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Renewable Energy 28 (2003) 873–886 www.elsevier.com/locate/renene

Technical and economical evaluation of solar thermal power generation

Theocharis Tsoutsosa,∗, Vasilis Gekasb, Katerina Marketakib

a Centre for Renewable Energy Sources (CRES), 19th km Marathon Avenue, 19009 Pikermi, Greece b Department of Environmental Engineering, Technical University of Crete, Crete, Greece

Received 23 July 2002; accepted 24 July 2002

Abstract

This article presents a feasibilty on a solar power system based on the Stirling dish (SD) technology, reviews and compares the available Stirling engines in the perspective of a solar Stirling system.

The system is evaluated, as a parameter to alleviate the energy system of the Cretan island while taking care of the CO2 emissions. In the results a sensitivity analysis was implemented, as well as a comparison with conventional power systems.

In the long-term, solar thermal power stations based on a SD can become a competitive option on the electricity market, if a concerted programme capable of building the forces of industry, finance, insurance and other decision makers will support the market extension for this promising technology.  2002 Elsevier Science Ltd. All rights reserved.

Keywords: Technical and economical evaluation; Solar electricity generation; Solar thermal power; Stir- ling engine

1. Introduction

The electrical generating demand has increased in the island of Crete due to the economic growth during recent years. The rate of this increase becomes dramatical during the summer. Conventional fossil fuel plants generate the electricity and this

∗ Corresponding author. Tel.:+30-1603-9900; fax:+30-1603-9904. E-mail address: [email protected] (T. Tsoutsos).

0960-1481/03/$ - see front matter 2002 Elsevier Science Ltd. All rights reserved. PII: S 0 9 6 0 -1 4 8 1 ( 0 2 ) 0 0 1 5 2 - 0

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energy production cost is very high (Table 1); this cost can be higher in other Greek islands [1].

The power generation should be increased over the next years in order to satisfy the power demand. The new power plants should be environmentally since there already exist some conventional fossil fuel power plants in the island.

Crete is very rich in renewable energy sources. In this paper the option of the establishment of solar thermal power station based on Stirling dish (SD) technology is evaluated to alleviate the energy system of the island.

The system can be a clean and efficient solution to the major energy problem of the island[2].

2. Solar Stirling engines

2.1. Solar thermal electric technology

Solar thermal electric power generating systems incorporate three different design alternatives:

� Parabolic trough collector: focus systems that concentrate sunlight onto tubes located along the focus line of a parabolic-shaped reflective trough.

� Power tower: focus central receiver systems that use large fields of sun-tracking reflectors (heliostats) to concentrate sunlight on a receiver placed on top of a tower.

� Parabolic dishes: focus dish systems reflect light into a receiver at the dish’ s focus [3,4].

Exceptional performance (almost 30%) has been demonstrated by SD systems, which belong to the third design type described above [5].

In general, meteorological, operational and demand side conditions are critical

Table 1 Costs of the conventional power supply systems in the island of Crete

Alternative power supply Investment( /kW) Operating costs systems

Fuel cost O&M variable O&M fixed ( /kWh) ( /kWh) ( /kW/year)

Gas turbines – 0.118 1.76 26.41 Diesel engines 34.37 0.026 1.17 22.01 Steam units 79.85 0.036 2.05 24.95 GT to CC conversion 50.03 0.079 1.46 17.61

Source: [1].

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when comparing the alternative solar power systems directly [6]. The comparison shows that each technology has its strengths and weaknesses, and a final decision on the implementation of a particular project can only be taken by considering the special circumstances at each site [7]. Moreover each technology has advanced vari- ants with different performance and costs [8]. In order to get an overview, a decision maker is forced to consult specialists on each technology.

2.2. Solar Stirling engines

Engine designs for SD applications are usually categorized as either kinematic or free-piston.

� Kinematic Stirling engines: both the power piston and the displacer (or the com- pression and the expansion pistons) are mechanically (kinematically) linked to a rotating power output shaft.

� Free-piston Stirling engine: they have only two moving parts, the displacer and the power piston, which travel back and forth between springs. A linear alternator is incorporated into the power piston to extract power from the engine. As elec- tricity is generated internally, there is no sliding seal at the high-pressure region of the engine therefore no oil lubrication is required. These designs promise long lifetimes with minimal maintenance requirements.

The technical challenges of the kinematic Stirling engine are sealing problems and complicated power modulation. Sealing problems can be avoided if a rotating alter- nator is integrated in the crankcase. The power modulation problem can be solved: (a) by varying the pressure level of the working space; and (b) by varying the piston stroke. The second power modulation method requires a mechanism to vary the piston stroke, a so-called swash plate. Varying the angle between the swash plate and the outgoing axis of the engine varies the piston stroke. Each of these power modulation methods results in a complex engine design, which includes a large num- ber of critical mechanical parts [9,10].

Free-piston Stirling engines have the advantages of kineatic Stirling engine, but avoid the technical problems. It can be hermetically sealed, eliminating the need for a working fluid make-up system typical of a kinematic Stirling engines. In addition there is no connection between the power piston and the displacer piston. Both the phase angle between them and the stroke of the power piston are therefore variable and the power developed by the engine depends on both. This means that, in principle at least, the power of the engine could be controlled without having to change the pressure. Therefore, free-piston Stirling engines have simple design [11].

The only disadvantage of the SD system is its cost. However, this cost is less than the cost of a photovoltaic unit and comparable to the cost of parabolic trough systems, which is used commercially in California. Furthermore, the combination of technical improvements and mass production could reduce this cost by over 50% [7].

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2.3. The Stirling engine and the environment

The Stirling engine is an environmentally very clean engine, because, when the heat comes from solar energy, the polluting emissions are almost zero. When the heat comes from hydrocarbon (HC) combustion, the emissions are also very low, because the fuel is burnt continuously and at near atmospheric pressure, in remark- able contrast to the interrupted, explosive combustion in petrol and diesel engines with relatively cold walls.

The combustion of fuel in a Stirling engine takes place in a space surrounded by hot walls, under adiabatic conditions. Because of this and because of the latitude in the choice of the air-to-fuel ratio the quantities of the CO produced and of the unburnt HCs are very low. Unfortunately, the more efficient combustion of a Stirling engine results in proportionately more CO2 being produced than with an equivalent internal engine. However, the CO2 is one of the most important contributors to the greenhouse effect. Therefore, if the Stirling is to maintain its position as an environmentally friendly engine, then some techniques for removing the exhaust CO2 must be used.

The preheating of combustion air leads to a high flame temperature (~2000°C), which favors the formation of NOx, yet these emissions are lower than expected. This is due to relatively short residence time of the gases at the high temperature, lower peak temperatures than in the internal combustion engine and the continuous combustion. The production of NOx can be reduced more: (a) by recirculating part of the flue gasses along with the incoming combustion air; and (b) by lowering the flame temperature. The Stirling cycle is not effected detrimentally due to the external heating of the engine.

Regarding the emission of toxic or other polluting substances, the Stirling engine is inherently cleaner than all other current heat engines [11].

2.4. Description of the SD solar electric generating system

The SD electric systems, providing net solar-to-electric conversion efficiencies reaching 30%, can operate as stand-alone units in remote locations or can be linked together in groups to provide utility-scale power [12].

Individual units range in size from 10–25 kW. They consist of a solar concentrator, and a power conversion unit located at the focal point of the dish. The unit consists of a cavity receiver and a Stirling heat engine with an electric generator or alternator. The concentrator reflects and concentrates solar radiation, which is then delivered to the receiver. The receiver absorbs concentrated sunlight, transferring its heat energy to a working fluid, in the Stirling engine. The working gas (typically H2 or He) is alternately heated and cooled. The engine works by compressing the working gas when it is cool and expanding it when it is hot. Expanding the hot gas that is required to compress the cool gas produces more power. This action produces a rising and falling pressure on the engine’ s piston, the motion of which is converted into mechanical power. An electric generator or an alternator converts the mechanical power into electricity [13].

Solar SD engines have advantages over more conventional power generation options because they:

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� produce zero emissions when operating on solar energy; � operate more quietly than diesel or gasoline engines; � are easier to operate and maintain than conventional engines; � start up and shut down automatically; and � operate for long periods with minimal maintenance.

Solar concentrators used for SD applications are generally point-focus parabolic dish concentrators. Because of the parabolic shape, the dishes have concentrations ratios ranging from 600–2000 and they can achieve temperatures in excess of 1500°C.

The size of the solar collector for SD systems is determined by the power output desired at maximum insolation levels (1000 W/m2) and the collector and power- conversion efficiencies. With current technologies, a 5 kW SD system requires a dish of ca 5.5 m, in diameter, and a 25 kW system requires a dish ca 10 m in diameter.

Concentrators can typically account for ca 25% of the cost of a SD system. Con- centrating reflectors can be divided in three categories as follows.

� Glass-faceted concentrators use spherically curved individually align glass mirror facets, mounted on an approximate parabolic-shaped structure.

� Full-surface parabolic concentrators: the entire surface forms an approximately parabolic shape.

� Stretched-membrane concentrators: can be a single-facet or multifaceted. The designs incorporating thin membranes stretched over both sides of a metal ring. The membranes may be thin plastic sheeting or thin metal sheeting with a reflec- tive coating applied to one of the membranes.

Tracking the sun’ s path increases the efficiency of the concentrator. There are two ways of implementing this:

� Azimuth-elevation tracking: in which the dish rotates in a plane parallel to the earth (azimuth) and in another plane perpendicular to it.

� Polar tracking method: in which the collector rotates about an axis parallel to the earth’ s axis of rotation and about the declination axis which is perpendicular to the polar axis.

3. Characteristics of the solar power plant

The design characteristics of a typical system (solar electricity system SD 25 kW) are shown in Table 2 [14].

Important performance advantages of the SD are its ability to operate earlier and later each day and it can also operate on cloudy days when solar energy is �2 kWh/m2. In addition, due to its low thermal inertia, it can generate power between passing clouds as a photovoltaic unit can. Central receiver and parabolic trough require 1–2 h of steady insolation between clouds for successful start-ups. During

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Table 2 Design characteristics of a solar electricity system SD 25 kW

Concentrator Glass area 91.01 m2

Aperture area 87.67 m2

Focal length 7.45 m Glass type No. 82 Commercial grade float. Thickness: 0.7

mm Radius of curvature 599, 616, 667, 698” Waviness �0.6 mr Reflectivity �90% Module dimensions 11.89 mH, 11.28 W Module weight 6.934 kg Stirling engine (kinematic) Engine dry weight 225 kg Displacement 380 cc Engine dimensions 66 cm W, 71 cm H, 58cm L Number of pistons 4. double acting Working fluid H2 or He Working fluid pressure 20 MPa Operating temperature 720°C Power control Fluid pressure Cooling Water/forced air fan Output power 27 kW (max), 22 kW (rated) Rated power efficiency 38–40% Power conversion unit Weight �680 kg Alternator Induction, 1800 rpm Alternator efficiency 92–94% Electrical power 480 V, 60 Hz, three phase Gross power rating 25 kW at 1.000W/m2

Peak net power efficiency 29–30% Minimum insolation 250–300 W/m2

Dimensions W=168 cm, H=122 cm, L=183 cm

Source: [10].

frequent cloud passes for such systems the start up efforts consume more power would then be generated [15] (Figs. 1 and 2).

The size of the solar power plant for this analysis is 50 MW and it’ s going to be located at a region with high solar radiation and low cost of land. The location of the solar thermal power plant for this study will be in southeast side of Crete (Lasithi) (Table 3), where the average annual solar radiation is high (1.728 kWh/m2) and land cost is low (23.5–29.0 k /ha).

4. Cost estimation

The selected economic indicators are: the net present value (NPV) and electricity generation cost.

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Fig. 1. Stirling Energy Systems, Inc. (SES)/Boeing, 25 kW SD system at sunset. Source: [15].

NPV � (E�O) 1�(1 � i)�N

i �CC,

where E is the annual income, O is the annual operating and maintenance cost, i is the discount rate and CC is the capital cost.

Electricity generation cost � NPV

Total electricity production .

The energy inflation is considered negligible. NPV and electricity generation cost are estimated for two different annual pro-

duction levels of 10 000 and 2000 SD systems (Tables 4 and 5). Other issues, such as siting as well as the optimal solar power plant size, were not covered by the current analysis.

A series of sensitivity analyses is undertaken in order to investigate the magnitude of the effect of the parameters variation on cost calculation. The parameters are:

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Fig. 2. McDonnell Douglas (currently Boeing) SD system. Source: [15].

Table 3 Weather conditions in Crete

Iraklio Ierapetra Rethimno Chania

Annual solar radiation (kWh/m2) 1785.4 1728.0 1739.9 1700.6 (slope 0°) Annual sunlight (h/year) 2816 3108 2694 2809 Average temperature per year (°C) 19.0 20.0 19.6 18.5

Source: [3].

� system capital purchase price; � discount rate; � annual solar radiation; � lifetime; � annual efficiency of the system; � market price of the electricity; and � size of the power plant.

5. Discussion and conclusions

The technology system, which was described, is a considerable alternative to deal with the energy problems of the island of Crete. It is also essential the timing of

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Table 4 Assumptions and data

Annual production rate of SD systems 10 000 2000

Technical data Number of units 25 25 Total power (MW) 50 50 Annual solar radiation (kWh/m2) 1.728 1.728 Annual generated electric energy (MWh) 69.711 69.711 Discount rate 10% 10% Lifetime (years) 30 30 Sale price of electricity ( /kWh) 0.073 0.073 System purchase price ( /kW) 555a 1.611a

Fixed cost Procurement of equipment (M ) 22.40 64.89 Transport & installation (M ) 3.36 9.73 Land purchase (M ) 1.90 1.90 Earthworks etc (M ) 2.20 9.96 Other costs (M ) 7.46 2.16 O&M Labor cost (k ) 2.2 2.2 Consumables (M ) 1.01 1.01

a [8].

Table 5 Results

Annual production rate of SD systems 10 000 2000

Electricity generation cost ( /kWh) 0.071 0.178 Net present value (k ) 1.380 �69.479

the high demand (midday, summer) and the high insolation offering a solution during the summer period.

Furthermore the substitution of an imported liquid fuel, the avoidance of the CO2 emissions, the creation of new jobs and the improvement of the living standard are essential benefits.

According to the results of the above analysis only the massive production of solar Stirling systems could provide a long-term economical feasible solution. The technical and economic evaluation shows that the SD technology offers a technical feasible and economic viable solution under the following conditions (Table 6):

� system purchase price �550 /kW; � discount rates �10%; � long lifetime (�25 years); � solar radiation �1700 kWh/m2;

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Table 6 Sensitivity analysis

Scenario

Scenario 1: Variation of system purchase price Power of plant 50 50 50 50 50 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 69711 69711 69711 69711 69711 electricity (MWh) Discount rate (%) 10 10 10 10 10 Lifetime (years) 30 30 30 30 30 Electricity sale 0.073 0.073 0.073 0.073 0.073 price ( /kWh) System purchase 440 550 660 770 880 price ( /kW) Results Capital cost 29.84 37.29 40.69 47.47 54.25 (million ) Operating and 1.012 1.012 1.012 1.012 1.012 maintenance cost (million ) Electricity 0.060 0.071 0.076 0.087 0.097 generation cost ( /kWr) Net present value 8.84 1.38 �2.01 �8.79 �15.57 (million ) Scenario 2: Variation of discount rate Power of plant 50 50 50 50 50 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 69711 69711 69711 69711 69711 electricity (MWh) Discount rate (%) 8 10 12 14 16 Lifetime (years) 30 30 30 30 30 Electricity sale 0.073 0.073 0.073 0.073 0.073 price ( /kWh) System purchase 550 550 550 660 770 price ( /kW) Results Capital cost 37.29 37.29 37.29 37.29 37.29 (million ) Operating and 1.012 1.012 1.012 1.012 1.012 maintenance cost (million ) Electricity 0.062 0.071 0.081 0.091 0.101 generation cost ( /kWr) Net present value 8.89 1.38 �4.24 �8.57 �11.95 (million )

(continued on next page)

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Table 6 (continued)

Scenario

Scenario 3: Variation of lifetime Power of plant 50 50 50 50 50 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 69711 69711 69711 69711 69711 electricity (MWh) Discount rate (%) 10 10 10 10 10 Lifetime (years) 24 30 36 42 48 Electricity sale 0.073 0.073 0.073 0.073 0.073 price ( /kWh) System purchase 550 550 550 550 550 price ( /kW) Results Capital cost 37.29 37.29 37.29 37.29 37.29 (million ) Operating and 1.012 1.012 1.012 1.012 1.012 maintenance cost (million ) Electricity 0.074 0.071 0.070 0.069 0.069 generation cost ( /kWr) Net present value �0.434 1.380 2.404 2.982 3.309 (million ) Scenario 4: Variation of annual solar radiation Power of plant 50 50 50 50 50 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 69711 69711 69711 69711 69711 electricity (MWh) Discount rate (%) 10 10 10 10 10 Lifetime (years) 30 30 30 30 30 Electricity sale 0.073 0.073 0.073 0.073 0.073 price ( /kWh) System purchase 550 550 550 550 550 price ( /kW) Results Capital cost 37.29 37.29 37.29 37.29 37.29 (million ) Operating and 1.012 1.012 1.012 1.012 1.012 maintenance cost (million ) Electricity 0.089 0.071 0.059 0.051 0.045 generation cost ( /kWr) Net present value �8.263 1.380 11.023 20.666 30.309 (million )

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Table 6 (continued)

Scenario

Scenario 5: Variation of annual efficiency of the system Power of plant 50 50 50 50 50 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 55769 69711 83653 97595 1.12E+08 electricity (MWh) Discount rate (%) 10 10 10 10 10 Lifetime (years) 30 30 30 30 30 Electricity sale 0.073 0.073 0.073 0.073 0.073 price ( /kWh) System purchase 550 550 550 550 550 price ( /kW) Results Capital cost 37.29 37.29 37.29 37.29 37.29 (million ) Operating and 1.012 1.012 1.012 1.012 1.012 maintenance cost (million ) Electricity 0.091 0.089 0.071 0.059 0.051 generation cost ( /kWr) Net present value �8.263 1.380 11.023 20.666 30.309 (million ) Scenario 6: Variation of the electricity sale price Power of plant 50 50 50 50 50 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 69711 69711 69711 69711 69711 electricity (MWh) Discount rate (%) 10 10 10 10 10 Lifetime (years) 30 30 30 30 30 Electricity sale 0.059 0.073 0.088 0.103 0.117 price ( /kWh) System purchase 550 550 550 550 550 price ( /kW) Results Capital cost 37.29 37.29 37.29 37.29 37.29 (million ) Operating and 1.012 1.012 1.012 1.012 1.012 maintenance cost (million ) Electricity 0.071 0.071 0.071 0.071 0.071 generation cost ( /kWr) Net present value �8.263 1.380 11.023 20.666 30.309 (million )

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Table 6 (continued)

Scenario

Scenario 7: Variation of the plant size Power of plant 40 50 60 70 80 (MW) Annual solar 1728 1728 1728 1728 1728 radiation (kWh/m2) Annual generated 55769 69711 83653 97595 11153 electricity (MWh) Discount rate (%) 10 10 10 10 12 Lifetime (years) 30 30 30 30 30 Electricity sale 0.073 0.073 0.073 0.073 0.073 price ( /kWh) System purchase 550 550 550 550 550 price ( /kW) Results Capital cost 29.84 37.29 44.75 52.21 59.67 (million ) Operating and 0.810 1.011 1.213 1.416 1.618 maintenance cost (million ) Electricity 0.071 0.071 0.071 0.071 0.071 generation cost ( /kWr) Net present value 1.121 1.401 1.681 1.961 2.242 (million )

� annual generated electricity � 69.711 MWh; � electricity sale price �0.073 /kWh.

When the annual rate production of SD systems is low, the establishment of a SD solar power plant is worthwhile on many islands of Greece, which high cost of conventional electricity generation (0.18–0.29 /kWh). The installation of a solar power plant in Crete is worthwhile only for high production rate of systems. The hybrid solar/fossil-fuel operation makes the system competitive with conventional fossil-fueled power plants in cost terms.

If externalities are included in cost estimation, the cost of electricity will be almost the same for both conventional and solar power generation. Therefore, if external costs are reflected in taxes, the SD system will be commercial.

In long-term period, solar thermal power stations based on a SD can become a competitive option on the electricity market, if a concerted programme capable of building the forces of industry, finance, insurance and other decision makers will support the market extension of this promising technology.

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Acknowledgments

The authors would like to acknowledge DOE/NREL and credit Stirling Energy Systems, as well as McDonnell Douglas (currently Boeing) for the figures.

References

[1] Centre for Renewable Energy Sources. Integrated resources planning for the island of Crete, SAVE project XVII/4.1031/Z/95-063. Centre for Renewable Energy Sources, 1999.

[2] Norton B, Eames P, Lo SNG. Full-energy-chain analysis of greenhouse gas emissions for solar thermal electric power generation systems. Renewable Energy 1998;15:131–6.

[3] Klaiss H, Kohne R, Nitsch J, Sprengel U. Solar thermal power plants for solar countries — tech- nology, economics and market potential. Appl Energy 1995;52:165–83.

[4] Marketaki K, Gekas V. Use of the thermodymamic cycle Stirling for electricity production. In: Proceedings of the 6th Panhellenic Symposium of Soft Energy Sources, 1999, p. 283–90

[5] http://solstice.crest.org/renewables/dish-stirling/ [6] Kotsaki E. Electricity production using solar thermal power systems — the THESEUS project. In:

Proceedings of the 6th Panhellenic Symposium of Soft Energy Sources, 1999, p. 267–74. [7] Trieb F, Langniss O, Klaiss H. Solar electricity generation — a comparative view of technologies,

costs and environmental impact. Solar Energy 1997;59(1/2):89–99. [8] http://www.stirlingenergy.com/Pages/marketdev.html. [9] Stone KW, Douglas MCD. Stirling energy systems (SES), Dish-Stirling Program. In: Proceedings

of 32nd Intersociety Conversion Engineering Conference, 1997, p. 1039–44. [10] De Graaf PJ. Multicylinder free-piston Stirling engine for application in Stirling —electric drive

systems. In: Proceedings of the 26th Intersociety Energy Conversion Engineering Conference — IECEC ‘ 91. Boston, MA, USA, 1991, v5, p. 205–10.

[11] Hargreaves CM. The Philips Stirling engine. Amsterdam: Elsevier Science, 1991. [12] http://www.energylan.sandia.gov/sunlab/pages/dishreceiv.htm [13] Johansson T, Kelly H, Reddy A, Williams R, editors. Renewable energy: sources for fuels and

electricity. Washington, DC: Island Press; 1993. [14] Gekas V, Marketaki K, Tsoutsos T. Solar Stirling thermal power generation, technical and economi-

cal evaluation for the island of Crete. Energy 2002; (in press). [15] Lopez CW, Stone KW. Design and performance of the southern California Edison Stirling dish. In:

Proceedings of the 1992 ASME–ISES–KSES International Solar Energy Conference, Maui HI, 1992, p. 945–52.

  • Technical and economical evaluation of solar thermal power generation
    • Introduction
    • Solar Stirling engines
      • Solar thermal electric technology
      • Solar Stirling engines
      • The Stirling engine and the environment
      • Description of the SD solar electric generating system
    • Characteristics of the solar power plant
    • Cost estimation
    • Discussion and conclusions
    • Acknowledgments
    • References