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Transcript of Portal through Mathematics - American Mathematical Society
Portal through Mathematics
Journey to Advanced Thinking
O.A. IvanovTranslated
by Robert G. Burns
AMS / MAA ANNELI LAX NEW MATHEMATICAL LIBRARY VOL 52
Originally published byThe Mathematical Association of America, 2017.
ISBN: 978-1-4704-4876-9LCCN: 2016960274
Copyright © 2018, held by the Amercan Mathematical SocietyPrinted in the United States of America.
Reprinted by the American Mathematical Society, 2018The American Mathematical Society retains all rightsexcept those granted to the United States Government.
⃝∞ The paper used in this book is acid-free and falls within the guidelinesestablished to ensure permanence and durability.
Visit the AMS home page at https://www.ams.org/
10 9 8 7 6 5 4 3 2 23 22 21 20 19 18
Council on Publications and Communications
Jennifer J. Quinn, Chair
Committee on Books
Jennifer J. Quinn, Chair
Anneli Lax New Mathematical Library Editorial Board
Karen Saxe, Editor
Timothy G. Feeman
John H. McCleary
Katharine Ott
Katherine S. Socha
James S. Tanton
Jennifer M. Wilson
ANNELI LAX NEW MATHEMATICAL LIBRARY
1. Numbers: Rational and Irrational by Ivan Niven
2. What is Calculus About? by W. W. Sawyer
3. An Introduction to Inequalities by E. F. Beckenbach and R. Bellman
4. Geometric Inequalities by N. D. Kazarinoff
5. The Contest Problem Book I Annual High School Mathematics Examinations
1950–1960. Compiled and with solutions by Charles T. Salkind
6. The Lore of Large Numbers by P. J. Davis
7. Uses of Infinity by Leo Zippin
8. Geometric Transformations I by I. M. Yaglom, translated by A. Shields
9. Continued Fractions by Carl D. Olds
10. Replaced by NML-34
11. Hungarian Problem Books I and II, Based on the Eotvos Competitions12.
}1894–1905 and 1906–1928, translated by E. Rapaport
13. Episodes from the Early History of Mathematics by A. Aaboe
14. Groups and Their Graphs by E. Grossman and W. Magnus
15. The Mathematics of Choice by Ivan Niven
16. From Pythagoras to Einstein by K. O. Friedrichs
17. The Contest Problem Book II Annual High School Mathematics Examinations
1961–1965. Compiled and with solutions by Charles T. Salkind
18. First Concepts of Topology by W. G. Chinn and N. E. Steenrod
19. Geometry Revisited by H. S. M. Coxeter and S. L. Greitzer
20. Invitation to Number Theory by Oystein Ore
21. Geometric Transformations II by I. M. Yaglom, translated by A. Shields
22. Elementary Cryptanalysis by Abraham Sinkov, revised and updated by
Todd Feil
23. Ingenuity in Mathematics by Ross Honsberger
24. Geometric Transformations III by I. M. Yaglom, translated by A. Shenitzer
25. The Contest Problem Book III Annual High School Mathematics Examina-
tions 1966–1972. Compiled and with solutions by C. T. Salkind and J. M.
Earl
26. Mathematical Methods in Science by George Polya
27. International Mathematical Olympiads—1959–1977. Compiled and with
solutions by S. L. Greitzer
28. The Mathematics of Games and Gambling, Second Edition by Edward
W. Packel
29. The Contest Problem Book IV Annual High School Mathematics Examina-
tions 1973–1982. Compiled and with solutions by R. A. Artino, A. M. Gaglione,
and N. Shell
30. The Role of Mathematics in Science by M. M. Schiffer and L. Bowden
31. International Mathematical Olympiads 1978–1985 and forty supplementary
problems. Compiled and with solutions by Murray S. Klamkin
32. Riddles of the Sphinx by Martin Gardner
33. U.S.A. Mathematical Olympiads 1972–1986. Compiled and with solutions
by Murray S. Klamkin
34. Graphs and Their Uses by Oystein Ore. Revised and updated by Robin
J. Wilson
35. Exploring Mathematics with Your Computer by Arthur Engel
36. Game Theory and Strategy by Philip D. Straffin, Jr.
37. Episodes in Nineteenth and Twentieth Century Euclidean Geometry by Ross
Honsberger
38. The Contest Problem Book V American High School Mathematics Examinations
and American Invitational Mathematics Examinations 1983–1988. Compiled
and augmented by George Berzsenyi and Stephen B. Maurer
39. Over and Over Again by Gengzhe Chang and Thomas W. Sederberg
40. The Contest Problem Book VI American High School Mathematics Examina-
tions 1989–1994. Compiled and augmented by Leo J. Schneider
41. The Geometry of Numbers by C. D. Olds, Anneli Lax, and Giuliana P. Davidoff
42. Hungarian Problem Book III, Based on the Eotvos Competitions 1929–1943,
translated by Andy Liu
43. Mathematical Miniatures by Svetoslav Savchev and Titu Andreescu
44. Geometric Transformations IV by I. M. Yaglom, translated by A. Shenitzer
45. When Life is Linear: from computer graphics to bracketology by Tim Chartier
46. The Riemann Hypothesis: A Million Dollar Problem by Roland van der Veen
and Jan van de Craats
47. Portal through Mathematics: Journey to Advanced Thinking by Oleg A. Ivanov.
Translated by Robert G. Burns.
Other titles in preparation.
MAA Service Center
P.O. Box 91112
Washington, DC 20090-1112
1-800-331-1MAA FAX: 1-240-396-5647
Contents
Foreword ix
Preface for an American Readership xi
Author’s Preface xiii
Part I Surprising and Easy 1
1 Surprising right triangles 3
2 Surprisingly short solutions of geometric problems 7
3 A natural assertion with a surprising proof 11
4 Surprising answers 17
5 A surprising connection between three sequences 23
Part II Algebra, Calculus, and Geometry: problems 27
6 Five problems and a function 29
7 Five solutions of a routine problem 33
8 Equations of the form f (x, y) = g(x, y) and their generalizations 39
9 The generalized version of Viete’s formula 49
10 Multiple roots of polynomials 55
11 Non-routine applications of the derivative 63
12 Complex numbers, polynomials, and trigonometry 71
13 Complex numbers and geometry 79
14 Areas of triangles and quadrilaterals 85
15 Constructions in solid geometry 93
16 Inequalities 101
17 Diophantine equations 111
18 Combinatorial tales 119
19 Integrals 129
vii
viii Contents
Part III Algebra, Calculus, and Geometry: theory (a little
way beyond high school mathematics) 139
20 Functional equations of elementary functions 143
21 Sequences given by recurrence relations 151
22 The “golden ratio” or solving equations of the form f (x) = x 161
23 Convex functions: inequalities and approximations 167
24 Taylor’s formula, Euler’s formula, and a combinatorial problem 177
25 Derivatives of vector-functions 187
26 Polynomials and trigonometric relations 199
27 Areas and volumes as functions of co-ordinates 207
28 Values of trigonometric functions and sequences satisfying a
certain recurrence relation 217
29 Do there exist further “numbers” beyond complex numbers? 223
Solutions of the supplementary problems 231
Index 303
Foreword
The teaching of elementary mathematics is often presented as a train track.
Students with early mastery of the mathematics “at their stop” are sent on the
next stop (bumped up a grade) without getting the chance to develop what
they know and see the landscape between stations. One of the biggest leaps
is between high school and university mathematics. What are we missing by
jumping to the next station?
Oleg Ivanov introduces us to the rich world between grade 12 plus or
minus epsilon mathematics (and here epsilon can be small or large!) and
university mathematics with a wonderful collection of mathematical tidbits
to intrigue, propel, and delight. Is there a natural way to find an explicit
formula for the nth Fibonacci number? The set of complex numbers is a field
that contains the real numbers; is there another such field? A rope is tied
around the Earth’s equator and then lengthened by 6 feet. How high can the
rope be raised off the equator to the same height all the way round? Now
suppose that the rope is pulled away from the Earth’s surface at just one
point. How high above the surface can that point of the rope be pulled?
The 29 mathematical themes presented in this text range in style and
content, background and outlook. Teachers and other life-long students of
mathematics occupy different places along the track between school and
beyond-school mathematics, and each will respond to the essays here in their
own ways. Ivanov has provided us a wide selection of deep and surprising
mathematical delights to reflect upon and savor. Wherever you are on the
track between high school mathematics and university courses, you can stop
and explore the landscape away from the track. Some things will be familiar
immediately, some will become clear a little later on. This book is a guide
to the landscape, with wonderful hikes mapped out, and promises to delight
the reader again and again.
Stop the train, pack your backpack, and follow Ivanov to the joy that
even elementary mathematics affords the explorer.
Karen Saxe for the NML Editorial Board
ix
Preface for anAmerican Readership
The purpose of this Preface is to give readers—be they teachers, students or
just someone interested in learning a little mathematics at first-year university
level (but occasionally dipping below and rising above that level)—an idea
of the level of mathematical expertise needed for a ready understanding of
each of the chapters—or “Themes”, as they are called—of the present book.
First a few words about the absolute minimum level of mathematical
skill assumed throughout. The reader should have a fairly clear idea of
the number hierarchy N ⊂ Z ⊂ Q ⊂ R ⊂ C, perhaps with the exception of
the final inclusion. The concept of a function is crucial. The reader is also
expected to know the basic facts about quadratic equations and have a good
idea of the use of mathematical induction. The basic Euclidean geometry of
triangles and circles and coordinate geometry as it applies to these figures
and parabolas is also taken for granted in not a few places. Thus possibly a
Grade 12 mathematics student and certainly a first year university calculus
student should be able to come to grips with most of the material of this
book. The more difficult or advanced Themes might be used to at least pique
the interest of high-school students, even if the techniques for answering
the questions raised are perhaps outside the high-school curriculum. Several
Themes start off gently, so that the first page or two can be read with interest
and profit by everyone: these are Themes 1, 3, 4, 12, 14, 15, 17, 18, and 22.
Robert Burns and Karen Saxe
xi
Author’s Preface
I have always been fascinated by the book “Proofs from THE BOOK” by
M. Aigner and G. M. Zigler. However, while most of the proofs that book
presents are indeed “elegant and amazing”, they tend not to be very easy; in
fact even the statements selected for proving are not so simple. The math-
ematical statements considered in the present book are, by contrast, con-
siderably more elementary. And furthermore, whereas the proofs of “Proofs
from THE BOOK” are really aimed only at professional mathematicians, the
beauty of the proofs contained in the present book can be appreciated by high
school teachers and students in schools offering more advanced mathemati-
cal instruction. It is precisely for this audience that this book is intended. It
aims at helping the teacher add variety to the lessons, and, I believe, should
bring the students to a better understanding of what mathematics is.
The book is divided into three parts. The title of Part 1, “Surprising
and Easy”, speaks for itself. Here are gathered intriguing mathematical facts
with the most striking proofs. Part 1 is by way of an introduction, where
the aim is to intrigue the reader. The other two parts are devoted to problem
solving: the problems of Part 2 involve only the standard concepts and facts
traditionally included in high school curricula, so that students may work
on these independently, while solving those of Part 3 will require a parallel
introduction to new concepts and ideas of proof. The Themes of Part 1 are
highly diverse—as indeed are those of Parts 2 and 3. Thus here the reader will
find: integer solutions of equations by geometric means (yielding surprising
answers); very short solutions of apparently difficult geometric problems,
obtained using analytic geometry; an unusual stereometric construction used
to solve a little known analogue of a well-known result of plane geometry;
an approximate solution of an unusual equation, obtained by means of the
calculus; and curious connections between the terms of three recurrence
sequences arising in the solution of a certain Theme 1 problem.
xiii
xiv Author’s Preface
Acknowledgements
The solution of mathematical problems and discussions of mathematical
topics with colleagues and students who have caught the mathematical bug,
provide a welcome sense of life’s repletion and the satisfaction it affords. I
may even say, more specifically, that without my colleagues and our mathe-
matical interchanges this book would never have been written. Thus some of
the mathematical ideas included here were topics of discussion with the panel
of judges of the Euler Olympiad, chaired by V. B. Nekrasov. It behooves me
to make special mention, however, of the role of some of my colleagues in
connection with the Themes of Part 1 of the present book.
The reduction to Pell’s equation of the equations appearing in the solution
of Problem 2 of Part 1 is due to V. M. Gol′khovoj. The fact that Problem 2
of Theme 2, although well known, would be the perfect example of the use
of algebraic methods in geometry, dawned on the author following a lecture
by R. R. Pimenov at the St. Petersburg Seminar for Mathematics Teachers.
The idea of the proof of the basic result of Theme 3 is due to A. Moshonkin.
It was B. I. Ryzhik who brought Problem 3 of Theme 4 to my attention. And
I am especially grateful to him for his constant encouragement to write this
book. Finally, it was B. M. Bekker who provided me with the first proof of
the basic result of Theme 5.
I thank all of the above from the bottom of my heart.
I am very grateful to Robert Burns, the translator of this book (and of
two others), and a friend whom I have known now for almost 20 years, for
his painstaking work producing the English versions of my books!
I am also deeply grateful to the Anneli Lax New Mathematics Library
Editorial Board and especially to its Chair, Karen Saxe, for much help in
improving the book and readying it for publication.
Oleg Ivanov, St. Petersburg, Russia
Solutions of thesupplementary problems
Theme 6. Five problems and a function
6.1. Observe first that since ax > 0, any solutions of ax = x must be positive.
Hence we may go over to the equivalent equation x ln a = ln x, or
ln a = ln xx
. We investigated the behavior of the function f (x) = ln xx
in
this section, and from our knowledge of that behavior we infer first that
the given equation has just one solution precisely if either ln a ≤ 0 or
ln a = 1e, that is, if a ∈ (0, 1] or a = e1/e, has exactly two solutions if
a ∈(1, e1/e
), and has no solutions for all other values of a. Figure 90
shows the graphs of y = ex/e and the line y = x, tangential to it at the
point (e, e). Note also that e1/e ≈ 1.44.
0 1 2 3 4
1
2
3
4
5
Figure 90
6.2. Method 1. We investigate the function f (x) = x4 2−x for x ≥ 1. Since
f ′(x) = 4x3 2−x − x4 2−x ln 2 = x3 2−x(4 − x ln 2),
this function is increasing on the interval[1, 4
ln 2
]and decreasing on[
4ln 2
,+∞). On our calculator (which is allowed!), we find that 4
ln 2≈
5.77. Hence the largest value of this function for natural values of x is
f (5) or f (6). Thus it only remains to compare these two values. Since
f (5) = 54
25 = 62532
≈ 19.5, while f (6) = 814
= 20.25, we conclude that
the largest term of the given sequence is x6.
231
232 Solutions of the supplementary problems
Method 2. Here is how best to solve this problem (or at least discuss its
solution) in a classroom of, for instance, grade tens. First one merely
calculates, that is, compiles a table of terms of the given sequence,
continuing the calculations until its behavior has become clear:
n 1 2 3 4 5 6 7
xn 0.5 4 10.125 16 19.5 20.25 18.8
It would seem that the largest term should be x6. So let’s try to prove
this directly: consider the inequality xn+1 < xn, that is, (n+1)4
2n+1 < n4
2n ,
which may be rewritten as(1 + 1
n
)4< 2. Since the left-hand expression
decreases with increasing n, once this inequality has been shown to
hold for some k, we can be sure it will then hold for all n ≥ k. From the
above table we see that this inequality holds for n = 6, so we infer that
it holds for all n ≥ 6. Hence the term x6 is the largest.
6.3. Instead of trying to minimize the given function, we minimize its loga-
rithm. Thus we want the least value of the function g(x) = x ln x. Since
g′(x) = ln x + 1, the desired least value is attained at x = 1e
≈ 0.37.
Hence the least value of the given function is e−1/e ≈ 0.69.
6.4. Consider the function f (x) = x1+1/x , whose values at natural n are
the given numbers n n√
n . As before, we consider the logarithm of this
function, that is, the function g(x) =(1 + 1
x
)ln x, for x ≥ 1. We have
g′(x) = −1
x2ln x +
(1 +
1
x
)1
x=
x + 1 − ln x
x2.
It is well known that x − 1 ≥ ln x for all x > 0, whence x + 1 − ln x >
0. Alternatively, we may differentiate. Since
(x + 1 − ln x)′ = 1 −1
x≥ 0 for x ≥ 1,
we infer that x + 1 − ln x ≥ 2 > 0 for x ≥ 1. Hence the function g is
increasing, so the function f is also increasing. We conclude, therefore,
that the numbers n n√
n, n = 1, 2, . . . are in increasing order in their
natural order.
Theme 7. Five solutions of a routine problem
7.1. Method 1. We wish to find all a for which the equation xx2+x+1
= a
has a solution. Rewrite the equation as ax2 + (a − 1)x + a = 0. When
Solutions of the supplementary problems 233
a = 0 we get x = 0. For a �= 0 this is a quadratic equation, so has a
(real) solution if and only if its discriminant is not negative. Thus we
obtain as the condition on a that it should satisfy (a + 1)(3a − 1) ≤ 0,
which holds for −1 ≤ a ≤ 13
.
Method 2. Clearly, f (0) = 0. Assuming x �= 0, we rewrite the expres-
sion for f (x) as
f (x) =1
x + 1x
+ 1.
Putting t = x + 1x
, we get f (x) = g(t) where g(t) = 1t+1
. Since |t | ≥ 2,
we need to find the values taken by g on the half-lines (−∞,−2] and
[2,+∞). We might illustrate the situation with Figure 91:
–4 –2 2 4 6 8
–1
13
1
Figure 91
However, it is in any case clear that the set of values taken by this
function on those half-lines is the union [−1, 0) ∪(0, 1
3
].
Method 3. Let’s see where the given function is monotonic (increasing
or decreasing). Its derivative is
f ′(x) =x2 + x + 1 − x(2x + 1)
(x2 + x + 1)2=
1 − x2
(x2 + x + 1)2.
Hence the function is decreasing on each of the intervals (−∞,−1] and
[1,+∞) and increasing on [−1, 1]. Since f (−1) = −1, f (1) = 13
and
f (x) → 0 as x → ±∞, we conclude that the range of f is the interval[−1, 1
3
](Figure 92).
7.2. Method 1. We rewrite the given equation as x2 + x + 1x
+ 1x2 = a,
and investigate the function f (x) = x2 + x + 1x
+ 1x2 . In order to see
where this function is increasing and where decreasing, we examine its
234 Solutions of the supplementary problems
–4 –2 2 4 6 8
–1
13
1
Figure 92
derivative
f ′(x) = 2x + 1 −1
x2−
2
x3=
2(x4 − 1)
x3+
x2 − 1
x2
=(x2 − 1)(2x2 + x + 2)
x3.
We see that f (x) increases on each of the intervals [−1, 0) and [1,+∞),
and decreases on (−∞,−1] and (0, 1]. Furthermore, f (−1) = 0,
f (1) = 4 and f (x) → +∞ as x → ∞ and as x → 0. Thus the graph
of the function has the following form (Figure 93):
–2 –1 1 2
2
4
6
8
Figure 93
Hence the equation f (x) = a has two solutions precisely for those a in
the interval (0, 4).
Method 2. Putting t = x + 1x
changes the equation to t2 + t = a + 2,
and once again, since∣∣x + 1
x
∣∣ ≥ 2, we need to examine this equation
only on the union of the intervals (−∞,−2] and [2,+∞). The graph
of the binomial t2 + t is shown in Figure 94.
Hence for a + 2 > 6, that is, for each a > 4, the quadratic equation
t2 + t = a + 2 has two solutions t1 and t2, one of which is less than
−2 and the other greater than 2. It follows that in this case the original
equation will have four solutions. If a = 4 then t1 < −2, and t2 = 2,
Solutions of the supplementary problems 235
–3 –2 –1 1 2 3
2
4
6
8
Figure 94
in which case the original equation has two negative solutions as well
as the solution x = 1. If 0 < a < 4 then once again we have t1 < −2,
but now 0 < t2 < 2, so that in this case the original equation has two
solutions.
In this last approach, we might instead have analyzed the situations
t1 ≤ −2 and t2 ≥ 2 by algebraic means, but shall not pursue this further.
7.3. We give several solutions of Part a) of the problem.
Method 1. We examine the graph of y =√
x + 3 to see how the number
of its points of intersection with the line y = 1 + ax varies with the slope
a of that line. Every such line passes through the point (0, 1), which
lies below the “half-parabola” y =√
x + 3. Figure 95 presents a sketch
of that half-parabola together with the line y = 1 + x3
(which passes
through the points (−3, 0) and (0, 1)) and two other straight lines. One
of the latter two lines has slope greater than 13
while the other has
negative slope.
–3 –2 2 4 6
1
3
Figure 95
Clearly, for 0 < a ≤ 13
the given equation will have two solutions while
for every other value of the parameter a it will have only one solution.
236 Solutions of the supplementary problems
Method 2. We rewrite the given equation as√
x + 3 − 1
x= a,
and sketch the graph of the function f (x) =√
x + 3 − 1
x. Its derivative
is
f ′(x) =x
2√
x+3−
√x + 3 + 1
x2
=x − 2(x + 3) + 2
√x + 3
2x2√
x + 3=
2√
x + 3 − x − 6
2x2√
x + 3.
On squaring both sides of the inequality 2√
x + 3 ≤ x + 6, we get the
inequality x2 + 8x + 24 ≥ 0, which is easily verified as valid for all x.
Hence f ′(x) < 0 everywhere on the domain of the function f , which
therefore decreases on that domain, that is, on the intervals [−3, 0)
and (0,+∞). It is easy to see that f (x) → 0 as x → +∞. All that
remains for us to be able to sketch the graph is to note that f (−3) = 13
.
From the following sketch it is clear that the equation in question has
two solutions for 0 < a ≤ 13
and just one for every other value of the
parameter a (Figure 96).
–3 2 4 6
1
3
Figure 96
Method 3. Setting t =√
x + 3 yields the equation at2 − t + 1 − 3a =0. The number of non-negative solutions of this equation will then be
the same as the number of solutions of the original equation. If a = 0
then t = 1. Assuming a �= 0, we rewrite the equation in the form
t2 −t
a+
1 − 3a
a= 0.
By Viete’s formula, if the constant term here is negative, then this
quadratic equation will have roots of opposite sign, and therefore just
one positive root. Thus if a < 0 or a > 13
there will be just one positive
Solutions of the supplementary problems 237
root. If a = 13
then the equation becomes t2 − 3t = 0, whence t = 0 or
3. Now suppose 0 < a < 13
. The discriminant of the equation is
1
a2−
4(1 − 3a)
a=
12a2 − 4a + 1
a2,
which is positive for all a, so the equation has two roots for all a in the
interval of present interest. Since for these a their product is positive
and their sum is 1a
> 0, both roots must be positive.
Method 4. Again we make the change of variable t =√
x + 3, but this
time rewrite the resulting equation in the form t−1t2−3
= a and investigate
the behavior of the function f (t) = t−1t2−3
for t ≥ 0. Since
f ′(t) = −t2 − 2t + 3
(t2 − 3)2< 0
for all t , this function is decreasing on each of the intervals [0,√
3 )
and (√
3 ,+∞). We also have f (t) → 0 as t → +∞ and f (0) = 13
.
Putting all this together we obtain the following sketch of the graph,
from which the solution of the problem can be read off (Figure 97).
1 2 3 4 5
–2
–1
1
2
3
4
Figure 97
We now see how each of the above four approaches works for Part b).
Method 1. The diagram is significantly different since now the point
through which all the relevant lines—those with equation of the
form y = ax + 2—pass, namely (0, 2), lies above the half-parabola
y =√
x + 3. Hence not all such lines meet the half-parabola, and
two of them are tangential to it. Let’s find those values of a for
which the line y = ax + 2 is tangential to the graph of y =√
x + 3.
The simplest way to do this is to see for which a the equation
(x + 3) = (ax + 2)2 has just one solution. The discriminant of this
equation is (4a − 1)2 − 4a2, which vanishes when 4a − 1 = 2a, that
is, a = 12
, or when 4a − 1 = −2a, that is, a = 16
. In Figure 98 the two
238 Solutions of the supplementary problems
dashed lines are the tangent lines y = x2
+ 2 and y = x6
+ 2, while the
solid line represents the straight line y = 2x3
+ 2 passing through the
points (−3, 0) and (0, 2).
–3 –2 2 4 6 8
1
3
Figure 98
From this diagram we can read off the answer: the given equation has
no solutions for 16
< a < 12
, exactly one solution for a = 16, a = 1
2, and
also for a ≤ 0 and a > 23, and two solutions for 1
2< a ≤ 2
3.
Method 2. We examine the behavior of the function f (x) =√x + 3 − 2
x. Its derivative is
f ′(x) =x
2√
x+3−
√x + 3 + 2
x2
=x − 2(x + 3) + 4
√x + 3
2x2√
x + 3=
4√
x + 3 − x − 6
2x2√
x + 3.
Thus this time we need to solve the inequality 4√
x + 3 ≤ x + 6.
Squaring both sides yields the inequality x2 − 4x − 12 ≥ 0, whence
x ∈ [−3,−2] ∪ [6,+∞). Hence the given function is decreasing on
each of the intervals [−3,−2] and [6,+∞) and increasing on each of
[−2, 0) and (0, 6]. Clearly, f (x) → 0 as x → +∞ and f (x) → ∞ as
x → 0. We tabulate the values of the function at the key values of x:
x −3 −2 6
f (x) 23
12
16
Here, then, is a sketch of the graph of the function (Figure 99), from
which the solution can be read off:
Method 3. The discriminant of the equation t2 − ta
+ 2−3aa
= 0 is12a2−8a+1
a2 , so this equation has solutions if and only if a ≤ 16
or a ≥ 12
.
Solutions of the supplementary problems 239
–3 2 4 6
3
Figure 99
The remaining argumentation and calculations are similar to those used
above in connection with the solution of Part a) by this method.
Method 4. We set t =√
x + 3 and investigate the function f (t) = t−2t2−3
for t ≥ 0. Since
f ′(t) = −(t − 1)(t − 3)
(t2 − 3)2,
this function is decreasing on the intervals [0, 1] and [3,+∞), increas-
ing on [1,√
3 ) and (√
3 , 2], and furthermore f (t) → 0 as t → +∞,
f (0) = 23
, f (1) = 12
and f (3) = 16
. Hence the graph is as shown in
Figure 100, whence the answer.
1 2 3 4 5
–2
–1
1
2
3
4
Figure 100
7.4. Method 1. The graph of y =√
4 − x2 is the upper semicircle of radius 2
with center at the origin of coordinates. The set defined by the equation
y = |x − 2a| − 3a is the absolute value function translated through the
vector (2a,−3a), so its graph looks like a big open “V”, or a checkmark,
with its “corner”, that is, vertex, at the point P (2a,−3a). The vertex P
lies on the straight line y = − 32x for all values of a. Figure 101 shows
the situation when the right-hand side of the “V” passes through the
right-most point of the semicircle.
240 Solutions of the supplementary problems
–3 –2 –1 1 2 3
–2
–1
1
2
3
Figure 101
The value of the parameter a in this situation is obtained by solving the
equation |2 − 2a| − 3a = 0. Observe first that a ≥ 0. We have either
2 − 2a = 3a, yielding a = 25
, or 2a − 2 = 3a, yielding a = −2, which
we can ignore. For a > 25
the graph of y = |x − 2a| − 3a will lie below
that depicted in Figure 101, so the original equation will have either one
solution of none. It is easy to check that in fact for a ∈ ( 25, 2] there is
just one solution and for a > 2 none.
As a decreases, starting from the value a = 25, the vertex P of the big
“V” moves up the line y = − 23x and the situation becomes that shown
in Figure 102a.
–3 –2 –1 1 2 3
–1
1
2
3
–3 –2 –1 1 2 3
–1
1
2
3
(a) (b)
Figure 102
Now suppose that the point P = (2a,−3a) is on the semicircle (as in
Figure 102b). For this to be the case we need 4a2 + 9a2 = 4, whence
a = − 2√13
. Since the slope of the tangent line to the semicircle at P is23
, our “V” lies above that tangent line, so that, apart from P , the “V”
has no other points of intersection with the semicircle. It follows that for
a < − 2√13
the original equation has no solutions and has exactly two
solutions for a ∈(− 2√
13, 2
5
].
Solutions of the supplementary problems 241
Method 2. Here is a sketch of the set of points (x, y) satisfying the
equation√
4 − x2 = |x − 2y| − 3y, that is, of its graph (Figure 103).
–3 –2 –1 1 2 3
–1
1
2
3
Figure 103
Its left-most point is (−2, 2), its lowest point(− 4√
13,− 2√
13
), and its
right-most point(2, 2
5
). Since for each value of the parameter a the
number of solutions of the original equation is equal to the number
of points of intersection of the above graph with the line y = a, we
immediately infer that the original equation has just one solution when
a = − 2√13
or a ∈(
25, 2
], two solutions when a ∈
(− 2√
13, 2
5
], and none
for all other values of a.
But of course we have yet to explain how the above sketch was arrived
at!
Suppose first that x − 2y ≥ 0. In this case the equation whose graph
we seek to construct simplifies to√
4 − x2 = x − 5y or y = 15
(x −√4 − x2 ). Since we are in the case y ≤ x
2, it follows that
15
(x −
√4 − x2
)≤
x
2, or − 3x ≤ 2
√4 − x2 .
The latter inequality is obviously true for x ∈ [0, 2]. Suppose x ≤ 0.
Squaring the second inequality above, we obtain 9x2 ≤ 16 − 4x2,
or x2 ≤ 1613
, whence x ∈[− 4√
13, 0
]. We conclude that y = 1
5(x −
√4 − x2 ) for x ∈
[− 4√
13, 2
].
In the case 2y ≥ x, the function we are investigating becomes y =−x −
√4 − x2. The inequality −2x − 2
√4 − x2 ≥ x is equivalent to
−3x ≥ 2√
4 − x2, which is easily shown to hold precisely when x ∈[−2,− 4√
13
].
Thus we have so far shown that
y =
⎧⎨⎩
−x −√
4 − x2 for x ∈[−2,− 4√
13
],
15
(x −√
4 − x2 ) for x ∈[− 4√
13, 2
].
242 Solutions of the supplementary problems
Consider first the function f (x) = −x −√
4 − x2 . Its derivative is
f ′(x) = −1 +x
√4 − x2
.
Since the relevant values of x are negative, it follows that f ′(x) < 0 for
those x. Hence for x ∈[−2,− 4√
13
]the function we are investigating is
decreasing.
Now consider the function f (x) = 15
(x −√
4 − x2 ). Differentiating,
we obtain
f ′(x) =1
5
(1 +
x√
4 − x2
).
Examining this to see where f ′(x) ≥ 0, we obtain the inequality√4 − x2 ≥ −x, whence x ≥ −
√2 . Since − 4√
13> −2, the function
in question is increasing for x ∈[− 4√
13, 2
].
The final data needed to obtain the above sketch of the graph of our
function are its values at x = ±2 and − 4√13
(see the table).
x −2 − 4√13
2
f (x) 2 − 2√13
25
Theme 8. On equations of the form f (x, y) = g(x, y)and their generalizations
8.1. Solution of Exercise 1. The straight line y = kx + b avoids the parabola
y = x2 precisely if the equation x2 − kx − b = 0 has no (real) solution,
which is the case precisely when its discriminant is negative: k2 + 4b <
0. Similarly, the line y = kx + b avoids the parabola y = −x2 + 6x − 8
precisely when the discriminant of the equation x2 + (k − 6)x + b +8 = 0 is negative, that is, (k − 6)2 − 4b − 32 < 0. Hence the straight
line y = kx + b avoids both of the given parabolas precisely if k and
b satisfy the system of inequalities k2 − 12k + 4 < 4b < −k2. This
system has solutions if and only if the inequality k2 − 12k + 4 < −k2
is solvable, that is, if and only if k2 − 6k + 2 < 0 is solvable—which it
is. It is satisfied by k = 1, for instance. With this value of k, the above
system of inequalities becomes −7 < 4b < −1, which has b = −1 as
a solution, for example. Hence the straight line y = x − 1 is just one
example of a line meeting neither of the two given parabolas.
Solutions of the supplementary problems 243
Solution of Exercise 2. There’s not much to prove here, of course. We
have
M(x0, y0) ∈ A ∪ B ⇐⇒ M ∈ A
or M ∈ B ⇐⇒ f (x0, y0) = 0
or g(x0, y0) = 0 ⇐⇒ f (x0, y0)g(x0, y0) = 0.
8.2. Suppose that q(x, y) = 0 is a quartic curve that is the union of two
closed curves, one of which is entirely contained in the interior of the
other, together with further points. Let K be one of these additional
points and L a point different from K in the (or a) region bounded by
the inner of the two curves. Let ax + by + c = 0 be an equation of the
line containing the points K and L, and consider the system{
q(x, y) = 0,
ax + by + c = 0.
On the one hand, solving this system reduces to solving a quartic equa-
tion in one variable, and therefore has at most four solutions, while on
the other hand the line KL meets the closed curves contained one in the
other in at least four points (see Figure 104), so has at least five points
in common with the given quartic curve. This contradiction establishes
the assertion of the problem.
Figure 104
8.3. The first question needing to be settled here is the following one: what
conditions on the coefficients of an equation of the form
a11x2 + 2a12xy + a22y
2 + 2a13x + 2a23y + a33 = 0,
ensure that it is the equation of a circle? Since a circle is defined by
an equation of the form a(x − x0)2 + a(y − y0)2 = d where ad > 0,
it is necessary that a12 = 0 and a11 = a22. We need to see how these
conditions can be satisfied by a linear combination of the two given
equations. We can ensure that there is no term in xy in such a linear
244 Solutions of the supplementary problems
combination by adding b12 times the first to −a12 times the second. The
coefficients of x2 and y2 in the resulting equation are then respectively
a11b12 − a12b11 and a22b12 − a12b22. Hence there exists a linear combi-
nation of the two given equations that is the equation of a circle only if
a11b12 − a12b11 = a22b12 − a12b22, or (a11 − a22)b12 = (b11 − b22)a12,
or
a11 − a22
a12
=b11 − b22
b12
.
This condition has a transparent geometric meaning, about which, how-
ever, the author will say nothing further except to note that it was this
that suggested the next problem to him.
8.4. If we choose our coordinate system with axes coinciding with the angle
bisectors, then the two angles (each considered as a pair of rays) are
contained in the respective straight-line pairs given by equations of the
form (x − a)2 = k1y2 and x2 = k2(y − b)2, or
x2 − k1y2 − 2ax + a2 = 0 and x2 − k2y
2 + 2k2by − k2b2 = 0.
Multiplying the first of these equations by 1 + k2 and the second by
−(1 + k1) and adding, we obtain a quadratic equation in x and y with
the sum of its degree-two terms equal to (k2 − k1)(x2 + y2). We have
thus obtained the equation of a circle passing through the four points of
intersection of the arms of the respective angles (Figure 105).
Figure 105
Of course, this problem also has a geometrical solution. Find it!
Theme 9. The generalized version of Viete’sformula
9.1. a) From x1 + x2 + x3 = 0 it follows that
x21 + x2
2 + x23 = −2(x1x2 + x2x3 + x3x1) = 6.
Solutions of the supplementary problems 245
b) From x1 + x2 + x3 = 0 it follows that
x31 + x3
2 + x33 = 3x1x2x3 = −3.
9.2. Set x1 = cos 2π9
, x2 = cos 8π9
and x3 = cos 14π9
. Since cos 2π3
=cos 8π
3= cos 14π
3= − 1
2and cos 3t = 4 cos3 t − 3 cos t , it follows that
x1, x2 and x3 are the roots of the cubic equation 4x3 − 3x + 12
= 0.
Hence we deduce, as in the solution of the preceding problem, that
x31 + x3
2 + x33 = 3x1x2x3 = − 3
8.
Of course, this problem partakes of the subject-matter of Theme 12,
where the idea behind it is developed much further.
9.3. The given condition on a , b, and c implies that (a + b + c)(ab + bc +ac) = abc, whence
0 = a2b + abc + a2c + ab2 + b2c + abc + abc + bc2 + ac2 − abc
= ab(a + c) + ac(a + c) + b2(a + c) + bc(a + c)
= (a + c)(b2 + ab + bc + ac) = (a + c)(a + b)(b + c),
so that at least one of the final three factors must be zero.
Here is a different solution using Viete’s formula. Consider the
polynomial
p(x) = (x − a)(x − b)(x − c) = x3 − Ax2 + Bx − C.
The assumption that (a + b + c)(ab + bc + ac) = abc then becomes
C = AB. Hence
p(x) = x3 − Ax2 + Bx − AB = x2(x − A) + B(x − A)
= (x − A)(x2 + B),
and we see that A is actually a root of the polynomial. Hence we must
have a + b + c = a or a + b + c = b or a + b + c = c, so that some
two of the given numbers add to zero.
In conclusion we note that this problem is often formulated instead as
follows. Prove that
if1
a+
1
b+
1
c=
1
a + b + c, then
1
a5+
1
b5+
1
c5=
1
(a + b + c)5.
9.4. Let x1 < x2 < x3 be the roots of the given polynomial. If they are in
arithmetical progression, then x1 + x2 + x3 = 3x2, whence, by Viete’s
246 Solutions of the supplementary problems
theorem, x2 = − a3. Thus − a
3is a root of the equation, that is,
−a3
27+
a3
9−
ab
3+ c =
2a3
27−
ab
3+ c = 0,
whence 2a3 + 27c = 9ab.
Suppose now that 2a3 + 27c = 9ab, or, equivalently, c = ab3
− 2a3
27. We
shall then have
x3 + ax2 + bx + c = x3 + ax2 + bx +ab
3−
2a3
27
= x3 +a3
27+ ax2 −
a3
9+ bx +
ab
3
=(x +
a
3
)(x2 −
ax
3+
a2
9
)
+ a(x +
a
3
) (x −
a
3
)+ b
(x +
a
3
)
=(x +
a
3
)(x2 +
2ax
3+ b −
2a2
9
).
Hence the number x1 = − a3
is one of the roots of the given equation. The
sum of the roots of the quadratic trinomial factor of the final expression
above is − 2a3
= 2x1, so if these roots are real and distinct then the three
roots of the original cubic will be in arithmetic progression. Hence
the necessary further condition on a, b and c for those roots to be in
arithmetic progression is that the quadratic trinomial
x2 +2ax
3+ b −
2a2
9
have two distinct real roots, or, equivalently, that its discriminant be
positive, which will be the case precisely if a2 > 3b.
Theme 10. Multiple roots of polynomials
10.1. Since the equation x3 + 3x2 − 4x + 2 = 1 − 7x may be rewritten
as (x + 1)3 = 0, it has just one solution. Hence the straight line
y = 1 − 7x has exactly one point of intersection with the graph of the
polynomial p(x) = x3 + 3x2 − 4x + 2. Furthermore, since the equa-
tion p(x) = 1 − 7x has the number −1 as a root of multiplicity three,
that straight line must be tangential to the graph of the cubic. It is easy
to see that this is the only line satisfying the conditions of the problem.
Solutions of the supplementary problems 247
It is worthwhile mentioning by the way that the point of intersection
of the graph and the line is a center of symmetry of that graph.
10.2. a) One such straight line is easy to find. For, since
x4 + 2x3 + x2 + 2x + 1 = x2(x + 1)2 + 2x + 1,
it follows that the line y = 2x + 1 is tangential to the graph of the
given polynomial function at the points with abscissas 0 and −1. It
seems intuitively clear (especially in view of the result of Problem
4) that this is the only such line. But let’s prove it rigorously. Thus
let y = ℓ1(x) and y = ℓ2(x) be equations of two lines each of which
is tangential to the graph of the given polynomial function p(x) of
degree 4 at two distinct points. Then
p(x) − ℓ1(x) = a(x − t1)2(x − t2)2 = a(q1(x)
)2,
p(x) − ℓ2(x) = a(x − u1)2(x − u2)2 = a(q2(x)
)2,
whence
ℓ2(x) − ℓ1(x) = a(q2(x) − q1(x)
)(q2(x) + q1(x)
),
which is impossible since the polynomial on the right-hand side of
this equation has degree at least 2 while that on the left-hand side
has degree at most 1.
b) If x1 and x2 are the abscissas of two points where the straight line
y = kx + d is tangential to the graph of the given polynomial, then
x1 and x2 must each be roots of multiplicity two of the equation
x4 + ax2 + bx + c = kx + d, that is, roots of multiplicity two of
the polynomial x4 + ax2 + (b − k)x + c − d. Since the coefficient
of x3 of this polynomial is zero, we have x1 + x2 = 0, whence
x4 + ax2 + (b − k)x + c − d = (x − x1)2(x + x1)2
= (x2 − x21 )2 = x4 − 2x2
1x2 + x41 .
Hence a = −2x21 , b − k = 0 and c − d = x4
1 , whence k = b and
d = c − x41 = c − a2
4. We conclude that the desired “double tan-
gent line” has equation y = bx + c − a2
4.
10.3. Clearly, we can position a circle of any radius so that it is tangential
to any given parabola at two distinct points. All one needs to do is to
place the circle inside the parabola and let it descend till they touch.
248 Solutions of the supplementary problems
Obviously, in this final position the center of the circle will lie on the
axis of symmetry of the parabola (Figure 106).
Figure 106
However, this is not what the problem is about. It asks rather whether
it is possible for just one of the two points of intersection not to be a
point of tangency.
Consider the parabola y = x2 and a circle (x − x0)2 + (y − y0)2 = r2.
The abscissas of the points of intersection of these two curves are the
solutions of the equation
(x − x0)2 + (x2 − y0)2 = r2,
an equation of degree 4. We are assuming that this equation has just
two roots x1 and x2, where x1 is the abscissa of a point of tangency of
the two curves and therefore a multiple root. If in fact x1 is a double
root, then x2 will also have to be double root, and the second point
of intersection of the parabola and circle will then also be a point of
tangency. However, is it not at least theoretically possible that the first
root x1 has multiplicity three?
Let’s suppose that the point A(1, 1) is one of the points of intersection
of the parabola y = x2 with some circle of radius r . The tangent line
to the parabola at that point has equation y = 2x − 1. Let P denote
the center of the circle. Since this straight line is also tangential to the
circle, the vector AP is perpendicular to the that line, and therefore
parallel to the vector a(−2, 1). Hence the point P has coordinates of
the form (1 − 2t, 1 + t), whence r2 = 5t2. Hence the abscissas of the
points of intersection of parabola and circle are roots of the equation
(x − 1 + 2t)2 +(x2 − 1 − t
)2 = 5t2.
By construction, for every t the number x = 1 is a multiple root of
this equation. Our idea is to choose the value of t so that it is a triple
Solutions of the supplementary problems 249
root. We now carry out the algebraic manipulation needed to exhibit
(x − 1)2 as a factor of the difference of the two sides of this equation:
f (x) = (x − 1 + 2t)2 +(x2 − 1 − t
)2 − 5t2
= (x − 1)2 + 4t(x − 1) +(x2 − 1
)2 − 2t(x2 − 1)
= (x − 1)(x − 1 + 4t + (x − 1)(x + 1)2 − 2t(x + 1)
)
= (x − 1)(x − 1 + (x − 1)(x + 1)2 − 2t(x − 1)
)
= (x − 1)2((x + 1)2 + 1 − 2t
).
Hence we see that x = 1 is a root of multiplicity greater than two if
and only if (x + 1)2 + 1 − 2t = 0 when x = 1, which occurs at the
value t = 52. Since for this value of t we have
f (x) = (x − 1)3(x + 3),
the second point of intersection of the parabola y = x2 and the circle
(x + 4)2 +(y − 7
2
)2 = 1254
is the point B(−3, 9). Figure 107 shows
the parabola and the circle we have just constructed.
–10 –5 –3 5–2
2
4
6
9
Figure 107
Exercise. Verify that the graph of the function f (x) is as sketched in
Figure 108.
–2 –1 1 2
–20
10
Figure 108
250 Solutions of the supplementary problems
Theme 11. Non-routine applications of thederivative
11.1. Since
∣∣f ′(y)∣∣=
∣∣∣∣ limx→y
f (x) − f (y)
x − y
∣∣∣∣= limx→y
∣∣∣∣f (x) − f (y)
x − y
∣∣∣∣ ≤ limx→y
|x − y|=0,
we infer that f ′(y) = 0 for all y ∈ R, so that f (x) is constant.
Here is a proof avoiding use of the derivative. Consider any numbers
a < b and subdivide the interval [a, b] into n equal subintervals by
means of points x0 = a < x1 < . . . < xn = b. By assumption, we have
|f (xk+1) − f (xk)| ≤ (xk+1 − xk)2 = (b−a)2
n2 , whence
|f (b) − f (a)| =
∣∣∣∣∣
n−1∑
k=0
(f (xk+1) − f (xk)
)∣∣∣∣∣
≤n−1∑
k=0
∣∣(f (xk+1) − f (xk))∣∣ =
(b − a)2
n.
Since the number n was arbitrary, and (b−a)2
n→ 0 as n → ∞, we
conclude that f (b) = f (a).
11.2. We may assume that a > b > 0. Rewriting the desired pair of inequal-
ities in the form
√ab
<
ab
− 1
ln ab
<
ab
+ 1
2
and setting t = ab
> 1, we obtain
√t <
t − 1
ln t<
t + 1
2, or
2(t − 1)
t + 1< ln t <
√t −
1√
t.
The following diagram shows what these inequalities look like geo-
metrically (Figure 109):
Now let’s prove them. Since
(ln t −
2(t − 1)
t + 1
)′=
1
t−
4
(t + 1)2=
(t − 1)2
t(t + 1)2≥ 0 ,
this difference is increasing. Since it is equal to zero at t = 1, it will
therefore be positive for t > 1, whence
ln t >2(t − 1)
t + 1.
Solutions of the supplementary problems 251
1 2 3 4 5
1
Figure 109
For the other difference we have(√
t −1
√t
− ln t
)′=
1
2√
t+
1
2√
t3−
1
t
=t + 1 −
√t
2√
t3=
(√
t − 1)2
2√
t3≥ 0,
showing that this function is also increasing. Since it is zero at t = 1,
it will be positive for all t > 1, whence
√t −
1√
t> ln t.
Remark. The inequality of this problem has an interesting interpreta-
tion. We first need to rewrite it as
2
a + b<
ln a − ln b
a − b<
1√
ab.
By the Mean-Value Theorem the quotient ln a−ln ba−b
is equal to the deriva-
tive of the logarithm function at some point c of the interval (b, a).
Since (ln x)′ = 1x
, we infer that
2
a + b<
1
c<
1√
ab, or
√ab < c <
a + b
2.
Thus it turns out that the “intermediate point” c lies between the
geometric and arithmetic means of the endpoints of the interval [b, a].
11.3. Since 4ab ≤ (a + b)2 while 2(a2 + b2) ≥ (a + b)2, neither of these
inequalities is any use in helping us to determine which of the num-
bers 8ab(a2 + b2) and (a + b)4 is larger. However, one can establish
8ab(a2 + b2) ≤ (a + b)4 by direct means (see the remark at the end of
the present solution).
252 Solutions of the supplementary problems
We shall prove that the inequality in question holds for all a, b ≥ 0
if and only if k ≥ n. Set u = (a + b)2 and v = 2ab. Then a2 + b2 =u − v and u ≥ 2v. The inequality in question then becomes
vk(u − v)n ≤(u
2
)k+n
, or(v
u
)k (1 −
v
u
)n
≤1
2k+n.
We now set t = vu
≤ 12, and examine the behavior of the function
f (t) = tk(1 − t)n on the interval[0, 1
2
]. We have
f ′(t) = ktk−1(1 − t)n − ntk(1 − t)n−1 = tk−1(1 − t)n−1(k − (k + n)t).
If k ≥ n then kk+n
≥ 12, so f (t) is increasing on the interval
[0, 1
2
],
whence f (t) ≤ f(
12
)= 1
2k+n . On the other hand, if k < n then kk+n
<12, whence we infer that the function f attains its largest value at some
interior point of the interval, which will therefore be greater than f(
12
).
Remark. Here is a different proof of the fact that if k ≥ n then the
inequality in question holds for all a, b ≥ 0. Set ℓ = k − n and rewrite
that inequality in the form
(ab)n(a2 + b2)n(ab)ℓ ≤(a + b)4n
8n·
(a + b)2ℓ
4ℓ.
It now only remains to observe that ab ≤ (a+b)2
4and ab(a2 + b2) ≤
(a+b)4
8, the latter inequality holding since
(a + b)4 − 8ab(a2 + b2) = (a − b)4 ≥ 0.
11.4. Suppose Mike turns off the road after walking along it for x km. Thus
the time he spends walking along the road is x5
hours. From that point
on he walks in a straight line through the fields to the pond, a distance
of√
4 + (2 − x)2 =√
x2 − 4x + 8 km. Hence that part of his journey
takes√
x2−4x+83
hours. Thus the time he takes to walk the whole route
is
t(x) =x
5+
√x2 − 4x + 8
3.
The derivative of this function is
t ′(x) =1
5+
x − 2
3√
x2 − 4x + 8.
Note that t ′(0) = 15
− 1
3√
2< 0, while t ′(2) = 1
5> 0. Hence the least
value of the function t(x) occurs at some point of the interval (0, 2). In
order to find that point we solve the inequality t ′(x) ≤ 0 for x ∈ [0, 2].
Solutions of the supplementary problems 253
We have, in succession,
1
5≤
2 − x
3√
x2 − 4x + 8,3√
x2 − 4x + 8 ≤ 5(2 − x),4x2 − 16x + 7 ≥0,
whence we get x ∈[0, 1
2
], and conclude that Mike should walk along
the road for only a half-kilometer before turning off and heading
directly for the pond.
In the second case, we need to minimize the function
t(x) =x
5+
√x2 − 4x + 20
3,
whose derivative is
t ′(x) =1
5+
x − 2
3√
x2 − 4x + 20.
Since t ′(0) = 15
− 1
3√
5> 0, we might suspect that in this case the
function is increasing on the whole interval [0, 2]. And in fact on
solving the inequality
1
5+
x − 2
3√
x2 − 4x + 20≥ 0,
we arrive at the inequality x2 − 4x − 5 ≤ 0, valid for all x ∈ [0, 2].
The following diagram shows the graphs of the function t(x) in each
of the two cases (Figure 110):
0.5 1.0 1.5 2.0
0.960.981.001.021.041.06
0.5 1.0 1.5 2.0
1.55
1.60
1.65
1.70
(a) (b)
Figure 110
In fact, it is more appropriate to solve this problem once and for all in
the general case. Thus let u and v denote the respective speeds with
which Mike walks along the road and through the fields. And denote
by a the distance along the road to the point from which the direct path
to the pond is at 90◦ to the road, and b the distance from this point to
254 Solutions of the supplementary problems
the pond. We then have
t(x) =x
u+
√x2 − 2ax + a2 + b2
v, x ∈ [0, a],
so that
t ′(x) =1
u+
x − a
v√
x2 − 2ax + a2 + b2.
We look for a relation between the various parameters of the problem
ensuring that the function t(x) attains its least value somewhere on
the interval (0, a). To this end, we solve the inequality t ′(x) ≤ 0. After
some routine algebraic manipulation, one arrives at the inequality
x2 − 2ax + a2 −b2v2
u2 − v2≥ 0.
The left-hand quadratic trinomial is negative at x = a (we are assuming
u > v). Hence in order for there to be a value of x in the interval (0, a)
for which this inequality is valid, the trinomial should be positive at
x = 0. Thus we require that a2 > b2v2
u2−v2 , or au >√
a2 + b2 v.
We conclude that if au >√
a2 + b2 v then Mike should say on the
road for the distance a − bv√u2−v2
, while if au ≤√
a2 + b2 v then he
should head straight for the pond from his starting point in the village.
11.5. This problem is, in fact, a routine exercise on the derivative. The author
included it in this section for the following reason. In his experience,
the standard reaction of students to the problem is to start “guessing”;
instead of beginning the honest labor of calculation, they try to guess
the answer based on their idea of “geometrical intuition”. Thus this
application of the derivative is, after all, non-routine, but only in the
sense of helping to overcome the students’ routine reaction to it.
We shall for convenience assume the side of the base of the pyramid
to have length 2. An apothem (the altitude of a side face measured
from the apex, see Figure 90a of the pyramid will form a side of an
isosceles triangle with base of length 2 and vertical angle of cosine 2326
(namely, the vertical triangle though the middle of the pyramid with
its base parallel to two sides of the pyramid’s base, shown in Figure
111b. Hence the length d of an apothem is d = 2
√133
(use the Law of
Cosines). A cross-section of the pyramid by a plane passing through
an edge of the square base will have the form of a trapezoid with one
base of length 2 (Figure 112a).
Solutions of the supplementary problems 255
d d d
2
(a) (b)
Figure 111
Let the length of the other base be 2x. We infer the height h of such
a trapezoid by applying the Law of Cosines to the triangle with sides
of lengths d and dx (Figure 112b) meeting at the apex at an angle of
cosine 2326
(and with base the middle line of the trapezoid, equal in
length to its height), obtaining
h =2
√3
√13x2 − 23x + 13 .
Hence the area of the cross-section is 2√3
(x + 1)√
13x2 − 23x + 13 .
Define f (x) = (x + 1)√
13x2 − 23x + 13 . With a view to finding the
h
d
h
2
dx
(a) (b)
Figure 112
256 Solutions of the supplementary problems
largest value of this function, we calculate its derivative:
f ′(x) =√
13x2 − 23x + 13 +(x + 1)(26x − 23)
2√
13x2 − 23x + 13
=52x2 − 43x + 3
2√
13x2 − 23x + 13.
We see that the derivative vanishes at x1 = 113
and x2 = 34
, with the
original function having a local maximum at x1 and a local minimum
at x2. Hence the largest of the relevant values of f (x) is either f (x1) or
f (1). Since f (x1) > f (0) =√
13 > 2√
3 = f (1), we conclude that
its largest value occurs at x1.
Thus the cross-section of the type in question with largest area is that
cutting each of two of the lateral edges of the pyramid in the ratio
1 : 12, measured from the apex.
Theme 12. Complex numbers, polynomials, andtrigonometry
12.1. Since the nth roots of unity other than 1 are precisely the roots of the
polynomial xn−1 + xn−2 + · · · + 1, we have
(x − z1)(x − z2) · · · (x − zn−1) = xn−1 + xn−2 + · · · + 1.
Substituting x = 1 in this equation, we obtain
(1 − z1)(1 − z2) · · · (1 − zn−1) = n.
12.2. The roots of the polynomial q(x) are the numbers cos α ± i sin α, so it
is enough to check that these are also roots of the polynomial pn(x).
Substituting these values for x in that polynomial and appealing to de
Moivre’s theorem, we obtain
(cos nα ± i sin nα) sin α − (cos α ± i sin α) sin nα + sin(n − 1)α
= cos nα sin α − cos α sin nα + sin(n − 1)α
= − sin(n − 1)α + sin(n − 1)α = 0,
as required.
12.3. a) Let ε be a cube root of unity other than 1. We look for all n
for which ε is a root of the polynomial (t + 1)n − tn − 1. Since
ε2 + ε + 1 = 0, we have ε + 1 = −ε2, so that
(ε + 1)n − εn − 1 = (−1)nε2n − εn − 1.
Solutions of the supplementary problems 257
We now examine the six cases corresponding to the six possible
remainders obtained on dividing n by 6:
If n = 6k then (−1)nε2n − εn − 1 = 1 − 1 − 1 �= 0.
If n = 6k + 1 then (−1)nε2n − εn − 1 = −ε2 − ε − 1 = 0.
If n = 6k + 2 then (−1)nε2n − εn − 1 = ε − ε2 − 1 �= 0.
If n = 6k + 3 then (−1)nε2n − εn − 1 = −1 − 1 − 1 �= 0.
If n = 6k + 4 then (−1)nε2n − εn − 1 = ε2 − ε − 1 �= 0.
If n = 6k + 5 then (−1)nε2n − εn − 1 = −ε − ε2 − 1 = 0.
We conclude that the number ε is a root of the polynomial
(t + 1)n − tn − 1 if and only if n = 6k ± 1. For these n this poly-
nomial is divisible by (t − ε1)(t − ε2) = t2 + t + 1, whence
(x
y+ 1
)n
−xn
yn− 1 = q
(x
y
)(x2
y2+
x
y+ 1
),
where q(t) is a polynomial of degree n − 3. Multiplying this equa-
tion throughout by yn, we see that the given polynomial is divisible
by x2 + xy + y2 if and only if n = 6k ± 1.
b) The solution of Part a) shows us that the given polynomial is divis-ible by x2 + xy + y2. It is obvious that it is also divisible by x + y.Using this information, we factor the given polynomial by meansof the following algebraic manipulations:
(x + y)7 − x7 − y7 = 7x6y+21x5y2+35x4y3+35x3y4+21x2y5+7xy6
= 7xy(x5 + 3x4y + 5x3y2 + 5x2y3 + 3xy4 + y5)
= 7xy(x5 + x4y + 2x4y + 2x3y2 + 3x3y2
+ 3x2y3 + 2x2y3 + 2xy4 + xy4 + y5)
= 7xy(x + y)(x4 + 2x3y + 3x2y2 + 2xy3 + y4)
= 7xy(x+y)(x2(x2+xy+y2)+xy(x2+xy + y2)
+ y2(x2 + xy + y2))
= 7xy(x + y)(x2 + xy + y2)2.
A different solution. Consider the polynomial p(t) = (t + 1)7 −t7 − 1. Among its roots are, obviously, 0 and −1, and also, as
we know from Part a), ε1 and ε2 where ε2i + εi + 1 = 0. Since
p′(t) = 7(t + 1)6 − 7t6, we have
p′(εi) = 7(εi + 1)6 − 7ε6i = (−ε2
i )6 − 1 = 0,
258 Solutions of the supplementary problems
so that each of the numbers ε1 and ε2 is actually a multiple root
of the polynomial p(t). Hence p(t) is divisible by the polynomial
t(t + 1)(t2 + t + 1)2. However, since p(t) has degree 6, we must in
fact have
p(t) = at(t + 1)(t2 + t + 1)2.
Putting t = 1 yields 126 = 18a, whence a = 7. Setting t = xy
, we
get the equation
(x
y+ 1
)7
−x7
y7− 1 = 7
x
y
(x
y+ 1
)(x2
y2+
x
y+ 1
)2
,
and multiplying throughout by y7, we get the desired factorization.
Theme 13. Complex numbers and geometry
13.1. a) The solution of this problem derives directly from the result of
Problem 12.1. Write εk = cos 2πk5
+ i sin 2πk5
, k = 1, 2, 3, 4; these are
just the 5th roots of unity other than 1. We may take the corresponding
points of the complex plane to be vertices of the pentagon in question,
with the vertex A1 lying on the real axis (that is, corresponding to 1).
Then
|A1A2|2|A1A3|2 = |1 − ε1|2|1 − ε2|2
= (1 − ε1)(1 − ε1)(1 − ε2)(1 − ε2)
= (1 − ε1)(1 − ε4)(1 − ε2)(1 − ε3) = 5
by the result of Problem 12.1.
b) Once Part a) has been solved, it is clear how to generalize
it. Consider a regular (2n + 1)-gon inscribed in the unit circle,
with vertices A1, . . . , A2n+1 at the (2n + 1)th roots of unity. Then
|A1A2| |A1A3| . . . |A1An+1| =√
2n + 1 .
13.2. Choose a coordinate system with origin at the center of the heptagon
and x-axis an arbitrarily chosen straight line through that center. For
convenience we may assume that the radius of the circumcircle of the
heptagon is 1. The coordinates of the kth vertex Ak of the heptagon may
then be taken to be(cos
(α + 2πk
7
), sin
(α + 2πk
7
)), k = 0, 1, . . . , 6, for
some angle α. The sum of the squares of the distances of the vertices
Solutions of the supplementary problems 259
from the line—that is, from the x-axis—is then
6∑
k=0
sin2(α + 2πk
7
)= 7
2− 1
2
6∑
k=0
cos(2α + 4πk
7
).
We shall show that the sum of cosines in the right-hand side of this
equation is equal to zero, whence it follows that the sum of the squares
of the distances in question is independent of α,, and therefore of the
orientation of the straight line relative to the heptagon.
Write u = cos 2α + i sin 2α and v = cos 2π7
+ i sin 2π7
. Since v7 =1 it follows that u + uv + . . . + uv6 = u(v7−1)
v−1= 0. It now only
remains to observe that the real part of this sum is equal to the sum∑6k=0 cos
(2α + 4πk
7
).
13.3. This problem may be solved, of course, by means of analytic geometry
or vector algebra. It might also serve to illustrate the use of geometric
transformations. However, as we shall see, the simplest approach of
all is just to calculate with complex numbers.
Suppose the vertices of the square ABCD correspond to complex
numbers u, v, w and t , and those of the square A1B1C1D1 to complex
numbers u1, v1, w1 and t1. We may assume that the vertices of the
two squares are read off counterclockwise. Then the line segment
AD, for instance, is obtained from the segment AB by means of a
counterclockwise rotation of the latter through 90◦, whence i(v − u) =t − u. Similarly, we have i(v1 − u1) = t1 − u1. Let A2, B2, C2 and D2
denote the midpoints of the respective segments AA1, BB1, CC1 and
DD1. The complex numbers corresponding to these points are given
by
u2 =u + u1
2, v2 =
v + v1
2, w2 =
w + w1
2, t2 =
t + t1
2.
Since
i(v2 − u2) = i
(v − u
2+
v1 − u1
2
)=
t − u
2+
t1 − u1
2= t2 − u2,
we see that if we rotate the line segment A2B2 through 90◦ about its
endpoint A2 it moves into the position of A2D2. Hence the segments
A2B2 and A2D2 are equal in length and perpendicular. The perpendic-
ularity and equality in length of the other adjacent pairs of sides of the
quadrilateral A2B2C2D2 are established similarly.
13.4. Let the given parallelogram be ABCD, and consider the squares
erected on the sides AB, BC and AD (as in Figure 113). We shall
260 Solutions of the supplementary problems
prove that the line segments KL and KM (in the notation of Fig-
ure 113) are equal in length and perpendicular. This time we shall
identify planar vectors with complex numbers. Let u denote the com-
plex number corresponding to the vector AB and by v the complex
number corresponding to the vector AD. Since the products ±iu and
±iv determine vectors perpendicular to AB and AD and of the same
respective lengths, they correspond to sides of the squares erected on
AB and AD. Hence the vector AK is determined by the number u−iu2
A B
CD
K
M
Lu
vviv
-iu
-iv
Figure 113
and AM by v+iv2
, and therefore the vector KM by
z =v + iv
2−
u − iu
2=
1
2
(v − u + i(u + v)
).
One shows similarly that the vector KL is defined by the number
w =v − iv
2+
u + iu
2=
1
2
(u + v + i(u − v)
).
Then since
iw =1
2
(i(u + v) − (u − v)
)= z,
we infer that the vector KM can be obtained from the vector KL by
rotating the latter through 90◦, as we wished to prove.
Solutions of the supplementary problems 261
13.5. We have
n∑
k=1
|z − zk|2 =n∑
k=1
(z − zk)(z − zk)
= n|z|2 − z
n∑
k=1
zk − z
n∑
k=1
zk +n∑
k=1
|zk|2 = n(|z|2 + 1
).
13.6. a) The given equality 1a
+ 1b
+ 1c
= 0 implies 1a
+ 1
b+ 1
c= 0, or
a|a|2 + b
|b|2 + c|c|2 = 0. Multiplying the later equality by a suitable
positive real number, we get an equation of the form αa + βb +γ c = 0 with α, β, γ > 0 and α + β + γ = 1. Interpreted geomet-
rically, this means that the origin of coordinates lies in the triangle
with the points a, b, c as vertices.
Here is the proof of this fact. Let αa + βb + γ c = 0 where
α, β, γ > 0 and α + β + γ = 1. We rewrite the equation αa +βb + γ c = 0 in the form
(1 − γ )
(α
1 − γa +
β
1 − γb
)+ γ c = 0.
Since α1−γ
+ β
1−γ= α+β
1−γ= 1, we infer that d lies on the line seg-
ment with endpoints a and b (Figure 114).
c
b
a
d
O
Figure 114
Then since (1 − γ )d + γ c = 0, the origin lies on the line segment
with endpoints d and c, and therefore in the triangle with vertices
a, b and c. Write d = α1−γ
a + β
1−γb.
b) If z0 is a solution of the given equation, then, writing ai = ci − z0,
we have 1a1
+ 1a2
+ 1a3
= 0. By the result of Part a) above, the origin
lies in the triangle with vertices a1, a2, a3. Hence z0 lies in the
triangle with vertices c1, c2, c3.
262 Solutions of the supplementary problems
c) Let p(x) = (x − c1)(x − c2)(x − c3) where |ci | ≤ 1. If p(x) has no
repeated root then the equation p′(x) = 0 has the same solutions as
p′(x)
p(x)=
1
x − c1
+1
x − c2
+1
x − c3
= 0.
By Part b) above this implies that the roots all lie in the triangle
with vertices at points in the unit circle, so that they must lie in that
circle. What if p(x) has a repeated root?
13.7. Let ε be a complex number satisfying ε2 + ε + 1 = 0. We choose our
coordinate system so that the center of the given equilateral triangle
ABC is at the origin. If the vertex A then corresponds to the complex
number u, the other two vertices will correspond to the numbers εu
and ε2u. Thus the problem comes down to showing that the inequality
|z − u| ≤ |z − εu| + |z − ε2u| holds for every complex number z. And
in fact we have
|z − u| = |(ε + ε2)(z − u)| = |ε2z − εu + εz − ε2u|
≤ |ε2z − εu| + |εz − ε2u| = |z − ε2u| + |z − εu|.
Theme 14. Areas of triangles and quadrilaterals
14.1. a) Since the diagonal AC divides our quadrilateral ABCD into tri-
angles of equal area, their heights h1 and h2 as measured from this
diagonal as base (see Figure 115a) must be equal. It follows that
the point P of intersection of the diagonals must be the midpoint of
the diagonal BD. For similar reasons, the point P must also be the
midpoint of the diagonal AC. Since the point of intersection of the
diagonals is the midpoint of both, it follows that the quadrilateral is a
parallelogram.
A
B
C
D
Ph1
h2
A B
CD
L
K
h1 h2
(a) (b)
Figure 115
Solutions of the supplementary problems 263
b) By assumption, the quadrilaterals ADKL and KCBL are of equal
area (see Figure 115b). Since, obviously, SDKL = SKCL (S denoting,
as before, area), it follows that SADL = SLCB . Since the bases of the
latter two triangles are equal in length, their heights h1 and h2 must also
be equal, so that the line segments AB and CD are parallel. Similarly,
we have AD ‖ BC. Hence the given quadrilateral is a parallelogram.
14.2. Denote by a, b and c the lengths of the sides of the original triangle,
and by α, β and γ the respective angles opposite those sides. Let
A1, B1 and C1 be the centers of the equilateral triangles erected on
the sides BC, AC and AB respectively, of the original triangle so
that, for instance, the points A and A1 lie on opposite sides of the
line segment BC. These are the vertices of the “external” Napoleonic
triangle (Figure 116). On the other hand, we have the points A2, B2
A
B
C
B1
C1
A1
A2
B2C2
d1
d2
α
Figure 116
and C2, also centers of equilateral triangles erected on the sides BC,
AC and AB respectively, but so that, for instance, the points A and A2
lie on the same side of the line segment BC; these are the vertices of
the “internal” Napoleonic triangle.
In Theme 13 it was proved that the triangle A1B1C1 is equilateral. It
can be proved similarly that the triangle A2B2C2 is also equilateral,
and this we shall assume done. Let d1 and d2 be the lengths of a side of
the triangles A1B1C1 and A2B2C2 respectively. We get an expression
for the length d1 by considering the triangle AB1C1. Since the angle
between the sides AB1 and AC1 is equal to α + π3
, AB1 = c√3, and
AC1 = b√3
, we have
d21 =
b2
3+
c2
3−
2bc
3cos
(α +
π
3
).
264 Solutions of the supplementary problems
Similarly, we have
d22 =
b2
3+
c2
3−
2bc
3cos
(α −
π
3
).
Hence
SA1B1C1− SA2B2C2
=√
3
4(d2
1 − d22 )
=bc
2√
3
(cos
(α −
π
3
)− cos
(α +
π
3
))
=bc√
3sin α sin
π
3
=bc
2sin α = SABC .
14.3. The assumption is that AB = BC = CD = 2. For each possible fixed
disposition of B, C and D, the triangle ABD has largest area when
its sides AB and BD are perpendicular to each other (Figure 117).
Similarly, for each given (possible) disposition of the points A, B
A D
CB
P
Figure 117
and C, the area of the triangle ACD will be largest when AC ⊥ CD.
Hence the quadrilateral ABCD will have greatest area when the points
B and C lie on the circle with diameter AD. The center P of this circle
is the midpoint of the line segment AD. For this quadrilateral we
have PA = PB = PC = PD and, since AB = BC = CD = 2, the
triangles APB, PBC and PCD are congruent. Hence the angle at the
vertex P of each of these isosceles triangles is equal to 60◦, so that in
fact they are equilateral. Thus the greatest area of such a quadrilateral
is 3√
3.
Solutions of the supplementary problems 265
Theme 15. Constructions in solid geometry
15.1. By means of a sufficient number of diagonals, subdivide each face of
the given polyhedron into triangles. Then for each face the outwards-
directed vector n perpendicular to that face and of length equal to its
area, will be the sum of vectors with the same direction as n and with
lengths equal to the areas of the triangles of the subdivision of that
face. It follows that we may assume without loss of generality that
all of the faces of the polyhedron are triangular. This assumed, we
choose an arbitrary point inside the polyhedron and join it by means
of straight line segments to the polyhedron’s vertices. Each face will
then form the base of a tetrahedron with apex at the chosen interior
point of the polyhedron. The polyhedron is thus subdivided into N ,
say, tetrahedrons. Let ai , bi , ci and di be vectors perpendicular to
the faces of the ith such tetrahedron (i = 1, . . . , N), of lengths equal
to the areas of the corresponding faces, and directed outwards from
the tetrahedron, and furthermore with di perpendicular to the base of
the ith tetrahedron. Thus di is perpendicular to the ith face of the
given polyhedron, and∑n
i=1 di is the sum of vectors perpendicular
to the faces of the polyhedron that we wish to show is zero. Since
ai + bi + ci + di = 0 (already proven), it follows that
0 =N∑
i=1
(ai + bi + ci + di) =N∑
i=1
di +N∑
i=1
(ai + bi + ci).
Hence the assertion we wish to prove will follow from the equation∑Ni=1(ai + bi + ci) = 0, which we shall now prove. Each lateral face
(that is, other than the base) of a tetrahedron of the subdivision of the
polyhedron is a face of exactly two such tetrahedrons. Hence the set
{ai, bi, ci} of all vectors corresponding to these faces consists of pairs
of oppositely directed vectors of equal length, which cancel in the sum.
15.2. The idea of the solution consists in examining the possible plane
projections of a regular tetrahedron. If the projection is a triangle then it
coincides with the projection of a face of the tetrahedron, so the largest
area of such a projection is the area of a face, namely a2√
34
where a is the
length of an edge of our tetrahedron. If the projection is a quadrilateral,
then its area S is 12d1d2 sin α, where d1 and d2 are the lengths of its
diagonals and α is the angle between them. Here the diagonals are the
projections of two opposite edges of the tetrahedron, whence it is clear
that S ≤ a2
2. It is also clear that this bound is attained precisely when
266 Solutions of the supplementary problems
the plane of projection is parallel to two of the tetrahedron’s skew
(or, equivalently, opposite) edges. Since√
34
< 12
we conclude that the
greatest area a projection can have is a2
2.
15.3. There are two different ways for the four edges of length 1 to be
arranged in the tetrahedron. If three of these edges are the sides of a
face, then that face will be an equilateral triangle, and so of area√
34
.
Since the height of the tetrahedron measured with this face as base is
at most 1, the maximal volume of such a tetrahedron is√
312
.
The other possibility is that the four edges of unit length form a closed,
connected, four-segment, broken line (the 1-skeleton of the tetrahedron
with one pair of opposite edges removed). Consider the parallelepiped
having the edges of the tetrahedron as diagonals of its faces. Those
four faces of the parallelepiped having an edge of the aforementioned
broken line segment as a diagonal must be rectangles, whence it fol-
lows, in particular, that there is an edge of the parallelepiped—namely,
a common edge of two such (adjacent) rectangular faces—that is an
altitude. Let x be the length of such an edge of the parallelepiped.
The two other faces of the parallelepiped must be rhombi with side of
length√
1 − x2 . The area of these faces will be greatest when they
are actually squares, of area 1 − x2. Since the volume v of the tetra-
hedron is a third of that of this rectangular parallelepiped, we have
v = 13x(1 − x2). It remains to find the largest value of this function
on the interval [0, 1]. Differentiating, we find that this value is attained
at x = 1√3
, whence we infer that the greatest volume such a tetrahe-
dron can have is 2
9√
3. It now only remains to observe that
√3
12> 2
9√
3,
whence we conclude that the tetrahedron of the required sort with
greatest volume is that with three edges forming an equilateral triangle
of side 1 and with another edge of length 1 perpendicular to this face.
15.4. Let n4 ⊥ (ABC) with |n4 | = SABC , n1 ⊥ (ABD) with |n1 | = SABD ,
n2 ⊥ (BCD) with |n2 | = SBCD , n3 ⊥ (ACD) with |n3 | = SACD . Let
αAD , αBD and αCD be the sizes of the dihedral angles at the indicated
edges. Observe that then the angle between the vectors n1 and n2, for
instance, is π − αAB . Hence n1 · n2 = −SABDSBCD cos αBD . Since
n24 = (n1 + n2 + n3)2 = n2
1 + n22 + n2
3 + 2n1 ·n2 + 2n2 ·n3 + 2n1 ·n3,
it follows that
S2ABC = S2
ABD + S2BCD + S2
ACD − 2SABDSBCD cos αBD
− 2SBCDSACD cos αCD − 2SABDSACD cos αAD.
Solutions of the supplementary problems 267
Thus the statement of Problem 6 may be considered as a sort of “three-
dimensional Pythagoras’ theorem”, and the above formula the analo-
gous “three-dimensional law of cosines”.
15.5. a) Consider a tetrahedron ABCD with the angles of the faces around
its apex D all right angles. For the sake of brevity, we write a = AD,
b = BD and c = CD. We look for solutions for a, b and c of the
system of equations
⎧⎪⎪⎨⎪⎪⎩
ab = 4,
bc = 6,
ac = 12,
since with such values of a, b and c we shall have SABD = 2,
SBCD = 3, and SACD = 6. Solving the above system we first see that
(abc)2 = 288 whence abc = 12√
2, and thence a = 2√
2, b =√
2
and c = 3√
2 . It remains to observe that then, by the formula of
Problem 6, S2ABC = 4 + 9 + 36 = 49, whence SABC = 7.
b) Consider the right triangle ABC with sides of lengths AC = 3,
BC = 4 and AB = 5. Its area is 6, and the radius of its incircle is
1. Let O be the center of the incircle. Since SACO = 32
, SBCO = 2
and SABO = 52
, if the side faces of the tetrahedron ABCD are
inclined to the base at an angle of 60◦, then their areas will be 3, 4
and 5.
Theme 16. Inequalities
16.1. a) The least value of the given function is 3 since
x +4
x2=
x
2+
x
2+
4
x2≥ 3
√x
2·x
2·
4
x2= 3,
with equality at x = 2.
b) The least value of the given function is 3 since
x2 +2
x= x2 +
1
x+
1
x≥ 3
√x2 ·
1
x·
1
x= 3,
with equality at x = 1. Note that the substitution t = 2x
transforms
this problem into the preceding one.
268 Solutions of the supplementary problems
16.2. Suppose (x, y, z) is any triple satisfying x2 + 2y2 + 3z2 = 6. Then by
the Cauchy-Schwarz inequality
|x + 2y + 3z| = |1 · x +√
2 ·√
2 y +√
3 ·√
3 y|
≤√
1 + 2 + 3√
x2 + 2y2 + 3z2 = 6.
Hence the given system has solutions only if |a| ≤ 6. Consider first the
case a = 6. Then for every solution of the system, the above inequality
is an equality, which occurs in the Cauchy-Schwarz inequality if and
only if the two n-tuples involved (here triples) are proportional. Hence
the triple (x,√
2 y,√
3 z) is proportional to the triple (1,√
2 ,√
3 ),
that is, x = t , y = t and z = t . The first equation x2 + 2y2 + 3z2 = 6
then yields t2 = 1, whence, in the present case, t = 1, and we infer
that in the case a = 6 the only solution is (x, y, z) = (1, 1, 1). In the
case a = −6 the only solution is (−1,−1,−1). For each a < 6 there
are in fact infinitely many solutions. This is easiest seen geometrically.
The first equation of the given system has graph an ellipsoid centered
at the origin, while the second is the equation of a plane parametrized
by a. The two planes corresponding to a = ±6 are tangent to the
ellipsoid and sandwich it between them. Intermediate planes—that is,
with |a| < 6—meet the ellipsoid in elliptical cross-sections.
16.3. a) The given inequality is valid since
2(ak+n+bk+n
)−(ak + bk
) (an + bn
)= ak+n−akbn + bk+n−anbk
= an(ak−bk
)−bn
(ak−bk
)
=(ak−bk
) (an−bn
)≥ 0,
regardless of whether a ≥ b or a ≤ b.
b) Since k + n = ℓ + m, k ≤ n and ℓ ≤ m, we have m − k = n − ℓ >
0. Write p = m − k. Then
(ak + bk
) (an + bn
)−
(aℓ + bℓ
) (am + bm
)
=(akbn − ambℓ
)−
(aℓbm − anbk
)
= akbℓ(bn−ℓ − am−k
)− aℓbk
(bm−k − an−ℓ
)
=(bp − ap
) (akbℓ − aℓbk
)
= akbk(bp − ap
) (bℓ−k − aℓ−k
)≥ 0
Solutions of the supplementary problems 269
regardless of whether a ≥ b or a ≤ b, in view of the fact that p > 0
and ℓ − k > 0.
16.4. a) Of course, this is immediate from the inequality between the arith-
metic and geometric means. However, the latter inequality follows
from this one, and in fact this represents one of the standard ways
of establishing it. For this reason we prove it instead by induc-
tion on the number n of factors. Thus suppose inductively that
x1x2 · · · xn = 1 implies x1 + x2 + · · · + xn > n provided these n
(positive) numbers are not all equal. Consider n + 1 positive num-
bers x1, . . . , xn+1 such that x1x2 · · · xnxn+1 = 1. If they are all equal
then they are all 1, and their sum is n + 1. Suppose on the other
hand that some are less than 1, some greater. Without loss of
generality we may assume (by re-indexing the numbers if nec-
essary) that xn < 1 < xn+1. Then (xn+1 − 1)(1 − xn) > 0, whence
xn + xn+1 > xnxn+1 + 1. Hence
x1 + x2 +· · ·+ xn + xn+1 > x1 +· · ·+ xn−1 + xnxn+1 + 1 ≥ n + 1
by the inductive assumption, since x1x2 · · · xn−1(xnxn+1) = 1.
b) The given inequality is a direct consequence of the result of Part a)
since the product of the terms in the left-hand sum is equal to 1.
16.5. Denote the lengths of the sides of the triangle by a, b and c, and its
area by S. Since
ha =2S
a, hb =
2S
b, hc =
2S
cand r =
2S
a + b + c,
the inequality ha + hb + hc ≥ 9r may be expressed in the form 1a
+1b
+ 1c
≥ 9a+b+c
or, equivalently, as
(a + b + c)
(1
a+
1
b+
1
c
)≥ 9.
We shall now give four proofs of this inequality. Once rewritten in the
form
31a
+ 1b
+ 1c
≤a + b + c
3,
we see that it is essentially just the inequality between the harmonic
and arithmetic means of three positive numbers. The second proof
uses the inequality between the arithmetic and geometric means of
270 Solutions of the supplementary problems
three numbers:
(a + b + c)
(1
a+
1
b+
1
c
)≥ 3
3√
abc · 31
3√
abc= 9.
For the third, we have
(a + b + c)
(1
a+
1
b+
1
c
)= 3 +
a
b+
b
a+
b
c+
c
b+
a
c+
c
a
≥ 3 + 2 + 2 + 2 = 9.
The final proof is via the Cauchy-Schwarz inequality, and this one is,
in the author’s opinion, the most natural:
(a + b + c)
(1
a+
1
b+
1
c
)
≥(√
a ·1
√a
+√
b ·1
√b
+√
c ·1
√c
)2
= 9.
16.6. We take the equation of the plane to be ax + by + cz = 1. Setting
y = z = 0, we get x = 1a
, so the point of intersection A of the plane
with the x-axis has coordinates(
1a, 0, 0
). Similarly, the plane meets the
other two coordinate axes in the points B(0, 1
b, 0
)and C
(0, 0, 1
c
). The
volume V of the tetrahedron ABCD is 16abc
. Since the point M(4, 2, 1)
lies on the plane, we have 4a + 2b + c = 1. By the inequality between
the arithmetic and geometric means of three numbers, we have
1 = 4a + 2b + c ≥ 33√
8abc = 63√
abc,
whence 13√
abc≥ 6. Hence 1
abc≥ 63 and then V ≥ 62 = 36. Equality
holds when 4a = 2b = c = 13
, that is, when a = 112
, b = 16
and c = 13
.
This answer has an interesting geometric interpretation. Since the ver-
tices of the face ABC of the tetrahedron are the points A(12, 0.0),
B(0, 6, 0) and C(0, 0, 3), the point M is the point of intersection of the
medians of that face, that is, the centroid or center of mass.
16.7. a) Squaring both sides and cancelling like terms, we get the inequality
x1y1 + x2y2 + · · · + xnyn
≤√
x21 + x2
2 + · · · + x2n
√y2
1 + y22 + · · · + y2
n ,
which is a consequence of the Cauchy-Schwarz inequality. It is
worth remarking that in terms of vectors x(x1, x2, . . . , xn) and
y(y1, y2, . . . , yn) in the (Euclidean) space Rn the given inequality
Solutions of the supplementary problems 271
may be rewritten in the form |x + y| ≤ |x| + | y|, standing revealed
as the familiar triangle inequality.
b) Consider plane vectors ai(xi, yi), i = 1, 2, . . . .k. From Part a), just
solved, we know that |a + b| ≤ |a| + |b|. Hence
|a1 + a2 + · · · + ak| ≤ |a1 + a2 + · · · + ak−1| + |ak|
≤ |a1 + a2 + · · · + ak−2| + |ak−1| + |ak|
≤ · · · ≤ |a1| + |a2| + · · · + |ak|.
c) The general inequality embracing those of both Parts a) and b) is
|a1 + a2 + · · · + ak| ≤ |a1| + |a2| + · · · + |ak|,
true for any vectors in Euclidean Rn.
Theme 17. Diophantine equations
17.1. a) Rewriting the given equation as (x − y)(x + y) = 2012 and setting
a = x − y and b = x + y, we get the equation ab = 2012. hence
at least one of the integers a, b must be even. However, the system
{x − y = a,
x + y = b
has integer solutions only if a and b have the same parity. Hence they
must both be even. Writing a = 2k and b = 2n, we obtain the equa-
tion kn = 503. Then since the number 503 is prime, we conclude
that the integer solutions of the given equation are just (1, 503),
(503, 1), (−1,−503) and (−503,−1). Thus the given equation has
exactly four solutions in integers.
b) If ab = 2014 then one of a and b must be even and the other odd.
But then the system
{x − y = a,
x + y = b
has no solutions in integers. Hence the given equation has no integer
solutions.
c) In the notation of Part a), we get kn = 504 = 23 · 32 · 7. The number
504 therefore has (3 + 1)(2 + 1)(1 + 1) = 24 natural divisors and
272 Solutions of the supplementary problems
hence 48 integer divisors. Hence the given equation has exactly 48
integer solutions.
17.2. a) Write the integer x in the form x = 2011k + d, where d may be
any of 0, 1, . . . 2010. Since[
x2010
]=
[x
2011
]+ 1 = k + 1, we must
have k + 1 ≤ x2010
< 2011, whence
2010k + 2010 ≤ 2011k + d < 2010k + 4020,
and therefore 2010 ≤ k + d < 4020, or 2010 ≤ k + d ≤ 4019.
Hence for each of the 2011 possible values of d there are 2010
values of the number k for which the number x = 2011k + d is a
solution of the given equation. Hence that equation has altogether
2010 · 2011 solutions.
b) The largest value of k is k = 4019, with d = 0. Hence the largest
solution of the given equation is the number x = 4019 · 2011 =8 082 209.
17.3. Two easy solutions of the given equation are the pairs (0, 0) and (2, 2).
Thus in searching for further solutions we may suppose y ≥ 3. Since
y3 + 1 = (y + 1)(y2 − y + 1) we must have y + 1 = 3a and y2 − y +1 = 3b where 2 ≤ a < b. Since 32a − 3a+1 + 3 = 3b, it follows that
3 = 3b + 3a+1 − 32a , which is impossible since the right-hand side is
divisible by 9 and the left-hand side is not so divisible.
17.4. Easy integer solutions of the equation 3x + 1 = 2y are the pairs (0, 1)
and (1, 2). Since the remainders on dividing a power of 3 by 8 are just
1 or 3, no number of the form 3x + 1 is divisible by 8, whence y ≤ 2.
Hence there are no further integer solutions of the given equation.
17.5. One should not be too surprised at seeing such a problem appear in
connection with the theme “Diophantine equations”. As you will now
see, the trigonometry is a red herring. Since the values of the sine and
cosine functions lie in the interval [−1, 1], the given equation holds if
and only if{
sin 1992π2
x= 1,
cos x = 1or
{sin 1992π2
x= −1,
cos x = −1.
Consider the second case: sin 1992π2
x= −1 implies 1992π2
x= −π
2+
2πk, k ∈ Z, and cos x = −1 implies x = π + 2πn, n ∈ Z. Hence
1992π2 =π2
2(2n + 1)(4k − 1), or 3984 = (2n + 1)(4k − 1),
which is impossible since 3984 is even.
Solutions of the supplementary problems 273
In the first case, one obtains similarly the equation n(4k + 1) = 1992
where n and k are integers. Thus 4k + 1 is a divisor of 1992 with
remainder 1 on division by 4. Since 1992 = 8 · 3 · 83, one calculates
that the only such divisors of 1992 are 1, 249, −3 and −83. The cor-
responding values of n are then n = 1992, 8,−664,−24 respectively.
Hence x = 3984π, 16π,−1328π,−48π .
17.6. Suppose the number m has (nonzero) remainder d on being divided by
17. From the table referred to in Problem 9, we see that whatever the
value of d there is an n for which the remainder on dividing 3n by 17
is 17 − d, so that 3n + m is divisible by 17.
Theme 18. Combinatorial tales
18.1. Of course, there are just two “tetrahedral dice”—a “right-handed” one
and a “left-handed” one, so to speak. To see this, place the tetrahedron
on the table with the face having four pips against the table top, and
rotate it about its vertical axis until the face with three pips is facing
you. The remaining faces have either one or two pips, and these can
be assigned in two ways, namely, with the face having one pip to the
right or to the left.
18.2. The following table, represents a chessboard with each white square
inscribed with the number of shortest paths by which a bishop can
reach that square starting from any of the four white squares of the first
row. These entries should be calculated starting from the first row and
proceeding upwards.
8 35 89 103 69
7 35 54 49 20
6 10 25 29 20
5 10 15 14 6
4 3 7 8 6
3 3 4 4 2
2 1 2 2 2
1 1 1 1 1
a b c d e f g h
Thus in each white square of the first row (squares b1, d1, f1 and h1)
we have, appropriately, the number 1. There is only one shortest way
of getting to the square a2, namely directly from b1, so that square
also contains the number 1. However, there are two shortest ways of
274 Solutions of the supplementary problems
getting to the square c2, namely directly either from square b1 or
d1. It follows that this table closely resembles Pascal’s triangle, the
difference being due to the fact that the white squares of the extreme
columns a and h have only one lower adjacent white square. Thus
the number of shortest paths to square a8, for example is equal to the
number of such paths to the square b7. Once the table is complete,
it only remains to total the numbers in the top row, yielding 296
paths.
18.3. We are interested in tickets with just three of the six winning numbers
marked. These three numbers may be any of the six winning numbers,
so the number of possibilities for them is(
6
3
)= 20. The three remaining
numbers must come from the 49 − 6 = 43 non-winning numbers, so
can be chosen in(
43
3
)= 12341 ways. Hence the number of tickets with
exactly three winning numbers marked is 20 · 12341 = 246820.
18.4. Suppose x1, x2, . . . , xk are non-negative integers constituting a solu-
tion of the equation x1 + x2 + · · · + xk = n. The numbers yi = xi + 1
will then be natural. The latter numbers constitute a solution of
the equation (y1 − 1) + (y2 − 1) + · · · + (yk − 1) = n, that is, of the
equation y1 + y2 + . . . + yk = n + k. Thus in view of the formula for
the number of solutions of the given equation in natural numbers (see
Problem 3), the number of solutions in non-negative integers is(n+k−1
k−1
).
18.5. In the partial solution of Problem 10 in the main text the case where
three edges of the tetrahedron are of length 20 inches and three of
length 33 inches was completely settled: if edges of the same length
are edges of a single face, then such a tetrahedron exists, but there is no
such tetrahedron in which three edges of the same length form an open,
continuous (triple-segmented) broken line—the only other possibility.
We now consider the remaining cases, in order of increasing com-
plexity. Of course, from six edges of either length one can construct a
(regular) tetrahedron. And a tetrahedron can have five edges of length
33 inches and just one of length 20 inches. However, it is not so easy
to see if there is one with the lengths the other way around: five edges
of length 20 inches and one of length 33 inches. To prove that this is
possible, we imagine two equilateral triangles of side 20 inches with
an edge in common, situated in the plane. The distance between their
opposing (that is, unattached) vertices is then 20√
3, which, as was
noted in the partial solution of Problem 10, exceeds 33. These two
triangles can, therefore, be bent up about their common edge until the
distance between their free vertices is 33 inches.
Solutions of the supplementary problems 275
It is easy to show similarly that there is a tetrahedron with two
opposite edges of length 20 inches and the other four of length 33
inches. But is there a tetrahedron with two opposite edges of length 33
inches and the rest of length 20 inches? Imagine laid out in the plane
two isosceles triangles having a common base of length 33 inches
and side edges of length 20 inches. The tetrahedron in question will
exist if and only if the distance between the opposing vertices of the
triangles exceeds 33 inches. We carry out the calculation in general
terms. As before, let a and b be positive numbers with a > b, and
let a now assume the role of the number 33 and b that of 20 in the
preceding picture. The tetrahedron in question will then exist precisely
if 2
√b2 − a2
4=
√4b2 − a2 > a. On solving this equation, we obtain
ab
<√
2 . In our case, we have ab
= 3320
> 32
>√
2, so there is no such
tetrahedron.
There are two more cases. Does there exist a tetrahedron with two
adjacent edges of length 20 and the rest of length 33? Once again we
carry out the argument in general terms. Thus, imagine laid out in the
plane an equilateral triangle of side a with an edge in common with
an isosceles triangle (lying outside it) with its equal sides of length
b, where, as before, b < a. A tetrahedron with two adjacent edges of
length b and the rest of length a will exist if and only if the distance
between opposing vertices of this figure is greater than a, that is, if the
inequality
a√
3
2+
√b2 −
a2
4> a
holds. Solving, we obtain the condition ab
< 1+√
3√2
≈ 1.93. In our con-
crete case, we have ab
= 3320
, so such a tetrahedron does exist.
We turn finally to the case where there are two adjacent edges of
the greater length and the rest of the shorter length. Thus imagine laid
out in the plane an equilateral triangle with side of length b, having an
edge in common with an isosceles triangle with equal sides of length
a, and lying inside that triangle. A tetrahedron with two adjacent sides
of length a and the rest of length b will exist if and only if the distance
between the free vertices of these two triangles is less than b, that is,
if the inequality
√a2 −
b2
4−
b√
3
2< b,
276 Solutions of the supplementary problems
holds. Solving, we obtain the condition ab
< 1+√
3√2
, as in the preceding
case. Hence such a tetrahedron exists.
Thus the final answer to Problem 10 is: there are nine such distinct
tetrahedrons. In conclusion, we remark that it follows from our inves-
tigation of this problem, that the number of distinct tetrahedrons with
edges of lengths a or b depends on which of the indicated intervals
the ratio ab
falls into (Figure 118). The greater this ratio the fewer
1 2 3 2
1+ 5
2
1+ 3
2
Figure 118
tetrahedrons there are.
Theme 19. Integrals
19.1. a) The number ln n is equal to the area under the graph of the
function y = 1x
and above the interval [1, n]:∫ n
11x
dx = ln x∣∣n1
=ln n − ln 1 = ln n. We estimate this area using “lower” rectangles
and then “upper” rectangles, as shown in Figure 119.
1 2 3 4 5
0.2
0.4
0.6
0.8
1.0
1 2 3 4 5
0.2
0.4
0.6
0.8
1.0
(a) (b)
Figure 119
Consider the rectangles with bases the intervals [k − 1, k], k =2, 3, . . . , n, and heights 1
k(the case n = 5 is shown in Figure 119a).
Since these rectangles all lie below the graph of the function in
question, the sum of their areas, namely∑n
k=21k, will be less than
the area under the graph, that is, less than ln n. To get the upper
estimate for ln n, one takes the rectangles on the intervals [k, k + 1],
k = 1, 2, . . . , n − 1, and heights 1k. Their union contains the area
Solutions of the supplementary problems 277
under the graph above the interval [1, n] (see Figure 119b), so the
sum∑n−1
k=11k
is greater than ln n.
b) The proof is similar to that of Part a):
1√
n+
1√
n + 1+ · · · +
1√
n2 − 1>
∫ n2
n
dx√
x= 2(n −
√n ).
19.2. The proof is similar to that of Part a) of the preceding problem:
1k + 2k + · · · + nk <
∫ n+1
0
xk dx =(n + 1)k+1
k + 1.
19.3. Under the given assumption,
∫ 1
0
(ax2 + bx + c) dx =a
3+
b
2+ c =
2a + 3b + 6c
6= 0,
so the given quadratic function can be neither everywhere positive nor
everywhere negative on the interval (0, 1), so must have a root in that
interval.
Although this solution may seem appealing, it does not really get
to the heart of the matter. Let’s try a different approach. Write p(x) =ax2 + bx + c and consider the sum
p(0) + 4p(
12
)+ p(1) = c + 4
(a
4+
b
2+ c
)+ a + b + c
= 2a + 3b + 6c = 0.
It follows that the numbers p(0), p(
12
)and p(1) cannot all have the
same sign, so the function p(x) must have opposite signs at certain
points of the interval [0, 1] and therefore vanish at some interior point
of that interval.
The connection between these two solutions is revealed in Simpson’s
formula—see Problem 19.7.
19.4. On changing a product of three cosines to a sum of cosines in the
standard manner, we obtain
cos k1x cos k2x cos k3x =1
4
(cos(k1 + k2 + k3)x + cos(k1 + k2 − k3)x
+ cos(k1 − k2 + k3)x + cos(k1 − k2 − k3)x).
In the first of the given integrals we have k1 = 1, k2 = 7 and k3 = 9.
Since these numbers are all odd, none of the corresponding numbers
278 Solutions of the supplementary problems
k1 ± k2 ± k3 can be zero, and the integral of each of the above sum-
mands will in this case be zero. Thus the answer is 0.
Since 2 + 7 − 9 = 0, the second of the given integrals will be equal
to∫ 2π
014dx = π
2.
19.5. We know that the function F (t) =∫ t
0f (x) dx is an antiderivative of
the function f (t), and that every antiderivative differs from this one by
a constant. The function F (t) is 2π -periodic if F (t + 2π ) = F (t), or
∫ t+2π
0
f (x) dx −∫ t
0
f (x) dx =∫ t+2π
t
f (x) dx =∫ 2π
0
f (x) dx = 0.
19.6. The ordinates (y-coordinates) of the points of intersection of the
straight line and parabola are given by yi = ax2i + bxi + c, i = 1, 2.
The area in question is equal to the difference between the area of the
trapezoid with bases y1 and y2, which is
y1 + y2
2(x2 − x1) =
a(x21 + x2
2 ) + b(x1 + x2) + 2c
2(x2 − x1) ,
and the area under the graph of the given quadratic function above the
interval [x1, x2], which is
a(x32 − x3
1 )
3+
b(x22 − x2
1 )
2+ c(x2 − x1).
Hence the desired area is
a(x22 + x2
1 )(x2 − x1)
2−
a(x32 − x3
1 )
3
=a(x2 − x1)
6(3x2
1 + 3x22 − 2x2
1 − 2x1x2 − 2x22 )
=a(x2 − x1)
6(x2
1 − 2x1x2 + x22 ) =
a(x2 − x1)3
6.
19.7. The inequality in question follows from Schwarz’s inequality, since
(∫ b
a
f (x) dx
)2
=(∫ b
a
1 · f (x) dx
)2
≤∫ b
a
1 dx ·∫ b
a
f 2(x) dx = (b − a)
∫ b
a
f 2(x) dx.
19.8. Consider first the special case a = 0 and b = 1. Since the equality in
question is supposed to hold for any polynomial of degree less than or
equal to 3, it should be valid in particular for the particular functions
f (x) = 1, f (x) = x and f (x) = x2. Replacing f in the given formula
Solutions of the supplementary problems 279
by each of these in turn, we obtain the system
⎧⎪⎪⎨⎪⎪⎩
1 = 16
(A + B + C),
12
= 16
(B2
+ C),
13
= 16
(B4
+ C),
or, after simplifying,
⎧⎪⎪⎨⎪⎪⎩
A + B + C = 6,
B + 2C = 6,
B + 4C = 8,
which has the unique solution A = C = 1, B = 4.
We have to show that these values of A, B, and C work for any
polynomial f (x) of degree at most 3 and any a and b, that is, that
∫ b
a
f (x) dx = b−a6
(f (a) + 4f
(a+b
2
)+ f (b)
).
is valid generally. To begin with, we verify this formula for the func-
tions f1(x) = 1, f2(x) = x, f3(x) = x2 and f4(x) = x3. The following
table gives the integrals of these functions:
n 1 2 3 4∫ b
afn(x) dx b − a b2−a2
2b3−a3
3b4−a4
4
We now calculate the right-hand side of the above equation for each
of the fi in turn. Thus for f1 we have
b−a6
(f1(a) + 4f1
(a+b
2
)+ f1(b)
)= b−a
6· 6 = b − a.
For f2 we have
b−a6
(f2(a) + 4f2
(a+b
2
)+ f2(b)
)= b−a
6·(a + 4 · a+b
2+ b
)
= b−a6
· 3(a + b) = b2−a2
2.
For f3 we have
b−a6
(f3(a) + 4f3
(a+b
2
)+ f3(b)
)= b−a
6·(a2 + 4 · (a+b)2
4+ b2
)
= b−a6
· 2(a2 + ab + b2) = b3−a3
3.
280 Solutions of the supplementary problems
And, finally,
b−a6
(f4(a) + 4f4
(a+b
2
)+ f4(b)
)
= b−a6
·(a3 + (a+b)3
2+ b3
)
= b−a6
· a+b2
· (2a2 − 2ab + 2b2 + a2 + 2ab + b2)
= b2−a2
12· 3(a2 + b2) = b4−a4
4.
It now only remains to observe that every polynomial f (x) of degree
3 or less can be written in the form c1f1(x) + c2f2(x) + c3f3(x) +c4f4(x). And then
∫ b
a
f (x) dx =∫ b
a
(4∑
i=1
cifi(x)
)dx
= ci
4∑
i=1
∫ b
a
fi(x) dx
= ci
4∑
i=1
b−a6
(fi(a) + 4fi
(a+b
2
)+ fi(b)
)
= b−a6
(f (a) + 4f
(a+b
2
)+ f (b)
).
19.9. Both the sphere and the truncated cone are solids of revolution. How-
ever, let’s instead integrate over areas of cross-sections. The area S(x)
of a cross-section of the sphere by a plane depends quadratically on
the distance x of the plane from the sphere’s center. Hence we may use
Simpson’s rule to calculate the integral∫ r
−rS(x) dx. In this case we
have a = −r , b = r , whence a+b2
= 0. Since planes at a distance r from
the center of the sphere are tangential to it, we have S(−r) = S(r) = 0.
Hence by Simpson’s rule 2r6
· 4πr2 = 43πr3.
Let r and R be the radii of the top and bottom of the truncated
cone, and h its height. The radius of a cross-section S(x) by a plane
parallel to the bases is a linear function of the distance x of the plane
from one or the other base. Hence the area of such a cross-section
is a quadratic function of that distance. The volume of the truncated
cone is∫ h
0S(x) dx. Since S(0) = πR2, S(h) = πr2, and the area of
the cross-section an equal distance from the bases is equal to π (R+r)2
4,
we conclude from Simpson’s rule that the desired volume is
h
6π(R2 + (R + r)2 + r2
)=
πh
3
(R2 + Rr + r2
).
Solutions of the supplementary problems 281
Theme 20. Functional equations ofelementary functions
20.1. Writing f (0) = b and g(x) = f (x) − f (0), we have
g
(x + y
2
)= f
(x + y
2
)− f (0) =
f (x) + f (y)
2− f (0)
=f (x) − f (0) + f (y) − f (0)
2
=g(x) + g(y)
2,
so g(x) satisfies the same relation but with g(0) = 0. Write a = g(1).
For all natural numbers n we have g(n) = g(n+1)+g(n−1)
2, whence
g(n + 1) = 2g(n) − g(n − 1). Setting n = 1 in this, we get g(2) = 2a.
Setting n = 2, we get g(3) = 2g(2) − g(1) = 4a − a = 3a. Arguing
inductively, we obtain more generally g(n) = an for all natural n.
Putting y = −x in the relation for g yields g(−x) = −g(x), and, argu-
ing inductively as before, we ultimately get g(k) = ak for all inte-
gers k. Putting y = 0 in the relation for g yields g(
x2
)= g(x)
2. Hence
g(
k2
)= a · k
2for all k ∈ Z, whence, by induction,
g
(k
2n
)= a ·
k
2n
for all integers k and non-negative integers n. Since every real number
x is the limit of a sequence (rn) of numbers of the form k2n (its binary
expansion), it follows that
g(x) = limn→∞
g(rn) = limn→∞
arn = ax,
whence g(x) = ax for all x ∈ R. Hence f (x) = ax + b, a “linear func-
tion in the high-school sense”.
20.2. In the solution of Problem 2 it was first shown that if the function
satisfying the conditions of the problem is not identically zero, then it
must be positive. It therefore makes sense to introduce the new function
g(x) = ln f (x), and then
g(x + y) = ln f (x + y) = ln(f (x)f (y)
)
= ln f (x) + ln f (y) = g(x) + g(y).
whence g(x) = αx and therefore f (x) = eαx = ax .
282 Solutions of the supplementary problems
20.3. Putting y = 0, we get f (0) = f (x) + f (0), so that f (x) = 0 for all
x ∈ R.
20.4. Write g(x) = f (ex). Then
g(x + y) = f (ex+y) = f (exey) = f (ex) + f (ey) = g(x) + g(y),
whence g(x) = αx. Thus f (ex) = αx, whence f (x) = α ln x, and, if
α �= 0, then f (x) = loga x for an appropriate number a.
20.5. Putting x = y = 0 in the given relation, we get f (0) = 2f (0)
1−f 2(0). Since
1 − f 2(0) �= 2, it follows that f (0) = 0. Putting y = −x then yields
f (−x) = −f (x). We cannot have |f (x)| = 1 for any x, since oth-
erwise f would be undefined at 2x. Hence by the assumption that
f is continuous and since f (0) = 0, the range of f (x) must be
contained in the interval (−1, 1). Suppose f (a) �= 0 for some num-
ber a. Then |f (2a)| = 2|f (a)|1−f 2(a)
≥ 2|f (a)|. Arguing inductively, we
get |f (2na)| ≥ 2n|f (a)| for all natural numbers n, contradicting the
boundedness of the function just established.
20.6. Setting k = 1, we obtain S1 · Sn = Sn, so that provided neither pro-
gression is just the zero sequence, we must have S1 = 1. Let d be the
common difference. Then S4 = S22 is equivalent to 6d + 4 = (d + 2)2,
whence d2 = 2d, and either d = 0 or d = 2. If d = 0 then Sn = n and
indeed SnSk = nk = Snk . If d = 2 then, as is well known, Sn = n2 (the
sum of the first n odd numbers), and SnSk = n2k2 = Snk . We conclude
that the given relation is satisfied by just three arithmetic progressions,
two of them the constant sequences consisting of all zeroes or all ones,
and the third the sequence of odd numbers.
Theme 21. Sequences given byrecurrence relations
21.1. Let b be the general term of the constant sequence satisfying the
given relation; thus b = qb + d. Write yn = xn − b. Substituting xn =yn + b and xn+1 = yn+1 + b in the given recurrence relation yields
yn+1 + b = q(yn + b) + d, or yn+1 = qyn,
since b = qb + d. Hence (yn) is a geometrical progression. Hence
if a is the first term of that progression, then yn = aqn−1, and xn =aqn−1 + b.
Solutions of the supplementary problems 283
21.2. By definition, xn = xn−1+xn−2
2. The characteristic equation of this recur-
rence relation is 2t2 − t − 1 = 0, and since the roots of this equation
are 1 and − 12
, we infer that xn = a + b(− 1
2
)n. From the assumptions
x0 = 0 and x1 = 1, it follows that a = −b = 23
. Hence
xn =2
3+
(−1)n−1
3 · 2n−1,
and the desired point is 23.
21.3. Answer: xn = c1Fn + c2Fn+1. Since the Fibonacci sequence (with
x0 = 0, x1 = 1) and its translate (x0 = 1, x1 = 1) satisfy the given
recurrence relation, the one shown here will also satisfy it. Let the first
two terms of any such sequence be x0 = a and x1 = b. Then a = c2
and b = c1 + c2, whence xn = (b − a)Fn + aFn+1.
21.4. a) Answer: any sequence with nth term of the form xn = an2 + bn +c. One might try informed guesswork to get this. Thus one might
first observe that the characteristic equation t3 − 3t2 + 3t − 1 = 0
of the given relation has t = 1 as a root of multiplicity three. The
sequences satisfying the recurrence relation xn+2 = 2xn+1 − xn,
whose characteristic equation has the root t = 1 of multiplicity
two, are, as we know (see Theorem 21.5), just the arithmetic pro-
gressions, that is, with nth term xn = an + b. Hence it is natural to
suspect that the sequence (xn) = (n2) might be one satisfying the
given relation. This is easy to check out, since, on the one hand,
(n + 3)2 = n2 + 6n + 9, and, on the other,
3(n + 2)2 − 3(n + 1)2 + n2 = 3n2 + 12n + 12
− 3n2 − 6n − 3 + n2 = n2 + 6n + 9.
However, there is another approach using an idea analogous to that
of the proof of Theorem 21.5. We set yn = xn+1 − xn, and note that
the given recurrence relation may be rewritten as
xn+3 − xn+2 = 2(xn+2 − xn+1) − (xn+1 − xn),
or yn+2 = 2yn+1 − yn. We infer that the sequence (yn) is an (arbi-
trary) arithmetic progression. Since xn − x0 =∑n−1
i=0 yi , and is
therefore equal to the sum of the first n terms of an arithmetic
progression, it will have quadratic form.
b) An example of a recurrence relation with the desired property
is xn+2 = 3xn − 2xn−1. The way to come up with this is to
284 Solutions of the supplementary problems
write down a cubic polynomial having 1 as a root of multiplic-
ity two—for example, (t − 1)2(t + 2) = t3 − 3t + 2—, and then
write down the recurrence relation having this as its characteristic
equation.
21.5. By contrast with the examples of Theme 21, here the desired recurrence
relation is not linear. A sequence (xn) is a geometric progression pre-
cisely ifxn+1
xn= xn
xn−1, or xn+1 = x2
n
xn−1. Of course, we are here including
constant sequences as geometric.
21.6. To solve this we use the solution of Problem 3 of Theme 21, where
it was shown that the Fibonacci number Fn+1 gives the number of
ways of tiling a 2 × n strip with 2 × 1 dominoes. Any two such tilings
differ only in the different arrangements of “vertical” tiles and pairs
of “horizontal tiles” (with one tile above the other in each pair). Let k
be the number of such horizontal pairs in a tiling. Then since 2k ≤ n,
we have k ≤ [n/2]. For each such k we need to count the number
of ways of choosing k 2 × 2 blocks in the 2 × n strip. For this we
argue as follows. For any particular such choice, imagine that the
vertical dominoes are black and that each 2 × 2 block consisting of
two horizontal dominoes has been replaced by a single vertical white
domino. Thus we now have a tiling of a 2 × (n − k) strip by dominoes
placed vertically, of which k are white and the rest black. The number
of such tilings is obviously(n−k
k
). Since each such tiling corresponds
to precisely one choice of k 2 × 2 blocks from the original 2 × n
strip, the number of the latter choices is likewise(n−k
k
). Summing(
n−k
k
)over k = 0, 1, . . . , [n/2], then gives the total number of tilings
of the 2 × n strip, which we know from the solution to Problem 3 to
be Fn+1.
Theme 22. The “golden ratio” or solvingequations of the form f (x) = x
22.1. Consider the function f (x) = x+2x+1
= 1 + 1x+1
on the interval [1,+∞).
It is, obviously, everywhere decreasing on that interval and
f ′(x) = − 1(x+1)2 > −1. The equation f (x) = x has the unique solu-
tion c =√
2 . Since x1 = 1 <√
2 , it follows from Theorem 22.1
that the sequence x1, x3, x5, . . . is increasing and the sequence
x2, x4, x6, . . . decreasing—both converging to√
2.
Solutions of the supplementary problems 285
It is worth mentioning in this connection that this sequence consists
of the successive finite continued fractions of the number√
2, since if
we define sn by
sn = 1 +1
2 +1
2 +1
2 + · · ·
(n − 1 fraction bars),
then
sn+1 = 1 +1
2 +1
2 +1
2 + · · ·
= 1 +1
1 + sn
=sn + 2
sn + 1,
and also s1 = 1.
22.2. a) An example of such a function is f (x) = 12
(x +
√x2 + 4
), whose
graph is sketched in Figure 120. This example shows that there is
Figure 120
no direct analogue of Theorem 22.1 for increasing functions.
b) That the equation f (x) = x has exactly one solution follows from
the fact that the function x − f (x) is increasing with slope at
least 1 − q > 0 at every point of its graph. For its derivative is
(x − f (x))′ = 1 − f ′(x) > 1 − q > 0 by assumption and it is not
difficult to prove (via the Mean-Value Theorem) that if a function
g defined on R has positive derivative bounded away from zero
then limx→±∞ g(x) = ±∞, so its graph must cross the x-axis, and
moreover at just one point.
22.3. Let f (c) = c. By the assumptions of the theorem c is then the only
solution of the equation f (x) = x.
286 Solutions of the supplementary problems
a) In the case x1 = c, the sequence defined by the recurrence rela-
tion xn+1 = f (xn) is constant. In the case x1 < c we have, by
assumption, that x2 = f (x1) > x1, and then in turn x2 = f (x1) <
f (c) = c. Thus x1 < x2 < c. The same argument shows that if
xn < c then xn < xn+1 < c, so by induction we conclude that if
x1 < c then the sequence (xn) is increasing and bounded above by
the number c. In the case x1 > c, we have x2 = f (x1) < x1 and
x2 = f (x1) > f (c) = c, and we conclude similarly that in this case
the sequence (xn) is decreasing and bounded below by c.
b) As shown above, in the case x1 < c the sequence (xn) is increasing
and bounded above. Hence by Weierstrass’s theorem it converges.
Let a denote its limit. Proceeding to the limit in the equation xn+1 =f (xn), we obtain f (a) = a. However, since by the assumptions of
the problem the equation x = f (x) has just one solution, we must
have a = c, that is, xn → c. The argument in the case x1 > c is
completely analogous.
22.4. Let’s consider the general case of a function of the form f (x) =√a + x and x1 =
√a , where a is any positive number. We consider
the function f (x) only for x in the interval [0,+∞). This function
is then easily seen to satisfy the conditions of Problem 22.3, whence
we infer that the sequence (xn) defined by xn+1 = f (xn), x1 =√
a,
converges to the solution of the equation√
a + x = x, that is, to the
number 1+√
1+4a
2. Hence, in particular: a) xn → 1+
√5
2; b) yn → 3.
22.5. 1) By the Mean-Value Theorem and the given assumptions, we have
for all numbers a, b that
|f (b) − f (a)| = |f ′(c)| |b − a| ≤ q |b − a|.a) Hence |xn+1 − xn| = |f (xn) − f (xn−1)| ≤ q |xn − xn−1|.b) The desired inequality follows from the chain of inequalities
|xn+1−xn| ≤ q |xn−xn−1| ≤ q2|xn−1−xn−2| ≤· · ·≤ qn|x1−x0|.c) We have
|xn+k−xn|=|xn+k−xn+k−1 + xn+k−1−xn+k−2+· · ·+xn+1 − xn|
≤ |xn+k−xn!+!k−1| + |xn+k−1 − xn+k−!2| + · · · + |xn+1−xn|
≤(qn+k−1+qn+k−2+· · ·+qn
)|x1−x0|
≤ (qn+qn+1+· · · )|x1−x0|
=qn
1 − q|x1 − x0|.
Solutions of the supplementary problems 287
2) From the inequalities of Part c) above (for all n, k) it follows that
the sequence (xn) is a so-called Cauchy sequence, that is—roughly
speaking—one whose terms get arbitrarily close to one another the
further along in the sequence one goes. It is a fundamental result of
mathematical analysis that every Cauchy sequence is convergent.
Thus suppose xn → c. Then proceeding to the limit in the equation
xn+1 = f (xn), we get c = f (c).
22.6. Before having your students work on this problem by themselves, try
to pique their interest—for instance, by showing them some pictures.
Figure 121a shows the behavior of the first seven terms of the sequence
of the given sort with first term chosen to be x1 = 2, and the same for
for the graph in Figure 121b except now with first term x1 = 5. It
seems pretty clear from these graphs that both sequences converge
to π . Figure 122 shows the sequence satisfying the given recurrence
1 2 3 4 5 6 7
2
1 2 3 4 5 6 7
4
(a) (b)
Figure 121
relation with first term x1 = −1. Here it would seem that the sequence
converges to −π . Thus although it might in principle be thought that
1 2 3 4 5 6 7
Figure 122
all solutions of the equation sin x = 0—all numbers of the form kπ—
should figure as limits of of sequences satisfying the given relation,
288 Solutions of the supplementary problems
these examples seem to indicate that for some reason the sequences in
question “refuse” to tend to 0, for example.
It is easy to see that the function f (x) = x + sin x is increas-
ing on the whole real line and moreover that f (x) > x for all
x ∈ (0, π ). Hence 0 = f (0) < f (x1) < f (π ) = π (where we are tak-
ing x1 ∈ (0, π )), that is, 0 < x2 < π . Note also that f (x1) > x1, so
that x2 > x1. It follows by induction that for any x1 ∈ (0, π ) the
resulting sequence (xn) is strictly increasing, positive, and bounded
above by π . Then since its limit must be a number of the form
kπ , that limit must in fact be π . Now let’s consider what hap-
pens if, for instance, x1 ∈ (−π, 0). Since sin x < 0 on this interval,
we have f (x) < x, whence x2 = f (x1) < x1. An induction shows
that in this case we obtain a decreasing sequence tending to −π .
The general answer is as follows: if x1 ∈ (2πk, π + 2πk), then the
sequence (xn) is increasing and converges to π + 2πk, while if x1 ∈(π + 2πk, 2π + 2πk), the sequence (xn) is decreasing and tends to
π + 2πk.
A question worth asking the students is the following one: “How
can the conditions of this problem be changed so that the analo-
gous sequences converge to numbers of the form 2πk?” Answer:
Consider the sequences satisfying the recurrence relation xn+1 =xn − sin xn.
Theme 23. Convex functions: inequalitiesand approximations
23.1. Since f ′(0) = n, the straight line with equation t = 1 + nx is tangen-
tial to the graph of y = (1 + x)n at the point (0, 1). Since the function
f (x) is convex, its graph lies above its tangent line, whence Bernoulli’s
inequality (1 + x)n ≥ 1 + nx for all x > −1.
a) The above argument goes through for the more general function
f (x) = (1 + x)α with α > 1. Hence (1 + x)α ≥ 1 + αx for all x ≥−1 provided α > 1. Figure 123a gives the geometric picture for
α = 43
.
b) For 0 < α < 1 the function f (x) = (1 + x)α is concave on the
interval (−1,∞), so that for all x ≥ −1 the inequality (1 + x)α ≤1 + αx holds. (In Figure 123b, α = 3
4.)
Solutions of the supplementary problems 289
(a) (b)
Figure 123
23.2. The standard special case of Jensen’s inequality for the function f (x) =1x
, convex on the interval (0,+∞), has the form
n
x1 + x2 + · · · + xn
≤1x1
+ 1x2
+ · · · + 1xn
n.
This may be rewritten as the inequality
n1x1
+ 1x2
+ · · · + 1xn
≤x1 + x2 + · · · + xn
n
between the harmonic and arithmetic means of n positive numbers.
However, in the author’s view this inequality is more naturally proved
by rewriting it in the form
(x1 + x2 + · · · + xn)
(1
x1
+1
x2
+ · · · +1
xn
)≥ n2
and appealing to the Cauchy-Schwarz inequality. Or one may establish
it as follows. Consider the inequality
x1 + x2 + · · · + xn
n≥ n
√x1x2 · · · xn ,
between the arithmetic and geometric means of n positive numbers,
and the same inequality, but this time applied to the reciprocals of
those numbers:
1x1
+ 1x2
+ · · · + 1xn
n≥
1
n√
x1x2 · · · xn
.
It is then immediate from these two inequalities that
n1x1
+ 1x2
+ · · · + 1xn
≤ n√
x1x2 · · · xn ≤x1 + x2 + · · · + xn
n.
290 Solutions of the supplementary problems
23.3. We raise both sides of the inequality
(x
p
1 + xp
2 + · · · + xpn
n
) 1p
≤(
xq
1 + xq
2 + · · · + xqn
n
) 1q
,
to the power p and rewrite the resulting inequality in terms of new
variables ti defined by xq
i = ti , i = 1, 2, . . . , n. Then since xi = t1/q
i ,
we have xp
i = tp/q
i , and the above inequality takes the form
tp
q
1 + tp
q
2 + · · · + tp
q
n
n≤
(t1 + t2 + · · · + tn
n
) p
q
.
It now only remains to observe that this inequality is Jensen’s inequality
as determined by the concave function f (x) = xp/q .
23.4. a) Since (sin x)′′ = − sin x < 0 for x ∈(0, π
2
], the sine function is
concave on that interval, so that its graph lies above every chord with
end-points having abscissas in the interval [0, π ]—a fact familiar
from sketches of the graph of y = sin x! In particular, the graph
of the sine function lies above the chord joining the points (0, 0)
and (π2, 1). Since this chord has equation y = 2x
πit follows that
sin x > 2xπ
for all x ∈(0, π
2
).
b) The idea is similar to that of the proof of the item a). The graph
of the sine function lies above the chord joining the points (0, 0)
and(
π6, 1
2
). Since this chord has equation y = 3x
πit follows that
sin x > 3xπ
for all x ∈(0, π
6
).
23.5. We proved in Part b) of the preceding problem that sin x > 3xπ
for
all x ∈(0, π
6
). Thus, in particular, sin π
30> 3
π· π
30= 1
10. Hence b =
a2 sin π
30
< 5a.
aa a a
a
b
b
b
Figure 124
Solutions of the supplementary problems 291
Here is another—geometric—solution. Lay off five copies of the given
triangle in the plane in such a way that neighboring copies have a side
of length b in common (as in Figure 124).
Since 5 · 12◦ = 60◦, the distance between the furthermost endpoints
of the bases of the first and fifth of these triangles is equal to b, which
is therefore less than the length of the broken line made up of the bases
of the five triangles, namely 5a.
Theme 25. Derivatives of vector-functions
25.1. Exercise1is just amatterofdifferentiating. InExample1,wehave f ′(t)=(a1, b1, c1). In Example 2, f ′(t) = (−aω sin ωt, aω cos ωt, 0), whence
| f ′(t)| =√
a2ω2 sin2 ωt + a2ω2 cos2 ωt = aω. In Example 3 we have
f ′(t) = (−aω sin ωt, aω cos ωt, b), whence | f ′(t)| =√
a2ω2 + b2.
Furthermore, the angle between the velocity vector and the z-axis has
cosine b√a2ω2+b2
and is therefore constant.
Exercise 2 may be done componentwise using the known rules for
differentiating an ordinary real-valued function, or directly from the
definition as the limit of a difference quotient, in which case the proofs
resemble the ones for real-valued functions. We give both proofs.
1) We have
(f (t) + g(t)
)′ = limh→0
1
h
[( f (t + h) + g(t + h)) − ( f (t) + g(t))
]
= limh→0
1
h
[( f (t + h) − f (t)) + (g(t + h) − g(t))
]
= limh→0
( f (t + h) − f (t)
h
)+ lim
h→0
( g(t + h) − g(t)
h
)
= f ′(t) + g′(t).
And here is the componentwise argument. Since, relative to
some Cartesian coordinate system, we have f (t) + g(t) =(f1(t) +
g1(t), f2(t) + g2(t), f3(t) + g3(t)), it follows that
(f (t) + g(t)
)′ =(f ′
1(t) + g′1(t), f ′
2(t) + g′2(t), f ′
3(t) + g′3(t)
)
=(f ′
1(t), f ′2(t), f ′
3(t))+
(g′
1(t), g′2(t), g′
3(t))
= f ′(t) + g′(t).
292 Solutions of the supplementary problems
2) We have
(ϕ(t) f (t)
)′ = limh→0
1
h
[ϕ(t + h) f (t + h) − ϕ(t) f (t)
]
= limh→0
1
h
[ϕ(t + h) f (t + h) + ϕ(t) f (t + h)
− ϕ(t) f (t + h) − ϕ(t) f (t)]
= limh→0
1
h
[(ϕ(t + h) − ϕ(t)) f (t + h) + ϕ(t)( f (t + h) − f (t))
]
= limh→0
[ϕ(t + h) − ϕ(t)
hf (t + h)
]+ lim
h→0
[ϕ(t)
f (t + h) − f (t)
h
]
= ϕ′(t) f (t) + ϕ(t) f ′(t).
For the componentwise argument, note first that
ϕ(t) f (t) =(ϕ(t)f1(t), ϕ(t)f2(t), ϕ(t)f3(t)
).
Hence
(ϕ(t) f (t)
)′ =(ϕ′(t)f1(t) + ϕ(t)f ′
1(t), ϕ′(t)f2(t) + ϕ(t)f ′2(t),
ϕ′(t)f3(t) + ϕ(t)f ′3(t)
)
= ϕ′(t)(f1(t), f2(t), f3(t)
)+ ϕ(t)
(f ′
1(t), f ′2(t), f ′
3(t))
= ϕ′(t) f (t) + ϕ(t) f ′(t).
3) The proof that(
f (t) · g(t))′ = f ′(t) · g(t) + f (t) · g′(t) is similar
to the preceding one. One inserts f (t) · g(t + h) − f (t) · g(t + h)
into the numerator of the difference quotient and breaks the limit
up into two limits (and uses the fact that the dot product distributes
over vector addition).
For the componentwise argument, note first that
f (t) · g(t) = f1(t)g1(t) + f2(t)g2(t) + f3(t)g3(t).
Hence
(f (t) · g(t)
)′ = f ′1(t)g1(t) + f1(t)g′
1(t) + f ′2(t)g2(t) + f2(t)g′
2(t)
+ f ′3(t)g3(t) + f3(t)g′
3(t)
= f ′(t) · g(t) + f (t) · g′(t).
Solutions of the supplementary problems 293
4) If f (t) is a constant vector on an interval of values of t , then
limh→0
f (t + h) − f (t)
h= lim
h→0
0
h= 0.
For the converse we use the representation of f (t) in terms
of components relative to some coordinate system, say f (t) =(f1(t), f2(t), f3(t)
). Then if f ′(t) = 0 for all t in an interval,
it follows that f ′i (t) = 0 (i = 1, 2, 3) on that interval, whence
fi(t) = const (i = 1, 2, 3) (the proof of which requires the Mean-
Value Theorem!). Hence f (t) = const .
25.2. Consider a point-particle moving in the plane of the triangle ABC,
and passing through the point M in question at time t0. Write Mt
for the position of the particle at time t . We define vector-functions
f (t), g(t) and h(t) by f (t) = MtA, g(t) = MtB and h(t) = MtC,
and write ϕ(t) = | f (t)| + |g(t)| + |h(t)|. By assumption, the func-
tion ϕ(t) attains its least value at the time t = t0, so we must have
ϕ′(t0) = 0. Since g(t) = MtB = MtA + AB = f (t) + AB, it follows
that g′(t) = f ′(t), and, similarly, h′(t) = f ′(t). Let v denote the value
of the derivative of these vector-functions at time t = t0, and by e1,
e2 and e3 the unit vectors parallel to the vectors MA, MB and MC
respectively. Then
0 = ϕ′(t0) = v · e1 + v · e2 + v · e3 = v · (e1 + e2 + e3).
Since the value of the velocity vector v at t0 may clearly be arranged
to be nonzero and not perpendicular to e1 + e2 + e3, we infer from
the fact that v · (e1 + e2 + e3) = 0 that e1 + e2 + e3 = 0. However,
the only way three planar unit vectors can sum to zero is if the angle
between each two of them is 120◦.
However, this argument is defective. It nowhere uses the assumption
in the problem that the triangle ABC be acute-angled. What has been
overlooked in the above argument is that if the point M should coincide
with one of the vertices of the triangle, then the function ϕ would
not be differentiable at t = t0 and Fermat’s result that the derivative
vanishes at a point where a function has a local extreme value would
be inapplicable.
Thus we need to complete the argument. It is not difficult to show
that if the triangle ABC is acute-angled, then the point M for which
the sum of its distances from the vertices is least cannot coincide with
a vertex.
294 Solutions of the supplementary problems
For the sake of completeness, we give the answer also in the case
where the triangle is not acute-angled. If its angles are still all less than
120◦, then the answer is as in the acute-angled case. If, on the other
hand, one of the angles is greater than or equal to 120◦, then the vertex
where the triangle has that angle is the point such that the sum of the
distances from it to the three vertices is least.
25.3. From f ′(t) = f (t) × h and a basic property of the cross product, it
follows that f ′(t) ⊥ f (t) and f ′(t) ⊥ h. Hence f ′(t) · f (t) = 0 and
f ′(t) · h = 0, whence | f (t)| = const and f (t) · h = const . Hence a
point-particle with motion given by f (t) is restricted to a sphere and
also to a plane, whence it follows that it must move in a circle. Further-
more, in view of the constancy of the angle between the vectors f (t)
and h (taken together with the given equation for f ′(t)), the quantity
| f ′(t)| is also constant. Hence if we introduce a rectangular Carte-
sian coordinate system with the z-axis parallel to the vector h, then in
terms of components referred to that frame, f (t) will have the form
(a cos ωt, a sin ωt, b).
25.4. We introduce a rectangular Cartesian coordinate system with z-axis
parallel to the vector H . Then from the solution of the preceding prob-
lem we have that the derivative f ′(t) of the vector-function f (t) giving
the motion of the electron, has components (a cos ωt, a sin ωt, b) rel-
ative to that frame. Hence in terms of its component functions, the
vector-function f (t) will have the form
(x0 − a
ωsin ωt, y0 + a
ωcos ωt, z0 + bt
),
showing that the electron does indeed move along a helix.
Theme 26. Polynomials andtrigonometric relations
26.1. In solving Problem 2 of this Theme, we showed that the numbers
x1 = cos 2π5
and x2 = cos 4π5
are both roots of multiplicity two of the
polynomial 16x5 − 20x3 + 5x − 1, the fifth of whose roots is 1. Hence
by Viete’s theorem we have x21x2
2 = 116
. Then since x1 > 0 and x2 < 0,
we conclude that x1x2 = − 14
.
26.2. It follows from the proof of Problem 3 that the square of the product in
question is equal to 2n + 1. Since all factors in the product are positive,
we conclude that it must be equal to√
2n + 1 .
Solutions of the supplementary problems 295
26.3. Since Tn(x) = 2xTn−1(x) − Tn−2(x), increasing n by 1 results in the
multiplication of the leading coefficient by the factor 2. Then since
T1(x) = x, the leading coefficient of the polynomial Tn(x) must be
2n−1.
26.4. (1) Since Tn(cos t) = cos nt , we have Tn(xk) = cos πk = (−1)k .
(2) if x ∈ (xk+1, xk) then x = cos t for some t ∈(
kπn
, (k+1)π
n
).
Since Tn(cos t) = cos nt , we have T ′n(cos t) sin t = n sin nt . Obviously
sin t > 0 on these intervals. And since kπ < nt < (k + 1)π , the func-
tion sin nt does not change sign on the interval(
kπn
, (k+1)π
n
). Hence the
derivative T ′n(x) preserves its sign on each of the intervals (xk+1, xk)
and Tn(x) is therefore monotonic on each of them. Since it is cer-
tainly continuous, Tn(x) is therefore monotonic on each closed interval
[xk+1, xk].
26.5. 1) Here one needs to “face the music” and verify directly that Tn(x) sat-
isfies the given differential equation—by means of differentiation and
algebraic manipulation—on each of the intervals (−∞,−1), (−1, 1)
and (1,+∞) separately. On the first and third of these one can use
the explicit form of Tn(x) given by Lemma 26.3, and on the interval
(−1, 1) the definition of the Chebyshev polynomials.
2) On making the substitution x = cos t , t ∈ [0, π ], in the given inte-
gral, we obtain the integral∫ π
0cos kx cos nx dx, and showing that this
vanishes is standard:
∫ π
0
cos kx cos nx dx =1
2
∫ π
0
(cos(k + n)x + cos(k − n)x
)dx
=1
2
(sin(k + n)x
k + n+
sin(k − n)x
k − n
)∣∣∣∣π
0
= 0.
26.6. Since the left-hand side of the given identity is a polynomial, it is
enough to prove that it holds on the interval [−1, 1]. Thus it suffices
to verify the identity
T 2n (cos t) − (cos2 t − 1)U 2
n−1(cos t) = 1.
Here the left-hand side is
cos2 nt +(sin t Un−1(cos t)
)2 = cos2 nt + sin2 nt = 1,
completing the verification.
296 Solutions of the supplementary problems
26.7. 1) Since Un−1(x) = 1n
T ′n(x), we have
Un−1(cos t) sin t =1
nT ′
n(cos t) sin t
= −1
n
(Tn(cos t)
)′ = −1
n(cos nt)′ = sin nt.
2) Making the substitution x = cos t , t ∈ [0, π ], in the given integral,
we get the integral
∫ π
0
Uk(cos t)Un(cos t) sin2 t dt
=∫ π
0
sin(k + 1)t sin(n + 1)t dt
=1
2
∫ π
0
(cos(k − n)t
− cos(k + n + 2)t)dt = 0.
Theme 27. Areas and volumes as functionsof co-ordinates
27.1. let A(x1, y1) be any point on the line ℓ. The point B(x2, y2) with
coordinates x2 = x1 − b and y2 = y1 + a is then also on the line ℓ
since
ax2 + by2 + c = a(x1 − b) + b(y1 + a) + c = ax1 + by1 + c = 0.
Consider the triangle ABM . The altitude of this triangle dropped from
the vertex M is the desired distance d from M to the line ℓ. The
formula for the Euclidean distance between two points gives |AB| =√a2 + b2 , whence
SABM =1
2
√a2 + b2 · d(M, ℓ).
On the other hand, by the formula (2) this area is equal to
1
2|(x0 − x1)(y2 − y1) − (y0 − y1)(x2 − x1)| =
1
2|a(x0 − x1) + b(y0 − y1)|
=1
2|ax0 + by0 − (ax1 + by1)|
=1
2|ax0 + by0 + c|.
Solutions of the supplementary problems 297
Hence
1
2
√a2 + b2 · d(M, ℓ) =
1
2|ax0 + by0 + c|,
whence the desired formula.
27.2. Since any polygon can be dissected into triangles, it suffices to prove
the formula (6) in the case that M is a triangle, with vertices A,B,C,
say. Since the area of a triangle is unchanged by translations we may
without loss of generality assume that the vertex C is the origin.
This assumed, consider the other vertices A(x1, y1), B(x2, y2) and their
images A1(a1x1 + b1y1, a2x1 + b2y1), B1(a1x2 + b1y2, a2x2 + b2y2)
under the mapping �. (Note that of course � fixes C.) Then since
(a1x1 + b1y1)(a2x2 + b2y2) − (a2x1 + b2y1)(a1x2 + b1y2)
= a1a2x1x2 + a1b2x1y2 + a2b1x2y1 + b1b2y1y2a1a2x1x2
− a2b1x1y2 − a1b2x2y1 − b1b2y1y2
= (a1b2 − a2b1)x1y2 − (a1b2 − a2b1)x2y1
= (a1b2 − a2b1)(x1y2 − x2y1),
the desired formula follows from the formula (1).
27.3. Under the translation taking the vertex D to the origin, the other
three vertices are sent to the points A1(x1 − x4, y1 − y4, z1 − z4),
B1(x2 − x4, y2 − y4, z2 − z4) and C1(x3 − x4, y3 − y4, z3 − z4), and
the volume of the original tetrahedron ABCD is the same as that of
the tetrahedron OA1B1C1. Consider the parallelepiped determined by
the edges OA1, OB1 and OC1. The area of the triangle OA1B1 is then
half that of the parallelogram defined by the edges OA1 and OB1, and
since the height of the parallelepiped as measured from the paralel-
logram containing the triangle OA1B1 is the height of the tetrahedron
as measured from that face as base, we obtain (as in the solution of
Problem 1 of Theme 15)
VABCD =1
3·
1
2V0 =
1
6V0,
where V0 is the volume of the parallelepiped. Hence from the for-
mula (3) we get the following formula for the volume of the given
298 Solutions of the supplementary problems
tetrahedron:
VABCD =1
6
∣∣∣∣∣∣
∣∣∣∣∣∣
x1 − x4 y1 − y4 z1 − z4
x2 − x4 y2 − y4 z2 − z4
x3 − x4 y3 − y4 z3 − z4
∣∣∣∣∣∣
∣∣∣∣∣∣.
27.4. Consider the vectors a(a1, a2) and b(b1, b2). Part a) is immediate from
the formula (5) with one pair of coordinates set equal to zero in that
formula, that is, from the formula
S(a, b) = a1b2 − a2b1
for the oriented area of the parallelogram.
For the proof of Part b) we need the additional vector c(c1, c2). Note
that S(d, d) = 0 for every vector d. The given system is xa + yb = c.
Hence
S(c, b) = S(xa + yb, b) = xS(a, b) + yS(b, b) = xS(a, b),
whence we get, via the formula (5), the desired formula for x. The
formula for y is obtained similarly.
Theme 28. Values of trigonometric functionsand sequences satisfying a certain recurrencerelation
28.1. We write xk = cos 2kπ2n+1
, as in Problem 9. We wish to prove that x1 �= xk
for all k = 2, 3, . . . , n. If x1 = xk , then
2kπ
2n + 1= ±
2π
2n + 1+ 2πm, m ∈ Z.
Simplifying, we get
2k−1 = ±1 + m(2n + 1), or 2k−1 ± 1 = m(2n + 1),
which is impossible since the number 2k−1 ± 1 is positive and less than
2n + 1.
28.2. We know that the first terms of periodic sequences of the sort in
question must lie in the interval [−1, 1], so we may write x1 = cos α,
and then xn+1 = cos 2nα. Hence x1 = xn+1 if and only if 2nα = ±α +2πk, whence
α =2πk
2n ± 1, and x1 = cos
2πk
2n ± 1.
Solutions of the supplementary problems 299
28.3. Consider the interval (u, v) with u = arccos β and v = arccos α. Thus
cos x ∈ (α, β) for all x ∈ (u + 2πm, v + 2πm), m ∈ Z. Choose the
natural number n large enough for 2π2n+1
< v − u to hold, and choose
the natural number m so that 2π2n+1
< u + 2πm. The common difference
of the arithmetic progression with kth term sk = 2πk2n+1
, is then less
than the length of the interval (u + 2πm, v + 2πm), so there exists
a natural number k such that u + 2πm < 2πk2n+1
< v + 2πm. Thus by
construction the number x = cos 2πk2n+1
is the first term of a periodic
sequence of the sort in question and lies in the interval (α, β).
28.4. Admittedly, the conditions of this problem are such that it looks rather
formidable. However, someone who has read the earlier Themes atten-
tively may guess from the shape of the graph that Chebyshev poly-
nomials (see Theme 26) are involved. Writing f (x) = 2x2 − 1 (the
Chebyshev polynomial T2(x)), we define
fn(x) = f (f (· · · (f︸ ︷︷ ︸n times
(x) · · · ).
The polynomial fn (the Chebyshev polynomial T2n(x)) has degree 2n,
and the polynomial given in the problem is just f3(x). Hence the abscis-
sas of the points of intersection of the graph of f3(x) with the line y = x
are the solutions of the equation f3(x) = x. Let a be any of these solu-
tions, and consider the sequence (xn) defined by the recurrence relation
xn+1 = 2x2n − 1 = f (xn) together with the specification x1 = a. Then
x2 = f (x1), x3 = f (x2) = f (f (x1)), and x4 = f3(x1) = f3(a) = a, so
that x4 = x1. Clearly, f (x) = x implies f3(x) = x, so the solutions of
the equation f3(x) = x include the numbers 1 and − 12, the first terms
of the constant sequences of the sort in question. For all sequences
with first term a solution of this equation other than 1 and − 12, we will
have x2 �= x1. But is it possible that x3 = x1? This would imply that
f (f (x1)) = x1, whence x1 = f (f (f (x1))) = f (x1), an impossibility.
We conclude that the roots other than 1 and − 12
are first terms of
sequences of the sort in question of period 3.
28.5. In the notation of the preceding solution, we have fn(x) = T2n(x),
the 2nth Chebyshev polynomial of the first kind. By Lemma 26.5,
on each subinterval [xk+1, xk] of the interval [−1, 1], where xk =cos πk
2n , k = 0, 1, 2, . . . , 2n, the function fn(x) is monotonic. Further-
more the image under fn of each of these subintervals is [−1, 1].
Hence the equation fn(x) = x has at least one solution in each of these
300 Solutions of the supplementary problems
subintervals. Since the number of such subintervals is 2n, which is also
the degree of fn(x), the equation fn(x) = x has precisely 2n real roots.
By the solution of the previous problem the roots of the equation
fn(x) = x are first terms of sequences of the required sort with xn+1 =xn. Hence the period d of such a sequence must be a divisor of n.
28.6. From the solution of the previous problem and the inclusion-exclusion
principle (see Problem 2 of Theme 24) it follows that the number of
solutions yielding sequences of period exactly n is
2n −∑
ki |n
2ki +∑
ki>kj |n
2(ki ,kj ) −∑
...
2(ki ,kj ,kl ) + · · · ,
where ki, kj , . . . are the positive divisors of n, and (ki, kj , . . .) denotes
the greatest common divisor of the numbers between the parentheses.
Theme 29. Do there exist further “numbers”beyond complex numbers?
29.1. a) We have
uu = (a + bi + cj + dk)(a − bi − cj − dk)
= a2 + b2 + c2 + d2 + a(bi + cj + dk) − a(bi + cj + dk)
− bcij − bcji − bdik − bdki − cdjk − cdkj
= a2 + b2 + c2 + d2 = |u|2.
b) Unquestionably, all one needs do here is calculate carefully. Since
we shall be needing the formula for the product of two quaternions a
little further on, let’s first do that calculation. If
u = a + bi + cj + dk and v = A = Bi + Cj + Dk,
then
uv = aA − bB − cC − dD + (aB + bA + cD − dC)i
+ (aC + cA + dB − bD)j + (aD + dA + bC − cB)k.
Then in order to get the formula for the product vu in the other order, all
we have to do is switch the big and small letters in the above formula.
Solutions of the supplementary problems 301
Thus
vu = aA − bB − cC − dD + (aB + bA + dC − cD)i
+ (aC + cA + bD − dB)j + (aD + dA + cB − bC)k.
Then in order to get the formula for the product v u, one needs to
introduce minus signs in front of each of the letters b, B, c, C, d,D.
This yields
v u = aA − bB − cC − dD + (−aB − bA + dC − cD)i
+ (−aC − cA + bD − dB)j + (−aD − dA + cB − bC)k.
It then only remains to observe that
uv = aA − bB − cC − dD − (aB + bA + cD − dC)i
− (aC + cA + dB − bD)j − (aD + dA + bC − cB)k = v u.
c) Using the equalities established in the previous two solutions
together with the associativity of the multiplication of quaternions,
we get
|uv|2 = (uv)(uv) = (uv)(v u) = (u(vv))u = (uu)|v|2 = |u|2|v|2.
d) From the above formula for the product of two quaternions it follows
that
|uv|2 = (aA − bB − cC − dD)2 + (aB + bA + cD − dC)2
+ (aC + cA + dB − bD)2 + (aD + dA + bC − cB)2,
and since
|u|2|v|2 = (a2 + b2 + c2 + d2)2(A2 + B2 + C2 + D2)2,
we infer via the result of Part c) the identity
(a2 + b2 + c2 + d2)2(A2 + B2 + C2 + D2)2
= (aA − bB − cC − dD)2 + (aB + bA + cD − dC)2
+ (aC + cA + dB − bD)2 + (aD + dA + bC − cB)2.
29.2. Writing u1 = b1i + c1j + d1k and u2 = b2i + c2j + d2k, we have
u1u2 = −(b1b2 + c1c2 + d1d2) + (b1c2 − b2c1)i
+(a2c1 − a1c2)j + (a1b2 − a2b1)k.
302 Solutions of the supplementary problems
The very notation i, j and k suggests that we should look for the
desired geometric interpretation in the vector space of space vectors,
that is, consider u1 and u2 as vectors u1(a1, b1, c1) and u2(a2, b2, c2).
The quantity b1b2 + c1c2 + d1d2 is then the dot product u1 · u2 of the
vectors u1 and u2, while the vector
(b1c2 − b2c1, a2c1 − a1c2, a1b2 − a2b1)
is one that has appeared several times before, for instance in Theme 27.
It is perpendicular to both of the vectors u1 and u2 and has magnitude
equal to the area of the parallelogram determined by those vectors. Of
course, this is none other than the cross product u1 × u2. We conclude
that if we identify the purely imaginary quaternions with the vectors
of Euclidean R3, then we shall have u1u2 = −u1 · u2 + u1 × u2.
Index
acceleration, 189
centripetal, 193
area
of the faces of a tetrahedron, 11
of planar regions, 129
of polygons, 215
of quadrilaterals, 66, 85, 262
of a trapezoid, 85, 131
of triangles, 85, 207, 208, 214, 263
signed, 214
Bernoulli’s inequality, 176, 288
Binet’s formula, 154
binomial
coefficients, 119, 160, 178
relations between, 120
theorem, 178
Cauchy sequence, 286
Cauchy’s mean-value theorem, 20, 180
Cauchy-Schwarz inequality, 105, 267
Ceva’s theorem, 88
Chebyshev polynomials
of the first kind, 202, 299
of the second kind, 204
properties of, 202, 203
circumcircle, 102
combinatorics, 119, 155, 184
complex numbers, 72, 73, 76, 79, 158, 224,
258
congruence of numbers with respect to a
modulus, 114
continued fraction(s), 163, 284
convergent sequences, 23, 143, 162, 163,
164, 174, 175, 281
Cramer’s rule, 216
curvature, 196
cyclic quadrilateral, 66
de Moivre’s theorem, 73, 79, 200, 256
determinant, 213
derivative, 30, 33, 53, 55, 57, 63, 66, 178,
233, 251
definition of, 188, 250
of vector-functions, 187
diophantine equations, 111, 271
distance from a point to a line, 215
division with remainder, 112, 115, 257, 272
divisors, 111
equation
of a circle, 7, 41, 43
of an ellipse, 34, 43
of a parabola, 9, 39
of a straight line, 8, 41
of a union of sets, 45, 243
set given by, 39, 243
Euler’s formula for complex exponents, 183
exponent rule, 143, 183
Fermat’s optical principle, 192
Fibonacci numbers, 153, 160, 162, 284
relations between, 155
field, 224
axioms of a, 223
first nontrivial limit, 19
functional equation, 143, 146
of exponential functions, 144
of linear functions, 143
of power functions, 144
functions
continuous, 143
contracting, 166, 286
convex, 167
differentiable, 146, 164
Fundamental Theorem
of Algebra, 224
of Calculus, 129, 134, 137
golden ratio, 161
graph of a function, 30, 33, 53, 55, 231, 233
helix, 188, 197
Heron’s formula, 102, 207
incircle, 89, 102
inclusion-exclusion formula for sets, 185
303
304 Index
inequalities
between arithmetic and geometric means
(a.m.–g.m. inequality), 101, 102, 103,
269
generalized version, 172
between arithmetic and harmonic means,
108, 269, 288
between arithmetic and quadratic means,
105
geometric interpretation of, 132
integral, 20, 129
application of, 131, 276
evaluation of, 130, 135, 138
Jensen’s inequality, 170
Law of Cosines, 66, 68, 208
generalization of, 266
length of a circle, 17
logarithm, 29, 250
means of two numbers, 101, 108, 167,
251
mean-value theorem, 165, 251, 286
Minkowski’s inequality, 106
multiplicity of a root, 57
Napoleon’s problem, 80
Newton’s tangent method, 24, 174
number e, 29, 186
optical property of ellipses, 191
orthogonal projection, 11, 211
parallelepiped, 93
Pell’s equation, 4, 205
periodic sequence(s), 219
permutation, 184
polynomials, 55
divisibility of, 71
factorizing of, 66, 226, 256
multiple roots of, 49, 57, 178, 247
roots of, 49, 63, 66, 199, 201, 243
prime number(s), 115, 116
probability, 123, 124, 184
pyramid, 254
Pythagoras’ theorem, 3, 17
generalization of, 97
Pythagorean triple(s), 3
quaternions, 229, 300
radius of curvature, 196
rational approximations, 143, 186
recurrence relation, 23, 151, 153, 162, 164,
202, 218
characteristic equation of, 156
Rolle’s theorem, 20, 169
roots of unity. 73, 74, 79, 81, 256, 258
rotation, 79, 80, 259
Schwarz’s inequality, 137, 278
signed area, 214
Simpson’s rule, 138, 278, 280
Snell’s law of refraction, 192
solid of revolution, 134
speed, 108, 189
of light in a medium, 192
tangent line, 24, 57, 60, 169, 191, 231, 247
Taylor polynomial, 179
Taylor series
for the exponential function, 181
for the sine and cosine functions, 181
Taylor’s theorem, 19, 180
for polynomials, 177
tetrahedron, 11, 93, 125
tiling, 153, 155, 284
tower of Hanoi, 151
triangle inequality, 11, 290
generalization of, 11
trigonometric relations, 73, 76, 199, 201, 258
values of trigonometric functions, 73, 217
vector-functions, 187
coordinates of, 187
vectors, 12, 79, 259, 265
cross product of, 96, 98, 195, 212, 301
non-coplanar, 15
velocity, 188
Viete’s formula, 49, 200, 201, 244
volume
of a cone, 135
of a doughnut, 135
of a parallelepiped, 93, 98, 212
of a solid of revolution, 134
of a tetrahedron, 93, 99, 266
Weierstrass’ theorem on continuous
functions, 225
Young’s inequality, 132
NML/52
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AMS / MAA ANNELI LAX NEW MATHEMATICAL LIBRARY
Portal through Mathematics is a collection of puzzles and problems mostly
on topics related to secondary mathematics.
The problems and topics are fresh and interesting and frequently
surprising. One example: the puzzle that asks how much length must be
added to a belt around the Earth’s equator to raise it one foot has probably
achieved old chestnut status. Ivanov, after explaining the surprising answer
to this question, goes a step further and asks, if you grabbed that too long
belt at some point and raised it as high as possible, how high would that
be? The answer to that is more surprising than the classic puzzle’s answer.
The book is organized into twenty-nine themes, each a topic from algebra,
geometry or calculus and each launched from an opening puzzle or
problem. There are excursions into number theory, solid geometry, physics
and combinatorics. Always there is an emphasis on surprise and delight.
And every theme begins at a level approachable with minimal background
requirements. With well over 250 puzzles and problems, there is some-
thing here sure to appeal to everyone.
Portal through Mathematics will be useful for prospective secondary
teachers of mathematics and may be used (as a supplementary resource)
in university courses in algebra, geometry, calculus, and discrete math-
ematics. It can be also used for professional development for teachers
looking for inspiration. However, the intended audience is much broader.
Every fan of mathematics will fi nd enjoyment in it.