MYSTERIES OF THE EQUILATERAL TRIANGLE - HIKARI Ltd
MYSTERIES OF THE EQUILATERAL TRIANGLE - HIKARI Ltd
MYSTERIES OF THE EQUILATERAL TRIANGLE - HIKARI Ltd
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Mathematical Recreations 109<br />
To form a trihexaflexagon, begin with a strip of paper with ten equilateral<br />
triangles numbered as shown in Figure 4.10. Then, fold along ab, fold along cd,<br />
fold back the protruding triangle and glue it to the back of the adjacent triangle<br />
and Voila! The assembled trihexaflexagon is a continuous band of hinged triangles<br />
with a hexagonal outline (“face”). If the trihexaflexagon is “pinch-flexed”<br />
[244], as shown, then one face will become hidden and a new face appears.This<br />
remarkable geometrical construction was discovered by Arthur H. Stone when<br />
he was a Mathematics graduate student at Princeton University in 1939. A<br />
Flexagon Committe consisting of Stone, Bryant Tuckerman, Richard P. Feynman<br />
and John W. Tukey was formed to probe its mathematical properties<br />
which are many and sundry [244].<br />
Figure 4.11: Bertrand’s Paradox [122]<br />
Recreation 11 (Bertrand’s Paradox [122]). The probability that a chord<br />
drawn at random inside a circle will be longer than the side of the inscribed<br />
equilateral triangle is equal to 1 1 , 3 2<br />
and 1<br />
4 [122]!<br />
With reference to the top of Figure 4.11, if one endpoint of the chord is fixed<br />
at A and the other endpoint is allowed to vary then the probability is equal<br />
to 1.<br />
Alternatively (Figure 4.11 bottom left), if the diameter perpendicular to<br />
3<br />
the chord is fixed and the chord allowed to slide along it then the probability<br />
is equal to 1.<br />
Finally (Figure 4.11 bottom right), if both endpoints of the<br />
2<br />
chord are free and we focus on its midpoint then the required probability is<br />
computed to be 1.<br />
Physical realizations of all three scenarios are provided in<br />
4<br />
[122] thus showing that caution must be used when the phrase “at random” is<br />
bandied about, especially in a geometric context.