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Solar Facilities for the European Research Area
Introduction to solar reactors
Gilles Flamant, CNRS-PROMES
SFERA II 2014-2017, Summer School, June 25-27 2014
CONTENT
Solar reactors for what?
Typology of solar reactors
Example of laboratory to pilot scale prototypes
Metrics for solar reactors
Modeling
SFERA II Summer School 2014 – Gilles Flamant
FOR WHAT?
1
To use solar heat for performing chemical reactions
Solar Heat → Chemical products
Renewable fuel production (solar fuels)
Chemical commodity production
Waste treatment
SFERA II Summer School 2014 – Gilles Flamant
Gases:
Hydrogen H2, Methane CH4 , Carbon monoxide CO and Syngas (mixture of H2 and CO)
Liquids:
Methanol CH3OH, Synthetic Hydrocarbons
-CH2-
Solid:
Metal produced by solar thermal reduction
SOLAR FUELS
SFERA II Summer School 2014 – Gilles Flamant
FOR WHAT?
SOLAR FUELS
SFERA II Summer School 2014 – Gilles Flamant
FOR WHAT?
To save fossil fuels consumption and CO2 emission:
Classical route: C + O2 = CO2 ∆H°r = -393 kJ/mol
The heat of combustion is the process heat for chemical reactions
To store solar energy for a long time without losses
To use solar energy in the transportation sector
SFERA II Summer School 2014 – Gilles Flamant
Solar Fuels
Water Splitting
Direct thermolysis Thermochemical cycles
H20
Cracking
Methane Splitting
CH4 H20
Steam reaction
Reforming Gasification
Fossil fuel Biomass
Concentrated solar energy
Solar Fuels: Hydrogen and
Syngas
C and CO2
SFERA II Summer School 2014 – Gilles Flamant
Solar Fuels
Thermal splitting
Water: H2O H2 + ½ O2 H° = 285.8 kJ/mol
Carbon Dioxide: CO2 CO + ½ O2 H° = 283 kJ/mol
Methane: CH4 2H2 + C H° = 74.6 kJ/mol
Four times less energy to split methane by comparison with water
Chemical routes
SFERA II Summer School 2014 – Gilles Flamant
Solar Fuels
Chemical routes Reforming and gasification with Steam and carbon
dioxide
Steam Methane Reforming (SMR) CH4 + H2O 3H2 + CO H° = 206 kJ/mole Water Gas Shift reaction (WGS) CO + H2O H2 + CO2 H° = - 42 kJ/mole Carbon dioxide Methane Reforming CH4 + CO2 2H2 + 2CO H° = 247 kJ/mole Coal steam gasification C + H2O H2 + CO H° = 131.3 kJ/mol Syngas to gasoline n(2H2 +CO) (-CH2-)n + nH2O H° = -165 kJ/mol
SFERA II Summer School 2014 – Gilles Flamant
Solar Fuels
Chemical routes ∆G° = ∆H° - T∆S°
∆G° = 0 at Tinv = ∆H° / ∆S°
SFERA II Summer School 2014 – Gilles Flamant
Solar Fuels
Chemical routes for Tinv reduction: Oxide-based thermochemical cycles
HT Solar Step -reduction, endothermal- : MxOy MxOy-1+ ½ O2 (1400°C-1800°C) LT step -oxidation, exothermal- : MxOy-1 + H2O/CO2 MxOy + H2/CO (400°C-1200°C) 2 families: Volatile oxides: ZnO/Zn, SnO2/SnO Non volatile oxides: MFe2O4, CeO2 ….
SFERA II Summer School 2014 – Gilles Flamant
Typology of solar
reactors
TYPOLOGY
Configuration 1: Use of an intermediate heat transfer fluid
Transfer of solar heat to the chemical reactor using a heat transfer fluid (HTF). At high temperature: molten salt (T < 600°C), molten metals, air and other gases. Main advantage: allow to use classical solution for the chemical reactor. Main drawback: heat losses in heat exchangers
SFERA II Summer School 2014 – Gilles Flamant
Configuration 2: Receiver-Reactor type
Receiver = reactor, no HTF Main advantage: allow to operate at high temperatures Main drawback: process control is complex
SFERA II Summer School 2014 – Gilles Flamant
TYPOLOGY
Configuration 2: Receiver-Reactor type, 2 options
Use of an opaque heat transfer wall Main advantage: allow to separate the chemical reaction and the radiation (better T control) Main drawback: limitation of heat transfer flux and wall temperature
Direct irradiation of the reactants Main advantage: allow to operate at high solar flux and temperature Main drawback: window is necessary, limitation in size and temperature
SFERA II Summer School 2014 – Gilles Flamant
TYPOLOGY
Example of laboratory
and pilot scale
prototypes
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 1
SFERA II Summer School 2014 – Gilles Flamant
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 1
CONFIGURATION 2
Heat transfer wall option
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Tubes
•7 single graphite tubes (26-18 mm)
•Graphite cavity (360x400x300 mm)
•Aperture diameter 13 cm
50 kW tube-reactor for methane cracking , CNRS Up to 2000K 5-10 kW tube-reactor for biomass
gasification, Univ of Colorado – NREL Up to 1400K
SFERA II Summer School 2014 – Gilles Flamant
10 kW rotating tube-reactor for calcite decomposition, PSI (Switzerland) Up to 1400K; SiC tubes.
5-10 kW fluid wall aerosol flow reactor for methane cracking, NREL and Univ. of Colorado. Graphite wall, up to 2000K
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Tubes
CONFIGURATION 2 Heat transfer wall
50 kW 2D-fluidized bed, CNRS Up to 1200K (tested with inert particles only); Inconel.
5 kW radiant plate or 2-cavity reactor for steel dust (metal recovery) or carbonaceous wastes processing , ETH and PSI (Switzerland); SiC wall, up to 1400K
SFERA II Summer School 2014 – Gilles Flamant
Two-cavity pilot reactor
300 kW radiant plate (or 2-cavity) reactor for ZnO carbothermal reduction (Zn metal production), SOLZINC EC Project 2001-2005, CNRS,ETH and PSI (Switzerland), WIS (Israel) and Scanarc (Sweden). SiC wall, up to 1500K.
ZnO + C → Zn + CO
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Radiant wall
Beam down facility at WIS Solar reactor
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Radiant wall
Experimental results
Wieckert et al. J Solar Energy Engng, 129 (2007)
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Radiant wall
Solsyn pilot plant at Plataforma Solar de Almeria (CESA-1 tower) PSI-ETH (Switzerland)
Solsyn pilot plant in operation
up to 200 kW solar power input
into solar reactor
Gasification of carbonaceous wastes
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Radiant wall
Wieckert C. et al. Energy & Fuel (2013) 27, 4770
Syngas composition average over complete test
0%
10%
20%
30%
40%
50%
60%
70%
80%
90%
100%
Bee
ch c
harco
al
Bee
ch c
harco
al
Low ran
k co
al
Low ran
k co
al
Low ran
k co
al
Ind. S
ludge
I
Ind. S
ludge
II
Fluff I
Fluff II
Fluff II
DSS-M
DSS-M
Bag
asse
Tire
chip
s
Tire
chip
s
Tire
chip
s
C3H6 (GC)
C2H6 (GC)
C2H4 (GC)
CO2 (GC)
CO (GC)
CH4 (GC)
H2 (GC)
SFERA II Summer School 2014 – Gilles Flamant
CONFIGURATION 2 Radiant wall
CONFIGURATION 2
Direct heating option
SFERA II Summer School 2014 – Gilles Flamant
SFERA II Summer School 2014 – Gilles Flamant
Four main categories:
• Fluidized bed • Rotary kiln • Entrained-particles • Porous media
SFERA II Summer School 2014 – Gilles Flamant
Fluidized Bed
First 1 kW fluidized bed at CNRS (1977) Decarbonation of calcite, 1200K
Lab FB with draft tube. Niigata University, Japan, for coke gasification and then to split water cycles using ferrites.
SFERA II Summer School 2014 – Gilles Flamant
Rotary Kiln
Solar rotary kiln developed by CNRS in the seventies to melt, to purify and to spheroidize refractory oxides (Al2O3, ZrO2, SiO2.)
SFERA II Summer School 2014 – Gilles Flamant
Rotary Kiln
The 400 kW rotary kiln particulate receiver combined with cold and hot storages and a 100 kW multi-stage fluidized bed heat exchanger developed at CNRS in the mid-eighties. Sand up to 1200K.
SFERA II Summer School 2014 – Gilles Flamant
Rotary Kiln
quartz window
cavity-receiver
water/gas
inlets/outlets
Zn + ½ O2
ZnO
Concentrated
Solar
Radiation
ZnO feeder
quartz window
cavity-receiver
water/gas
inlets/outlets
Zn + ½ O2
ZnO
Concentrated
Solar
Radiation
ZnO feeder
Improved 10 kW rotary solar reactor for ZnO reduction developed at ETH/PSI
1 kW reduced pressure rotary kiln developed at PROMES-CNRS.
SFERA II Summer School 2014 – Gilles Flamant
Entrained particles
Vortex flow solar reactor developed at ETH/PSI for carbonaceous matter gasification
10 kW tornado solar reactor developed at WIS for methane splitting.
SFERA II Summer School 2014 – Gilles Flamant
POROUS MEDIA
Monolith honeycomb,
Ceramic foams or fibers or fins or wires
Porous monolithic ceramics
SFERA II Summer School 2014 – Gilles Flamant
Monolith honeycomb
Principle of the solar cycling of reactive honeycomb monolith for hydrogen production using 2-step thermochemical cycles based on ferrite. The ferrite material is deposited on SiSiC honeycomb and experiences successive reduction and hydrolysis cycles in the temperature ranges 1400-1700K and 1100K-1300K respectively.
SFERA II Summer School 2014 – Gilles Flamant
Monolith honeycomb
HYDROSOL-II EC project resulted in the development of a 50-100 kW pilot reactor tested at PSA-CIEMAT
SFERA II Summer School 2014 – Gilles Flamant
Counter Rotating Ring Receiver Reactor Recuperator (CR5). The reactor is composed of a stack of disks on which the redox material is deposited (the disk may also be composed of the redox material itself). Reactor developed by SANDIA Nat. Lab (USA) for CO2 or H2O splitting using 2-step redox reactions.
Porous support
SFERA II Summer School 2014 – Gilles Flamant
Ceramic foam
Porous reactor based on cerium oxide developed by the alliance ETH/PSI and CALTECH. 2kW reactor with reduction temperatures in the range 1700K-1910K and oxidation temperature of about 1100K.
500 cycles.
Solar reactor for methane reforming based on catalyst-on-foam concept developed by DLR.
SFERA II Summer School 2014 – Gilles Flamant
Ceramic fin
Pin-fins porcupine solar reactor developed at WIS (Israel)
SFERA II Summer School 2014 – Gilles Flamant
Metrics for solar reactors
SFERA II Summer School 2014 – Gilles Flamant
Efficiencies
Chemical (thermochemical) efficiency
ηch = mo,RXR∆Hr(To→Tr) / (Qsolar + Qaux) m for molar flow, R for reactant, r for reaction, XR is the conversion of R, Qsolar is the incident solar power at the entrance of reactor. For solar fuels: ηch = mfuel.LHVfuel/ (Qsolar + Qaux)
Overall reactor efficiency
ηov = ηch + ηth
With ηth = [mo,R (1-XR)∫ToTrCp,RdT + FI ∫To
TrCp,IdT] / (Qsolar + Qaux)
I for inert gas
SFERA II Summer School 2014 – Gilles Flamant
Efficiencies
For reforming and gasification
Solar-to-fuel energy conversion efficiency (Qaux = 0)
Energetic upgrade factor
For example, solar gasification of coal (C + H2O) leads to U = 1.33
SFERA II Summer School 2014 – Gilles Flamant
Example
Efficiency of the 50 kW SR for methane cracking
cracking
0
2
4
6
8
10
12
14
1698 K 1798 K 1808 K 1873 K
Thermochemical efficiency (%)
Thermal efficiency (%)
Ar=49 NL/min
CH4=21 NL/min
Ar=49 NL/min
CH4=21 NL/min
Ar=49 NL/min
CH4=21 NL/min
Ar=21 NL/min
CH4=21 NL/min solar
)Treactor(Products)T(ReactantCHCH0,
ch044
.X.m
Q
H s
solar
T
T
)Treactor(Products)(ReactantsCHCH0,CH
T
T
CHCH0,
th
..X.m.dCp).X1.(mreactor
0
0444
reactor
0
44
Q
dTCpmHT ArArT
The best thermochemical efficiency is reached for 50% of CH4 and exceeds 10%
SFERA II Summer School 2014 – Gilles Flamant
Dynamic modeling of solar reactors
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Zno decomposition in a solar reactor
Internal Energy U
Inlet Outlet
External Power Qsolar
Solid ZnO + N2
at To Reactor + Reaction at T
O2 + Zn + ZnO + N2
All gas species at T
ZnO (s) Zn (g) + ½ O2 H° = 479 kJ/mol, 2000K Zn (s) + H2O ZnO + H2 H° = -62 kJ/mol, 800K
Charvin at al. Chem. Engng Res. & Des. (2008) 86
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Mass balance
Unsteady mass balance equation for compound j (j = ZnO, Zn, O2, N2) N2 is added as sweeping and quenching gas
n = mole number F: molar flow rate y: mole fraction ν: stoichiometric coefficient
(For solid ZnO)
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Heat balance
General form: q + FinHin = FoutHout + dU/dt
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Results
Size effect
Lab-scale
Ind. scale
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Results
Chemical Threshold effect
50 MW scale
Effect of pressure
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Industrial scale 50 MW
Results
Thermal inertia effect
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Overall process optimization: from heliostats to fuels
Pitz-Paal et al. Solar Energy, 85 (2011)
Heliostat field must be associated with a CPC secondary concentrator to increase the mean concentration ratio.
Optimization procedure
Solar reactor
Heliostat field
SFERA II Summer School 2014 – Gilles Flamant
Modeling
Expected overall efficiencies: 40% for gasification and 30% for zinc oxide splitting
Overall process optimization: from heliostats to fuels
Solar Facilities for the European Research Area
Welcome in the solar thermochemistry world
SFERA II 2014-2017, Summer School, June 25-27 2014