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Fuel Cell Technology
Topics
1. A Very Brief History
2. Electrolysis
3. Fuel Cell Basics
- Electrolysis in
Reverse
- Thermodynamics
- Components
- Putting It
Together
4. Types of Fuel Cells
- Alkali
- Molten Carbonate
- Phosphoric Acid
- Proton Exchange
Membrane
- Solid Oxide
5. Benefits
6. Current Initiatives
- Automotive
Industry
- Stationary Power
Supply Units
- Residential Power
Units
7. Future
A Very Brief History
Considered a curiosity in the
1800’s. The first fuel cell was
built in 1839 by Sir William
Grove, a lawyer and gentleman
scientist. Serious interest in
the fuel cell as a practical
generator did not begin until
the 1960's, when the U.S. space
program chose fuel cells over
riskier nuclear power and more
expensive solar energy. Fuel
cells furnished power for the
Gemini and Apollo spacecraft,
and still provide electricity
and water for the space
shuttle.(1)
s this have to do with fuel cells?”
By providing
energy from a
battery, water
(H2
O) can be
dissociated into
the diatomic
molecules of
hydrogen (H2
)
and oxygen (O2
).
Figure 1
Basics
lectrolysis in reverse.”
fuel
cell
H2O
O2
H2
heat
work
The familiar process of electrolysis
requires work to proceed, if the
process is put in reverse, it should
be able to do work for us
spontaneously.
The most basic “black box”
representation of a fuel cell in
action is shown below:
Figure 2
uel Cell Basics
hermodynamics
H2(g) + ½O2(g) H2O(l)
Other gases in the fuel and air inputs
(such as N2 and CO2) may be present,
but as they are not involved in the
electrochemical reaction, they do not
need to be considered in the energy
calculations.
69.91
J/mol·K
205.14
J/mol·K
130.68
J/mol·K
Entropy
(S)
-285.83
kJ/mol
00Enthalpy
(H)
H2O (l)O2H2
1 Thermodynamic properties at 1Atm and 29
Enthalpy is defined as the energy of a
system plus the work needed to make
room for it in an environment with
constant pressure.
Entropy can be considered as the
measure of disorganization of a
uel Cell Basics
hermodynamics
f the chemical reaction using Hess’ Law:
ΔHreaction = ΣHproducts – ΣHreactants
= (1mol)(-285.83 kJ/mol) – (0)
= -285.83 kJ
py of chemical reaction:
ΣSproducts – ΣSreactants
mol)(69.91 J/mol·K)] – [(1mol)(130.68 J/mol·K) + (½mol)(2
63.34 J/K
gained by the system:
= TΔS
= (298K)(-163.34 J/K)
= -48.7 kJ
uel Cell Basics
hermodynamics
free energy is then calculated by:
ΔH – TΔS
= (-285.83 kJ) – (-48.7 kJ)
= -237 kJ
done on the reaction, assuming reversibility a
W = ΔG
one on the reaction by the environment is:
sferred to the reaction by the environment
W = ΔG = -237 kJ
ΔQ = TΔS = -48.7 kJ
More simply stated:
The chemical reaction can do 237 kJ of
work and produces 48.7 kJ of heat to
the environment.
Fuel Cell Basics
Components
Anode: Where the fuel reacts or
"oxidizes", and releases electrons.
Cathode: Where oxygen (usually from
the air) "reduction" occurs.
Electrolyte: A chemical compound that
conducts ions from one electrode
to the other inside a fuel cell.
Catalyst: A substance that causes or
speeds a chemical reaction
without itself being affected.
Cogeneration: The use of waste heat to
generate electricity. Harnessing
otherwise wasted heat boosts the
efficiency of power-generating
systems.
Reformer: A device that extracts
pure hydrogen from
l Cell Basics
tting it together.
Figure 3
Types of Fuel Cells
The five most common types:
•Alkali
•Molten Carbonate
•Phosphoric Acid
•Proton Exchange Membrane
•Solid Oxide
Types of Fuel Cells
Vorteil: Keine aufwendige Brenngas-Aufbereitung
Nachteil: Hohe Betriebstemperaturen = Hohe System-Kosten
 Starke Material-Beanspruchung
SOFC
Alkali Fuel Cell
compressed
hydrogen and
oxygen fuel
potassium
hydroxide (KOH)
electrolyte
~70% efficiency
150˚C - 200˚C
operating temp.
300W to 5kW
output
requires pure hydrogen
fuel and platinum
catylist ($$)→
liquid filled container →
corrosive leaks
Figure 4
Molten Carbonate Fuel Cell (MCFC)
carbonate salt
electrolyte
60 – 80%
efficiency
~650˚C operating
temp.
cheap nickel
electrode
catylist
up to 2 MW
constructed, up
to 100 MW designs
exist
Figure 5
The operating temperature is
too hot for many applications.
carbonate ions are consumed in
the reaction inject CO→ 2 to
compensate
hosphoric Acid Fuel Cell (PAFC)
phosphoric acid
electrolyte
40 – 80% efficiency
150˚C - 200˚C
operating temp
11 MW units have
been tested
sulphur free
gasoline can be
used as a fuel
Figure 6
The electrolyte
is very corrosive
Platinum
catalyst is very
Proton Exchange Membrane (PEM)
thin permeable
polymer sheet
electrolyte
40 – 50%
efficiency
50 – 250 kW
80˚C operating
temperature
electrolyte will not
leak or crack
temperature good for
home or vehicle use
Figure 7
Solid Oxide Fuel Cell (SOFC)
hard ceramic
oxide
electrolyte
~60% efficient
~1000˚C
operating
temperature
cells output
up to 100 kWhigh temp / catalyst can extract
the hydrogen from the fuel at the
electrode
high temp allows for power
generation using the heat, but
limits use
Figure 8
Benefits
Efficient: in theory and in practice
Portable: modular units
Reliable:few moving parts to wear out
or break
Fuel Flexible: With a fuel reformer,
fuels such as natural gas, ethanol,
methanol, propane,
gasoline, diesel, landfill
gas,wastewater, treatment
digester gas, or even ammonia can be
used
Environmental: produces heat and
water (less than combustion in both
terial‘s challenges of the PEM Fuel Cel
11/06/15 Fuel Cell Fundamentals 20
Review of Membrane
(Nafion) Properties
• Chemical Structure
• Proton Conduction
Process
• Water Transport and
Interface Reactions
PSSA
poly(sty
rene-co-
styrenes
ulfonic
acid)
(PSSA)
Nafion,TM
Membrane C
Dow
PESA
(Polyepoxy-
succinic Acid)
α,β,β-
Trifluorosty
rene grafted
onto
poly(tetrafl
uoro-
ethylene)
with post-
sulfonation)
Poly –
AMPSPoly(2-acrylamido-
2-methylpropane
sulfonate)
cal structures of some membrane mater
Nafion Membrane
Chemical Structure
Nafion Membrane
on Conduction Process
The water transport
through Nafion
Membrane
Water flux due to electroosmotic drag (mol/cm2
s) is: Nw, drag = Iξ(λ)/F.
Where: I is the cell current, ξ(λ) is the electroosmotic drag coefficient at a
given state of membrane hydration λ(=N(H2O)/N(SO3H) and F is the Faraday
constant. This flux acts to dehyddrate the anode side of a cell and to
introduce additional water at the cathode side.
The buildup of water at the cathode (including the product water
from the cathode reaction) is reduced, in turn, by diffusion back down the
resulting water concentration gradient (and by hydraulic permeation of water
in differentially pressurized cells where the cathode is held at higher overall
pressure). The fluxes (mol/cm2
s) brought about by the latter two
mechanisms within the membrane are:
Nw,diff = -D(λ)∆c/ ∆z, Nw,hyd = -khyd(λ)∆P/ ∆z
where D is the diffusion coefficient in the ionomer at water content λ, ∆c/ ∆z
is a water concentration gradient along the z-direction of membrane
thickness, khyd is the hydraulic permeability of the membrane, and ∆P/ ∆z is a
pressure gradient along z.
The water transport
through Nafion
Membrane
Many techniques have been
introduced to prevent the
dehydration of the anode
(including the introduction of
liquid water into the anode
and/or cathode, etc. – which,
however, can lead to “flooding”
problems that inhibit mass
transfer).
However, the overall question of
“water management,” including the
issue of drag as a central
component, has been solved to a
very significant extent by the
application of sufficiently thin
PFSA membranes (<100 µm thick) in
PEFCs, combined with humidification
of the anode fuel gas stream.
Water Transport (& Interface
Reactions)
in Nafion Membrane of the PEM Fuel
Cell
Material‘s challenges of the SOFC
SOFC
Solid Oxide Fuel Cell
Air side = cathode: High oxygen partial pressure
1
conductance
d
σ= µ
Fuel side= anode: H2 + H2O= low oxygen partial pressure
H2 + 1/2O2  H2O
H2
O2
H2O
SOFC
Electromotive Force (EMF)
Chemical Reactions in 2 separated compartements:
- Cathode (Oxidation):
- Anode (Reduction):
½O2 + 2e-
 O2-
H2 + O2-
 H2O + 2e-
EMF of a galvanic Cell:
(1) EMF = ∆Gr /-z F
∆G = Free Enthalpie
z = number of charge carriers
F = Faraday Constant
∆G0= Free Enthalpie in
standart state
R = Gas Constant
SOFC: ½O2 + H2  H2O
( )2
0 0.5
2 2
ln
( ) ( )
a H O
G G RT
a H a O
∆ = ∆ +(2)
difference of ∆G between anode und cathode 
( )
( )
2
2
ln
4
p ORT
EMK
F p O
=
K
A
Nernst Equation:
SOFC
Elektrochemische Potential
Oxygen ions migrate due to an electrical
and chemical gradient
2 2
( ) ( ) 2O O Fµ µ ϕ− −
∆ = ∆ − ∆%
2
( )Oµ −
∆ %
Chemical
Potential
Electrical
Potential
Electrochemichal
Potential
Driving force for the O2-
Diffusion through the electrolyte are the
different oxygen partial pressures at the anode and the cathode
side:
2
( )
2
i
ij O
F
σ
µ −
= − ∆ %
ji = ionic current
σi= ionic conductivity
SOFC
engl. Open Circuit Voltage (OCV)
2
( )
2
i
ij O
F
σ
µ −
= − ∆ %2 2
( ) ( ) 2O O Fµ µ ϕ− −
∆ = ∆ − ∆%
2
( ) 0Oµ −
∆ =%
What happems in case :
0ij =
No current
Electrical potential difference = chemical potetialOCV
SOFC
Leistungs-Verluste
Under load decrease of cell voltage
and internal losses
U(I) = OCV - I(RE+ RC+RA) - ηC - ηA
(RE+ RC+RA)
OCV
ηC
ηA
cell current I [mA/cm2
]
cellvoltageU(I)[V]
Ohmic resistances
Non ohmic resistances=
over voltages
SOFC
Überspannungen
Over voltages exist at interfaces of
• Elektrolyte - Cathode
• Elektrolyte - Anode
Reasons:
•Kinetic hindrance of the electrochemical reactions
•Bad adheasion of electrode and electrolyte
•Diffusion limitations at high current densities
SOFC
Ohm‘s losses
800nm
Kathode Anode
Reduce electrolyte thickness
Past Future
SOFC
Leistungs-Verluste
(1)Open circuit voltage (OCV), I = 0
(2)SOFC under Load  U-I curve
(3) Short circuit, Vcell = 0
0.0 0.5 1.0 1.5 2.0
0.0
0.2
0.4
0.6
0.8
1.0
900°C
in Luft/Wasserstoff
Stromdichte [A/cm
2
]
Zellspannung[V]
0.0
0.1
0.2
0.3
0.4
0.5
Leistung[W/cm
2
]
(1)
(2)
(3)
(RE+ RC+RA)
OCV
ηC
ηA
cell current I [mA/cm2]
cellvoltageU(I)[V]
(RE+ RC+RA)
OCV
ηC
ηA
cell current I [mA/cm2]
cellvoltageU(I)[V]
1
2
3
SOFC
( )
*
U L
R f T
I A σ
∆
= = =
0
log( )aE
T kT
σ
σ = −
1
. aT vs E
T
σ ⇒
Electrical resistance:
Electrical conductivity: U : voltage [V]
I : current [A]
R : resistivity [ohm]
∆L : distance between both
inner wires [cm]
A : sample surface [cm2]
σ : conductivity [S/m]
Ea : activation energy [eV]
T : temperature [K]
K : Boltzmann constant
How to determine the electrical conductance
IinputUmeasured
SOFC
SOFC-Designs
SOFC
Tubular design
i.e. Siemens-Westinghouse design
Planar design
i.e. Sulzer Hexis, BMW design
Segment-type tubular design
SOFC Design
SOFC
Tubular Design – Siemens-Westinghouse
air flow anode (fuel)
cathode
interconnection
cathode
(air)
Why was tubular design
developed in 1960s by
Westinghouse?
• Planar cell: Thermal
expansion mismatch
between ceramic and
support structures leads to
problems with the gas
sealing  tubular design
was invented
Advantages of tubular
design:
• At cell plenum: depleted air
and fuel react  heat is
generated  incoming
oxidant can be pre-heated.
• No leak-free gas
manifolding needed in this
SOFC
anode (fuel)
cathode
(air)
electrolyte
Tubular Design – Siemens-Westinghouse
To overcome problems new
Siemens-Westinghouse „HPD-
SOFC“ design:
New: Flat cathode tube with
ligaments
Advantages of HPD-SOFC:
• Ligaments within cathode  short
current pathways  decrease of
ohmic resistance
• High packaging density of cells
compared to tubular designSiemens-Westinghouse shifted from
basic technology to cost reduction and
scale up.
Power output: Some 100 kW can be
produced.
SOFC
Planar Design – Sulzer Hexis
anode (fuel)
electrolyte
cathode (air)
interconnect Advantages of planar
design:
• Planer cell design of bipolar
plates  easy stacking  no
long current pathways
• Low-cost fabrication
methods, i.e. Screen printing
and tape casting can be
used.
Drawback of tubular
design:
• Life time of the cells 3000-
7000h  needs to be
improved by optimization of
mechanical and
electrochemical stability of
used materials.
SOFC
Planar Design – BMW
electrolyte
anode
porous metallic substrate
Fe-26Cr-(Mo, Ti, Mn, Y2O3) alloy
cathode
Cathode current collector
bipolar plate
bipolar plate
Air channel
Fuel channel
20-50 µm
5-20 µm
15-50 µm
Plasma spray
Plasma spray
Plasma spray
Application
Batterie replacement in the
BMW cars of the 7-series.
Power output: 135 kW is
aimed.
Current Initiatives
Automotive Industry
Most of the major auto manufacturers have
fuel cell vehicle (FCV) projects currently
under way, which involve all sorts of fuel
cells and hybrid combinations of
conventional combustion, fuel reformers and
battery power.
Considered to be the first gasoline powered
fuel cell vehicle is the H20 by GM:
GMC S-10 (2001)
fuel cell battery hybr
low sulfur gasoline fue
25 kW PEM
40 mpg
112 km/h top speed
Figure 9
Fords Adavanced
Focus FCV (2002)
fuel cell battery
hybrid
85 kW PEM
~50 mpg
(equivalent)
4 kg of
compressed H2 @
5000 psi
Approximately 40
fleet vehicles
are planned as a
market
introduction for
Germany,
Vancouver and
California for
Current Initiatives
Automotive Industry
Figure 10
Figure 11
Chrysler NECAR 5 (introduced in 2000)
85 kW PEM
fuel cell
methanol fuel
reformer
required
150 km/h top
speed
this model completed a California to Washing
permit for Japanese roads
Current Initiatives
Automotive Industry
Figure 12
Mitsubishi Grandis FCV minivan
fuel cell /
battery
hybrid
68 kW PEM
compressed
hydrogen
fuel
140 km/h top
speed
Plans are to launch as a
production vehicle for Europe in
2004.
Current Initiatives
Automotive Industry
Figure 13
Current Initiatives
Stationary Power Supply Units
A fuel cell installed at McDonald’s
restaurant, Long Island Power
Authority to install 45 more fuel
More than 2500 stationary fuel cell
systems have been installed all over
the world - in hospitals, nursing homes,
hotels, office buildings, schools,
utility power plants, and an airport
terminal, providing primary power or
backup. In large-scale building
systems, fuel cells can reduce
facility energy service costs by 20%
to 40% over conventional energy
service.
Figure 14
Current Initiatives
Residential Power Units
There are few residential fuel cell
power units on the market but many
designs are undergoing testing and
should be available within the next
few years. The major technical
difficulty in producing residential fuel
cells is that they must be safe to
install in a home, and be easily
maintained by the average homeowner.
Residential
fuel cells
are typically
the size of a
large deep
freezer or
furnace, such
as the Plug
Power 7000
unit shown
here, and cost
$5000 - $10
000.
If a power company was to install a
residential fuel cell power unit in a
home, it would have to charge the
homeowner at least 40 ¢/kWh to be
Figure 15
Future
“...projections made by car companies
themselves and energy and automotive
experts concur that around 2010, and
perhaps earlier, car manufacturers
will have mass production capabilities
for fuel cell vehicles, signifying the
time they would be economically
available to the average consumer.”
Auto Companies on Fuel Cells, Brian Walsh and Peter
Moores, posted on www.fuelcells.org
Technical and engineering innovations
are continually lowering the capital
cost of a fuel cell unit as well as
the operating costs, but it is expected
that mass production will be of the
greatest impact to affordability.
A commercially available fuel cell
power plant would cost about
$3000/kW, but would have to drop
below $1500/kW to achieve widespread
market penetration.
http://www.fuelcells.org/fcfaqs.htm
Future
internal
combustion
obsolete?
solve pollution
problems?
common in homes?
better designs?
higher
efficiencies?
cheaper
electricity?
reduced
petroleum
dependency?
References
(1) FAQ section, fuelcells.org
(2) Long Island Power Authority press release: Plug Power
Fuel Cell Installed at McDonald’s Restaurant, LIPA to
Install 45 More Fuel Cells Across Long Island, Including Homes,
http://www.lipower.org/newscenter/pr/2003/feb26.fuelce
ll.html
(3) Proceedings of the 2000 DOE Hydrogen Program Review:
Analysis of Residential Fuel Cell Systems & PNGV
Fuel Cell Vehicles,
http://www.eere.energy.gov/hydrogenandfuelcells/pdfs/2
8890mm.pdf
Figures
1, 3 http://hyperphysics.phy-
astr.gsu.edu/hbase/thermo/electrol.html
4 – 8 http://fuelcells.si.edu/basics.htm
10
http://www.moteurnature.com/zvisu/2003/focus_fcv/focus
_fcv.jpg
11
http://www.granitestatecleancities.org/images/Hydrogen_F
uel_Cell_Engine.jpg
12
http://www.in.gr/auto/parousiaseis/foto_big/Necar07_2883.
jpg
13
http://www3.caradisiac.com/media/images/le_mag/mag138/o
eil_mitsubishi_grandis_big.jpg
14
http://www.lipower.org/newscenter/pr/2003/feb26.fuelce

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Fuelcell

  • 2. Topics 1. A Very Brief History 2. Electrolysis 3. Fuel Cell Basics - Electrolysis in Reverse - Thermodynamics - Components - Putting It Together 4. Types of Fuel Cells - Alkali - Molten Carbonate - Phosphoric Acid - Proton Exchange Membrane - Solid Oxide 5. Benefits 6. Current Initiatives - Automotive Industry - Stationary Power Supply Units - Residential Power Units 7. Future
  • 3. A Very Brief History Considered a curiosity in the 1800’s. The first fuel cell was built in 1839 by Sir William Grove, a lawyer and gentleman scientist. Serious interest in the fuel cell as a practical generator did not begin until the 1960's, when the U.S. space program chose fuel cells over riskier nuclear power and more expensive solar energy. Fuel cells furnished power for the Gemini and Apollo spacecraft, and still provide electricity and water for the space shuttle.(1)
  • 4. s this have to do with fuel cells?” By providing energy from a battery, water (H2 O) can be dissociated into the diatomic molecules of hydrogen (H2 ) and oxygen (O2 ). Figure 1
  • 5. Basics lectrolysis in reverse.” fuel cell H2O O2 H2 heat work The familiar process of electrolysis requires work to proceed, if the process is put in reverse, it should be able to do work for us spontaneously. The most basic “black box” representation of a fuel cell in action is shown below: Figure 2
  • 6. uel Cell Basics hermodynamics H2(g) + ½O2(g) H2O(l) Other gases in the fuel and air inputs (such as N2 and CO2) may be present, but as they are not involved in the electrochemical reaction, they do not need to be considered in the energy calculations. 69.91 J/mol·K 205.14 J/mol·K 130.68 J/mol·K Entropy (S) -285.83 kJ/mol 00Enthalpy (H) H2O (l)O2H2 1 Thermodynamic properties at 1Atm and 29 Enthalpy is defined as the energy of a system plus the work needed to make room for it in an environment with constant pressure. Entropy can be considered as the measure of disorganization of a
  • 7. uel Cell Basics hermodynamics f the chemical reaction using Hess’ Law: ΔHreaction = ΣHproducts – ΣHreactants = (1mol)(-285.83 kJ/mol) – (0) = -285.83 kJ py of chemical reaction: ΣSproducts – ΣSreactants mol)(69.91 J/mol·K)] – [(1mol)(130.68 J/mol·K) + (½mol)(2 63.34 J/K gained by the system: = TΔS = (298K)(-163.34 J/K) = -48.7 kJ
  • 8. uel Cell Basics hermodynamics free energy is then calculated by: ΔH – TΔS = (-285.83 kJ) – (-48.7 kJ) = -237 kJ done on the reaction, assuming reversibility a W = ΔG one on the reaction by the environment is: sferred to the reaction by the environment W = ΔG = -237 kJ ΔQ = TΔS = -48.7 kJ More simply stated: The chemical reaction can do 237 kJ of work and produces 48.7 kJ of heat to the environment.
  • 9. Fuel Cell Basics Components Anode: Where the fuel reacts or "oxidizes", and releases electrons. Cathode: Where oxygen (usually from the air) "reduction" occurs. Electrolyte: A chemical compound that conducts ions from one electrode to the other inside a fuel cell. Catalyst: A substance that causes or speeds a chemical reaction without itself being affected. Cogeneration: The use of waste heat to generate electricity. Harnessing otherwise wasted heat boosts the efficiency of power-generating systems. Reformer: A device that extracts pure hydrogen from
  • 10. l Cell Basics tting it together. Figure 3
  • 11. Types of Fuel Cells The five most common types: •Alkali •Molten Carbonate •Phosphoric Acid •Proton Exchange Membrane •Solid Oxide
  • 12. Types of Fuel Cells Vorteil: Keine aufwendige Brenngas-Aufbereitung Nachteil: Hohe Betriebstemperaturen = Hohe System-Kosten  Starke Material-Beanspruchung SOFC
  • 13. Alkali Fuel Cell compressed hydrogen and oxygen fuel potassium hydroxide (KOH) electrolyte ~70% efficiency 150˚C - 200˚C operating temp. 300W to 5kW output requires pure hydrogen fuel and platinum catylist ($$)→ liquid filled container → corrosive leaks Figure 4
  • 14. Molten Carbonate Fuel Cell (MCFC) carbonate salt electrolyte 60 – 80% efficiency ~650˚C operating temp. cheap nickel electrode catylist up to 2 MW constructed, up to 100 MW designs exist Figure 5 The operating temperature is too hot for many applications. carbonate ions are consumed in the reaction inject CO→ 2 to compensate
  • 15. hosphoric Acid Fuel Cell (PAFC) phosphoric acid electrolyte 40 – 80% efficiency 150˚C - 200˚C operating temp 11 MW units have been tested sulphur free gasoline can be used as a fuel Figure 6 The electrolyte is very corrosive Platinum catalyst is very
  • 16. Proton Exchange Membrane (PEM) thin permeable polymer sheet electrolyte 40 – 50% efficiency 50 – 250 kW 80˚C operating temperature electrolyte will not leak or crack temperature good for home or vehicle use Figure 7
  • 17. Solid Oxide Fuel Cell (SOFC) hard ceramic oxide electrolyte ~60% efficient ~1000˚C operating temperature cells output up to 100 kWhigh temp / catalyst can extract the hydrogen from the fuel at the electrode high temp allows for power generation using the heat, but limits use Figure 8
  • 18. Benefits Efficient: in theory and in practice Portable: modular units Reliable:few moving parts to wear out or break Fuel Flexible: With a fuel reformer, fuels such as natural gas, ethanol, methanol, propane, gasoline, diesel, landfill gas,wastewater, treatment digester gas, or even ammonia can be used Environmental: produces heat and water (less than combustion in both
  • 19. terial‘s challenges of the PEM Fuel Cel
  • 20. 11/06/15 Fuel Cell Fundamentals 20 Review of Membrane (Nafion) Properties • Chemical Structure • Proton Conduction Process • Water Transport and Interface Reactions
  • 21. PSSA poly(sty rene-co- styrenes ulfonic acid) (PSSA) Nafion,TM Membrane C Dow PESA (Polyepoxy- succinic Acid) α,β,β- Trifluorosty rene grafted onto poly(tetrafl uoro- ethylene) with post- sulfonation) Poly – AMPSPoly(2-acrylamido- 2-methylpropane sulfonate) cal structures of some membrane mater
  • 24. The water transport through Nafion Membrane Water flux due to electroosmotic drag (mol/cm2 s) is: Nw, drag = Iξ(λ)/F. Where: I is the cell current, ξ(λ) is the electroosmotic drag coefficient at a given state of membrane hydration λ(=N(H2O)/N(SO3H) and F is the Faraday constant. This flux acts to dehyddrate the anode side of a cell and to introduce additional water at the cathode side. The buildup of water at the cathode (including the product water from the cathode reaction) is reduced, in turn, by diffusion back down the resulting water concentration gradient (and by hydraulic permeation of water in differentially pressurized cells where the cathode is held at higher overall pressure). The fluxes (mol/cm2 s) brought about by the latter two mechanisms within the membrane are: Nw,diff = -D(λ)∆c/ ∆z, Nw,hyd = -khyd(λ)∆P/ ∆z where D is the diffusion coefficient in the ionomer at water content λ, ∆c/ ∆z is a water concentration gradient along the z-direction of membrane thickness, khyd is the hydraulic permeability of the membrane, and ∆P/ ∆z is a pressure gradient along z.
  • 25. The water transport through Nafion Membrane Many techniques have been introduced to prevent the dehydration of the anode (including the introduction of liquid water into the anode and/or cathode, etc. – which, however, can lead to “flooding” problems that inhibit mass transfer). However, the overall question of “water management,” including the issue of drag as a central component, has been solved to a very significant extent by the application of sufficiently thin PFSA membranes (<100 µm thick) in PEFCs, combined with humidification of the anode fuel gas stream.
  • 26. Water Transport (& Interface Reactions) in Nafion Membrane of the PEM Fuel Cell
  • 28. SOFC Solid Oxide Fuel Cell Air side = cathode: High oxygen partial pressure 1 conductance d σ= µ Fuel side= anode: H2 + H2O= low oxygen partial pressure H2 + 1/2O2  H2O H2 O2 H2O
  • 29. SOFC Electromotive Force (EMF) Chemical Reactions in 2 separated compartements: - Cathode (Oxidation): - Anode (Reduction): ½O2 + 2e-  O2- H2 + O2-  H2O + 2e- EMF of a galvanic Cell: (1) EMF = ∆Gr /-z F ∆G = Free Enthalpie z = number of charge carriers F = Faraday Constant ∆G0= Free Enthalpie in standart state R = Gas Constant SOFC: ½O2 + H2  H2O ( )2 0 0.5 2 2 ln ( ) ( ) a H O G G RT a H a O ∆ = ∆ +(2) difference of ∆G between anode und cathode  ( ) ( ) 2 2 ln 4 p ORT EMK F p O = K A Nernst Equation:
  • 30. SOFC Elektrochemische Potential Oxygen ions migrate due to an electrical and chemical gradient 2 2 ( ) ( ) 2O O Fµ µ ϕ− − ∆ = ∆ − ∆% 2 ( )Oµ − ∆ % Chemical Potential Electrical Potential Electrochemichal Potential Driving force for the O2- Diffusion through the electrolyte are the different oxygen partial pressures at the anode and the cathode side: 2 ( ) 2 i ij O F σ µ − = − ∆ % ji = ionic current σi= ionic conductivity
  • 31. SOFC engl. Open Circuit Voltage (OCV) 2 ( ) 2 i ij O F σ µ − = − ∆ %2 2 ( ) ( ) 2O O Fµ µ ϕ− − ∆ = ∆ − ∆% 2 ( ) 0Oµ − ∆ =% What happems in case : 0ij = No current Electrical potential difference = chemical potetialOCV
  • 32. SOFC Leistungs-Verluste Under load decrease of cell voltage and internal losses U(I) = OCV - I(RE+ RC+RA) - ηC - ηA (RE+ RC+RA) OCV ηC ηA cell current I [mA/cm2 ] cellvoltageU(I)[V] Ohmic resistances Non ohmic resistances= over voltages
  • 33. SOFC Überspannungen Over voltages exist at interfaces of • Elektrolyte - Cathode • Elektrolyte - Anode Reasons: •Kinetic hindrance of the electrochemical reactions •Bad adheasion of electrode and electrolyte •Diffusion limitations at high current densities
  • 34. SOFC Ohm‘s losses 800nm Kathode Anode Reduce electrolyte thickness Past Future
  • 35. SOFC Leistungs-Verluste (1)Open circuit voltage (OCV), I = 0 (2)SOFC under Load  U-I curve (3) Short circuit, Vcell = 0 0.0 0.5 1.0 1.5 2.0 0.0 0.2 0.4 0.6 0.8 1.0 900°C in Luft/Wasserstoff Stromdichte [A/cm 2 ] Zellspannung[V] 0.0 0.1 0.2 0.3 0.4 0.5 Leistung[W/cm 2 ] (1) (2) (3) (RE+ RC+RA) OCV ηC ηA cell current I [mA/cm2] cellvoltageU(I)[V] (RE+ RC+RA) OCV ηC ηA cell current I [mA/cm2] cellvoltageU(I)[V] 1 2 3
  • 36. SOFC ( ) * U L R f T I A σ ∆ = = = 0 log( )aE T kT σ σ = − 1 . aT vs E T σ ⇒ Electrical resistance: Electrical conductivity: U : voltage [V] I : current [A] R : resistivity [ohm] ∆L : distance between both inner wires [cm] A : sample surface [cm2] σ : conductivity [S/m] Ea : activation energy [eV] T : temperature [K] K : Boltzmann constant How to determine the electrical conductance IinputUmeasured
  • 38. SOFC Tubular design i.e. Siemens-Westinghouse design Planar design i.e. Sulzer Hexis, BMW design Segment-type tubular design SOFC Design
  • 39. SOFC Tubular Design – Siemens-Westinghouse air flow anode (fuel) cathode interconnection cathode (air) Why was tubular design developed in 1960s by Westinghouse? • Planar cell: Thermal expansion mismatch between ceramic and support structures leads to problems with the gas sealing  tubular design was invented Advantages of tubular design: • At cell plenum: depleted air and fuel react  heat is generated  incoming oxidant can be pre-heated. • No leak-free gas manifolding needed in this
  • 40. SOFC anode (fuel) cathode (air) electrolyte Tubular Design – Siemens-Westinghouse To overcome problems new Siemens-Westinghouse „HPD- SOFC“ design: New: Flat cathode tube with ligaments Advantages of HPD-SOFC: • Ligaments within cathode  short current pathways  decrease of ohmic resistance • High packaging density of cells compared to tubular designSiemens-Westinghouse shifted from basic technology to cost reduction and scale up. Power output: Some 100 kW can be produced.
  • 41. SOFC Planar Design – Sulzer Hexis anode (fuel) electrolyte cathode (air) interconnect Advantages of planar design: • Planer cell design of bipolar plates  easy stacking  no long current pathways • Low-cost fabrication methods, i.e. Screen printing and tape casting can be used. Drawback of tubular design: • Life time of the cells 3000- 7000h  needs to be improved by optimization of mechanical and electrochemical stability of used materials.
  • 42. SOFC Planar Design – BMW electrolyte anode porous metallic substrate Fe-26Cr-(Mo, Ti, Mn, Y2O3) alloy cathode Cathode current collector bipolar plate bipolar plate Air channel Fuel channel 20-50 µm 5-20 µm 15-50 µm Plasma spray Plasma spray Plasma spray Application Batterie replacement in the BMW cars of the 7-series. Power output: 135 kW is aimed.
  • 43. Current Initiatives Automotive Industry Most of the major auto manufacturers have fuel cell vehicle (FCV) projects currently under way, which involve all sorts of fuel cells and hybrid combinations of conventional combustion, fuel reformers and battery power. Considered to be the first gasoline powered fuel cell vehicle is the H20 by GM: GMC S-10 (2001) fuel cell battery hybr low sulfur gasoline fue 25 kW PEM 40 mpg 112 km/h top speed Figure 9
  • 44. Fords Adavanced Focus FCV (2002) fuel cell battery hybrid 85 kW PEM ~50 mpg (equivalent) 4 kg of compressed H2 @ 5000 psi Approximately 40 fleet vehicles are planned as a market introduction for Germany, Vancouver and California for Current Initiatives Automotive Industry Figure 10 Figure 11
  • 45. Chrysler NECAR 5 (introduced in 2000) 85 kW PEM fuel cell methanol fuel reformer required 150 km/h top speed this model completed a California to Washing permit for Japanese roads Current Initiatives Automotive Industry Figure 12
  • 46. Mitsubishi Grandis FCV minivan fuel cell / battery hybrid 68 kW PEM compressed hydrogen fuel 140 km/h top speed Plans are to launch as a production vehicle for Europe in 2004. Current Initiatives Automotive Industry Figure 13
  • 47. Current Initiatives Stationary Power Supply Units A fuel cell installed at McDonald’s restaurant, Long Island Power Authority to install 45 more fuel More than 2500 stationary fuel cell systems have been installed all over the world - in hospitals, nursing homes, hotels, office buildings, schools, utility power plants, and an airport terminal, providing primary power or backup. In large-scale building systems, fuel cells can reduce facility energy service costs by 20% to 40% over conventional energy service. Figure 14
  • 48. Current Initiatives Residential Power Units There are few residential fuel cell power units on the market but many designs are undergoing testing and should be available within the next few years. The major technical difficulty in producing residential fuel cells is that they must be safe to install in a home, and be easily maintained by the average homeowner. Residential fuel cells are typically the size of a large deep freezer or furnace, such as the Plug Power 7000 unit shown here, and cost $5000 - $10 000. If a power company was to install a residential fuel cell power unit in a home, it would have to charge the homeowner at least 40 ¢/kWh to be Figure 15
  • 49. Future “...projections made by car companies themselves and energy and automotive experts concur that around 2010, and perhaps earlier, car manufacturers will have mass production capabilities for fuel cell vehicles, signifying the time they would be economically available to the average consumer.” Auto Companies on Fuel Cells, Brian Walsh and Peter Moores, posted on www.fuelcells.org Technical and engineering innovations are continually lowering the capital cost of a fuel cell unit as well as the operating costs, but it is expected that mass production will be of the greatest impact to affordability. A commercially available fuel cell power plant would cost about $3000/kW, but would have to drop below $1500/kW to achieve widespread market penetration. http://www.fuelcells.org/fcfaqs.htm
  • 50. Future internal combustion obsolete? solve pollution problems? common in homes? better designs? higher efficiencies? cheaper electricity? reduced petroleum dependency?
  • 51. References (1) FAQ section, fuelcells.org (2) Long Island Power Authority press release: Plug Power Fuel Cell Installed at McDonald’s Restaurant, LIPA to Install 45 More Fuel Cells Across Long Island, Including Homes, http://www.lipower.org/newscenter/pr/2003/feb26.fuelce ll.html (3) Proceedings of the 2000 DOE Hydrogen Program Review: Analysis of Residential Fuel Cell Systems & PNGV Fuel Cell Vehicles, http://www.eere.energy.gov/hydrogenandfuelcells/pdfs/2 8890mm.pdf Figures 1, 3 http://hyperphysics.phy- astr.gsu.edu/hbase/thermo/electrol.html 4 – 8 http://fuelcells.si.edu/basics.htm 10 http://www.moteurnature.com/zvisu/2003/focus_fcv/focus _fcv.jpg 11 http://www.granitestatecleancities.org/images/Hydrogen_F uel_Cell_Engine.jpg 12 http://www.in.gr/auto/parousiaseis/foto_big/Necar07_2883. jpg 13 http://www3.caradisiac.com/media/images/le_mag/mag138/o eil_mitsubishi_grandis_big.jpg 14 http://www.lipower.org/newscenter/pr/2003/feb26.fuelce

Hinweis der Redaktion

  1. PE (polymer electrolyte) FCs utilize a polymeric electrolyte. NafionTM, a perfluorinated polymer with sidechains terminating in sulfonic acid moieties, and its close perfluorosulfonic acid (PFSA) relatives, are currently the state-of-the-art in membranes for PEFCs, satisfying an array of requirements for effective, long-term use in fuel cells. They combine well the important requirements for a membrane in a PEFC, namely: high protonic conductivity, high chemical stability under typical operating conditions, and low gas permeabilities. Typically, thickness of PFSA membranes for PEFCs range between 50 and 175 m. The main source of PFSA membranes is DuPont (USA), where these membranes were invented in the 1960’s and made into a commercial product for the chlor-alkali industry. Other sources of developmental PFSA membranes have been Dow Chemical (USA), Asahi Glass (Japan), and Asahi Chemicals (Japan).
  2. The most important property of ionomeric membranes employed in polymer electrolyte fuel cells is the high protonic conductivity they provide at the current densities typically required in PEFCs. The specific conductivity of fully hydrated PFSA (immersed) membranes is about 0.1 S/cm at room temperature, and about 0.15 S/cm at the typical cell operation temperature of 80ºC. These high protonic conductivities provide the basis for the high power densities achievable in PEFCs. The dependence of proton mobility in PFSA membranes on water content is, however, quite critical, and demands effective cell and stack design to maintain a high level of water through the thickness of the membrane for the complete range of dynamic operation.
  3. The number of water molecules carried through the membrane per proton is a central factor in determinating the water profiles in the membrane of an operating PEFC. There is an important difference between the electroosmotic drag coefficient, (), a characteristic of an ionomeric membrane with fixed water content and flat water profile, and the net water flux through an operating fuel cell. The latter is the resultant of several water transport modes in the cell. For fully hydrated and (immersed) Nafion 1100 membranes, a drag coefficient of 2.5 H2O/SO3H is measured, whereas for a membrane equilibrated with vapor-phase water the drag coefficient is close to 1.0 H2O/H+ over a wide range of water contents. The lack of dependence of the drag coefficient on membrane nanostructure suggests that the drag coefficient is determined by the basic elements of the proton transport process; I.e.; via the hydronium ion or complex..