A point is placed inside an equilateral triangle so that its
distances from the three vertices are 5, 12, and 13. Find the area of the
triangle.
Solution 1. Our solution combines ideas from Fondanaiche, LoPresti, Rexhepi, Robinson, and Sengupta.
FIGURE 1
In Figure 1, ΔABC has sides of length s and an interior point P. A clockwise rotation through 60° about A takes C to B and P to a point P'; thus AP' = AP = 5, BP' = 13, and (because ΔAP'P is equilateral), P'P = 5. It follows that ΔBP'P has sides 5, 12, and 13, whence the angle at P is 90°. Consequently, ∠BPA = 60° + 90° = 150°. The cosine law (with cos 150° = –√3/2) then says that s satisfies
s2 = AB2 = 52 + 122 –
2·5·12cos 150° = 169 + 60√3.
The area of ΔABC is therefore
which equals about 118.18.
Fondanaiche avoided using the cosine law in his solution by extending BP to the foot of the perpendicular from A, called H in the above diagram on the right. ΔAPH is then a right triangle with angles of 30° and 60°, so that AH = 5/2 and PH = (5√3)/2, whence
as before.
2 Collignon's Solution.
FIGURE 2
For this solution we rotate P clockwise through 60° about A to get C', about B to get A', and about C to get B'. We note that ΔAC'B is congruent to ΔAPC, ΔBA'C is congruent to
ΔBPA, and
ΔCB'A
is congruent toΔCPB; this tells us
that the area of the hexagon AC'BA'CB' is exactly twice the area [ABC] that we seek. We see that the hexagon consists of
three equilateral triangles (whose equal sides have length 5, 12, and 13), and
three congruent right triangles. Thus,
2[ABC] = [AC'BA'CB']
= [AC'P] + [BA'P] + [CB'P] + 3[PC'B]
and [ABC]
= 169(√3/4) + 45.
3 Nadauld's Solution.
Instead of rotating the point P, we reflect it in the sides AB to get C', BC to get A', and CA to get B'. Because each triangle inside ΔABC that shares the vertex P (such as
FIGURE 3
ΔAPB) is
congruent to its reflected image (namely ΔAC'B), the area
[AC'BA'CB'] of the outside
hexagon is twice the area [ABC]
of the given triangle. Each of the triangles AC'B', BA'C',
CB'A' are isosceles with an apex angle of
120°; indeed, each is composed of a pair of 30-60 right triangles with
respective hypotenuses 5, 12, and 13. The sides opposite the 120° angles
therefore have lengths B'C' = 5√3, C'A' = 12√3, and A'B' = 13√3,
which implies that ∠A'C'B' = 90°. Consequently,
2[ABC] = [AC'BA'CB']
= [AC'B'] + [BA'C'] + [CB'A'] + [A'B'C']
and [ABC]
= 169(√3/4) + 45.
Solution 4. A version of this solution came from de Visme, Stadler, and Teitelman. We present Stadler's solution.
Let α, β, and γ be the three angles at P; specifically let α = BPC, β = ∠CPA, and γ = ∠APB. Let s be the side of the triangle. Then, by the Law of Cosines:
,
and (*)
Because α + β + γ = 2, we have ; whence , and finally,
We insert the values from (*) into this equation and get a sixth
degree equation for the side s, namely
s2(s4 - 338 s2 + 17761) =
0.
(A computer algebra system is helpful in this last step!) This
last equation has the solutions s2 =0, and s2 = 169 ±
60√3. A quick check exhibits that only the solution s2 = 169 + 60√3 satisfies α +
β + γ = 2. This value of s2 produces
the value [ABC]
= 169(√3/4) + 45 for the area of the triangle.
Comments. Several
correspondents noted that there is nothing special about a 5-12-13 right
triangle. The same four arguments would produce the area of ΔABC any time
the distances a, b, and c to the vertices from P satisfy
a2 + b2 = c2. Robinson
further generalized the problem; he found the area [ABC] for any point P inside the triangle
in terms of the distances a =
PA, b =
PB, and c =
PC. In fact, our solution 3 (from Nadauld) gives
us the answer with no further work: instead of finding the area of ΔA'B'C' by
using properties of right triangles, we can use Heron's formula and
obtain,
[ABC] = ½ [AC'BA'CB']
= ½ ([AC'B'] + [BA'C'] + [CB'A'] + [A'B'C'])
A remarkable consequence of this argument is that no matter where P is chosen inside the equilateral triangle, the distances a, b, c satisfy the triangle inequality; in other words, the distances from P to the vertices are not arbitrary, but must form the sides of ΔA'B'C'. Dimitrie Pompeïu made this observation in 1936. In fact, Pompeïu's Theorem states that'
For any point P in the plane of DABC, the lengths of the line segments PA, PB, PC correspond to the sides of a triangle except when P lies on the circumcircle of ΔABC, in which case the reflections of P in the sides, namely A', B', C', would lie on a line.
Sengupta pointed us to the MathWorld web page
where there is a neat formula from Martin Gardner (Mathematical Carnival: A New Round-Up of Tantalizers and Puzzles from Scientific American, New York: Vintage Books, 1977, pages 56-57 and 63) for the side s of the equilateral triangle:
3(a4 + b4 +
c4 + s4)=(a2 + b2 + c2 +
s2 )2 ;
this equation can be obtained by replacing [ABC] with s2√3/4 in Robinson's equation just above, then rearranging terms. Richard Guy reports (in Unsolved Problems in Number Theory, 2nd ed. New York: Springer-Verlag, 1994; see especially Section D19, page 183) that a computer search showed that a = 57, b = 65, c = 73, and s = 112 is the smallest example for which all the parameters are integers. Moreover, there is an infinite family of integer solutions given by
a = m2 + n2, b = m2 + mn + n2, c = m2 – mn + n2,
with m = 2(u2 + v2), n = u2 + 4uv + v2
with m = 2(u2 + v2), n = u2 + 4uv + v2
and, therefore,
s = 8(u2 – v2)(u2 + uv + v2).
Our own modest search found the problem discussed at least twice by Dr. Math:
whose source was a Mensa problem around 2002, and item 55022 where there is a discussion from 1998. It can also be found as problem 3682 in School Science and Mathematics around 1975 (according to Stanley Rabinowitz's Index to Math Problems 1975-1979, p. 135). See also Charles W. Trigg, Mathematical Quickies: 270 Stimulating Problems with Solutions. Dover (1985); originally published in 1967.
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