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Bertrand's Paradox

Bertrand's Paradox calculator. Random chords in a circle: Method 1 gives 1/3, Method 2 gives 1/2, Me

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GEOMETRIC PROBABILITYRandom chord in a circle

Bertrand's Paradox โ€” Random Chord: 1/3, 1/2, or 1/4

Same question, three valid answers. Method 1 (endpoints): 1/3. Method 2 (radial): 1/2. Method 3 (midpoint): 1/4. "Random" is ambiguous without a selection method.

Examples โ€” Click to Load

Selection Method

Visual: Circle, Triangle & Sample Chords

Green = long chord, Red = short chord

Method 1: Two random points on the circle

Theoretical P(long chord) = 0.3333333333333333 (33%)

Simulation

bertrand_paradox.sh
METHOD 1 โ€” P = 0.3333333333333333
Theoretical P
33%
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Bertrand's Paradox (Chord)
Method 1: P(long chord)
0.3333333333333333
1/3, 1/2, 1/4
numbervibe.com/calculators/statistics/bertrand-paradox

Method Comparison โ€” All Three Probabilities

Simulation Results โ€” Long vs Short Chords

Run simulation to see results

โš ๏ธFor educational and informational purposes only. Verify with a qualified professional.

๐Ÿ“‹ Key Takeaways

  • โ€ข The same question "what is a random chord?" gives 3 different valid answers depending on the selection method
  • โ€ข This paradox shows that probability requires a well-defined sample space โ€” "random" alone is ambiguous
  • โ€ข Method 1 (endpoints): P=1/3, Method 2 (radial): P=1/2, Method 3 (midpoint): P=1/4
  • โ€ข The paradox is resolved by noting each method defines a different probability measure on the space of chords
  • โ€ข Modern resolution: Jaynes (1973) argued Method 2 (P=1/2) is the "natural" answer based on maximum entropy

๐Ÿ’ก Did You Know

๐ŸŽฉJoseph Bertrand posed this in 1889 to show that geometric probability needs careful definitions
๐Ÿ”ฌE.T. Jaynes in 1973 argued using maximum entropy principle that P=1/2 is the 'correct' answer
๐Ÿ“The paradox is a founding problem in geometric probability and measure theory
๐ŸŽฏPhysical experiments (dropping straws on a circle) consistently give results near 1/2, supporting Jaynes
๐ŸงฎThe paradox inspired rigorous definitions of probability measures on continuous spaces
๐Ÿ“ŠThis is related to the Buffon's needle problem โ€” another geometric probability classic
๐Ÿค”There are actually infinitely many valid answers, not just three โ€” depending on the distribution over chords

๐Ÿ“– How It Works

1. The Setup

Equilateral triangle inscribed in a circle. A chord is longer than a triangle side if it subtends an arc > 120ยฐ. We ask: P(random chord > side).

2. Method 1: Random Endpoints โ€” P=1/3

Fix one point on the circle, choose another uniformly. Chord is long if the other point falls in the "long chord" arc (1/3 of circumference).

3. Method 2: Random Radial Point โ€” P=1/2

Choose a random radius, pick a random point on it, draw perpendicular chord. Chord is long if the point is closer to center than the midpoint of a triangle side (which bisects the radius).

4. Method 3: Random Midpoint โ€” P=1/4

Choose a random point inside the circle as the chord's midpoint. Chord is long if midpoint falls within inner circle of radius r/2. Area ratio = ฯ€(r/2)ยฒ/(ฯ€rยฒ) = 1/4.

๐ŸŽฏ Expert Tips

Always define your sample space

Probability without a well-defined measure is meaningless

Jaynes' resolution

Maximum entropy suggests Method 2 when you have no prior information

Physical verification

Drop spaghetti on a circle โ€” it empirically supports P=1/2

This generalizes

The lesson applies to any continuous probability: specify HOW randomness is generated

โš–๏ธ Method Comparison

AspectMethod 1Method 2Method 3
ConstructionRandom endpoints on circleRandom point on random radiusRandom midpoint in disk
Probability1/31/21/4
Physical meaningPick 2 points on rimDrop perpendicular from radiusThrow dart at disk

โ“ Frequently Asked Questions

Which answer (1/3, 1/2, or 1/4) is "correct"?

All three are correct under their respective selection procedures. The paradox shows that 'random chord' is underspecified โ€” you must define HOW the chord is chosen.

What does this paradox teach us about probability?

Probability requires a well-defined sample space and measure. 'Random' alone is ambiguous for continuous spaces.

How did Jaynes resolve the paradox?

Jaynes (1973) used the maximum entropy principle: with no prior information, Method 2 (P=1/2) maximizes entropy and is the 'natural' choice. Physical experiments support this.

What is geometric probability?

Geometric probability assigns probabilities based on geometric measures (length, area, volume). Bertrand's paradox is a classic example where different geometric parameterizations give different answers.

How do physical experiments relate to the paradox?

Dropping straws or needles onto a circle naturally implements something like Method 2. Experiments consistently yield P โ‰ˆ 1/2, supporting Jaynes' resolution.

Is this related to the Monty Hall problem?

Both involve careful specification of randomness. Monty Hall is about conditional probability; Bertrand's paradox is about defining the sample space. Different lessons, but both show that 'random' needs precision.

What is the maximum entropy principle?

When you have no prior information, choose the distribution that maximizes entropy (uncertainty). Jaynes argued this singles out Method 2 as the 'least informative' prior.

How does this paradox apply to real-world problems?

Whenever you model 'random' selection in continuous spaces (e.g., random sampling, Monte Carlo methods), you must specify the distribution. The paradox is a cautionary tale for statisticians and modelers.

๐Ÿ“Š Infographic Stats

1/3
Method 1 Answer
1/2
Method 2 Answer
1/4
Method 3 Answer
1889
Year Published

โš ๏ธ Disclaimer: This calculator demonstrates Bertrand's chord paradox for educational purposes. Each method is mathematically valid; the paradox illustrates that "random" must be precisely defined. Simulations are subject to random variation.

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