Team Play Solutions
Part i: There are many lines with slope 1 that thread the lattice; for
example, any line of the form y = x+b having a y-intercept in the range
1 ≤ b ≤ 3 will do, such as y = x+√2. (We omit the sketch of the line
and the nearby lattice squares.) Note that there are plenty of such lines
that cleanly thread the lattice.
Next we consider slope − 12 lines. In this case any line of the form
y = − 12x + b with 4 ≤ b ≤ 5 works; all except the b = 4 and b = 5
intercepts cleanly thread. (There are other answers as well.) For slope 23 ,
however, we must choose the y-intercept carefully. Two possible answers
are y = 23x + 1 and y =
2
3x + 4
1
3 . Every possible answer only barely
threads the lattice, though. Finally, any line of the form y = 3x+ b with
1 ≤ b ≤ 2 will thread the lattice; all except b = 1 and b = 2 cleanly
thread. (Again, other answers are possible.)
Part ii: Suppose that we have drawn a line in the plane with slope m
that cleanly threads the lattice. Consider a reflection of the entire plane
over the horizontal line y = 3. It straight-forward to verify that the
lattice squares wind up in exactly the same positions as before, while
the reflected line has slope −m. Clearly the new line still cleanly threads
the lattice, so we’re done. The same type of argument can be used to
show that there is also a line with slope 1m that cleanly threads the
lattice by reflecting the diagram over the line y = x. Finally, if we
perform both of these reflections (in either order), we obtain a line with
slope − 1m that cleanly threads the lattice.
Part iii: The lower endpoint of the shadow is found by determining the
equation of the line through the lower right corner of the (5, 5)-square,
which has coordinates (6, 5). This equation is y = 34x +
1
2 . Since the
y-intercept is 12 , the shadow cast on the y-axis must begin at y =
1
2 . In
the same way we find that the line throught the upper left corner (5, 6)
is y = 34x+2
1
4 , so the upper endpoint of the shadow on the y-axis is 2
1
4 .
Hence, the length of the shadow is 2 14 − 12 = 1 34 .
Part iv: Since the (5, 5)-square’s shadow overlaps with that of the (0, 0)-
square, it stands to reason that the (10, 10)-squares’s shadow will overlap
with that of the (5, 5)-square. Indeed, the lines with slope 34 that just
touch the (10, 10)-square on either side are y = 34x+1
3
4 and y =
3
4x+4.
Thus its shadow on the y-axis is the segment from y = 1 34 to y = 4,
which is higher than the shadow of the (5, 5)-square but overlaps it.
Consider the shadows of the squares along the main diagonal, which
include the (−5,−5), (0, 0), (5, 5), (10, 10)-squares, and so on. We claim
that they form an interlocking set of shadows which cover the entire
y-axis. We have already seen that each such shadow has length 1 34 .
Furthermore, as we step from one square to the next along the diagonal,
the shadow is raised by the same amount at each step. But we have
already seen the lower endpoint of the shadow moved up from y = 12 to
y = 1 34 in going from the (5, 5)-square to the (10, 10)-square, a shift of
only 1 14 . Hence all these shadows overlap, as claimed.
We are now able to conclude that no line with slope 34 is able to
thread the lattice. For any such line must intersect the y-axis at a point
which is in the interior of some shadow. This shadow is cast by some
square via a slope 34 line; hence our line must have passed through the
interior of this square, which means that it does not thread the lattice.
Part v: To begin, it is easy to confirm that the shadow cast by the
(0, 0)-square stretches from y = −pq to y = 1. (Check this.) Now let
the (5c, 5d)-square be an arbitrary square in the lattice. If this square is
to cast a shadow which overlaps with that of the (0, 0)-square, then the
line with slope m = pq and passing through (5c+ 1, 5d) (the lower right
corner of the square) must have a y-intercept b satisfying −pq < b < 1.
We can determine the y-intercept by writing
y = mx+ b =⇒ 5d = p
q
(5c+ 1) + b =⇒ b = 5d− p
q
(5c+ 1).
Hence we wish to find integers c and d such that
−p
q
< 5d− p
q
(5c+ 1) < 1 =⇒ 0 < dq − cp < p+ q
5
.
But p and q are relatively prime positive integers (we can safely assume
that the fraction pq is written in lowest terms), hence there is a multiple
of q which is exactly 1 greater than a multiple of p. (This is a standard
fact from elementary number theory; you should test it out if you are
unfamiliar with it.) Let dq and cp be these multiples, so that dq−cp = 1.
Since p+ q > 5, we have found a solution to the above inequality.
Part vi: Our argument will closely mimic part iv. Let c and d be the
integers found in the previous part. The idea is that whenever we step
from a square in the lattice to the square 5c units away in the x-direction
and 5d units away in the y-direction, we reach a new square whose
shadow is slightly higher than but overlaps with the previous shadow.
The whole sequence of squares obtained in this manner will provide a
set of interlocking shadows which completely cover the y-axis. Hence no
line with slope pq can thread the lattice, using the same logic as above.
Finally, it turns out that whenever p+q = 5 there is a line with slope
m = pq that threads the lattice, but only barely. And slopes for which
p + q < 5 permit lines that cleanly thread the lattice, as the first part
suggests. In case you were wondering, a line with an irrational slope
can never thread the lattice. (Can you prove this?) Of course, there is a
natural extension to lattices in which every kth square is shaded, instead
of every fifth square. The same sorts of results hold in this more general
setting, a fact which the reader is invited to confirm.
c© Greater Testing Concepts 2008
January 2009
Round One Solutions
Greater Testing Concepts The Mandelbrot Team Play
PO Box 760 web.mandelbrot.org
Potsdam, NY 13676 info@mandelbrot.org
Team Play Solutions
Part i: Substituting in b = 0 we obtain FaF0 + Fa+1F1 = Fa+1. Since
F0 = 0 and F1 = 1, this reduces to just Fa+1 = Fa+1, which is obviously
true. Next, substituting b = 1 gives FaF1 + Fa+1F2 = Fa+2. Since
F2 = 1 also, this time the relationship reduces to Fa + Fa+1 = Fa+2,
which is again clearly true by definition of the Fibonacci sequence.
When a = 5 and b = 7 we must confirm that F5F7+F6F8 = F13. We
first compute F5 = 5, F6 = 8, F7 = 13 and F8 = 21. Hence the left-hand
side becomes (5)(13) + (8)(21) = 65+ 168 = 233. But F13 = 233, so the
relationship holds in this case as well.
Part ii: We have seen that the relationship FaFb +Fa+1Fb+1 = Fa+b+1
holds for b = 0 and b = 1. To prove that it holds in general, we assume
that it is true for all values of b from b = 0 up to b = k, for some fixed
number k. We will then argue that it is also true for b = k + 1, from
which the result will follow by induction.
Since the statement is true for b = k − 1 and b = k, we know that
FaFk−1 + Fa+1Fk = Fa+k and FaFk + Fa+1Fk+1 = Fa+k+1
holds for all a ≥ 0. Adding these two equalities yields
Fa(Fk−1 + Fk) + Fa+1(Fk + Fk+1) = Fa+k + Fa+k+1,
which simplifies to FaFk+1 + Fa+1Fk+2 = Fa+k+2. But this is exactly
the case b = k + 1 which we wished to prove, so we are done.
Part iii: Replacing b by a−1 in the identity FaFb+Fa+1Fb+1 = Fa+b+1
we find that FaFa−1+Fa+1Fa = F2a. Factoring out an Fa on the left, we
have Fa(Fa−1+Fa+1) = F2a. Since the product of Fa and another integer
(namely Fa−1+Fa+1) gives F2a, we conclude that F2a is a multiple of Fa.
We can use the same technique again by choosing b = 2a−1 instead.
This time we obtain FaF2a−1+Fa+1F2a = F3a. We cannot immediately
factor out an Fa as before, but we already know that F2a is a multiple
of Fa, hence the entire left-hand side must be also. More precisely, we
could substitute our expression for F2a from above, ultimately yielding
Fa(F2a−1 + Fa−1Fa+1 + F 2a+1) = F3a,
making it clear that F3a is also a multiple of Fa.
Part iv: The first eight rows of the Fibonomial triangle look like
1
1 1
1 1 1
1 2 2 1
1 3 6 3 1
1 5 15 15 5 1
1 8 40 60 40 8 1
1 13 104 260 260 104 13 1
Part v: The identity
((
n+1
k+1
))
= Fn−k+1
((
n
k
))
+ Fk
((
n
k+1
))
is one of many
marvelous relationships among the Fibonacci numbers. To prove it, we
use the formula defining
((
n
k
))
, then find a common denominator. To
save space, we have already cancelled all the factors from Fn−k down to
F1 in the expression for
((
n
k
))
. We find that
Fn−k+1
((
n
k
))
+ Fk
((
n
k + 1
))
= Fn−k+1
Fn · · ·Fn−k+1
Fk · · ·F1 + Fk
Fn · · ·Fn−k
Fk+1 · · ·F1
= Fk+1Fn−k+1
Fn · · ·Fn−k+1
Fk+1 · · ·F1 + FkFn−k
Fn · · ·Fn−k+1
Fk+1 · · ·F1
= (Fk+1Fn−k+1 + FkFn−k)
Fn · · ·Fn−k+1
Fk+1 · · ·F1
= (Fn+1)
Fn · · ·Fn−k+1
Fk+1 · · ·F1 =
((
n+ 1
k + 1
))
.
In the fourth line we used the identity FaFb + Fa+1Fb+1 = Fa+b+1 with
a = k and b = n − k. These steps are valid as long as n > k (so that((
n
k+1
))
is defined) and k > 0 (so that we can write Fk · · ·F1). When
k = 0 the identity reduces to just Fn+1 = Fn+1, which is obviously true.
Assuming that all the entries in one row of the Fibonomial triangle
are integers, we can now deduce that all the entries in the next row
are also. The above identity ensures that
((
n+1
k+1
))
is an integer, except
that it doesn’t apply to
((
n+1
0
))
,
((
n+1
1
))
or
((
n+1
n+1
))
since we must have
n > k > 0. But it is routine to check that these Fibonomials have values
1, Fn+1 and 1, which are still integers.
Part vi: The following statements are all equivalent to the original one:
F 2n+1 − F 2n−1 = 2F 2n + F 2n−1 − F 2n−2
(Fn+1 − Fn−1)(Fn+1 + Fn−1) = 2F 2n + (Fn−1 − Fn−2)(Fn−1 + Fn−2)
(Fn)(Fn+1 + Fn−1) = 2F 2n + (Fn−1 − Fn−2)(Fn)
Fn+1 + Fn−1 = 2Fn + Fn−1 − Fn−2
Now cancelling the Fn−1 term and using Fn − Fn−2 = Fn−1, we arrive
at Fn+1 = Fn + Fn−1, which is clearly true.
It appears that the coefficients in these remarkable identities are
Fibonomial numbers! Following the same pattern, we conjecture that
F 4n+1 = 5F
4
n + 15F
4
n−1 − 15F 4n−2 − 5F 4n−3 ± F 4n−4,
where it is not clear yet whether we should use a ‘+’ or a ‘−’ for the
final term. Testing our conjecture for n = 5 yields
84 = 5(54) + 15(34)− 15(24)− 5(14)± (14)
= 3125 + 1215− 240− 5± 1
= 4095± 1.
Since 84 = 212 = 4096, it is now clear that we should use the ‘+’ sign.
In general, it turns out that the plus and minus signs alternate in pairs.
Thanks to Ron Knott for assembling an informative web page from
which some of the material on this test was drawn. The interested reader
should Google “Knott fibonomial” to visit his page.
c© Greater Testing Concepts 2009
February 2009
Round Two Solutions
Greater Testing Concepts The Mandelbrot Team Play
PO Box 760 web.mandelbrot.org
Potsdam, NY 13676 info@mandelbrot.org
Team Play Solutions
Part i: Proving that 4ISU ∼= 4IWU is fairly routine—we are given
that US ∼= UW , we know that IS ∼= IW since each segment is a radius
of the incircle, and clearly IU ∼= IU . So 4ISU ∼= 4IWU by SSS.
But it is also possible to prove that 4ISU ∼= 4IWU without using
the fact that US ∼= UW . Just argue that IS ∼= IW and IU ∼= IU as
before, observe that 6 IWU and 6 ISU are right angles becauseW and S
are points of tangency, then use HL (hypotenuse-leg) congruence. (This
is how it is possible to deduce that US ∼= UW in the first place.)
Regardless, we next show that m6 WIS = m6 B. Since the sum of
the angles of quadrilateral IWUS is 360◦ and 6 IWU and 6 ISU are right
angles, it follows that m6 WIS + m6 WUS = 180◦. But we also have
m6 AUV +m6 WUS = 180◦, so we deduce that m6 WIS = m 6 AUV .
Lastly, m6 AUV = m6 ABC = m6 B, by the given.
Dividing the above result by two gives 12m6 WIS =
1
2m
6 B. Since
m6 WIU = m 6 SIU and together these two angles make up 6 WIS, we
conclude that each is equal to 12m 6 WIS. Hence m6 SIU =
1
2m
6 B.
Part ii: It is common knowledge that the three angle bisectors of a tri-
angle each pass through the center I of the inscribed circle. Therefore
we know that m 6 RBI = 12m6 B, just as m6 SIU =
1
2m
6 B. (If desired,
one could prove that4RBI ∼= 4TBI using HL congruence, but it is OK
to omit this step.) Furthermore, m 6 BRI = m6 ISU = 90◦. Therefore
4BRI ∼ 4ISU by AA similarity.
Comparing ratios in these similar triangles yields SU/IS = RI/BR.
But IS = IR = r and BR = sb by the givens. Therefore multiplying
through by IS yields SU = r2/sb, as desired.
Part iii: In an analogous fashion one may show that 4ITV ∼ 4CRI,
which leads to TV = r2/sc upon comparing equal ratios. (We omit the
details.) Next note that UV = UW +WV = SU + TV . Thus
UV =
r2
sb
+
r2
sc
= r2
(
sb + sc
sbsc
)
= r2
(
a
rra
)
=
ar
ra
,
where we used the fact that sb+ sc = 2s− b− c = (a+ b+ c)− b− c = a
and also that sbsc = rra, as mentioned in the Facts section.
Part iv: It is possible to prove the given equality solely by algebraic
means, utilizing some of the relationships listed in the Facts section. It
is quite satisfying to watch this identity resolve itself, if you enjoy that
sort of thing. We leave the demonstration to the interested reader, and
instead follow the advice to try a geometric approach.
Based on our previous work, we recognize the quantities appearing
in the given expression. Thus sa − (r2/sc) = AT − TV = AV , and in
the same way sa − (r2/sb) = AS − SU = AU . Of course b = AC and
c = AB, so proving the given equality is tantamount to proving that
AC/AB = AV/AU . And clearly this would follow at once if we could
show that 4ABC ∼ 4AUV . But this is straight-forward; we are given
that 6 AUV ∼= 6 ABC and both triangles share 6 A. Hence the triangles
are similar by AA, and you’re done.
Part v: To prove this unexpected area equality we will first find an
expression for area(BCUV ). To begin, since4ABC ∼ 4AUV we know
that the ratio of their areas is equal to the square of the ratios of their
sides. Thus
area(AUV )
area(ABC)
=
(
UV
BC
)2
=
(
ar/ra
a
)2
=
r2
r2a
.
Letting K = area(ABC), we have area(AUV ) = Kr2/r2a, which means
that area(BCUV ) = area(ABC)− area(AUV ) = K −Kr2/r2a. Hence
area(BCUV ) = K
(
1− r
2
r2a
)
= rasa
(
1 +
r
ra
)(
1− r
ra
)
.
Multiplying ra(1 + r/ra) gives (r+ ra), which is one part of the desired
expression. It remains to show that sa(1 − r/ra) = UV = ar/ra. This
is equivalent to sa(ra− r) = ar, upon multiplying through by ra. Using
the fact rasa = rs we find that
sa(ra − r) = rasa − sar = rs− (s− a)r = ar,
which completes the argument.
Part vi: This formula is reminiscent of Hero’s formulaK =
√
ssasbsc for
a triangle. Except here we have a quadrilateral, and we are multiplying
sides lengths instead of quantities like sa. Nonetheless, the formula is
correct, as we shall show.
First note that BV = BT + TV = sb + r2/sc = (sbsc + r2)/sc. In
the same manner we find that CU = (sbsc + r2)/sb. Therefore we have
√
(BC)(BV )(CU)(UV ) =
√
a
(
sbsc + r2
sc
)(
sbsc + r2
sb
)(
ra
ra
)
= a(sbsc + r2)
√
r
(sbsc)ra
= a(rra + r2)
√
r
(rra)ra
=
(
ra
ra
)
(ra + r)
= (UV )(ra + r)
= area(BCUV ),
according to the result of the previous part.
Well-read students may be familiar with a delightful area formula for
quadrilaterals which possess both an incircle and a circumcircle (neither
condition occurs in general). It states that if the quadrilateral has sides
of length a, b, c and d then its area is given by
√
abcd. This provides an
alternate means of proving the given statement, as long as one explains
why this formula works, and also verifies that BCUV has a circumcircle.
c© Greater Testing Concepts 2009
March 2009
Round Three Solutions
Greater Testing Concepts The Mandelbrot Team Play
PO Box 760 web.mandelbrot.org
Potsdam, NY 13676 info@mandelbrot.org
January 2009
Round One Test Time Limit:
60 minutes�
�
�
�
Setup: consider an infinite sheet of graph paper in which every fifth square is filled in.
More precisely, plot every point (x, y) in the Cartesian plane with 5c ≤ x ≤ 5c + 1 and
5d ≤ y ≤ 5d+1 for integers c and d, meaning that the x and y coordinates are each at most
one more than a multiple of five. We call this collection of squares a lattice, and refer to a
given square by the coordinates of its lower left corner. A portion of the lattice is shown
below, including the (0, 0)-square, the (5, 0)-square, the (0, 5)-square and the (5, 5)-square.
Now let y = mx + b be the equation of a line. We say that this line
cleanly threads the lattice if it does not intersect any of the squares in
the lattice at all. Next, we say that the line barely threads the lattice if
the line contains the vertices of some of the squares, but does not pass
through their interiors. Finally, if a line crosses into the interior of any
square then it does not thread the lattice. These three situations are
illustrated by the top, middle, and bottom lines in the diagram.�
�
�
�
Problems
Part i: (4 points) Find a line with slope 1 that threads the lattice. Give the equation of
such a line and sketch it in the plane along with at least four nearby lattice squares. Now do
the same for lines having slopes −1
2
, 2
3
and 3. Which line only barely threads the lattice?
Part ii: (5 points) Show that if there is a line with slope m that cleanly threads the lattice,
then there are lines with slope −m, 1
m
and − 1
m
that also cleanly thread the lattice. (You do
not need to work with equations of lines here; a geometric argument is sufficient.)
Part iii: (4 points) Suppose that light rays with slope 3
4
shine from the right. Describe the
shadow cast onto the y-axis by the (5, 5)-square. (Give its endpoints and length.)
Part iv: (5 points) Continuing the previous part, demonstrate that there is another square
in the lattice whose shadow is slightly higher than but overlaps with that of the (5, 5)-square.
Extend these ideas to prove that a slope 3
4
line cannot thread the lattice.
Part v: (5 points) In general, let m = p
q
be a slope which is a positive rational number,
and consider light rays with slope m. Prove that if p + q > 5 then there exists a square in
the lattice whose shadow on the y-axis overlaps with the shadow cast by the (0, 0)-square.
Part vi: (5 points) Let m = p
q
be a positive fraction with p+ q > 5 as before. Prove that
a slope m line cannot thread the lattice. Finally, conjecture what happens if p+ q = 5.
c© Greater Testing Concepts 2008
February 2009
Round Two Test Time Limit:
60 minutes�
�
�
�
Facts: The Fibonacci numbers are the sequence of integers 0, 1, 1, 2, 3, 5, 8, 13, 21, 34, . . .
in which each number is the sum of the two previous numbers. The kth Fibonacci number is
written Fk, so this sequence satisfies F0 = 0, F1 = 1, and Fk+1 = Fk + Fk−1 for k ≥ 1.�
�
�
�
Setup: We will write “k Fibonacci-factorial,” denoted as FF (k), to represent the product
of the k Fibonacci numbers from Fk down to F1. Thus FF (5) = 5 · 3 · 2 · 1 · 1 = 30. We also
declare that FF (0) = 1. We can now define
((
n
k
))
, called a Fibonomial, as((
n
k
))
=
FF (n)
FF (k) · FF (n− k) .
Thus
((
5
3
))
= FF (5)
FF (3)·FF (2) =
30
2·1 = 15. One can also confirm that
((
7
6
))
= 13 and that
((
0
0
))
= 1.
�
�
�
�
Problems
Part i: (4 points) One of the more delightful relationships among the Fibonacci numbers
states that FaFb + Fa+1Fb+1 = Fa+b+1. To begin, explain why this statement is true when
b = 0 or b = 1. Also confirm the equality when a = 5 and b = 7.
Part ii: (5 points) Now prove that FaFb + Fa+1Fb+1 = Fa+b+1 holds for all a ≥ 0 and all
b ≥ 0 by using induction on b. (The previous part demonstrates the base cases.)
Part iii: (5 points) By choosing a strategic value for b in the above relationship, show that
for a ≥ 1, F2a is a multiple of Fa. Based on this, next show that F3a is also a multiple of Fa.
Part iv: (4 points) There is a “Fibonomial triangle” whose nth row consists of the numbers((
n
0
))
,
((
n
1
))
, up to
((
n
n
))
. Compute rows n = 0 through n = 7, listing them on top of one
another in a triangular arr
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