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Solution to Problem 82-16: Malevolent traffic lights

Citation for published version (APA):

Lossers, O. P. (1983). Solution to Problem 82-16: Malevolent traffic lights. SIAM Review, 25(4), 571-572. https://doi.org/10.1137/1025129

DOI:

10.1137/1025129

Document status and date: Published: 01/01/1983

Document Version:

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(2)

PROBLEMSAND SOLUTIONS 571

andsatisfies

N

SinceMisnonnegative,

N

<=

(Tx Ty)i

<=

max

[0,

j=,

Mij(x

y)g

<=i<=N.

[(Tx

Ty)l

Ml(x

y)l,

_-< _-<N.

j--!

Since

Spr [M]

< 1, one can then find a vector norm

I]x]l

and associated matrix norm

I[M][

< such that

rx

Ty[I

<=

IIM[I

IIx

Yll

soris a contractionoperator.

A Sumof Legendre Polynomials Problem83-20", by M. L. GLASSER

(Clarkson

College).

Determinethesums

S,

-

Z

{Znpn(

cOSO)

}l,,

1,2, 3,"

n=0

Editorialnote.The proposerhas determined the sumsfor and2.

SOLUTIONS

Malevolent TrafficLights

Problem 82-16, byJ. C.LAGARIAS(BellLaboratories,

Murray

Hill,NJ).

Can the red-green pattern of traffic lights separate two cars, originally bumper-to-bumper, byanarbitrarydistance?Wesupposethat:

(1)

Two cars travel up a semi-infinite street with traffic lights set at one block intervals.Car startsupthe street at time 0andcar2 at time

to

> 0.

(2)

Bothcarstravel ataconstantspeed when in motion.Carshalt instantlyatany

intersection with a red light, and accelerateinstantlyto fullspeed when the light turns

green. If thecarhas enteredanintersectionasthelightturnsred,itdoesnotstop.

(3)

Eachlightcycles periodically, alternatelyred and greenwithredtimezj,green

time

,

andinitialphase

0

(i.e.,phaseattime0)atintersection j.

Canonedefinetriplets(kj,I.j,

Oj)

(j 1,2, sothat

{(hi,

t):

j 1, 2, isa

finite setandsothat car gets arbitrarily far ahead ofcar2?

Solution by O. P. LOSSERS (Eindhoven University of Technology, Eindhoven, The Netherlands).

The answer is yes as we shall now prove. We consider two types oftraffic lights

(I) 3, u

a/2,

(II)

u

b/2,

whereaand b arechosenin such a way that

a/b

is

irrational. Thephases of the lightsarechosen insuchaway thatthe first car neverhasto

stop. This is easily accomplished. However, we can manipulate more with the phases.

Suppose

that the second cararrives at a light of type Iwith adelay ofra

+

0 seconds (rcN,0<0<

a).

Thephase ischosen in sucha way that the lightchanges

1/20

seconds aftercar passes.Sothedelayofcar2increases to(r

+ 1/2)a +

1/20.

Ifwehad only used lights of type thedelay would monotonicallyincrease to

(r

+

1)a.

Asimilarstatement is true forlights of typeII. Ateachintersectionwestillhave thechoiceof the type of light. Wechoose thistypeinsuchaway thatthe increase is maximal. Since

a/b

isirrational,no

(3)

572 PROBLEMSAND SOLUTIONS

Also solved by the proposer.

Editorial note. The proposer shows that if all thecycle times are commensurable then any two cars remain within a bounded distanceof each other, no matter how the lightsarespecified.

[C.C.R.]

ADefiniteIntegral

Problem 82-17,by PETERHENRIC!(SwissFederalInstituteofTechnology, Zurich).

Theintegral

I=

fo

sin7rx

(-1)

k/l

k(k

+

1)dx

k=l (X -t- k)

arosein connection with astudyofindefinite numericalintegration of periodicfunctions. Find its value.

Solution by ANDREW H. VAN TUYL (Naval Surface

Weapons

Center, Silver Spring,

MD).

Let

(-

1)k+lk(k

+

1)

(1)

f

(x)

=,

(x

+

k)

Wewill considerthe integral

(2)

Im

fo

f(x)

sin

(2m

+

1)rx

dx,

rn 0, 1,2, which isequaltothegiven integral whenrn 0. Wecanverifythat

t2e-(X+l)tdt (3)

f(x)

1

(1

+

e-t)

oo byexpanding

(1

+

e-t)

-3 in powers ofe-t

in

(3)

and integratingtermbyterm. From

(2)

and (3),weobtain

t2 e-t

dt I (2m

+

1)r

[(2m

q-

1)27r

q-

t21(1

-+-e-t)

(2m

+

1)Tr (4)

J0

2 (2m

+

)271-2

(2m

+

1)271-2

q- 4t dt cosh (2m

+

1)Tr

(2m

+

1)371-3

where (5)

Jm

dt

[(2m

+

1)27r

+

4/2]

cosh2

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