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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.

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