can reach 35 %, also, it
indicates that the efficiency of the central receiver
collectors is around 21 %, while the efficiency of
the Linear Fresnel reflector is 19 %, finally, the
Parabolic trough collector has the lowest efficiency
which estimated approx. 14 %.
In addition, the concentration ratio differences
for CSPs are shown in Figure 10 clarifying that the
point focuses concentrators (Parabolic dish reflector
and Central receiver collector) own the highest
concentration ratio as it can reach 1300 for the
parabolic dish reflector and 1000 for the Central
receiver collector. Compared with linear focus
concentrators (Parabolic trough and linear Fresnel
reflector) which are estimated to be the parabolic
trough at 70 and the linear Fresnel reflector at 50.
Fig. 10: Concentration ratio differences for CSPs.
Finally, Figure 11 illustrates the differences in
receiver temperature for all CSPs, the highest
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temperature can be obtained from parabolic dish
reflectors as it can reach Up to 1500 °C, then the
central receiver collector with 1000 °C, followed by
the Linear Fresnel reflector with 500 °C, and last is
the parabolic through with around 400 °C.
Fig. 11: Receiver temperature differences for CSPs.
According to the previous comparisons, we can
see that the receiver of parabolic dish reflectors has
a higher temperature than the other CSPs, in
addition to the highest efficiency and concentration
ratio of the others. However, the cost of
construction is more expensive than the others. So,
it is used to supply prime movers such as the
Bryton cycle, Rankine cycle, organic Rankine
cycle, and micro gas turbines, which require high
operating temperatures. On the other hand, the
Linear Fresnel reflector is the cheapest price among
the CSPs. So, it is used for producing usable heat in
the medium and high-temperature range.
3.2 Heat Transfer Fluid (HTF)
Heat transfer fluids (HTF) play a critical role in
collecting energy from the solar field and
transporting it to the power plant. As shown in
Figure 12 the different HTF uses with the solar
application, [38].
Fig. 12: Characteristics of the ideal HTFs
A detailed accounting of exergy is presented in
Figure 13; the liquid Sodium has the best
performance within the selected HTFs, especially in
the higher range of temperatures. In contrast to the
molten salt, liquid sodium can supply heat to the
high-temperature sCO2 Brayton cycle, which has a
higher efficiency of thermal-to-electrical and will
cost less than that of a steam Rankine cycle. As a
result of the lower external wall temperature of
liquid sodium, the receiver performance at lower
temperatures is marginally better than that of
molten salt, even taking into account the exergy
losses in the heat exchanger. Despite its low cost
and dual role as an HTF and TES, molten salt
continues to be a competitive working fluid in
central tower CSP systems, [39]. Water/steam can
connect with the steam turbine directly, which
saves the cost of equipment such as the heat
exchanger, but it has difficulty integrating with the
storage system, [40], [41], [42].
Fig. 13: Detailed exergy of the best-case
configurations found for each working fluid, [20],
[40].
Exergy destruction in absorption was large
during the boiling process because of the low
external wall temperature, while exergy losses in
external radiation are low, [43]. SCO2 seems that it
is not a promising HTF selection for the receiver.
Dealing with high working temperatures and
pressure in the tubes of the receiver causes higher
exergy losses than the anticipated savings resulting
from the direct connection to a sCO2 Brayton cycle.
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Air seems that it is not a strong HTF due to its poor
thermophysical properties, which cause extremely
high external wall temperatures. It has the largest
exergy destruction in internal convection and in
pumping work, across all the fluids. It has to
operate at a lower temperature with low flux to
avoid high external wall temperature, even though
it can work at a high-temperature range (e.g., 800–
1000 °C). Air receivers, if it is feasible, will be
required to make use of channels with enhanced
heat transfer, [20], [38], [44].
Fig. 14: Comparison between receiver efficiency
and Tmax for the selected HTFs
Figure 14 shows a comparison between receiver
efficiency and Tmax for the selected (HTFs), which
shows that the liquid sodium has the highest
performance, then molten salt follows it.
4 Conclusion
As a result of differing tracking strategies and
methods for focusing light, concentrated solar
power generates different receiver temperatures and
varying efficiencies. The Parabolic dish reflector
has the highest receiver temperature which can
reach Up to 1500 °C the highest efficiency value of
about 35 %, and the highest concentration ratio in a
range of 1300. Despite this, it is the most expensive
technique among CSPs it can reach 8000 USD/kW.
while the central receiver collector can record the
temperature of 1000 °C with an efficiency of 21 %
and a concentration ratio of approximately 1000
with a high cost of investment. As an alternative, the
Linear Fresnel reflector is the most efficient and
economical, as it is the least expensive investment,
but it has a limited concentration ratio, estimated at
50, and its receiver temperature can reach 500°C
with a 19% efficiency. The parabolic trough
collector receiver temperature can reach 400 °C
with an efficiency of 14 % and a concentration ratio
of about 70 with a low cost of investment. Finally,
the performance of a range of heat transfer fluids in
the tubular receivers. Among the study of HTF, it is
shown that a strong performance benefit of using the
liquid sodium at a high-temperature range with a
system efficiency of 45.47 %, it also remains better
than the molten salts that have n efficiency of 41.42
% even though at low-temperature range.
Acknowledgement:
We would like to thank the reviewers and the
Editors-in-Chief for spending their valuable time on
the article and we are grateful to all the foundations
that supported us. Special thanks to the Deanship of
Scientific Research, Al-Hussein Bin Talal
University, Maan, Jordan, which funded this
research under grant number 268/2023.
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DOI: 10.37394/232013.2023.18.10
Mohamed R. Gomaa, Riad Ahmad, M. A. Nawafleh
E-ISSN: 2224-347X
Volume 18, 2023
Transactions on Heat and Mass Transfer, Vol.
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WSEAS TRANSACTIONS on FLUID MECHANICS
DOI: 10.37394/232013.2023.18.10
Mohamed R. Gomaa, Riad Ahmad, M. A. Nawafleh
E-ISSN: 2224-347X
Volume 18, 2023
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9163893
Contribution of Individual Authors to the
Creation of a Scientific Article (Ghostwriting
Policy)
The authors equally contributed to the present
research, at all stages from the formulation of the
problem to the final findings and solution under
project supervisor Mohamed R. Gomaa.
Sources of Funding for Research Presented in a
Scientific Article or Scientific Article Itself
This research was funded by the Deanship of
Scientific Research, Al-Hussein Bin Talal
University, Maan, Jordan, grant number 268/2023.
Data Availability Statement:
The manuscript has no associated data.
Conflict of Interest
The authors have no conflict of interest to declare.
Creative Commons Attribution License 4.0
(Attribution 4.0 International, CC BY 4.0)
This article is published under the terms of the
Creative Commons Attribution License 4.0
https://creativecommons.org/licenses/by/4.0/deed.en
_US
WSEAS TRANSACTIONS on FLUID MECHANICS
DOI: 10.37394/232013.2023.18.10
Mohamed R. Gomaa, Riad Ahmad, M. A. Nawafleh
E-ISSN: 2224-347X
Volume 18, 2023