eduardo zarza basic concepts
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basic conceptsTRANSCRIPT
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 1
Eduardo ZarzaCIEMAT-Plataforma Solar de Almera,
Apartado 22, Tabernas, E-04200 AlmeraPhone: 950387931 E-mail: [email protected]
Basic principles of solar radiation and STE plants
3rd SFERA Summer School
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 2
) Solar Concentrating Systems) Solar Thermal Electricity (STE) Plants
) The Sun and the solar radiationndice de la Presentacin
) STE technologies comparison
Basic principles of Solar Radiation and STE Plants
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 3
) Solar Concentrating Systems) Solar Thermal Electricity (STE) Plants
) The Sun and the solar radiationndice de la Presentacin
) STE technologies comparison
Basic principles of Solar Radiation and STE Plants
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 4
The Sun and the Solar radiation
Sun is a huge nuclear reactor (7x105
km radius)
emitting a great amount of radiant energy (3,8x1023
kW, 5800K), which can be easily converted into thermal energy
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 5
Spectral Solar Irradiance
0,0 0,5 1,0 1,5 2,0 2,50
250
500
750
1000
1250
1500
1750
2000
2250
Extraterrestrial solar radiation
Wave length (m)
S
p
e
c
t
r
a
l
s
o
l
a
r
i
r
r
a
d
i
a
n
c
e
(
W
/
m
2
m
)
Solar radiation at ground level(Air Mass = 1.5)
LE
L
L/LE = 1.5
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 6
The Sun and the Solar radiation
The Earth intercepts only 1,7x1014
kW of solar radiation (10 days
known fossil fuels resources)
The solar irradiance outside the atmosphere is almost constant (its value is called Solar Constant, 1367 W/m2)
Solar radiation at ground level has two components: Direct Radiation and Difuse Radiation.
Sun is a huge nuclear reactor (7x105
km radius)
emitting a great amount of radiant energy (3,8x1023
kW, 5800K), which can be easily converted into thermal energy
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 7
Direct and Difuse Solar RadiationDi
rect
Radia
tion
Dire
ctRa
diatio
n
Dire
ctRa
diatio
n Diffuse Radiation
Diffuse RadiationDiffuse Radiation
b) d /4 c) d > a) d < /10
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 8
The Sun and the Solar radiation
The Earth intercepts only 1,7x1014
kW of solar radiation (10 days
known fossil fuels resources)
The solar irradiance outside the atmosphere is almost constant (its value is called Solar Constant, 1367 W/m2)
Solar radiation at ground level has two components: Direct Radiation and Difuse Radiation.
Only Direct Solar Radiation can be concentrated.
Solar radiation reaching any point is not composed of a single ray, but of a cone of rays within a solid angle of 32
(approx.).
Sun is a huge nuclear reactor (7x105
km radius)
emitting a great amount of radiant energy (3,8x1023
kW, 5800K), which can be easily converted into thermal energy
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 9
The Sun and the Solar radiation
= inicidence angle
= Reflection angle
=
Reflecting surface
32
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 10
) Solar Concentrating Systems) Centrales Termosolares y Crecimiento Sostenible
) The Sun and the solar radiation
) Situacin actual ) Conclusiones
ndice de la Presentacin
Introduccin a los SistemasSolaresTrmicos deConcentracin
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 11
Solar Radiation and its Concentration Solar Concentration: Why?
Since solar radiation suffers a significant attenuation in its way to the Earth (from 63,2 MW/m2 to 1 kW/m2) we have to concentrate solar radiation in order to compensate for its low flux density at the Earth surface and thus achieve higher temperatures and efficiencies.
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 12
Dependence of the Efficiency and the Optimum Working Temperature on the Solar Radiation Concentration Factor
= f(C, T)
Efficiency versus concentration factor
0
0.25
0.5
0.75
1
0 1000 2000 3000 4000
Temperatura (K)
1.000
5.000
10.000
20.000
Carnot
C=250
0
0.25
0.5
0.75
1
0 1000 2000 3000 4000
Temperature (K)
S
y
s
t
e
m
E
f
f
i
c
i
e
n
c
y
1.000
5.000
10.000
20.000
Carnot
C=250
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 13
Solar Radiation and its Concentration
Solar Concentration: Why?Since solar radiation suffers a significant attenuation in its way to the Earth (from 63,2 MW/m2 to 1 kW/m2) we have to concentrate solar radiation in order to compensate for its low flux density at the Earth surface and thus achieve higher temperatures and efficiencies.
Ways to concentrate the direct solar radiationa) by Reflection
b) by Refraction
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 14
Direct radiation
Reflecting surface
Receiver
Direct radiation
a) by Reflection
Direct Solar Radiation can be concentrated by Reflection and by Refraction:
Receiver
Direct radiation
b) by Refraction
Fresnel lens
Solar Radiation and its Concentration
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 15
Solar Radiation and its Concentration
Limiting factors for solar concentration
Theoretical and practical limits for solar concentration Point focus concentrators: 46200 (theoretical); 5000 y 10000 (practical) Linear focus concentrators: 220, (theoretical); 20
80 (practical)
a) The apparent size of solar sphere is 32as seen from the Earthb) Inaccuracies and optical errors of solar concentrators
Solar Concentration: Why?Since solar radiation suffers a significant attenuation in its way to the Earth (from 63,2 MW/m2 to 1 kW/m2) we have to concentrate solar radiation in order to compensate for its low flux density at the Earth surface and thus achieve higher temperatures and efficiencies.
Ways to concentrate the direct solar radiationa) by Reflection
b) by Refraction
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 16
32
Actual shape
Theoretical shape
Concentration limit due to the Sun disk size
Concentration
= L/ddL
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 17
) Solar Concentrating Systems) Solar Thermal Electricity Plants
) The Sun and the solar radiation
) Situacin actual ) Conclusiones
ndice de la Presentacin
Introduccin a los SistemasSolaresTrmicos deConcentracin
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 18
Solar Thermal Electricity PlantsWhat is a Solar Thermal Electricity (STE) plant ?A STE plant is a system where
solar radiation is concentrated and then converted intothermal energy at medium/high temperature (300C
800C). This thermal energy is then used in a thermodynamic cycle to produce electricity.
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 19
Optical Concentrator
RECEIVER
Waste Heat
Heat
Thermallosses
Opticallosses
Simplified Scheme of a typical STE PlantSimplified Scheme of a typical STE PlantDirect Solar Radiation
ConcentratedSolar Radiation
ThermalStorage
Solar System
Mechanical energy
G Electricity generator
ThermodynamicCycle
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 20
What is a Solar Thermal Electricity (STE) plant ?
9 There is a huge market worldwide for these solar plants
9 These plants do not increase the emissions of CO2 :
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Every GWh
of electricity produced by a STP plant saves 800 tons of CO2
9 There are many Countries with good solar radiation level
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A STP plant saves 2000 Tons of CO2
per year and MWe
installed
Why are Solar Thermal Power plants interesting nowadays ?
9 These plants demand a lot of manpower for construction, as well as for O&M
9 It is already profitable in some Countries due to public subsidies or incentives
9 The technology is mature enough for commercial deployment
A STE plant is a system where
solar radiation is concentrated and then converted intothermal energy at medium/high temperature (300C
800C). This thermal energy is then used in a thermodynamic cycle to produce electricity.
Solar Thermal Electricity Plants
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 21
100 mHeliostat field
Receiver
Power Conversion System
Tower
Current Technologies for STE plants (I)Central Receiver Technology
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 22
Receiver Tube
Parabolic trough concentratorStructure
Current Technologies for STE plants (II)Parabolic Trough Collectors
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 23
Solar field
Power Conversion System
STE Plant with Parabolic Trough Collectors
Current Technologies for STE plants (II)
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 24
ConcentratorReceiver
Structure
Stirling DishesCurrent Technologies for STE plants (III)
Solar Stirling engine
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 25
Receiver pipe
Rectangular reflectors
Linear Fresnel ConcentratorCurrent Technologies for STE plants (and IV)
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 26
Technologies comparison
PTC CentralReceiver
ParabolicDishes
LFC
Unit plant powerWorking temperaturePeak efficiency (solar-electric) Yearly net Efficiency
15-200 MW390 C20 %
11-16 %
15-100 MW575 C23 %
7-20 %
9-25 kW750 C30 %
12-25 %
15-200 MW390C
1813
Current status
Technological riskStorage availabilityHybrid designs
Available
LowSiSi
Available
LowSiSi
Prototypes-Demonstration
LowSiSi
Available
High-MediumSiSi
Solar Thermal Electricity Plants
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Almera (Spain), June 27-28 , 20123rd SFERA Summer School 27
End of Slide Show
! Thank you for your attention
Basic principles of solar radiation and STE plants
3rd SFERA Summer School
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