Solution to Problem 64-14: Resistance of a ladder network
Citation for published version (APA):
Bouwkamp, C. J. (1966). Solution to Problem 64-14: Resistance of a ladder network. SIAM Review, 8(1), 111-112. https://doi.org/10.1137/1008019
DOI:
10.1137/1008019
Document status and date: Published: 01/01/1966
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PROBLEMS AND SOLUTIONS 111
Problem 64-14, Resistance
of
a LadderNetwork, byWILLIAM D. FRYER (Cornell
Aeronautical Laboratory).
Findthe input resistance R,, to then-sectionladdernetwork as shown in the
figure. Also, determinelim,
R.
Solutionby
C. J. BOUWKAMP
(Technological University, Eindhoven,Nether-lands).
Divide all the resistances of the n-section ladder network by 2. Then the resulting network has input resistance
R,/2
and the(n
+
1)-section ladder network is aseries connection ofaunit resistor andanetworkconsisting of tworesistors in parallel, one of value 1 and theother of value
R,/2.
Consequently,wemust havetherecurrencerelation
2+2R
R1
2, R,+I2+R.
n 1,2,3,....Oae method of findingan explicit expression for
R
is to let R, p,/q,, wherep,+ 2pn -[- 2qn qn+l Pn
+
2q, p 2q 2.It then follows that p and q are two linearly independent solutions of the recurrence relation
f+
4f+
+
2f
0 whose solutions must be of the formf+
A (2
+
/)"
+
B(2
/).
Hence,
p[(2-t-
/)
+
(2-
V/)],
q[(2-t-
V/)
-
(2-
/)].
Fiscally,+
+
(2
R,(2
+
(2
andlimn
Rn
%//-.
Also solved by
E. C. BITTNER
(National Aeronautics andSpace
Adminis-tration),
T.
S. ENGLAR, JR. (Research
Institute forAdvanced Studies),M. Fox
(Sylvania Electronics Systems),
J. M. HoLT
(Collins Radio Corporation),R.
KELISKY
(IBM Watson
ResearchCenter),
P.G.
KIRMSER(Kansas State
Uni-versity),
B.
K.LARKIN
(Martin Company),J. D. Lwso (Oak
Ridge Institute of Nuclear Studies),W. C. LYNCH (Case
Institute of Technology),.E. LXN
and G.
STOODLEY (Grumman
Aircraft Engineering Corporation),I. :NAVOT,
tWO solutions(Israel
Institute ofTechnology, Haifa,Israel), R. OnVEC
(Price Waterhouse and Company),K.
A.
POST (Technological University, Eindhoven,112 PROBLEMS AND SOLUTIONS
(California Research Corporation),
L.
H. RUSSELL (General
Precision,Inc.),
P.
A. SCHEINOK (Hahnemann
Medical College),K. P. SHAMBROOK
(Westing-houseElectric Corporation),
R. SINGLETON
(Middletown, Connecticut),R. D.
SMALLWOOD (Stanford
University),S.
SPITAL
(CaliforniaState
PolytechnicCollege),
S.
WALIGSRSKI
(Institute of Mathematical Machines,Warsaw,
Po-land), and theproposer.Editorial
Note.
The recurrence relation forR
can also be solved by findingthe nth powerof the matrix
[ ].
Wligorski lso determines lira
R
for the network in which the elements of the rth section, 2-
nd 2-,
gre replaced bya
-
and a-’,
r 1, 2, n.The limit is
R
{+
1-+
(+
1-a)
+4a}
nd is ewluted bymeans of the periodic continued frctionwhich is obtained
from therecurrencerelation.
Navot refers to
A.
C.BTEW,
The Theoryof
ElectricalArtifical
Lines andFilters, Chpmn nd Hll, London, 1930, Chp. 3, where ldder networks re
nMyzedin terms ofcontinuntsndto
A. M.
MoGh-VocE, Laddernetworlanalysis using Fibonacci numbers,
IRE Trans.
Circuit Theory, CT-6(1959).
pp. 321-322, for similar problem.Problem64-15,
On
aProbabilityof
Overlap, byMURRAY S. LAMKIN (Ford
Scien-tificLaboratory).Prove directlyor by animmediate application of atheoremin statistics that
the conjecture in the following abstract from Mathematical Reviews, March, 1964, p. 589, is valid:
"OLESKIEWICZ,
M. The probability that threeindependent phenomenonof
equalduration will overlap. (Polish, Russian and Englishsummaries)
Prace Mat.
64(1960), 1-7.
The vlue
P3
ofthe probability that3stochastically independentphenomeonof equalduration
to
which alloccurduring the time-F
to
willoverlapis shown by geometrical methods to be equal to(3tt0
-
2to3)/t
.
The author makes the conjecture that a similar formula holds for n independentevents,
namelyP
ntto
-
n 1)to
n)/t’.
Solutionby
P. C.
HEMMER
(NorgesTekniskeHcgskole, Trondheim, Norway).We
note that an overlap has to start simultaneouslywiththeonset of one of the n events. The probability of overlap whenthis one event is assumed to be number 1 gives1/n
of the desired probabilityP.
Denote
the whole time by(0,
-F
to)
and let event number 1 occur in(,
to),
where is uniformlydistributed in
(0, t). An
overlap exists if and only if the other n- 1 eventsoccur attime
.
Independence anduniform distributionguarantee the following probability forthis to happen:f(/t)
n-if 0