22
1 Overcoming Headway Limitations in Personal Rapid Transit Systems J. Edward Anderson, Ph.D., P. E. 1 3 rd Conference on Pod Cars, Malmö, Sweden, 9-10 December 2009 Abstract Theoretical and experimental work performed over four decades has shown how, based on open literature, to design PRT systems capable of serving a wide variety of needs. Over these four decades enormous advances have taken place in the computer art and in other components essential to PRT control, thus making it wholly practical to build short-headway PRT systems that will be safe and relia- ble. A safety standard for PRT is recommended. 1. Introduction Except for small applications, the future of PRT, or Pod Cars, depends on safe and reliable oper- ation at fractional second headways. This conclusion was reached in 1973 by the United States Urban Mass Transportation Administration and in many papers listed in the Bibliography Sec- tion of reference [1]. However, it ran counter to a railroad-safety requirement adopted by the United States Congress in 1911, which was that if one train stops instantly, the train behind must be able to stop before colliding with it. This is the commonly known brick-wall stop criterion, which is a reasonable safety requirement for railroads. But we all know that it has not prevented serious accidents in railroads there are evidentially more complex considerations involved. As is well known, enormous improvements have been made in many technological areas since 1911. The purpose of this paper is to examine how those technological improvements can affect the future of Pod Cars. 2. The 1973 Position of the Urban Mass Transportation Administration (UMTA) On page 2, I reproduce a page from the United States Congress Congressional Record [2] that documents hearings held on March 27, 1973. On that page, the statements by UMTA Adminis- trator Frank Herringer that are of interest here are the following: . . . “a High-Capacity PRT could carry as many passengers as a rapid rail system for about a quarter the cost.” . . . “A DOT program leading to the development of a short, one-half to one second headway, high-capacity PRT system will be initiated in fiscal year 1974.” 1 Managing Director, PRT International, LLC, www.prtinternational.com . 5164 Rainier Pass, Minneapolis, Minnesota, USA, (763) 586-0877, [email protected] .

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1

Overcoming Headway Limitations in Personal Rapid Transit Systems

J. Edward Anderson, Ph.D., P. E.1

3rd

Conference on Pod Cars, Malmö, Sweden, 9-10 December 2009

Abstract

Theoretical and experimental work performed over four decades has shown how,

based on open literature, to design PRT systems capable of serving a wide variety

of needs. Over these four decades enormous advances have taken place in the

computer art and in other components essential to PRT control, thus making it

wholly practical to build short-headway PRT systems that will be safe and relia-

ble. A safety standard for PRT is recommended.

1. Introduction

Except for small applications, the future of PRT, or Pod Cars, depends on safe and reliable oper-

ation at fractional second headways. This conclusion was reached in 1973 by the United States

Urban Mass Transportation Administration and in many papers listed in the Bibliography Sec-

tion of reference [1]. However, it ran counter to a railroad-safety requirement adopted by the

United States Congress in 1911, which was that if one train stops instantly, the train behind must

be able to stop before colliding with it. This is the commonly known brick-wall stop criterion,

which is a reasonable safety requirement for railroads. But we all know that it has not prevented

serious accidents in railroads — there are evidentially more complex considerations involved. As

is well known, enormous improvements have been made in many technological areas since 1911.

The purpose of this paper is to examine how those technological improvements can affect the

future of Pod Cars.

2. The 1973 Position of the Urban Mass Transportation Administration (UMTA)

On page 2, I reproduce a page from the United States Congress Congressional Record [2] that

documents hearings held on March 27, 1973. On that page, the statements by UMTA Adminis-

trator Frank Herringer that are of interest here are the following:

. . . “a High-Capacity PRT could carry as many passengers as a rapid rail system for about a

quarter the cost.”

. . . “A DOT program leading to the development of a short, one-half to one second headway,

high-capacity PRT system will be initiated in fiscal year 1974.”

1 Managing Director, PRT International, LLC, www.prtinternational.com.

5164 Rainier Pass, Minneapolis, Minnesota, USA, (763) 586-0877, [email protected].

2

3

So, why didn’t the UMTA program proceed? In short, it was too much too soon for an estab-

lished transportation industry [3]. To use a phrase coined by ARPA-E, an agency of the U. S.

Department of Energy, Personal Rapid Transit is disruptive and transformational. To quote

from a Funding Opportunity Announcement released by ARPA-E on April 27, 2009:

“This is the first solicitation for the Advanced Research Projects Agency – Energy (ARPA-E).

ARPA-E is a new organization within the Department of Energy (DOE), created specifically to

foster research and development (R&D) of transformational energy-related technologies. Trans-

formational technologies are by definition technologies that disrupt the status quo. They are not

merely better than current technologies, they are significantly better. Often, a technology is con-

sidered transformational when it so outperforms current approaches that it causes an industry to

shift its technology base to the new technology. The Nation needs transformational energy-

related technologies to overcome the threats posed by climate change and energy security, aris-

ing from its reliance on traditional uses of fossil fuels and the dominant use of oil in transporta-

tion.” (Emphasis added.)

Today, the situation is very different than it was in 1973. Automobile manufacturing companies

continue to do what they know how to do and what their shareholders expect. More and more

automobile manufacturers in more and more countries believe they need to build more and more

automobiles ever year, notwithstanding that cities are already clogged with automobiles, and that

the enormous land requirements of automobiles (30% in residential areas, and 50% to 70% in

major activities centers) cause low-density living patterns that will be more and more difficult to

serve as energy gets more and more expensive. Forty years of experience of government subsidy

of conventional scheduled, all-stop transit shows that a relatively small fraction of the urban

population opts for these systems. In 1968, studies authorized by the United States Congress and

funded through the newly founded Urban Mass Transportation Administration concluded that if

the United States encourages only expansion of its conventional scheduled, all-stop transit sys-

tems, congestion will continually worsen, but if the new personal transit systems are deployed, it

will be possible to reverse the trend [4]. A great gap exists between automobiles and convention-

al transit, a gap that can be filled by systems we have called High-Capacity PRT or in Sweden

Pod Cars.

3. Advances in Computer Technology since 1973

While every Pod Car Conference attendee is well aware of the enormous advances in computer

technology since 1973, i.e. 36 years ago, it is worthwhile to review these advances quantitatively

to the extent we can without becoming computer historians.

4

Since about 1960, computer memory has followed a “law” pronounced by Intel Co-Founder

Gordon Moore: It has doubled every 18 months! In 36 years there are 24 18-month periods

and 224

is 16,777,216.

How about computer speed? In 1975 the state of the art was about 2 kilobytes per second.

Today, high performance computers run at 12 gigabytes per second, an improvement by a

factor of 6,000,000.

Reliability: The main problem with continuously decreasing the size of computer compo-

nents is heat dissipation. Too much heat destroys the tiny transistors. By backing off the

present maximum transistor density by one order of magnitude, safety-critical microproces-

sors hardly ever fail, and these devices are now tiny compared to their size even a decade

ago.

As to the ease of computer programming, any experienced computer programmer will attest

to enormous improvements.

Computer design tools likewise have improved in sophistication and speed by many orders

of magnitude. In 1975 we did all our computing on mainframe computers costing hundreds

of dollars an hour for computer time. Since the 1980s, the personal computer has become

more and more useful — now for many uses taking over the function formerly assigned to

the work station.

4. Calculating Headway

Consider how we calculate headway: In the following illustration, one vehicle of length L, co-

lored green, is cruising to the right at a speed V and is followed by another green vehicle of the

same size traveling at the same speed at a nose-to-tail separation H.

L Dfailure stop

H

Vtc Demergency stop

At a certain instant, the lead vehicle decelerates to a stop at the right-most red position a distance

Dfailure stop ahead. The vehicle behind senses the failure and after a time tc begins to decelerate to

a stop in distance Demergency stop. The stopping distance is given by the equation

5

𝑆𝑡𝑜𝑝 𝐷𝑖𝑠𝑡𝑎𝑛𝑐𝑒 =1

2𝑉 × 𝑆𝑡𝑜𝑝𝑇𝑖𝑚𝑒 𝑆𝑡𝑜𝑝𝑇𝑖𝑚𝑒 =

𝑉

𝐴+

𝐴

𝐽

in which A is the deceleration and J is the jerk. From the diagram, we have

𝐻 = 𝑉𝑡𝑐 +1

2𝑉 𝐸𝑚𝑒𝑟𝑔𝑒𝑛𝑐𝑦𝑆𝑡𝑜𝑝𝑇𝑖𝑚𝑒 − 𝐹𝑎𝑖𝑙𝑢𝑟𝑒𝑆𝑡𝑜𝑝𝑇𝑖𝑚𝑒

The time headway is the nose-to-nose separation divided by speed V. Thus

𝑇𝑖𝑚𝑒 𝐻𝑒𝑎𝑑𝑤𝑎𝑦 =𝐿 + 𝐻

𝑉=

𝐿

𝑉+ 𝑡𝑐 +

1

2 𝐸𝑚𝑒𝑟𝑔𝑒𝑛𝑐𝑦𝑆𝑡𝑜𝑝𝑇𝑖𝑚𝑒 − 𝐹𝑎𝑖𝑙𝑢𝑟𝑒𝑆𝑡𝑜𝑝𝑇𝑖𝑚𝑒

It is clear that the shortest time headway is obtained if the reaction time tc is very short and if no

reasonable failure can cause a vehicle to stop in a time shorter than any vehicle can stop if the

emergency brakes are applied [5]. Thus, for a fractional-second-headway PRT system, the time

headway is given by

𝑇𝑖𝑚𝑒 𝐻𝑒𝑎𝑑𝑤𝑎𝑦 =𝐿

𝑉+ 𝑡𝑐

5. How do we keep Vehicles from Crashing?

The means of control I recommend is described in Reference [6]. This strategy can be classified

as an “asynchronous point follower.” It is “asynchronous” because the operation of a PRT sys-

tem is entirely demand activated. Such a system requires no clock synchronization for any rea-

son other than that calculation of speed and position must be done in real time and, just as in the

automobile system, merge conflicts are resolved at each merge. The strategy I recommend is a

“point follower” because the vehicles closely follow speeds and positions that are calculated as

functions of real time, are commanded by wayside computers, and are monitored by these way-

side computers. I have found [7, 19] that the code required to operate an asynchronous point-

following strategy is the simplest that can be devised.

The instruments we use today to measure position and speed are much more accurate than we

need and today our computers respond to and correct speed and position two hundred times per

second. Wayside zone controllers closely monitor vehicle motion and cause the vehicles to slow

to creep speed if an anomaly is sensed. The state of the art now is such that computers routinely

land airplanes on aircraft-carrier decks, a much more complex problem because both the airplane

and the carrier deck are subject to three translational and three rotational motions, while we need

only be concerned with PRT motion in one direction, with the merging of two one-dimensional

streams the most complex maneuver. More detail on this fundamentally important question fol-

lows.

6

6. The 1990’s Automated Highway Project (PATH2)

The picture to the right is of six 17-ft (5.18 meter) long Buick automobiles operating during the

1990s under automatic control on a freeway near San Diego, California [8]. At 60 mph or 26.8

meters per second the closest headway these vehicles operated at was a nose-to-tail spacing of

seven feet (2.13 m). Thus the minimum time headway

was (5.18 + 2.13)/26.8 = 0.273 seconds, which is closer

than we need in a PRT system. At such a close headway,

the emergency braking time must be as short as the fail-

ure braking time, in which case tc = H/V = 2.13/26.8 =

0.080 sec. The PATH program was funded by the United

States Federal Government and was monitored by the Na-

tional Highway Traffic Safety Board. Thus, if high-

capacity PRT could be classified as a type of automated

highway, safety certification would already be in hand. Figure 1. Buicks operating at short headway.

7. The Minimum-Headway Graph

A series of plots of the headway equation of Section 4 is shown in Figure 2 for a vehicle length

appropriate to a PRT vehicle. It can be seen that to achieve fractional-second headways, the fail-

ure deceleration cannot be much more than the emergency deceleration of any vehicle.

Figure 2. Minimum Time Headway.

2 PATH = Partners for Advanced Transit & Highways.

5 10 15 20 25 30

SPEED, meters per second

0.0

0.5

1.0

1.5

2.0

2.5

3.0

MIN

IMU

M T

IME

HE

AD

WA

Y,

se

co

nd

s

MINIMUM T IME HEADW AY in a PRT SYSTEM

Vehicle Length 2.75 m, Control Time Constant 80 msec

E me rge ncy braking rate 0.5g, Failure rate Af

Af = 0 .5g

Af = 0 .6g

Af = 0 .7g

Af = 0 .8g

Af = 1g

Af = 2g

Af = 3g

Af = 4g

Af = 5g

E me rge ncy Je rk 2g, Failure Je rk 10g

7

8. The Use of Linear Induction Motors

In the PATH Program, described in Section 6, the vehicles are propelled and braked through the

wheels. High-capacity in PRT can be attained much more safety and reliably in all reasonable

weather conditions if we propel and brake the vehicles using linear induction motors (LIMs).

The operation of LIMs is described in the Appendix. Let us compare the characteristics of these

two means of propulsion and braking:

Braking rate

Wheel braking depends on friction, grade, or wind and it is necessary to assume the worst

conditions when calculation the minimum safe headway. LIM braking is constant as com-

manded, independent of friction, grade, or wind and we can depend on a LIM-operated ve-

hicle to stop as quickly as a failed vehicle independent of the friction of the running surface.

Reaction time

Based on the data I have seen, it takes several hundred milliseconds for the full effect of a

wheel-brake command to be felt. When a LIM is operational braking is almost instantaneous.

Moving parts

A vehicle propelled and braked through wheels has many moving parts. With LIM propul-

sion and braking the only moving part is a fan need for air cooling of the LIM, and that is not

a safety critical item. If one of at least two fans on a LIM were to fail, and the vehicle has two

LIMs, the one with the defective fan can be shut off and the vehicle stopped at the next sta-

tion, where passengers would egress, following which the vehicle would be sent empty to the

nearest maintenance station.

How can we obtain an adequate braking force?

With propulsion and braking through wheels (in PRT usually rubber tired) the running surface

must be sufficiently rough to enable any vehicle to stop quickly on a wet or icy surface.

Raytheon, having opted for propulsion and braking through wheels in Phase II of the Chicago

PRT project, discovered too late that wet-weather operation required them to roughen the

running surface by bonding to it a type of sand used on aircraft carrier decks to prevent crew

members from sliding on a wet deck. Two problems result:

1. If the irrevocable emergency brakes need to be applied on a dry, roughened surface,

the deceleration rate is between 0.7 and 0.9 g, which is enough to throw an unre-

8

strained passenger into the windshield. Yet the Chicago RTA lawyers insisted that

there be no restraining devices in the vehicles — they didn’t want to set precedence.

This problem was never resolved.

2. Repeated acceleration and braking through the rubber tires leaves some tire material

imbedded in the roughened surface, and eventually the surface must be replaced, re-

sulting in a large maintenance cost.

With LIM propulsion and primary braking, we want the running surface to be as smooth as prac-

tical, and we want the wheels to be rollers only, i.e., no braking through the wheels. In this case,

in the remote chance that a wheel bearing were to freeze, the decelerating force will be less than

about 20% of one quarter of the gross weight of the vehicle, which would cause a deceleration

rate of no more than about 0.05g.

There must be a backup emergency braking system. We have proposed a pair of brake shoes

supported from the lower surface of the vehicle chassis through parallelogram linkages, so that

they remain parallel to and very close to the running surface. Each of two independent brake

shoes is activated by a no-power-on, no-power-off ball-screw actuator and is restrained from

moving past the point of maximum extension, thus satisfying the requirement that they be irre-

vocable. No-power-on means that power is not required to maintain the on condition and simi-

larly for the off condition. The actuators are electrically connected to activate from an auxiliary

on-board battery if vehicle emergency deceleration is a tolerance less than commanded emergen-

cy deceleration. Each brake shoe will be fitted with a high-friction braking surface, while the

main support tires will be selected for low friction.

Each of two LIMs is driven by a variable-frequency, variable-voltage drive. Study of such

drives interacting with a LIM shows that at each speed there is a frequency that minimizes cur-

rent, and that this frequency increases linearly with speed. Since the electrical losses increase as

the square of the current, it is important to operate the LIMs close to the frequency at each speed

that minimizes current.

9. The Hardware for Control

Operation of the control system requires on-board and wayside sensors of position and speed, a

communication link between the vehicles and wayside zone controllers, a communication link

between the zone controllers and a central computer, and computers on each vehicle, at wayside

zones, and in a central location.

9

For on-board position and speed measurement we use digital encoders [9]. The position accu-

racy of these devices is currently well under one millimeter. Since time can be measured to a

few nanoseconds, speed accuracy by differentiation is well better than we need.

For continuous communication between vehicles to zone controllers we use a commercially

available leaky cable inside the guideway only a centimeter away from transmitters and re-

ceivers mounted on the vehicle. The antenna required for these devices is only about 15 cm

in diameter. Such cables were not commercially available in the 1970s, which made the

communications problem then more difficult.

For communication between each wayside zone controller and a central computer we use fi-

ber optic cables.

For wayside position and speed measurement we use strategically spaced pairs of magnetic

markers inside the guideway.

Our computers on board vehicles, at wayside zones, and in a central location will be checked

dual duplex (see Section 10).

For independent backup emergency control that would be activated in the highly unlikely case

of a failure of the software of the primary emergency control system we will use either a sonar

or radar position sensing system.

All of these components are available as commodities or easily designed.

10. The 1984 Boeing Advanced Group Rapid Transit (AGRT) Program

Reference [10] and its 50 references document the extensive work of Boeing Aerospace Compa-

ny on the federally funded AGRT program. Notwithstanding the 25 years that have passed since

this work was completed, it is the most recent work related to automated transit funded by the

United States Government, it is the most well-documented work as a precursor to our work on

PRT control, it contains much useful information that can guide any new PRT control group, and

it was performed by a first-class group of control engineers. Moreover, it is available to the pub-

lic, and it was a valuable source of information for our Chicago RTA PRT Design Study [11],

which work is also available.

Safety Criterion. UMTA retained the Battelle Memorial Institute as its safety contractor on

the AGRT program. Battelle specified that AGRT had to be as safe as a modern rapid rail

system. When Boeing managers asked for a more specific definition, they were told to as-

sume that it was as if the vital relay that determines the safety of a modern rapid rail system

10

had a mean time to failure (MTBF) of one million years. So the design criterion for AGRT

was set as a control system MTBF of one million years for unsafe failures.

Boeing tested the microprocessor redundancy configurations shown in Figure 3, which is re-

produced from reference [12], and recommended the Dual Duplex configuration. I recently

learned that Honeywell currently also recommends Dual Duplex. The way the Duplex system

worked is as follows: The microprocessors, CH. 1 and CH. 2, were compared every 40 milli-

seconds. If the two outputs are the same, a safe-to-proceed signal is generated that cancels a

command to apply the emergency brakes. If the two outputs disagree, the vehicle came to a

stop, which was service interruption but not an unsafe failure. An unsafe failure would occur

only if the two microprocessors transmitted the same incorrect output.

The Boeing 1984 MTBF estimate in years [12] was as follows:

MTBUF MTBSI MTBF

Duplex: 400 million 0.6 0.6

Triplex: 140 million 1900 0.4

Dual-Duplex: 200 million 1400 0.3

MTBUF = Mean Time Between Unsafe Failures

MTBSI = Mean Time Between Service Interruptions

MTBF = Mean Time Between Failures of each unit

In a system of 1000 vehicle, the failure rate within the system would of course be 1/1000

times the above values.

Boeing’s AGRT work, which was performed in the late 1970s and early 1980s, does not

mention self-checking software; however, by 1991 in the Chicago Phase I PRT Design

11

Study [11] Raytheon engineers with whom I worked recommended self-checking software,

which has the added advantage that the microprocessor with a failure can be identified. This

extends the system MTBUF remarkably.

11. Requirements for High-Capacity PRT System Safety and Reliability[5]

Few moving parts in the vehicle.

No safety-critical moving parts in the motors.

Propulsion and braking independent of friction.

No moving track parts in the switch.

Redundant motors, sensors, and power supply.

Checked Dual Duplex computers.

Safety-critical, fault-tolerant hardware and software with built-in tests.

Dual independent emergency braking.

Exclusive guideway.

Result: The chance of injury is close to zero!

12. Examples of Safe Design

Each wayside zone controller (ZC) emits its speed signal every 100 millisecs.

With no speed signal the vehicles are programmed to stop.

Each ZC receives position and speed from each vehicle every 100 millisecs.

With no communication, the cognizant ZC stops the speed signal and reports upstream.

Independent wayside means for measuring position and speed of each vehicle.

All commands returned and verified before action is taken.

Thruster temperature sensors report possible over-heat conditions.

The emergency brake command is ON unless OFF is received every 100 millisecs.

When the switch is thrown, a command is given to stop unless canceled in 500 milliseconds

(the switch-throw time with tolerance) by a signal from a proximity sensor.

Sonar or radar back-up emergency control available in case of a software fault.

13. Do Reliability Requirements increase with System Size?

Define DEPENDABILITY = 1 – Person-Hours of delay/Person-Hours of operation. This is a

valuable quantity that cannot be measured routinely in conventional transit systems without great

expense and inconvenience, but it is the primary measure of system on-time performance [13].

Because a PRT system must know every trip destination, dependability can routinely be both

measured in an operating system and calculated in advance during the system development

process. These calculations were performed during our Phase I PRT Design Study [11] with a

12

resulting estimate of dependability of 99.967% [14]. An important conclusion from reference

[13] is that dependability is independent of system size.

My paper on optimum reliability allocation [15] comes to a similar conclusion: The component

reliability needed to minimize life cycle cost of the entire system while meeting a given depen-

dability requirement is independent of system size.

14. The Recommended Control Strategy

From system simulation work [7, 19] done during the above-mentioned Chicago project, I found

[6], as mentioned above, that the best strategy for operation of a PRT system of any size or con-

figuration is an asynchronous point follower. Just as in a highway system, the events in a PRT

network are determined by actions of individuals such as when and how much time they need to

ingress and egress from vehicles, which can be treated as a normal distribution with a certain

mean and a certain variance. There is no need for clock synchronization for any reason other

than to calculate commanded maneuvers in real time. The latter of course is a function not found

in a highway system, but one that permits precise control of the position and speed of each ve-

hicle at all times, whether the speed is changing or held constant. The speed and position of each

vehicle can now be measured more accurately than necessary by means of commercially availa-

ble digital encoders. With this information and with a high-gain control system the vehicles

closely follow commanded maneuvers.

In reference [16] I show that if one can assume the propulsion system can be represented at least

roughly as a first-order lag, the required control gains can be calculated in terms of well-

understood quantities – an assumed vehicle mass, a natural frequency, a damping ratio, and a

dimensionless parameter that lies between 0 and 1. The gains are as follows:

2 1

2 12

Assumed vehicle mass

Control system natural frequency, radians per sec

= Damping ratio

= A dimensional parameter between 0 and 1.

c n

c n

c

n

Position Gain m

Speed Gain m

m

Also in reference [16] I showed the results, reproduced in Figure 4, of simulating a PRT control

system using the above position and speed gains. Note that the error in speed is magnified by a

factor of 1000. An error of about 2 mm/sec is seen at the beginning and the end of a maneuver

from rest to line speed while the commanded speed profile moves from constant jerk to constant

13

acceleration and back again. A large wind gust produces a deviation in actual speed from com-

manded speed barely more than one mm/sec.

Figure 4. Simulated Response to a Wind Gust.

I used this control scheme in a full-sized, passenger-

carrying LIM-propelled vehicle Knutson Construction

Company, working with Taxi 2000 Corporation, trans-

ported to the 2003 Minnesota State Fair (Figure 5).

Thousands of rides were given during the 12 days of the

Fare with no noticeable rough motion as the vehicle

started and later stopped. There were no control-system

failures even though there was no redundancy.

Figure 5. State Fair Exibit of Taxi 2000.

15. Calculation of Maneuvers

To provide point-following control, code is necessary to calculate each of the following maneuv-

ers. Such calculations are discussed in the Boeing AGRT work [10], were developed in our Chi-

cago project [11], and have been carried out by others [18]. These maneuvers are:

Starting with given speed and acceleration within the valid range, cause the vehicle to slip

back a given distance and then return to line speed. Figure 6 shows such a maneuver, which

is used at the command point ahead of each merge. The merge routine causes each vehicle

behind the vehicle that slips at the merge command point to also slip if the minimum-

headway requirement would otherwise be violated. In this way, potential merge conflicts

are resolved without resorting to synchronization.

14

Starting with given speed and acceleration within the valid range, cause the vehicle to ma-

neuver to a different speed and zero acceleration, for example maneuver from a station to

line speed. Figure 7 shows such a maneuver.

Figure 6. A typical slip maneuver taking place at a line-to-line merge.

Figure 7. A typical transition from a station to the main line.

In Figure 7, acceleration maintains its maximum comfort value until the speed reaches half

line speed, then declines linearly until it has reduced to half the maximum value, whereupon

it drops at the maximum jerk rate to zero. If this procedure was not followed, the accelera-

tion power, shown in Figure 7, would have almost doubled the value shown, which means

that the electric current would have doubled. Since the losses in the linear motor increase as

the square of the current, the heat dissipation capability would have had to quadruple, which

would have significant consequences for the size, weight, and cost of the variable frequency

0 1 2 3 4

TIME, seconds

-2

0

2

4

6

8

10

12

14

SP

EE

D,

met

ers/

sec;

AC

CE

LE

RA

TIO

N, m

eter

s/se

c2

ACCELERATIONSPEED

A TYPICAL SLIP MANEUVER

0 1 2 3 4 5 6 7 8

TIME, seconds

-5

-3

-1

1

3

5

7

9

11

13

15

17

AC

CE

L, m

/s2;

SP

EE

D, m

/s; A

CC

EL P

OW

ER

, wat

ts/k

g

TYPICAL STATION-TO-LINE-SPEED MANEUVER

ACCELERATIONSPEEDACCELERATION POWER

15

drive. Lack of understanding of this point has caused the variable frequency drives in some

LIM-propelled vehicles to be much larger than necessary.

Starting with given speed and acceleration within the valid range, cause the vehicle to dece-

lerate to as stop in a given distance.

Starting with zero speed and zero acceleration, cause the vehicle to advance a given distance

and then stop. This is a special case of the third maneuver, but desirable because it is a

common maneuver within stations and the code is much simpler.

Starting with given speed and acceleration within the valid range, cause the vehicle to un-

dergo an emergency stop or a deceleration to a safe creep speed.

16. Conventional Safety Philosophy

As mentioned in Section 1, the conventional railway safety philosophy is and has been in the

United Sates since passed into law in the 1911 Railway Safety Act that if one train stops instant-

ly the train behind must be able to stop before colliding. This makes sense in railways. Collision

avoidance in conventional railways depends on a carefully manufactured, highly reliable vital

relay. It is held open against gravity by an electromagnet and if the train ahead has stopped, a

current in the rail is cut and the relay falls. In an extremely unlikely circumstance in which the

vital relay sticks and fails to drop when train ahead has stopped, a collision may occur. It is fun-

damental that the simultaneous occurrence of two independent events in close proximity in space

and time sets up a possibility for a collision. This is unavoidable in any moving system! For

example, if in an emergency situation in an automobile the brakes fail or the steering system

goes awry when needed a collision is possible.

17. Recommended PRT Safety Philosophy

In our work on high-capacity PRT our philosophy is and has been that if one vehicle were to stop

instantly someone would have been killed [6]. Thus, we design so that the probability of one

vehicle stopping instantly is extremely and acceptably low. Away from a diverge point in a sys-

tem using exclusive guideways with no interference from other modes of travel, there is no sys-

tem-induced situation that could cause a vehicle to stop instantly. We have, however, needed to

study passage through a diverge point, diagramed in Figure 8, very carefully and have also ana-

lyzed [17] situations in which an event outside the system could cause an accident in the system.

16

Figure 8. A vehicle approaching a diverge point.

18. Design of the Guideway Diverge

The problem of safety as a vehicle passes through a diverge point is considered in detail in refer-

ence [17], assuming a specific means of switching. There it is shown how to design the switch-

ing procedure in such a way that to set up the conditions for possible impact with the diverge

junction would require the simultaneous occurrence of two independent highly unlikely failures

in close proximity in space and time plus an “Act of God” such as a lightning stroke that could, if

it occurred at precisely the right time and was of a specific shape, cause the switch to throw even

though measures are taken to shield the switch torquer from a voltage spike.

In general the requirements for safe passage through diverge sections of the guideway are the

following:

The vehicle must be constrained to one side of guideway so that under normal circumstances

it cannot be forced away from that side as a result of a combination of the maximum cross-

wind that would be permitted under operational conditions (the Chicago RTA specified the

maximum cross wind to be 70 mph [112 km/hr]) plus the maximum unbalanced passenger

load.

In the distance ahead of the diverge point through which the vehicle moves at line speed

during the switch-throw time, the design must prevent an unauthorized throw of the switch

as a result of, for example, a lightning stroke.

The front of both vehicle and the wayside diverge junction must by design be as narrow as

practical to minimize the probability of impaling the vehicle on the diverge junction in the

remote possibility that the vehicle became unconstrained.

19. Design Requirements for Minimum Safe Headway

With some repetition from Section 11, the design requirements to achieve the minimum practical

safe headway are as follows:

All controllers on board and at wayside are checked dual duplex.

The switch is bi-stable, in-vehicle, and conservatively designed.

The switch torquer is shielded from stray voltage spikes.

There is either instantaneous back-up to primary power or there is no mode in which prima-

ry power can fail suddenly.

17

If power is supplied from wayside, the power-pickup shoes must be designed so that there is

no reasonable way they can fall off or in any emergency situation rotate and short out the

power rails.

Propulsion and primary braking must be frictionless.

The emergency braking system must be completely independent of primary braking.

Independent sonar or radar back up must be provided for collision warning in case of a

software error in the primary control system, even when it has been thoroughly checked.

20. The Mean Time between Unsafe Failures

In reference [17], the following mean times to failure (MTBF) are calculated:

Type of component failure MTBF, years

On-Board computer system 400 (10)18

Communication system 137,000

On-Board Encoder system 214,000

On-Board Propulsion system 700,000

Vehicle incapable of moving 75,000

Pushing incidents w/500 vehicles 150

Zone controller 30(10)18

Vehicle-vehicle collision 1012

Merge collision 1013

Estimated life time of the universe 13.6(10)9

Auto accident rate ÷ PRT accident rate 20(10)12

These results are based on data obtained during the Chicago PRT design study [11], which oc-

curred 18 years ago! How much better can we do today?

21. Proposed PRT Safety Standard

From the National Transportation Statistics data for the year 2006 the number of passenger-miles

by private automobile in the United States was 2,640,170(10)6. The number of injuries in auto

accidents was 1,475,000 and the number of fatalities was 16,520. Thus, the number of miles

(km) per injury was 1,790,000 (2,880,000), and the ratio of injuries to fatalities was 89.3.

I recommend that safety in Pod Cars (PRT) be measured in terms of unsafe incidents per 1012

km

of travel in occupied vehicles. In the auto system there would be at least 347,000. This quantity

can be measured routinely just as Dependability can be calculated routinely. An “unsafe inci-

dent” should be defined as one that requires vehicles to slow down to a creep speed3 low enough

3 Stopping completely will create much anxiety without under microprocessor control increasing safety and will give

passengers no comfort in soon being able to alight at a station.

18

so that a collision with the vehicle ahead would not cause a deceleration of more than 0.5 g.

Such incidents would be required to be reported to authorities. Considering the auto injury rate, I

recommend that an unsafe Pod Car (PRT) system be defined as one in which the distance tra-

velled for one unsafe incident be less than 1012

km. This is such a large number that for many

years it will have to be estimated through exhaustive investigation of all failure modes.

22. Early Applications

Early applications will by necessity have to be small, in which case headways between 2 and

3 seconds are sufficient. These headways do not violate the 1911 Railway Safety Act.

The system should be designed with shorter headways in mind.

The system must be tested at shorter headways without passengers until safety is assured.

It will be necessary to inspect independently and rigorously all aspects of the control system.

23. Conclusions

The state of the art of computers and other critical components needed in a high-capacity PRT

system is today such that we can design and build PRT systems suitable to be expanded to serve

entire metropolitan areas, thus making fully practical the essential pioneering work of The Aero-

space Corporation led by its genius Vice President Dr. Jack H. Irving [18]. An unsafe Pod Car

(PRT) system should be defined as one in which there is more than one unsafe incident in 1012

km of travel in occupied vehicles. Finally, we observe that High-Capacity PRT has much more

in common with an automated highway than with a railroad.

24. References

[1] J. E. Anderson 2005. “The Future of High-Capacity Personal Rapid Transit,” www.prtnz.com.

[2] Department of Transportation and Related Agencies Appropriations for 1974. Hearings held on March

27, 1973 before a Sub-committee of the Committee on Appropriations, House of Representatives, Ninety-

Third Congress, John J. McFall, Chairman, Part I, Urban Mass Transportation Administration, page 876.

See page 11 for a reproduction of page 876.

[3] J. E. Anderson, 2009. “Evolution of Personal Rapid Transit,” www.prtnz.com.

[4] W. F. Hamilton and D. K. Nance. 1969. “Systems Analysis of Urban Transportation.” Scientific

American, July 1969.

[5] J. E. Anderson, 1988, “Safe Design of Personal Rapid Transit Systems," Journal of Advanced Trans-

portation (JAT), 28:1:1-15. www.prtnz.com.4

4 Posted with permission.

19

[6] J. E. Anderson, 1998. "Control of Personal Rapid Transit Systems," JAT, 32:57-74. www.prtnz.com.

[7] J. E. Anderson, 1998. “Simulation of the Operation of Personal Rapid Transit Systems.” Computers in

Railways VI, WIT Press, Boston, Southampton, 523-532. www.prtnz.com.

[8] California Partners for Advanced Transit and Highways.

http://repositories.cdlib.org/its/path/reports/UCB-ITS-PRR-97-26/

[9] R. P. Lang and D. J. Warren. 1984. “Microprocessor Based Speed and Position Measurement Sys-

tem,” Automated Transportation Systems, Boeing Aerospace Company, an IEEE Paper.

[10] D. D. Lyttle, D. B. Freitag, and D. H. Christenson , 1986. “Advanced Group Rapid Transit Phase IIB

Executive Summary & Final Report,” UMTA-WA-06-0011-86-1. Available to the public through the Na-

tional Technical Information Service, Springfield, Virginia 22161. 205pp.

[11] Personal Rapid Transit. 1992. Phase I Baseline Documentation, Volume I & II, System Design Re-

port, System Element Design Report.

[12] R. C. Milnor & R. S. Washington, 1984. “Effects of System Architecture on Safety and Reliability

of Multiple Microprocessor Control Systems,” IEEE Conference Paper.

[13] J. E. Anderson. 1992. "Dependability as a Measure of On-Time Performance of Personal Rapid

Transit Systems," JAT, 26:3(1992):101-212. www.prtnz.com.

[14] 1991. Fault Tree Analysis/Reliability, Availability, Maintainability Report. Personal Rapid Transit

Program, Stone & Webster Engineering Corporation, Prepared for Regional Transportation Authority,

Chicago, Illinois, Table 5-1, page 5-3.

[15] J. E. Anderson. 1977. "Life-Cycle Costs and Reliability Allocation in Automated Transit,"

High Speed Ground Transportation, 11:1:1-18. www.prtnz.com.

[16] J. E. Anderson. 1997. "Longitudinal Control of a Vehicle," JAT, 31:3:237-247. www.prtnz.com.

[17] J. E. Anderson. 2000. “Failure Modes and Effects Analysis and Minimum Headway in PRT,”

www.skyloop.org, www.prtnz.com.

[18] Jack H. Irving, Harry Bernstein, C. L. Olson, and Jon Buyan, 1978. Fundamentals of Personal Rapid

Transit, Lexington Books, D. C. Heath and Company.

[19] J. E. Anderson, 2000. “A Review of the State of the Art of Personal Rapid Transit.” JAT, 34:1:3-29.

www.prtnz.com.

20

We call our system an “Intelligent Transportation-Network System” (ITNS)The Generic Name “Personal Rapid Transit” (PRT)

“Make big plans; aim high in hope and work, remembering that a noble, logical diagram once recorded will never die, but long after we are gone will be a living thing, asserting itself with ever growing insistency.”

Daniel H. BurnhamChicago Planner

Hats off to Sweden for its big plan for Pod Cars!

www.prtinternational.com

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Appendix. The Linear Induction Motor

The basic principles of electromagnetic induction upon which a linear induction motor operates are illu-

strated in Figure A-1. If a magnet moves at a speed V the magnetic flux ahead of the magnet increases in

time with respect to a fixed surface and the magnetic flux behind the magnet decreases with time. The

way Mother Nature works, a time varying magnetic field induces an electric field proportional to the rate

of change of the magnetic field. If the magnet moves along a conducting surface, the induced electric

field causes a current in the plate proportional to it. With the North and South poles as shown in Figure

A-1, the current is counterclockwise ahead of the moving magnet and clockwise behind. Under the mid-

dle of the magnet the induced currents come out of the paper towards the left in Figure 1 and here the

magnetic field is of maximum strength and is downward. This is the principle of electromagnetic induc-

tion, which was discovered in 1820.

Figure A-1. Current induced by a moving magnet.

A property of nature is that when an electric current passes across a magnetic field a force is produced

perpendicular to both the current and the magnetic field. James Clerk Maxwell, in the mid 1850s, derived

the laws under which these phenomena work in a set of equations now called Maxwell’s equations. The

remarkable fact is that these equations have proved time and again to be exact. In Figure A-1 the force on

the plate is to the right. If the conducting plate is resting on a low-friction surface, the plate will be

dragged along with the magnet.

To achieve the speed V, the person or object moving the magnet must overcome the force F on the mag-

netic, which force is equal and opposite to the force induced in the conducting plate. If the conducting

plate is fastened down and above it there is a vehicle containing a traveling magnetic field moving to the

right, the force F moves the vehicle to the left. It is thus necessary to devise a way to produce such a

traveling magnetic field.

A means for producing a traveling magnetic field is illustrated in Figure A-2. In the middle illustration,

the elongated object containing slots is one of a stack of thin iron sheets stamped out with a die. The bot-

tom view shows the same iron sheets in edge view stacked up as in a transformer. Three sets of coils are

wound as indicated and are connected as shown in either the illustration on the left or on the right. The

left illustration show what is called a “delta” connection after the Greek letter ∆ that it resembles, and the

one on the right is a “Y” connection. A three-phase alternating voltage is applied to the three windings

22

with a frequency that increases with speed, with the voltages phased as shown in the top diagram. With

the delta connection the voltage is applied directly across each set of coils. With the Y-connection each

phase of the voltage is applied across two coils. The delta connection may therefore be used for high

thrust and the Y connection for moderate thrust.

Figure A-2. A means for producing a travelling magnetic field.

There is a frequency of oscillation of the voltage that minimizes the current and that frequency increases

linearly with speed. This is important because the electrical resistance losses are proportional to the

square of the current, and thus the surface needed to dissipate the heat generated is proportional to the

square of the current. The drive’s volume increases as the three halves power of its surface area. Hence

the required volume of the drive must increase in portion to the cube of the maximum current. For this

reason, maintaining the frequency of oscillation of the voltage close to optimum is very important. Linear

induction motors have been under development for many decades and several books have been written

describing them in technical detail.