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Fuel Cell and
Hydrogen Energy Systems
Loh Kee Shyuan
Puri Pujangga
Universiti Kebangsaan Malaysia (UKM)
National University of Malaysia
18 June 2014
7th Asian School on Renewable Energy
Fuel Cell Institute, UKM
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Outline
• Introduction
• Types of fuel cells and hydrogen production
systems
• Basic performance and cost
• Applications
• Future prospects
2
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Chronology of Fuel Cell Development
• 1839 - Sir William Grove, first electrochemical H2/O2
reaction to generate energy
• 1950s - GE developed the solid-ion exchange H2 fuel cell
used by NASA
• 1960s- GE produced the fuel cell-based electrical power
system for NASA Gemini and Apollo space capsules
• 1960s other fuel cells discovered – phosphoric acid, SOFC,
molten carbonate
• 1970s – Vehicle manufacturers began to experiment FCEV.
• 1990 – The California Air Resource Board introduced the
Zero Emission Vehicle (ZEV) Mandate.
• 2000 – Fuel cell buses were deployed as part of the
HyFleet/CUTE project
• 2007 – fuel cell started to be sold commercially as APU
• 2008 – Honda begins leasing the FCX fuel cell electric
vehicle.
• 2009 – Large scale of residential CHP programme in Japan.
4
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
What is Fuel Cell?
5
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
How does fuel cell work?
• In a typical fuel cell, gas (hydrogen) is fed
continuously to the anode compartment and an
oxidant (e.g. oxygen from the air) is fed
continuously to the cathode (positive electrode)
compartment. Electrochemical reactions take
place at the electrodes to produce electric
current.
6
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
How does fuel cell work?
• At the anode:
H2  2H+ + 2e-
• At the cathode:
½ O2 + 2H+ + 2e-  H2O
• Overall:
H2 + ½ O2  H2O
7
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Main Components
• Electrode: a thin catalyst layer pressed between the ionomer membrane and
porous, electrically conductive substrate.
• 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.
• Bipolar plates: connecting the anode of one cell to the cathode of the
adjacent cell.
• Gas diffusion layer: a layer between the catalyst layer and bipolar plates, also
called electrode substrate or diffusor/current collector.
8
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Main Components
9
Endplate
Bipolar plate
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Schematic overview of the three phase boundary
10
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell vs Battery
• Converting chemical energy to electrical energy.
• Works like a battery but does not run down or
need recharging.
• Produce electricity as long as fuel is supplied.
11
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Comparison of Fuel Cells with Internal Combustion Engines
12
Chemical energy of fuels Electrical Energy
Thermal Energy Mechanical Energy
Fuel Cell
ICE-1
ICE-2
ICE-3
Schematic of energy conversion in Fuel cells and Internal
Combustion Engines (ICE)
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell as Power Alternative
13
ICEs
- operate by burning fuel to create heat, heat is converted into
mechanical energy and then electric power.
- the efficiency of this conversion process is greatly affected by
losses of waste heat and friction.
- In contrast, fuel cells efficiently convert fuel directly into
electricity via an electrochemical reaction
- Like an ICE, fuel cells conveniently use fuel from and they
operate continuously as long as fuel is supplied.
- However, fuel cells do not burn fuel and therefore do not
produce the air pollutants resulting from combustion.
Batteries
- energy storage devices; they can only produce power
intermittently as they must be recharged.
- recharging process is lengthy, inconvenient, and shifts pollution,
efficiency and cost issues up the power line to central electrical
power plants.
- Batteries and fuel cells are both electrochemical (no combustion)
devices that have high efficiency and quiet operation.
- A battery stores its energy in its electrodes. Electricity is released
as the stored energy is consumed.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
High energy-conversion efficiency
14
Thermodynamic efficency for fuel cells and Carnot efficiency for heat
engines.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Overview of fuel cell types
• They are usually differentiated by the
type of fuel used, operating pressure
and temperature, area of application.
• Fuel cells can be distinguished by the
type of electrolyte material used as a
medium for the internal transfer of
ions (protons).
• The type of electrolyte determines
the operating temperature on which
the type of catalyst depends.
• The choice of fuel and oxidant for any
FC depends on their electrochemical
activity, cost, and easiness of fuel and
oxidant delivery and removal of
reaction by-products.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Overview of fuel cell types
17
Fuel Cell Electrolyte Qualified
Power (W)
Working
Temperature
(◦C)
Electrical
Efficiency
Status
Alkaline fuel cell Aqueous alkaline solution
(e.g., potassium hydroxide)
10 kW to 100
kW
60-120 35-55 Commercial/Rese
arch
Direct methanol
fuel cell
Polymer membrane
(ionomer)
100 kW to 1
mW
60-200 20-30 Commercial/Rese
arch
Phosphoric acid
fuel cell
Molten phosphoric acid
(H3PO4)
up to 10 MW 150-220 40 Commercial/Rese
arch
Molten
carbonate fuel
cell
Molten alkaline carbonate
(e.g., sodium bicarbonate
NaHCO3)
100 MW 600-650 >50 Commercial/Rese
arch
Solid oxide fuel
cell
O
2-
-conducting ceramic oxide
(e.g., zirconium dioxide,
ZrO2)
up to 100
MW
700–1000 >50 Commercial/Rese
arch
Proton exchange
membrane fuel
cell
Polymer membrane
(ionomer) (e.g., Nafion® or
Polybenzimidazole fiber)
100 W to
500 kW
50-100 35-45 Commercial/Rese
arch
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Characteristics of Fuel Cells
18
Fuel Cells Attractive Attributes Undesirable Attributes
Phosphoric Acid
Fuel Cell (PAFC).
-Low temperatures suitable for portable
device applications
-Ability for variable power output
-Broad fuel choice
-Uses expensive platinum as a
catalyst.
-Electrolyte is poor conductor at low
temperatures
Proton Exchange
Membrane Fuel Cell
(PEM).
-Low operating temperature suitable for
transportation and portable devices
-High power density
-Uses expensive platinum as a
catalyst
-Sensitivity to fuel impurities
Molten Carbonate
Fuel Cell (MCFC)
-High operating temperature improves
efficiency for base load power plants.
-Not suitable for small-sized
applications
Solid Oxide Fuel Cell
(SOFC)
-High operating temperature improves
efficiency for base load power plants.
-Solid electrolyte improves conductivity
- Electrolyte is made from ceramics
and solid zirconium oxide that is a
rare mineral
Alkaline Fuel Cells
(AFC)
-Low temperature and high fuel-to-
electricity efficiency
-Requirement of pure hydrogen and
allergic to carbon dioxide
Direct Methanol
Fuel Cells (DMFC).
-Eliminates need for fuel reformer drawing
hydrogen directly from the anode
-Low temperatures suitable for portable
devices
-Fuel crossing from anode to cathode
without producing electricity
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel cell Basic Chemistry & Thermodynamics
20
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel cell Basic Chemistry & Thermodynamics
21
T (K) ΔH ΔG ΔS Eth (V)
298.15 -286.02 -237.34 -0.16328 1.23
333.15 -284.85 -231.63 -0.15975 1.20
353.15 -284.18 -228.42 -0.15791 1.184
373.15 -283.52 -225.24 -0.15617 1.167
Change of enthalpy, Gibbs Free Energy, and Entropy of hydrogen/oxygen fuel cell reaction with temperature and resulting
theoretical cell potential
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel cell Basic Chemistry & Thermodynamics
22
• Effect of pressure
 For the H2/O2 fuel cell reaction, the Nernst equation
becomes:
 By introducing Eq (1),
 Therefore, cell potential is higher at higher reactant
pressures.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Electrochemistry
• Electrode kinetics
 Electrochemical reactions involve transfer of electrical charge and change of Gibbs
energy.
 The rate of electrochemical reaction is determined by an activation energy barrier
that the charge overcome in moving from electrolyte to electrode or vice versa.
 Faraday’s Law: current density is proportional to the charge transferred and the
consumption of reactant per unit area:
 i = nFj
 The consumption of the reactant species is proportional to their surface
concentration. For the forward reaction, the flux is:
 jf =kfCOx and jb = kbCRd
 The net current generated is the difference between the electrons released and
consumed:
 i =nF (kfCOx − kbCRd)
 At equilibrium, the net current should equal zero because the reaction will proceed
in both directions simultaneously at the same rate.
 The rate which reaction proceed at equilibrium is called the exchange current
density.
23
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Electrochemistry
• Exchange current density
– The exchange current density is analogous to the rate constant chemical
reaction.
– i0 is concentration dependent, is a function of temperature, also a function
of catalyst loading and catalyst specific surface area.
– The effective exchange current density at any temperature and pressure is
given as:
24



















ref
c
ref
r
cc
ref
T
T
RT
E
P
Laii 1exp
Pr
00

Where
i0
ref = reference exchange current density (at
ref T, P) per unit catalyst surface are,Acm-2
Pt.
ac = catalyst specific area.
Lc = catalyst loading.
Pr = reactant partial pressure, kPa.
Pr
ref = reference pressure, kPa.
γ = pressure coefficient (0.5 to1.0).
Ec = activation energy (66 kJ/mol for O2
reduction on Pt).
R = gas constant, 8.314 Jmol-1K-1
T = temperature, K.
Tref = reference temperatire. 298.15 K
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Electrochemistry
• Voltage Losses
 Activation polarization
 Internal Currents and crossovers losses
 Ohmic (resistive) losses
 Concentration polarization
25
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Electrochemistry
26
• Voltage different from equilibrium is
need to get the electrochemical
reaction going – activation
polarization













 
aacc
rcell
aactcactraccell
i
i
F
RT
i
i
F
RT
EE
VVEEEE
,0,0
,,
lnln

• each H2 molecule that diffuse results
in fewer electrons that travel to the
external circuit
• the losses are minor during fuel cell
operation, BUT significant when fuel
cell operates at low current densities,
or it is at open circuit voltage.







0
, ln
i
i
F
RT
EE
loss
rOCVcell

Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Electrochemistry
27
• Ohmic losses occur due to the
resistance of the flow of ions in the
electrolyte and resistance to the flow
of electrons.
• Concentration polarization occur
when a reactant is rapidly consumed
at the electrode by the
electrochemical reaction so that
concentration gradients are
established.cieiiii RRRR ,,, 








ii
i
nF
RT
V
L
L
conc ln
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Electrochemistry
• Three types of losses in
fuel cell.
• Activation losses are by far
the largest losses at any
current density.
• The cell voltage is
therefore:
28
ohmcconcactaconcactrcell VVVVVEV  )()(
i
aL
aL
cL
cL
aoacoc
PTrcell iR
ii
i
nF
RT
ii
i
nF
RT
i
i
F
RT
i
i
F
RT
EE 



 )ln()ln()ln()ln(
,
,
,
,
,,
,,

Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Polarization Curve
• A polarization curve is the most important characteristic of a fuel
cell and its performance.
• It would be useful to see what effect each of the parameters has
on the polarization curve shape.
29
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Sensitivity of parameters in polarization curve
• Effect of transfer coefficient/Tafel slope
• Effect of exchange current density
• Effect of H2 crossover and internal current loss
• Effect of internal resistance
• Effect of limiting current density
• Effect of operating pressure
• Air vs oxygen
30
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Sensitivity of parameters in polarization curve
Effect of transfer coefficient on fuel cell performance
α =0.5
α =1.5
α=1
Effect of exchange current density on fuel cell polarization
curve.
Effect of cell internal resistance on its polarization curve. Effect of operating pressure on fuel cell polarization curve
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Theoretical Fuel Cell Efficiency
• Assuming that all of the Gibbs free energy can be converted into
electrical energy, the maximum possible efficiency of a fuel cell is:
η= ΔG/ ΔH = 237.34/ 286.02 = 83%
• Maximum theoretical fuel cell efficiency:
η= ΔG/ ΔHLHV = 228.74/ 241.98 = 94.5%
• If both ΔG/ ΔH are divided by nF, the fuel cell efficiency may be
expressed as a ratio of two potentials:
η= (ΔG/nF)/ (ΔH/nF)HHV = 1.23/1.482 = 0.83
• The fuel cell efficiency is always proportional to the cell potential.
32
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Basic performance of fuel cell
• The overall performance of fuel cell may be evaluated on the basis of the
current-voltage diagram.
Journal of Power Sources 113 (2003) 37–43
Effect of cell temperature on performance. E-TEK 20% Pt/C; Pt =0:12 mg/cm2.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Basic performance of fuel cell
Journal of Power Sources 113 (2003) 37–43
Effect of Pt loading on performance for electrodes made using E-TEK 20% Pt/C, 35/45/45 ˚C.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Implication and Use of Fuel Cell Polarization Curve
• Fuel cell polarization curve may be used for
diagnostic purposes, as well as for sizing and
control of a fuel cell.
• From potential-current relationship, other
information about the fuel cell may also become
available just by rearranging the potential-
current data.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Use of polarization curve for fuel cell sizing
• H2/air fuel cell polarization curve is given with
the followings parameters:
α = 1, i0 = 0.001 mAcm-2, Ri = 0.2Ωcm-2
Operating conditions: T =60˚C, P=101.3 kPa
Operating point is selected at 0.6 V. Active area is
100 cm2.
(a) Calculate nominal power output.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Solution
• Power output is
Wel = Vcell x i x A
Vcell = 0.6 V
A =100 cm2
i = ???
• Current density must be determined from the polarization curve. Because no H2 crossover and
internal current losses and no limiting current are given, the fuel cell polarization curve may b
calculated from:
Where
Er = 1.482-0.000845T + 0.0000431T ln(PH2PO2
0.5)
= 1.482-0.000845 (333.15) + 0.0000431 (333.15) ln (0.21)0.5
=1.189 V
R=8.314 Jmol-1K-1
T=333.15K
α =1
n = 2
F =96485 C mol-1
Io = 0.001 mAcm-2
Ri = 0.2 Ωcm2
Current cannot be explicitly calculated from the previous equation.
37
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Solution
( b) The engineers improved fuel cell performance by improving internal
resistance to Ri = 0.15 Ohm-cm2.calculate power gain at 0.6 V
• From the new polarization curve, the current density is:
I = 1.25 Acm-2
Power output is, Wel = 0.6 x 1.25 x 100 = 75.0 W
Power gain is ΔW = 75.0 – 58.2 = 16.8 W or 28.9%
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Solution
(c) The engineer found out that there was not enough air flow to operate
this fuel cell at a higher current density. Calculate the power and efficiency
gain if the improved fuel cell is to be operated at the original current
density.
Vcell = 1.189 – (8.314x333.15)/(1x96485) ln (970/0.001) – 0.97 x 0.15
= 0.648 V
New power output is, Wel = 0.648 x 0.97 x 100 = 62.9 W
Power gain is, ΔW 62.9 -58.2 = 4.7 W or 8%
The efficiency before improvement was:
η=Vcell/1.482 = 0.6/1.482 =0.405
The efficiency after improvement is:
η=Vcell/1.482 =0.648/1.482 = 0.437
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Solution
Fuel cell power output is
58.2 = Vcell x i x 100
Another Vcell-i relationship is obtained from
the polarization curve:
Vcell = 1.189 – (8.314x333.15)/(1x96485) ln
(i/0.001) – i x 0.15
Again, by iteration or graphically the solution
is:
Vcell = 0.666 V
i = 875 mACm-2
Noted that point “a” and “d” lay on two
different polarization curve but in the
same constant power line.
The new efficiency is
η = Vcell/1.482 = 0.666/1.482 = 0.449
(d) The engineer realized that there is no need for additional power. Calculate the
efficiency gain if the improved fuel cell is to be operated at the original power output.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Cost expectations-Fuel cell costs
• The US Department of Energy (DOE) had aimed (in 2007)
to demonstrate fossil fuelled PEMFC CHP systems for
under $750/kW by 2011 and under $450/kW by 2020.
• These targets were recently revised to $1200/kW by 2015
and $1000/kW by 2020, for a complete 2 kW natural gas
fuelled PEMFC system.
• The DOE’s SECA programme established cost targets for
3-10 kW stationary SOFC systems, initially starting at
$800/kW by 2005, then falling to $700/kW by 2008 and
$400/kW by 2010.
• Their cost reduction efforts now aim to demonstrate fuel
cell stacks for $175/kW and complete systems for
$700/kW
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Type of fuel cells application?
46
There are many different uses of fuel cells being utilized right now. Some of these
uses are…
•Power sources for vehicles such as cars, trucks, buses and even boats and submarines
•Power sources for spacecraft, remote weather stations and military technology
•Batteries for electronics such as laptops and smart phones
•Sources for uninterruptable power supplies.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Type of fuel cells application?
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel cell vehicles by various automakers
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Layout of Honda FCX Powertrain
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Specification of several fuel cell vehicles
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen stations
51
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Toyota FCHV-BUS at FC Expo
52
•90 kW PEFC Fuel cell stack: twice
•Motor: AC synchronous 80 kW twice
•Hydrogen tank: Compressed hydrogen gas
35 MPa / 150 liter, five (version 2002) or
seven (version 2005)
•Passenger capacity: 63 (included 22 seats)
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Residential Fuel Cell
53
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Fuel Cell Technologies Forging Cross-industry Collaboration
• Google, one of the pilot customers, has a 400-
kilowatt installation at its main campus. Over 18
months, the project delivered 3.8 million kilowatt
hours of electricity.
• Wal-Mart has installed two 400 KW systems at retail
locations in Southern California.
• Bank of America is putting in a 500 KW installation at
a call center in Southern California.
• Coke too is putting in a 500 KW installation, at its
Odwalla plant in Dinuba, Calif. That fuel cell will run
on re-directed biogas and provide up to 30 percent
of the plant’s electricity needs.
• Cox Enterprises is putting in a 400 KW installation at
its KTVU TV station in Oakland, Calif.
• E-commerce giant e-Bay is using a 500 KW
installation at its San Jose, Calif., facility that will run
on biogas.
• FedEx has installed five 100 KW Bloom boxes at its
package sorting facility in Oakland.
54
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Alternative Energy
56
• Increasing of energy demand
• Depletion of fossil fuel in near future
• Reducing negative impact on
environmental
Renewable Energy 31 (2006) 719–727
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
What is our choices?
• Pressing need to find alternative renewable,
sustainable and clean energy source.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Alternative energy
• Sustainable – ability of an energy source to
continue providing energy for a long period of
time
• Renewable – energy that comes from resources
which are continually replenished
• Clean ‐ does not pollute the atmosphere when
used/produced
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen properties
• Gaseous, odorless, colorless, tasteless,
flammable, explosive
• Bonds with many other elements
• Seldom found in pure form in nature
• Liquid at -253 ˚C (20 K)
• Not an energy source, it is an energy
carrier/store
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen safety
• Hydrogen Vehicle Safety.
– The Ford Motor Company, in their report to the US
Department of Energy included this statement:
“Overall, we judge the safety of a hydrogen
FCV system to be potentially better than the
demonstrated safety record of gasoline or
propane, and equal to or better than that of
natural gas.”
60
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen safety
61
Hydrogen Vehicle Gasoline Vehicle Hydrogen Vehicle Gasoline Vehicle Hydrogen Vehicle Gasoline Vehicle
One minute after ignition; hydrogen
fire nearly extinguished
The pictures below were taken 3
seconds after ignition
The following pictures compare
hydrogen and gasoline fires from an
experiment conducted at the
University of Miami.
The car on the left contained high pressure hydrogen tanks with 175,000 btu of energy and the
car on the right had a conventional gasoline tank with just five pints of gasoline or about 70,000
btus of energy. Spark plugs were installed outside both vehicles to ignite a leaking hydrogen
tank and a leaking gasoline line.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen Production Paths
62
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen production methods
• Main methods
-Thermal
-Electrochemical
-Biological
• Others
-Chemical reaction
-etc
Primary method Process Source/Feed
stock
Energy
Thermal Stream reforming Natural gas High temperature steam
(autothermal)
Thermochemical
water splitting
Water High temperature heat from
nuclear reactor
Gasification Coal, Biomass High temperature (&
pressure) steam & oxygen
Pyrolysis Biomass Moderately high
temeprature
Electrochemcal Electrolysis Water Electricity from solar, wind,
hydro & nuclear
Photoelectrochemi
cal
Water Direct from sunlight
Biological Photobiological Water & algae
strains
Direct sunlight
Anaerobic/ferm
entation
Biomass &
microorganis
m
Food source
Anaerobic
degistion
Biomass High temperature heat
Fermentative
microorganisms
Biomass High temperature heat
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen production technologies
Steam methane reforming :
• widely used in the chemical and refining industries.
• Considered the cheapest way of producing hydrogen.
• Reforming involves the reaction of desulphurized natural gas with high-
temperature steam over a Ni-based catalyst.
• This produces syngas-mainly a mixture of H2 and CO.
• The CO is then converted to H2 and CO2 via a water gas shift reaction.
• High purity (up to 99.99%) H2 is separated using pressure swing adsorption
method.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen production technologies
Coal gasification:
• well-established commercial technology
• competitive with SMR only where oil and/or
natural gas are expensive.
• coal could replace natural gas and oil as the
primary feedstock for hydrogen production, since
it is so plentiful in the world.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen production technologies
Electrolysis of water :
• Water molecules can be separated using electricity. But we use
electricity to produce hydrogen to produce electricity again.
• Pure water is in many places a scarce resource.
• The electricity for the electrolysis needs to be produced and the
water needs to be purified (soft de-ionized water is needed).
• Reaction:
• Electricity can be obtained at a large scale from nuclear reactors
but the hydrogen needs to be stored and transported, and nuclear
fuel is not a renewable source of energy.
• At a VERY small scale wind or solar power can be used, but this
energy is available only when there is wind or sunlight.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen production technologies
Biomass gasification and pyrolysis:
• Provide two ways to produce H2 from biomass.
• The processes can be adapted to a range of feedstock:
switch grass, plant scraps, garbage, willow, sugar cane
waste.
• Both techniques are followed by a reforming stage.
• Gasifier may be heated indirectly and directly.
• With pyrolysis, biomass is rapidly heated in the absence
of O2, the vapors are then condensed to form pyrolysis
oil.
• This pyrolysis oil can be used as feedstock for H2
production.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Conversion of Biomass
Pyrolysis
Gasification
Combustion
No oxygen
With oxygen
(partial oxidation)
With oxygen
(complete oxidation)
Organic material + heat -> charcoal +oil +gases
Organic material + O2 +H2O-> H2 +CO2 +CO+ others
Organic material + O2-> CO2 +H2O
Slow &Low (<450ºC)
-Max char 35%wt
Intermediate (450-500ºC)
-Typical 10-15% has. 20-30% char,
45-65% oil
Fast & high (>500ºC)
-(>550ºC – mas oil 70%)
-(>600ºC - max gas 80%)
High (>800ºC)
Low (start 200‐300ºC)
(>1000ºC)
Gas-Syngas
CO2
H2O
CO
CH4 etc
Heat
Solid-char
Liquid-oil
Hydrogen
Transfrom
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen Storage Alternatives
• Compressed Gas Storage
• Solid State Storage
• Liquid Hydrogen Storage
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Compressed Gas Storage
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
High Pressure Gas
• High-pressure hydrogen is stored in cylinders.
• Conventional cylinders – cylindrical shaped
sidewall section with hemispherical end
domes.
• Conformal Cylinders – Use multiple cylinders
in tandem and distort the cylindrical shape in
order to increase the usable volume.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Hydrogen Cylinders
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Metal Hydrides
• Principle used is that some metals readily
absorb gaseous hydrogen under conditions of
high pressure and moderate temperature to
form metal hydrides
• These metal hydrides release the hydrogen
gas when heated at low pressure and
relatively high temperature
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Metal Hydrides
• There are many types of specific metal
hydrides
• Primarily they are based on metal alloys of
magnesium, nickel, iron and titanium
• They are divided into:
• high hydrogen desorption temperature
• low hydrogen desorption temperature
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Metal Hydrides
• High hydrogen desorption temperature
• Less expensive
• Holds more hydrogen
• Requires significant amount of heat to release
hydrogen
• Low hydrogen desorption temperature
• Heat from an engine is sufficient to release hydrogen
• Sometime in this case it releases hydrogen at
ambient temperatures
• It needs to be pressurized to overcome this problem
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Metal Hydrides
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Metal Hydrides
Advantages
• Hydrogen becomes part of the chemical
structure of the metal itself and therefore
does not require high pressures or cryogenic
temperatures for operation
• Since hydrogen is released from the hydride
for use at low pressure, hydrides are the most
intrinsically safe of all methods of storing
hydrogen
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Metal Hydrides
Disadvantages
• They have low mass energy density
• Best metal hydrides contain only 8% hydrogen by
weight
• very heavy and expensive
• Metal hydride storage systems can be up to 30
times heavier and ten times larger than a gasoline
tank with the same energy content
• They must be charged with only very pure hydrogen
• If they become contaminated there is loss of
capacity
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Liquid Hydrogen Storage
Liquid hydrogen storage tank (850,000 gallons) at NASA KSC
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Liquid Hydrogen
• The storage of liquefied cryogenic gases is a
proven and tested technology.
• Hydrogen was first liquefied by J. Dewar in
1898.
• In liquid form, hydrogen can only be stored
under cryogenic temperatures.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Advantages
• Liquid hydrogen: high energy/mass ratio, three times
that of gasoline.
• It is the most energy dense fuel in use (excluding
nuclear reactions fuels), which is why it is employed in
all space programs
• Compared with compressed hydrogen, liquid hydrogen
has much lower storage pressure  the risk caused by
high pressure may be reduced to some extent.
• Liquid hydrogen (LH2) tanks can store more hydrogen in
a given volume than compressed gas tanks.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Disadvantages
• Requires extremely low temperatures of -423 F/-
2520
C.
• Boil-off losses / vaporization of hydrogen due to
heat leakage constitute a major disadvantage.
• A highly sophisticated and expensive production
and processing system is necessary in order to
minimize losses caused by diffusion, evaporation
and impurity.
• Evaporation losses on todays tank installations
are between 0.3 and 3% per day.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Summary of H2 Storage
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Cost expectations-Hydrogen production costs
• H2 production from natural gas by steam reforming
methods is well established.
• At low (pipeline) pressure, it is about 1.0 US$kg-1 (based
on inexpensive natural gas, assumed at 1.5 US$ GJ-1).
• Simbeck and Chang (2002) estimate the delivered H2 cost
from biomass waste is about 2.5 US$kg-1.
• Conventional small-scale electrolyzer H2 cost have been
estimated as 8-12 US$kg-1.
• Larger unit using surplus wind power may attain a cost
down to 2 US$kg-1
• The H2 cost based on coal gasification is estimated as over
12 US$kg-1
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Cost and performance characteristics of various hydrogen production
Process
Energy Required
(kWh/Nm3)
Ideal
Energy Required
(kWh/Nm3)
Practical
Status of Tech.
Efficiency
[%]
Costs Relative
to SMR
Steam methane reforming
(SMR)
0.78 2-2.5 mature 70-80 1
Methane/ NG pyrolysis R&D to mature 72-54 0.9
H2S methane reforming 1.5 - R&D 50 <1
Landfill gas dry reformation R&D 47-58 ~1
Partial oxidation of heavy oil 0.94 4.9 mature 70 1.8
Naphtha reforming mature
Steam reforming of waste oil R&D 75 <1
Coal gasification (TEXACO) 1.01 8.6 mature 60 1.4-2.6
Partial oxidation of coal mature 55
Steam-iron process R&D 46 1.9
Chloralkali electrolysis mature by-product
Grid electrolysis of water 3.54 4.9 R&D 27 3-10
Solar & PV-electrolysis of
water
R&D to mature 10 >3
High-temp. electrolysis of
water
R&D 48 2.2
Thermochemical water
splitting
early R&D 35-45 6
Biomass gasification R&D 45-50 2.0-2.4
Photobiological early R&D <1
Photolysis of water early R&D <10
Photoelectrochemical
decomp. of water
early R&D
Photocatalytic decomp. of
water
early R&D
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Cost of various hydrogen production technologies
Technology Cost range (US$
(2000)/GJH2
Additional cost
of CO2 capture
Comments
SMR, large-scale
(>1000MW)
SMR, small-scale
(<5MW)
5.25-7.26
11.50-40.40
$7.26 cost
increases to
$8.59/GJ with
CCS Prohibitive
Cost highly dependent
on natural gas prices.
Transitional
technology. Cost highly
dependent on natural
has prices, plant size
and purity of H2
required.
Coal gastification 5.4-6.8 Average of 11% Coal price more stable
and predicatable than
natural gas.
Biomass
gasification
(>10MW)
7.54-32.61
(av.14.31)
Not given (with
CCS technology,
would become
carbon
negative)
Size ranges from 25 to
303 MW and affects
cost.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Cost of various hydrogen production technologies
Technology Cost range (US$
(2000)/GJH2
Additional cost of
CO2 capture
Comments
Biomass pyrolysis
(>10MW)
6.19-14.98 Not given (with CCS
technology would
become carbon
negative)
Size ranges form 36
to 150MW; cost
redued by sale of
co-products
Electrolysis, Large
scale (>1MW)
11-75 Emissions (and CCS
options) depend on
source of electricity
Size ranges from 2
to 376MW, but
little effect on cost;
cost very
dependent on
assumed price of
electricity
Electrolysis, small-
scale (<1MW)
28-133 Emissions (and CCS
options) depend on
source of electricity
Size ranges from
0.03 to 0.79MW,
cost very size-
dependent.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Wind/ Hydrogen Projects
• Greece
 RES2H2 Project
• Spain
 RES2H2 Project
 ITHER Project
• Canada
Ramea Island
Prince Edward Island
• United Kingdom
HARI Project
PURE Project
• United Stated
 Basin electric, Wind-to-Hydrogen Energy Pilot Project
 National RE Lab and Xcel Energy, Wind-to-Hydrogen Project
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
PURE Project
• The project aims to demonstrate how wind power and hydrogen
technology can be combined to meet the energy needs of a remote
rural industrial estate.
• PURE was conceived to test and demonstrate safe and effective
long-term use and storage of hydrogen produced by renewable
energy using wind-powered electrolysis of water, and to regenerate
the stored energy into electric energy with a fuel cell.
• The key components of the system are:
 Wind turbines: Two 15 kW (Proven Ltd)
 Electrolyzer: 15 kW alkaline operating at 55 bar (AccaGen SA)
 Hydrogen storage: 44 Nm3 in H2 cylinders
 PEM fuel cell: 5 kW (Plug Power).
• The electrolyzer section consists of an AccaGen electrolyzer unit
assembled with advanced cells specifically designed and
manufactured by AccaGen SA for wind application, capable of
operating up to 55 bar.
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Basin Electric, Wind-to-Hydrogen Energy Pilot Project
• this project was to research the application of hydrogen
production from wind energy, allowing for continued wind
energy development in remote wind-rich areas and
mitigating the necessity for electrical transmission
expansion.
• The report completed on August 2005 found that the
proposed hydrogen production system would produce
between 8,000 kg and 20,000 kg of hydrogen annually.
• The cost of the hydrogen produced ranged from $20 to
$10 per kilogram.
• The hydrogen-production system utilizes a bipolar alkaline
electrolyzer nominally capable of producing 30 Nm3/h (2.7
kg/h).
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Future energy landscape
91
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
Furture Energy Landscape
Loh Kee Shyuan
7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 93
THANK YOU
ksloh@ukm.edu.my

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Fuel Cell and Hydrogen Energy Systems Overview

  • 1. Fuel Cell and Hydrogen Energy Systems Loh Kee Shyuan Puri Pujangga Universiti Kebangsaan Malaysia (UKM) National University of Malaysia 18 June 2014 7th Asian School on Renewable Energy Fuel Cell Institute, UKM
  • 2. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Outline • Introduction • Types of fuel cells and hydrogen production systems • Basic performance and cost • Applications • Future prospects 2
  • 3.
  • 4. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Chronology of Fuel Cell Development • 1839 - Sir William Grove, first electrochemical H2/O2 reaction to generate energy • 1950s - GE developed the solid-ion exchange H2 fuel cell used by NASA • 1960s- GE produced the fuel cell-based electrical power system for NASA Gemini and Apollo space capsules • 1960s other fuel cells discovered – phosphoric acid, SOFC, molten carbonate • 1970s – Vehicle manufacturers began to experiment FCEV. • 1990 – The California Air Resource Board introduced the Zero Emission Vehicle (ZEV) Mandate. • 2000 – Fuel cell buses were deployed as part of the HyFleet/CUTE project • 2007 – fuel cell started to be sold commercially as APU • 2008 – Honda begins leasing the FCX fuel cell electric vehicle. • 2009 – Large scale of residential CHP programme in Japan. 4
  • 5. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 What is Fuel Cell? 5
  • 6. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 How does fuel cell work? • In a typical fuel cell, gas (hydrogen) is fed continuously to the anode compartment and an oxidant (e.g. oxygen from the air) is fed continuously to the cathode (positive electrode) compartment. Electrochemical reactions take place at the electrodes to produce electric current. 6
  • 7. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 How does fuel cell work? • At the anode: H2  2H+ + 2e- • At the cathode: ½ O2 + 2H+ + 2e-  H2O • Overall: H2 + ½ O2  H2O 7
  • 8. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Main Components • Electrode: a thin catalyst layer pressed between the ionomer membrane and porous, electrically conductive substrate. • 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. • Bipolar plates: connecting the anode of one cell to the cathode of the adjacent cell. • Gas diffusion layer: a layer between the catalyst layer and bipolar plates, also called electrode substrate or diffusor/current collector. 8
  • 9. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Main Components 9 Endplate Bipolar plate
  • 10. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Schematic overview of the three phase boundary 10
  • 11. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell vs Battery • Converting chemical energy to electrical energy. • Works like a battery but does not run down or need recharging. • Produce electricity as long as fuel is supplied. 11
  • 12. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Comparison of Fuel Cells with Internal Combustion Engines 12 Chemical energy of fuels Electrical Energy Thermal Energy Mechanical Energy Fuel Cell ICE-1 ICE-2 ICE-3 Schematic of energy conversion in Fuel cells and Internal Combustion Engines (ICE)
  • 13. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell as Power Alternative 13 ICEs - operate by burning fuel to create heat, heat is converted into mechanical energy and then electric power. - the efficiency of this conversion process is greatly affected by losses of waste heat and friction. - In contrast, fuel cells efficiently convert fuel directly into electricity via an electrochemical reaction - Like an ICE, fuel cells conveniently use fuel from and they operate continuously as long as fuel is supplied. - However, fuel cells do not burn fuel and therefore do not produce the air pollutants resulting from combustion. Batteries - energy storage devices; they can only produce power intermittently as they must be recharged. - recharging process is lengthy, inconvenient, and shifts pollution, efficiency and cost issues up the power line to central electrical power plants. - Batteries and fuel cells are both electrochemical (no combustion) devices that have high efficiency and quiet operation. - A battery stores its energy in its electrodes. Electricity is released as the stored energy is consumed.
  • 14. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 High energy-conversion efficiency 14 Thermodynamic efficency for fuel cells and Carnot efficiency for heat engines.
  • 15.
  • 16. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Overview of fuel cell types • They are usually differentiated by the type of fuel used, operating pressure and temperature, area of application. • Fuel cells can be distinguished by the type of electrolyte material used as a medium for the internal transfer of ions (protons). • The type of electrolyte determines the operating temperature on which the type of catalyst depends. • The choice of fuel and oxidant for any FC depends on their electrochemical activity, cost, and easiness of fuel and oxidant delivery and removal of reaction by-products.
  • 17. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Overview of fuel cell types 17 Fuel Cell Electrolyte Qualified Power (W) Working Temperature (◦C) Electrical Efficiency Status Alkaline fuel cell Aqueous alkaline solution (e.g., potassium hydroxide) 10 kW to 100 kW 60-120 35-55 Commercial/Rese arch Direct methanol fuel cell Polymer membrane (ionomer) 100 kW to 1 mW 60-200 20-30 Commercial/Rese arch Phosphoric acid fuel cell Molten phosphoric acid (H3PO4) up to 10 MW 150-220 40 Commercial/Rese arch Molten carbonate fuel cell Molten alkaline carbonate (e.g., sodium bicarbonate NaHCO3) 100 MW 600-650 >50 Commercial/Rese arch Solid oxide fuel cell O 2- -conducting ceramic oxide (e.g., zirconium dioxide, ZrO2) up to 100 MW 700–1000 >50 Commercial/Rese arch Proton exchange membrane fuel cell Polymer membrane (ionomer) (e.g., Nafion® or Polybenzimidazole fiber) 100 W to 500 kW 50-100 35-45 Commercial/Rese arch
  • 18. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Characteristics of Fuel Cells 18 Fuel Cells Attractive Attributes Undesirable Attributes Phosphoric Acid Fuel Cell (PAFC). -Low temperatures suitable for portable device applications -Ability for variable power output -Broad fuel choice -Uses expensive platinum as a catalyst. -Electrolyte is poor conductor at low temperatures Proton Exchange Membrane Fuel Cell (PEM). -Low operating temperature suitable for transportation and portable devices -High power density -Uses expensive platinum as a catalyst -Sensitivity to fuel impurities Molten Carbonate Fuel Cell (MCFC) -High operating temperature improves efficiency for base load power plants. -Not suitable for small-sized applications Solid Oxide Fuel Cell (SOFC) -High operating temperature improves efficiency for base load power plants. -Solid electrolyte improves conductivity - Electrolyte is made from ceramics and solid zirconium oxide that is a rare mineral Alkaline Fuel Cells (AFC) -Low temperature and high fuel-to- electricity efficiency -Requirement of pure hydrogen and allergic to carbon dioxide Direct Methanol Fuel Cells (DMFC). -Eliminates need for fuel reformer drawing hydrogen directly from the anode -Low temperatures suitable for portable devices -Fuel crossing from anode to cathode without producing electricity
  • 19.
  • 20. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel cell Basic Chemistry & Thermodynamics 20
  • 21. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel cell Basic Chemistry & Thermodynamics 21 T (K) ΔH ΔG ΔS Eth (V) 298.15 -286.02 -237.34 -0.16328 1.23 333.15 -284.85 -231.63 -0.15975 1.20 353.15 -284.18 -228.42 -0.15791 1.184 373.15 -283.52 -225.24 -0.15617 1.167 Change of enthalpy, Gibbs Free Energy, and Entropy of hydrogen/oxygen fuel cell reaction with temperature and resulting theoretical cell potential
  • 22. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel cell Basic Chemistry & Thermodynamics 22 • Effect of pressure  For the H2/O2 fuel cell reaction, the Nernst equation becomes:  By introducing Eq (1),  Therefore, cell potential is higher at higher reactant pressures.
  • 23. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Electrochemistry • Electrode kinetics  Electrochemical reactions involve transfer of electrical charge and change of Gibbs energy.  The rate of electrochemical reaction is determined by an activation energy barrier that the charge overcome in moving from electrolyte to electrode or vice versa.  Faraday’s Law: current density is proportional to the charge transferred and the consumption of reactant per unit area:  i = nFj  The consumption of the reactant species is proportional to their surface concentration. For the forward reaction, the flux is:  jf =kfCOx and jb = kbCRd  The net current generated is the difference between the electrons released and consumed:  i =nF (kfCOx − kbCRd)  At equilibrium, the net current should equal zero because the reaction will proceed in both directions simultaneously at the same rate.  The rate which reaction proceed at equilibrium is called the exchange current density. 23
  • 24. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Electrochemistry • Exchange current density – The exchange current density is analogous to the rate constant chemical reaction. – i0 is concentration dependent, is a function of temperature, also a function of catalyst loading and catalyst specific surface area. – The effective exchange current density at any temperature and pressure is given as: 24                    ref c ref r cc ref T T RT E P Laii 1exp Pr 00  Where i0 ref = reference exchange current density (at ref T, P) per unit catalyst surface are,Acm-2 Pt. ac = catalyst specific area. Lc = catalyst loading. Pr = reactant partial pressure, kPa. Pr ref = reference pressure, kPa. γ = pressure coefficient (0.5 to1.0). Ec = activation energy (66 kJ/mol for O2 reduction on Pt). R = gas constant, 8.314 Jmol-1K-1 T = temperature, K. Tref = reference temperatire. 298.15 K
  • 25. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Electrochemistry • Voltage Losses  Activation polarization  Internal Currents and crossovers losses  Ohmic (resistive) losses  Concentration polarization 25
  • 26. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Electrochemistry 26 • Voltage different from equilibrium is need to get the electrochemical reaction going – activation polarization                aacc rcell aactcactraccell i i F RT i i F RT EE VVEEEE ,0,0 ,, lnln  • each H2 molecule that diffuse results in fewer electrons that travel to the external circuit • the losses are minor during fuel cell operation, BUT significant when fuel cell operates at low current densities, or it is at open circuit voltage.        0 , ln i i F RT EE loss rOCVcell 
  • 27. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Electrochemistry 27 • Ohmic losses occur due to the resistance of the flow of ions in the electrolyte and resistance to the flow of electrons. • Concentration polarization occur when a reactant is rapidly consumed at the electrode by the electrochemical reaction so that concentration gradients are established.cieiiii RRRR ,,,          ii i nF RT V L L conc ln
  • 28. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Electrochemistry • Three types of losses in fuel cell. • Activation losses are by far the largest losses at any current density. • The cell voltage is therefore: 28 ohmcconcactaconcactrcell VVVVVEV  )()( i aL aL cL cL aoacoc PTrcell iR ii i nF RT ii i nF RT i i F RT i i F RT EE      )ln()ln()ln()ln( , , , , ,, ,, 
  • 29. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Polarization Curve • A polarization curve is the most important characteristic of a fuel cell and its performance. • It would be useful to see what effect each of the parameters has on the polarization curve shape. 29
  • 30. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Sensitivity of parameters in polarization curve • Effect of transfer coefficient/Tafel slope • Effect of exchange current density • Effect of H2 crossover and internal current loss • Effect of internal resistance • Effect of limiting current density • Effect of operating pressure • Air vs oxygen 30
  • 31. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Sensitivity of parameters in polarization curve Effect of transfer coefficient on fuel cell performance α =0.5 α =1.5 α=1 Effect of exchange current density on fuel cell polarization curve. Effect of cell internal resistance on its polarization curve. Effect of operating pressure on fuel cell polarization curve
  • 32. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Theoretical Fuel Cell Efficiency • Assuming that all of the Gibbs free energy can be converted into electrical energy, the maximum possible efficiency of a fuel cell is: η= ΔG/ ΔH = 237.34/ 286.02 = 83% • Maximum theoretical fuel cell efficiency: η= ΔG/ ΔHLHV = 228.74/ 241.98 = 94.5% • If both ΔG/ ΔH are divided by nF, the fuel cell efficiency may be expressed as a ratio of two potentials: η= (ΔG/nF)/ (ΔH/nF)HHV = 1.23/1.482 = 0.83 • The fuel cell efficiency is always proportional to the cell potential. 32
  • 33. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Basic performance of fuel cell • The overall performance of fuel cell may be evaluated on the basis of the current-voltage diagram. Journal of Power Sources 113 (2003) 37–43 Effect of cell temperature on performance. E-TEK 20% Pt/C; Pt =0:12 mg/cm2.
  • 34. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Basic performance of fuel cell Journal of Power Sources 113 (2003) 37–43 Effect of Pt loading on performance for electrodes made using E-TEK 20% Pt/C, 35/45/45 ˚C.
  • 35. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Implication and Use of Fuel Cell Polarization Curve • Fuel cell polarization curve may be used for diagnostic purposes, as well as for sizing and control of a fuel cell. • From potential-current relationship, other information about the fuel cell may also become available just by rearranging the potential- current data.
  • 36. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Use of polarization curve for fuel cell sizing • H2/air fuel cell polarization curve is given with the followings parameters: α = 1, i0 = 0.001 mAcm-2, Ri = 0.2Ωcm-2 Operating conditions: T =60˚C, P=101.3 kPa Operating point is selected at 0.6 V. Active area is 100 cm2. (a) Calculate nominal power output.
  • 37. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Solution • Power output is Wel = Vcell x i x A Vcell = 0.6 V A =100 cm2 i = ??? • Current density must be determined from the polarization curve. Because no H2 crossover and internal current losses and no limiting current are given, the fuel cell polarization curve may b calculated from: Where Er = 1.482-0.000845T + 0.0000431T ln(PH2PO2 0.5) = 1.482-0.000845 (333.15) + 0.0000431 (333.15) ln (0.21)0.5 =1.189 V R=8.314 Jmol-1K-1 T=333.15K α =1 n = 2 F =96485 C mol-1 Io = 0.001 mAcm-2 Ri = 0.2 Ωcm2 Current cannot be explicitly calculated from the previous equation. 37
  • 38. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Solution ( b) The engineers improved fuel cell performance by improving internal resistance to Ri = 0.15 Ohm-cm2.calculate power gain at 0.6 V • From the new polarization curve, the current density is: I = 1.25 Acm-2 Power output is, Wel = 0.6 x 1.25 x 100 = 75.0 W Power gain is ΔW = 75.0 – 58.2 = 16.8 W or 28.9%
  • 39. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Solution (c) The engineer found out that there was not enough air flow to operate this fuel cell at a higher current density. Calculate the power and efficiency gain if the improved fuel cell is to be operated at the original current density. Vcell = 1.189 – (8.314x333.15)/(1x96485) ln (970/0.001) – 0.97 x 0.15 = 0.648 V New power output is, Wel = 0.648 x 0.97 x 100 = 62.9 W Power gain is, ΔW 62.9 -58.2 = 4.7 W or 8% The efficiency before improvement was: η=Vcell/1.482 = 0.6/1.482 =0.405 The efficiency after improvement is: η=Vcell/1.482 =0.648/1.482 = 0.437
  • 40. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Solution Fuel cell power output is 58.2 = Vcell x i x 100 Another Vcell-i relationship is obtained from the polarization curve: Vcell = 1.189 – (8.314x333.15)/(1x96485) ln (i/0.001) – i x 0.15 Again, by iteration or graphically the solution is: Vcell = 0.666 V i = 875 mACm-2 Noted that point “a” and “d” lay on two different polarization curve but in the same constant power line. The new efficiency is η = Vcell/1.482 = 0.666/1.482 = 0.449 (d) The engineer realized that there is no need for additional power. Calculate the efficiency gain if the improved fuel cell is to be operated at the original power output.
  • 41. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Cost expectations-Fuel cell costs • The US Department of Energy (DOE) had aimed (in 2007) to demonstrate fossil fuelled PEMFC CHP systems for under $750/kW by 2011 and under $450/kW by 2020. • These targets were recently revised to $1200/kW by 2015 and $1000/kW by 2020, for a complete 2 kW natural gas fuelled PEMFC system. • The DOE’s SECA programme established cost targets for 3-10 kW stationary SOFC systems, initially starting at $800/kW by 2005, then falling to $700/kW by 2008 and $400/kW by 2010. • Their cost reduction efforts now aim to demonstrate fuel cell stacks for $175/kW and complete systems for $700/kW
  • 42. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
  • 43. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
  • 44. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014
  • 45.
  • 46. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Type of fuel cells application? 46 There are many different uses of fuel cells being utilized right now. Some of these uses are… •Power sources for vehicles such as cars, trucks, buses and even boats and submarines •Power sources for spacecraft, remote weather stations and military technology •Batteries for electronics such as laptops and smart phones •Sources for uninterruptable power supplies.
  • 47. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Type of fuel cells application?
  • 48. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel cell vehicles by various automakers
  • 49. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Layout of Honda FCX Powertrain
  • 50. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Specification of several fuel cell vehicles
  • 51. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen stations 51
  • 52. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Toyota FCHV-BUS at FC Expo 52 •90 kW PEFC Fuel cell stack: twice •Motor: AC synchronous 80 kW twice •Hydrogen tank: Compressed hydrogen gas 35 MPa / 150 liter, five (version 2002) or seven (version 2005) •Passenger capacity: 63 (included 22 seats)
  • 53. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Residential Fuel Cell 53
  • 54. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Fuel Cell Technologies Forging Cross-industry Collaboration • Google, one of the pilot customers, has a 400- kilowatt installation at its main campus. Over 18 months, the project delivered 3.8 million kilowatt hours of electricity. • Wal-Mart has installed two 400 KW systems at retail locations in Southern California. • Bank of America is putting in a 500 KW installation at a call center in Southern California. • Coke too is putting in a 500 KW installation, at its Odwalla plant in Dinuba, Calif. That fuel cell will run on re-directed biogas and provide up to 30 percent of the plant’s electricity needs. • Cox Enterprises is putting in a 400 KW installation at its KTVU TV station in Oakland, Calif. • E-commerce giant e-Bay is using a 500 KW installation at its San Jose, Calif., facility that will run on biogas. • FedEx has installed five 100 KW Bloom boxes at its package sorting facility in Oakland. 54
  • 55.
  • 56. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Alternative Energy 56 • Increasing of energy demand • Depletion of fossil fuel in near future • Reducing negative impact on environmental Renewable Energy 31 (2006) 719–727
  • 57. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 What is our choices? • Pressing need to find alternative renewable, sustainable and clean energy source.
  • 58. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Alternative energy • Sustainable – ability of an energy source to continue providing energy for a long period of time • Renewable – energy that comes from resources which are continually replenished • Clean ‐ does not pollute the atmosphere when used/produced
  • 59. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen properties • Gaseous, odorless, colorless, tasteless, flammable, explosive • Bonds with many other elements • Seldom found in pure form in nature • Liquid at -253 ˚C (20 K) • Not an energy source, it is an energy carrier/store
  • 60. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen safety • Hydrogen Vehicle Safety. – The Ford Motor Company, in their report to the US Department of Energy included this statement: “Overall, we judge the safety of a hydrogen FCV system to be potentially better than the demonstrated safety record of gasoline or propane, and equal to or better than that of natural gas.” 60
  • 61. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen safety 61 Hydrogen Vehicle Gasoline Vehicle Hydrogen Vehicle Gasoline Vehicle Hydrogen Vehicle Gasoline Vehicle One minute after ignition; hydrogen fire nearly extinguished The pictures below were taken 3 seconds after ignition The following pictures compare hydrogen and gasoline fires from an experiment conducted at the University of Miami. The car on the left contained high pressure hydrogen tanks with 175,000 btu of energy and the car on the right had a conventional gasoline tank with just five pints of gasoline or about 70,000 btus of energy. Spark plugs were installed outside both vehicles to ignite a leaking hydrogen tank and a leaking gasoline line.
  • 62. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen Production Paths 62
  • 63. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen production methods • Main methods -Thermal -Electrochemical -Biological • Others -Chemical reaction -etc Primary method Process Source/Feed stock Energy Thermal Stream reforming Natural gas High temperature steam (autothermal) Thermochemical water splitting Water High temperature heat from nuclear reactor Gasification Coal, Biomass High temperature (& pressure) steam & oxygen Pyrolysis Biomass Moderately high temeprature Electrochemcal Electrolysis Water Electricity from solar, wind, hydro & nuclear Photoelectrochemi cal Water Direct from sunlight Biological Photobiological Water & algae strains Direct sunlight Anaerobic/ferm entation Biomass & microorganis m Food source Anaerobic degistion Biomass High temperature heat Fermentative microorganisms Biomass High temperature heat
  • 64. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen production technologies Steam methane reforming : • widely used in the chemical and refining industries. • Considered the cheapest way of producing hydrogen. • Reforming involves the reaction of desulphurized natural gas with high- temperature steam over a Ni-based catalyst. • This produces syngas-mainly a mixture of H2 and CO. • The CO is then converted to H2 and CO2 via a water gas shift reaction. • High purity (up to 99.99%) H2 is separated using pressure swing adsorption method.
  • 65. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen production technologies Coal gasification: • well-established commercial technology • competitive with SMR only where oil and/or natural gas are expensive. • coal could replace natural gas and oil as the primary feedstock for hydrogen production, since it is so plentiful in the world.
  • 66. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen production technologies Electrolysis of water : • Water molecules can be separated using electricity. But we use electricity to produce hydrogen to produce electricity again. • Pure water is in many places a scarce resource. • The electricity for the electrolysis needs to be produced and the water needs to be purified (soft de-ionized water is needed). • Reaction: • Electricity can be obtained at a large scale from nuclear reactors but the hydrogen needs to be stored and transported, and nuclear fuel is not a renewable source of energy. • At a VERY small scale wind or solar power can be used, but this energy is available only when there is wind or sunlight.
  • 67. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen production technologies Biomass gasification and pyrolysis: • Provide two ways to produce H2 from biomass. • The processes can be adapted to a range of feedstock: switch grass, plant scraps, garbage, willow, sugar cane waste. • Both techniques are followed by a reforming stage. • Gasifier may be heated indirectly and directly. • With pyrolysis, biomass is rapidly heated in the absence of O2, the vapors are then condensed to form pyrolysis oil. • This pyrolysis oil can be used as feedstock for H2 production.
  • 68. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Conversion of Biomass Pyrolysis Gasification Combustion No oxygen With oxygen (partial oxidation) With oxygen (complete oxidation) Organic material + heat -> charcoal +oil +gases Organic material + O2 +H2O-> H2 +CO2 +CO+ others Organic material + O2-> CO2 +H2O Slow &Low (<450ºC) -Max char 35%wt Intermediate (450-500ºC) -Typical 10-15% has. 20-30% char, 45-65% oil Fast & high (>500ºC) -(>550ºC – mas oil 70%) -(>600ºC - max gas 80%) High (>800ºC) Low (start 200‐300ºC) (>1000ºC) Gas-Syngas CO2 H2O CO CH4 etc Heat Solid-char Liquid-oil Hydrogen Transfrom
  • 69. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen Storage Alternatives • Compressed Gas Storage • Solid State Storage • Liquid Hydrogen Storage
  • 70. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Compressed Gas Storage
  • 71. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 High Pressure Gas • High-pressure hydrogen is stored in cylinders. • Conventional cylinders – cylindrical shaped sidewall section with hemispherical end domes. • Conformal Cylinders – Use multiple cylinders in tandem and distort the cylindrical shape in order to increase the usable volume.
  • 72. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Hydrogen Cylinders
  • 73. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Metal Hydrides • Principle used is that some metals readily absorb gaseous hydrogen under conditions of high pressure and moderate temperature to form metal hydrides • These metal hydrides release the hydrogen gas when heated at low pressure and relatively high temperature
  • 74. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Metal Hydrides • There are many types of specific metal hydrides • Primarily they are based on metal alloys of magnesium, nickel, iron and titanium • They are divided into: • high hydrogen desorption temperature • low hydrogen desorption temperature
  • 75. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Metal Hydrides • High hydrogen desorption temperature • Less expensive • Holds more hydrogen • Requires significant amount of heat to release hydrogen • Low hydrogen desorption temperature • Heat from an engine is sufficient to release hydrogen • Sometime in this case it releases hydrogen at ambient temperatures • It needs to be pressurized to overcome this problem
  • 76. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Metal Hydrides
  • 77. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Metal Hydrides Advantages • Hydrogen becomes part of the chemical structure of the metal itself and therefore does not require high pressures or cryogenic temperatures for operation • Since hydrogen is released from the hydride for use at low pressure, hydrides are the most intrinsically safe of all methods of storing hydrogen
  • 78. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Metal Hydrides Disadvantages • They have low mass energy density • Best metal hydrides contain only 8% hydrogen by weight • very heavy and expensive • Metal hydride storage systems can be up to 30 times heavier and ten times larger than a gasoline tank with the same energy content • They must be charged with only very pure hydrogen • If they become contaminated there is loss of capacity
  • 79. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Liquid Hydrogen Storage Liquid hydrogen storage tank (850,000 gallons) at NASA KSC
  • 80. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Liquid Hydrogen • The storage of liquefied cryogenic gases is a proven and tested technology. • Hydrogen was first liquefied by J. Dewar in 1898. • In liquid form, hydrogen can only be stored under cryogenic temperatures.
  • 81. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Advantages • Liquid hydrogen: high energy/mass ratio, three times that of gasoline. • It is the most energy dense fuel in use (excluding nuclear reactions fuels), which is why it is employed in all space programs • Compared with compressed hydrogen, liquid hydrogen has much lower storage pressure  the risk caused by high pressure may be reduced to some extent. • Liquid hydrogen (LH2) tanks can store more hydrogen in a given volume than compressed gas tanks.
  • 82. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Disadvantages • Requires extremely low temperatures of -423 F/- 2520 C. • Boil-off losses / vaporization of hydrogen due to heat leakage constitute a major disadvantage. • A highly sophisticated and expensive production and processing system is necessary in order to minimize losses caused by diffusion, evaporation and impurity. • Evaporation losses on todays tank installations are between 0.3 and 3% per day.
  • 83. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Summary of H2 Storage
  • 84. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Cost expectations-Hydrogen production costs • H2 production from natural gas by steam reforming methods is well established. • At low (pipeline) pressure, it is about 1.0 US$kg-1 (based on inexpensive natural gas, assumed at 1.5 US$ GJ-1). • Simbeck and Chang (2002) estimate the delivered H2 cost from biomass waste is about 2.5 US$kg-1. • Conventional small-scale electrolyzer H2 cost have been estimated as 8-12 US$kg-1. • Larger unit using surplus wind power may attain a cost down to 2 US$kg-1 • The H2 cost based on coal gasification is estimated as over 12 US$kg-1
  • 85. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Cost and performance characteristics of various hydrogen production Process Energy Required (kWh/Nm3) Ideal Energy Required (kWh/Nm3) Practical Status of Tech. Efficiency [%] Costs Relative to SMR Steam methane reforming (SMR) 0.78 2-2.5 mature 70-80 1 Methane/ NG pyrolysis R&D to mature 72-54 0.9 H2S methane reforming 1.5 - R&D 50 <1 Landfill gas dry reformation R&D 47-58 ~1 Partial oxidation of heavy oil 0.94 4.9 mature 70 1.8 Naphtha reforming mature Steam reforming of waste oil R&D 75 <1 Coal gasification (TEXACO) 1.01 8.6 mature 60 1.4-2.6 Partial oxidation of coal mature 55 Steam-iron process R&D 46 1.9 Chloralkali electrolysis mature by-product Grid electrolysis of water 3.54 4.9 R&D 27 3-10 Solar & PV-electrolysis of water R&D to mature 10 >3 High-temp. electrolysis of water R&D 48 2.2 Thermochemical water splitting early R&D 35-45 6 Biomass gasification R&D 45-50 2.0-2.4 Photobiological early R&D <1 Photolysis of water early R&D <10 Photoelectrochemical decomp. of water early R&D Photocatalytic decomp. of water early R&D
  • 86. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Cost of various hydrogen production technologies Technology Cost range (US$ (2000)/GJH2 Additional cost of CO2 capture Comments SMR, large-scale (>1000MW) SMR, small-scale (<5MW) 5.25-7.26 11.50-40.40 $7.26 cost increases to $8.59/GJ with CCS Prohibitive Cost highly dependent on natural gas prices. Transitional technology. Cost highly dependent on natural has prices, plant size and purity of H2 required. Coal gastification 5.4-6.8 Average of 11% Coal price more stable and predicatable than natural gas. Biomass gasification (>10MW) 7.54-32.61 (av.14.31) Not given (with CCS technology, would become carbon negative) Size ranges from 25 to 303 MW and affects cost.
  • 87. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Cost of various hydrogen production technologies Technology Cost range (US$ (2000)/GJH2 Additional cost of CO2 capture Comments Biomass pyrolysis (>10MW) 6.19-14.98 Not given (with CCS technology would become carbon negative) Size ranges form 36 to 150MW; cost redued by sale of co-products Electrolysis, Large scale (>1MW) 11-75 Emissions (and CCS options) depend on source of electricity Size ranges from 2 to 376MW, but little effect on cost; cost very dependent on assumed price of electricity Electrolysis, small- scale (<1MW) 28-133 Emissions (and CCS options) depend on source of electricity Size ranges from 0.03 to 0.79MW, cost very size- dependent.
  • 88. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Wind/ Hydrogen Projects • Greece  RES2H2 Project • Spain  RES2H2 Project  ITHER Project • Canada Ramea Island Prince Edward Island • United Kingdom HARI Project PURE Project • United Stated  Basin electric, Wind-to-Hydrogen Energy Pilot Project  National RE Lab and Xcel Energy, Wind-to-Hydrogen Project
  • 89. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 PURE Project • The project aims to demonstrate how wind power and hydrogen technology can be combined to meet the energy needs of a remote rural industrial estate. • PURE was conceived to test and demonstrate safe and effective long-term use and storage of hydrogen produced by renewable energy using wind-powered electrolysis of water, and to regenerate the stored energy into electric energy with a fuel cell. • The key components of the system are:  Wind turbines: Two 15 kW (Proven Ltd)  Electrolyzer: 15 kW alkaline operating at 55 bar (AccaGen SA)  Hydrogen storage: 44 Nm3 in H2 cylinders  PEM fuel cell: 5 kW (Plug Power). • The electrolyzer section consists of an AccaGen electrolyzer unit assembled with advanced cells specifically designed and manufactured by AccaGen SA for wind application, capable of operating up to 55 bar.
  • 90. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Basin Electric, Wind-to-Hydrogen Energy Pilot Project • this project was to research the application of hydrogen production from wind energy, allowing for continued wind energy development in remote wind-rich areas and mitigating the necessity for electrical transmission expansion. • The report completed on August 2005 found that the proposed hydrogen production system would produce between 8,000 kg and 20,000 kg of hydrogen annually. • The cost of the hydrogen produced ranged from $20 to $10 per kilogram. • The hydrogen-production system utilizes a bipolar alkaline electrolyzer nominally capable of producing 30 Nm3/h (2.7 kg/h).
  • 91. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Future energy landscape 91
  • 92. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 Furture Energy Landscape
  • 93. Loh Kee Shyuan 7th Asian School on Renewable Energy, Puri Pujangga UKM, Malaysia, 16th-20th June 2014 93 THANK YOU ksloh@ukm.edu.my