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Title: Energy and the New Reality, Volume 1: Energy Efficiency and the Demand for Energy Services Chapter 5: Transportation Energy Use L. D. Danny Harvey harvey@geog.utoronto.ca


1
Energy and the New Reality, Volume 1Energy
Efficiency and the Demand for Energy Services
Chapter 5 Transportation Energy Use L. D.
Danny Harveyharvey_at_geog.utoronto.ca
Publisher Earthscan, UKHomepage
www.earthscan.co.uk/?tabid101807
  • This material is intended for use in lectures,
    presentations and as handouts to students, and is
    provided in Powerpoint format so as to allow
    customization for the individual needs of course
    instructors. Permission of the author and
    publisher is required for any other usage. Please
    see www.earthscan.co.uk for contact details.

2
Transportation Energy Use, Outline
  • Trends in movement of people and goods
  • Energy use by different modes of transport
  • Role of urban form and infrastructure
  • Role of vehicle choice today
  • Technical options for reducing energy use in
  • - Cars and light trucks
  • - Inter-city rail and buses
  • - Passenger aircraft
  • - Freight transport

3
Technical options for cars light trucks
  • Downsizing
  • Drive-train efficiency (thermal, mechanical,
    transmission)
  • Reduced loads (requiring the engine to do less
    work)
  • Hybrid electric vehicles (HEVs)
  • Plug-in hybrid electric vehicles (FCVs)
  • Fuel cell vehicles (FCVs)

4
Issue with fuel cell vehicles
  • Cost and performance of fuel cells
  • Constraints on supply of precious-metal catalysts
  • Difficulties with on-board processing of
    hydrocarbon fuels
  • Difficulties with on-board storage of hydrogen
    and development of H2 supply infrastructure

5
Figure 5.1 Proportion of different fuels usedfor
world transportation
Source Gilbert and Pearl (2007, Transport
Revolutions Moving People and Freight Without
Oil, Earthscan, London)
6
Figure 5.2a Breakdown of transportation energy
use in OECD countries in 2005
7
Figure 5.2b Break down of transportation energy
usein non-OECD countries in 2005
8
Figure 5.3a Variation in world passenger-km
movement of people
Source Gilbert and Pearl (2007, Transport
Revolutions Moving People and Freight Without
Oil, Earthscan, London)
9
Figure 5.3b Variation in world tonne-km movement
of freight
Source Gilbert and Pearl (2007, Transport
Revolutions Moving People and Freight Without
Oil, Earthscan, London)
10
Figure 5.4 Historical variation in world
passenger-km transport by aircraft
Source Gilbert and Pearl (2007, Transport
Revolutions Moving People and Freight Without
Oil, Earthscan, London)
11
Figure 5.5 Growth in the number of passenger and
commercial vehicles worldwide
12
Figure 5.6 Historical variation in the number of
cars per 1000 people
Source Gilbert and Pearl (2007, Transport
Revolutions Moving People and Freight Without
Oil, Earthscan, London)
13
Figure 5.7 Breakdown of total travel in USA
Source Gilbert and Pearl (2007, Transport
Revolutions Moving People and Freight Without
Oil, Earthscan, London)
14
From Table 5.1, energy intensities of different
modes of travel within cities
  • Gas guzzling car (20 litres/100 km), one person
  • 6.5 MJ/person-km (7.8 MJ/p-km primary
    energy)
  • Energy efficient car (8 litres/100 km), 4
    persons
  • 0.65 MJ/person-km (0.78 MJ/p-km primary
    energy)
  • Diesel bus, typical US loading 1-2 MJ/person-km
  • Light rail 0.8 MJ/person-km of electricity, 2
    MJ/person-km primary energy
  • Heavy rail 0.4 MJ/person-km electricity, 1.0
    MJ/person-km primary energy
  • Walking 0.13 MJ/person-km food energy
  • Bicycling 0.1 MJ/person-km food energy

15
From Table 5.3, primary-energy intensities of
different modes of travel between cities
  • Gas guzzling car (12 litres/100 km, 4 people)
  • 1.16 MJ/person-km
  • Fuel efficient car (6 litres/100 km, 4 people)
  • 0.58 MJ/person-km
  • Intercity bus 0.28 MJ/person-km
  • Diesel train 0.2-0.5 MJ/person-km
  • High speed electric train 0.2-0.4 MJ/person-km
  • Air 0.6-1.5 MJ/person-km

16
From Table 5.4 The complete energy picture for
transportation involves
  • On-site fuel or electricity use
  • Upstream energy use in producing and supplying
    the fuel or electricity (this and on-site energy
    give primary energy use for the operation of the
    vehicle, which is what is given in the preceding
    two slides)
  • The energy used to make the vehicle (embodied
    energy), averaged over the total distance
    travelled during the lifetime of the vehicle
  • The energy used to make and maintain the
    infrastructure for the vehicles (roads, rail
    lines, airports), averaged over the total
    distance travelled during the lifetime of the
    vehicle

17
Some prominent results from Table 5.4
  • Vehicleinfrastructure embodied energy for urban
    light and heavy rail, interurban car and
    interurban rail is about ½ the directupstream
    operating energy use
  • Embodied energy for short air travel (trips of
    390 km) exceeds the operating energy
  • For international air travel (average distance of
    7500 km), the aircraft embodied energy is
    important (about 40 of the operating energy)

18
Figure 5.8 Relationship between private
transportationenergy use and urban density
Source Newman and Kenworthy (1999,
Sustainability and Cities Overcoming Automobile
Dependence, Island Press, Washington)
19
Compact urban form with different land uses
(residential, retail, offices, schools and
daycare centres, medical) intermixed reduces
transportation energy requirements by
  • Reducing the distances that need to be travelled
  • Making is more practical and economical to serve
    the reduced travel demand with high-quality
    (i.e., rail-based) public transit
  • Increasing the viability of walking and bicycling

Once people start using transit, there is a
further reduction in travel demand (in the
distances travelled) because people start
planning their trips to be more efficient (i.e.,
combining errands in one trip)
20
Bicyclingwalking share (in terms of number of
trips taken) in selected cities in 2001
  • Amsterdam, 52
  • Copenhagen, 39
  • Hong Kong, 38 (another 46 by public transit)
  • Sao Paulo, 37
  • Berlin, 36
  • New York, 9
  • Atlanta, 0

21
Importance of Choice of Car/Truck (fuel use is
given for city driving)
  • Pickup truck, 16 to 26 litres/100 km
  • SUV, 8 to 26 litres/100 km
  • Minivan, 11 to 21 litres/100 km
  • Large car, 11 to 26 litres/ 100 km
  • Mid-size car, 9 to 24 liters/100 km
  • Subcompact car, 8 to 21 litres/100 km
  • Subcompact hybrid, 6 litres/100 km
  • 2-seater, 7 to 29 liters/100 km

22
Figure 5.9a Mix of vehicles purchased in the US
in 1975
Source Friedman et al (2001, Drilling in
Detroit Tapping Automaker Ingenuity to Build
Safe and Efficient Automobile, Union of Concerned
Scientists)
23
Figure 5.9b Mix of vehicle purchased in the US in
2000
Source Friedman et al (2001, Drilling in
Detroit Tapping Automaker Ingenuity to Build
Safe and Efficient Automobile, Union of Concerned
Scientists)
24
Figure 5.10 Risks posed by different cars
Source Ross and Wenzel (2002, An Analysis of
Traffic Deaths by Vehicle Type and Model, ACEEE)
25
Types of automobiles
  • Spark ignition (SI) runs on gasoline, with
    power output reduced by reducing the flow of fuel
    and throttling (partially blocking) the airflow,
    causing a major loss of efficiency at part load
    (which is the typical driving condition)
  • Compression ignition (CI) runs on diesel fuel,
    which is ignited by compression without the need
    for spark plugs. More efficient than SI engines
    due to absence of throttling, high compression
    ratio and lean fuel mixture (high airfuel ratio)
  • Internal combustion engine (ICE) refers to
    engines where combustion occurs in cylinders.
    Both SI and CI engines are ICEs

26
Pollution controls
  • SI engines use 3-way catalytic converters to
    oxidize (add oxygen to) CO and hydrocarbons in
    the exhaust while reducing (removing oxygen from)
    NOx
  • This requires a stoichiometric airfuel ratio
  • Until recently, 3-way catalytic converters could
    not reduce NOx in diesel exhaust because of the
    excess oxygen
  • Recent advances that entail the use of ammonia
    have solved this problem
  • Much stricter (and comparable) emission standards
    can be expected for both gasoline and diesel
    vehicles in the future.

27
However ....
  • Stricter pollution controls require ultra-low S
    concentrations in the fuel ( 10 ppm, vs 10-250
    today in gasoline and 10-500 ppm today in diesel
    fuel)
  • Achieving the very low S content in fuels
    increases refinery energy use by about 1.5, and
    the stricter pollution controls for diesel trucks
    (at least) would increase fuel use by 4-10

28
Figure 5.11a Fuel Economy Trend
Source Zachariadis, T. (2006, Energy Policy 34,
17731785, http//www.sciencedirect.com/science/jo
urnal/03014215)
29
Figure 5.11b Car/light truck fuel economy trend
Source Zachariadis, T. (2006, Energy Policy 34,
17731785, http//www.sciencedirect.com/science/jo
urnal/03014215)
30
Figure 5.12a Trends in automobile mass
Source Zachariadis, T. (2006, Energy Policy 34,
17731785, http//www.sciencedirect.com/science/jo
urnal/03014215)
31
Figure 5.12b Trends in automobile acceleration
and top speed
Source Zachariadis, T. (2006, Energy Policy 34,
17731785, http//www.sciencedirect.com/science/jo
urnal/03014215)
32
Figure 5.12c Trends in engine power and
power/displacement
Source Zachariadis, T. (2006, Energy Policy 34,
17731785, http//www.sciencedirect.com/science/jo
urnal/03014215)
33
Figure 5.13 Auto Loads vs. Speed
34
Figure 5.14 Fuel Use vs Speed
35
Figs 5.15-5.16 Energy flow in a typical present
day car (8.9 litres/100 km, 26.4 mpg) (left) and
advanced vehicle (4.0 litres/100 km, 58.4 mpg)
(right)
36
Options to Improve the Fuel Economy of Cars and
Light Trucks, Part 1
  • Improve engine thermal efficiency (fraction of
    fuel energy supplied to the pistons, through
    combustion)
  • Improve engine mechanical efficiency (fraction of
    piston energy transferred to the drive shaft)
  • Improve the transmission efficiency (fraction of
    drive shaft energy transferred to the wheels)

37
Methods to improve engine thermal efficiency
  • Leaner fuelair mixture (but worsens NOx
    emissions)
  • Variable compression ratio (currently fixed)
    saves 10-15 if combined with supercharged
    downsized engine
  • Direct injection gasoline fuel sprayed directly
    into cylinders at high pressure saves 4-6
  • Variable stroke (switch between 2-stroke
    operation during acceleration and 4-stroke
    operation at high speeds) saves 25
  • Resultant fuel use would be 0.85 x 0.95 x 0.75
    0.60, a savings of 40 (best case)

38
Methods to improve engine mechanical efficiency
  • Aggressive transmission management running at
    optimal gear ratio at all times, which makes the
    engine operate at the torque-rpm combination that
    maximizes the engine efficiency for any given
    driving condition.
  • Smaller engines (most of the time the engine
    operates at a small fraction of its peak power).
    10 smaller saves 6.6 in fuel because the engine
    on average will operate more efficiently
  • Variable valve control instead of throttling of
    air flow in gasoline engines saves up to 10
  • Reduced friction through better lubricants and
    other measures 1-5 savings
  • Automatic idle-off when stopped saves 1-2

39
Increasing the transmission efficiency
  • As noted above, the way in which the transmission
    is operated affects the engine mechanical
    efficiency
  • The transmission itself is another source of
    energy loss, which can be reduced
  • Typical transmission efficiencies today
  • - automatic, 70-80
  • - manual, 94
  • Future automatic 88 with continuously variable
    transmission
  • Energy use if we go from 70 to 88 is multiplied
    by 70/88 0.795, a savings of about 20

40
Combining the savings from different steps
  • Certainly do not add the savings, because the
    savings from each successive step applies only to
    the remaining energy use, not to the original
    energy use
  • Instead, multiply the individual factors
    representing the reduction in fuel use in each
    step
  • Thus, if improved engine thermal efficiency,
    engine mechanical efficiency and improved
    transmission efficiency save 40, 10 and 20,
    respectively, then multiply 0.6 x 0.9 x 0.8 to
    get the overall fuel requirement
  • In the above example, this would be 0.432 a
    savings of 56.8
  • The factor of 0.432 would be multiplied by a
    further factor to represent the effect of reduced
    loads, giving an even larger potential savings

41
Options to Improve the Fuel Economy of Cars and
Light Trucks, Part 2
  • Reduced tire rolling resistance through
    higher-pressure tires
  • Reduced aerodynamic resistance through changes in
    car shape
  • Reduced vehicle weight (affects energy use during
    acceleration and when climbing hills)
  • Reduced vehicle accessory loads

42
Comparing Figures 5.15 and 5.16
  • The energy flow to the wheels increases from
    14.8 to 22.7 of the fuel input
  • Thus, for the same energy flow, we need only
    14.8/22.7 0.652 as much fuel (a savings of
    34.8)
  • The loads on the wheels (due to reduced rolling
    and aerodynamic resistance and reduced vehicle
    weight) drop from 429.9 kJ/km to 298.0 kJ/km, so
    the fuel requirement from this alone would be
    multiplied by 298.0/429.9 0.693 (a savings of
    30.7)
  • The overall fuel requirement is multiplied by
    0.652 x 0.693 0.452 (a savings of 54.8, which
    is lt 34.830.7)
  • Cross-check the ratio of fuel inputs at the tops
    of the two figures is 1302/2882 0.452

43
Alternative vehicle drive trains
  • Hybrid gasoline-electric or diesel-electric
    vehicles (HEVs)
  • Plug-in hybrid electric vehicles (PHEVs)
  • All-electric or battery electric vehicles (BEVs)
  • Fuel cell vehicles (FCVs)

44
Hybrid electric vehicles
  • Use the engine to supply average power
    requirements and to recharge a battery, with the
    battery used to meet peak requirements
    (acceleration, hill climbing)
  • This allows downsizing of the engine, thereby
    reducing friction losses
  • It also allows the engine to operate closer to
    the torque-rpm combination that maximizes its
    mechanical efficiency

45
Other energy savings in HEVs occur through
  • Regenerative braking using vehicle kinetic
    energy to recharge the battery
  • Elimination of idling when stopped
  • Shifting power steering and other accessories to
    more efficient electric operation
  • However, the Toyota Prius is not much more
    fuel-efficient than a 1993 Honda Civic because
    the technology has largely gone into giving
    better acceleration rather than improving fuel
    economy

46
Figure 5.17 Gasoline-battery hybrid vehicle
(parallel drive-train option)
47
PHEVs
  • The idea here is to recharge the battery from the
    AC power grid (i.e., by plugging it in when
    parked) and using the battery until the battery
    energy drops, then switching to the gasoline (or
    diesel) engine
  • This requires batteries with greater storage
    capacity than in HEVs, giving 40-60 km driving
    range on the battery
  • Since most trips are shorter than this, a large
    portion of total distance travelled could be
    shifted to electricity in this way

48
PHEVs (continued)
  • The key issues are the cost of the battery, the
    mass of the battery (cars with heavier batteries
    will need more energy for acceleration and
    climbing hills), the amount of energy stored
    (usually represent in Wh), which determines the
    driving range, and the peak power output from the
    battery (W), which determines how fast the
    vehicle can accelerate
  • The key battery performance parameters are thus
    specific energy, Wh/kg, and specific power, W/kg

49
Figure 5.18 Specific power and specific energy
of different batteries
50
Figure 5.19 Battery cost vs battery powerenergy
ratio
60
51
Figure 5.20 kWh-fuel trade off
52
Figure 5.21 Gasoline savings with PHEVs as
afunction of electric driving range for US
driving patterns
53
Figure 5.22 Contributions to air conditioning
energy requirements
Source Kromer and Heywood (2007, Electric
Powertrains Opportunities and Challenges in the
U.S. Light-Duty Vehicle Fleet, Laboratory for
Energy and the Environment, MIT)
54
Figure 5.23 AC and non-AC energy Use (with AC
energy use given as a percentage of the driving
energy use)
Source Kromer and Heywood (2007, Electric
Powertrains Opportunities and Challenges in the
U.S. Light-Duty Vehicle Fleet, Laboratory for
Energy and the Environment, MIT)
55
Figure 5.24 Ratio of energy use by hybrid
vehicles to energy use by conventional vehicles,
with and without AC
56
Fuel Cell Vehicles
  • A fuel cell is an electrochemical device that
    produces electricity, water and heat
  • It requires a hydrogen-rich fuel
  • There had been some effort to develop systems to
    convert gasoline on-board into a hydrogen-rich
    fuel that in turn would be fed to the fuel cell,
    but these efforts have largely been abandoned

57
  • Instead, pure hydrogen fuel would be stored on
    board the vehicle
  • The major issues are
  • - How to store the hydrogen
  • - How to build up a hydrogen-distribution
    infrastructure
  • - What energy sources would be used to make
    hydrogen
  • - Cost of fuel cells and of hydrogen fuel

58
Attractions of hydrogen FCVs
  • Zero pollution emissions
  • Much lower noise
  • The hydrogen could be produced by electrolysis
    (splitting) of water using electricity supplied
    from renewable wind, solar or hydro sources of
    energy
  • Thus, zero greenhouse gas emissions and
    sustainable energy supply

59
Options for Onboard Storage of H2
  • As a gas compressed to 700 atm pressure
  • over 3 times the volume and 1.4 times the
    weight of gasolinetank in a gasoline-powered
    vehicle with the same driving range
  • - energy equiv to 10 that of the stored
    hydrogen would be needed for compression
  • As liquid hydrogen, at 20 K ( -253ºC)
  • just over 2 times the volume but half the
    weight of the gasolinetank
  • - energy equiv to 1/3 that of the stored
    hydrogen would be needed for liquefaction
    (possibly reduced to 20 in the future)
  • As a metal hydride
  • almost 4 times the weight but only 80 of
    the volume of gasolinetank. More mining and
    processing of metals needed.

60
Table 5.18, mass and volume to store 3.9 kg of
usable hydrogen or gasoline equivalent,
sufficient for a 610 km driving range
61
Figure 5.25 Ballard 85-kW fuel cell for
automotive applications
Source Little (2000, Cost Analysis of Fuel Cell
System for Transportation, Baseline System Cost
Estimate, Task 1 and 2 Final Report to Department
of Energy, Cambridge)
62
Figure 5.26 Ballard 85-kW fuel cell
Source www.ballard.com
63
Figure 5.27 Fuel cell-battery hybrid vehicle
64
Figure 5.28 Efficiency of fuel cell vs output
Box 5.1, at the end of this file, contains
Figures 5.29 and 5.30
Source Kromer and Heywood (2007, Electric
Powertrains Opportunities and Challenges in the
U.S. Light-Duty Vehicle Fleet, Laboratory for
Energy and the Environment, MIT)
65
Thus,
  • A hydrogen FCV would operate at a typical
    efficiency of 60, which is about three times
    the efficiency of a typical ICE (internal
    combustion engine) vehicle today
  • This in turn reduces the amount of energy (as H2)
    that needs to be stored on the vehicle for a
    given driving range by a factor of 3
  • This in turn is critical because any system of
    onboard hydrogen storage will be bulky and/or
    heavy in relation to the amount of energy stored
  • The high efficiency also greatly reduces the
    amount of wind or solar power that would need to
    be installed in order to produce enough hydrogen
    to replace petroleum for transportation

66
Problems
  • Fuel cells suitable for use in cars need to be
    able to operate at low temperature (120ºC)
  • Low-temperature fuel cells require precious-metal
    catalysts (Pt and ruthenium) in order to operate
    (these catalysts are also needed in 3-way
    catalytic converters, but would not be needed for
    such in H2 FCVs)
  • Supplies of Pt are quite limited the
    availability of Pt could be a significant
    constraint on the long-term viability of H2 FCVs
  • Hydrogen could instead be used in ICEs (with much
    less pollution), but with only a 10-20
    efficiency gain so the problem of being able to
    store enough H2 onboard in order to get a
    reasonable driving range would arise

67
Figure 5.31 Distribution of Exploitable Pt
Resources
68
Box 5.3 Constructing a scenario for Pt demand
69
Figure 5.32a Pt Scenario for future automobile
fleets of 1, 2 or 5 billion (compared to about
700 million passenger vehicles and 100 million
commercial vehicles today)
70
Figure 5.33a Scenario for the growth in vehicle
production rate and vehicle population used for
the 5-billion-vehicle case in the previous slide
71
Figure 5.33b Scenario for the growth in the
fraction of new vehicles and of total vehicle
stock as fuel cell vehicles
72
Figure 5.32b Cumulative Pt consumption for the 3
fleets,assuming 90 recycling of Pt from
discarded vehicles
73
Bottom-line on Pt constraint
  • A vehicle fleet reaching 5 billion (which would
    result from a human population of 10 billion with
    European levels of car ownership) and consisting
    entirely of FCVs would have a cumulative Pt
    demand by 2100 equal to the upper limit of the
    estimated amount of Pt that could be mined
  • This leaves no room for other uses of Pt (such as
    in jewelry and electronics)

74
4 ways of using solar-energy to power cars
  • Using solar electricity to charge batteries
  • Using solar electricity to make H2 for use in a
    fuel cell
  • Using solar energy to grow biomass that is
    converted to methanol and used in a fuel cell
  • Using solar energy to grow biomass that is
    converted into ethanol and used in an ICE

75
Steps, solar energy to battery
  • PV modules, 15 efficiency
  • DC to AC conversion, 85
  • Transmission, 96 (say)
  • Battery charging, 95
  • Drive train, 87
  • Overall sunlight to wheels energy transfer
    10.1

76
Steps, solar energy to H2 Fuel cell
  • PV modules, 15 efficiency
  • PV to electrolyzer coupling, 85
  • Production of hydrogen and compression to 30 atm,
    80
  • Transmission 1000 km at 30 atm pressure, 98
  • Compression from 30 to 700 atm pressure, 90
  • Fuel cell, 50
  • Drive train, 87
  • Overall sunlight to wheels energy transfer
    3.9

77
Steps, solar energy to methanol to fuel cell
(methanol is another candidate as a fuel for
fuel cells)
  • Photosynthesis, 1 efficiency
  • Biomass to methanol, 67
  • Transport, 98 (say)
  • Fuel cell, 45 (less than using H2)
  • Drive train, 87
  • Overall sunlight to wheels energy transfer
    0.26

78
Steps, solar energy to ethanol, used in an
advanced ICE
  • Photosynthesis, 1 efficiency
  • Biomass to ethanol, 67
  • Transport, 98 (say)
  • ICE, 20
  • Drive train, 87
  • Overall sunlight to wheels energy transfer
    0.11

79
Conclusion
  • Direct use of renewably-based electricity to
    recharge batteries makes far better use of the
    renewable electricity than using it to make H2 to
    for use in a fuel cell (extra steps mean extra
    losses)
  • The land area required to convert sunlight to H2
    and drive a given distance is 20 times less
    than growing biomass to make methanol for use in
    a fuel cell, or 40 times less than growing
    biomass to make ethanol
  • This is because the efficiency of PV modules (15
    or more) is vastly greater than the efficiency
    of photosynthesis ( 1)

80
Thus, the best bet seems to move to plug-in
hybrid vehicles that are recharged with solar- or
wind-generated electricity, with maybe a small
amount of hydrogen as a range extender in order
to eventually get completely off of fossil
fuelsLiquid biofuels would be a distant second
best as a range extender, but might be needed if
problems with H2 cannot be resolvedSwapping the
battery for a freshly charged battery every 100
km might be another solutionIn any case, the
underlying vehicle should be as efficient as
possible to minimize the electricity and/or
hydrogen or biofuel requirements.
81
Figure 5.34 Fuel-efficient cars
82
Figure 5.35 Drive-train cost components (NPVnet
present value)
83
Figure 5.36 Lifecycle costs for alternative
vehicles
84
Inter-City Rail Transport
  • French TGV (Train à grand vitesse)
  • German ICE (Inter-city express)
  • Japanese Shinkansen

85
Recall
  • Energy use to move people by cars is 2.5
    MJ/person km with 1 person per car, and projected
    to be 1 MJ/person-km with advanced future
    vehicles ( 0.25 MJ/person-km if you pack 4
    people into the car)
  • The energy required in todays high speed trains
    is 0.08 to 0.15 MJ/person-km

86
Figure 5.37 Energy intensity for successive
generations of the German Intercity Express (ICE)
high-speed trains
Source Kemp (2007, T618 Traction Energy
Metrics, Lancaster University, Lancaster,
www.rssb.co.uk)
87
Figure 5.38 Shinkansen energy use
88
Caveats
  • The savings are not quite as large as they appear
    to be, because high speed trains use electricity
    which will typically be generated at an
    efficiency of only 35-40
  • So, divide the (electrical) energy use by the
    train by (0.35 to 0.4 times the transmission and
    transformer efficiencies) to get fuel use at the
    powerplant that generates the electricity
  • Compare this with the amount of crude oil needed
    to produce the gasoline energy that is saved when
    people switch to trains. This will be the saved
    gasoline divided by the efficiency in making
    gasoline from oil, about 0.85

89
Caveats (continued)
  • The energy requirements for high speed trains
    increase rapidly with increasing speed beyond
    about 300 km per hour
  • The absolute time savings over a given distance
    gets smaller and smaller for each additional
    increment of speed
  • Faster trains increase total transportation
    demand so some of the passengers on the train
    are people who would not have travelled at all
  • Thus, careful market analysis is required to
    determine if the introduction of high-speed
    trains really does save energy

90
Aircraft Energy Use
91
Major types of aircraft
  • Turbojet
  • Turbo fan (popularly called jets)
  • Turbo prop

All three have, as their core, a gas turbine (the
gas turbines now used to generate electricity
using natural gas were derived from aircraft
turbines developed for the military)
92
In a true jet, all of the air thrown behind the
aircraft passes through the turbine, where
combustion of fuel occurs. This is found only in
military fighter jets
93
In commercial jet aircraft, most of the air
thrown behind the jet bypasses the turbine, as it
is accelerated by a big fan attached to the
turbine (this is what you see when you look at a
the engine of a commercial jet)
94
A third option is for the turbine to drive a
propeller that is in front of the turbine
95
The performance of an aircraft is represented by
the specific air range, which is the distance
that can be travelled per MJ of fuel energy used.
It depends on 3 factors
  • The amount of thrust produced by the engines per
    kg of fuel used
  • The aircraft drag for a given velocity
  • The aircraft weight

96
The thrust generated by the engine is equal to
the product of mass x velocity of the air thrown
behind the engineDoubling the mass of air
thrown and cutting its speed in half gives the
same thrust, but much less kinetic energy (which
varies with v2) needs to be added in this
caseThus, the engine needs to do less work
while producing the same thrust
97
This is why turbofan aircraft were developed
  • The larger the bypass ratio, the greater the
    amount of air that is thrown behind the engine,
    but the less it needs to be accelerated
  • This tends to make the engine more effective
  • However, this requires a larger engine casing,
    which increases the drag and weight
  • Thus, there is an optimal bypass ratio, which is
    where we are now not much further improvement
    can be expected

98
Figure 5.40a Trends in thrust specific fuel
consumption (fuel consumption per unit of thrust
generated smaller is better)
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
99
Figure 5.40b Trend in lift/drag ratio (larger is
better)
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
100
Figure 5.40c Trend in ratio of empty weight to
maximum allowed take-off weight (smaller is
better).
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
101
Observations from the previous figures
  • The big improvement has been in thrust specific
    fuel consumption (TSFC) decreasing by about 50
    for long-haul aircraft from 1959 to 1998,
    achieved in part through development of engines
    with larger bypass ratios
  • Turboprop aircraft have about 20 smaller TSFC
    than turbofan aircraft
  • No trend in lift/drag ratio improvements in
    overall aerodynamics have offset the impact of
    fatter engines with larger bypass ratios
  • A slight upward trend in ratio of empty to full
    weight related in part of extra in-flight
    entertainment systems

102
The energy requirement per passenger-km under
cruising conditions is equal to the reciprocal of
the (specific air range x seating capacity). It
is shown by the coloured (solid) symbols in the
next figure
103
Figure 5.40d Aircraft energy intensity (MJ used
per available seat-km)
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
104
Other factors affecting energy use per km
travelled by air travel
  • Distance the most energy-intensive part of the
    flight is the takeoff. On longer flights, this
    energy use is spread over more kms, reducing the
    average energy use per km
  • The airborne efficiency related to distance
    flown (and thus flying time) to the shortest
    distance between the starting and ending points
  • The ground efficiency the ratio of flying hours
    to total hours (including taxiing)

105
Figure 5.41a Ground efficiency for different
aircraft and distances travelled
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
106
Figure 5.41b Airborne efficiency for different
aircraft and travel distances
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
107
Figure 5.42 Energy intensity averaged over the
entire flight (including taxiing, waiting to take
off, circling before landing)
Source Babikian et al (2002, Journal of Air
Transport Management 8, 389400,
http//www.sciencedirect.com/science/journal/09696
997)
108
See Figure 5.37d again note the difference
between energy intensity while cruising (solid
symbols) and overall flight energy intensity
(open symbols)
109
Prospects for the future
  • Weight reductions through increasing use of
    C-fibre composite materials
  • 10-25 further improvement in engine efficiency
  • Overall reduction in fleet average energy use per
    passenger-km of 20-25 from 1995 to 2030 seems to
    be quite feasible
  • Shifting from turbofan (jet) to the latest
    turboprop aircraft for distances up to 1000 km
    also reduces energy use
  • The most efficient aircraft will still be many
    times as energy intensive as high-speed trains

110
Freight Transport
111
Figure 5.43 Freight transport modes
112
Figure 5.44 Variation of freight energy intensity
with distance transported, and difference
between modes of transport
Source Skolsvik et al (2000b, Study of
Greenhouse Gas Emissions from Ships, Appendices,
International Marine Organization, London)
113
Figure 5.45 Variation freight energy intensity
with capacity factor
Source Skolsvik et al (2000b, Study of
Greenhouse Gas Emissions from Ships, Appendices,
International Marine Organization, London)
114
Prospects for reducing road freight transport
energy intensity (that, reducing energy use per
tonne-km of transport)
  • Improved diesel engine thermal efficiency (from
    45 to 55)
  • Hybrid diesel-electric trucks 25-45 savings
    for delivery vehicles in urban settings
  • Elimination of idling in heavy trucks (averages
    about 2400 hours/year) through use of auxiliary
    power units such as fuel cells for air
    conditioning and other loads (high-temp fuel
    cells, not requiring Pt catalysts, could be used)

115
Prospects for reducing road freight transport
energy intensity (continued )
  • Improved aerodynamics
  • Improved loading factor
  • Reduced speed

116
Net resultA 50 or better reduction in the
energy intensity of freight transport by new
trucks is achievable over the next two decades.
More time would be required to see this
improvement over the entire fleet of trucks
117
Locomotives for Freight Trains
  • Ideal candidate for early application of fuel
    cells (on-board fuel storage and start-up time
    are not an issue)
  • Upfront costs less important than for passenger
    vehicles because fuel cost savings over a 20-30
    year lifespan are important

118
Figure 5.46 Locomotive energy flow with a diesel
engine used to generate electricity that in turn
drives an electric motor
119
Figure 5.47 Locomotive energy flow using a fuel
cell to generate electricity that in turn drives
an electric motor
120
Reducing the energy intensity of shipping
  • The International Maritime Organization has
    identified measures that could be phased in and
    which would reduce shipping energy intensity by
    37 over 20 years and by 45 over 30 years
  • Small wind turbines on a vertical axis (Flettner
    rotors) fitted to ships and connected to
    propellers could potentially reduce the remaining
    energy requirement by 30-40 (already used by the
    German wind turbine manufacture Enercon on the
    barges used to transport its offshore wind
    turbines to where they are installed)

121
Reducing the need to transport freight
  • The previous discussion has focused on the energy
    intensity of freight transport the energy used
    to transport a given amount of freight a given
    distance
  • Globalization and free trade deals have caused
    global freight movement to increase much faster
    than the growth of the global economy

122
  • This growth has depended on cheap fuel and
    unequal wages, worker benefits, and health,
    safety and environmental standards in different
    countries (and, in some cases, artificial
    exchange rates)
  • With the inevitable increase in fuel costs and a
    reduction in the differences between countries,
    the trend toward ever greater trade may very well
    be reversed, thereby contributing to reduced
    freight transportation energy use
  • Conscious effort by consumers to buy
    locally-produced products can also contribute to
    this

123
Impacts of e-commerce
  • Allows greater transport distances and greater
    delivery frequencies (tending to increase energy
    use), but can also be used to improve the
    distribution system
  • Can result in greater use of packaging
  • Can result in reduced warehouse building area by
    facilitating just-in-time delivery, thereby
    reducing warehouse energy use
  • Can permit electronic grocery shopping and home
    delivery services

124
To maximize the energy savings from e-shopping
and home delivery, a re-organization of the
relationship between suppliers, distribution and
collection centres, and retailers would need to
occur. This might happen spontaneously from the
need for improved logistics
125
Figure 5.48 Flow of goods from producers to
consumers at present (left) and as might occur
with an energy-efficient e-commerce arrangement
Source Bratt and Persson (2001, European Council
for an Energy Efficient Economy, 2001 Summer
Proceedings 3, 480492)
126
Box 5.1 Efficiency of a fuel cellThe
efficiency of a fuel cell is equal to the product
of three efficiencies
  • The reversible efficiency
  • The voltage efficiency (high operating voltage
    gives a larger voltage efficiency)
  • The Faradic efficiency (almost always 1.0)

127
Figure 5.29a Factors contributing to the
reduction in the voltage of a PEM fuel cell
compared to the theoretical maximum voltage
128
Figure 5.29b Variation of the efficiency and
power density of a PEM fuel cell with current
density. A smaller current density means that a
larger and hence more expensive fuel cell is
needed for a given power.
129
Figure 5.30a Variation of voltage of a PEM cell
with current density for operation at 50oC and at
different pressures.
130
Figure 5.30b Variation of voltage of a PEM cell
with current density for operation at 70oC and at
different pressures.
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