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This ready reference is unique in collating in one scientifically precise and comprehensive handbook the widespread data on what is feasible and realistic in modern fuel cell technology.
Edited by one of the leading scientists in this exciting area, the short, uniformly written chapters provide economic data for cost considerations and a full overview of demonstration data, covering such topics as fuel cells for transportation, fuel provision, codes and standards.
The result is highly reliable facts and figures for engineers, researchers and decision makers working in the field of fuel cells.
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Cover
Related Titles
Title Page
Copyright
Preface
Part I: Transportation
I-1 Propulsion
I-1.1 Benchmarks and Definition of Criteria
1: Battery Electric Vehicles
References
2: Passenger Car Drive Cycles
Abstract
2.1 Introduction
2.2 Drive Cycles for Passenger Car Type Approval
2.3 Drive Cycles from Research Projects
2.4 Drive Cycle Characteristics
2.5 Graphic Representation of Selected Drive Cycles
2.6 Conclusion
References
3: Hydrogen Fuel Quality
Abstract
3.1 Introduction
3.2 Hydrogen Fuel
3.3 Fuel Quality Effects
3.4 Fuel Quality for Fuel Cell Vehicles
3.5 Single Cell Tests
3.6 Field Data
3.7 Fuel Quality Verification
3.8 Conclusion
References
4: Fuel Consumption
Abstract
4.1 Introduction
4.2 Hydrogen Production
4.3 Hydrogen Packaging
4.4 Hydrogen Consumption in FCEVs
4.5 Conclusion
References
I-1.2 Demonstration
I-1.2.1 Passenger Cars
5: Global Development Status of Fuel Cell Vehicles
Abstract
5.1 Introduction
5.2 Update on Recent Activities of Car Manufacturers
5.3 Key Data and Results from Demonstration Programs
5.4 Technical Data of Fuel Cell Vehicles
5.5 Conclusions
References
6: Transportation – China – Passenger Cars
Abstract
6.1 Introduction
6.2 National R&D Strategy (2011–2015)
6.3 Government Policy
6.4 Published Technical Standards
6.5 Demonstrations
6.6 Commercialization – Case of SAIC Motor
6.7 Conclusions
References
7: Results of Country Specific Program – Korea
Abstract
7.1 Introduction
7.2 FCV Demonstration Program
7.3 Summary
8: GM HydroGen4 – A Fuel Cell Electric Vehicle based on the Chevrolet Equinox
Abstract
8.1 Introduction
8.2 Technology
8.3 Conclusions
Acknowledgments
References
I-1.2.2 Buses
9: Results of Country Specific Programs – USA
Abstract
9.1 Introduction
9.2 FCEB Descriptions
9.3 SunLine Advanced Technology Fuel Cell Electric Bus
9.4 Zero Emission Bay Area Program
9.5 SunLine American Fuel Cell Bus
9.6 Conclusion
References
I-1.3 PEM fuel cells
10: Polymer Electrolytes
Abstract
10.1 Introduction
10.2 Membrane Properties
10.3 Conclusions
References
11: MEAs for PEM Fuel Cells
Abstract
11.1 Introduction
11.2 MEA Basic Components (PEMs, Catalysts, GDLs and Gaskets)
11.3 MEA Performance, Durability, and Cost Targets for Transportation
11.4 MEA Robustness and Sensitivity to External Factors
11.5 Technology Gaps
11.6 Conclusion
References
12: Gas Diffusion Layer
Abstract
12.1 Introduction
12.2 Macroporous Substrate
12.3 Microporous Layer
12.4 Characterization of GDL
12.5 Conclusion
References
13: Materials for PEMFC Bipolar Plates
Abstract
13.1 Introduction
13.2 Composite BP Materials
13.3 Metallic BP Materials
Acknowledgments
References
14: Single Cell for Proton Exchange Membrane Fuel Cells (PEMFCs)
Abstract
14.1 Introduction
14.2 Main Components of a Single Cell for a PEMFC
14.3 Assembly of a Single Cell
14.4 Measurement of a Single Cell Performance
14.5 Conclusions
References
I-1.4 Hydrogen
I-1.4.1 On board storage
15: Pressurized System
Abstract
15.1 Introduction
15.2 High Pressure Storage System
15.3 Cost
15.4 Conclusions
References
16: Metal Hydrides
16.1 Metal Hydrides as Hydrogen Storage Media
16.2 Classes of Metal Hydrides
16.3 How Metal Hydrides Could Be Improved
References
17: Cryo-Compressed Hydrogen Storage
Abstract
17.1 Introduction
17.2 Thermodynamic Principles
17.3 System Design and Operating Principles
17.4 Validation and Safety
17.5 Summary
References
I-1.4.2 On board safety
18: On-Board Safety
Abstract
18.1 Introduction
18.2 High Pressure Fuel Container System
18.3 Hydrogen Refueling Requirements and Safety
18.4 Conclusions
References
I-2 Auxiliary power units (APU)
19: Fuels for APU Applications
Abstract
19.1 Introduction
19.2 Diesel Fuel
19.3 Jet Fuel
19.4 Other Fuels
19.5 Conclusion
References
20: Application Requirements/Targets for Fuel Cell APUs
Abstract
20.1 Introduction
20.2 DOE Technical Targets
References
21: Fuel Cells for Marine Applications
Abstract
21.1 Introduction
21.2 Possible Fuel Cell Systems for Ships
21.3 Maritime Fuel Cell Projects
21.4 Development Goals for Future Systems
21.5 Conclusions
References
22: Reforming Technologies for APUs
Abstract
22.1 Introduction
22.2 Guideline
Appendix 22.A
Abbreviation
List of Symbols
Definitions
References
23: PEFC Systems for APU Applications
Abstract
23.1 Introduction
23.2 PEFC Operation with Reformate
23.3 Application Concepts
23.4 System Design
23.5 System Efficiency
23.6 System Test
23.7 Conclusion
References
24: High Temperature Polymer Electrolyte Fuel Cells
Abstract
24.1 Introduction
24.2 Operating Behavior of Cells and Stacks
24.3 System Level
References
25: Fuel Cell Systems for APU. SOFC: Cell, Stack, and Systems
References
Part II: Stationary
26: Deployment and Capacity Trends for Stationary Fuel Cell Systems in the USA
Abstract
26.1 Fuel-Cell Backup Systems
26.2 Fuel-Cell Combined Heat and Power and Electricity
References
27: Specific Country Reports: Japan
Abstract
27.1 Introduction
27.2 Start of the Sales of Residential Fuel Cell Systems
27.3 Market Growth of the Ene-Farm
27.4 Technical Development of the Ene-Farm
27.5 Sales of the Ene-Farm for Condominiums
27.6 Conclusions
References
28: Backup Power Systems
Abstract
28.1 Introduction
28.2 Application and Power Levels
28.3 Advantages
28.4 Fuel Choice
28.5 Product Parameters
28.6 Economics
28.7 Conclusion
References
29: Stationary Fuel Cells – Residential Applications
Abstract
29.1 Introduction
29.2 Key Characteristics
29.3 Technical Performance
29.4 Economic and Market Status
29.5 Conclusions
References
30: Fuels for Stationary Applications
Abstract
30.1 Introduction
30.2 Natural Gas
30.3 Biogas, Landfill Gas, and Biomethane
30.4 (Bio)ethanol
30.5 Hydrogen
References
31: SOFC: Cell, Stack and System Level
Abstract
31.1 Introduction
31.2 Cell Concepts and Materials
31.3 Cell Designs
31.4 Stack Concepts
31.5 Stationary Systems
31.6 Performance and Durability Parameters
References
Part III: Materials Handling
32: Fuel Cell Forklift Systems
Abstract
32.1 Introduction
32.2 Forklift Classification
32.3 Load Profile of Horizontal Order Pickers
32.4 Energy Supply for Forklifts
32.5 Systems Setup and Hybridization
32.6 Cost Comparison of Different Propulsion Systems for Forklifts
References
33: Fuel Cell Forklift Deployment in the USA
Abstract
33.1 Fuel Cell-Powered Material Handling Equipment
References
Part IV: Fuel Provision
34: Proton Exchange Membrane Water Electrolysis
Abstract
34.1 Introduction
34.2 Bibliographic Analysis of PEM Electrolysis versus Water Electrolysis
34.3 Electrocatalysts Used in PEM Water Electrolysis
34.4 Anode Supports for PEM Water Electrolysis
34.5 Membranes for PEM Electrolysis
34.6 Stack and System Costs in PEM Electrolysis
34.7 PEM Electrolysis Systems in Comparison with Competing Technologies
References
35: Power-to-Gas
Abstract
35.1 Introduction
35.2 Main Components and Process Steps
35.3 Transport and Application of H2 and CH4
35.4 Current Developments: Pilot Plants
35.5 Conclusion
References
Part V: Codes and Standards
36: Hydrogen Safety and RCS (Regulations, Codes, and Standards)
Abstract
36.1 Introduction
36.2 Hydrogen Safety
Non-Metallic Materials
36.3 Hydrogen Regulations, Codes, and Standards (RCS) International Activities
36.4 Conclusions
Acknowledgments
References
Index
EULA
Table 1.1
Table 1.2
Table 1.3
Table 1.4
Table 2.1
Table 3.1
Table 3.2
Table 3.3
Table 3.4
Table 4.1
Table 4.2
Table 4.3
Table 5.1
Table 5.2
Table 5.3
Table 5.4
Table 5.5
Table 5.6
Table 5.7
Table 5.8
Table 5.9
Table 5.10
Table 5.11
Table 5.12
Table 5.13
Table 5.14
Table 5.15
Table 5.16
Table 6.1
Table 6.2
Table 6.3
Table 7.1
Table 7.2
Table 7.3
Table 7.4
Table 8.1
Table 8.2
Table 9.1
Table 9.2
Table 9.3
Table 9.4
Table 10.1
Table 10.2
Table 10.3
Table 10.4
Table 10.5
Table 10.6
Table 11.1
Table 11.2
Table 11.3
Table 11.4
Table 11.5
Table 12.1
Table 12.2
Table 12.3
Table 12.4
Table 12.5
Table 12.6
Table 13.1
Table 14.1
Table 15.1
Table 15.2
Table 15.3
Table 15.4
Table 16.1
Table 17.1
Table 17.2
Table 17.3
Table 17.4
Table 17.5
Table 17.6
Table 18.1
Table 18.2
Table 18.3
Table 19.1
Table 19.2
Table 19.3
Table 19.4
Table 19.5
Table 19.6
Table 19.7
Table 19.8
Table 19.9
Table 20.1
Table 21.1
Table 21.2
Table 21.3
Table 21.4
Table 22.1
Table 22.2
Table 22.3
Table 22.4
Table 22.5
Table 22.6
Table 22.7
Table 23.1
Table 23.2
Table 24.1
Table 24.2
Table 24.3
Table 24.4
Table 25.1
Table 26.1
Table 26.2
Table 26.3
Table 26.4
Table 27.1
Table 29.1
Table 29.2
Table 29.3
Table 29.4
Table 29.5
Table 29.6
Table 30.1
Table 30.2
Table 30.3
Table 30.4
Table 30.5
Table 30.6
Table 31.1
Table 31.2
Table 31.3
Table 31.4
Table 31.5
Table 31.6
Table 31.7
Table 31.8
Table 31.9
Table 31.10
Table 32.1
Table 32.2
Table 32.3
Table 32.4
Table 32.5
Table 32.6
Table 32.7
Table 33.1
Table 33.2
Table 33.3
Table 34.1
Table 34.2
Table 34.3
Table 34.4
Table 34.5
Table 34.6
Table 34.7
Table 35.1
Table 35.2
Table 35.3
Table 35.4
Table 36.1
Table 36.2
Figure 1.1
Figure 1.2
Figure 1.3
Figure 1.4
Figure 2.1
Figure 2.2
Figure 3.1
Figure 6.1
Figure 6.2
Figure 6.3
Figure 6.4
Figure 7.1
Figure 7.2
Figure 8.1
Figure 8.2
Figure 8.3
Figure 8.4
Figure 8.5
Figure 8.6
Figure 9.1
Figure 9.2
Figure 9.3
Figure 9.4
Figure 9.5
Figure 9.6
Figure 9.7
Figure 9.8
Figure 9.9
Figure 11.1
Figure 14.1
Figure 14.2
Figure 15.1
Figure 15.2
Figure 17.1
Figure 17.2
Figure 17.3
Figure 17.4
Figure 17.5
Figure 18.1
Figure 18.2
Figure 18.3
Figure 18.4
Figure 21.1
Figure 22.1
Figure 22.2
Figure 22.3
Figure 22.4
Figure 23.1
Figure 24.1
Figure 24.2
Figure 24.3
Figure 24.4
Figure 25.1
Figure 25.2
Figure 25.3
Figure 25.4
Figure 25.5
Figure 26.1
Figure 26.2
Figure 26.3
Figure 26.4
Figure 26.5
Figure 26.6
Figure 26.7
Figure 26.8
Figure 26.9
Figure 27.1
Figure 27.2
Figure 27.3
Figure 27.4
Figure 28.1
Figure 29.1
Figure 29.2
Figure 29.3
Figure 29.4
Figure 31.1
Figure 31.2
Figure 31.3
Figure 32.1
Figure 32.2
Figure 32.3
Figure 32.4
Figure 33.1
Figure 34.1
Figure 34.2
Figure 34.3
Figure 35.1
Figure 35.2
Figure 35.3
Figure 35.4
Figure 35.5
Figure 36.1
Cover
Table of Contents
Begin Reading
Part 1
Chapter 1
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Gao, F., Blunier, B., Miraoui, A. (eds.)
2012
Print ISBN: 978-1-848-21339-5
Bagotsky, V.S.
2 Edition
2012
Print ISBN: 978-1-118-08756-5
Jiang, S.P., Yan, Y. (eds.)
2013
Print ISBN: 978-3-527-33041-6
Stolten, D. (ed.)
2010
Print ISBN: 978-3-527-32711-9
Stolten, D., Emonts, B. (eds.)
2012
Print ISBN: 978-3-527-33012-6
Edited by Detlef Stolten, Remzi C. Samsun and Nancy Garland
All books published by Wiley-VCH are carefully produced. Nevertheless, authors, editors, and publisher do not warrant the information contained in these books, including this book, to be free of errors. Readers are advised to keep in mind that statements, data, illustrations, procedural details or other items may inadvertently be inaccurate.
Library of Congress Card No.: applied for
British Library Cataloguing-in-Publication DataA catalogue record for this book is available from the British Library.
Bibliographic information published by the Deutsche NationalbibliothekThe Deutsche Nationalbibliothek lists this publication in the Deutsche Nationalbibliografie; detailed bibliographic data are available on the Internet at <http://dnb.d-nb.de>.
© 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Boschstr. 12, 69469 Weinheim, Germany
All rights reserved (including those of translation into other languages). No part of this book may be reproduced in any form — by photoprinting, microfilm, or any other means — nor transmitted or translated into a machine language without written permission from the publishers. Registered names, trademarks, etc. used in this book, even when not specifically marked as such, are not to be considered unprotected by law.
Print ISBN: 978-3-527-33240-3ePDF ISBN: 978-3-527-69389-4ePub ISBN: 978-3-527-69391-7Mobi ISBN: 978-3-527-69390-0oBook ISBN: 978-3-527-69392-4
Fuel cell technology made substantial progress in the last decade, although this was not always reflected in the public mind due to unrealistically high expectations and partial overselling in the previous decade. The automotive industry for one made strong and steady progress and is edging ever closer to bringing fuel cell-based vehicles to market.
Hyundai and Toyota produced cars using the world's first dedicated manufacturing lines for fuel cell vehicles. In the stationary sector, fuel cells also became more prominent through the deployment of over 100,000 residential systems in Japan, amongst other countries, as well as portable applications (the latter, however, remain focused on special market segments and niches).
At this stage, systems analysis with respect to the widespread implementation of fuel cells becomes highly important, particularly in this case. For given that fuel cells constitute a cleaner and more efficient energy conversion solution, they typically substitute existing technologies. Hence, a comparative analysis of performance, longevity and costs is paramount.
This book compiles cutting edge research to comprehensively convey the current status of the technology. It is intended as a data reference book for people familiar with energy analyses and/or fuel cells and hydrogen.
I-1 Propulsion
I-1.1 Benchmarks and definition of criteria
Bruno Gnörich and Lutz Eckstein
RWTH Aachen University, Institut für Kraftfahrzeuge, Steinbachstraße 7, 52074 Aachen, Germany
Keywords: battery electric vehicles; concept car; electric machines; hydrogen fuel cell electric vehicles; Li-ion batteries
In the early years of motor vehicle history, the most frequently used propulsion system was an electric drivetrain with batteries as energy storage. Power sockets were more common than petrol stations. From the 1920s, the increasing density of fueling stations made battery electric vehicles less desirable due to the longer recharging times.
It took many decades before the aspect of emissions and scarcity of primary energy resources (re)surfaced and, as of today, a significant number of series production vehicles from major car manufacturers are available to end customers. E-mobility stakeholders also stress the potential linkage of battery electric vehicles and the energy sector to create a smart grid where vehicles could act as balancing loads when plugged into the charging pole.
In general terms, and with electricity being a secondary energy carrier just like hydrogen, this underlines the necessity to assess the well-to-wheel efficiency, emissions, and sustainability of such drivetrains.
Figure 1.1 illustrates a simplified overview of the well-to-wheel energy conversion for the main propulsion technologies, with focus on the battery electric vehicle (BEV). Electricity can be produced from any of the primary or secondary sources, including hydrogen.
Figure 1.1 Energy conversion pathways for motor vehicles with focus on BEVs [1].
It becomes clear that electric vehicles benefit from the versatile electricity pathways, making them in theory the most sustainably propelled types of vehicles. This includes battery and hydrogen fuel cell electric vehicles (FCEV).
These differ only by the delivery of electricity to the traction motor(s), and this synergy is beneficial when creating BEVs and FCEVs with identical motors.
Battery electric vehicles have several benefits over conventional vehicles. They feature low noise emissions and do not produce local pollutants like NOx, particulate matter, or other toxic substances and gases. They therefore are predestined for urban traffic, where the limited driving range does not obstruct adequate usage.
The average driving range of any passenger vehicle in Germany in 2012 was 49.2 km per day, over an average of 3.9 journeys [1]. The power requirement in urban traffic is approximately 10–15 kWmech, which is significantly lower than the requirement for extra-urban traffic (>30 kW at 100 km h−1). The main bottleneck in this market is the lack of acceptance of a vehicle with limited driving range and high purchase costs.
The only full-range BEV as of early 2015 is the Tesla Model S with its large 85 kWh battery and a range of up to 500 km. Tesla has used a combination of conventional Li-ion battery technology and powerful motors in a very aerodynamic body (cd = 0.24) to create a well-received vehicle in the luxury car segment. It mainly addresses markets with government subsidies, substantial CO2 emissions taxation, or good coverage of quick-charging infrastructure, Tesla's Supercharger stations.
Several BEVs are so-called purpose-designed vehicles that have been specifically developed as electric vehicles and that are not derived from an internal combustion engine (ICE) vehicle (Table 1.1). Tesla's Model S aside, such vehicles are mostly in the micro to compact car segment, like the Peugeot iOn, BMW i3, or Nissan Leaf. Conversion design examples include the Volkswagen e-Golf and the Smart fortwo electric drive. In the case of newly developed vehicles such as the Mercedes-Benz B-class, different propulsion options have been considered from the start of the development process, using one platform for conventional versions and an adapted platform for natural gas powered and electric versions.
Table 1.1 Series production battery electric vehicles. (Source: manufacturers.)
Parameter
Smart fortwo ed
Peugeot iON
Nissan Leaf
BMW i3
VW e-Golf
Mercedes B-Class
Tesla Model S
Vehicle data
Class
Sub-compact
Compact
Compact
Lower middle
Lower middle
Lower middle
Luxury class
Price (2015) (€)
23 680
29 393
23 790
34 950
34 900
27 102
85 900
Driving performance
Range (km)
145
150
200
190
190
200
502
Consumption (kWh per 100 km)
15.1
15.9
12.4
12.9
12.7
16.6
18.1
0 to 100 km h
−1
(s)
11.5
15.9
11.3
7.2
10.4
7.9
4.6
Maximum speed (km h
−1
)
125
130
145
150
140
160
250
Battery
Type
Lithium ion
Lithium ion
Lithium ion
Lithium ion
Lithium ion
Lithium ion
Lithium ion
Capacity (kWh)
17.6
16
24
18.8
24.2
28
85
Max. charging power (kW)
22
62.5
6.6
4.6
17.6
11
120
Electric motor
Type
PSM
PSM
SM
HSM
PSM
SM
ASM
Nominal power (kW)
55
49
80
125
85
132
2 × 384
Torque (Nm)
130
196
280
250
270
340
491
In general, electric drivetrains have a moderate amount of drivetrain components and a straightforward structure. The novel components are the battery system and the electric motor. Furthermore, auxiliary components need adjusting such as the steering and braking system as well as the heating and cooling systems (thermal management).
The latter has become a vital aspect of drivetrain development and aims to combine energy demand analyses and efficiency optimization across all on-board energy requirements. Examples include the use of thermal inertias of components such as the battery, the passenger compartment, or thermochemical storage systems and to include thermal management in the vehicle energy management system.
Battery electric vehicles use high-energy batteries to maximize driving range. Today, almost all BEVs use Li-ion batteries with energy densities of up to 150 Wh kg−1. For example, the Volkswagen e-Golf has a battery with a density of 140 Wh kg−1 (230 Wh l−1) and a total energy capacity of 24 kWh at 323 V [2]. This results in a total driving range of up to 190 km. The driving range is influenced by several factors, like driving resistance (e.g., tyre pressure, load, topography), driving speed pattern (acceleration, velocity), and battery specific parameters like temperature and its state of health. The aim to increase the energy density is therefore a high priority. From an automotive point of view, the specifications must also cover costs, thermal management, durability, and end-of-life aspects.
Notable technologies today are mostly based on lithium ion batteries but also on nickel-metal-hydride batteries (e.g., Toyota) and double layer capacitors (supercapacitors) for use in high-power applications (e.g., KERS, heavy duty) (Table 1.2). In BEVs, they could be used as an optional add-on for high-performance applications.
Table 1.2 Specifications of different battery types used in electric vehicles (BEV/HEV). (Source: manufacturers.)
NiMH
Li-ion
Li-ion
Supercapacitor
Manufacturer
PEVE
Hitachi
Sanyo
Maxwell
Shape
Prismatic
Cylindrical
Prismatic
Cylindrical
Cathode
Ni(OH)
2
LiMn
2
O
4
LiNiMnCo
Graphite
Anode
Rare earth AB
5
Amorphous carbon
Amorphous carbon
Graphite
Cell capacity (Ah)
6.5
4.4
25
0.56
Cell voltage (V)
1.2
3.3
3.6
2.7
Energy density (Wh kg
−1
)
46
56
76
5.4
Power density (Wh kg
−1
)
1300
3000
600
6600
Operation temperature (°C)
−20 to +50
−30 to +50
−30 to +50
−40 to +65
Market
Toyota HEV
GM HEV
VW BEV
Faun HEV
Electrochemical high temperature cells (e.g., ZEBRA) are no longer considered for most applications in passenger cars due to their critical thermal management. Apart from capacitors, all automotive battery technologies are secondary cells with reversible electrochemical energy conversion, an essential prerequisite for electric cars.
In principle, all of the energy storage technologies presented here are feasible for traction application in road vehicles. Due to their limited energy and power density, lead-acid batteries only play a role in niche applications and two-wheel vehicles.
Electric machines are electromechanical converters, where energy conversion takes place by means of a force on the mechanical and induced voltage on the electrical side. In principle, every electric machine can be operated as motor or as a generator. For every electric machine, operational limits for speed, torque, and power exist (Figure 1.2). A distinction must be made between nominal values and maximum values. Nominal values (MNom, PNom) can be applied permanently; maximum values (Mmax, Pmax) only for a short period, otherwise mechanical and thermal failure may occur and affect the durability of the machine [1].
Figure 1.2 Operating range of electric machines [1].
Operation of electric machines can be divided into two areas: base load range and field weakening range. In the base load range the machine is capable of delivering maximum torque (MNom or MMax) at all speeds from standstill. Nominal power is then available at nominal speed (nNom):
For a permanent operation the nominal power must not be exceeded. As a result, the output torque decreases with higher speeds:
Equation (1.2) describes the area of constant power, achieved by a weakening of the magnetic field.
DC machines use DC current to induce an electromagnetic field to drive the rotor, whereas AC machines are driven by alternating current. Today, almost all machines used in electric vehicles are synchronous or asynchronous three-phase AC machines due to their high efficiency (Table 1.3). High efficiency can also be achieved with permanently excited machines, but their permanent magnets are expensive. Transverse flux or reluctance machines combine the characteristics of the other machine types.
Table 1.3 Basic categories and examples of electric machines.
Electric machines
DC machines
AC machines
Asynchronous
Synchronous
Electrical excitation
Permanent excitation
Advanced
(BL) DCM (brushless) DC motor
ASM induction (asynchronous motor)
SM (synchronous motor)
PSM (permanent magnet synchronous motor)
SRMPSM (switched reluctance motor)
TFMPSM (transverse flux motor)
HSMPSM (hybrid synchronous motor)
Induction (asynchronous) machines (ASM) are powered by electromagnetic induction from the magnetic field in the stator winding. The rotation of the magnetic field is asynchronous to the operating speed of the machine. This is referred to as the slip of the ASM, and is necessary for torque transfer (Table 1.4). Example vehicles are Tesla's Roadster and Model S.
Table 1.4 Technical assessment of selected types of electric machines [3].
Motor type
ASM
SM
PSM
HSM
Control
O
+
O
O
Noise emissions
O
+
++
++
Thermal limits
++
+
O
O
Costs
+
O
−
−
Safety
++
++
O
O
Maximum speed (min
−1
)
>10 000
>10 000
>10 000
>12 000
Continuous torque (Nm kg
−1
)
0.60–2.65
0.60–0.75
0.95–1.72
2.08–3.43
Continuous power (kW kg
−1
)
0.20–0.89
0.15–1.10
0.30–1.07
1.12–1.82
Maximum efficiency (%)
83–91
81–95
81–95
95
Example vehicle
Tesla Model S
Renault Fluence Z.E.
Smart Fortwo ed
BMW i3
Synchronous motors (SMs) contain three-phase electromagnets and create the magnetic field rotating synchronous to the rotor speed. Renault's Fluence Z.E. uses a synchronous machine as traction motor. Permanent magnet synchronous machines (PSM) contain neodymium magnets or other rare earth magnets to create the electromagnetic field. Example vehicles are the Smart fortwo electric drive and the Volkswagen e-Golf.
Hybrid synchronous machines (HSM) are a specific type of synchronous machine containing both permanent magnets and electromagnetic winding. This permits higher motor speeds due to the stronger magnetic field. The BMW i3 uses HSM technology.
Depending on the concept, electric machines can be placed at different positions of the drivetrain. There are many possibilities from a simple connection to the gearbox to direct integration into the gearbox. A special configuration is the wheel hub drive, which represents an integration of the electric machine directly into the wheel hub. This is beneficial with regard to the vehicle package, as differentials and drive shafts become superfluous, and in view of functionalities that can be implemented into the propulsion algorithm, such as ABS, traction control, and torque vectoring. However, the higher unsprung mass needs to be addressed in suspension design. Wheel hub motors are not yet deployed in any series (passenger) vehicle. Integrative solutions featuring lower mass are currently being developed, for example, the Active Wheel system by Michelin with a nominal power of 30 kW per wheel and a mass of 7 kg [4].
Electric machines for traction applications in road vehicles are currently substantially more expensive than combustion engines of identical power. Synchronous machines cost approximately €50 kWmech−1 including voltage converter, which is four-time higher than for combustion engines [5].
Drivetrain topologies in battery electric vehicles can consist of twin motors powering individual wheels to permit versatile control strategies such as torque vectoring for e-differential applications or innovative steering geometries for minimal turning circles, as seen in the recent SpeedE BEV concept car (Figure 1.3) [6]. It features 400 V twin motors at the rear wheels and a 48 V steer-by-wire system with a maximum steering angle of 90°.
Figure 1.3 Innovative steering sytsem in the SpeedE BEV concept car with twin RWD motors and torque vectoring. (Source: fka.)
The SpeedE vehicle also features steering with sidesticks instead of a steering wheel, which allows for new interior design layouts and innovative operability concepts (Figure 1.4).
Figure 1.4 Minimal turning circle with electric torque vectoring in the SpeedE BEV concept car.
Recent BEV developments and market success of some vehicles show that electric vehicles are mature and that they will grow their share in the vehicle population for the foreseeable future. R&D progress, especially in battery and motor technology, will strengthen electric and sustainable mobility.
It may be the new driving experience features that pave the way for even more EVs in the future, regardless of the drivetrain technology itself. X-by-wire, connectivity, and user interface novelties will have an impact on the EV market prospects, since these innovations will need electric energy to function.
This underlines the fact that developments for BEVs are not necessarily showstoppers for FCEVs but can complement the effort to create clean and sustainable mobility for the future.
1.
Eckstein, L. (2010)
Alternative Vehicle Propulsion Systems
, Schriftenreihe Automobiltechnik, Aachen, ISBN: 978-3-940374-33-2.
2.
Huslage, J. (7 October 2014) The next generation of automotive batteries! Presented at World of Energy Solutions, Stuttgart, Germany, 6–8 October 2014.
3.
Ernst, C. (2014)
Energetische, ökologische und ökonomische Lebenszyklusanalyse elektrifizierter Antriebsstrangkonzepte
, Schriftenreihe, Automobiltechnik, Dissertation RWTH Aachen University, Aachen, ISBN: 978-3-940374-80-6.
4.
Oliva, P. (2009) Michelin arbeitet seit zwölf Jahren am neuen Rad. Interview, Automobiltechnische Zeitschrift (ATZ), March 2009.
5.
Gnörich, B. (2009) HySYS Technical Workshop. Result of expert discussion. Aachen, May 2009.
6.
Eckstein, L.
et al.
(2013) The wheel-individually steerable front axle of the research vehicle SpeedE. Presented at the Aachen Colloquium Automobile and Engine Technology, Aachen, 7–9 October 2013.
Thomas Grube
Forschungszentrum Jülich GmbH, IEK-3: Electrochemical Process Engineering, Leo-Brandt-Strasse, 52425 Jülich, Germany
The evaluation of road vehicles requires standardized methods for the determination of fuel consumption and emissions. A constitutive part of such methods is the drive cycle that is typically used for chassis dynamometer tests. A large variety of country or region specific drive cycles for vehicle type approval exists worldwide. Other drive cycle definitions result from research projects related to specific assessments in vehicle development and evaluation. This chapter introduces selected drive cycles that are considered relevant as they apply for regions with large vehicle fleets or are otherwise commonly used. The focus here is on passenger cars; however, notably, such drive cycle definitions also exist for buses and trucks.
Keywords: alternative powertrains; drive cycle; well-to-tank analysis
For the assessment of environmental impact and resource use of vehicle and fuel systems, fuel consumption and air pollutant emissions of vehicles must be determined. To achieve reproducible results of respective measurements standardized test procedures must be applied. This is carried out on the basis of legal regulations in many countries. Ambient conditions, fuel specifications as well as load conditions of the vehicles tested are defined here. Moreover, a drive cycle that consists of time-dependent speed data points or rotational-speed and torque data points is detailed. Special rules may apply for alternative powertrain configurations.
Vehicle load, traffic, topographic road conditions, and driver behavior have, among others, a great impact on fuel economy and exhaust emissions. Consequently, drive cycles strongly simplify real-world car driving. The selection of a preferable realistic drive cycle is therefore decisive regarding environmental performance ratings and, not least, consumer information.
Besides their application for type approval purposes, drive cycles are used for specific tasks in vehicle development and for specific assessments in the field of energy systems analysis, particularly in tank-to-wheel analyses of road vehicles.
In the following, relevant examples of up-to-date drive cycles that are used for type approval procedures are presented. The respective speed–time graphs of the above-mentioned drive cycles can be found below in Figure 2.2 (numbers 1–14). A more comprehensive compilation of in total 256 drive cycles can be found in Barlow et al. [1]. Moreover, Rakopoulos [2] and Delphi [3] provide summarized information on worldwide vehicle emission standards also including the respective drive cycles.
The drive cycle that is relevant for type approval of light passenger and commercial vehicles in the European Union is specified in Council Directive 70/220 [4]. In the literature it is referred to as the NEDC (New European Drive Cycle) or MVEG-B (Motor Vehicle Emissions Group) drive cycle. The MVEG-B drive cycle consists of two parts that are also separately used: the ECE (Economic Commission for Europe) drive cycle for urban driving and the Extra Urban Drive Cycle (EUDC) representing driving at elevated speeds. With regulation (EC) No. 715/2007 of the European Parliament and of the Council [5] the European Commission is asked to review the drive cycle and possibly replace it “…reflecting changes in vehicle specifications and driver behavior” [5, p. L171/172]. The proposed new drive cycle for the European Union is the Worldwide Harmonized Light Duty Test Cycle (WLTC).
Drive cycles related to the US Federal (Tier 1-3) and California (Low Emission Vehicle, LEV 1-3) vehicle emissions legislation are the Urban Dynamometer Driving Schedule (UDDS), the Federal Test Procedure (FTP), the Highway Fuel Economy Test (HWFET), and the US06 and the SC03 driving cycles. US06 and SC03 supplement the FTP with the aim of also including driving with higher accelerations and higher speeds (US06) and the use of air conditioning (SC03) [6]. The FTP drive cycle is basically the UDDS repeating the first 505 s of the UDDS at its end.
Vehicle type approval in Japan requires the new drive cycle JC08 that came into effect in 2011, replacing the former cycles 11 Mode, known as Cold Cycle and 10–15 Mode known as Hot Cycle. These two outdated drive cycles are not shown in Figure 2.2 below.
Apart from the aforementioned drive cycles for type approval procedures various research activities, international projects and other initiatives lead to the definition of drive cycles that should reflect car driving in a more representative way. Three examples are given here based on information and data given in Reference [7]. The research projects MODEM and HYZEM resulted in the definition of drive cycle sets on the basis of monitoring fleets of 58 (MODEM) and 77 (HYZEM) cars. These cars were operated in France, UK, Germany, and Greece. The total distance covered was more than 160 000 km for the two projects. The subsequent ARTEMIS project made use of the databases provided by MODEM and HYZEM and included additional data from car monitoring in Italy and Switzerland. The MODEM, HYZEM, and ARTEMIS full drive cycles and the respective sub-cycles can be found in Figure 2.2, numbers 15–26 (see below).
Selected parameters that allow for comparison of drive cycles will be presented in the following. The equations used for the calculation of the respective values are based on information in Reference [1] and rely on speed–time data points. The time resolution of available drive cycles is typically one second. During this time interval acceleration is considered constant. Speed–time values from real dynamometer tests or from dynamic simulations may deviate as the desired values from the drive cycle definitions cannot accurately be followed by real drivers or by the driver model that is part of a control circuit in dynamic simulations.
Basic characteristics of drive cycles are duration, distance, and average speed (see Eqs. (2.1)–(2.3)):
Definitions: n is the number of speed–time data points; speed values are given in km h−1; indices are one-based, that is, the first index is one.
With increasing average speed, drive cycles can roughly be grouped into urban, extra-urban, or rural and motorway driving. Mechanical energy use basically increases with average speed. However, urban driving may also show high energy turnover, if frequency and duration of acceleration periods increase. For this reason, various parameters can be used to provide additional information on drive cycle characteristics. Examples of such parameters are: relative positive acceleration (RPA) and relative negative acceleration (RNA) and standstill time (see Eqs. (2.4)–(2.6)). The RPA and RNA are measures for the dynamic properties of a drive cycle. High values indicate high numbers of acceleration and deceleration periods:
The calculation results of Eqs. (2.1)–(2.6) related to the 26 drive cycles presented in this chapter can be found in Table 2.1. It can be seen that drive cycle durations range from 323 to 3207 s. Values for the total distance are between 1.7 km (MODEM-slow urban) and 61 km (HYZEM). Average speeds are high for the MODEM-motorway (102 km h−1) and ARTEMIS-motorway (97 km h−1) cycles and low for the drive cycles MODEM-slow urban (14 km h−1) and ECE and ARTEMIS-urban (both with 18 km h−1).
Table 2.1 Drive cycle characteristics of selected passenger car drive cycles. For speed–time graphs see Figure 2.2. RPA: relative positive acceleration; RNA: relative negative acceleration. For equations related to the displayed parameters see Section 2.4.
Cycle name
Duration (s)
Distance (km)
Average speed (km h
−1
)
RPA (m s
−2
)
RNA (m s
−2
)
Relative time standing (%)
(1) MVEG-B
1180
11
33
0.12
−0.11
24
(2) ECE
780
4.0
18
0.15
−0.13
31
(3) EUDC
400
6.9
62
0.09
−0.09
10
(4) WLTC
1800
23
46
0.16
−0.15
11
(5) WLTC-low
589
3.1
19
0.22
−0.20
25
(6) WLTC-middle
433
4.7
39
0.21
−0.19
11
(7) WLTC-high
455
7.1
56
0.14
−0.13
6.4
(8) WLTC-very high
323
8.3
92
0.13
−0.12
1.9
(9) UDDS
1372
12
31
0.19
−0.16
18
(10) FTP
1874
18
34
0.18
−0.16
18
(11) HWFET
765
17
78
0.09
−0.07
0.65
(12) SFTP-US06
600
13
77
0.22
−0.20
6.7
(13) SFTP-SC03
594
5.8
35
0.22
−0.19
18
(14) JC08
1204
8.2
24
0.19
−0.17
29
(15) MODEM
1948
25
46
0.19
−0.17
15
(16) MODEM-slow urban
451
1.7
14
0.28
−0.23
33
(17) MODEM-road
695
8.5
44
0.23
−0.21
11
(18) MODEM-free flow urban
352
2.2
23
0.32
−0.28
18
(19) MODEM-motorway
450
13
102
0.12
−0.11
1.8
(20) HYZEM
3207
61
68
0.15
−0.14
8.5
(21) HYZEM-urban
560
3.5
22
0.28
−0.24
24
(22) HYZEM-rural
843
11
48
0.22
−0.20
9.8
(23) HYZEM-highway
1804
46
92
0.13
−0.12
3.2
(24) ARTEMIS-urban
993
4.9
18
0.34
−0.28
26
(25) ARTEMIS-road
1082
17
57
0.18
−0.17
2.8
(26) ARTEMIS-motorway
1068
29
97
0.14
−0.13
1.4
RPA and RNA values are typically close. ARTEMIS-urban (0.34 and −0.28) and MODEM-free flow urban (0.32 and −0.28) are in the higher range of values. EUDC (0.09 and −0.09) and HWFET (0.09 and −0.07) show comparably low RPAs and RNAs. Interestingly, the ARTEMIS-urban drive cycle with the shortest distance (4.9 km) and one of the lowest average speeds (18 km h−1) has the overall highest RPA and RNA (0.34 and −0.28). Other cycles with high RPAs are the US cycles UDDS, FTP, US06, and SC03. Finally, high shares of standstill periods can be found for MODEM-slow urban (33%) and JC08 (29%).
Based on passenger car simulations carried out in Reference [8] results for the mechanical energy requirements of the drive cycles presented here are displayed in Figure 2.1. Considering urban driving, it can be seen that for drive cycles with high RPAs and RNAs the mechanical energy values are also comparably high. In extra-urban driving ARTEMIS-road, EUDC, and WLTC-high show lowest mechanical energy values due to comparably low average speeds. For motorway driving the HWFET cycle has the lowest mechanical energy, again due to a low average speed that is here combined with a low RPA.
Figure 2.1 Mechanical energy (Em) at the wheels of a passenger car with a mass of 1251 kg, a cross-sectional area of 2.1 m2, and an air drag coefficient of 0.32. Values are derived from dynamic powertrain simulation results [8]. The numbers in the figure correspond to the numbering in Table 2.1.
Speed–time data points of the selected drive cycles are shown in Figure 2.2. The first part of the figure is dedicated to drive cycles that are part of vehicle type approval regulations (drive cycles with the numbers 1–14). Subsequent drive cycles have been designed on the basis of data from vehicle monitoring in international research projects. Further explanations can be found in Sections 2.2 and 2.3. Descriptive parameters that allow for characterization of drive cycles have been introduced in Section 2.4.
Figure 2.2 Speed–time graphs of selected drive cycles. The drive cycle numbers correspond to the numbering in Table 2.1.
This chapter has presented relevant drive cycles designed for vehicle type approval and for other specific tasks of vehicle powertrain evaluation. Some parameters that allow for a first characterization of drive cycles regarding their dynamic properties and mechanical energy requirements have been defined. Consequently, the drive cycle-specific spectrum of load points in combination with the performance characteristics of powertrain configurations is decisive for the actual results of fuel economy and emissions assessments. In this regard drive cycles are widely used as the basis for dynamometer tests and as time-dependent input variables for dynamic powertrain simulations. Such simulations may usefully be applied for technical development as well as for various systems analysis tasks. Measurements based on dynamometer and real-word tests of vehicles, however, provide the required data for vehicle type approval as well as for environmental assessments.
1.
Barlow, T.J.
et al.
(2009)
A Reference Book of Driving Cycles For Use in the Measurement of Road Vehicle Emissions
, Transportation Research Laboratory (TRL), Wokingham, Berkshire, UK.
2.
Rakopoulos, C.D. and Giakoumis, E.G. (2009)
Diesel Engine Transient Operation: Principles of Operation and Simulation Analysis
, Springer, London. ISBN: 978-1-84882-375-4.
3.
Delphi Automotive LLP (2012) Worldwide Emissions Standards – Passenger Cars and Light Duty Vehicles.
4.
The Council of the European Communities, Brussels (2006) Council Directive of 20 March 1970 on the approximation of the laws of the Member States on measures to be taken against air pollution by emissions from motor vehicles.
5.
European Commission, Brussels (2007) Regulation (EC) No 715/2007 of the European Parliament and of the Council of 20 June 2007 on type approval of motor vehicles with respect to emissions from light passenger and commercial vehicles (Euro 5 and Euro 6) and on access to vehicle repair and maintenance information, in Commission, E. (ed.).
6.
Environmental Protection Agency (1996) Final Regulations For Revisions to the Federal Test Procedure for Emissions from Motor Vehicles, Federal Register/Vol. 61, No. 205.
7.
André, M. (2004) The ARTEMIS European driving cycles for measuring car pollutant emissions.
Sci. Total Environ.
,
334–335
, 73–84.
8.
Grube, T. (2014). Potential der Stromnutzung in Pkw-Antrieben zur Reduzierung des Kraftstoffbedarfs. Technische Universität Berlin, Fakultät V – Verkehrs- und Maschinensysteme, Dissertation.
James M. Ohi
3024 Carter Circle, Denver, CO 80222, USA
This chapter gives a brief overview of fuel quality as specified in ISO 14687-2:2012 for hydrogen dispensed for use in polymer electrolyte fuel cell (PEMFC) road vehicle systems.
Keywords: fuel quality; hydrogen fuel; ISO 14687-2:2012; PEM fuel cells; road vehicle systems
An international effort to establish a fuel quality standard for hydrogen began in 2004 to address the accelerating pace of fuel cell vehicle (FCV) demonstration projects in Asia, North America, and Europe. Adoption of such a standard would remove one variable in the data obtained from these demonstration projects and would also facilitate eventual commercialization of fuel cell vehicles. The contaminants and their recommended limits included in the standard published in 2012 are shown in Table 3.1. Verification of fuel quality is to be conducted at the dispenser nozzle under applicable standardized sampling and analytical methods or at other locations or methods acceptable to the supplier and customer. As the table was based on then current knowledge, contaminants not listed should not be assumed to be benign.
Table 3.1 Directory of limiting characteristics (maximum allowable limits of contaminants) ISO 14687-2:2012.
Characteristics (assay)
Type I, Type II Grade D
Hydrogen fuel index (minimum mole fraction)
a)
99.97%
Total non-hydrogen gases
300 µmol mol
−1
Maximum concentration of individual contaminants (
µmol mol
−1
)
Water (H
2
O)
5
Total hydrocarbons
b)
(methane basis)
2
Oxygen (O
2
)
5
Helium (He)
300
Total nitrogen (N
2
) and argon (Ar)
b
100
Carbon dioxide (CO
2
)
2
Carbon monoxide (CO)
0.2
Total sulfur compounds
c)
(H
2
S basis)
0.004
Formaldehyde (HCHO)
0.01
Formic acid (HCOOH)
0.2
Ammonia (NH
3
)
0.1
Total halogenated compounds
d)
(halogenate ion basis)
0.05
Maximum particulates concentration
1 mg kg
−1
Note: For the constituents that are additive, such as total hydrocarbons and total sulfur compounds, the sum of the constituents are to be less than or equal to the acceptable limit. The tolerances in the applicable gas testing method are to be the tolerance of the acceptable limit.
a)
The hydrogen fuel index is determined by subtracting the “total non-hydrogen gases” in this table, expressed in mole percent, from 100 mole percent.
b)
Total hydrocarbons include oxygenated organic species. Total hydrocarbons are measured on a carbon basis (µmol-C mol
−1
). Total hydrocarbons may exceed 2 µmol mol
−1
due only to the presence of methane, in which case the summation of methane, nitrogen, and argon is not to exceed 100 ppm.
c)
As a minimum, includes H
2
S, COS, CS
2
, and mercaptans, which are typically found in natural gas.
d)
Includes, for example, hydrogen bromide (HBr), hydrogen chloride (HCl), chlorine (Cl
2
), and organic halides (R–X).
Given the near-term focus of the standard, contaminants and their limitations are specified for hydrogen produced and purified by steam methane reforming (SMR) of natural gas and pressure-swing adsorption (PSA), respectively, and stored on board FCVs with high-pressure gaseous storage containers. Testing and analysis were focused on five “critical constituents”: carbon monoxide (CO), sulfur (S) species, ammonia (NH3), methane (CH4) and other inert gases, and particulate matter (PM) under 10 microns in diameter. These constituents are those most likely to affect PEM fuel cell performance and durability as well as the cost of hydrogen produced by SMR and purified by PSA to the levels required by the standard. Table 3.2 shows the relative difficulty of removing these key contaminant species from hydrogen produced by SMR and purified by PSA.
Table 3.2 Relative difficulty of removing selected contaminants species from hydrogen produced by SMR and purified by PSA. (Source: Chevron Technology Ventures.)
Species
Adsorption force
ISO 14687 specification (ppm)
SMR (mol.%)
Purification ratio for SMR
Overall effect
Helium (He)
Zero
300 (total inert)
500 ppm
5
Not possible
Hydrogen (H
2
)
Weak
99.97%
75–80
Impacts PSA recovery and capital cost
Oxygen (O
2
)
5
—
—
Impacts PSA recovery and capital cost
Argon (Ar)
100 (total inert)
500 ppm
5
Impacts PSA recovery and capital cost
Nitrogen (N
2
)
100 (total inert)
1000 ppm
10
Impacts PSA recovery and capital cost
Carbon monoxide (CO)
0.2
0.1–4
200 000
Impacts PSA recovery and capital cost
Methane (CH
4
)
2 (incl. THC)
0.5–3
15 000
Impacts PSA recovery and capital cost
Carbon dioxide (CO
2
)
2
15–18
90 000
Relatively easier to remove
Total HCs
2 (incl CH
4
)
0.5
2500
Relatively easier to remove
Ammonia
Strong
0.1
Low ppm
Relatively easier to remove
Total sulfur
Strong
0.004
Relatively easier to remove
Halogenates
Strong
0.05
Relatively easier to remove
Water (H
2
O)
Strong
5
Dew point
Relatively easier to remove
The effects of minute amounts of specific contaminants on PEM fuel cell performance and durability must be considered within the larger context of the causes and mechanisms of PEM fuel cell degradation, that is, the gradual decline in power output during operation in road vehicles. These mechanisms include degradation of mechanical properties due to dissolution and sintering of platinum particles, thinning of the membrane, and corrosion of carbon support materials [2]. Contaminants such as CO and hydrogen sulfide (H2S) adsorb on the surface of the catalyst and impede the electrode charge-transfer process, leading to losses due to higher cell overpotential. Contaminants such as NH3 form cations that through ion exchange with protons in the ionomer inhibit proton conduction and create large ohmic losses. Contaminants can also decrease mass transfer by changing water and/or gas transport in the gas diffusion layer. The effects of fuel contaminants on performance and durability are themselves complex and are just one contributing factor among many other considerations discussed in References [2,3].
Hydrogen quality must be maintained from the fueling nozzle receptacle to the anode inlet, which encompasses on-board storage and balance-of-plant (BOP) fuel system components. Fuel quality must be considered in the context of the synergistic operation of the PEM fuel cell vehicle subsystems that are critical to overall system efficiency and durability. For example, efficient compression, cleanup, and delivery of air are critical to cathode operation, and the heat exchange subsystem must maintain uniform stack temperature during cold and hot thermal and load excursions. The water management subsystem must maintain consistency in stack performance from sub-freezing to high temperature and low relative humidity (RH) operations. Furthermore, the hydrogen storage and delivery subsystem affects anode performance and life, particularly since a highly active low anode catalyst loading is necessary to meet system cost objectives. Vehicular operations that are critical to fuel cell performance include temperature of operation, shut down/start up procedure, extent of time operating at idle and full load potential (i.e., degree of hybridization, etc.), and transient/steady-state demands, among other parameters.
The maximum allowable concentrations of selected non-hydrogen constituents are based on a limited number of tests under a small set of primarily constant operating conditions using single-cells that do not reflect the state-of-art of PEM fuel cell design and engineering. That said, the specifications represent a consensus of international experts from industry, universities, and national laboratories and, as stated in ISO 14687-2, they should provide adequate requirements for the pre-commercial phase of technology development of PEM fuel cells for road vehicles. Each test laboratory followed a cell conditioning procedure based on recommendations from the cell manufacturer. The following parameters and conditions were followed by each laboratory for baseline testing:
temperature: 80 °C;
RH: 75% anode/25% cathode (in accordance with manufacturer recommendations);
pressure: 150 kPa (abs);
electrical load: 1 A cm
−2
stoics: 1.2/2.0 (anode/cathode).
Given the limited time available, testing focused on obtaining critical data points:
contaminants to be tested: CO, NH
3
, halogenates, ISO mixture (CO, H
2
S, NH
3
, inerts);
contaminant levels: two for each contaminant – (1) at ISO specification level, (2) at 10× specification level;
test duration: (300 h or until performance drops by >60 mV) or as suitable for a contaminant.
As an example, the results of single cell tests for the effects of CO are summarized in Figure 3.1. The test conditions included anode platinum loading of 0.05 mg cm−2, constant current (1 A cm−2), 100% relative humidity at 80 °C, and constant dosage (20 ppm h−1 CO) obtained by varying both concentration and exposure times. These results show that cell performance losses increase with CO concentration but decrease with cell temperature.
Figure 3.1 Summary of CO tests with 0.05 mg-Pt cm−2 at different temperatures [4].
Data on the effects of fuel quality on the performance and durability of PEM fuel cell vehicles under real-world fueling and driving conditions are very limited. Such vehicles have been and continue to be demonstrated in Asia, Europe, and North America, but the main focus of these demonstrations has been on key technical targets, primarily durability (hours of FC stack operation) and vehicle range. Fueling with hydrogen is at a pre-commercial stage, and the quality of such fuel, delivered or produced on-site, is controlled carefully by fuel providers to minimize or eliminate the effect of fuel quality on the performance and durability of the very expensive PEM fuel cell demonstration vehicles. The Japan Hydrogen and Fuel Cell Demonstration Project (JHFC) was the first demonstration in the world of concurrent operation of stations with hydrogen produced from different feedstocks and methods. These feedstocks and methods included: reforming of natural gas, naptha, gasoline, methanol, LPG, and kerosene; electrolysis of water; and liquefaction of hydrogen. Furthermore, JHFC gathered and made available data on fuel quality from these stations. These data were derived from continuous monitoring of CO and CH4 at the PSA exit of six stations and batch analysis of N2, CO, CO2, CH4, O2, and H2O at different intervals (bimonthly, quarterly, semiannually) at various stations. Table 3.3 shows fuel quality data in parts per million (ppm) from one station (Senju) using natural gas reformed on site.
Table 3.3 Fuel quality data (ppm) from the Senju fueling station (ND: “not detected”).
March 2004
February 2005
September 2005
December 2007
December 2008
CO
0.02
0.02
ND
ND
0.01
CO
2
ND
ND
ND
ND
ND
CH
4
0.08
ND
0.08
ND
ND
NMHC
ND
ND
ND
ND
ND
C
6
H
6
ND
ND
ND
ND
ND
S-compounds
ND
ND
ND
ND
ND
MeOH
ND
ND
ND
ND
ND
HCHO
ND
ND
ND
ND
ND
CH
3
CHO
ND
ND
ND
ND
ND
HCOOH
ND
ND
ND
ND
ND
CH
3
COCH
3
ND
ND
ND
ND
ND
NH
3
ND
ND
ND
ND
ND
Halogen
—
—
—
ND
ND
O
2
ND
ND
ND
ND
ND
H
2
O
24.0
0.9
ND
ND
ND
Ar
4.95
0.11
0.73
1.5
1.34
N
2
3.03
0.12
3.59
10.4
6.91
He
ND
ND
ND
ND
ND
Standardized analytical methods and instrumentation are required to verify compliance with the specifications. ASTM International developed and is validating consensus analytic procedures to enable laboratories to verify whether a particular fuel sample meets these specifications using standardized instrumentation and test procedures [6]. Table 3.4 shows analytical sampling and measurement of contaminants at hydrogen fueling stations conducted by the JHFC. These data indicate that existing analytical instrumentation and methods are sensitive enough to detect and measure contaminants in hydrogen fuel at the levels specified by the ISO standard (Reference [1] footnote 5).
Table 3.4 Analytical sampling and measurement of contaminants at hydrogen fueling stations.
Impurities
Analytical methods
a)