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Fuel Cells in Energy Technology
(9)
Werner Schindler
Department of Physics – Nonequilibrium Chemical Physics
TU München
summer term 2013
- Source
- Distribution
- CO poisoning
- Emissions
(true zero, CO2)
Focus on
- Hydrogen
- Methanol
(liquid, high energy
density)
2
Hydrogen Production
Industrial production of hydrogen
- from natural gas by steam reforming
- from methane decomposition
- from oxidation of hydrocarbons (oil)
- from coal
- from methanol by steam reforming
- as a side product of chemical syntheses
- from biomass
- from water by electrolysis
Water electrolysis is one of the techniques with highest
energy demand.
(Partial) Oxidation of hydrocarbons is exothermic.
5
Source and distribution
available for natural gas, but reforming required to achieve a H2 rich fuel
10
Some background reading on fuel reforming
J. Larmine, A. Dicks:
Fuel cell systems explained, ch. 8, pp. 229
John Wiley & Sons, 2nd Ed. 2003
ISBN-13: 978-0387344447
Photographs of the book covers from www.amazon.de
R. O'Hayre, W. Colella, Suk-Won Cha, F.B. Prinz:
Fuel Cell Fundamentals, ch. 11, pp. 371
John Wiley & Sons, 2nd Ed., 2009
ISBN-13: 978-0470258439
M. Kaltschmidt, H. Hartmann, H. Hofbauer:
Energie aus Biomasse
Springer, 2nd Ed., 2009
ISBN-13: 978-3540850946
11
Despite
- increasing energy demand (China, India, etc.)
- definitely decreasing resources
- and as a result definitely increasing prices
12
Hydrogen production from hydrocarbons
- Remove impurities from the (natural) supply
- Utilize efficient processes (choose appropriate fuel supply)
- Maximize hydrogen output
- Remove CO and CO2 from the output
13
Principal chemical reactions
Reactions with water / hydrogen:
CnHm + n H2O → n CO + (n+m/2) H2 DH > 0 (steam reforming)
CO + H2O → CO2 + H2 DH = -38 kJ / mol (water-gas shift)
CO + 3 H2 → CH4 + H2O DH = -206 kJ / mol (methanization)
Oxidations:
CnHm + (n+m/4) O2 → n CO2 + m/2 H2O DH << 0 (complete combustion)
CnHm + n/2 O2 → n CO + m/2 H2 DH < 0 (partial combustion)
CO + ½ O2 → CO2 DH = -286 kJ / mol (CO oxidation)
Carbon formation:
2 CO → C + CO2
CnHm → n C + m/2 H2
CnHm → Olefines → Polymers → Coke (thermal cracking, pyrolysis)
Depending on reaction educts and operation conditions the following processes for
hydrogen production are distinguished:
Steam-Reforming: CnHm + n H2O → n CO + (n+m/2) H2 DH > 0 (endotherm)
Partial Oxidation: CnHm + n/2 O2 → n CO + m/2 H2 DH < 0 (without steam, exotherm)
CnHm + n/2 O2 → n CO + m/2 H2 DH < 0 (with steam, autotherm)
CnHm + n H2O → n CO + (n+m/2) H2 DH > 0 14
Hydrogen production via fuel reforming -
overview
• Steam reforming (SR)
• Partial oxidation (POX) reforming
• Autothermal reforming (AR)
• Gasification
• Anaerobic digestion (AD)
15
1. Catalytic Steam Reforming
using light hydrocarbons which vaporize completely without formation of carbon
Required for protection of
catalysts in the reformer
(basically metal oxide sorbents like ZnO
which remove H2S to a few ppm
due to sulphurization)
Ni based catalyst
CnHm + n H2O → n CO + (n + m/2) H2
CO + H2O → CO2 + H2
CO + 3 H2 → CH4 + H2O
n=1, m=4: methane
strongly endothermic –
energy supplied from combustion
process of gas or oil 16
Steam reforming of methane
Source: J. Larminie, A. Dicks: Fuel cell systems explained, 2nd ed., Wiley, 2003
Equilibrium concentrations of steam
reformation reactant gases as a
function of temperature at 1 bar and a
fixed steam to carbon ratio
CH4 + H2O → CO + 3H2 DH = 206 kJ/mol CO + H2O → CO2 + H2 DH = -41 kJ/mol Catalysts:
• Ni or noble metals (reforming)
• Water gas shift at T > 400 °C
(HTS): Fe3O4/Cr2O3 catalyst
• Water gas shift at T < 270 °C
(LTS): Cu/ZnO catalyst
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Methanol is a promising candidate to substitute fossil hydrocarbons
Reverse methanol synthesis reaction:
CH3OH → CO + 2H2 ∆H = 91.7 kJ / mol
(endothermic > 700 °C without catalyst, at 300 - 450 °C with CuNi or ZnCr alloy catalysts)
Watergas shift reaction
CO + H2O → CO2 + H2 ∆H = -41.0 kJ / mol
Steam reforming
CH3OH + H2O → CO2 + 3H2 ∆H = 50.7 kJ / mol
• Catalysts CuO-ZnO or CuO-Cr2O3
• Molar ratio of water to methanol between 0.67 and 1.5
• Excess steam lowers carbon formation
• 1.5 m3 H2 per kg methanol
• Up to 2000 m3/h
Methanol steam reforming
18
Methanol oxidation complicated pathway
-> reform and use hydrogen
A commercial fuel cell running on methanol
Source: http://www.ultracellpower.com/sp.php?rmfc (May 17, 2009)
Reformed methanol fuel cell (RMFC)
19
A conceptual micro-scale methanol fuel
processor
Source: J. Larminie, A. Dicks: Fuel
cell systems explained, 2nd ed.,
Wiley, 2003
20
Catalytic steam reforming in the Haldor
Topsoe heat exchange reformer
Source: J. Larminie, A. Dicks: Fuel cell
systems explained, 2nd ed., Wiley, 2003
Haldor Topsoe is a Danish
catalyst company.
http://www.topsoe.com/
ca. 675°C
ca. 830°C
Designed for PAFC systems.
Heat for the reforming reaction is
provided by the combustion of lean
anode exhaust gas.
21
Two examples of external reformers
Source: R. O'Hayre et al.: Fuel cell fundamentals. 2nd ed., Wiley, 2009
Honda Home Energy Station
ca. 2 m3 H2 per hour from methane
Pacific Northwest National Laboratory
microfuel processor
22
2. Partial oxidation hydrocarbons
The complete combustion of propane does not yield hydrogen:
C3H8 + 5 O2 3 CO2 + 4 H2O
In a partial oxidation a hydrocarbon is oxidized with less than the stoichiometric amount
of oxygen (incomplete combustion):
Propane C3H8 + 3/2 O2 3 CO + 4 H2
General hydrocarbon CxHy + 3/2 O2 x CO +y/2 H2
Source: R. O'Hayre et al.: Fuel cell fundamentals. 2nd ed., Wiley, 2009 23
3. Autothermal reforming is a combination
of steam reforming and partial oxidation
Endothermic steam reforming including water gas shift reaction:
CH4 + 2 H2O(l) CO2 + 4 H2 DH = +253.4 kJ/mol
Exothermic partial oxidation:
CH4 + 1/2 O2 CO + H2 DH = -35.7 kJ/mol
The stoichiometry of the sum reaction can be adjusted to give a reaction
with zero reaction enthalpy:
CH4 + 1.115 H2O(l) + 0.44 O2 CO2 + 3.11 H2 DH = 0 kJ/mol
(Assumption: reactants and products enter reactor at 298 K and 1 bar)
For a detailed discussion see:
R. O'Hayre et al.: Fuel cell fundamentals. 2nd ed., Wiley, 2009, pp.379 24
Reforming
Hotspot Fuel Processor
• based on methanol
• produces 6000 l H2 per hour
• can supply1 kW fuel cell
• achieves 20 s after start-up 75% production
General Motors Truck
with gasoline reformer (arrow)
25
Summary on steam reforming, partial
oxidation and autothermal reforming
Source: R. O'Hayre et al.: Fuel cell fundamentals. 2nd ed., Wiley, 2009 26
27
A comparison of steam reforming, partial
oxidation and autothermal reforming
Source: R. O'Hayre et al.:
Fuel cell fundamentals. 2nd
ed., Wiley, 2009
27
C + H2O → CO + H2 H = 131.4 kJ/mol
Heat for this endothermic reaction is supplied by the direct combustion of a portion of the
coal.
Ash content, composition, agglomeration, sulphur content make it a complicated process
4. Coal gasification
Source: K. Kordesch, G. Simader: Fuel cells and their applications, VCH, Weinheim, 1996 28
5. Production of biogas from manure
Source: R. A. Zahoransky: Energietechnik, Vieweg/Teubner, 2009 30
Yield of biogas from digestion of biomass
Data from: R. A. Zahoransky: Energietechnik, Vieweg/Teubner, 2009
Digestion temperature 30 °C
FM: fresh mass
31
Most gasifiers produce hydrocarbons
(primarily CH4)
Initial reaction step reforms these
into CO and H2:
CH4 + H2O → CO + 3 H2 ∆H = 206.3 kJ/mol
Adjustment of CO to H2 ratio via the water-gas
shift reaction:
CO + H2O → CO2 + H2 ∆H = -41.2 kJ/mol
After this point different paths for methanol and
hydrogen production
Hydrogen and methanol from solid
biomass
Source: K. Kordesch, G. Simader: Fuel cells and their applications, VCH, Weinheim, 1996 33
Fuel cell operation temperature
may be less important when a
reforming process is considered
in a complete system! 34
35
SOFC – advantages of internal reforming of natural gas:
- Cost efficiency, minimization of components in SOFC systems;
- Increase of efficiency;
- Heat consumption by endothermic steam reforming process
lowers the necessity for air cooling of the stack;
- Faster load response.
SOFC – disadvantages of internal reforming of natural gas:
- Carbon formation in the anode chamber;
- Changes in the temperature distribution in the stack, and
large temperature gradients due to the gas flow.