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I ' ' . --.- :··· ,"") .. :,. ,,I ';:: ··:·::,? ..,.- -- FRA-OR&O 75-63 PS-26 1-a 05 -- THE -- IMPACT OF THE U.S. ENERGY SITUATION ON HIGH SPEED GROUND TRANSPORTATION DECEMBER 1975 TECHNICAL REPORT Document is available to the public through the National Technical Informati on Servi ce, Springfield, Virginia 22151 Prepared for S.C.R.T.O. LIBRARY . FEDERAL RAILROAD ADMINISTRATION Office of Research . an·d Development Washington, D.C.

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Page 1: 1975 - Reports - THE IMPACT OF THE U.S. ENERGY ...libraryarchives.metro.net/DPGTL/usdot/1975-the-impact-of...capacity flexibility. In the long term, HSGT modes may have to adapt to

I

' ' . --.- :··· ,"") .. :,. ,,I

';:: ··:·::,?

..,.- --

FRA-OR&O 75-63

PS-26 1-a-·05 --THE--IMPACT OF THE U.S. ENERGY SITUATION

ON HIGH SPEED GROUND TRANSPORTATION

DECEMBER 1975

TECHNICAL REPORT

Document is available to the publ ic through the National Technical

Information Service, Springfield, Virginia 22151

Prepared for

S.C.R.T.O. LIBRARY.

FEDERAL RAILROAD ADMINISTRATION Office of Research .an·d Development

Washington, D.C.

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..

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TECHNICAL REPORT ST AND ARD TITLE P M, F

1. Report No. 2. Government Accrssion No. 3. Recipient's Catalog No. -----~-------.-----:---::---,-------·1 FRA-ORD & D 75-63

4. Title ond Subtitle

THE IMPACT OF THE U.S. ENERGY SITUATION ON HIGH SPEED GROUND TRANSPORTATION

7. Authorls)

5. Report Dote

December 1975 ---6. Performing Orgoni 1otion Code

8. · Performing Organization Report No.

Wi 11 <>.rd E. Fr.,,.a .... i.._z,.,_e _ _______ ___________ -+-...;:MTc:.=R:.:..-_;6::..:8:..:0:..:8::__ _________ ---l 9 . Perfo rming O rgoni2otio11 Nome ond Address 10. Work Unit No.

The MITRE Corporation, Westgate Park, McLean, VA 11. Contract or Grant No .

FR-30015 ---------------·-t--- --- ------- ---- - -------------------.1 13. Type of R.,port and Period Covered

12. Sponsoring Aguncy Nome and Address

Office of Research, Development and Demonstration Federal Railroad Administration

Technical Report

2100 2nd Street, S.W. 14 . Sponsor ing Agency Code

Washington, D.C. 20590 ~-----~~---------------- ----------'------------------15. Supplementary Notes

16. Abstract

U. S. energy supply issues for the next few decades are sunnnarized with a view toward their impact on high speed ground transportation (HSGT) modes. As background, the energy characteristics of intercity passenger modes, including 300 mph tracked levitated vehicle (TLV) systems, are presented and discussed. In the short and mid terms (through 1985 or 1990), energy shortages are seen to impact HSGT modes mainly through increased operating (fuel) costs; and the need for greater capacity flexibility. In the long term, HSGT modes may have to adapt to non-fossil fuels. Research topics for addressing energy impacts on HSGT are suggested.

17. Key Words

High Speed Ground Transportation, Tracked Levitated Vehicle, Energy

18, Distribution Statement

Document available to the public through National Technical Information Service, Springfield, VA 22151

~------ --------- ·- - -·•-·- ----·---- --- -----------.----------; 19 . Se c urrty Clossif . (of this report ) 20. Security Clossif . (of this page) 21, No. of Pages 22. Price

Unclassified Unclassified 41 ~----·---- ··---- -··- -···~-------··- ·- --- ------_._------_._----·-----· Form DOT F 1700.7 10-691

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01269

T . ...l . l. .:-: ·· . : ) -: ~_--_:_; ,. F -~-· ::?

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LIST OF ILLUSTRATIONS

INTRODUCTION

U.S. ENERGY SUPPLY

TABLE OF CONTENTS

U.S. TRANSPORTATION ENERGY CONSUMPTION

RAIL AND BUS SYSTEMS

TRACKED LEVITATED VEHICLE SYSTEMS

IMPACT OF ENERGY SHORTAGES ON HSGT

RESEARCH TOPICS

REFERENCES

APPENDIX A: CONVERSION FACTORS

i

Page

ii

1

3

13

21

25

33

37

39

41

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LIST OF ILLUSTRATIONS

Figure Number

1

2

3

4

5

6

7

8

9

10

11

12

13

14

Energy Flow Patterns in the U.S.A.-1970

"Supply/Demand" (1960-1985) B/D Oil Equivalent

U.S. Energy Future Without Self-sufficiency

Self-s ufficiency by 1980 Through Conservation and Expanded Production

Approximate Supply/Price Scale for Petroleum and other Fos~il Fuels (Suggested by the Hudson Institute)

U.S. Transportation Energy Distribution by Mode (1970)

Distribution of Transportation Energy by Mode

Distribution of Transportation Energy by Purpose

Historical Variation in Energy Intensiveness for Passenger Modes .

Cruise Energy Intensiveness, Bus and New Rail

Motive Power Requirements for TLV Systems

Specific Energy Requirements for Various Transportation Modes

Distribution of U.S. Domestic Air Travel, 1968

Modal Comparison of Fuel Economy

ii

4

5

6

8

9

14

17

17

18

22

26

28

29

31

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LIST OF l:LLUSTRATIONS ' (Continued)

Table Number

I

II

III

U.S. Transportation Energy-1970

Reported Modal Fuel Economy ,

Energy Crisis Cost Factor~

iii

Page

16

20

34

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.

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INTRODUCTION

The purpose of this paper is to sunnnarize the current U.S. energy

supply situation and recent government projections for the future, to

describe the energy characteristics of U.S. transportation modes,

to discuss the potential impact of energy supply changes on high speed

ground transportation (HSGT), and to delineate those R&D areas

essential to acconnnodating HSGT to future energy situations. The intent

is not to present a thorough analysis of U.S. transportation energy

issues, but rather to provide a working paper that can stimulate

discussion on the topic.

1

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U.S. ENERGY SUPPLY

The overall energy flow pattern for the United States in 1970 is

comprehensively illustrated in Figure 1, which shows energy sources,

energy consuming sectors, and energy use efficiency (fraction of

consumed energy which performs the intended function - moving a

vehicle, heating a building, driving an electric generator, etc.).

Nearly 25% of all U.S. energy is consumed by the transportation sector,

more than 95% of it in the form of petroleum and natural gas liquids.

An insignificant portion of transportation energy is supplied as

electric power. Electric power is almost entirely dependent on fossil

fuels as the energy source; less than 2% of the electric power generated

in 1970.was dependent on nuclear energy, while 6% was hydropower.

Projections of energy supplies for the future involve many assump­

tions which make all projections necessarily tentative. Nevertheless,

projections, such as that shown in Figure 2, are essential to the

planning process. Figure 2 shows projected supply, by domestic source,

and projected demand through the year 2000. The difference in the

demand/domestic supply projections represents imported energy require­

ments and/or shortages. Shortages will be accommodated through con­

servation and other demand-reducing measures.

If conservation were not employed and the energy demand curve of

Figure 2 continued to rise, the U.S. energy future might be as portrayed

in Figure 3. Such a projection, from a recent report of the U.S.

3

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GEOTHERMAL 0.007

HYDROELECTRIC 0.85

NUCLEAR 0.24

NATURAL GAS

24.3

1.0

22.6

NATURAL GAS LIQUIDS

22.0- -

IMPORTS

ELECTRICAL CONVERSION ANO LINE LOSSES 9.8

ENO USES

RESIDENTIAL/

- ~ COMMERCIAL -<:.: 15.9

- - - - 15.6

INDUSTRIAL 21.0

NONE'N'::RGY

4.0

TRANS­

PORTATION 16.3

FIGURE 1

REJECTED

31.2

All VALUES ARE

IN UNITS QF 1015

BTU. TOTAL PRO­

DUCTION= 71.6 x l015 BTU

CONVERSION:*

I BTU= 1055 JOULE

1rA MORE COMPLETE TABLE A~EARSATTHEENDOF THIS PAPER.

SOURCE, AUSTIN ET AL. LAWRENCE LIVERMORE LABORATORIES, 1972

ENERGY FLOW PATTERNS IN THE U.S.A.-1970

-

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"SUPPLY/DEMAND" 11960-19851

1/D Oil EflUfYAUNT n YEARS 80 .------,------r-----~----~-------,,-----~---~ 80

70

60

!,O

LU 0 0 (lJ

z 40 ~ ....I ....I

i

30

20

10

SOURCE:

CONVERSION:

B/DOE BARRELS PER DAY

OF OIL. EQUIVALENT

1 BARREL (42 GALS.)~ .159rn3

"SURPLUS OIL"

I ---,/

EARLY I - -EST. .-- .--

.--RECENT I

EST.

YEAR

"UNDERSTANDING THE NATIONAL ENERGY DILEMMA", A REPORT OF THE JOINT COMMITTEE ON ATOMIC ENERGY,

--

15 AUGUST 1973. FIGURE 2 "SUPPLY/DEMAND"

(1960-1985)

•GEO.

NUCLEAR

DOM. GAS

~

COAL

SHL. OIL ALASKA -----lJOM . OIL

..... L '85

B/O OIL EQUIVALENT VS YEARS

5

70

60

50

40

30

20

10

(I

LU 0 e al z 0 ::; ....I

i

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130

110

~ 90 µ:l

~ H :::> O' µ:l

ci 70 0

~ ~ -Cl)

,-l

; 50

z 0 H ,-l ,-l H 30 ~

10

1970 1980

SOURCE:

Conversion:

1 barrel (42 gal.)= 3 .159 m

DOMESTIC NONFOSSIL ENERGY

IMPORTED FOSSIL ENERGY

DOMESTIC FOSSIL ENERGY

1990 2000 2010 YEAR

2020 2030 2040 2050

AEC, THE NATION's ENERGY FUTURE, December 1973

FIGURE 3 U.S. ENERGY FUTURE WITHOUT SELF-SUFFICIENCY

6

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Atomic Energy Commission (AEC), acknowledges growing reliance on im­

ported fossil energy and assumes a nearly steady supply of domestic

fossil energy (relying heavily on increased use of coal and, possibly,

oil shale) combined with rapid growth in domestic non-fossil energy.

If, however, the U.S. were to become self-sufficient from an energy

standpoint by 1980, the AEC report suggests, in Figure 4, how this

might be done through a combination of energy conservation and expanded

domestic fossil and non-fossil energy production. Conservation efforts

would have to reduce formerly projected imports by 1/3 by 1980, while

increased domestic energy production would account for the remaining

2/3. Since formerly projected energy imports for 1980 amounted to 25%

of projected energy demand, then conservation strategies, if self­

sufficiency is to be realized by 1980, would entail an 8% (1/3 of 25%)

reduction in projected demand by that year. Because transportation

accounts for 25% of all U.S. energy consumption, conservation measures

of this magnitude will have a major impact on the evolution of trans­

portation systems over the next decade or two.

The need to introduce non-petroleum fuels into our energy supply

to meet expected demand over the next few decades raises the prospect

of alternative fuels to which transportation systems must adapt. The

availability of new domestic fossil fuel sources, in the short and

mid terms (1974-1980 and 1980-1990, respectively) will be a function

of world oil prices. Figure 5, suggested by the Hudson Institute at

a recent symposium at the MITRE Corporation, indicates an approximate

7

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12

9

6

3

0 .:;....___,;._.____......_ _ __.__..._ _ _,,_,.___~L--'--.....,__;L------'-'.___..__,..___......._.__

1973

Conversion:

1 barrel (42 gal.)

IMPORT REPLACEMENT

1975

3 = .159m

1977 YEAR

(Million Barrels/Day Oil Equivalent)

Formerly Projected Imports

Conservation Savings*

Expanded Domestic Nonfossil Production

Expanded Domestic Fossil Production

1979

1973

6.5

YEAR

1980

1980

12.0

4.7

1.5

5.8

*Includes both conservation techniques and energy real price increases.

SOURCE: AEC, THE NATION's ENERGY FUTURE, December 1973

FIGURE 4 SELF-SUFFICIENCY BY 1980 THROUGH CONSERVATION

AND EXPANDED PRODUCTION

8

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9 I COAL LIQUIFICATION ,..:i

ij 8 OIL SHALE

OIL SANDS ,::Q

7 -<n-.. I ALASKAN FIELDS i::,:J 6 I TERTIARY RECOVERY OFFSHORE WELLS u H STRIPPER WELLS ~ p... 5 ,..:i H 0

4 I u .s. & REST OF WORLD PRESENT PRODUCTION

3

2 I MIDDLE EAST PRODUCTION

SHORT TERM MID TERM

FIGURE 5 APPROXIMATE SUPPLY/PRICE SCALE FOR PETROLEUM AND OTHER FOSSIL FUELS

(SUGGESTED BY THE HUDSON INSTITUTE)

9

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supply/price scale for new petroleum and other fossil fuels. The

Middle East oil is a large supply and the cheapest to produce; it is

the only fossil fuel that can be produced at a profit for a price as

* low as $2 to $3 per barrel • Production from the U.S. and most of

the rest of the world is more expensive than Middle East oil. At

a price of $5 to $6 per barrel, it becomes profitable to work small

producer "stripper" wells and to stimulate existing wells to greater

production. In the same higher price range, new Alaskan and offshore

supplies could be brought in. Finally, at a price of $7 to $9 a

barrel, working of oil sands, oil shale and coal-based liquid fuels

begins to look profitable.

None of the alternative fossil fuels indicated in Figure 5 will

affect transportation systems except, of course, by way of increased

unit costs for fuel. The various required grades of fossil fuels now

in use (gasoline, kerosene, diesel fuel, etc.) can all be produced

from oil sands, oil shale, and coal. With the potential growing use

of non-fossil energy sources (nuclear, solar, geothermal, etc.) there

is the prospect that non-fossil energy may have to be used by the trans­

portation sector, particularly if unforeseen extraction or environ­

mental problems make the use of coal and oil shale impractical. With

abundant electric and/or solar power available, the possibility of

using alcohol (methanol) and hydrogen as alternative transportation

fuels needs to be considered. The potential for using stored electric,

* The current price of $11 to $12 per barrel for Middle East oil is artificially high, and does not reflect production cost.

10

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* mechanical, and high temperature thermal energy in transportation

systems also needs study. Alcohol, while more expensive and lower in

specific energy content than hydrogen, offers the advantage of con­

venient storage and transport as a liquid. Hydrogen suffers from

inconvenient and costly storage and handling problems, but is otherwise

a potentially viable alternate to fossil fuels. The unique safety

aspects of hydrogen as a fuel must be addressed. Hydrogen, the cleanest

burning of all chemical fuels, could well permit the use of on-board

power generation for intercity ground transportation systems in dense

urban corridors where air quality standards would otherwise force the

use of wayside electric power. Of all transportation modes, large

aircraft appear to be the best suited for use of hydrogen as a fuel.

Electric, mechanical, and thermal stored energy systems are clean

and compatible with total energy systems, but require major improvements

in energy density before application to intercity systems can be

considered.

* N.V. Philips Aachen Laboratory, Federal Republic of Germany, has pioneered recent advances in storage of thermal energy as the heat of fusion in fluoride eutectic salts. Hp to 10 times the energy density of the lead-acid battery have been achieved.

11

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U.S. TRANSPORTATION ENERGY CONSUMPTION

The 1970 distribution of energy among the various transportation

modes for freight and passenger servic'!e is displayed in Figure 6.

The energy considered here is only the operating fuel energy. As

Dr. Hirst has demonstrated (Ref. 7) the total energy associated with

a mode should account for its manufacturing energy input, the energy

associated with distributing, maintaining, licensing, housing, and

insuring the vehicles, as well as the fuel energy required to operate

the system. For the automobile, Dr. Hirst calculated that the total

energy consumed by the automobile on the above basis is nearly twice

the operating fuel energy requirement.

Looking only at fuel energy, Figure 6 shows that better than half

(56%) of transportation fuel energy is consumed by the automobile,

with urban auto usage consuming the larger share. Note that light

trucks when used for personal transportation are included in the

statistics for the automobile. Freight consumes nearly 25% of all

transportation fuel, with two-thirds of this amount going to trucking.

Thus, the fuel consumed by all highway vehicles is three-quarters of

the total for transportation. Eleven percent of the total goes

to recreational vehicles, general aviation, and the military, with the

military consuming by far the largest share. The air passenger mode

consumes about 7%, several times what bus and passenger rail together

consumed. Auto and air are the dominating energy consumers, in the

aggregate, for intercity travel.

13

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*INCLUDES p OF LIGHT TRERSONAL USE UCKS

DATA SOURCES· • MOTOR VE. • HIRST HICLE MANUFA • srnoM:t:Jt ]!12 124) crnnrns Assoc.,

1972

• AMERICAN TRANSNUARY 1973 (25) • CIVIL A IT ASSOC • CAMPB/L~ONAUTICS BOAR ii 11971-1972 (26) • MALLIAR , APRIL 1973 (28) , 971 (27)

IS & STROMBOTN . E,JEBRUARY 1973 (29)

SOURCE: FRAIZE ET THE MIT AL, FEB .•

74 RE CORP.,

U.S. TRANSPORTATION FIGURE 6 ENERG y DISTRIBUTION B . 14 y MOOE (1970)

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..

A more detailed analysis of transportation energy consumption,

again for 1970, is given by Table 1 which presents not only the energy

consumption for each mode, but the useful transport work (passenger­

miles or ton-miles), the load factor, and the energy intensiveness

(Btu/pass. mi., or Btu/ton mi.). Energy intensiveness is the energy

consumed per unit of useful transport work (passenger-miles or ton-miles),

and is,therefore, inversely related to a transport mode's efficiency.

The historical trends in U.S. transportation energy consumption

are displayed in Figures 7 and 8. Figure 7,showing the energy dis­

tribution according to mode, displays the growth in highway and air

modes at the expense of a declining rail mode. A portion of the

decline in railroad energy consumption is due to the improved efficiency

of the diesel engine locomotives which were replacing the relatively

inefficient steam locomotives in the early part of the period. Figure 8

displays the growing fraction of transportation energy consumed in

passenger service (60% in 1970).

The efficiency of energy use is expressed either in terms of energy

intensiveness (energy consumption per unit of useful transport work,

such as passenger miles, seat miles, ton miles, etc.) or in terms of

fuel economy (e.g., seat miles/gal., pass. miles/Ral., ton milP.s/

gal., etc.); one is the inverse of the other. The historical trends

in energy intensiveness (Btu/pass. mile) for U.S. passenger modes

between 1950 and 1970 is presented in Figure 9. In this period, the

only significant changes in energy intensiveness occurred for the

15

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TABLE I U.S. TRANSPORTATION ENERGY-1970

MOnf TRANSPORT WORK l OAll FACTOR

(Pass.Mi. or Ton mt I

PASSENCER SFRVln

Auto Urh,Ul G9x 10 17 1 4 pas5/vP-h.

tnt1•1cI1v Alf(ANATf

I 04 20

( Srn;tlt ,·dr-, )URf-/\KDOWN (J;i 19

Simi & 1:omp,1cl c;ns ID AlJlO MOD[ 1 73 19

I 1qh1 Tnu.:k 08 1.4

A" Short haul f • !JOO rm ) 018 Long haul I bOO nu I ..!Ql i\lfl MODf 119 119'½,

Hu, \J1b,ln 017 1 Q prl~'i/vPh

ln1eri:11y .028 22

School .062 25 BUS MOOE 097 19.2

H,i1I Urban 007 2s·v., Intercity 011 37% RAIL MODE .018

ALL PASSENGER SERVICE 20Mx 10 12p,t<.\ nu

f REIGHl SERVICE Truck S1nqle Umts 15 1.09 ton mi.I

vch m1.

Comh1nat•ons ALTERNATE

.35 9 21

( ~~::llfl!~r~::p: ) BREAKDOWN ( .39 ) 11

TRUCK MOnE 50 HJ H,ul 17

Au 004 P1pt!lllll! 43

I ~•1,,te1way 60

2~:.: 10 1210n mt 1\L L FREIGHT SERVICE

OTHFA

Gener di Av•dllOll

Rt'P1!<Hlonal Vehicles M1l1ldl',,'

TOTAL TRANSPORTATION

O<1ta Sou,ces • Motor Vehicle Manuf1teturers A!!,SOC., '72 ! 14)

• Hirs1, Man:h '72 !24) • Stromhomo, Jan. '73 (261 • MHlham & Strombntne, Feh ·7:4 (29) • Ame11r.an Trnn,11 Assoc., 'JI ·n (261

• Camphell, April '73 128) • Civil Aeronau11cs Boartt, 1971 (27)

CONVERSION:

1 BTU = 1055 JOULE

1 TON= 907.2 KG

1 MILE= 1.609 KM

1 TON MILE~ 1460 KG KM

1 BTU/PASS Ml = 656 JOULE/PASS-KM

1 BTU/TON Ml= .723 JOULl;/KG-KM

16

ENERGY INTENSlVENf.SS fBtu/paH.nH or Btu/Ion ni1 )

(Al current load lac101)

7550 ( 12 1 mpg)

3250 I 16 0 mpql 3220 i212mool 5300 t12.9m119)

4980 113.6 mpyl 9000 I 10 1 mpgl

1noo 8120 9300 2940 I 4 4 rnpq)

10/0 I S.f> mpg)

770 I 6 75 mpgl t240 I 5 5 mnql 4300 2730 3330 --5250 Btu/pas'i rTu

10650 Btu/Ion m,

3440

5600 676

37500 420 750 --

1780 Btu/ton m1.

ENERGY CONSUMPl lON

11015 Btul

Ad1ht1ve

Suhrotals Totals

5 2 3.4

( 7 ~~ )

~ 8 fi

n 72 BB

110 1 10 .06 03 04

""i2 12

.03 03

06 06 -10 6

1 6

1 2

Ia ?H 52 15 1H 45 -

4 1

10 ,o

1 5 -16 5

SOUl~Cl FRAl/'f, W. !_, r T AL. THE MITIH COHP., FF.8. 1914

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"

--r '

/ /

,_ w mu "

/ /

u --, ([J

>-.., a: w z w 2 Q ,_ ;' a: 0 a. 50 V, z <t "-,_ _J

<t :, z z <t .. n . . , w ,, er w

" 1960

I I

I I

I /-

,/

I

I I

I 15

1-­w .., 0 -::>

"' >-10 ~

w z w

~ ~ a: 0 a. V, z <I a: t--

5 ;j ::, z z <I _J

<I

o t--

t--~ ,oo a ::, (Il .,,, >-.., a: w z w z Q t--;:! a: 0 CL 50 V, z <I a: t--__J

<I ::, z z <t ... 0 t--z w u a: w a.

ORNL-DWG 72-15~9~ r ------------

I I

I I

I

,✓/-,I

/ /

/ -~---~,, --.,..,,, OTHER

INTER-CITY FREIGHT

1960

I I

I 15

,n

g t--­w .., 0 :,

<D

>­.., 10 er

w z w z 0 .= ;:! a: 0 a. V, z <t a: t--

5 ;j ::, z z <I _J <[ t­o t--

FIGURE 7 DISTRIBUTION OF TRANSPORTATION

ENERGY BY MODE

FIGURE 8 DISTRIBUTION OF TRANSPORTATION

ENERGY-BY PURPOSE

CONVERSION:

l BTU= 1055 JOULE

SOURCE: HIRST, E., ENERGY INTENSIVENESS OF PASSENGER AND FREIGHT TRANSPORT MODES, 1950-1970, OAK RIDGE NATIONAi,... LABORATORY, REPORT ORNL·NSF-EP-44, APRIL 1973.

17

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~ .E I

---Q)

O' C Q) 1/1 1/1 0 a.

' ::, (I)

(/) (/) w z w > (/)

z w I-z >-(.'.)

a:: w z w

8000 -

6000

4000 --

2000

0 1950

ORNL-DWG 72-11918

URBAN AUTO

URBAN MASS TRANSIT

INTER-CITY AUTO

RAILROAD

1 1960 1970

FIGURE 9

CONVF HSION,

I A TU/PASS Ml ~ 656 JOULE/PASS KM

SOUllCf, HI RS I, E., OP. Cl r ., APRIL 1913

HISTORICAL VARIATION IN ENERGY INTENSIVENESS FOR PASSENGER MODES

18

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intercity mass modes:

• energy intensiveness for air increased rapidly (by a factor

of 2) with the advent of higher speeds made possible by the

commercial jet engine around 1960;

• energy intensiveness for rail declined rapidly in the first

half of the period (1950-1960) as steam locomotives were phased

out;

• intercity bus became less efficient as highway speeds

increased.

The energy intensiveness (or fuel economy) on a passenger mile

basis incorporates the effect of load factor; energy usage on a seat

mile basis allows comparison of system potential performance without

regard to load factor and is, therefore, a more objective measure

for comparing transportation vehicle systems on an energy basis.

The fuel economy for a number of passenger modes, as reported by several

investigators, is sunnnarized in Table II. Both seat-mile/gallon and

passenger-mile/gallon bases are used. Table II illustrates the

difficulty in obtaining consistent values of fuel economy for a given

mode. Not only is there the obvious difference between passenger

miles, seat miles, and vehicle miles (the effects of load factor and

vehicle seating configuration, both of which affect the quality of

service in a direction opposite to fuel economy), but also the differences

in vehicle speed, cruise performance versus overall duty-cycle perform­

ance, measured versus calculated performance, and reliability of data

sources that must be taken into account.

19

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'l'AHLE I l

REPORTED MODAL FUEL ECONOMY

'

INVESTIGATOR DOT/TSC DOT/OTEP RICE (Reference) (1) (2) (3)

UNITS PSGR PSGR SEAT mpg mpg mpg

AUTOMOBILE SUBCOMPACT

AVERAGE )0 30 61,

INTERCITY BUS 110 104 215

TRAIN

CROSS COUNTRY 50 150• 144

METROLINER 75

COMMUTER 200

SUBURBAN 400

Al Rl'LANE

WIDE l\ODll-:ll .IE'I' 40

AVERAt:E 16 JI, '14

SOURCE: For Tabll' LI - Nutll'r, k. D., "A Perspectivt.• on Transportat lon Fuel Economy," The Ml TRE Corpora­tion, March 1974.

REFERENCES FOR TABLE II

' HIRST HIRST

' NCHP

(4) (5) i, (6)

PSf,R PSGR PSGR mpg mpg I mpg

i I

12 ]8 i )2

]25 82 ! 125

I

80 1+6 80

100

200

l2

14 I h 71

I

DOT /OST FRAIZE (7) (8)

SEAT SEAT mpg mpg

JOO LOO

'JOO 250

210 210

'

(i'j

'>2

i 'lb

LIEB AUSTEN (9) (10)

SEAT SEAT mpg mpg

85 91

78

270

22

seot mile/gal E

42', seat km/m3

MOOZ (11)

PSGR mpg

25

78

50

18

1. Transportation Systems Center, "Transportation F.nc._•rgy Conserv,Hlon Options," (DRAFT) DiscuRsion PaperR, Report No. DP-SP-11, October 1973.

2. U.S. Department of Transportation Energy Policy, U.S. DOT (Lnfurmal pl..rnning papers), November 1973.

J. Rice, R. A., "System Energy as a Factor 1n Considering Future Transporlatlon," /\SHE pap,•r 70-WA/Ener 8, December 1970.

4. Hirst, Eric, "Energy Consumption for Transportation lu the U.S.," 0;1k Ridge National Laboratory, ORNL-NSF-EP-15, March 1973.

5. Hirst, Eric, 11 Energy l ntens 1 vencss of PARHP.ngl" r and Freight Transportat 1 on Modet. 1 ORNL-NSF-EP-44, April 1973.

6. National Commission on Materials Policy, Final Report, June 1973.

7. J.S. DOT, Office of tht.• Sl•cret.,ry, "High Speed Ground Transportation /\ltl"rnatlves Study,"· January 197'1.

8. Fraize, W. E., P. Dyson, S. W. Gouse, Jr., "Energy nnd EnvlronmC'nlal AspeclH of U.S. TrnnHportntion, MITRE pnper MTP-191, February 1974.

9. l.leh, J., MITRF. lnt,•nrnl memorandum D2J-M2'18A, .July 197'\.

10. Austen nntl Hel lnum, 11P11HH1•11gt•r C:;1r VtlPI l~cnnomy--'l'ri•1u1~; and lnf)uc>nclny, Fat'lllrH," SAE paper 1)0790,

Sl•ptl•mht•r 197].

11. MllOZ, W. 1-:., "Em•rgy Trend:--i and Tlwlr Futurf' i-:fre(·ls llpnn Tr,rnHporrat llin," HAND Corporntion Pllpf'r l'-5046, ,luly '1073_

12. FLIGHT Internn~ional, "Wht•re llil!'-1 all rhe Fuel Cone," N11vl·mbt.>r 1973- Ntl'J'I•:: v:!111l'S f<1r Ettru~w:rn Vl'hkl1'S.

20

FLIGHT (12)

SEAT mpg

120

450 .. 393

57-68

4 l

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' .

RAIL AND BUS SYSTEMS

The impact of speed for intercity bus and new rail systems is

demonstrated in Figure 10, which shows cruise energy intensiveness

(But/seat mile) as a function of cruise speed. Figure 10 illustrates

several factors that bear on the energy consumption of bus and rail

systems:

• At high speeds (above 50 mph) aerodynamic drag predominates

for rail systems (the same is true for bus, but is not

illustrated by calculation in Figure 10).

• On the basis of cruise performance, a rail system can, for the

same energy expended per seat mile, operate at twtce the

cruise speed of highway vehicles (i.e., bus). The major rea­

sons for the cruise energy advantage of rail over bus are:

•• Reduced rolling friction (steel wheels on rail yield 1/10

the rolling resistance of rubber tires on concrete).

•• Better fineness ratio (volume to frontal area) and, hence,

lower aerodynamic drag for rail compared to bus.

• Because of the relatively small effect of vehicle weight on

cruise performance of rail systems, rail vehicles can be con­

siderably heavier in terms of weight/seat than bus, thereby

providing greater flexibility in vehicle design, including

the option for more spacious seating and other on-board

passenger services. However, vehicle weight exacts an energy

cost in actual duty cycles which include acceleration and

21

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"' "'

.. • .. C

! .. • ! ~ >

! .. ! ►

" 0:

!

1aa,

-

NOTE

• GREV>-tOUND MC-7 ANO IPT CURVES ARE CALCULATED. • TURBOTAAIN & METROLINEA PERFORMANCE IS

CALCULATED USING SOME EMPI AICAL OAT A TO JUSTIFY DRAG COEFFICIENTS.

• TGV PERFORMANCE 15 A PROJECTION OF THE FRENCH NATIONAL RAILWAY iSNCF) BASED ON TEST DATA FOR THE TGVOOl EXPERIMENTAL TURBOTAAIN (RAILWAY GAZETTE INTERNATIONAL, SEPTEMBER 1973).

• HST PERFORMANCE IS BASED ON INSTALLED POWER ANO ATTAINED TEST SPEED (RAILWAY GAZETTE tNTERfl,jATIONAL. SEPTEMBER 1973)

• ROHR TURBOT RAIN DATA 15 FROM AVIATION WEEK, 2c JUNE 1974.

GREYHOUND BUS 1«:-7 47SEATS 711 LB/SEAT

,.P.o' .-.1~f."'

,..,:,:z.'\) ,,t-,.1.Co

~ff\'-

50

CONVERSION CRUISE SPEED. IIPH

1 LB '536KG

I MPH 1 609 KM HR

l MPG 425 KM.'",t3 FIGURE 10

100

1 BTu,sEAT MILE= 656 JOULE/SEAT MILE CRUISE ENERGY INTENSIVENESS, BUS AND NEW RAIL

IIETROLINER 312SEA1S Z75G LB/SEAT.

TURBOTRAIN -SEATS 118& LWSEA T

150

0 ..... RllJRaJTRAIN J1•SEATS 1910 LB/SEAT

-SEATS -UIISEAT

IWtlO'ft.O PASSBmE.R TRAIN (IPTI :m&EAT 1415 LIi/SEAT

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grade requirements. Therefore, weight is not an insignificant

factor by any means, and attempts to reduce weight are a major

goal of all new high speed rail development efforts.

• The propulsion system efficiency has a direct effect on energy

consumption (not motive power); the IPT model assumes an efficient

regenerative gas turbine having an overall efficiency (engine

plus transmission) of 28%; for the Turbotrain, using an air-

craft gas turbine, the overall efficiency is approximately

16%; for the electrified Metroliner, the overall conversion

efficiency is approximately 25%.

In addition to rolling resistance and fineness ratio, which affect

cruise performance, rail systems have two other inherent energy-related

advantages over bus:

• Rail rights-of-way are generally more levtl than highway,

• Rail travel involves less stop and start in getting out of a

terminal and onto the main right-of-way than does bus.

As opposed to the inherent advantages of rail systems, as listed

above, there are several practical operating characteristics of rail

systems which tend to increase their energy intensiveness:

• Most passenger trains use electric drive, either diesel-elec­

tric or wholly electrified. The efficiency of the mechanical­

to-electrical-to-mechanical conversions is lower than direct

mechanical transmission used in the bus. On the other hand,

the larger train diesels work under more nearly constant load

23

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and can therefore achieve a higher efficiency for the prime

mover. The effects will tend to compensate.

• Rail coach seating is far less dense than bus. In general,

rail seating approximates first class air while bus approxi­

mates economy class air in seats per unit of floor space.

• Intercity trains frequently carry baggage cars, dining cars,

and lounge cars which are normally not included in seat-mile

estimation. Parlor cars and sleepers are very low density

seating vehicles.

• Rail costs have been dominated by fixed costs and labor costs

so that strong incentives for fuel economy have not existed

as has been the case for bus.

24

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TRACKED LEVITATED VEHICLE SYSTEMS

In the High Speed Ground Alternatives Study (Ref. 15), prepared

by the MITRE Corporation for the U.S. DOT, the cruise performance and

energy cost of improved rail systems and tracked levitated vehicles

(TLVs) were estimated. Both magnetically levitated (MAGLEV) and air­

cushion levitated vehicle concepts were considered. For all TLV sys­

tems, the motive power requirements, based on the state-of-knowledge

as of late 1972, were calculated. The results are shown, as a function

of cruise speed, in Figure 11 for three hypothetical 300 pass~nger,

300,000 lb. (136,000 kg) gross weight vehicles:

• Tracked air cushion cehicle (TACV) using static air cushions.

• Tracked repulsion MAGLEV vehicle using on-board superconducting

magnet coils.

• Tracked attraction MAGLEV vehicle.

On the basis of power alone, this comparison shows a decided ad­

vantage for the attraction MAGLEV system, because the magnetic drag is

estimated to be considerably less than the comparable suspension-related

drag for either of the other two systems. For all systems, aerodynamic

drag is the same. For TLV systems, support and guidance power is rela­

tively large, compared to _the rolling resistance of rail systems (see

Figure 10). At 300 mph cruise, aerodynamic drag accounts for only 54%

of the motive power requirements for the TACV. The corresponding per­

centages for repulsion and attraction MAGLEV are 59% and 76% respect­

ively.

25

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20

15 ~ MOMENTUM DRAG .,

10 AIR SUPPLY COMPRESSOR

5 AERODYNAMl C DRAG

0

20

REPULSION 15,000 ,....

15 MAGLEV - } MAGN£TIC ~ DRAG & M CRYOGENIC 0 .... 10 POWER .....

I 5 AERODYNAMIC ~

\ DRAG '\ .... ~ 0 FOPI ALL SYSTEMS:

300 PASS,

20 300,000 LB. GROSS WT. 126 FT.2 FRONTAL AREA

ATTRACTION .40 DRAG COE FF. 15 MAGLEV

10

5 AERODYNAMIC DRAG

0 0 100 200 300

SPEED (mph)

CONVERSION: SOURCE: U.S. DOT; HIGH SPEED GROUND

ALTERNATIVES STUDY,

1 LB • .4536 K9 JANUARY 1973,

1 FT2 • .0929 M 1 HP - .7467 KW 1 MPH • 1 .609 I( M/H Pl

FIGURE 11 • MOTIVE POWER REQUIREMENTS FOR TLV SYSTEMS

.26

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The 300 mph cruise performance for the TLV systems is shown in

comparison with other modes in Figure 12. Each system is shown at

its rated cruise speed, and for each,the energy intensiveness (Btu/

seat mile) has been estimated. The aircraft data include the estimat­

ed energy for the landing/take-off (LTO) cycle, because the LTO

energy, at least for short-haul trips of 300 miles (483 km) or so is

not negligible. Figure 12 indicates that future TLV systems can

effectively compete, on an energy per seat-mile basis, with short­

haul aircraft while offering a cruise speed of 300 mph (483 km/hr)

(as opposed to 565 mph (910 km/hr) for short-haul aircraft). In

intercity service, TLV sytems can provide city-center to city-center

service so that the door-to-door time for TLV and short-haul may be

comparable in spite of the significant difference in cruise speed,

The role for TLV systems as an alternate to short-haul air

service in congested corridors will not involve significant savings

in the total transportation energy budget for the United States.

Figure 13 shows the cumulative distribution of fuel consumed and

passenger miles for scheduled U.S. domestic air travel for 1968.

If, for example, all air traffic for trips below 500 miles (810 km)

in length were picked up by TLV systems, the maximum fuel savings

involved would be less than 20% of the air mode fuel budget, or less

than 1.5% of the nation's transportation energy budget.

Thus, while total energy savings will not likely, by itself, be

a strong justification for TLV systems, there will be many situations

27

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N ::c

AUTO, 4 PASS., 60 MPH

i>>>>>>-.,, ,:::,y::,::,,::,,>,::,,,,, > >>I AMTRAK METROLINER, 382 PASS.

150 MPH I 170 MPH I TURBOTRAIN 144 PASS.

R&O UNCERTAINTY

ALL ENERGY ESTIMATES ARE FOR CRUISE ONLY, EXCEPT FOR AIR MODES FOR WHICH LANDING/ TAKE-OFF(LTO)ENERGYISINCLUDED

SOURCES: GROUND MODES-U.S. DOT (321 DC-9-30-MCDONNELL-DOUGLAS (33) 8747-WEISS (34) L TO DATA-EPA (35)

TRACKED LEVITATED VEHICLE (FUTURE): 300 MPH

I',,,, ,::,::,:,:,:,:,:,:,:,::,:,y,::,;,::,.;:,,::,::,::,,,,,,, ,::,::,,::,,,,,,,, ,,,,,,::,,::,::,,::,::,::,::,::,::,::,::,,1c < < 4 8747, 2760 MILE TRIP, INCLUDING L TO CYCLE, 315 PASS., 580 MPH

0 .5 1.0

CONVERSION:

1 BTU1SEAT MILE== 656 JOULE 1 SEAT KM

1 MPH== 1 609 KMtHA

1 FT"" .3048M

1.5 2.0 2.5

SPECIFIC ENERGY, 103 BTU FUEL/SEAT MILE

FIGURE 12

3.0 3.5

SOURCE: FRA1ZE, ""· E. ET AL, THE MITRE CORP., REPORT MTP-391 FEBRUARv 1974

SPECIFIC ENERGY REQUIREMENTS FOR VARIOUS TRANSPORTATION MODES

4.0

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100

90

80

70

CUMULATIVE 60

DISTRIBUTION OF Al R PASSENGER- 50 MILES AND FUEL CONSUMPTION (¾) 40

i...J ,0

30

20

10

0 0 500

CO>.,\, E RSIO._,

1 Ml LE a 1 609 '( M

1 LB SEAT M'LE • .2819 KG SEAT KM

FUEL

PASSENGER MILES

1000 1500 2000

TRIP LENGTH (MILES)

FIGURE 13

PASS. Ml. DATA SOURCE: CIVIL AERONAUTICS BOARD, 1969 (40)

ASSUMED FUEL CONSUMPTION:

0-200 Ml 200-400 400-600 600-1000 1000-2000 > 2000

2500

.2 LB/SEAT MILE

.13

.11

.10

.09

.085

3000 3500

SOURCE, FRAIZE, W. E., ET AL,

4000

THE M,TRE CORP., REPORT MTP 391, FE6. 1974

DISTRIBUTION OF U.S. DOMESTIC AIR TRAVEL, 1968

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in congested intercity corridors where TLV's will be an attractive

alternate, offering:

• City-center to city-center service.

• Reduced energy consumption compared to the short-haul air

alternative.

• Flexibility, through wayside electric power, to utilize a

wide range of basic energy sources,

• Reduced air corridor and highway congestion,

In summary, the potential fuel economy (seat miles/gallon) is

displayed, for the most important passenger transportation systems,

as a function of cruise speed in Figure 14. TLV systems are seen

again to fill in the speed regime gap between 150 and 300 mph (483

km/hr), All ground systems are seen to fall below an envelope of shape

2 given by 1/(speed) ; this defines the aerodynamic drag of vehicles

at sea level. Aircraft performance rises above this envelope because

of operation in reduced air density.

None of the above discussion of energy should be construed to

imply that energy is or will be the major determining force in HSGT

system development. Othe.r important travel-related factors not dis­

cussed here are: convenience, speed, safety, and comfort.

30

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JOO

200

z 0 -' -' < t3 a: w 0.. ., w -'

~ ... < w .,

100

0

0

..

BICYCLE (PETROLEUM TO PRODUCE FOOD ENERGY)

SUBURBAN TRAINS

INTERCITY BUS

INTERCITY TRAINS

MOTORBIKE 11 PSGRI

Ml NICAR OR MOTORCYCLE 12 PSGRI

' ' ' COMPACT CAR

FUTURE HIGH SPEED GROUND

1/ U.S. SEDAN (6 PSGRI

-' ~' -'~ JET AIRCRAFT -

~ ' -~ ' ~ ~ ~ PROP. AIRCRAFT ~ ~

100 200 JOO 400 500

MILES PER HOUR

CONVERSION

1 MILE/HA 1.609 KM/HA 3

1 Sf AT MILE/GAL 425 SEA.I KM/M

SOURCL: NUTTER, 11.0., THE MITRE CORP, MAR. 1974

FIGURE 14 MODAL COMPARISON OF FUEL ECONOMY

31

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...

IMPACT OF ENERGY SHORTAGES ON HSGT

Short term energy shortages of the sort experienced during the

winter of '74, will likely be addressed through higher fuel costs, con­

servation measures wherever possible, and, for the private automobile

driver, rationing either by regulation or through inconvenience in the

purchase of fuel. Intercity service would not likely be severly cur­

tailed because the bulk of any energy "short-fall" will be taken-up

by the automobile user. On the other hand intercity mass transportation

modes are apt to be strained to over-capacity as fuel supplies for

automobile travel become less dependable.

In the mid-term, a steady state supply-demand equilibrium at the

higher price established by new domestic energy sources would likely be

realized. Prices might continue to rise slowly as domestic fuel sources

begin to run short and become more expensive to extract.

In both the short and mid-terms (through 1985 or 1990), the major

energy impact on HSGT will be through increased cost. Table Ill

illustrates the effect of energy cost increases of 50% and 200% on

the total cost of travel for several major modes. The automobile

mode will suffer by far the biggest impact of rising fuel costs,

because virtually the only cost perceived by the privare automobile

operator is fuel cost. This suggests that fuel cost increases will

produce strong pressure to shift traffic from auto to the mass modes;

but, since the mass modes are relatively insensitive to fuel costs

(a three-fold increases in fuel cost yields less than a 20% increase in

travel cost), there will be little economic pressure to shift among the

33

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;_; .;:-

TABLE III

ENERGY CRISES COST FACTORS

Cost of Travel ~on-Energy Energy

:t-1ode Related Portion Related Portion (C ) n (C) e

Auto 0% 100%

Air 90 10

Bus 95 5

IPT 97.5 2.5

TLV 95 5

* C = C t n + Fe (Ce)

**Fe= 1.5: 50% fuel cost increase

= 3.0: 200% fuel cost increase

Total Cost Factor {Ct)* Energy Crisis Equals: (F )**

1.5 3.0 e

1.5 3.0

1.05 1.20

1.025 1.10

1.0125 1.05

1.025 1.10

SOURCE: U.S. DOT, High Speed Ground Transportation Alternatives Study, Jan. 1973

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I.,

mass modes. The mass modes can best accomodate future fuel cost in-

creases by building in the ability to rapidly increase system capacity.

Finally, in the long term (2000 and beyond), transportation will

adapt to long term stable energy sources with a range of fuels:

POTENTIAL LONG-TERM ENERGY SOURCES

Solar/Geothermal/Wind

Nuclear

Coal

Oil Shale

COMPATIBLE FUELS

Hydrogen Methanol Electricity Stored Thermal Energy

Electricity Hydrogen

Electricity Distillates Methane Hydrogen

Distillates Electricity

HSGT systems developed over the next 10 to 20 years should be

designed for compatibility with the most likely long-term fuels to be

available during the systems's lifetime.

35

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-

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RESEARCH TOPICS

Among the topics for research effort that will address the energy

aspects of future HSGT are the following:

Systems Studies and Analysis

• Motivation for use of mass transportation systems.

• The impact of regulation and operating procedures on modal

fuel efficiency.

• Measures to improve load factor.

• Land use/transportation relationships.

• Revised transportation demand projections, accounting for fuel

supply shortages and changes.

• Passenger/freight service compatibility.

Technology R&D

• Rail electrification costs, benefits, and environmental impact.

• Hydrogen and methanol utilization as transportation fuels.

• Use of stored e1ectric, mechanical, and high temperature thermal

energy.

• Environmental impact of fossil fuel usage.

• Efficient engines (internal and external combustion prime movers)

having a wide range of fuel flexibility.

• Improved power transmissions for ground vehicles.

• Means for reduced rolling resistance and aerodynamic drag for

groW1d vehicles.

• Rail/right-of-way/suspension design to acconnnodate optimally

both passenger and freight service.

37

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,

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REFERENCES

1. Austin, A.L., et al., Energy: Uses, Sources, Issues, Report UCRL-51221, Lawrence Livermore Laboratory, May 1972.

2. Understanding the National Energy Dilemna, a Report of the Joint Committee on Atomic Energy, 15 August 1973.

3. The Nation's Energy Future, U.S. Atomic Energy Commission, December 1973.

4. Fraize, W.E., et al., The MITRE Corportation, Report MTP-391, Energy and Environmental Aspects of U.S. Transportation, February 1974.

5. Motor Vehicle Manufacturers Association of the U.S., Inc., 1972 Automobile Facts and Figures.

6. Hirst, Eric, Energy Consumption for Transportation in the U.S., Report ORNL-NSF-EP-15, Oak Ridge National Laboratory, March 1972.

7. Strombotne, Richard L., Energy Usage Related Activities of the U.S. Department of Transportation, International Automobile En­gineering Congress and Exposition, 8-12 January 1973.

8. American Transit Association, '71 - '72 Transit Fact Book.

9. Civil Aeronautics Board, Handbook of Airline Statistics, 1971 Edition.

10. Campbell, M. Earl, "The Energy Outlook for Transportation in the United States," Traffic Quarterly, April 1973.

11. Malliaris, A.C., and Strombotne, R.L., Demand for Energy by the Transportation Sector and Opportunities of Energy Conservation, presented to the Conference on "Energy: Demand, Conservation, and Institutional Problems," Massachusetts Institute of Technology, February 1973.

12. Hirst, Eric, Energy Intensiveness of Passenger and Freight Trans­port Modes, 1950-1970, Report Mo. ORNL-NSF-EP-44, Oak Ridge National Laboratory, April 1973.

13. R. D. Nutter, A Perspective of Transportation Fuel Economy, The MITRE Corportation, MTP-396, April 1974.

14. U. S. Department of Transportation, High Speed Ground Transportation Alternatives Study, PB-220 079, January 1973.

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REFERENCES Cont'd

15. DC-9 Series 30 General Performance, Report No. MDC-J0594, Revised 7 June 1971, McDonnell Douglas Corp.

16. Weiss, G.L., Letter-to-the-Editor, The Washington Post, 22 January 1974.

17. Environmental Protection Agency, Compilation of Air Pollutant Emission Factors, Air Programs Office, February 1972.

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APPENDIX A

CONVERSION FACTORS

(English to SI Units)

• 1 ft .2048 (m) = metre

1 mile = 1.609 km

1 lbm = .4536 kilogram (kg)

1 ton ::::! 907.2 kg

1 gallon .003785 m 3 =

1 barrel (petroleum) = .159m3

1 BTU = 1055 joule (J)

1 horsepower (HP) = .7457 kilowatt

1 mile/ gallon = 425 km/m3

1 ton-mile = 1460 kg km

1 BTU/pass mile = 656 J/pass-km

1 BTU/ton mile = .723 J/kg-km

:-

,.

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